var bibbase_data = {"data":"<img src=\"//bibbase.org/img/ajax-loader.gif\" id=\"spinner\"\n  style=\"display: none;\" alt=\"Loading..\" />\n\n<div id=\"bibbase\">\n\n  <script type=\"text/javascript\">\n    var bibbase = {\n      params: {\"bib\":\"https://bibbase.org/f/NkS9m4R3ieFPicBbH/nanokafedra2002-2023.bib\",\"noBootstrap\":\"1\",\"jsonp\":\"1\",\"folding\":\"1\",\"theme\":\"default\",\"host\":\"bibbase.org\"},\n      data: [{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Hidden symmetry of the anomalous bluetongue virus capsid and its role in the infection process\",\"volume\":\"15\",\"issn\":\"1744-6848\",\"url\":\"https://pubs.rsc.org/en/content/articlelanding/2019/sm/c9sm01335k\",\"doi\":\"10.1039/C9SM01335K\",\"abstract\":\"Clear understanding of the principles that control the arrangement of proteins and their self-assembly into viral shells is very important for the development of antiviral strategies. Here we consider the structural peculiarities and hidden symmetry of the anomalous bluetongue virus (BTV) capsid. Each of its three concentric shells violates the paradigmatic geometrical model of Caspar and Klug, which is otherwise well suited to describe most of the known icosahedral viral shells. As we show, three icosahedral spherical lattices, which are commensurate with each other and possess locally hexagonal (primitive or honeycomb) order, underlie the proteinaceous shells of the BTV capsid. This interpretation of the multishelled envelope allows us to discuss the so-called “symmetry mismatch” between its layers. We also analyze the structural stability of the considered spherical lattices on the basis of the classical theory of spherical packing and relate the proximity of the outer spherical lattice to destabilization with the fact that during infection of the cell VP2 trimers are detached from the surface of the BTV capsid. An electrostatic mechanism that can assist in this detachment is discussed in detail.\",\"language\":\"en\",\"number\":\"38\",\"urldate\":\"2023-11-11\",\"journal\":\"Soft Matter\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Konevtsova\"],\"firstnames\":[\"Olga\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Roshal\"],\"firstnames\":[\"Daria\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Božič\"],\"firstnames\":[\"Anže\",\"Lošdorfer\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Podgornik\"],\"firstnames\":[\"Rudolf\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergey\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2019\",\"note\":\"Publisher: The Royal Society of Chemistry\",\"pages\":\"7663–7671\",\"bibtex\":\"@article{konevtsova_hidden_2019,\\n\\ttitle = {Hidden symmetry of the anomalous bluetongue virus capsid and its role in the infection process},\\n\\tvolume = {15},\\n\\tissn = {1744-6848},\\n\\turl = {https://pubs.rsc.org/en/content/articlelanding/2019/sm/c9sm01335k},\\n\\tdoi = {10.1039/C9SM01335K},\\n\\tabstract = {Clear understanding of the principles that control the arrangement of proteins and their self-assembly into viral shells is very important for the development of antiviral strategies. Here we consider the structural peculiarities and hidden symmetry of the anomalous bluetongue virus (BTV) capsid. Each of its three concentric shells violates the paradigmatic geometrical model of Caspar and Klug, which is otherwise well suited to describe most of the known icosahedral viral shells. As we show, three icosahedral spherical lattices, which are commensurate with each other and possess locally hexagonal (primitive or honeycomb) order, underlie the proteinaceous shells of the BTV capsid. This interpretation of the multishelled envelope allows us to discuss the so-called “symmetry mismatch” between its layers. We also analyze the structural stability of the considered spherical lattices on the basis of the classical theory of spherical packing and relate the proximity of the outer spherical lattice to destabilization with the fact that during infection of the cell VP2 trimers are detached from the surface of the BTV capsid. An electrostatic mechanism that can assist in this detachment is discussed in detail.},\\n\\tlanguage = {en},\\n\\tnumber = {38},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Soft Matter},\\n\\tauthor = {Konevtsova, Olga V. and Roshal, Daria S. and Božič, Anže Lošdorfer and Podgornik, Rudolf and Rochal, Sergey},\\n\\tmonth = oct,\\n\\tyear = {2019},\\n\\tnote = {Publisher: The Royal Society of Chemistry},\\n\\tpages = {7663--7671},\\n}\\n\\n\",\"author_short\":[\"Konevtsova, O. V.\",\"Roshal, D. S.\",\"Božič, A. L.\",\"Podgornik, R.\",\"Rochal, S.\"],\"key\":\"konevtsova_hidden_2019\",\"id\":\"konevtsova_hidden_2019\",\"bibbaseid\":\"konevtsova-roshal-boi-podgornik-rochal-hiddensymmetryoftheanomalousbluetongueviruscapsidanditsroleintheinfectionprocess-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://pubs.rsc.org/en/content/articlelanding/2019/sm/c9sm01335k\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"Hertz-to-terahertz dielectric response of nanoconfined water molecules\",\"url\":\"https://ieeexplore.ieee.org/document/8873987\",\"doi\":\"10.1109/IRMMW-THz.2019.8873987\",\"abstract\":\"Broad-band dielectric spectroscopy, heat capacity measurements and molecular dynamic simulations are applied to study excitations of interacting electric dipoles spatially arranged in a network with an inter-dipole distance of 5-10 Å. The dipoles with magnitude of 1.85 Debye are represented by single H2O molecules located in voids (0.5 nm size) formed by ions of the crystal lattice of cordierite. We discover emergence of nontrivial disordered paraelectric phase of dipolar system with signs of phase transition below 3 K.\",\"urldate\":\"2023-11-11\",\"booktitle\":\"2019 44th International Conference on Infrared, Millimeter, and Terahertz Waves (IRMMW-THz)\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Belyanchikov\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Savinov\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bednyakov\"],\"firstnames\":[\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bedran\"],\"firstnames\":[\"Z.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Thomas\"],\"firstnames\":[\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Loidl\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lunkenheimer\"],\"firstnames\":[\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Uykur\"],\"firstnames\":[\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"B.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2019\",\"note\":\"ISSN: 2162-2035\",\"pages\":\"1–3\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\DNQPGUUM\\\\\\\\Belyanchikov и др. - 2019 - Hertz-to-terahertz dielectric response of nanoconf.pdf:application/pdf;IEEE Xplore Abstract Record:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\RR6G2M8H\\\\\\\\8873987.html:text/html\",\"bibtex\":\"@inproceedings{belyanchikov_hertz--terahertz_2019,\\n\\ttitle = {Hertz-to-terahertz dielectric response of nanoconfined water molecules},\\n\\turl = {https://ieeexplore.ieee.org/document/8873987},\\n\\tdoi = {10.1109/IRMMW-THz.2019.8873987},\\n\\tabstract = {Broad-band dielectric spectroscopy, heat capacity measurements and molecular dynamic simulations are applied to study excitations of interacting electric dipoles spatially arranged in a network with an inter-dipole distance of 5-10 Å. The dipoles with magnitude of 1.85 Debye are represented by single H2O molecules located in voids (0.5 nm size) formed by ions of the crystal lattice of cordierite. We discover emergence of nontrivial disordered paraelectric phase of dipolar system with signs of phase transition below 3 K.},\\n\\turldate = {2023-11-11},\\n\\tbooktitle = {2019 44th {International} {Conference} on {Infrared}, {Millimeter}, and {Terahertz} {Waves} ({IRMMW}-{THz})},\\n\\tauthor = {Belyanchikov, M. and Savinov, M. and Bednyakov, P. and Bedran, Z. and Thomas, V. and Torgashev, V. and Prokhorov, A. and Loidl, A. and Lunkenheimer, P. and Zhukova, E. and Uykur, E. and Dressel, M. and Gorshunov, B.},\\n\\tmonth = sep,\\n\\tyear = {2019},\\n\\tnote = {ISSN: 2162-2035},\\n\\tpages = {1--3},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\DNQPGUUM\\\\\\\\Belyanchikov и др. - 2019 - Hertz-to-terahertz dielectric response of nanoconf.pdf:application/pdf;IEEE Xplore Abstract Record:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\RR6G2M8H\\\\\\\\8873987.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Belyanchikov, M.\",\"Savinov, M.\",\"Bednyakov, P.\",\"Bedran, Z.\",\"Thomas, V.\",\"Torgashev, V.\",\"Prokhorov, A.\",\"Loidl, A.\",\"Lunkenheimer, P.\",\"Zhukova, E.\",\"Uykur, E.\",\"Dressel, M.\",\"Gorshunov, B.\"],\"key\":\"belyanchikov_hertz--terahertz_2019\",\"id\":\"belyanchikov_hertz--terahertz_2019\",\"bibbaseid\":\"belyanchikov-savinov-bednyakov-bedran-thomas-torgashev-prokhorov-loidl-etal-hertztoterahertzdielectricresponseofnanoconfinedwatermolecules-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://ieeexplore.ieee.org/document/8873987\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Structural Peculiarities of the Intermediate Phase in Zr-Rich Lead Zirconate Titanate\",\"volume\":\"61\",\"issn\":\"1090-6460\",\"url\":\"https://doi.org/10.1134/S1063783419100056\",\"doi\":\"10.1134/S1063783419100056\",\"abstract\":\"This paper presents the results of X-ray diffraction studies on a single crystal of lead zirconate titanate PbZr0.993Ti0.007O3 in the region of existence of an intermediate ferroelectric phase. In addition to the known superstructure reflections of the M type qM = $$\\\\left\\\\\\\\ \\\\\\\\frac\\\\1\\\\\\\\2\\\\,\\\\frac\\\\1\\\\\\\\2\\\\,0\\\\ \\\\right\\\\\\\\$$and the first-order satellite reflections qM + \\\\δ, δ, δ\\\\, unknown second-order satellites have been observed near qM and near the Bragg reflections. Structural model of regular system of antiphase domains is used for diffraction calculation. The model is shown to describe the first- and second-orders satellite reflections in the vicinity of qM, but it cannot explain the appearance of satellites around the main Bragg peaks. A possible origin of the system of the superstructures observed in the intermediate phase is discussed.\",\"language\":\"en\",\"number\":\"10\",\"urldate\":\"2023-11-11\",\"journal\":\"Physics of the Solid State\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Andronikova\"],\"firstnames\":[\"D.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bronwald\"],\"firstnames\":[\"I.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"N.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chernyshov\"],\"firstnames\":[\"D.\",\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Filimonov\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vakhrushev\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2019\",\"keywords\":\"ferroelectrics, phase transitions, and crystal structure, perovskite structure, X-ray scattering\",\"pages\":\"1772–1778\",\"bibtex\":\"@article{andronikova_structural_2019,\\n\\ttitle = {Structural {Peculiarities} of the {Intermediate} {Phase} in {Zr}-{Rich} {Lead} {Zirconate} {Titanate}},\\n\\tvolume = {61},\\n\\tissn = {1090-6460},\\n\\turl = {https://doi.org/10.1134/S1063783419100056},\\n\\tdoi = {10.1134/S1063783419100056},\\n\\tabstract = {This paper presents the results of X-ray diffraction studies on a single crystal of lead zirconate titanate PbZr0.993Ti0.007O3 in the region of existence of an intermediate ferroelectric phase. In addition to the known superstructure reflections of the M type qM = \\\\$\\\\${\\\\textbackslash}left{\\\\textbackslash}\\\\{ \\\\{{\\\\textbackslash}frac\\\\{1\\\\}\\\\{2\\\\},{\\\\textbackslash}frac\\\\{1\\\\}\\\\{2\\\\},0\\\\} {\\\\textbackslash}right{\\\\textbackslash}\\\\}\\\\$\\\\$and the first-order satellite reflections qM + \\\\{δ, δ, δ\\\\}, unknown second-order satellites have been observed near qM and near the Bragg reflections. Structural model of regular system of antiphase domains is used for diffraction calculation. The model is shown to describe the first- and second-orders satellite reflections in the vicinity of qM, but it cannot explain the appearance of satellites around the main Bragg peaks. A possible origin of the system of the superstructures observed in the intermediate phase is discussed.},\\n\\tlanguage = {en},\\n\\tnumber = {10},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physics of the Solid State},\\n\\tauthor = {Andronikova, D. A. and Bronwald, I. A. and Leontyev, N. G. and Leontyev, I. N. and Chernyshov, D. Yu. and Filimonov, A. V. and Vakhrushev, S. B.},\\n\\tmonth = oct,\\n\\tyear = {2019},\\n\\tkeywords = {ferroelectrics, phase transitions, and crystal structure, perovskite structure, X-ray scattering},\\n\\tpages = {1772--1778},\\n}\\n\\n\",\"author_short\":[\"Andronikova, D. A.\",\"Bronwald, I. A.\",\"Leontyev, N. G.\",\"Leontyev, I. N.\",\"Chernyshov, D. Y.\",\"Filimonov, A. V.\",\"Vakhrushev, S. B.\"],\"key\":\"andronikova_structural_2019\",\"id\":\"andronikova_structural_2019\",\"bibbaseid\":\"andronikova-bronwald-leontyev-leontyev-chernyshov-filimonov-vakhrushev-structuralpeculiaritiesoftheintermediatephaseinzrrichleadzirconatetitanate-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1063783419100056\"},\"keyword\":[\"ferroelectrics\",\"phase transitions\",\"and crystal structure\",\"perovskite structure\",\"X-ray scattering\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Chirality manifestation in elastic coupling between the layers of double-walled carbon nanotubes\",\"volume\":\"11\",\"issn\":\"2040-3372\",\"url\":\"https://pubs.rsc.org/en/content/articlelanding/2019/nr/c9nr03853a\",\"doi\":\"10.1039/C9NR03853A\",\"abstract\":\"The search for new relatively easy physicochemical methods for the structural identification of carbon nanotubes represents a key challenge. Here, analyzing the experimental data on double-walled carbon nanotubes (DWCNTs) obtained by us and taken from the literature, we have expressed the magnitude of elastic coupling between two tubular walls forming a DWCNT as a simple function dependent not only on DWCNT diameters but also on the difference between the chirality angles of the constituent nanotubes. To get this quite unexpected result, which allows us to relate more precisely the structural parameters of a DWCNT with frequencies of its radial breathing-like modes (RBLM), we have developed a new model for the RBLM dynamics that takes into account a possible deposition of water molecules from ambient air onto the DWCNT surface. The model constructed allows us to predict the higher prevalence of DWCNTs comprising two walls with identical handedness. The application of the results obtained for the identification of DWCNTs is also considered.\",\"language\":\"en\",\"number\":\"34\",\"urldate\":\"2023-11-11\",\"journal\":\"Nanoscale\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergei\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Levshov\"],\"firstnames\":[\"Dmitry\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Avramenko\"],\"firstnames\":[\"Marina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Arenal\"],\"firstnames\":[\"Raul\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Cao\"],\"firstnames\":[\"Thi\",\"Thanh\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nguyen\"],\"firstnames\":[\"Van\",\"Chuc\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sauvajol\"],\"firstnames\":[\"Jean-Louis\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Paillet\"],\"firstnames\":[\"Matthieu\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2019\",\"note\":\"Publisher: The Royal Society of Chemistry\",\"pages\":\"16092–16102\",\"file\":\"Supplementary Information PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\EJHII2SI\\\\\\\\Rochal и др. - 2019 - Chirality manifestation in elastic coupling betwee.pdf:application/pdf\",\"bibtex\":\"@article{rochal_chirality_2019,\\n\\ttitle = {Chirality manifestation in elastic coupling between the layers of double-walled carbon nanotubes},\\n\\tvolume = {11},\\n\\tissn = {2040-3372},\\n\\turl = {https://pubs.rsc.org/en/content/articlelanding/2019/nr/c9nr03853a},\\n\\tdoi = {10.1039/C9NR03853A},\\n\\tabstract = {The search for new relatively easy physicochemical methods for the structural identification of carbon nanotubes represents a key challenge. Here, analyzing the experimental data on double-walled carbon nanotubes (DWCNTs) obtained by us and taken from the literature, we have expressed the magnitude of elastic coupling between two tubular walls forming a DWCNT as a simple function dependent not only on DWCNT diameters but also on the difference between the chirality angles of the constituent nanotubes. To get this quite unexpected result, which allows us to relate more precisely the structural parameters of a DWCNT with frequencies of its radial breathing-like modes (RBLM), we have developed a new model for the RBLM dynamics that takes into account a possible deposition of water molecules from ambient air onto the DWCNT surface. The model constructed allows us to predict the higher prevalence of DWCNTs comprising two walls with identical handedness. The application of the results obtained for the identification of DWCNTs is also considered.},\\n\\tlanguage = {en},\\n\\tnumber = {34},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Nanoscale},\\n\\tauthor = {Rochal, Sergei and Levshov, Dmitry and Avramenko, Marina and Arenal, Raul and Cao, Thi Thanh and Nguyen, Van Chuc and Sauvajol, Jean-Louis and Paillet, Matthieu},\\n\\tmonth = aug,\\n\\tyear = {2019},\\n\\tnote = {Publisher: The Royal Society of Chemistry},\\n\\tpages = {16092--16102},\\n\\tfile = {Supplementary Information PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\EJHII2SI\\\\\\\\Rochal и др. - 2019 - Chirality manifestation in elastic coupling betwee.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Rochal, S.\",\"Levshov, D.\",\"Avramenko, M.\",\"Arenal, R.\",\"Cao, T. T.\",\"Nguyen, V. C.\",\"Sauvajol, J.\",\"Paillet, M.\"],\"key\":\"rochal_chirality_2019\",\"id\":\"rochal_chirality_2019\",\"bibbaseid\":\"rochal-levshov-avramenko-arenal-cao-nguyen-sauvajol-paillet-chiralitymanifestationinelasticcouplingbetweenthelayersofdoublewalledcarbonnanotubes-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://pubs.rsc.org/en/content/articlelanding/2019/nr/c9nr03853a\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Some dynamic features of ferroelectric thin films\",\"volume\":\"1260\",\"issn\":\"1742-6596\",\"url\":\"https://dx.doi.org/10.1088/1742-6596/1260/9/092004\",\"doi\":\"10.1088/1742-6596/1260/9/092004\",\"abstract\":\"The dynamic problem of the surface acoustic wave propagation in a thin-film structure is investigated. The propagation of plane waves in the film-substrate structure is considered. Thin film is made of barium titanate oxide, and solid substrate is made of magnesium oxide. Ferroelectric film is subjected to misfit strain because of the deposition. Assumed that the solid substrate retains its properties due to the large difference in the hardness of the materials. Built Green function, obtained phase velocities and electromechanical coupling coefficients in the C-phase of BaTiO3. The present investigation is of practical interest for developing high-frequencies smart ferroelectric devices for engineering applications.\",\"language\":\"en\",\"number\":\"9\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics: Conference Series\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Levi\"],\"firstnames\":[\"M.\",\"O.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kalinchuk\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2019\",\"note\":\"Publisher: IOP Publishing\",\"pages\":\"092004\",\"file\":\"IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\7XMUB7ZU\\\\Łevi и др. - 2019 - Some dynamic features of ferroelectric thin films.pdf:application/pdf\",\"bibtex\":\"@article{levi_dynamic_2019,\\n\\ttitle = {Some dynamic features of ferroelectric thin films},\\n\\tvolume = {1260},\\n\\tissn = {1742-6596},\\n\\turl = {https://dx.doi.org/10.1088/1742-6596/1260/9/092004},\\n\\tdoi = {10.1088/1742-6596/1260/9/092004},\\n\\tabstract = {The dynamic problem of the surface acoustic wave propagation in a thin-film structure is investigated. The propagation of plane waves in the film-substrate structure is considered. Thin film is made of barium titanate oxide, and solid substrate is made of magnesium oxide. Ferroelectric film is subjected to misfit strain because of the deposition. Assumed that the solid substrate retains its properties due to the large difference in the hardness of the materials. Built Green function, obtained phase velocities and electromechanical coupling coefficients in the C-phase of BaTiO3. The present investigation is of practical interest for developing high-frequencies smart ferroelectric devices for engineering applications.},\\n\\tlanguage = {en},\\n\\tnumber = {9},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics: Conference Series},\\n\\tauthor = {Levi, M. O. and Kalinchuk, V. V. and Shirokov, V. B.},\\n\\tmonth = aug,\\n\\tyear = {2019},\\n\\tnote = {Publisher: IOP Publishing},\\n\\tpages = {092004},\\n\\tfile = {IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\7XMUB7ZU\\\\\\\\Levi и др. - 2019 - Some dynamic features of ferroelectric thin films.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Levi, M. O.\",\"Kalinchuk, V. V.\",\"Shirokov, V. B.\"],\"key\":\"levi_dynamic_2019\",\"id\":\"levi_dynamic_2019\",\"bibbaseid\":\"levi-kalinchuk-shirokov-somedynamicfeaturesofferroelectricthinfilms-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/1742-6596/1260/9/092004\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Low-frequency phonon dynamics and related thermal properties of axially stressed single-walled carbon nanotubes\",\"volume\":\"31\",\"issn\":\"0953-8984\",\"url\":\"https://dx.doi.org/10.1088/1361-648X/ab285c\",\"doi\":\"10.1088/1361-648X/ab285c\",\"abstract\":\"Synthesis temperatures of composite materials are usually far less than the ones of their use, thus carbon nanotubes (CNTs) embedded into a polymer matrix undergo significant axial stress. We develop a continuous theory, which describes the dynamics of stressed single-walled (SW-) CNTs and predicts their low-frequency phonon spectra. The changes in dispersion laws of SWCNT low-frequency phonon modes due to the axial stress of different signs are discussed. Then, the results obtained are used to analyze low-temperature (T \\\\textless 70 K) heat capacity and thermal conductivity of individual nanotubes. We demonstrate that compressive stress leads to increase in heat capacity CV of an individual SWCNT, while tensile stress causes CV to decrease. In the latter case at T → 0 heat capacity diminishes according to a linear law T instead of a power one T1/2. Nevertheless, according to our results, axial stress hardly affects low-temperature thermal conductance of SWCNTs. Influence of investigated effects on the corresponding macroscopic properties of CNT-based composite materials are also discussed.\",\"language\":\"en\",\"number\":\"42\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics: Condensed Matter\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Chalin\"],\"firstnames\":[\"Dmitrii\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Avramenko\"],\"firstnames\":[\"Marina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Parmeggiani\"],\"firstnames\":[\"Andrea\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergei\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2019\",\"note\":\"Publisher: IOP Publishing\",\"pages\":\"425302\",\"bibtex\":\"@article{chalin_low-frequency_2019,\\n\\ttitle = {Low-frequency phonon dynamics and related thermal properties of axially stressed single-walled carbon nanotubes},\\n\\tvolume = {31},\\n\\tissn = {0953-8984},\\n\\turl = {https://dx.doi.org/10.1088/1361-648X/ab285c},\\n\\tdoi = {10.1088/1361-648X/ab285c},\\n\\tabstract = {Synthesis temperatures of composite materials are usually far less than the ones of their use, thus carbon nanotubes (CNTs) embedded into a polymer matrix undergo significant axial stress. We develop a continuous theory, which describes the dynamics of stressed single-walled (SW-) CNTs and predicts their low-frequency phonon spectra. The changes in dispersion laws of SWCNT low-frequency phonon modes due to the axial stress of different signs are discussed. Then, the results obtained are used to analyze low-temperature (T {\\\\textless} 70 K) heat capacity and thermal conductivity of individual nanotubes. We demonstrate that compressive stress leads to increase in heat capacity CV of an individual SWCNT, while tensile stress causes CV to decrease. In the latter case at T → 0 heat capacity diminishes according to a linear law T instead of a power one T1/2. Nevertheless, according to our results, axial stress hardly affects low-temperature thermal conductance of SWCNTs. Influence of investigated effects on the corresponding macroscopic properties of CNT-based composite materials are also discussed.},\\n\\tlanguage = {en},\\n\\tnumber = {42},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics: Condensed Matter},\\n\\tauthor = {Chalin, Dmitrii and Avramenko, Marina and Parmeggiani, Andrea and Rochal, Sergei},\\n\\tmonth = jul,\\n\\tyear = {2019},\\n\\tnote = {Publisher: IOP Publishing},\\n\\tpages = {425302},\\n}\\n\\n\",\"author_short\":[\"Chalin, D.\",\"Avramenko, M.\",\"Parmeggiani, A.\",\"Rochal, S.\"],\"key\":\"chalin_low-frequency_2019\",\"id\":\"chalin_low-frequency_2019\",\"bibbaseid\":\"chalin-avramenko-parmeggiani-rochal-lowfrequencyphonondynamicsandrelatedthermalpropertiesofaxiallystressedsinglewalledcarbonnanotubes-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/1361-648X/ab285c\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Influence of chemical substitution on broadband dielectric response of barium-lead M-type hexaferrite\",\"volume\":\"21\",\"issn\":\"1367-2630\",\"url\":\"https://dx.doi.org/10.1088/1367-2630/ab2476\",\"doi\":\"10.1088/1367-2630/ab2476\",\"abstract\":\"We report on the electrodynamic properties of the single crystalline lead-substituted M-type barium hexaferrite, Ba0.3Pb0.7Fe12O19, performed in the broad frequency range including radio-frequency, terahertz and sub-terahertz bands, which are particularly important for the development of microelectronic devices. We demonstrate how changing on a molecular level the chemical characteristics (composition, intermolecular interaction, spin-orbital interaction) of lead-substituted M-type hexaferrite influences its radio-frequency and terahertz electrodynamic response. Our results indicate a critical temperature range, 50 K \\\\textless T \\\\textless 70 K, where significant changes of the electrodynamic response occur that are interpreted as freezing of dynamical oscillations of bi-pyramidal Fe(2b) ions. In the range 5–300 K, the heat capacity shows no sign of any phase transition and is solely determined by electron and phonon contributions. An anomalous electrodynamic response is detected at 1–2 THz that features a rich set of absorption resonances which are associated with electronic transitions within the fine-structured Fe2+ ground state and are visualized in the spectra due to magnetostriction and electron–phonon interaction. We show that lead substitution of barium in barium hexaferrite, BaFe12O19, leads to the emergence of a pronounced dielectric and magnetic relaxational dynamics at radio-frequencies and that both dynamics have the same characteristic relaxation times, thus evidencing the bi-relaxor-like nature of Ba0.3Pb0.7Fe12O19. We associate the origin of the relaxations as connected with the motion of magnetic domain walls. In order to unveil crucial influence of chemical substitution on electrodynamic characteristics of the compound, we analyze our results on substituted compound in comparison with the data available for pristine barium (BaFe12O19) and pristine lead (PbFe12O19) hexaferrites. The obtained spectroscopic data on the dielectric properties of Ba0.3Pb0.7Fe12O19 provide insight into fundamental phenomena responsible for the absorption mechanisms of the compound and demonstrates that chemical ionic substitution is an effective tool to tune the dielectric properties of the whole family of hexaferrites.\",\"language\":\"en\",\"number\":\"6\",\"urldate\":\"2023-11-11\",\"journal\":\"New Journal of Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Alyabyeva\"],\"firstnames\":[\"Liudmila\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"Victor\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"Elena\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vinnik\"],\"firstnames\":[\"Denis\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"Anatoliy\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gudkova\"],\"firstnames\":[\"Svetlana\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Góngora\"],\"firstnames\":[\"David\",\"Rivas\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ivek\"],\"firstnames\":[\"Tomislav\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tomić\"],\"firstnames\":[\"Silvia\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Novosel\"],\"firstnames\":[\"Nikolina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Starešinić\"],\"firstnames\":[\"Damir\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dominko\"],\"firstnames\":[\"Damir\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Jagličić\"],\"firstnames\":[\"Zvonko\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"Martin\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zherebtsov\"],\"firstnames\":[\"Dmitry\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"Boris\",\"P.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2019\",\"note\":\"Publisher: IOP Publishing\",\"pages\":\"063016\",\"file\":\"IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\4XWDRV9S\\\\\\\\Alyabyeva и др. - 2019 - Influence of chemical substitution on broadband di.pdf:application/pdf\",\"bibtex\":\"@article{alyabyeva_influence_2019,\\n\\ttitle = {Influence of chemical substitution on broadband dielectric response of barium-lead {M}-type hexaferrite},\\n\\tvolume = {21},\\n\\tissn = {1367-2630},\\n\\turl = {https://dx.doi.org/10.1088/1367-2630/ab2476},\\n\\tdoi = {10.1088/1367-2630/ab2476},\\n\\tabstract = {We report on the electrodynamic properties of the single crystalline lead-substituted M-type barium hexaferrite, Ba0.3Pb0.7Fe12O19, performed in the broad frequency range including radio-frequency, terahertz and sub-terahertz bands, which are particularly important for the development of microelectronic devices. We demonstrate how changing on a molecular level the chemical characteristics (composition, intermolecular interaction, spin-orbital interaction) of lead-substituted M-type hexaferrite influences its radio-frequency and terahertz electrodynamic response. Our results indicate a critical temperature range, 50 K {\\\\textless} T {\\\\textless} 70 K, where significant changes of the electrodynamic response occur that are interpreted as freezing of dynamical oscillations of bi-pyramidal Fe(2b) ions. In the range 5–300 K, the heat capacity shows no sign of any phase transition and is solely determined by electron and phonon contributions. An anomalous electrodynamic response is detected at 1–2 THz that features a rich set of absorption resonances which are associated with electronic transitions within the fine-structured Fe2+ ground state and are visualized in the spectra due to magnetostriction and electron–phonon interaction. We show that lead substitution of barium in barium hexaferrite, BaFe12O19, leads to the emergence of a pronounced dielectric and magnetic relaxational dynamics at radio-frequencies and that both dynamics have the same characteristic relaxation times, thus evidencing the bi-relaxor-like nature of Ba0.3Pb0.7Fe12O19. We associate the origin of the relaxations as connected with the motion of magnetic domain walls. In order to unveil crucial influence of chemical substitution on electrodynamic characteristics of the compound, we analyze our results on substituted compound in comparison with the data available for pristine barium (BaFe12O19) and pristine lead (PbFe12O19) hexaferrites. The obtained spectroscopic data on the dielectric properties of Ba0.3Pb0.7Fe12O19 provide insight into fundamental phenomena responsible for the absorption mechanisms of the compound and demonstrates that chemical ionic substitution is an effective tool to tune the dielectric properties of the whole family of hexaferrites.},\\n\\tlanguage = {en},\\n\\tnumber = {6},\\n\\turldate = {2023-11-11},\\n\\tjournal = {New Journal of Physics},\\n\\tauthor = {Alyabyeva, Liudmila N. and Torgashev, Victor I. and Zhukova, Elena S. and Vinnik, Denis A. and Prokhorov, Anatoliy S. and Gudkova, Svetlana A. and Góngora, David Rivas and Ivek, Tomislav and Tomić, Silvia and Novosel, Nikolina and Starešinić, Damir and Dominko, Damir and Jagličić, Zvonko and Dressel, Martin and Zherebtsov, Dmitry A. and Gorshunov, Boris P.},\\n\\tmonth = jun,\\n\\tyear = {2019},\\n\\tnote = {Publisher: IOP Publishing},\\n\\tpages = {063016},\\n\\tfile = {IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\4XWDRV9S\\\\\\\\Alyabyeva и др. - 2019 - Influence of chemical substitution on broadband di.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Alyabyeva, L. N.\",\"Torgashev, V. I.\",\"Zhukova, E. S.\",\"Vinnik, D. A.\",\"Prokhorov, A. S.\",\"Gudkova, S. A.\",\"Góngora, D. R.\",\"Ivek, T.\",\"Tomić, S.\",\"Novosel, N.\",\"Starešinić, D.\",\"Dominko, D.\",\"Jagličić, Z.\",\"Dressel, M.\",\"Zherebtsov, D. A.\",\"Gorshunov, B. P.\"],\"key\":\"alyabyeva_influence_2019\",\"id\":\"alyabyeva_influence_2019\",\"bibbaseid\":\"alyabyeva-torgashev-zhukova-vinnik-prokhorov-gudkova-gngora-ivek-etal-influenceofchemicalsubstitutiononbroadbanddielectricresponseofbariumleadmtypehexaferrite-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/1367-2630/ab2476\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Group-Theoretical Classification of Aristotypes of Cation and Anion Orders in Perovskites\",\"volume\":\"64\",\"issn\":\"1562-689X\",\"url\":\"https://doi.org/10.1134/S1063774519030258\",\"doi\":\"10.1134/S1063774519030258\",\"abstract\":\"A group-theoretical classification of cation and anion orders of crystals with a perovskite structure is presented. Aristotypes are idealized structures (phases), from which the low-symmetry ordered modifications of perovskites are formed as a result of rotations and deformation of octahedra, as well as the cooperative Jahn–Teller effect and other physical phenomena. Seven aristotype classes have been distinguished, which are characterized by the atomic ordering in each of Wyckoff positions and simultaneous atomic ordering in several positions. The critical and secondary (improper) order parameters, describing the formation of ordered structures, are determined. The classification proposed makes it possible to systematize a variety of known phases, establish genetic structural links between low-symmetry ordered structures, and design new materials.\",\"language\":\"en\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Crystallography Reports\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"M.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2019\",\"pages\":\"386–391\",\"bibtex\":\"@article{talanov_group-theoretical_2019,\\n\\ttitle = {Group-{Theoretical} {Classification} of {Aristotypes} of {Cation} and {Anion} {Orders} in {Perovskites}},\\n\\tvolume = {64},\\n\\tissn = {1562-689X},\\n\\turl = {https://doi.org/10.1134/S1063774519030258},\\n\\tdoi = {10.1134/S1063774519030258},\\n\\tabstract = {A group-theoretical classification of cation and anion orders of crystals with a perovskite structure is presented. Aristotypes are idealized structures (phases), from which the low-symmetry ordered modifications of perovskites are formed as a result of rotations and deformation of octahedra, as well as the cooperative Jahn–Teller effect and other physical phenomena. Seven aristotype classes have been distinguished, which are characterized by the atomic ordering in each of Wyckoff positions and simultaneous atomic ordering in several positions. The critical and secondary (improper) order parameters, describing the formation of ordered structures, are determined. The classification proposed makes it possible to systematize a variety of known phases, establish genetic structural links between low-symmetry ordered structures, and design new materials.},\\n\\tlanguage = {en},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Crystallography Reports},\\n\\tauthor = {Talanov, M. V. and Talanov, V. M. and Shirokov, V. B.},\\n\\tmonth = may,\\n\\tyear = {2019},\\n\\tpages = {386--391},\\n}\\n\\n\",\"author_short\":[\"Talanov, M. V.\",\"Talanov, V. M.\",\"Shirokov, V. B.\"],\"key\":\"talanov_group-theoretical_2019\",\"id\":\"talanov_group-theoretical_2019\",\"bibbaseid\":\"talanov-talanov-shirokov-grouptheoreticalclassificationofaristotypesofcationandanionordersinperovskites-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1063774519030258\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Ferroelectric multiple-valued logic units\",\"volume\":\"543\",\"issn\":\"0015-0193\",\"url\":\"https://doi.org/10.1080/00150193.2019.1592436\",\"doi\":\"10.1080/00150193.2019.1592436\",\"abstract\":\"Employing many-valued logic (MVL) data processing allows to dramatically increase the performance of computing circuits. Here we propose to employ ferroelectrics for the material implementation of MVL units basing on their ability to pin the polarization as a sequence of multi-stable states. Two conceptual ideas are considered. As the first system, we suggest using the strained ferroelectric films that can host the polarization states, allowing the effective field-induced multilevel switching between them. As the second one, we propose to employ the ferroelectric nano-samples that confine the topologically protected polarization textures, which may be used as MVL structural elements. We demonstrate that these systems are suitable for engineering of the 3-, 4- and even 5-level logic units and consider the circuit design for such elements.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Lukyanchuk\"],\"firstnames\":[\"Igor\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zaitseva\"],\"firstnames\":[\"Elena\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Levashenko\"],\"firstnames\":[\"Vitaly\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kvassay\"],\"firstnames\":[\"Miroslav\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kondovych\"],\"firstnames\":[\"Svitlana\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tikhonov\"],\"firstnames\":[\"Yuri\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Baudry\"],\"firstnames\":[\"Laurent\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"Anna\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2019\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2019.1592436\",\"keywords\":\"Ferroelectrics, switching, domain, hysteresis, multiple-valued logic, skyrmion, topological structures, vortex\",\"pages\":\"213–221\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\VXZHNBRF\\\\Łukyanchuk и др. - 2019 - Ferroelectric multiple-valued logic units.pdf:application/pdf\",\"bibtex\":\"@article{lukyanchuk_ferroelectric_2019,\\n\\ttitle = {Ferroelectric multiple-valued logic units},\\n\\tvolume = {543},\\n\\tissn = {0015-0193},\\n\\turl = {https://doi.org/10.1080/00150193.2019.1592436},\\n\\tdoi = {10.1080/00150193.2019.1592436},\\n\\tabstract = {Employing many-valued logic (MVL) data processing allows to dramatically increase the performance of computing circuits. Here we propose to employ ferroelectrics for the material implementation of MVL units basing on their ability to pin the polarization as a sequence of multi-stable states. Two conceptual ideas are considered. As the first system, we suggest using the strained ferroelectric films that can host the polarization states, allowing the effective field-induced multilevel switching between them. As the second one, we propose to employ the ferroelectric nano-samples that confine the topologically protected polarization textures, which may be used as MVL structural elements. We demonstrate that these systems are suitable for engineering of the 3-, 4- and even 5-level logic units and consider the circuit design for such elements.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Lukyanchuk, Igor and Zaitseva, Elena and Levashenko, Vitaly and Kvassay, Miroslav and Kondovych, Svitlana and Tikhonov, Yuri and Baudry, Laurent and Razumnaya, Anna},\\n\\tmonth = apr,\\n\\tyear = {2019},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/00150193.2019.1592436},\\n\\tkeywords = {Ferroelectrics, switching, domain, hysteresis, multiple-valued logic, skyrmion, topological structures, vortex},\\n\\tpages = {213--221},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\VXZHNBRF\\\\\\\\Lukyanchuk и др. - 2019 - Ferroelectric multiple-valued logic units.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Lukyanchuk, I.\",\"Zaitseva, E.\",\"Levashenko, V.\",\"Kvassay, M.\",\"Kondovych, S.\",\"Tikhonov, Y.\",\"Baudry, L.\",\"Razumnaya, A.\"],\"key\":\"lukyanchuk_ferroelectric_2019\",\"id\":\"lukyanchuk_ferroelectric_2019\",\"bibbaseid\":\"lukyanchuk-zaitseva-levashenko-kvassay-kondovych-tikhonov-baudry-razumnaya-ferroelectricmultiplevaluedlogicunits-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/00150193.2019.1592436\"},\"keyword\":[\"Ferroelectrics\",\"switching\",\"domain\",\"hysteresis\",\"multiple-valued logic\",\"skyrmion\",\"topological structures\",\"vortex\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Properties of the low-frequency phonon spectra of ferroelectric barium titanate-based heterostructures\",\"volume\":\"543\",\"issn\":\"0015-0193\",\"url\":\"https://doi.org/10.1080/00150193.2019.1592446\",\"doi\":\"10.1080/00150193.2019.1592446\",\"abstract\":\"Polarized Raman spectra of the epitaxial Ba0.5Sr0.5TiO3 film, bi-color BaTiO3/Ba0.5Sr0.5TiO3 superlattice and tri-color BaTiO3/Ba0.5Sr0.5TiO3/SrTiO3 superlattice were studied in a broad temperature range of 80–700 K. Based on the temperature dependence of the polar modes we determined the phase transitions temperatures in the studied heterostructures. In the sub-THz frequency range of the Y(XZ)Y¯spectra, we revealed the coexistence of the Debye-type central peak and soft mode in bi-color BaTiO3/Ba0.5Sr0.5TiO3 superlattice.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Gor’kovaya\"],\"firstnames\":[\"E.\",\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tikhonov\"],\"firstnames\":[\"Yu.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lukyanchuk\"],\"firstnames\":[\"I.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzane\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ortega\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kumar\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"R.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2019\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2019.1592446\",\"keywords\":\"Raman spectroscopy, soft mode, central peak, superlattice, thin film\",\"pages\":\"36–47\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\¶CXC4STE\\\\\\\\Gor’kovaya и др. - 2019 - Properties of the low-frequency phonon spectra of .pdf:application/pdf\",\"bibtex\":\"@article{gorkovaya_properties_2019,\\n\\ttitle = {Properties of the low-frequency phonon spectra of ferroelectric barium titanate-based heterostructures},\\n\\tvolume = {543},\\n\\tissn = {0015-0193},\\n\\turl = {https://doi.org/10.1080/00150193.2019.1592446},\\n\\tdoi = {10.1080/00150193.2019.1592446},\\n\\tabstract = {Polarized Raman spectra of the epitaxial Ba0.5Sr0.5TiO3 film, bi-color BaTiO3/Ba0.5Sr0.5TiO3 superlattice and tri-color BaTiO3/Ba0.5Sr0.5TiO3/SrTiO3 superlattice were studied in a broad temperature range of 80–700 K. Based on the temperature dependence of the polar modes we determined the phase transitions temperatures in the studied heterostructures. In the sub-THz frequency range of the Y(XZ)Y¯spectra, we revealed the coexistence of the Debye-type central peak and soft mode in bi-color BaTiO3/Ba0.5Sr0.5TiO3 superlattice.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Gor’kovaya, E. D. and Tikhonov, Yu. A. and Torgashev, V. I. and Mikheykin, A. S. and Lukyanchuk, I. A. and Mezzane, D. and Ortega, N. and Kumar, A. and Katiyar, R. S. and Razumnaya, A. G.},\\n\\tmonth = apr,\\n\\tyear = {2019},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/00150193.2019.1592446},\\n\\tkeywords = {Raman spectroscopy, soft mode, central peak, superlattice, thin film},\\n\\tpages = {36--47},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\PCXC4STE\\\\\\\\Gor’kovaya и др. - 2019 - Properties of the low-frequency phonon spectra of .pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Gor’kovaya, E. D.\",\"Tikhonov, Y. A.\",\"Torgashev, V. I.\",\"Mikheykin, A. S.\",\"Lukyanchuk, I. A.\",\"Mezzane, D.\",\"Ortega, N.\",\"Kumar, A.\",\"Katiyar, R. S.\",\"Razumnaya, A. G.\"],\"key\":\"gorkovaya_properties_2019\",\"id\":\"gorkovaya_properties_2019\",\"bibbaseid\":\"gorkovaya-tikhonov-torgashev-mikheykin-lukyanchuk-mezzane-ortega-kumar-etal-propertiesofthelowfrequencyphononspectraofferroelectricbariumtitanatebasedheterostructures-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/00150193.2019.1592446\"},\"keyword\":[\"Raman spectroscopy\",\"soft mode\",\"central peak\",\"superlattice\",\"thin film\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"pH-induced morphological changes of proteinaceous viral shells\",\"volume\":\"9\",\"copyright\":\"2019 The Author(s)\",\"issn\":\"2045-2322\",\"url\":\"https://www.nature.com/articles/s41598-019-41799-6\",\"doi\":\"10.1038/s41598-019-41799-6\",\"abstract\":\"Changes in environmental pH can induce morphological changes in empty proteinaceous shells of bacteriophages in vitro that are very similar to changes occurring in viral capsids in vivo after encapsidation of DNA. These changes in capsid shape and size cannot be explained with a simple elastic model alone. We propose a new theoretical framework that combines the elasticity of thin icosahedral shells with the pH dependence of capsid charge distribution. Minimization of the sum of elastic and electrostatic free energies leads to equilibrium shapes of viral shells that depend on a single elastic parameter and the detailed configuration of the imbedded protein charges. Based on the in vitro shell reconstructions of bacteriophage HK97 we elucidate the details of how the reversible transition between Prohead II and Expansion Intermediate II states of the HK97 procapsid is induced by pH changes, as well as some other features of the bacteriophage maturation.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Scientific Reports\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Roshal\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Konevtsova\"],\"firstnames\":[\"O.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lošdorfer\",\"Božič\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Podgornik\"],\"firstnames\":[\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2019\",\"note\":\"Number: 1 Publisher: Nature Publishing Group\",\"keywords\":\"Biological physics, Molecular self-assembly\",\"pages\":\"5341\",\"file\":\"Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\MGU2DMMM\\\\\\\\Roshal и др. - 2019 - pH-induced morphological changes of proteinaceous .pdf:application/pdf\",\"bibtex\":\"@article{roshal_ph-induced_2019,\\n\\ttitle = {{pH}-induced morphological changes of proteinaceous viral shells},\\n\\tvolume = {9},\\n\\tcopyright = {2019 The Author(s)},\\n\\tissn = {2045-2322},\\n\\turl = {https://www.nature.com/articles/s41598-019-41799-6},\\n\\tdoi = {10.1038/s41598-019-41799-6},\\n\\tabstract = {Changes in environmental pH can induce morphological changes in empty proteinaceous shells of bacteriophages in vitro that are very similar to changes occurring in viral capsids in vivo after encapsidation of DNA. These changes in capsid shape and size cannot be explained with a simple elastic model alone. We propose a new theoretical framework that combines the elasticity of thin icosahedral shells with the pH dependence of capsid charge distribution. Minimization of the sum of elastic and electrostatic free energies leads to equilibrium shapes of viral shells that depend on a single elastic parameter and the detailed configuration of the imbedded protein charges. Based on the in vitro shell reconstructions of bacteriophage HK97 we elucidate the details of how the reversible transition between Prohead II and Expansion Intermediate II states of the HK97 procapsid is induced by pH changes, as well as some other features of the bacteriophage maturation.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Scientific Reports},\\n\\tauthor = {Roshal, D. and Konevtsova, O. and Lošdorfer Božič, A. and Podgornik, R. and Rochal, S.},\\n\\tmonth = mar,\\n\\tyear = {2019},\\n\\tnote = {Number: 1\\nPublisher: Nature Publishing Group},\\n\\tkeywords = {Biological physics, Molecular self-assembly},\\n\\tpages = {5341},\\n\\tfile = {Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\MGU2DMMM\\\\\\\\Roshal и др. - 2019 - pH-induced morphological changes of proteinaceous .pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Roshal, D.\",\"Konevtsova, O.\",\"Lošdorfer Božič, A.\",\"Podgornik, R.\",\"Rochal, S.\"],\"key\":\"roshal_ph-induced_2019\",\"id\":\"roshal_ph-induced_2019\",\"bibbaseid\":\"roshal-konevtsova-lodorferboi-podgornik-rochal-phinducedmorphologicalchangesofproteinaceousviralshells-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.nature.com/articles/s41598-019-41799-6\"},\"keyword\":[\"Biological physics\",\"Molecular self-assembly\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Absorbing Two-Dimensionally Periodic Structures on New Plasmonic Materials\",\"volume\":\"61\",\"issn\":\"1573-9120\",\"url\":\"https://doi.org/10.1007/s11141-019-09938-1\",\"doi\":\"10.1007/s11141-019-09938-1\",\"abstract\":\"We study theoretically two-dimensionally periodic gratings of plasmonic strips on substrates which contain dielectric and plasmonic layers. The developed electrodynamic model is based on solving the vector integro-differential equation of diffraction by three-dimensional dielectric bodies by the Galerkin method. It is shown that at the resonant frequencies of the surface plasmon polariton, these structures absorb almost 100% of the energy of the incident radiation in a wide wavelength range. The use of nonmetal plasmonic materials makes it possible to create a wideband absorber of infrared waves.\",\"language\":\"en\",\"number\":\"11\",\"urldate\":\"2023-11-11\",\"journal\":\"Radiophysics and Quantum Electronics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Lerer\"],\"firstnames\":[\"A.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golovacheva\"],\"firstnames\":[\"E.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ivanova\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Makhno\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2019\",\"pages\":\"801–805\",\"bibtex\":\"@article{lerer_absorbing_2019,\\n\\ttitle = {Absorbing {Two}-{Dimensionally} {Periodic} {Structures} on {New} {Plasmonic} {Materials}},\\n\\tvolume = {61},\\n\\tissn = {1573-9120},\\n\\turl = {https://doi.org/10.1007/s11141-019-09938-1},\\n\\tdoi = {10.1007/s11141-019-09938-1},\\n\\tabstract = {We study theoretically two-dimensionally periodic gratings of plasmonic strips on substrates which contain dielectric and plasmonic layers. The developed electrodynamic model is based on solving the vector integro-differential equation of diffraction by three-dimensional dielectric bodies by the Galerkin method. It is shown that at the resonant frequencies of the surface plasmon polariton, these structures absorb almost 100\\\\% of the energy of the incident radiation in a wide wavelength range. The use of nonmetal plasmonic materials makes it possible to create a wideband absorber of infrared waves.},\\n\\tlanguage = {en},\\n\\tnumber = {11},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Radiophysics and Quantum Electronics},\\n\\tauthor = {Lerer, A. M. and Golovacheva, E. V. and Ivanova, I. N. and Makhno, V. V. and Timoshenko, P. E.},\\n\\tmonth = apr,\\n\\tyear = {2019},\\n\\tpages = {801--805},\\n}\\n\\n\",\"author_short\":[\"Lerer, A. M.\",\"Golovacheva, E. V.\",\"Ivanova, I. N.\",\"Makhno, V. V.\",\"Timoshenko, P. E.\"],\"key\":\"lerer_absorbing_2019\",\"id\":\"lerer_absorbing_2019\",\"bibbaseid\":\"lerer-golovacheva-ivanova-makhno-timoshenko-absorbingtwodimensionallyperiodicstructuresonnewplasmonicmaterials-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1007/s11141-019-09938-1\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Electrocatalytic Properties of Rh/C and Pt-Rh/C Catalysts Fabricated by the Method of Electrochemical Dispersion\",\"volume\":\"55\",\"issn\":\"1608-3342\",\"url\":\"https://doi.org/10.1134/S1023193519030066\",\"doi\":\"10.1134/S1023193519030066\",\"abstract\":\"The Pt/C, Rh/C, and Pt-Rh/C catalytic systems with uniform distribution of metal phase over the surface of carbon support and an average size of Pt and Rh nanoparticles of 7.3 and 6.5 nm, respectively, are fabricated by the method of electrochemical dispersion of metals in the aqueous electrolytes containing Na+. It is shown that the double-layer potential E = 300 mV (RHE) is the optimal potential of CO adsorption for determining the electrochemically active surface area of Pt/C, Rh/C, and Pt-Rh/C catalysts by the method of oxidative desorption of CO. The introduction of Rh into the Pt/C catalyst enables us to increase the specific activity and reduce the potential of the onset of methanol oxidation.\",\"language\":\"en\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Russian Journal of Electrochemistry\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Faddeev\"],\"firstnames\":[\"N.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"A.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leont′ev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"N.\",\"V.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2019\",\"keywords\":\"electrochemical dispersion, fuel cell, electrocatalysis, platinum, rhodium\",\"pages\":\"346–350\",\"bibtex\":\"@article{faddeev_electrocatalytic_2019,\\n\\ttitle = {Electrocatalytic {Properties} of {Rh}/{C} and {Pt}-{Rh}/{C} {Catalysts} {Fabricated} by the {Method} of {Electrochemical} {Dispersion}},\\n\\tvolume = {55},\\n\\tissn = {1608-3342},\\n\\turl = {https://doi.org/10.1134/S1023193519030066},\\n\\tdoi = {10.1134/S1023193519030066},\\n\\tabstract = {The Pt/C, Rh/C, and Pt-Rh/C catalytic systems with uniform distribution of metal phase over the surface of carbon support and an average size of Pt and Rh nanoparticles of 7.3 and 6.5 nm, respectively, are fabricated by the method of electrochemical dispersion of metals in the aqueous electrolytes containing Na+. It is shown that the double-layer potential E = 300 mV (RHE) is the optimal potential of CO adsorption for determining the electrochemically active surface area of Pt/C, Rh/C, and Pt-Rh/C catalysts by the method of oxidative desorption of CO. The introduction of Rh into the Pt/C catalyst enables us to increase the specific activity and reduce the potential of the onset of methanol oxidation.},\\n\\tlanguage = {en},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Russian Journal of Electrochemistry},\\n\\tauthor = {Faddeev, N. A. and Kuriganova, A. B. and Leont′ev, I. N. and Smirnova, N. V.},\\n\\tmonth = apr,\\n\\tyear = {2019},\\n\\tkeywords = {electrochemical dispersion, fuel cell, electrocatalysis, platinum, rhodium},\\n\\tpages = {346--350},\\n}\\n\\n\",\"author_short\":[\"Faddeev, N. A.\",\"Kuriganova, A. B.\",\"Leont′ev, I. N.\",\"Smirnova, N. V.\"],\"key\":\"faddeev_electrocatalytic_2019\",\"id\":\"faddeev_electrocatalytic_2019\",\"bibbaseid\":\"faddeev-kuriganova-leontev-smirnova-electrocatalyticpropertiesofrhcandptrhccatalystsfabricatedbythemethodofelectrochemicaldispersion-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1023193519030066\"},\"keyword\":[\"electrochemical dispersion\",\"fuel cell\",\"electrocatalysis\",\"platinum\",\"rhodium\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"High-pressure container for the research of phase transitions of ferroelectrics under variable hydrostatic pressure, electric field strength and temperature\",\"volume\":\"8\",\"issn\":\"22254293\",\"url\":\"http://red.jfop.ru/jfop-1901-022029\",\"doi\":\"10.25210/jfop-1901-022029\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Физические основы приборостроения\",\"author\":[{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Southern Federal University\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontiev\"],\"firstnames\":[\"I.N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Panich\"],\"firstnames\":[\"A.E.\"],\"suffixes\":[]},{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Southern Federal University\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smotrakov\"],\"firstnames\":[\"V.G.\"],\"suffixes\":[]},{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Southern Federal University\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fesenko\"],\"firstnames\":[\"O.E.\"],\"suffixes\":[]},{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Southern Federal University\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2019\",\"pages\":\"22–29\",\"bibtex\":\"@article{southern_federal_university_high-pressure_2019,\\n\\ttitle = {High-pressure container for the research of phase transitions of ferroelectrics under variable hydrostatic pressure, electric field strength and temperature},\\n\\tvolume = {8},\\n\\tissn = {22254293},\\n\\turl = {http://red.jfop.ru/jfop-1901-022029},\\n\\tdoi = {10.25210/jfop-1901-022029},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физические основы приборостроения},\\n\\tauthor = {{Southern Federal University} and Leontiev, I.N. and Panich, A.E. and {Southern Federal University} and Smotrakov, V.G. and {Southern Federal University} and Fesenko, O.E. and {Southern Federal University}},\\n\\tmonth = mar,\\n\\tyear = {2019},\\n\\tpages = {22--29},\\n}\\n\\n\",\"author_short\":[\"Southern Federal University\",\"Leontiev, I.\",\"Panich, A.\",\"Southern Federal University\",\"Smotrakov, V.\",\"Southern Federal University\",\"Fesenko, O.\",\"Southern Federal University\"],\"key\":\"southern_federal_university_high-pressure_2019\",\"id\":\"southern_federal_university_high-pressure_2019\",\"bibbaseid\":\"southernfederaluniversity-leontiev-panich-southernfederaluniversity-smotrakov-southernfederaluniversity-fesenko-southernfederaluniversity-highpressurecontainerfortheresearchofphasetransitionsofferroelectricsundervariablehydrostaticpressureelectricfieldstrengthandtemperature-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://red.jfop.ru/jfop-1901-022029\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"series\":\"Materials Science for Green Energy Ifran City\",\"title\":\"Enhancement of dielectric properties of lead-free BCZT ferroelectric ceramics by grain size engineering\",\"volume\":\"127\",\"issn\":\"0749-6036\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0749603617323121\",\"doi\":\"10.1016/j.spmi.2018.03.004\",\"abstract\":\"Lead-free Ba0.85Ca0.15Ti0.9Zr0.1O3 (BCZT) ceramics had attracted much attention for the fabrication of microelectronic devices by virtue of their excellent dielectric, ferroelectric and piezoelectric properties. To understand the effects of both mean grain size and grain size distribution on the dielectric properties of lead-free Ba0.85Ca0.15Ti0.9Zr0.1O3 (BCZT) ferroelectric relaxors, an original method was proposed. It is based on the surfactant-assisted solvothermal processing coupled with low-temperature conventional sintering at 1250 °C. In this way, three highly dense BCZT with different mean grain size and dissimilar grain size distribution were designed. A significant increase of dielectric properties was obtained by a control of grain size and densification process. The dielectric constants measured were ranged from 5370 to 9646 and the dielectric loss was enhanced by 70%. Surprisingly, it was evidenced that there is unequivocal link between mean grain size with dielectric properties. Indeed, it was found that the presence of high density of refined grains leads to an improvement of dielectric properties due to an enhancement of densification. This work may provide a new strategy to design ferroelectric materials with enhanced properties.\",\"urldate\":\"2023-11-11\",\"journal\":\"Superlattices and Microstructures\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Hanani\"],\"firstnames\":[\"Z.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzane\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Amjoud\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fourcade\"],\"firstnames\":[\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Luk'yanchuk\"],\"firstnames\":[\"I.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gouné\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2019\",\"keywords\":\"BCZT, Dielectric, Ferroelectric, Lead-free, Microstructure, Relaxor\",\"pages\":\"109–117\",\"file\":\"Принятая версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\ZTGFIZUV\\\\a̋nani и др. - 2019 - Enhancement of dielectric properties of lead-free .pdf:application/pdf;ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\ÆC2RSBJ\\\\§0749603617323121.html:text/html\",\"bibtex\":\"@article{hanani_enhancement_2019,\\n\\tseries = {Materials {Science} for {Green} {Energy} {Ifran} {City}},\\n\\ttitle = {Enhancement of dielectric properties of lead-free {BCZT} ferroelectric ceramics by grain size engineering},\\n\\tvolume = {127},\\n\\tissn = {0749-6036},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0749603617323121},\\n\\tdoi = {10.1016/j.spmi.2018.03.004},\\n\\tabstract = {Lead-free Ba0.85Ca0.15Ti0.9Zr0.1O3 (BCZT) ceramics had attracted much attention for the fabrication of microelectronic devices by virtue of their excellent dielectric, ferroelectric and piezoelectric properties. To understand the effects of both mean grain size and grain size distribution on the dielectric properties of lead-free Ba0.85Ca0.15Ti0.9Zr0.1O3 (BCZT) ferroelectric relaxors, an original method was proposed. It is based on the surfactant-assisted solvothermal processing coupled with low-temperature conventional sintering at 1250 °C. In this way, three highly dense BCZT with different mean grain size and dissimilar grain size distribution were designed. A significant increase of dielectric properties was obtained by a control of grain size and densification process. The dielectric constants measured were ranged from 5370 to 9646 and the dielectric loss was enhanced by 70\\\\%. Surprisingly, it was evidenced that there is unequivocal link between mean grain size with dielectric properties. Indeed, it was found that the presence of high density of refined grains leads to an improvement of dielectric properties due to an enhancement of densification. This work may provide a new strategy to design ferroelectric materials with enhanced properties.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Superlattices and Microstructures},\\n\\tauthor = {Hanani, Z. and Mezzane, D. and Amjoud, M. and Fourcade, S. and Razumnaya, A. G. and Luk'yanchuk, I. A. and Gouné, M.},\\n\\tmonth = mar,\\n\\tyear = {2019},\\n\\tkeywords = {BCZT, Dielectric, Ferroelectric, Lead-free, Microstructure, Relaxor},\\n\\tpages = {109--117},\\n\\tfile = {Принятая версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\ZTGFIZUV\\\\\\\\Hanani и др. - 2019 - Enhancement of dielectric properties of lead-free .pdf:application/pdf;ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\AEC2RSBJ\\\\\\\\S0749603617323121.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Hanani, Z.\",\"Mezzane, D.\",\"Amjoud, M.\",\"Fourcade, S.\",\"Razumnaya, A. G.\",\"Luk'yanchuk, I. A.\",\"Gouné, M.\"],\"key\":\"hanani_enhancement_2019\",\"id\":\"hanani_enhancement_2019\",\"bibbaseid\":\"hanani-mezzane-amjoud-fourcade-razumnaya-lukyanchuk-goun-enhancementofdielectricpropertiesofleadfreebcztferroelectricceramicsbygrainsizeengineering-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0749603617323121\"},\"keyword\":[\"BCZT\",\"Dielectric\",\"Ferroelectric\",\"Lead-free\",\"Microstructure\",\"Relaxor\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Harnessing ferroelectric domains for negative capacitance\",\"volume\":\"2\",\"copyright\":\"2019 The Author(s)\",\"issn\":\"2399-3650\",\"url\":\"https://www.nature.com/articles/s42005-019-0121-0\",\"doi\":\"10.1038/s42005-019-0121-0\",\"abstract\":\"A pressing quest for overcoming Boltzmann tyranny in low-power nanoscale electronics ignited an extensive search for the devices possessing the negative circuit constants. The emergent concept of the ferroelectric-based negative capacitance triggered then the explosive activity in the field. However, most of the research addressed transient negative capacitance, leaving the basic question of the existence of the steady-state negative capacitance unresolved. Here, we show that the ferroelectric nanodot capacitor hosts a stable two-domain state realizing the static reversible negative capacitance device thus opening routes for the extensive use of the negative capacitance in domain wall-based nanoelectronics.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Communications Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Luk’yanchuk\"],\"firstnames\":[\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tikhonov\"],\"firstnames\":[\"Y.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sené\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vinokur\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2019\",\"note\":\"Number: 1 Publisher: Nature Publishing Group\",\"keywords\":\"Ferroelectrics and multiferroics, interfaces and thin films, Surfaces\",\"pages\":\"1–6\",\"file\":\"Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\T4E6X2XN\\\\Łuk’yanchuk и др. - 2019 - Harnessing ferroelectric domains for negative capa.pdf:application/pdf\",\"bibtex\":\"@article{lukyanchuk_harnessing_2019,\\n\\ttitle = {Harnessing ferroelectric domains for negative capacitance},\\n\\tvolume = {2},\\n\\tcopyright = {2019 The Author(s)},\\n\\tissn = {2399-3650},\\n\\turl = {https://www.nature.com/articles/s42005-019-0121-0},\\n\\tdoi = {10.1038/s42005-019-0121-0},\\n\\tabstract = {A pressing quest for overcoming Boltzmann tyranny in low-power nanoscale electronics ignited an extensive search for the devices possessing the negative circuit constants. The emergent concept of the ferroelectric-based negative capacitance triggered then the explosive activity in the field. However, most of the research addressed transient negative capacitance, leaving the basic question of the existence of the steady-state negative capacitance unresolved. Here, we show that the ferroelectric nanodot capacitor hosts a stable two-domain state realizing the static reversible negative capacitance device thus opening routes for the extensive use of the negative capacitance in domain wall-based nanoelectronics.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Communications Physics},\\n\\tauthor = {Luk’yanchuk, I. and Tikhonov, Y. and Sené, A. and Razumnaya, A. and Vinokur, V. M.},\\n\\tmonth = feb,\\n\\tyear = {2019},\\n\\tnote = {Number: 1\\nPublisher: Nature Publishing Group},\\n\\tkeywords = {Ferroelectrics and multiferroics, interfaces and thin films, Surfaces},\\n\\tpages = {1--6},\\n\\tfile = {Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\T4E6X2XN\\\\\\\\Luk’yanchuk и др. - 2019 - Harnessing ferroelectric domains for negative capa.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Luk’yanchuk, I.\",\"Tikhonov, Y.\",\"Sené, A.\",\"Razumnaya, A.\",\"Vinokur, V. M.\"],\"key\":\"lukyanchuk_harnessing_2019\",\"id\":\"lukyanchuk_harnessing_2019\",\"bibbaseid\":\"lukyanchuk-tikhonov-sen-razumnaya-vinokur-harnessingferroelectricdomainsfornegativecapacitance-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.nature.com/articles/s42005-019-0121-0\"},\"keyword\":[\"Ferroelectrics and multiferroics\",\"interfaces and thin films\",\"Surfaces\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Ferromagnetism and Giant Paramagnetism of Copper Nanoparticles in Carbon Matrix\",\"volume\":\"55\",\"issn\":\"1941-0069\",\"url\":\"https://ieeexplore.ieee.org/document/8476555\",\"doi\":\"10.1109/TMAG.2018.2862413\",\"abstract\":\"Systematic X-ray diffraction, transmission electron microscopy (TEM), Raman and magnetic measurements were performed to study the structural and magnetic properties of copper nanoparticles (NPs) in carbon matrix. The weight concentration of Cu in carbon matrix is 8 wt%. The carbon-coated core-shell structures with bimodal size distribution with 4 and 300 nm average sizes of NPs are confirmed by scanning electron microscopy and TEM. Our results on magnetization carried out by vibrational magnetometer for copper NPs provide a strong evidence for coexistence of ferromagnetism and giant paramagnetism in wide range of temperature and magnetic field. The magnetic susceptibility at T = 10 K shows high value of giant paramagnetism with χ = 5×10-5 emu/gCuOe while ferromagnetic behavior with hysteresis is preserved up to the room temperature.\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"IEEE Transactions on Magnetics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kocharian\"],\"firstnames\":[\"Armen\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gyulasaryan\"],\"firstnames\":[\"Harutyun\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Estiphanos\"],\"firstnames\":[\"Medhanie\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Avramenko\"],\"firstnames\":[\"Marina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nelms\"],\"firstnames\":[\"Katherine\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bernal\"],\"firstnames\":[\"Oscar\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sharoyan\"],\"firstnames\":[\"Eduard\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Manukyan\"],\"firstnames\":[\"Aram\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2019\",\"note\":\"Conference Name: IEEE Transactions on Magnetics\",\"pages\":\"1–4\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\DCWF2WPV\\\\\\\\Kocharian и др. - 2019 - Ferromagnetism and Giant Paramagnetism of Copper N.pdf:application/pdf;IEEE Xplore Abstract Record:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\CA3E5JSV\\\\\\\\8476555.html:text/html\",\"bibtex\":\"@article{kocharian_ferromagnetism_2019,\\n\\ttitle = {Ferromagnetism and {Giant} {Paramagnetism} of {Copper} {Nanoparticles} in {Carbon} {Matrix}},\\n\\tvolume = {55},\\n\\tissn = {1941-0069},\\n\\turl = {https://ieeexplore.ieee.org/document/8476555},\\n\\tdoi = {10.1109/TMAG.2018.2862413},\\n\\tabstract = {Systematic X-ray diffraction, transmission electron microscopy (TEM), Raman and magnetic measurements were performed to study the structural and magnetic properties of copper nanoparticles (NPs) in carbon matrix. The weight concentration of Cu in carbon matrix is 8 wt\\\\%. The carbon-coated core-shell structures with bimodal size distribution with 4 and 300 nm average sizes of NPs are confirmed by scanning electron microscopy and TEM. Our results on magnetization carried out by vibrational magnetometer for copper NPs provide a strong evidence for coexistence of ferromagnetism and giant paramagnetism in wide range of temperature and magnetic field. The magnetic susceptibility at T = 10 K shows high value of giant paramagnetism with χ = 5×10-5 emu/gCuOe while ferromagnetic behavior with hysteresis is preserved up to the room temperature.},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {IEEE Transactions on Magnetics},\\n\\tauthor = {Kocharian, Armen and Gyulasaryan, Harutyun and Estiphanos, Medhanie and Avramenko, Marina and Nelms, Katherine and Bernal, Oscar and Sharoyan, Eduard and Manukyan, Aram},\\n\\tmonth = feb,\\n\\tyear = {2019},\\n\\tnote = {Conference Name: IEEE Transactions on Magnetics},\\n\\tpages = {1--4},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\DCWF2WPV\\\\\\\\Kocharian и др. - 2019 - Ferromagnetism and Giant Paramagnetism of Copper N.pdf:application/pdf;IEEE Xplore Abstract Record:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\CA3E5JSV\\\\\\\\8476555.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Kocharian, A.\",\"Gyulasaryan, H.\",\"Estiphanos, M.\",\"Avramenko, M.\",\"Nelms, K.\",\"Bernal, O.\",\"Sharoyan, E.\",\"Manukyan, A.\"],\"key\":\"kocharian_ferromagnetism_2019\",\"id\":\"kocharian_ferromagnetism_2019\",\"bibbaseid\":\"kocharian-gyulasaryan-estiphanos-avramenko-nelms-bernal-sharoyan-manukyan-ferromagnetismandgiantparamagnetismofcoppernanoparticlesincarbonmatrix-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://ieeexplore.ieee.org/document/8476555\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Incommensurate instability and diffuse scattering at Brillouin zone boundary in Zr-rich lead zirconate titanate\",\"volume\":\"538\",\"issn\":\"0015-0193\",\"url\":\"https://doi.org/10.1080/00150193.2019.1569987\",\"doi\":\"10.1080/00150193.2019.1569987\",\"abstract\":\"Detailed study of the X-ray diffuse scattering in the paraelectric phase of the PbZr0.985Ti0.015O3 was carried out. We concentrated on the analysis of the scattering peculiarities in the vicinities of M- and R- points of the Brillouin zone. We have observed a critical increase of the diffuse scattering at the position Q ≈ (0.47 + h 0.53 + k l) slightly aside of M point on cooling to the intermediate phase. We attribute observed critical scattering to a mixed mode containing both oxygen octahedral tilts and antiparallel cationic displacements. Tentative conclusion is made describing earlier reported complicated set of the satellite peaks around M-point as the result of the soft-mode driven incommensurate phase transition.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Andronikova\"],\"firstnames\":[\"D.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bronwald\"],\"firstnames\":[\"Iu.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontiev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontiev\"],\"firstnames\":[\"N.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chernyshov\"],\"firstnames\":[\"D.\",\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Filimonov\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vakhrushev\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2019\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2019.1569987\",\"keywords\":\"phase transitions, diffuse scattering, Ferroelectricity\",\"pages\":\"65–73\",\"bibtex\":\"@article{andronikova_incommensurate_2019,\\n\\ttitle = {Incommensurate instability and diffuse scattering at {Brillouin} zone boundary in {Zr}-rich lead zirconate titanate},\\n\\tvolume = {538},\\n\\tissn = {0015-0193},\\n\\turl = {https://doi.org/10.1080/00150193.2019.1569987},\\n\\tdoi = {10.1080/00150193.2019.1569987},\\n\\tabstract = {Detailed study of the X-ray diffuse scattering in the paraelectric phase of the PbZr0.985Ti0.015O3 was carried out. We concentrated on the analysis of the scattering peculiarities in the vicinities of M- and R- points of the Brillouin zone. We have observed a critical increase of the diffuse scattering at the position Q ≈ (0.47 + h 0.53 + k l) slightly aside of M point on cooling to the intermediate phase. We attribute observed critical scattering to a mixed mode containing both oxygen octahedral tilts and antiparallel cationic displacements. Tentative conclusion is made describing earlier reported complicated set of the satellite peaks around M-point as the result of the soft-mode driven incommensurate phase transition.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Andronikova, D. A. and Bronwald, Iu. A. and Leontiev, I. N. and Leontiev, N. G. and Chernyshov, D. Yu. and Filimonov, A. V. and Vakhrushev, S. B.},\\n\\tmonth = jan,\\n\\tyear = {2019},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/00150193.2019.1569987},\\n\\tkeywords = {phase transitions, diffuse scattering, Ferroelectricity},\\n\\tpages = {65--73},\\n}\\n\\n\",\"author_short\":[\"Andronikova, D. A.\",\"Bronwald, I. A.\",\"Leontiev, I. N.\",\"Leontiev, N. G.\",\"Chernyshov, D. Y.\",\"Filimonov, A. V.\",\"Vakhrushev, S. B.\"],\"key\":\"andronikova_incommensurate_2019\",\"id\":\"andronikova_incommensurate_2019\",\"bibbaseid\":\"andronikova-bronwald-leontiev-leontiev-chernyshov-filimonov-vakhrushev-incommensurateinstabilityanddiffusescatteringatbrillouinzoneboundaryinzrrichleadzirconatetitanate-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/00150193.2019.1569987\"},\"keyword\":[\"phase transitions\",\"diffuse scattering\",\"Ferroelectricity\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"New Electrochemical Approach for the Synthesis of Pd-PdO/C Electrocatalyst and Application to Formic Acid Electrooxidation\",\"volume\":\"4\",\"copyright\":\"© 2019 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim\",\"issn\":\"2365-6549\",\"url\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201901628\",\"doi\":\"10.1002/slct.201901628\",\"abstract\":\"Pd-PdO/C catalyst for formic acid electrooxidation has been synthesized via electrochemical dispersion of Pd foil electrodes under pulse alternating current conditions in NaCl aqueous electrolyte. About 35 wt% of the as-prepared Pd-PdO/C specimen is PdO as revealed by X-ray diffraction. The microstructural characteristics and catalytic activity of the synthesized Pd/C catalyst have been compared with those of a Pt/C catalyst prepared under the same conditions. Pd nanoparticles of Pd-PdO/C catalyst exhibit smaller average dimensions and narrower particle size distribution – 7.4±0.5 nm and 1.9±0.5 respectively for Pd and PdO particles. The process of ethanol electrooxidation on the catalyst was characterized by high overvoltage (up to 800 mV). The overvoltage of the formic acid electrochemical oxidation on Pd/C is 590 mV less than on Pt/C.\",\"language\":\"en\",\"number\":\"29\",\"urldate\":\"2023-11-11\",\"journal\":\"ChemistrySelect\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"Alexandra\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Faddeev\"],\"firstnames\":[\"Nikita\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Allix\"],\"firstnames\":[\"Mathieu\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rakhmatullin\"],\"firstnames\":[\"Aydar\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\",\"V.\"],\"suffixes\":[]}],\"year\":\"2019\",\"note\":\"_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/slct.201901628\",\"keywords\":\"alternating current, electrochemical dispersion, formic acid, fuel cell, Pd/C\",\"pages\":\"8390–8393\",\"file\":\"Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\QME9WT8N\\\\\\\\slct.html:text/html\",\"bibtex\":\"@article{kuriganova_new_2019,\\n\\ttitle = {New {Electrochemical} {Approach} for the {Synthesis} of {Pd}-{PdO}/{C} {Electrocatalyst} and {Application} to {Formic} {Acid} {Electrooxidation}},\\n\\tvolume = {4},\\n\\tcopyright = {© 2019 Wiley-VCH Verlag GmbH \\\\& Co. KGaA, Weinheim},\\n\\tissn = {2365-6549},\\n\\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201901628},\\n\\tdoi = {10.1002/slct.201901628},\\n\\tabstract = {Pd-PdO/C catalyst for formic acid electrooxidation has been synthesized via electrochemical dispersion of Pd foil electrodes under pulse alternating current conditions in NaCl aqueous electrolyte. About 35 wt\\\\% of the as-prepared Pd-PdO/C specimen is PdO as revealed by X-ray diffraction. The microstructural characteristics and catalytic activity of the synthesized Pd/C catalyst have been compared with those of a Pt/C catalyst prepared under the same conditions. Pd nanoparticles of Pd-PdO/C catalyst exhibit smaller average dimensions and narrower particle size distribution – 7.4±0.5 nm and 1.9±0.5 respectively for Pd and PdO particles. The process of ethanol electrooxidation on the catalyst was characterized by high overvoltage (up to 800 mV). The overvoltage of the formic acid electrochemical oxidation on Pd/C is 590 mV less than on Pt/C.},\\n\\tlanguage = {en},\\n\\tnumber = {29},\\n\\turldate = {2023-11-11},\\n\\tjournal = {ChemistrySelect},\\n\\tauthor = {Kuriganova, Alexandra B. and Faddeev, Nikita A. and Leontyev, Igor N. and Allix, Mathieu and Rakhmatullin, Aydar and Smirnova, Nina V.},\\n\\tyear = {2019},\\n\\tnote = {\\\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/slct.201901628},\\n\\tkeywords = {alternating current, electrochemical dispersion, formic acid, fuel cell, Pd/C},\\n\\tpages = {8390--8393},\\n\\tfile = {Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\QME9WT8N\\\\\\\\slct.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Kuriganova, A. B.\",\"Faddeev, N. A.\",\"Leontyev, I. N.\",\"Allix, M.\",\"Rakhmatullin, A.\",\"Smirnova, N. V.\"],\"key\":\"kuriganova_new_2019\",\"id\":\"kuriganova_new_2019\",\"bibbaseid\":\"kuriganova-faddeev-leontyev-allix-rakhmatullin-smirnova-newelectrochemicalapproachforthesynthesisofpdpdocelectrocatalystandapplicationtoformicacidelectrooxidation-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201901628\"},\"keyword\":[\"alternating current\",\"electrochemical dispersion\",\"formic acid\",\"fuel cell\",\"Pd/C\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Anomalous small viral shells and simplest polyhedra with icosahedral symmetry: the rhombic triacontahedron case\",\"volume\":\"75\",\"copyright\":\"Copyright (c) 2019 International Union of Crystallography\",\"issn\":\"2053-2733\",\"shorttitle\":\"Anomalous small viral shells and simplest polyhedra with icosahedral symmetry\",\"url\":\"https://journals.iucr.org/a/issues/2019/01/00/eo5089/\",\"doi\":\"10.1107/S2053273318015656\",\"abstract\":\"The symmetry of the capsomers forming a viral shell determines the polyhedron underlying the shell structure. If the capsid is self-assembled from dimers, this is the rhombic triacontahedron with 30 equivalent rhombic faces.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Acta Crystallographica Section A: Foundations and Advances\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Pimonov\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Konevtsova\"],\"firstnames\":[\"O.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2019\",\"note\":\"Number: 1 Publisher: International Union of Crystallography\",\"pages\":\"135–141\",\"bibtex\":\"@article{pimonov_anomalous_2019,\\n\\ttitle = {Anomalous small viral shells and simplest polyhedra with icosahedral symmetry: the rhombic triacontahedron case},\\n\\tvolume = {75},\\n\\tcopyright = {Copyright (c) 2019 International Union of Crystallography},\\n\\tissn = {2053-2733},\\n\\tshorttitle = {Anomalous small viral shells and simplest polyhedra with icosahedral symmetry},\\n\\turl = {https://journals.iucr.org/a/issues/2019/01/00/eo5089/},\\n\\tdoi = {10.1107/S2053273318015656},\\n\\tabstract = {The symmetry of the capsomers forming a viral shell determines the polyhedron underlying the shell structure. If the capsid is self-assembled from dimers, this is the rhombic triacontahedron with 30 equivalent rhombic faces.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Acta Crystallographica Section A: Foundations and Advances},\\n\\tauthor = {Pimonov, V. V. and Konevtsova, O. V. and Rochal, S. B.},\\n\\tmonth = jan,\\n\\tyear = {2019},\\n\\tnote = {Number: 1\\nPublisher: International Union of Crystallography},\\n\\tpages = {135--141},\\n}\\n\\n\",\"author_short\":[\"Pimonov, V. V.\",\"Konevtsova, O. V.\",\"Rochal, S. B.\"],\"key\":\"pimonov_anomalous_2019\",\"id\":\"pimonov_anomalous_2019\",\"bibbaseid\":\"pimonov-konevtsova-rochal-anomaloussmallviralshellsandsimplestpolyhedrawithicosahedralsymmetrytherhombictriacontahedroncase-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.iucr.org/a/issues/2019/01/00/eo5089/\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Тепловые флуктуации и резонансные свойства сканирующих зондов на основе углеродных нанотрубок\",\"volume\":\"61\",\"issn\":\"0367-3294\",\"url\":\"https://journals.ioffe.ru/articles/47244\",\"doi\":\"10.21883/FTT.2019.03.47244.237\",\"abstract\":\"AbstractThe design of cantilevers and microelectromechanical systems based on carbon nanotubes necessitates a thorough study of their thermal fluctuations and resonance properties. This work aims at the simulation of thermal fluctuations and power spectral density for single-walled carbon nanotubes in the context of the continuous model of elastic cylindrical membranes with nonmacroscopic thicknesses. The conditions imposed on the geometry of this probe and providing its stable operation, as well as the high lateral resolution determined by only the radius of the nanotube independently on its thermal vibrations, are found, as well. The most intensive resonance modes, making the greatest contribution to the thermal fluctuations of carbon nanotubes, are established, and their frequencies are found analytically. , Проектирование кантилеверов и микроэлектромеханических систем с использованием углеродных нанотрубок неразрывно связано с изучением их тепловых флуктуаций и резонансных свойств. В настоящей работе для одностенных углеродных нанотрубок производится расчет тепловых флуктуаций и спектральной плотности интенсивности колебаний в рамках континуальной модели упругих цилиндрических мембран, не обладающих макроскопической толщиной. Найдены налагаемые на геометрию такого зонда условия, выполнение которых обеспечивает как стабильность его работы, так и высокое латеральное разрешение, определяющееся только радиусом нанотрубки и не зависящее от величины ее тепловых колебаний. Определены самые интенсивные резонансные моды, дающие наибольший вклад в тепловые флуктуации углеродных нанотрубок, а также получено аналитическое выражение для их частот.\",\"language\":\"ru\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Чалин\"],\"firstnames\":[\"Д.В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Авраменко\"],\"firstnames\":[\"М.В.\"],\"suffixes\":[]}],\"year\":\"2019\",\"pages\":\"514\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\GE9CNIBE\\\\\\\\Чалин и Авраменко - 2019 - Тепловые флуктуации и резонансные свойства сканиру.pdf:application/pdf\",\"bibtex\":\"@article{__2019,\\n\\ttitle = {Тепловые флуктуации и резонансные свойства сканирующих зондов на основе углеродных нанотрубок},\\n\\tvolume = {61},\\n\\tissn = {0367-3294},\\n\\turl = {https://journals.ioffe.ru/articles/47244},\\n\\tdoi = {10.21883/FTT.2019.03.47244.237},\\n\\tabstract = {AbstractThe design of cantilevers and microelectromechanical systems based on carbon nanotubes necessitates a thorough study of their thermal fluctuations and resonance properties. This work aims at the simulation of thermal fluctuations and power spectral density for single-walled carbon nanotubes in the context of the continuous model of elastic cylindrical membranes with nonmacroscopic thicknesses. The conditions imposed on the geometry of this probe and providing its stable operation, as well as the high lateral resolution determined by only the radius of the nanotube independently on its thermal vibrations, are found, as well. The most intensive resonance modes, making the greatest contribution to the thermal fluctuations of carbon nanotubes, are established, and their frequencies are found analytically.\\n          , \\n            Проектирование кантилеверов и микроэлектромеханических систем с использованием углеродных нанотрубок неразрывно связано с изучением их тепловых флуктуаций и резонансных свойств. В настоящей работе для одностенных углеродных нанотрубок производится расчет тепловых флуктуаций и спектральной плотности интенсивности колебаний в рамках континуальной модели упругих цилиндрических мембран, не обладающих макроскопической толщиной. Найдены налагаемые на геометрию такого зонда условия, выполнение которых обеспечивает как стабильность его работы, так и высокое латеральное разрешение, определяющееся только радиусом нанотрубки и не зависящее от величины ее тепловых колебаний. Определены самые интенсивные резонансные моды, дающие наибольший вклад в тепловые флуктуации углеродных нанотрубок, а также получено аналитическое выражение для их частот.},\\n\\tlanguage = {ru},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Чалин, Д.В. and Авраменко, М.В.},\\n\\tyear = {2019},\\n\\tpages = {514},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\GE9CNIBE\\\\\\\\Чалин и Авраменко - 2019 - Тепловые флуктуации и резонансные свойства сканиру.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Чалин, Д.\",\"Авраменко, М.\"],\"key\":\"__2019\",\"id\":\"__2019\",\"bibbaseid\":\"---2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/47244\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Synthesis of Co3O4/CoOOH via electrochemical dispersion using a pulse alternating current method for lithium-ion batteries and supercapacitors\",\"volume\":\"86\",\"issn\":\"1293-2558\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S129325581830551X\",\"doi\":\"10.1016/j.solidstatesciences.2018.10.005\",\"abstract\":\"We report a convenient, low-cost and ecofriendly approach for the fabrication of a Co3O4/CoOOH electrode material intended for lithium ion batteries (LIBs) and supercapacitors (SCs) using the electrochemical dispersion of the cobalt foil through the pulse alternating current (PAC) method. The synthesized material is a Co3O4/CoOOH composite (with about 10–15 wt% CoOOH) in the form of nanosheets with a length of approximately 200 nm and a thickness of 10–20 nm. It is found to exhibit high reversible discharge specific capacities and good cycling behavior while tested as the anode material in LIBs. Measuring the reversible capacitance at high (2C) and low (C/20) cycling rates gives the values of 610 mAh g−1 and 1030 mAh g−1, respectively. The specimen possesses excellent performance as the electrode for SCs with the retention of capacitance up to 98% at the current density increasing from 0.5 to 10 A g−1. After 1000 cycles at a current density of 10 A g−1 the electrode maintains about 90% of its initial capacitance which evidences the long cycle life. Hence, electrochemically prepared Co3O4/CoOOH seems to be a promising candidate for high-performance LIBs and SCs applications.\",\"urldate\":\"2023-11-11\",\"journal\":\"Solid State Sciences\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Chernysheva\"],\"firstnames\":[\"Daria\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vlaic\"],\"firstnames\":[\"Codruta\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pudova\"],\"firstnames\":[\"Lyudmila\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ivanov\"],\"firstnames\":[\"Svetlozar\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Avramenko\"],\"firstnames\":[\"Marina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Allix\"],\"firstnames\":[\"Mathieu\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rakhmatullin\"],\"firstnames\":[\"Aydar\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"Olga\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bund\"],\"firstnames\":[\"Andreas\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2018\",\"pages\":\"53–59\",\"file\":\"ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\9GU5I35X\\\\§129325581830551X.html:text/html\",\"bibtex\":\"@article{chernysheva_synthesis_2018,\\n\\ttitle = {Synthesis of {Co3O4}/{CoOOH} via electrochemical dispersion using a pulse alternating current method for lithium-ion batteries and supercapacitors},\\n\\tvolume = {86},\\n\\tissn = {1293-2558},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S129325581830551X},\\n\\tdoi = {10.1016/j.solidstatesciences.2018.10.005},\\n\\tabstract = {We report a convenient, low-cost and ecofriendly approach for the fabrication of a Co3O4/CoOOH electrode material intended for lithium ion batteries (LIBs) and supercapacitors (SCs) using the electrochemical dispersion of the cobalt foil through the pulse alternating current (PAC) method. The synthesized material is a Co3O4/CoOOH composite (with about 10–15 wt\\\\% CoOOH) in the form of nanosheets with a length of approximately 200 nm and a thickness of 10–20 nm. It is found to exhibit high reversible discharge specific capacities and good cycling behavior while tested as the anode material in LIBs. Measuring the reversible capacitance at high (2C) and low (C/20) cycling rates gives the values of 610 mAh g−1 and 1030 mAh g−1, respectively. The specimen possesses excellent performance as the electrode for SCs with the retention of capacitance up to 98\\\\% at the current density increasing from 0.5 to 10 A g−1. After 1000 cycles at a current density of 10 A g−1 the electrode maintains about 90\\\\% of its initial capacitance which evidences the long cycle life. Hence, electrochemically prepared Co3O4/CoOOH seems to be a promising candidate for high-performance LIBs and SCs applications.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Solid State Sciences},\\n\\tauthor = {Chernysheva, Daria and Vlaic, Codruta and Leontyev, Igor and Pudova, Lyudmila and Ivanov, Svetlozar and Avramenko, Marina and Allix, Mathieu and Rakhmatullin, Aydar and Maslova, Olga and Bund, Andreas and Smirnova, Nina},\\n\\tmonth = dec,\\n\\tyear = {2018},\\n\\tpages = {53--59},\\n\\tfile = {ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\9GU5I35X\\\\\\\\S129325581830551X.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Chernysheva, D.\",\"Vlaic, C.\",\"Leontyev, I.\",\"Pudova, L.\",\"Ivanov, S.\",\"Avramenko, M.\",\"Allix, M.\",\"Rakhmatullin, A.\",\"Maslova, O.\",\"Bund, A.\",\"Smirnova, N.\"],\"key\":\"chernysheva_synthesis_2018\",\"id\":\"chernysheva_synthesis_2018\",\"bibbaseid\":\"chernysheva-vlaic-leontyev-pudova-ivanov-avramenko-allix-rakhmatullin-etal-synthesisofco3o4cooohviaelectrochemicaldispersionusingapulsealternatingcurrentmethodforlithiumionbatteriesandsupercapacitors-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S129325581830551X\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Non-isothermal decomposition of platinum acetylacetonate as a cost-efficient and Size-Controlled Synthesis of Pt/C nanoparticles\",\"volume\":\"117\",\"issn\":\"1566-7367\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S1566736718303686\",\"doi\":\"10.1016/j.catcom.2018.08.022\",\"abstract\":\"A simple two-stage synthesis of Pt/C nanoparticles based on the non-isothermal decomposition of platinum acetylacetonate is presented. It allows not only production of Pt nanoparticles, but also their sizes control during the synthesis. The heating rate is the key factor for tuning the average Pt nanoparticle size. The electrochemical surface area of produced nanoparticles enlarges with rising heating rate, which can enrich 103 m2/g. The growth dynamics of Pt/C nanoparticles is tracked via in-situ XRD. Furthermore, the electrocatalytic activity of Pt/C catalysts is studied as a function of platinum particle size in cases of ethanol electro-oxidation and oxygen reduction reactions.\",\"urldate\":\"2023-11-11\",\"journal\":\"Catalysis Communications\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kulbakov\"],\"firstnames\":[\"Anton\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"Alexandra\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Allix\"],\"firstnames\":[\"Mathieu\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rakhmatullin\"],\"firstnames\":[\"Aydar\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"NinaV.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"Olga\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\",\"N.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2018\",\"keywords\":\"Pt/C, In-situ, Pt acetylacetonate, Size control, Thermal decomposition\",\"pages\":\"14–18\",\"bibtex\":\"@article{kulbakov_non-isothermal_2018,\\n\\ttitle = {Non-isothermal decomposition of platinum acetylacetonate as a cost-efficient and {Size}-{Controlled} {Synthesis} of {Pt}/{C} nanoparticles},\\n\\tvolume = {117},\\n\\tissn = {1566-7367},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S1566736718303686},\\n\\tdoi = {10.1016/j.catcom.2018.08.022},\\n\\tabstract = {A simple two-stage synthesis of Pt/C nanoparticles based on the non-isothermal decomposition of platinum acetylacetonate is presented. It allows not only production of Pt nanoparticles, but also their sizes control during the synthesis. The heating rate is the key factor for tuning the average Pt nanoparticle size. The electrochemical surface area of produced nanoparticles enlarges with rising heating rate, which can enrich 103 m2/g. The growth dynamics of Pt/C nanoparticles is tracked via in-situ XRD. Furthermore, the electrocatalytic activity of Pt/C catalysts is studied as a function of platinum particle size in cases of ethanol electro-oxidation and oxygen reduction reactions.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Catalysis Communications},\\n\\tauthor = {Kulbakov, Anton A. and Kuriganova, Alexandra B. and Allix, Mathieu and Rakhmatullin, Aydar and Smirnova, NinaV. and Maslova, Olga A. and Leontyev, Igor N.},\\n\\tmonth = dec,\\n\\tyear = {2018},\\n\\tkeywords = {Pt/C, In-situ, Pt acetylacetonate, Size control, Thermal decomposition},\\n\\tpages = {14--18},\\n}\\n\\n\",\"author_short\":[\"Kulbakov, A. A.\",\"Kuriganova, A. B.\",\"Allix, M.\",\"Rakhmatullin, A.\",\"Smirnova, N.\",\"Maslova, O. A.\",\"Leontyev, I. N.\"],\"key\":\"kulbakov_non-isothermal_2018\",\"id\":\"kulbakov_non-isothermal_2018\",\"bibbaseid\":\"kulbakov-kuriganova-allix-rakhmatullin-smirnova-maslova-leontyev-nonisothermaldecompositionofplatinumacetylacetonateasacostefficientandsizecontrolledsynthesisofptcnanoparticles-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S1566736718303686\"},\"keyword\":[\"Pt/C\",\"In-situ\",\"Pt acetylacetonate\",\"Size control\",\"Thermal decomposition\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Effect of Thermal Treatment on the Atomic Structure and Electrochemical Characteristics of Bimetallic PtCu Core–Shell Nanoparticles in PtCu/C Electrocatalysts\",\"volume\":\"122\",\"issn\":\"1932-7447\",\"url\":\"https://doi.org/10.1021/acs.jpcc.8b03696\",\"doi\":\"10.1021/acs.jpcc.8b03696\",\"abstract\":\"Supported PtCu/C electrocatalysts containing core–shell bimetallic PtCu nanoparticles were synthesized by sequential chemical reduction of Cu2+ and Pt(IV) in a carbon suspension, prepared on the basis of ethylene glycol–water solvent, and then treated at different temperatures in the range from 250 to 350 °C. The structural characterization of “as-prepared” PtCu nanoparticles and of those obtained after the thermal treatments was performed by transmission electron microscopy, X-ray diffraction, and Pt L3- and Cu K-edge extended X-ray absorption fine structure spectroscopy. The atomic cluster models of PtCu nanoparticles before and after the thermal treatment, reflecting the character of the components’ distribution, were generated. The electrochemical performance of the obtained PtCu/C electrocatalysts in oxygen reduction reaction was studied by cycling and linear voltammetry.\",\"number\":\"30\",\"urldate\":\"2023-11-11\",\"journal\":\"The Journal of Physical Chemistry C\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Pryadchenko\"],\"firstnames\":[\"Vasiliy\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Belenov\"],\"firstnames\":[\"Sergey\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shemet\"],\"firstnames\":[\"Darya\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Srabionyan\"],\"firstnames\":[\"Vasiliy\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Avakyan\"],\"firstnames\":[\"Leon\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Volochaev\"],\"firstnames\":[\"Vadim\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"Alexey\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bdoyan\"],\"firstnames\":[\"Karina\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zizak\"],\"firstnames\":[\"Ivo\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Guterman\"],\"firstnames\":[\"Vladimir\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bugaev\"],\"firstnames\":[\"Lusegen\",\"A.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2018\",\"note\":\"Publisher: American Chemical Society\",\"pages\":\"17199–17210\",\"bibtex\":\"@article{pryadchenko_effect_2018,\\n\\ttitle = {Effect of {Thermal} {Treatment} on the {Atomic} {Structure} and {Electrochemical} {Characteristics} of {Bimetallic} {PtCu} {Core}–{Shell} {Nanoparticles} in {PtCu}/{C} {Electrocatalysts}},\\n\\tvolume = {122},\\n\\tissn = {1932-7447},\\n\\turl = {https://doi.org/10.1021/acs.jpcc.8b03696},\\n\\tdoi = {10.1021/acs.jpcc.8b03696},\\n\\tabstract = {Supported PtCu/C electrocatalysts containing core–shell bimetallic PtCu nanoparticles were synthesized by sequential chemical reduction of Cu2+ and Pt(IV) in a carbon suspension, prepared on the basis of ethylene glycol–water solvent, and then treated at different temperatures in the range from 250 to 350 °C. The structural characterization of “as-prepared” PtCu nanoparticles and of those obtained after the thermal treatments was performed by transmission electron microscopy, X-ray diffraction, and Pt L3- and Cu K-edge extended X-ray absorption fine structure spectroscopy. The atomic cluster models of PtCu nanoparticles before and after the thermal treatment, reflecting the character of the components’ distribution, were generated. The electrochemical performance of the obtained PtCu/C electrocatalysts in oxygen reduction reaction was studied by cycling and linear voltammetry.},\\n\\tnumber = {30},\\n\\turldate = {2023-11-11},\\n\\tjournal = {The Journal of Physical Chemistry C},\\n\\tauthor = {Pryadchenko, Vasiliy V. and Belenov, Sergey V. and Shemet, Darya B. and Srabionyan, Vasiliy V. and Avakyan, Leon A. and Volochaev, Vadim A. and Mikheykin, Alexey S. and Bdoyan, Karina E. and Zizak, Ivo and Guterman, Vladimir E. and Bugaev, Lusegen A.},\\n\\tmonth = aug,\\n\\tyear = {2018},\\n\\tnote = {Publisher: American Chemical Society},\\n\\tpages = {17199--17210},\\n}\\n\\n\",\"author_short\":[\"Pryadchenko, V. V.\",\"Belenov, S. V.\",\"Shemet, D. B.\",\"Srabionyan, V. V.\",\"Avakyan, L. A.\",\"Volochaev, V. A.\",\"Mikheykin, A. S.\",\"Bdoyan, K. E.\",\"Zizak, I.\",\"Guterman, V. E.\",\"Bugaev, L. A.\"],\"key\":\"pryadchenko_effect_2018\",\"id\":\"pryadchenko_effect_2018\",\"bibbaseid\":\"pryadchenko-belenov-shemet-srabionyan-avakyan-volochaev-mikheykin-bdoyan-etal-effectofthermaltreatmentontheatomicstructureandelectrochemicalcharacteristicsofbimetallicptcucoreshellnanoparticlesinptcucelectrocatalysts-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1021/acs.jpcc.8b03696\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"PtIr/C Catalysts Synthesized by Electrochemical Dispersion Method for Proton Exchange Membrane Fuel Cells\",\"volume\":\"54\",\"issn\":\"1608-3342\",\"url\":\"https://doi.org/10.1134/S1023193518060113\",\"doi\":\"10.1134/S1023193518060113\",\"abstract\":\"PtIr/C electrocatalyst with the metal phase uniformly distributed over the carbon support surface and the average size of PtIr nanoparticles of 5.9 nm is synthesized by electrochemical dispersion of Pt90Ir10 alloy under the action of alternating pulse current. It is shown that the presence of iridium within the composition of a Pt/C catalyst lowers down the overpotential of CO oxidation and increases catalyst’s specific activity with respect to electrochemical oxidation of ethanol.\",\"language\":\"en\",\"number\":\"6\",\"urldate\":\"2023-11-11\",\"journal\":\"Russian Journal of Electrochemistry\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"A.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leont’ev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"N.\",\"V.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2018\",\"keywords\":\"electrochemical dispersion, fuel cell, electrocatalysis, platinum, iridium\",\"pages\":\"561–565\",\"bibtex\":\"@article{kuriganova_ptirc_2018,\\n\\ttitle = {{PtIr}/{C} {Catalysts} {Synthesized} by {Electrochemical} {Dispersion} {Method} for {Proton} {Exchange} {Membrane} {Fuel} {Cells}},\\n\\tvolume = {54},\\n\\tissn = {1608-3342},\\n\\turl = {https://doi.org/10.1134/S1023193518060113},\\n\\tdoi = {10.1134/S1023193518060113},\\n\\tabstract = {PtIr/C electrocatalyst with the metal phase uniformly distributed over the carbon support surface and the average size of PtIr nanoparticles of 5.9 nm is synthesized by electrochemical dispersion of Pt90Ir10 alloy under the action of alternating pulse current. It is shown that the presence of iridium within the composition of a Pt/C catalyst lowers down the overpotential of CO oxidation and increases catalyst’s specific activity with respect to electrochemical oxidation of ethanol.},\\n\\tlanguage = {en},\\n\\tnumber = {6},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Russian Journal of Electrochemistry},\\n\\tauthor = {Kuriganova, A. B. and Leont’ev, I. N. and Smirnova, N. V.},\\n\\tmonth = jun,\\n\\tyear = {2018},\\n\\tkeywords = {electrochemical dispersion, fuel cell, electrocatalysis, platinum, iridium},\\n\\tpages = {561--565},\\n}\\n\\n\",\"author_short\":[\"Kuriganova, A. B.\",\"Leont’ev, I. N.\",\"Smirnova, N. V.\"],\"key\":\"kuriganova_ptirc_2018\",\"id\":\"kuriganova_ptirc_2018\",\"bibbaseid\":\"kuriganova-leontev-smirnova-ptirccatalystssynthesizedbyelectrochemicaldispersionmethodforprotonexchangemembranefuelcells-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1023193518060113\"},\"keyword\":[\"electrochemical dispersion\",\"fuel cell\",\"electrocatalysis\",\"platinum\",\"iridium\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Crystallography Based on Synchrotron Radiation: Experiments of Russian Users of the ESRF BM01 Diffraction Beam Line\",\"volume\":\"12\",\"issn\":\"1819-7094\",\"shorttitle\":\"Crystallography Based on Synchrotron Radiation\",\"url\":\"https://doi.org/10.1134/S1027451018030084\",\"doi\":\"10.1134/S1027451018030084\",\"abstract\":\"The review deals with studies carried out at the BM01 diffraction beam line of the European Synchrotron Radiation Facility. X-ray diffraction analysis of single-crystal proton conductors demonstrates the possibilities of a precise diffraction experiment in which phase transitions associated with the release of crystallization water and transformation of the network of hydrogen contacts are investigated. Scanning of reciprocal space with the help of a 2D detector enables us to determine the new phase symmetry in a thin-film multiferroic sample based on bismuth ferrite (the given phase is stable only under thin-film conditions). A combination of Bragg and diffusion scattering processes is employed to investigate the interdependence between the structure and dynamics of a crystal lattice and the physical properties of a relaxor material with a perovskite-like structure. The complementarity and synergy of neutron and synchrotron experiments are demonstrated using the combined study of materials from the manganese-silicide group, which has revealed a nontrivial relationship between magnetic and crystallographic chiralities in noncollinear magnets. Although the given review is limited to only a few experiments carried out by Russian scientists at the BM01 beam line, they still illustrate a variety of problems that can be solved using a modern diffraction station where the bending magnet of a third-generation synchrotron is employed as the synchrotron radiation source.\",\"language\":\"en\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Surface Investigation: X-ray, Synchrotron and Neutron Techniques\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Dmitriev\"],\"firstnames\":[\"V.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chernyshov\"],\"firstnames\":[\"D.\",\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dyadkin\"],\"firstnames\":[\"V.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Makarova\"],\"firstnames\":[\"I.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Andronikova\"],\"firstnames\":[\"D.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bronwald\"],\"firstnames\":[\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Burkovsky\"],\"firstnames\":[\"R.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vakhrushev\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Filimonov\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grigoriev\"],\"firstnames\":[\"S.\",\"V.\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2018\",\"keywords\":\"crystallography, synchrotron X-ray diffraction, X-ray analysis\",\"pages\":\"395–407\",\"bibtex\":\"@article{dmitriev_crystallography_2018,\\n\\ttitle = {Crystallography {Based} on {Synchrotron} {Radiation}: {Experiments} of {Russian} {Users} of the {ESRF} {BM01} {Diffraction} {Beam} {Line}},\\n\\tvolume = {12},\\n\\tissn = {1819-7094},\\n\\tshorttitle = {Crystallography {Based} on {Synchrotron} {Radiation}},\\n\\turl = {https://doi.org/10.1134/S1027451018030084},\\n\\tdoi = {10.1134/S1027451018030084},\\n\\tabstract = {The review deals with studies carried out at the BM01 diffraction beam line of the European Synchrotron Radiation Facility. X-ray diffraction analysis of single-crystal proton conductors demonstrates the possibilities of a precise diffraction experiment in which phase transitions associated with the release of crystallization water and transformation of the network of hydrogen contacts are investigated. Scanning of reciprocal space with the help of a 2D detector enables us to determine the new phase symmetry in a thin-film multiferroic sample based on bismuth ferrite (the given phase is stable only under thin-film conditions). A combination of Bragg and diffusion scattering processes is employed to investigate the interdependence between the structure and dynamics of a crystal lattice and the physical properties of a relaxor material with a perovskite-like structure. The complementarity and synergy of neutron and synchrotron experiments are demonstrated using the combined study of materials from the manganese-silicide group, which has revealed a nontrivial relationship between magnetic and crystallographic chiralities in noncollinear magnets. Although the given review is limited to only a few experiments carried out by Russian scientists at the BM01 beam line, they still illustrate a variety of problems that can be solved using a modern diffraction station where the bending magnet of a third-generation synchrotron is employed as the synchrotron radiation source.},\\n\\tlanguage = {en},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Surface Investigation: X-ray, Synchrotron and Neutron Techniques},\\n\\tauthor = {Dmitriev, V. P. and Chernyshov, D. Yu. and Dyadkin, V. A. and Makarova, I. P. and Leontyev, I. N. and Andronikova, D. A. and Bronwald, I. and Burkovsky, R. G. and Vakhrushev, S. B. and Filimonov, A. V. and Grigoriev, S. V.},\\n\\tmonth = may,\\n\\tyear = {2018},\\n\\tkeywords = {crystallography, synchrotron X-ray diffraction, X-ray analysis},\\n\\tpages = {395--407},\\n}\\n\\n\",\"author_short\":[\"Dmitriev, V. P.\",\"Chernyshov, D. Y.\",\"Dyadkin, V. A.\",\"Makarova, I. P.\",\"Leontyev, I. N.\",\"Andronikova, D. A.\",\"Bronwald, I.\",\"Burkovsky, R. G.\",\"Vakhrushev, S. B.\",\"Filimonov, A. V.\",\"Grigoriev, S. V.\"],\"key\":\"dmitriev_crystallography_2018\",\"id\":\"dmitriev_crystallography_2018\",\"bibbaseid\":\"dmitriev-chernyshov-dyadkin-makarova-leontyev-andronikova-bronwald-burkovsky-etal-crystallographybasedonsynchrotronradiationexperimentsofrussianusersoftheesrfbm01diffractionbeamline-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1027451018030084\"},\"keyword\":[\"crystallography\",\"synchrotron X-ray diffraction\",\"X-ray analysis\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Optical Properties of Barium Strontium Niobate SBN61 Films\",\"volume\":\"60\",\"issn\":\"1090-6460\",\"url\":\"https://doi.org/10.1134/S1063783418050293\",\"doi\":\"10.1134/S1063783418050293\",\"abstract\":\"Heteroepitaxial Sr0.61Ba0.39Nb2O6 films have been formed on MgO(001) substrates by RF deposition in an oxygen atmosphere. The film orientation with respect to the substrate is investigated using X-ray diffraction. The permittivity dispersion parameters in the visible range are determined by measuring optical transmission spectra. The films are found to have a wider band gap and a smaller refractive index as compared with the single-crystal material.\",\"language\":\"en\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Physics of the Solid State\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pavlenko\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Stryukov\"],\"firstnames\":[\"D.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Revinskii\"],\"firstnames\":[\"Yu.\",\"V.\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2018\",\"pages\":\"1005–1010\",\"bibtex\":\"@article{shirokov_optical_2018,\\n\\ttitle = {Optical {Properties} of {Barium} {Strontium} {Niobate} {SBN61} {Films}},\\n\\tvolume = {60},\\n\\tissn = {1090-6460},\\n\\turl = {https://doi.org/10.1134/S1063783418050293},\\n\\tdoi = {10.1134/S1063783418050293},\\n\\tabstract = {Heteroepitaxial Sr0.61Ba0.39Nb2O6 films have been formed on MgO(001) substrates by RF deposition in an oxygen atmosphere. The film orientation with respect to the substrate is investigated using X-ray diffraction. The permittivity dispersion parameters in the visible range are determined by measuring optical transmission spectra. The films are found to have a wider band gap and a smaller refractive index as compared with the single-crystal material.},\\n\\tlanguage = {en},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physics of the Solid State},\\n\\tauthor = {Shirokov, V. B. and Pavlenko, A. V. and Stryukov, D. V. and Revinskii, Yu. V.},\\n\\tmonth = may,\\n\\tyear = {2018},\\n\\tpages = {1005--1010},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Pavlenko, A. V.\",\"Stryukov, D. V.\",\"Revinskii, Y. V.\"],\"key\":\"shirokov_optical_2018\",\"id\":\"shirokov_optical_2018\",\"bibbaseid\":\"shirokov-pavlenko-stryukov-revinskii-opticalpropertiesofbariumstrontiumniobatesbn61films-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1063783418050293\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Electrochemically synthesized Pt-based catalysts with different carbon supports for proton exchange membrane fuel cell applications\",\"volume\":\"28\",\"issn\":\"0959-9436\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0959943618301834\",\"doi\":\"10.1016/j.mencom.2018.07.036\",\"abstract\":\"The Pt/C catalysts containing various types of carbon support were prepared via electrochemical oxidation/dispersion. Their different catalytic activity in CO-stripping and ethanol electrooxidation was revealed.\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Mendeleev Communications\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"Alexandra\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"Olga\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\",\"V.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2018\",\"pages\":\"444–446\",\"bibtex\":\"@article{kuriganova_electrochemically_2018,\\n\\ttitle = {Electrochemically synthesized {Pt}-based catalysts with different carbon supports for proton exchange membrane fuel cell applications},\\n\\tvolume = {28},\\n\\tissn = {0959-9436},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0959943618301834},\\n\\tdoi = {10.1016/j.mencom.2018.07.036},\\n\\tabstract = {The Pt/C catalysts containing various types of carbon support were prepared via electrochemical oxidation/dispersion. Their different catalytic activity in CO-stripping and ethanol electrooxidation was revealed.},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Mendeleev Communications},\\n\\tauthor = {Kuriganova, Alexandra B. and Leontyev, Igor N. and Maslova, Olga A. and Smirnova, Nina V.},\\n\\tmonth = jul,\\n\\tyear = {2018},\\n\\tpages = {444--446},\\n}\\n\\n\",\"author_short\":[\"Kuriganova, A. B.\",\"Leontyev, I. N.\",\"Maslova, O. A.\",\"Smirnova, N. V.\"],\"key\":\"kuriganova_electrochemically_2018\",\"id\":\"kuriganova_electrochemically_2018\",\"bibbaseid\":\"kuriganova-leontyev-maslova-smirnova-electrochemicallysynthesizedptbasedcatalystswithdifferentcarbonsupportsforprotonexchangemembranefuelcellapplications-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0959943618301834\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Electric-field-dependent mechanical and electrical properties of barium strontium titanate films for tunable device applications\",\"volume\":\"657\",\"issn\":\"0040-6090\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0040609018302918\",\"doi\":\"10.1016/j.tsf.2018.04.029\",\"abstract\":\"Developing the novel electric field tunable, reconfigurable, adaptive and frequency-agile microwave devices with specific properties involves technological and scientific activities in the studying of material properties. Measurements of its properties could be a difficult and expensive issue, especially when it concerns thin-film ferroelectrics. Their electromechanical properties change significantly under applied DC bias field. The material coefficients of barium strontium titanate thin films are still unknown; therefore, it is expedient to carry out their calculations. In the present paper, the linear equations of piezoelectric effect have been written for thin barium strontium titanate films under DC bias electric field in paraelectric phase (induced piezoelectric effect) based on the grand potential of Landau theory of phase transitions. The dependence of material constants for thin films of Ba0.65Sr0.35TiO3 (BST65) on the applied planar field at different lattice misfit strains has been studied for this phase. All induced piezoelectric moduli show extreme behavior during field alteration. Elastic moduli show similar abnormal behavior. The alterations increase as misfit strain is approaching the critical value.\",\"urldate\":\"2023-11-11\",\"journal\":\"Thin Solid Films\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kalinchuk\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2018\",\"keywords\":\"Phenomenological theory, Phase transitions, Barium strontium titanate, Ferroelectric thin film\",\"pages\":\"8–15\",\"bibtex\":\"@article{shirokov_electric-field-dependent_2018,\\n\\ttitle = {Electric-field-dependent mechanical and electrical properties of barium strontium titanate films for tunable device applications},\\n\\tvolume = {657},\\n\\tissn = {0040-6090},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0040609018302918},\\n\\tdoi = {10.1016/j.tsf.2018.04.029},\\n\\tabstract = {Developing the novel electric field tunable, reconfigurable, adaptive and frequency-agile microwave devices with specific properties involves technological and scientific activities in the studying of material properties. Measurements of its properties could be a difficult and expensive issue, especially when it concerns thin-film ferroelectrics. Their electromechanical properties change significantly under applied DC bias field. The material coefficients of barium strontium titanate thin films are still unknown; therefore, it is expedient to carry out their calculations. In the present paper, the linear equations of piezoelectric effect have been written for thin barium strontium titanate films under DC bias electric field in paraelectric phase (induced piezoelectric effect) based on the grand potential of Landau theory of phase transitions. The dependence of material constants for thin films of Ba0.65Sr0.35TiO3 (BST65) on the applied planar field at different lattice misfit strains has been studied for this phase. All induced piezoelectric moduli show extreme behavior during field alteration. Elastic moduli show similar abnormal behavior. The alterations increase as misfit strain is approaching the critical value.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Thin Solid Films},\\n\\tauthor = {Shirokov, V. B. and Kalinchuk, V. V. and Timoshenko, P. E.},\\n\\tmonth = jul,\\n\\tyear = {2018},\\n\\tkeywords = {Phenomenological theory, Phase transitions, Barium strontium titanate, Ferroelectric thin film},\\n\\tpages = {8--15},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Kalinchuk, V. V.\",\"Timoshenko, P. E.\"],\"key\":\"shirokov_electric-field-dependent_2018\",\"id\":\"shirokov_electric-field-dependent_2018\",\"bibbaseid\":\"shirokov-kalinchuk-timoshenko-electricfielddependentmechanicalandelectricalpropertiesofbariumstrontiumtitanatefilmsfortunabledeviceapplications-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0040609018302918\"},\"keyword\":[\"Phenomenological theory\",\"Phase transitions\",\"Barium strontium titanate\",\"Ferroelectric thin film\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"Macroscopic monolayer of plasmon coupled gold nanoparticles on mirror for fluorescence enhancement\",\"volume\":\"10716\",\"url\":\"https://www.spiedigitallibrary.org/conference-proceedings-of-spie/10716/107161F/Macroscopic-monolayer-of-plasmon-coupled-gold-nanoparticles-on-mirror-for/10.1117/12.2315071.full\",\"doi\":\"10.1117/12.2315071\",\"abstract\":\"We study an ability of a large quasi-homogeneous monolayer of Au plasmon coupled nanoparticles separated from continuous Au film by polymer spacer to enhance a fluorescence of adsorbed molecular species. A fluorescence response of Methylene Blue molecules is studied as a function of polymer film thickness. A change of plasmonic properties of a system, its ability to enhance a fluorescence and the possible heating of a structure upon light absorption are discussed.\",\"urldate\":\"2023-11-11\",\"booktitle\":\"Saratov Fall Meeting 2017: Optical Technologies in Biophysics and Medicine XIX\",\"publisher\":\"SPIE\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kaydashev\"],\"firstnames\":[\"V.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zolotukhin\"],\"firstnames\":[\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Belanova\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Anokhin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zharinov\"],\"firstnames\":[\"V.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2018\",\"pages\":\"357–363\",\"bibtex\":\"@inproceedings{kaydashev_macroscopic_2018,\\n\\ttitle = {Macroscopic monolayer of plasmon coupled gold nanoparticles on mirror for fluorescence enhancement},\\n\\tvolume = {10716},\\n\\turl = {https://www.spiedigitallibrary.org/conference-proceedings-of-spie/10716/107161F/Macroscopic-monolayer-of-plasmon-coupled-gold-nanoparticles-on-mirror-for/10.1117/12.2315071.full},\\n\\tdoi = {10.1117/12.2315071},\\n\\tabstract = {We study an ability of a large quasi-homogeneous monolayer of Au plasmon coupled nanoparticles separated from continuous Au film by polymer spacer to enhance a fluorescence of adsorbed molecular species. A fluorescence response of Methylene Blue molecules is studied as a function of polymer film thickness. A change of plasmonic properties of a system, its ability to enhance a fluorescence and the possible heating of a structure upon light absorption are discussed.},\\n\\turldate = {2023-11-11},\\n\\tbooktitle = {Saratov {Fall} {Meeting} 2017: {Optical} {Technologies} in {Biophysics} and {Medicine} {XIX}},\\n\\tpublisher = {SPIE},\\n\\tauthor = {Kaydashev, V. E. and Zolotukhin, P. and Belanova, A. and Anokhin, A. S. and Zharinov, V. S. and Kaidashev, E. M.},\\n\\tmonth = apr,\\n\\tyear = {2018},\\n\\tpages = {357--363},\\n}\\n\\n\",\"author_short\":[\"Kaydashev, V. E.\",\"Zolotukhin, P.\",\"Belanova, A.\",\"Anokhin, A. S.\",\"Zharinov, V. S.\",\"Kaidashev, E. M.\"],\"key\":\"kaydashev_macroscopic_2018\",\"id\":\"kaydashev_macroscopic_2018\",\"bibbaseid\":\"kaydashev-zolotukhin-belanova-anokhin-zharinov-kaidashev-macroscopicmonolayerofplasmoncoupledgoldnanoparticlesonmirrorforfluorescenceenhancement-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.spiedigitallibrary.org/conference-proceedings-of-spie/10716/107161F/Macroscopic-monolayer-of-plasmon-coupled-gold-nanoparticles-on-mirror-for/10.1117/12.2315071.full\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"SERS of Methylene Blue induced by plasmonic coupled nanoparticle arrays\",\"volume\":\"10716\",\"url\":\"https://www.spiedigitallibrary.org/conference-proceedings-of-spie/10716/107161E/SERS-of-Methylene-Blue-induced-by-plasmonic-coupled-nanoparticle-arrays/10.1117/12.2315007.full\",\"doi\":\"10.1117/12.2315007\",\"abstract\":\"We study the surface enhanced Raman scattering of Methylene Blue (MB) dye molecules induced by large quasihomogeneous arrays of plasmon coupled 5-8 nm Au nanoparticle separated by distances less than 10 nm. Also, the variation of the fluorescence enhancement/SERS properties for as-prepared coupled particles and agglomerated particles obtained upon heat treatment and percolation-like films is analyzed for two measurement protocols, i.e. when measured through the solution and for a monolayer of MB molecules chemisorbed on a surface.\",\"urldate\":\"2023-11-11\",\"booktitle\":\"Saratov Fall Meeting 2017: Optical Technologies in Biophysics and Medicine XIX\",\"publisher\":\"SPIE\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kaydashev\"],\"firstnames\":[\"V.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lyanguzov\"],\"firstnames\":[\"N.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Anokhin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chernishov\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2018\",\"pages\":\"350–356\",\"bibtex\":\"@inproceedings{kaydashev_sers_2018,\\n\\ttitle = {{SERS} of {Methylene} {Blue} induced by plasmonic coupled nanoparticle arrays},\\n\\tvolume = {10716},\\n\\turl = {https://www.spiedigitallibrary.org/conference-proceedings-of-spie/10716/107161E/SERS-of-Methylene-Blue-induced-by-plasmonic-coupled-nanoparticle-arrays/10.1117/12.2315007.full},\\n\\tdoi = {10.1117/12.2315007},\\n\\tabstract = {We study the surface enhanced Raman scattering of Methylene Blue (MB) dye molecules induced by large quasihomogeneous arrays of plasmon coupled 5-8 nm Au nanoparticle separated by distances less than 10 nm. Also, the variation of the fluorescence enhancement/SERS properties for as-prepared coupled particles and agglomerated particles obtained upon heat treatment and percolation-like films is analyzed for two measurement protocols, i.e. when measured through the solution and for a monolayer of MB molecules chemisorbed on a surface.},\\n\\turldate = {2023-11-11},\\n\\tbooktitle = {Saratov {Fall} {Meeting} 2017: {Optical} {Technologies} in {Biophysics} and {Medicine} {XIX}},\\n\\tpublisher = {SPIE},\\n\\tauthor = {Kaydashev, V. E. and Lyanguzov, N. V. and Anokhin, A. S. and Chernishov, A. and Kaidashev, E. M.},\\n\\tmonth = apr,\\n\\tyear = {2018},\\n\\tpages = {350--356},\\n}\\n\\n\",\"author_short\":[\"Kaydashev, V. E.\",\"Lyanguzov, N. V.\",\"Anokhin, A. S.\",\"Chernishov, A.\",\"Kaidashev, E. M.\"],\"key\":\"kaydashev_sers_2018\",\"id\":\"kaydashev_sers_2018\",\"bibbaseid\":\"kaydashev-lyanguzov-anokhin-chernishov-kaidashev-sersofmethyleneblueinducedbyplasmoniccouplednanoparticlearrays-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.spiedigitallibrary.org/conference-proceedings-of-spie/10716/107161E/SERS-of-Methylene-Blue-induced-by-plasmonic-coupled-nanoparticle-arrays/10.1117/12.2315007.full\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Properties of Thin Films of Barium–Strontium Titanate Solid Solutions by Induced Piezoelectric Effect\",\"volume\":\"63\",\"issn\":\"1562-6903\",\"url\":\"https://doi.org/10.1134/S1028335818040092\",\"doi\":\"10.1134/S1028335818040092\",\"abstract\":\"Piezoelectric effect equations have been derived by linearizing the nonlinear equations of state of a thin film existing in a paraelectric phase in the presence of an external electrical field (induced piezoelectric effect). The behavior of the piezoelectric and elastic constants of thin films of a solid barium–strontium titanate solution BST065 (x = 0.65) in a planar field at different misfit strain values has been studied numerically.\",\"language\":\"en\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Doklady Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kalinchuk\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2018\",\"pages\":\"142–146\",\"bibtex\":\"@article{shirokov_properties_2018,\\n\\ttitle = {Properties of {Thin} {Films} of {Barium}–{Strontium} {Titanate} {Solid} {Solutions} by {Induced} {Piezoelectric} {Effect}},\\n\\tvolume = {63},\\n\\tissn = {1562-6903},\\n\\turl = {https://doi.org/10.1134/S1028335818040092},\\n\\tdoi = {10.1134/S1028335818040092},\\n\\tabstract = {Piezoelectric effect equations have been derived by linearizing the nonlinear equations of state of a thin film existing in a paraelectric phase in the presence of an external electrical field (induced piezoelectric effect). The behavior of the piezoelectric and elastic constants of thin films of a solid barium–strontium titanate solution BST065 (x = 0.65) in a planar field at different misfit strain values has been studied numerically.},\\n\\tlanguage = {en},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Doklady Physics},\\n\\tauthor = {Shirokov, V. B. and Kalinchuk, V. V. and Timoshenko, P. E.},\\n\\tmonth = apr,\\n\\tyear = {2018},\\n\\tpages = {142--146},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Kalinchuk, V. V.\",\"Timoshenko, P. E.\"],\"key\":\"shirokov_properties_2018\",\"id\":\"shirokov_properties_2018\",\"bibbaseid\":\"shirokov-kalinchuk-timoshenko-propertiesofthinfilmsofbariumstrontiumtitanatesolidsolutionsbyinducedpiezoelectriceffect-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1028335818040092\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Computational study of the shift of the G band of double-walled carbon nanotubes due to interlayer interactions\",\"volume\":\"97\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.97.165417\",\"doi\":\"10.1103/PhysRevB.97.165417\",\"abstract\":\"The interactions between the layers of double-walled carbon nanotubes induce a measurable shift of the G bands relative to the isolated layers. While experimental data on this shift in freestanding double-walled carbon nanotubes has been reported in the past several years, a comprehensive theoretical description of the observed shift is still lacking. The prediction of this shift is important for supporting the assignment of the measured double-walled nanotubes to particular nanotube types. Here, we report a computational study of the G-band shift as a function of the semiconducting inner layer radius and interlayer separation. We find that with increasing interlayer separation, the G band shift decreases, passes through zero and becomes negative, and further increases in absolute value for the wide range of considered inner layer radii. The theoretical predictions are shown to agree with the available experimental data within the experimental uncertainty.\",\"number\":\"16\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Popov\"],\"firstnames\":[\"Valentin\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Levshov\"],\"firstnames\":[\"Dmitry\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sauvajol\"],\"firstnames\":[\"Jean-Louis\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Paillet\"],\"firstnames\":[\"Matthieu\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2018\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"165417\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\VT7RDBBS\\\\¶opov и др. - 2018 - Computational study of the shift of the G band of .pdf:application/pdf\",\"bibtex\":\"@article{popov_computational_2018,\\n\\ttitle = {Computational study of the shift of the {G} band of double-walled carbon nanotubes due to interlayer interactions},\\n\\tvolume = {97},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.97.165417},\\n\\tdoi = {10.1103/PhysRevB.97.165417},\\n\\tabstract = {The interactions between the layers of double-walled carbon nanotubes induce a measurable shift of the G bands relative to the isolated layers. While experimental data on this shift in freestanding double-walled carbon nanotubes has been reported in the past several years, a comprehensive theoretical description of the observed shift is still lacking. The prediction of this shift is important for supporting the assignment of the measured double-walled nanotubes to particular nanotube types. Here, we report a computational study of the G-band shift as a function of the semiconducting inner layer radius and interlayer separation. We find that with increasing interlayer separation, the G band shift decreases, passes through zero and becomes negative, and further increases in absolute value for the wide range of considered inner layer radii. The theoretical predictions are shown to agree with the available experimental data within the experimental uncertainty.},\\n\\tnumber = {16},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Popov, Valentin N. and Levshov, Dmitry I. and Sauvajol, Jean-Louis and Paillet, Matthieu},\\n\\tmonth = apr,\\n\\tyear = {2018},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {165417},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\VT7RDBBS\\\\\\\\Popov и др. - 2018 - Computational study of the shift of the G band of .pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Popov, V. N.\",\"Levshov, D. I.\",\"Sauvajol, J.\",\"Paillet, M.\"],\"key\":\"popov_computational_2018\",\"id\":\"popov_computational_2018\",\"bibbaseid\":\"popov-levshov-sauvajol-paillet-computationalstudyoftheshiftofthegbandofdoublewalledcarbonnanotubesduetointerlayerinteractions-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.97.165417\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Finite-element analysis of scattering parameters of surface acoustic wave bandpass filter formed on barium titanate thin film\",\"volume\":\"9\",\"issn\":\"1947-5411\",\"url\":\"https://doi.org/10.1080/19475411.2018.1447045\",\"doi\":\"10.1080/19475411.2018.1447045\",\"abstract\":\"The frequency dependence of scattering parameters of interdigital surface acoustic wave transducers placed on ferroelectric barium titanate (BaTiO3) epitaxial film in c-phase coated over magnesium oxide has been studied using the finite-element method (FEM) approach along with the perfectly matched layer (PML) technique. The interdigital transducer which has a comb-like structure with aluminum electrodes excites the mechanical wave. The distance between the fingers allows tuning the frequency properties of the wave propagation. The magnesium oxide is taken as the substrate. The two-dimensional model of two-port surface acoustic wave filter is created to calculate scattering parameters and to show how to design the fixture in COMSOLTM. Some practical computational challenges of finite element modeling of SAW devices in COMSOLTM are shown. The effect of lattice misfit strain on acoustic properties of heterostructures of BaTiO3 epitaxial film in c-phase at room temperature is discussed in present article for two low-frequency surface acoustic resonances.\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"International Journal of Smart and Nano Materials\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"Pavel\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kalinchuk\"],\"firstnames\":[\"Valery\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"Vladimir\",\"B.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2018\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/19475411.2018.1447045\",\"keywords\":\"thin films, ferroelectrics, COMSOL, finite element method (FEM), SAW filters\",\"pages\":\"88–98\",\"file\":\"Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\ÅZMSR86\\\\\\\\Timoshenko и др. - 2018 - Finite-element analysis of scattering parameters o.pdf:application/pdf\",\"bibtex\":\"@article{timoshenko_finite-element_2018,\\n\\ttitle = {Finite-element analysis of scattering parameters of surface acoustic wave bandpass filter formed on barium titanate thin film},\\n\\tvolume = {9},\\n\\tissn = {1947-5411},\\n\\turl = {https://doi.org/10.1080/19475411.2018.1447045},\\n\\tdoi = {10.1080/19475411.2018.1447045},\\n\\tabstract = {The frequency dependence of scattering parameters of interdigital surface acoustic wave transducers placed on ferroelectric barium titanate (BaTiO3) epitaxial film in c-phase coated over magnesium oxide has been studied using the finite-element method (FEM) approach along with the perfectly matched layer (PML) technique. The interdigital transducer which has a comb-like structure with aluminum electrodes excites the mechanical wave. The distance between the fingers allows tuning the frequency properties of the wave propagation. The magnesium oxide is taken as the substrate. The two-dimensional model of two-port surface acoustic wave filter is created to calculate scattering parameters and to show how to design the fixture in COMSOLTM. Some practical computational challenges of finite element modeling of SAW devices in COMSOLTM are shown. The effect of lattice misfit strain on acoustic properties of heterostructures of BaTiO3 epitaxial film in c-phase at room temperature is discussed in present article for two low-frequency surface acoustic resonances.},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {International Journal of Smart and Nano Materials},\\n\\tauthor = {Timoshenko, Pavel E. and Kalinchuk, Valery V. and Shirokov, Vladimir B.},\\n\\tmonth = apr,\\n\\tyear = {2018},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/19475411.2018.1447045},\\n\\tkeywords = {thin films, ferroelectrics, COMSOL, finite element method (FEM), SAW filters},\\n\\tpages = {88--98},\\n\\tfile = {Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\AAZMSR86\\\\\\\\Timoshenko и др. - 2018 - Finite-element analysis of scattering parameters o.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Timoshenko, P. E.\",\"Kalinchuk, V. V.\",\"Shirokov, V. B.\"],\"key\":\"timoshenko_finite-element_2018\",\"id\":\"timoshenko_finite-element_2018\",\"bibbaseid\":\"timoshenko-kalinchuk-shirokov-finiteelementanalysisofscatteringparametersofsurfaceacousticwavebandpassfilterformedonbariumtitanatethinfilm-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/19475411.2018.1447045\"},\"keyword\":[\"thin films\",\"ferroelectrics\",\"COMSOL\",\"finite element method (FEM)\",\"SAW filters\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Large-scale synthesis of ZnO nanostructures by pulse electrochemical method and their photocatalytic properties\",\"volume\":\"76\",\"issn\":\"1369-8001\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S1369800117320528\",\"doi\":\"10.1016/j.mssp.2017.12.011\",\"abstract\":\"In this paper, we report a simple environment-friendly and large-scale approach to synthesis of highly crystalline zinc oxide nanostructures using pulse alternating current (PAC). The morphological results demonstrate flower-like architectures of nanoparticle-based and nanorod-based zinc oxide (ZnO-NPs and ZnO-NRs) obtained in KCl and NaCl as electrolytes. The photocatalytic activity of the obtained materials was performed in methylene blue dye degradation reaction under UV light irradiation. A high efficiency of ~ 90% within 60min with excellent rate constant (k = 0.0386min−1) was observed in the presence of ZnO-NPs synthesized in 2M KCl which is attributed to the larger specific surface area (27m2g−1), total pore volume and more defective structure.\",\"urldate\":\"2023-11-11\",\"journal\":\"Materials Science in Semiconductor Processing\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Ulyankina\"],\"firstnames\":[\"Anna\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Avramenko\"],\"firstnames\":[\"Marina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhigunov\"],\"firstnames\":[\"Denis\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2018\",\"keywords\":\"Electrochemical synthesis, Nanocrystalline materials, Photocatalytic activity, Pulse alternating current, Semiconductors, ZnO\",\"pages\":\"7–13\",\"bibtex\":\"@article{ulyankina_large-scale_2018,\\n\\ttitle = {Large-scale synthesis of {ZnO} nanostructures by pulse electrochemical method and their photocatalytic properties},\\n\\tvolume = {76},\\n\\tissn = {1369-8001},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S1369800117320528},\\n\\tdoi = {10.1016/j.mssp.2017.12.011},\\n\\tabstract = {In this paper, we report a simple environment-friendly and large-scale approach to synthesis of highly crystalline zinc oxide nanostructures using pulse alternating current (PAC). The morphological results demonstrate flower-like architectures of nanoparticle-based and nanorod-based zinc oxide (ZnO-NPs and ZnO-NRs) obtained in KCl and NaCl as electrolytes. The photocatalytic activity of the obtained materials was performed in methylene blue dye degradation reaction under UV light irradiation. A high efficiency of {\\\\textasciitilde} 90\\\\% within 60min with excellent rate constant (k = 0.0386min−1) was observed in the presence of ZnO-NPs synthesized in 2M KCl which is attributed to the larger specific surface area (27m2g−1), total pore volume and more defective structure.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Materials Science in Semiconductor Processing},\\n\\tauthor = {Ulyankina, Anna and Leontyev, Igor and Avramenko, Marina and Zhigunov, Denis and Smirnova, Nina},\\n\\tmonth = mar,\\n\\tyear = {2018},\\n\\tkeywords = {Electrochemical synthesis, Nanocrystalline materials, Photocatalytic activity, Pulse alternating current, Semiconductors, ZnO},\\n\\tpages = {7--13},\\n}\\n\\n\",\"author_short\":[\"Ulyankina, A.\",\"Leontyev, I.\",\"Avramenko, M.\",\"Zhigunov, D.\",\"Smirnova, N.\"],\"key\":\"ulyankina_large-scale_2018\",\"id\":\"ulyankina_large-scale_2018\",\"bibbaseid\":\"ulyankina-leontyev-avramenko-zhigunov-smirnova-largescalesynthesisofznonanostructuresbypulseelectrochemicalmethodandtheirphotocatalyticproperties-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S1369800117320528\"},\"keyword\":[\"Electrochemical synthesis\",\"Nanocrystalline materials\",\"Photocatalytic activity\",\"Pulse alternating current\",\"Semiconductors\",\"ZnO\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Nature of Local Symmetry Violations of Ions in the Magnetic Subsystem of Magnetoplumbite Crystal, According to Raman Scattering Spectroscopy Data\",\"volume\":\"82\",\"issn\":\"1934-9432\",\"url\":\"https://doi.org/10.3103/S1062873818030140\",\"doi\":\"10.3103/S1062873818030140\",\"abstract\":\"The structure of an M-type lead hexaferrite (magnetoplumbite) crystal is studied via the diffraction of synchrotron radiation. The crystal model contains two iron ions positions with dynamic disorder. The dynamics of the crystal lattice in the temperature range of 80 to 775 K is studied by Raman scattering. Particular attention is given to the discussing the nature of the local disorder of iron ions in the trigonal bipyramidal environment of oxygen ions.\",\"language\":\"en\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Bulletin of the Russian Academy of Sciences: Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Anokhin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"E.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"B.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bush\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2018\",\"pages\":\"266–268\",\"bibtex\":\"@article{mikheykin_nature_2018,\\n\\ttitle = {Nature of {Local} {Symmetry} {Violations} of {Ions} in the {Magnetic} {Subsystem} of {Magnetoplumbite} {Crystal}, {According} to {Raman} {Scattering} {Spectroscopy} {Data}},\\n\\tvolume = {82},\\n\\tissn = {1934-9432},\\n\\turl = {https://doi.org/10.3103/S1062873818030140},\\n\\tdoi = {10.3103/S1062873818030140},\\n\\tabstract = {The structure of an M-type lead hexaferrite (magnetoplumbite) crystal is studied via the diffraction of synchrotron radiation. The crystal model contains two iron ions positions with dynamic disorder. The dynamics of the crystal lattice in the temperature range of 80 to 775 K is studied by Raman scattering. Particular attention is given to the discussing the nature of the local disorder of iron ions in the trigonal bipyramidal environment of oxygen ions.},\\n\\tlanguage = {en},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Bulletin of the Russian Academy of Sciences: Physics},\\n\\tauthor = {Mikheykin, A. S. and Anokhin, A. S. and Torgashev, V. I. and Zhukova, E. S. and Gorshunov, B. P. and Prokhorov, A. S. and Bush, A. A.},\\n\\tmonth = mar,\\n\\tyear = {2018},\\n\\tpages = {266--268},\\n}\\n\\n\",\"author_short\":[\"Mikheykin, A. S.\",\"Anokhin, A. S.\",\"Torgashev, V. I.\",\"Zhukova, E. S.\",\"Gorshunov, B. P.\",\"Prokhorov, A. S.\",\"Bush, A. A.\"],\"key\":\"mikheykin_nature_2018\",\"id\":\"mikheykin_nature_2018\",\"bibbaseid\":\"mikheykin-anokhin-torgashev-zhukova-gorshunov-prokhorov-bush-natureoflocalsymmetryviolationsofionsinthemagneticsubsystemofmagnetoplumbitecrystalaccordingtoramanscatteringspectroscopydata-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.3103/S1062873818030140\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Piezoelectric coefficients of the barium-strontium titanate film on a (111)-oriented substrate\",\"volume\":\"324\",\"issn\":\"1757-899X\",\"url\":\"https://dx.doi.org/10.1088/1757-899X/324/1/012006\",\"doi\":\"10.1088/1757-899X/324/1/012006\",\"abstract\":\"Within the framework of the phenomenological theory of phase transitions, we consider properties of the Ba0.8Sr0.2TiO3 (BST80) film grown on a (111)-oriented cubic substrate. The film was revealed to exhibit three ferroelectric phases with different orientations of spontaneous polarization. It is shown that some piezoelectric moduli should demonstrate anomalous behavior near the phase boundaries.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"IOP Conference Series: Materials Science and Engineering\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shakhovoy\"],\"firstnames\":[\"R.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pan’kin\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kalinchuk\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2018\",\"note\":\"Publisher: IOP Publishing\",\"pages\":\"012006\",\"file\":\"IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\74MIZ5W7\\\\§hirokov и др. - 2018 - Piezoelectric coefficients of the barium-strontium.pdf:application/pdf\",\"bibtex\":\"@article{shirokov_piezoelectric_2018,\\n\\ttitle = {Piezoelectric coefficients of the barium-strontium titanate film on a (111)-oriented substrate},\\n\\tvolume = {324},\\n\\tissn = {1757-899X},\\n\\turl = {https://dx.doi.org/10.1088/1757-899X/324/1/012006},\\n\\tdoi = {10.1088/1757-899X/324/1/012006},\\n\\tabstract = {Within the framework of the phenomenological theory of phase transitions, we consider properties of the Ba0.8Sr0.2TiO3 (BST80) film grown on a (111)-oriented cubic substrate. The film was revealed to exhibit three ferroelectric phases with different orientations of spontaneous polarization. It is shown that some piezoelectric moduli should demonstrate anomalous behavior near the phase boundaries.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {IOP Conference Series: Materials Science and Engineering},\\n\\tauthor = {Shirokov, V. B. and Shakhovoy, R. A. and Pan’kin, A. V. and Kalinchuk, V. V.},\\n\\tmonth = mar,\\n\\tyear = {2018},\\n\\tnote = {Publisher: IOP Publishing},\\n\\tpages = {012006},\\n\\tfile = {IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\74MIZ5W7\\\\\\\\Shirokov и др. - 2018 - Piezoelectric coefficients of the barium-strontium.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Shakhovoy, R. A.\",\"Pan’kin, A. V.\",\"Kalinchuk, V. V.\"],\"key\":\"shirokov_piezoelectric_2018\",\"id\":\"shirokov_piezoelectric_2018\",\"bibbaseid\":\"shirokov-shakhovoy-pankin-kalinchuk-piezoelectriccoefficientsofthebariumstrontiumtitanatefilmona111orientedsubstrate-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/1757-899X/324/1/012006\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"address\":\"Cham\",\"series\":\"Springer Proceedings in Physics\",\"title\":\"Growth and Study of Zinc Oxide Nanorods Arrays on Piezoelectric Substrates\",\"isbn\":\"978-3-319-78919-4\",\"doi\":\"10.1007/978-3-319-78919-4_2\",\"abstract\":\"Our studies have shown the possibility of using the thermal synthesisSynthesismethod from Zn vapors to obtain ZnO nanorodsZnO nanorods (ZnO NRs)arrays as a sensitive element for UV radiation SAW sensors. The piezoelectricPiezoelectricproperties of the LiNbO3 substrate typically degrade upon nanorods growth at elevated temperature. This limitation is solved by using additional annealing of prepared structureStructureat 550 °C in an oxygen atmosphere. The obtained ZnO NRs were investigated by scanning electron microscopy and photoluminescence.\",\"language\":\"en\",\"booktitle\":\"Advanced Materials\",\"publisher\":\"Springer International Publishing\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Zhilin\"],\"firstnames\":[\"D.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Karapetyan\"],\"firstnames\":[\"G.\",\"Y.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kutepov\"],\"firstnames\":[\"M.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Minasyan\"],\"firstnames\":[\"T.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yatsenko\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]}],\"editor\":[{\"propositions\":[],\"lastnames\":[\"Parinov\"],\"firstnames\":[\"Ivan\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chang\"],\"firstnames\":[\"Shun-Hsyung\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gupta\"],\"firstnames\":[\"Vijay\",\"K.\"],\"suffixes\":[]}],\"year\":\"2018\",\"keywords\":\"Carbothermal Method, LiNbO3 Substrate, structureStructure, synthesisSynthesis, Zinc Oxide Nanorod Arrays\",\"pages\":\"25–31\",\"bibtex\":\"@inproceedings{zhilin_growth_2018,\\n\\taddress = {Cham},\\n\\tseries = {Springer {Proceedings} in {Physics}},\\n\\ttitle = {Growth and {Study} of {Zinc} {Oxide} {Nanorods} {Arrays} on {Piezoelectric} {Substrates}},\\n\\tisbn = {978-3-319-78919-4},\\n\\tdoi = {10.1007/978-3-319-78919-4_2},\\n\\tabstract = {Our studies have shown the possibility of using the thermal synthesisSynthesismethod from Zn vapors to obtain ZnO nanorodsZnO nanorods (ZnO NRs)arrays as a sensitive element for UV radiation SAW sensors. The piezoelectricPiezoelectricproperties of the LiNbO3 substrate typically degrade upon nanorods growth at elevated temperature. This limitation is solved by using additional annealing of prepared structureStructureat 550 °C in an oxygen atmosphere. The obtained ZnO NRs were investigated by scanning electron microscopy and photoluminescence.},\\n\\tlanguage = {en},\\n\\tbooktitle = {Advanced {Materials}},\\n\\tpublisher = {Springer International Publishing},\\n\\tauthor = {Zhilin, D. A. and Karapetyan, G. Y. and Kutepov, M. E. and Minasyan, T. A. and Yatsenko, V. I. and Kaidashev, E. M.},\\n\\teditor = {Parinov, Ivan A. and Chang, Shun-Hsyung and Gupta, Vijay K.},\\n\\tyear = {2018},\\n\\tkeywords = {Carbothermal Method, LiNbO3 Substrate, structureStructure, synthesisSynthesis, Zinc Oxide Nanorod Arrays},\\n\\tpages = {25--31},\\n}\\n\\n\",\"author_short\":[\"Zhilin, D. A.\",\"Karapetyan, G. Y.\",\"Kutepov, M. E.\",\"Minasyan, T. A.\",\"Yatsenko, V. I.\",\"Kaidashev, E. M.\"],\"editor_short\":[\"Parinov, I. A.\",\"Chang, S.\",\"Gupta, V. K.\"],\"key\":\"zhilin_growth_2018\",\"id\":\"zhilin_growth_2018\",\"bibbaseid\":\"zhilin-karapetyan-kutepov-minasyan-yatsenko-kaidashev-growthandstudyofzincoxidenanorodsarraysonpiezoelectricsubstrates-2018\",\"role\":\"author\",\"urls\":{},\"keyword\":[\"Carbothermal Method\",\"LiNbO3 Substrate\",\"structureStructure\",\"synthesisSynthesis\",\"Zinc Oxide Nanorod Arrays\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"In Situ Investigation of Non-Isothermal Decomposition of Pt Acetylacetonate as One-Step Size-Controlled Synthesis of Pt Nanoparticles\",\"volume\":\"215\",\"copyright\":\"© 2018 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim\",\"issn\":\"1862-6319\",\"url\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssa.201800488\",\"doi\":\"10.1002/pssa.201800488\",\"abstract\":\"Interest in the development of state-of-the-art methods for synthesis of Pt nanoparticles is dictated by both unique properties of platinum itself and the wide range of platinum nanoparticles applications. Platinum acetylacetonate and platinum nanoparticles produced by the thermal decomposition of Pt(acac)2 are studied via in situ X-ray diffraction and Raman spectroscopy, thermal gravimetry, scanning (SEM), and transmission electronic microscopy (TEM). The experiments are made at heating rates of 1 and 5 K min−1. A comparative analysis of SEM, TEM, and XRD data highlights the formation of coarse Pt particles with sizes of ≈60–160 nm, which are composed of nanoparticles with dimensions of 1.9 and 4.1 nm for 1 K min−1- and 5 K min−1-heating rates, respectively. The desirable average size of nanoparticles upon their synthesis can thus be achieved by a simple tuning of the heating rate of acetylacetate thermal decomposition. The present results open up the possibility to use a trivial non-isothermal thermal decomposition method in the synthesis of both supported and unsupported nanoparticles of predetermined size for other chemical elements such as Pd, Ni, Co, etc. from their acetylacetonates.\",\"language\":\"en\",\"number\":\"23\",\"urldate\":\"2023-11-11\",\"journal\":\"physica status solidi (a)\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kulbakov\"],\"firstnames\":[\"Anton\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Allix\"],\"firstnames\":[\"Mathieu\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rakhmatullin\"],\"firstnames\":[\"Aydar\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"Alexey\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Popov\"],\"firstnames\":[\"Yuri\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"Olga\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\",\"N.\"],\"suffixes\":[]}],\"year\":\"2018\",\"note\":\"_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssa.201800488\",\"keywords\":\"in situ characterizations, platinum acetylacetonate, Pt nanoparticles, thermal decomposition\",\"pages\":\"1800488\",\"bibtex\":\"@article{kulbakov_situ_2018,\\n\\ttitle = {In {Situ} {Investigation} of {Non}-{Isothermal} {Decomposition} of {Pt} {Acetylacetonate} as {One}-{Step} {Size}-{Controlled} {Synthesis} of {Pt} {Nanoparticles}},\\n\\tvolume = {215},\\n\\tcopyright = {© 2018 WILEY-VCH Verlag GmbH \\\\& Co. KGaA, Weinheim},\\n\\tissn = {1862-6319},\\n\\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssa.201800488},\\n\\tdoi = {10.1002/pssa.201800488},\\n\\tabstract = {Interest in the development of state-of-the-art methods for synthesis of Pt nanoparticles is dictated by both unique properties of platinum itself and the wide range of platinum nanoparticles applications. Platinum acetylacetonate and platinum nanoparticles produced by the thermal decomposition of Pt(acac)2 are studied via in situ X-ray diffraction and Raman spectroscopy, thermal gravimetry, scanning (SEM), and transmission electronic microscopy (TEM). The experiments are made at heating rates of 1 and 5 K min−1. A comparative analysis of SEM, TEM, and XRD data highlights the formation of coarse Pt particles with sizes of ≈60–160 nm, which are composed of nanoparticles with dimensions of 1.9 and 4.1 nm for 1 K min−1- and 5 K min−1-heating rates, respectively. The desirable average size of nanoparticles upon their synthesis can thus be achieved by a simple tuning of the heating rate of acetylacetate thermal decomposition. The present results open up the possibility to use a trivial non-isothermal thermal decomposition method in the synthesis of both supported and unsupported nanoparticles of predetermined size for other chemical elements such as Pd, Ni, Co, etc. from their acetylacetonates.},\\n\\tlanguage = {en},\\n\\tnumber = {23},\\n\\turldate = {2023-11-11},\\n\\tjournal = {physica status solidi (a)},\\n\\tauthor = {Kulbakov, Anton A. and Allix, Mathieu and Rakhmatullin, Aydar and Mikheykin, Alexey S. and Popov, Yuri V. and Smirnova, Nina V. and Maslova, Olga and Leontyev, Igor N.},\\n\\tyear = {2018},\\n\\tnote = {\\\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssa.201800488},\\n\\tkeywords = {in situ characterizations, platinum acetylacetonate, Pt nanoparticles, thermal decomposition},\\n\\tpages = {1800488},\\n}\\n\\n\",\"author_short\":[\"Kulbakov, A. A.\",\"Allix, M.\",\"Rakhmatullin, A.\",\"Mikheykin, A. S.\",\"Popov, Y. V.\",\"Smirnova, N. V.\",\"Maslova, O.\",\"Leontyev, I. N.\"],\"key\":\"kulbakov_situ_2018\",\"id\":\"kulbakov_situ_2018\",\"bibbaseid\":\"kulbakov-allix-rakhmatullin-mikheykin-popov-smirnova-maslova-leontyev-insituinvestigationofnonisothermaldecompositionofptacetylacetonateasonestepsizecontrolledsynthesisofptnanoparticles-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssa.201800488\"},\"keyword\":[\"in situ characterizations\",\"platinum acetylacetonate\",\"Pt nanoparticles\",\"thermal decomposition\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Influence of Carbon Support on Catalytic Layer Performance of Proton Exchange Membrane Fuel Cells\",\"volume\":\"9\",\"issn\":\"1868-5994\",\"url\":\"https://doi.org/10.1007/s12678-017-0416-4\",\"doi\":\"10.1007/s12678-017-0416-4\",\"abstract\":\"Pt-based catalysts supported onto various carbon nanotubes (CNTs) and carbon black Vulcan XC-72 have been studied in this work. The samples have been prepared via electrochemical dispersion technique. The carbon nanotubes exhibit the mesoporous morphology with the pore size of 5—30 nm, while Vulcan XC-72 support exhibits a microporous structure. The agglomeration of Pt particles (5—7 nm) is found to be more extended at the carbon nanotubes compared to the carbon black. The examination of the synthesized catalysts in a catalytic membrane electrode assembly layer reveals that CNTs favor a power density higher than in the carbon black support owing to a more suitable porous structure of the catalyst layer. Moreover, the maximum characteristics of membrane electrode assembly are obtained for few-walled carbon nanotubes with a broad carbon having size distribution.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Electrocatalysis\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Novikova\"],\"firstnames\":[\"Ksenia\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"Alexandra\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gerasimova\"],\"firstnames\":[\"Ekaterina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"Olga\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rakhmatullin\"],\"firstnames\":[\"Aydar\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dobrovolsky\"],\"firstnames\":[\"Yuri\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2018\",\"keywords\":\"Carbon nanotubes, Carbon support, Catalytic layer structure, PEM fuel cell, Pt/C\",\"pages\":\"22–30\",\"bibtex\":\"@article{novikova_influence_2018,\\n\\ttitle = {Influence of {Carbon} {Support} on {Catalytic} {Layer} {Performance} of {Proton} {Exchange} {Membrane} {Fuel} {Cells}},\\n\\tvolume = {9},\\n\\tissn = {1868-5994},\\n\\turl = {https://doi.org/10.1007/s12678-017-0416-4},\\n\\tdoi = {10.1007/s12678-017-0416-4},\\n\\tabstract = {Pt-based catalysts supported onto various carbon nanotubes (CNTs) and carbon black Vulcan XC-72 have been studied in this work. The samples have been prepared via electrochemical dispersion technique. The carbon nanotubes exhibit the mesoporous morphology with the pore size of 5—30 nm, while Vulcan XC-72 support exhibits a microporous structure. The agglomeration of Pt particles (5—7 nm) is found to be more extended at the carbon nanotubes compared to the carbon black. The examination of the synthesized catalysts in a catalytic membrane electrode assembly layer reveals that CNTs favor a power density higher than in the carbon black support owing to a more suitable porous structure of the catalyst layer. Moreover, the maximum characteristics of membrane electrode assembly are obtained for few-walled carbon nanotubes with a broad carbon having size distribution.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Electrocatalysis},\\n\\tauthor = {Novikova, Ksenia and Kuriganova, Alexandra and Leontyev, Igor and Gerasimova, Ekaterina and Maslova, Olga and Rakhmatullin, Aydar and Smirnova, Nina and Dobrovolsky, Yuri},\\n\\tmonth = jan,\\n\\tyear = {2018},\\n\\tkeywords = {Carbon nanotubes, Carbon support, Catalytic layer structure, PEM fuel cell, Pt/C},\\n\\tpages = {22--30},\\n}\\n\\n\",\"author_short\":[\"Novikova, K.\",\"Kuriganova, A.\",\"Leontyev, I.\",\"Gerasimova, E.\",\"Maslova, O.\",\"Rakhmatullin, A.\",\"Smirnova, N.\",\"Dobrovolsky, Y.\"],\"key\":\"novikova_influence_2018\",\"id\":\"novikova_influence_2018\",\"bibbaseid\":\"novikova-kuriganova-leontyev-gerasimova-maslova-rakhmatullin-smirnova-dobrovolsky-influenceofcarbonsupportoncatalyticlayerperformanceofprotonexchangemembranefuelcells-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1007/s12678-017-0416-4\"},\"keyword\":[\"Carbon nanotubes\",\"Carbon support\",\"Catalytic layer structure\",\"PEM fuel cell\",\"Pt/C\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"On the Evaluation of the Average Crystalline Size and Surface Area of Platinum Catalyst Nanoparticles\",\"volume\":\"255\",\"copyright\":\"© 2018 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim\",\"issn\":\"1521-3951\",\"url\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201800240\",\"doi\":\"10.1002/pssb.201800240\",\"abstract\":\"In the present work, the effect of grain size distribution on the diffraction profile shape is inspected via analysis of the mutual ratio of Lorentz and Gauss components in pseudo-Voigt function which is used for simulating X-ray profiles of nanoparticles. As established from the plotted dependences, the error in the average Pt nanoparticles size determination reaches 56% and the discrepancy between calculated Pt nanoparticle surface areas attains 60%. Furthermore, the determination error becomes greater with increasing the Lorentz contribution to pseudo-Voigt function, or, in fact, with enlarging particle size distribution. The empirically found electrochemical surface area of Pt/C electrocatalyst is compared with that evaluated from XRD data using the Scherrer formula and particle size distribution data analysis.\",\"language\":\"en\",\"number\":\"10\",\"urldate\":\"2023-11-11\",\"journal\":\"physica status solidi (b)\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"Alexandra\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Allix\"],\"firstnames\":[\"Mathieu\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rakhmatullin\"],\"firstnames\":[\"Aydar\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"Pavel\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"Olga\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"Alexey\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\",\"V.\"],\"suffixes\":[]}],\"year\":\"2018\",\"note\":\"_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201800240\",\"keywords\":\"X-ray diffraction, Pt/C, average nanoparticle size, catalysts, specific surface area\",\"pages\":\"1800240\",\"bibtex\":\"@article{leontyev_evaluation_2018,\\n\\ttitle = {On the {Evaluation} of the {Average} {Crystalline} {Size} and {Surface} {Area} of {Platinum} {Catalyst} {Nanoparticles}},\\n\\tvolume = {255},\\n\\tcopyright = {© 2018 WILEY-VCH Verlag GmbH \\\\& Co. KGaA, Weinheim},\\n\\tissn = {1521-3951},\\n\\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201800240},\\n\\tdoi = {10.1002/pssb.201800240},\\n\\tabstract = {In the present work, the effect of grain size distribution on the diffraction profile shape is inspected via analysis of the mutual ratio of Lorentz and Gauss components in pseudo-Voigt function which is used for simulating X-ray profiles of nanoparticles. As established from the plotted dependences, the error in the average Pt nanoparticles size determination reaches 56\\\\% and the discrepancy between calculated Pt nanoparticle surface areas attains 60\\\\%. Furthermore, the determination error becomes greater with increasing the Lorentz contribution to pseudo-Voigt function, or, in fact, with enlarging particle size distribution. The empirically found electrochemical surface area of Pt/C electrocatalyst is compared with that evaluated from XRD data using the Scherrer formula and particle size distribution data analysis.},\\n\\tlanguage = {en},\\n\\tnumber = {10},\\n\\turldate = {2023-11-11},\\n\\tjournal = {physica status solidi (b)},\\n\\tauthor = {Leontyev, Igor N. and Kuriganova, Alexandra B. and Allix, Mathieu and Rakhmatullin, Aydar and Timoshenko, Pavel E. and Maslova, Olga A. and Mikheykin, Alexey S. and Smirnova, Nina V.},\\n\\tyear = {2018},\\n\\tnote = {\\\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201800240},\\n\\tkeywords = {X-ray diffraction, Pt/C, average nanoparticle size, catalysts, specific surface area},\\n\\tpages = {1800240},\\n}\\n\\n\",\"author_short\":[\"Leontyev, I. N.\",\"Kuriganova, A. B.\",\"Allix, M.\",\"Rakhmatullin, A.\",\"Timoshenko, P. E.\",\"Maslova, O. A.\",\"Mikheykin, A. S.\",\"Smirnova, N. V.\"],\"key\":\"leontyev_evaluation_2018\",\"id\":\"leontyev_evaluation_2018\",\"bibbaseid\":\"leontyev-kuriganova-allix-rakhmatullin-timoshenko-maslova-mikheykin-smirnova-ontheevaluationoftheaveragecrystallinesizeandsurfaceareaofplatinumcatalystnanoparticles-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201800240\"},\"keyword\":[\"X-ray diffraction\",\"Pt/C\",\"average nanoparticle size\",\"catalysts\",\"specific surface area\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Commensurability between protein nanotubes in contractile ejection nanomachines\",\"volume\":\"10\",\"issn\":\"2040-3372\",\"url\":\"https://pubs.rsc.org/en/content/articlelanding/2018/nr/c7nr06940e\",\"doi\":\"10.1039/C7NR06940E\",\"abstract\":\"Contractile ejection nanomachines being sheath–tube assemblies create an opening in the cell membrane to translocate molecules or ions across it. Here, on the most structurally investigated examples of the bacteriophage T4 tail and pyocin R2, we show that the rearrangement of the sheath structure resulting in its contraction and twist occurs in such a way that the contracted sheath becomes commensurate with the inner tube. This fact dictates the previously unknown simple geometrical relationship between the nanotube symmetries. Using the Frank and van der Merwe classical theory of commensurability, we study an interaction between two protein nanotubes forming such nanomachines and obtain an expression for the corresponding energy, which depends on the tube structures and their mutual arrangement. The appearance of commensurability between the contracted sheath and the inner tube decreases both the interaction energy and the total energy of the system. It improves the nanomachine efficiency, since the energy gain obtained increases the torque of the inner tube piercing the cell membrane.\",\"language\":\"en\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Nanoscale\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergey\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Roshal\"],\"firstnames\":[\"Daria\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Myasnikova\"],\"firstnames\":[\"Anna\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorman\"],\"firstnames\":[\"Vladimir\",\"L.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2018\",\"note\":\"Publisher: The Royal Society of Chemistry\",\"pages\":\"758–764\",\"file\":\"Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\J2A5BG4M\\\\\\\\Rochal и др. - 2018 - Commensurability between protein nanotubes in cont.pdf:application/pdf;Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\TABA9EAQ\\\\\\\\Rochal и др. - 2018 - Commensurability between protein nanotubes in cont.pdf:application/pdf\",\"bibtex\":\"@article{rochal_commensurability_2018,\\n\\ttitle = {Commensurability between protein nanotubes in contractile ejection nanomachines},\\n\\tvolume = {10},\\n\\tissn = {2040-3372},\\n\\turl = {https://pubs.rsc.org/en/content/articlelanding/2018/nr/c7nr06940e},\\n\\tdoi = {10.1039/C7NR06940E},\\n\\tabstract = {Contractile ejection nanomachines being sheath–tube assemblies create an opening in the cell membrane to translocate molecules or ions across it. Here, on the most structurally investigated examples of the bacteriophage T4 tail and pyocin R2, we show that the rearrangement of the sheath structure resulting in its contraction and twist occurs in such a way that the contracted sheath becomes commensurate with the inner tube. This fact dictates the previously unknown simple geometrical relationship between the nanotube symmetries. Using the Frank and van der Merwe classical theory of commensurability, we study an interaction between two protein nanotubes forming such nanomachines and obtain an expression for the corresponding energy, which depends on the tube structures and their mutual arrangement. The appearance of commensurability between the contracted sheath and the inner tube decreases both the interaction energy and the total energy of the system. It improves the nanomachine efficiency, since the energy gain obtained increases the torque of the inner tube piercing the cell membrane.},\\n\\tlanguage = {en},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Nanoscale},\\n\\tauthor = {Rochal, Sergey B. and Roshal, Daria S. and Myasnikova, Anna E. and Lorman, Vladimir L.},\\n\\tmonth = jan,\\n\\tyear = {2018},\\n\\tnote = {Publisher: The Royal Society of Chemistry},\\n\\tpages = {758--764},\\n\\tfile = {Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\J2A5BG4M\\\\\\\\Rochal и др. - 2018 - Commensurability between protein nanotubes in cont.pdf:application/pdf;Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\TABA9EAQ\\\\\\\\Rochal и др. - 2018 - Commensurability between protein nanotubes in cont.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Rochal, S. B.\",\"Roshal, D. S.\",\"Myasnikova, A. E.\",\"Lorman, V. L.\"],\"key\":\"rochal_commensurability_2018\",\"id\":\"rochal_commensurability_2018\",\"bibbaseid\":\"rochal-roshal-myasnikova-lorman-commensurabilitybetweenproteinnanotubesincontractileejectionnanomachines-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://pubs.rsc.org/en/content/articlelanding/2018/nr/c7nr06940e\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"series\":\"Semiconductor materials for green energy and environmental applications\",\"title\":\"Copper oxides for energy storage application: Novel pulse alternating current synthesis\",\"volume\":\"73\",\"issn\":\"1369-8001\",\"shorttitle\":\"Copper oxides for energy storage application\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S1369800117313975\",\"doi\":\"10.1016/j.mssp.2017.08.001\",\"abstract\":\"Copper oxide powders (CuOx) were reported to be electrochemically obtained under pulse alternating current by a facile and inexpensive one-pot method. The effect of the synthesis conditions on the copper electrode oxidation rate and product morphology and composition was studied. The CuOx products were characterized by X-ray powder diffraction (XRD), Raman spectroscopy, X-ray absorption near-edge structure (XANES) spectroscopy, energy dispersive spectroscopy (EDS), scanning electron microscopy (SEM) and transmission electron microscopy (TEM). Depending on the synthesis conditions, the powders reveal different morphologies and composition, such as Cu2O octahedra, Cu2O decorated with CuO or Cu2O-CuO bilayered composite. Cyclic voltammetry and charge-discharge measurements were used to study the electrochemical energy conversion properties of the materials. The results of the electrocatalytic study indicate that the powder with Cu2O-CuO bilayered polyhedra is suitable for use in methanol oxidation; and the powder with Cu2O octahedra has shown a good specific capacitance for supercapacitors.\",\"urldate\":\"2023-11-11\",\"journal\":\"Materials Science in Semiconductor Processing\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Ulyankina\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"O.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Allix\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rakhmatullin\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nevzorova\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Valeev\"],\"firstnames\":[\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yalovega\"],\"firstnames\":[\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"N.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2018\",\"pages\":\"111–116\",\"bibtex\":\"@article{ulyankina_copper_2018,\\n\\tseries = {Semiconductor materials for green energy and environmental applications},\\n\\ttitle = {Copper oxides for energy storage application: {Novel} pulse alternating current synthesis},\\n\\tvolume = {73},\\n\\tissn = {1369-8001},\\n\\tshorttitle = {Copper oxides for energy storage application},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S1369800117313975},\\n\\tdoi = {10.1016/j.mssp.2017.08.001},\\n\\tabstract = {Copper oxide powders (CuOx) were reported to be electrochemically obtained under pulse alternating current by a facile and inexpensive one-pot method. The effect of the synthesis conditions on the copper electrode oxidation rate and product morphology and composition was studied. The CuOx products were characterized by X-ray powder diffraction (XRD), Raman spectroscopy, X-ray absorption near-edge structure (XANES) spectroscopy, energy dispersive spectroscopy (EDS), scanning electron microscopy (SEM) and transmission electron microscopy (TEM). Depending on the synthesis conditions, the powders reveal different morphologies and composition, such as Cu2O octahedra, Cu2O decorated with CuO or Cu2O-CuO bilayered composite. Cyclic voltammetry and charge-discharge measurements were used to study the electrochemical energy conversion properties of the materials. The results of the electrocatalytic study indicate that the powder with Cu2O-CuO bilayered polyhedra is suitable for use in methanol oxidation; and the powder with Cu2O octahedra has shown a good specific capacitance for supercapacitors.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Materials Science in Semiconductor Processing},\\n\\tauthor = {Ulyankina, A. and Leontyev, I. and Maslova, O. and Allix, M. and Rakhmatullin, A. and Nevzorova, N. and Valeev, R. and Yalovega, G. and Smirnova, N.},\\n\\tmonth = jan,\\n\\tyear = {2018},\\n\\tpages = {111--116},\\n}\\n\\n\",\"author_short\":[\"Ulyankina, A.\",\"Leontyev, I.\",\"Maslova, O.\",\"Allix, M.\",\"Rakhmatullin, A.\",\"Nevzorova, N.\",\"Valeev, R.\",\"Yalovega, G.\",\"Smirnova, N.\"],\"key\":\"ulyankina_copper_2018\",\"id\":\"ulyankina_copper_2018\",\"bibbaseid\":\"ulyankina-leontyev-maslova-allix-rakhmatullin-nevzorova-valeev-yalovega-etal-copperoxidesforenergystorageapplicationnovelpulsealternatingcurrentsynthesis-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S1369800117313975\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Photoluminescence from an individual double-walled carbon nanotube\",\"volume\":\"96\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.96.195410\",\"doi\":\"10.1103/PhysRevB.96.195410\",\"abstract\":\"We report direct and unambiguous evidence of the existence of inner semiconducting tube (ISCT) photoluminescence (PL) from measurements performed on four individual freestanding index-identified double-walled carbon nanotubes (DWNTs). Based on thorough Rayleigh scattering, Raman scattering, and PL experiments, we are able to demonstrate that the ISCT PL is observed with a quantum yield estimated to be a few 10−6 independent of the semiconducting or metallic nature of the outer tube. This result is mainly attributed to ultrafast exciton transfer from the inner to outer tube. Furthermore, by carrying out PL excitation experiments on the (14,1)@(15,12) DWNT, we show that the ISCT PL can be detected through the optical excitation of the outer tube, indicating that the exciton transfer can also occur in the opposite way.\",\"number\":\"19\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Levshov\"],\"firstnames\":[\"Dmitry\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Parret\"],\"firstnames\":[\"Romain\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tran\"],\"firstnames\":[\"Huy-Nam\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Michel\"],\"firstnames\":[\"Thierry\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Cao\"],\"firstnames\":[\"Thi\",\"Thanh\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nguyen\"],\"firstnames\":[\"Van\",\"Chuc\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Arenal\"],\"firstnames\":[\"Raul\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Popov\"],\"firstnames\":[\"Valentin\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergei\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sauvajol\"],\"firstnames\":[\"Jean-Louis\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zahab\"],\"firstnames\":[\"Ahmed-Azmi\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Paillet\"],\"firstnames\":[\"Matthieu\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2017\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"195410\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\6UGH2Z3Z\\\\Łevshov и др. - 2017 - Photoluminescence from an individual double-walled.pdf:application/pdf;APS Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\4XVAB652\\\\¶hysRevB.96.html:text/html\",\"bibtex\":\"@article{levshov_photoluminescence_2017,\\n\\ttitle = {Photoluminescence from an individual double-walled carbon nanotube},\\n\\tvolume = {96},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.96.195410},\\n\\tdoi = {10.1103/PhysRevB.96.195410},\\n\\tabstract = {We report direct and unambiguous evidence of the existence of inner semiconducting tube (ISCT) photoluminescence (PL) from measurements performed on four individual freestanding index-identified double-walled carbon nanotubes (DWNTs). Based on thorough Rayleigh scattering, Raman scattering, and PL experiments, we are able to demonstrate that the ISCT PL is observed with a quantum yield estimated to be a few 10−6 independent of the semiconducting or metallic nature of the outer tube. This result is mainly attributed to ultrafast exciton transfer from the inner to outer tube. Furthermore, by carrying out PL excitation experiments on the (14,1)@(15,12) DWNT, we show that the ISCT PL can be detected through the optical excitation of the outer tube, indicating that the exciton transfer can also occur in the opposite way.},\\n\\tnumber = {19},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Levshov, Dmitry I. and Parret, Romain and Tran, Huy-Nam and Michel, Thierry and Cao, Thi Thanh and Nguyen, Van Chuc and Arenal, Raul and Popov, Valentin N. and Rochal, Sergei B. and Sauvajol, Jean-Louis and Zahab, Ahmed-Azmi and Paillet, Matthieu},\\n\\tmonth = nov,\\n\\tyear = {2017},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {195410},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\6UGH2Z3Z\\\\\\\\Levshov и др. - 2017 - Photoluminescence from an individual double-walled.pdf:application/pdf;APS Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\4XVAB652\\\\\\\\PhysRevB.96.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Levshov, D. I.\",\"Parret, R.\",\"Tran, H.\",\"Michel, T.\",\"Cao, T. T.\",\"Nguyen, V. C.\",\"Arenal, R.\",\"Popov, V. N.\",\"Rochal, S. B.\",\"Sauvajol, J.\",\"Zahab, A.\",\"Paillet, M.\"],\"key\":\"levshov_photoluminescence_2017\",\"id\":\"levshov_photoluminescence_2017\",\"bibbaseid\":\"levshov-parret-tran-michel-cao-nguyen-arenal-popov-etal-photoluminescencefromanindividualdoublewalledcarbonnanotube-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.96.195410\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Observation of dielectric universalities in albumin, cytochrome C and Shewanella oneidensis MR-1 extracellular matrix\",\"volume\":\"7\",\"copyright\":\"2017 The Author(s)\",\"issn\":\"2045-2322\",\"url\":\"https://www.nature.com/articles/s41598-017-15693-y\",\"doi\":\"10.1038/s41598-017-15693-y\",\"abstract\":\"The electrodynamics of metals is well understood within the Drude conductivity model; properties of insulators and semiconductors are governed by a gap in the electronic states. But there is a great variety of disordered materials that do not fall in these categories and still respond to external field in an amazingly uniform manner. At radiofrequencies delocalized charges yield a frequency-independent conductivity σ1(ν) whose magnitude exponentially decreases while cooling. With increasing frequency, dispersionless conductivity starts to reveal a power-law dependence σ1(ν)∝νswith s \\\\textless 1 caused by hopping charge carriers. At low temperatures, such Universal Dielectric Response can cross over to another universal regime with nearly constant loss ε″∝σ1/ν = const. The powerful research potential based on such universalities is widely used in condensed matter physics. Here we study the broad-band (1–1012 Hz) dielectric response of Shewanella oneidensis MR-1 extracellular matrix, cytochrome C and serum albumin. Applying concepts of condensed matter physics, we identify transport mechanisms and a number of energy, time, frequency, spatial and temperature scales in these biological objects, which can provide us with deeper insight into the protein dynamics.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Scientific Reports\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Motovilov\"],\"firstnames\":[\"K.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Savinov\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"E.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pronin\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gagkaeva\"],\"firstnames\":[\"Z.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grinenko\"],\"firstnames\":[\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sidoruk\"],\"firstnames\":[\"K.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Voeikova\"],\"firstnames\":[\"T.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Barzilovich\"],\"firstnames\":[\"P.\",\"Yu\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grebenko\"],\"firstnames\":[\"A.\",\"K.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lisovskii\"],\"firstnames\":[\"S.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bednyakov\"],\"firstnames\":[\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pokorný\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"B.\",\"P.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2017\",\"note\":\"Number: 1 Publisher: Nature Publishing Group\",\"keywords\":\"Biomaterials – proteins, Polymers\",\"pages\":\"15731\",\"file\":\"Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\4QFUHD76\\\\\\\\Motovilov и др. - 2017 - Observation of dielectric universalities in albumi.pdf:application/pdf\",\"bibtex\":\"@article{motovilov_observation_2017,\\n\\ttitle = {Observation of dielectric universalities in albumin, cytochrome {C} and {Shewanella} oneidensis {MR}-1 extracellular matrix},\\n\\tvolume = {7},\\n\\tcopyright = {2017 The Author(s)},\\n\\tissn = {2045-2322},\\n\\turl = {https://www.nature.com/articles/s41598-017-15693-y},\\n\\tdoi = {10.1038/s41598-017-15693-y},\\n\\tabstract = {The electrodynamics of metals is well understood within the Drude conductivity model; properties of insulators and semiconductors are governed by a gap in the electronic states. But there is a great variety of disordered materials that do not fall in these categories and still respond to external field in an amazingly uniform manner. At radiofrequencies delocalized charges yield a frequency-independent conductivity σ1(ν) whose magnitude exponentially decreases while cooling. With increasing frequency, dispersionless conductivity starts to reveal a power-law dependence σ1(ν)∝νswith s {\\\\textless} 1 caused by hopping charge carriers. At low temperatures, such Universal Dielectric Response can cross over to another universal regime with nearly constant loss ε″∝σ1/ν = const. The powerful research potential based on such universalities is widely used in condensed matter physics. Here we study the broad-band (1–1012 Hz) dielectric response of Shewanella oneidensis MR-1 extracellular matrix, cytochrome C and serum albumin. Applying concepts of condensed matter physics, we identify transport mechanisms and a number of energy, time, frequency, spatial and temperature scales in these biological objects, which can provide us with deeper insight into the protein dynamics.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Scientific Reports},\\n\\tauthor = {Motovilov, K. A. and Savinov, M. and Zhukova, E. S. and Pronin, A. A. and Gagkaeva, Z. V. and Grinenko, V. and Sidoruk, K. V. and Voeikova, T. A. and Barzilovich, P. Yu and Grebenko, A. K. and Lisovskii, S. V. and Torgashev, V. I. and Bednyakov, P. and Pokorný, J. and Dressel, M. and Gorshunov, B. P.},\\n\\tmonth = nov,\\n\\tyear = {2017},\\n\\tnote = {Number: 1\\nPublisher: Nature Publishing Group},\\n\\tkeywords = {Biomaterials – proteins, Polymers},\\n\\tpages = {15731},\\n\\tfile = {Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\4QFUHD76\\\\\\\\Motovilov и др. - 2017 - Observation of dielectric universalities in albumi.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Motovilov, K. A.\",\"Savinov, M.\",\"Zhukova, E. S.\",\"Pronin, A. A.\",\"Gagkaeva, Z. V.\",\"Grinenko, V.\",\"Sidoruk, K. V.\",\"Voeikova, T. A.\",\"Barzilovich, P. Y.\",\"Grebenko, A. K.\",\"Lisovskii, S. V.\",\"Torgashev, V. I.\",\"Bednyakov, P.\",\"Pokorný, J.\",\"Dressel, M.\",\"Gorshunov, B. P.\"],\"key\":\"motovilov_observation_2017\",\"id\":\"motovilov_observation_2017\",\"bibbaseid\":\"motovilov-savinov-zhukova-pronin-gagkaeva-grinenko-sidoruk-voeikova-etal-observationofdielectricuniversalitiesinalbumincytochromecandshewanellaoneidensismr1extracellularmatrix-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.nature.com/articles/s41598-017-15693-y\"},\"keyword\":[\"Biomaterials – proteins\",\"Polymers\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Simple theory of low-temperature thermal conductivity in single- and double-walled carbon nanotubes\",\"volume\":\"96\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.96.155413\",\"doi\":\"10.1103/PhysRevB.96.155413\",\"abstract\":\"Low-temperature phonon thermal conductance (PTC) of any 1D system increases proportionally to the temperature. However, here we show that in single- and double-walled carbon nanotubes (CNTs), starting from 3–6 K, the PTC increases faster than the linear function, since the low-frequency modes of dispersion curves, which do not tend to zero together with the wave vector, are excited. To develop the PTC theory, we combine the Landauer's ballistic approach with the simple continuous model proposed for the calculation of the low-frequency phonon spectra of both free nanotubes and those interacting with an environment. The approach obtained is valid not only for commensurate double-walled CNTs, but also for incommensurate ones. The temperature-dependent relation between the PTC of double-walled CNT and those of its constituent SWNTs is obtained and discussed. The low-temperature heat transfer in bulk materials originated from CNTs is also considered and the upper limit of thermal conductivity of such materials is determined. We argue that the ideal material consisting of CNTs can challenge diamond only when the mean length of its defect-free nanotubes reaches at least one hundred of micrometers.\",\"number\":\"15\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Chalin\"],\"firstnames\":[\"D.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Avramenko\"],\"firstnames\":[\"M.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2017\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"155413\",\"bibtex\":\"@article{chalin_simple_2017,\\n\\ttitle = {Simple theory of low-temperature thermal conductivity in single- and double-walled carbon nanotubes},\\n\\tvolume = {96},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.96.155413},\\n\\tdoi = {10.1103/PhysRevB.96.155413},\\n\\tabstract = {Low-temperature phonon thermal conductance (PTC) of any 1D system increases proportionally to the temperature. However, here we show that in single- and double-walled carbon nanotubes (CNTs), starting from 3–6 K, the PTC increases faster than the linear function, since the low-frequency modes of dispersion curves, which do not tend to zero together with the wave vector, are excited. To develop the PTC theory, we combine the Landauer's ballistic approach with the simple continuous model proposed for the calculation of the low-frequency phonon spectra of both free nanotubes and those interacting with an environment. The approach obtained is valid not only for commensurate double-walled CNTs, but also for incommensurate ones. The temperature-dependent relation between the PTC of double-walled CNT and those of its constituent SWNTs is obtained and discussed. The low-temperature heat transfer in bulk materials originated from CNTs is also considered and the upper limit of thermal conductivity of such materials is determined. We argue that the ideal material consisting of CNTs can challenge diamond only when the mean length of its defect-free nanotubes reaches at least one hundred of micrometers.},\\n\\tnumber = {15},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Chalin, D. V. and Avramenko, M. V. and Rochal, S. B.},\\n\\tmonth = oct,\\n\\tyear = {2017},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {155413},\\n}\\n\\n\",\"author_short\":[\"Chalin, D. V.\",\"Avramenko, M. V.\",\"Rochal, S. B.\"],\"key\":\"chalin_simple_2017\",\"id\":\"chalin_simple_2017\",\"bibbaseid\":\"chalin-avramenko-rochal-simpletheoryoflowtemperaturethermalconductivityinsingleanddoublewalledcarbonnanotubes-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.96.155413\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Quasicrystalline and crystalline types of local protein order in capsids of small viruses\",\"volume\":\"29\",\"issn\":\"0953-8984\",\"url\":\"https://dx.doi.org/10.1088/1361-648X/aa7211\",\"doi\":\"10.1088/1361-648X/aa7211\",\"abstract\":\"Like metal alloys and micellar systems in soft matter, the viral capsid structures can be of crystalline and quasicrystalline types. We reveal the local quasicrystalline order of proteins in small spherical viral capsids using their nets of dodecahedral type. We show that the structure of some of the viral shells is well described in terms of a chiral pentagonal tiling, whose nodes coincide with centers of mass of protein molecules. The chiral protein packing found in these capsids originates from the pentagonal Penrose tiling (PPT), due to a specific phason reconstruction needed to fit the protein order at the adjacent dodecahedron faces. Via examples of small spherical viral shells and geminate capsid of a Maize Streak virus, we discuss the benefits and shortcomings of the usage of a dodecahedral net in comparison to icosahedral one, which is commonly applied for the modeling of viral shells with a crystalline local order.\",\"language\":\"en\",\"number\":\"28\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics: Condensed Matter\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Konevtsova\"],\"firstnames\":[\"O.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pimonov\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorman\"],\"firstnames\":[\"V.\",\"L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2017\",\"note\":\"Publisher: IOP Publishing\",\"pages\":\"284002\",\"bibtex\":\"@article{konevtsova_quasicrystalline_2017,\\n\\ttitle = {Quasicrystalline and crystalline types of local protein order in capsids of small viruses},\\n\\tvolume = {29},\\n\\tissn = {0953-8984},\\n\\turl = {https://dx.doi.org/10.1088/1361-648X/aa7211},\\n\\tdoi = {10.1088/1361-648X/aa7211},\\n\\tabstract = {Like metal alloys and micellar systems in soft matter, the viral capsid structures can be of crystalline and quasicrystalline types. We reveal the local quasicrystalline order of proteins in small spherical viral capsids using their nets of dodecahedral type. We show that the structure of some of the viral shells is well described in terms of a chiral pentagonal tiling, whose nodes coincide with centers of mass of protein molecules. The chiral protein packing found in these capsids originates from the pentagonal Penrose tiling (PPT), due to a specific phason reconstruction needed to fit the protein order at the adjacent dodecahedron faces. Via examples of small spherical viral shells and geminate capsid of a Maize Streak virus, we discuss the benefits and shortcomings of the usage of a dodecahedral net in comparison to icosahedral one, which is commonly applied for the modeling of viral shells with a crystalline local order.},\\n\\tlanguage = {en},\\n\\tnumber = {28},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics: Condensed Matter},\\n\\tauthor = {Konevtsova, O. V. and Pimonov, V. V. and Lorman, V. L. and Rochal, S. B.},\\n\\tmonth = jun,\\n\\tyear = {2017},\\n\\tnote = {Publisher: IOP Publishing},\\n\\tpages = {284002},\\n}\\n\\n\",\"author_short\":[\"Konevtsova, O. V.\",\"Pimonov, V. V.\",\"Lorman, V. L.\",\"Rochal, S. B.\"],\"key\":\"konevtsova_quasicrystalline_2017\",\"id\":\"konevtsova_quasicrystalline_2017\",\"bibbaseid\":\"konevtsova-pimonov-lorman-rochal-quasicrystallineandcrystallinetypesoflocalproteinorderincapsidsofsmallviruses-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/1361-648X/aa7211\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Dielectric spectrum of multicomponent relaxor ceramics based on PZT\",\"volume\":\"509\",\"issn\":\"0015-0193\",\"url\":\"https://doi.org/10.1080/00150193.2017.1290499\",\"doi\":\"10.1080/00150193.2017.1290499\",\"abstract\":\"The dielectric spectrum of multicomponent relaxor ceramic based on PZT was studied. In non-polarized sample, Debye-type dispersion region is found with the dispersion frequency of the order of 106 Hz. During polarization of the sample, this dispersion is suppressed. It is assumed that upon cooling from the paraphrase, without applied electric field, the relaxor ceramics transition to the dipole glass state occurs. Polarization converts it into a ferroelectric state, which is confirmed by characteristic piezoresonance response in the dielectric spectrum.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Akbaeva\"],\"firstnames\":[\"G.M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sitalo\"],\"firstnames\":[\"E.I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gavrilyachenko\"],\"firstnames\":[\"V.G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Panchenko\"],\"firstnames\":[\"E.M.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2017\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2017.1290499\",\"keywords\":\"dielectric properties, Lead zirconate titanate, relaxor\",\"pages\":\"10–13\",\"bibtex\":\"@article{akbaeva_dielectric_2017,\\n\\ttitle = {Dielectric spectrum of multicomponent relaxor ceramics based on {PZT}},\\n\\tvolume = {509},\\n\\tissn = {0015-0193},\\n\\turl = {https://doi.org/10.1080/00150193.2017.1290499},\\n\\tdoi = {10.1080/00150193.2017.1290499},\\n\\tabstract = {The dielectric spectrum of multicomponent relaxor ceramic based on PZT was studied. In non-polarized sample, Debye-type dispersion region is found with the dispersion frequency of the order of 106 Hz. During polarization of the sample, this dispersion is suppressed. It is assumed that upon cooling from the paraphrase, without applied electric field, the relaxor ceramics transition to the dipole glass state occurs. Polarization converts it into a ferroelectric state, which is confirmed by characteristic piezoresonance response in the dielectric spectrum.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Akbaeva, G.M. and Sitalo, E.I. and Gavrilyachenko, V.G. and Panchenko, E.M.},\\n\\tmonth = mar,\\n\\tyear = {2017},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/00150193.2017.1290499},\\n\\tkeywords = {dielectric properties, Lead zirconate titanate, relaxor},\\n\\tpages = {10--13},\\n}\\n\\n\",\"author_short\":[\"Akbaeva, G.\",\"Sitalo, E.\",\"Gavrilyachenko, V.\",\"Panchenko, E.\"],\"key\":\"akbaeva_dielectric_2017\",\"id\":\"akbaeva_dielectric_2017\",\"bibbaseid\":\"akbaeva-sitalo-gavrilyachenko-panchenko-dielectricspectrumofmulticomponentrelaxorceramicsbasedonpzt-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/00150193.2017.1290499\"},\"keyword\":[\"dielectric properties\",\"Lead zirconate titanate\",\"relaxor\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Static and dynamic hidden symmetries of icosahedral viral capsids\",\"volume\":\"9\",\"issn\":\"2040-3372\",\"url\":\"https://pubs.rsc.org/en/content/articlelanding/2017/nr/c7nr04020b\",\"doi\":\"10.1039/C7NR04020B\",\"abstract\":\"Viral shells self-assemble from identical proteins, which tend to form equivalent environments in the resulting assembly. However, in icosahedral capsids containing more than 60 proteins, they are enforced to occupy not only the symmetrically equivalent locations but also the quasi-equivalent ones. Due to this important fact, static and dynamic symmetries of viral shells can include additional hidden components. Here, developing the Caspar and Klug ideas concerning the quasi-equivalence of protein environments, we derive the simplest hexagonal tilings, that in principle could correspond to the local protein order in viral shells, and apply the resulting theory to nucleocytoplasmic large dsDNA viruses. In addition, analyzing the dynamic symmetry of the P22 viral shell, we demonstrate that the collective critical modes responsible for the protein reorganization during the procapsid maturation are approximately equivalent to the normal modes of the isotropic spherical membrane with O(3) symmetry. Furthermore, we establish the relationship between the dynamic symmetry of the P22 procapsid and the protein arrangement regularities that appear only in the mature capsid.\",\"language\":\"en\",\"number\":\"34\",\"urldate\":\"2023-11-11\",\"journal\":\"Nanoscale\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergey\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Konevtsova\"],\"firstnames\":[\"Olga\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorman\"],\"firstnames\":[\"Vladimir\",\"L.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2017\",\"note\":\"Publisher: The Royal Society of Chemistry\",\"pages\":\"12449–12460\",\"file\":\"Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\BKZZ384I\\\\\\\\Rochal и др. - 2017 - Static and dynamic hidden symmetries of icosahedra.pdf:application/pdf\",\"bibtex\":\"@article{rochal_static_2017,\\n\\ttitle = {Static and dynamic hidden symmetries of icosahedral viral capsids},\\n\\tvolume = {9},\\n\\tissn = {2040-3372},\\n\\turl = {https://pubs.rsc.org/en/content/articlelanding/2017/nr/c7nr04020b},\\n\\tdoi = {10.1039/C7NR04020B},\\n\\tabstract = {Viral shells self-assemble from identical proteins, which tend to form equivalent environments in the resulting assembly. However, in icosahedral capsids containing more than 60 proteins, they are enforced to occupy not only the symmetrically equivalent locations but also the quasi-equivalent ones. Due to this important fact, static and dynamic symmetries of viral shells can include additional hidden components. Here, developing the Caspar and Klug ideas concerning the quasi-equivalence of protein environments, we derive the simplest hexagonal tilings, that in principle could correspond to the local protein order in viral shells, and apply the resulting theory to nucleocytoplasmic large dsDNA viruses. In addition, analyzing the dynamic symmetry of the P22 viral shell, we demonstrate that the collective critical modes responsible for the protein reorganization during the procapsid maturation are approximately equivalent to the normal modes of the isotropic spherical membrane with O(3) symmetry. Furthermore, we establish the relationship between the dynamic symmetry of the P22 procapsid and the protein arrangement regularities that appear only in the mature capsid.},\\n\\tlanguage = {en},\\n\\tnumber = {34},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Nanoscale},\\n\\tauthor = {Rochal, Sergey B. and Konevtsova, Olga V. and Lorman, Vladimir L.},\\n\\tmonth = aug,\\n\\tyear = {2017},\\n\\tnote = {Publisher: The Royal Society of Chemistry},\\n\\tpages = {12449--12460},\\n\\tfile = {Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\BKZZ384I\\\\\\\\Rochal и др. - 2017 - Static and dynamic hidden symmetries of icosahedra.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Rochal, S. B.\",\"Konevtsova, O. V.\",\"Lorman, V. L.\"],\"key\":\"rochal_static_2017\",\"id\":\"rochal_static_2017\",\"bibbaseid\":\"rochal-konevtsova-lorman-staticanddynamichiddensymmetriesoficosahedralviralcapsids-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://pubs.rsc.org/en/content/articlelanding/2017/nr/c7nr04020b\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Anticorrosion properties and physicochemical characteristics of organic films based on heterocyclic imidazole derivative\",\"volume\":\"53\",\"issn\":\"2070-206X\",\"url\":\"https://doi.org/10.1134/S207020511702023X\",\"doi\":\"10.1134/S207020511702023X\",\"language\":\"en\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Protection of Metals and Physical Chemistry of Surfaces\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shpan’ko\"],\"firstnames\":[\"S.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sidorenko\"],\"firstnames\":[\"E.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Semenchev\"],\"firstnames\":[\"A.\",\"F.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lyanguzov\"],\"firstnames\":[\"N.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Anisimova\"],\"firstnames\":[\"V.\",\"A.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2017\",\"pages\":\"335–342\",\"bibtex\":\"@article{shpanko_anticorrosion_2017,\\n\\ttitle = {Anticorrosion properties and physicochemical characteristics of organic films based on heterocyclic imidazole derivative},\\n\\tvolume = {53},\\n\\tissn = {2070-206X},\\n\\turl = {https://doi.org/10.1134/S207020511702023X},\\n\\tdoi = {10.1134/S207020511702023X},\\n\\tlanguage = {en},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Protection of Metals and Physical Chemistry of Surfaces},\\n\\tauthor = {Shpan’ko, S. P. and Sidorenko, E. N. and Semenchev, A. F. and Lyanguzov, N. V. and Anisimova, V. A.},\\n\\tmonth = mar,\\n\\tyear = {2017},\\n\\tpages = {335--342},\\n}\\n\\n\",\"author_short\":[\"Shpan’ko, S. P.\",\"Sidorenko, E. N.\",\"Semenchev, A. F.\",\"Lyanguzov, N. V.\",\"Anisimova, V. A.\"],\"key\":\"shpanko_anticorrosion_2017\",\"id\":\"shpanko_anticorrosion_2017\",\"bibbaseid\":\"shpanko-sidorenko-semenchev-lyanguzov-anisimova-anticorrosionpropertiesandphysicochemicalcharacteristicsoforganicfilmsbasedonheterocyclicimidazolederivative-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S207020511702023X\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Intrinsic phonon properties of double-walled carbon nanotubes*\",\"volume\":\"8\",\"issn\":\"2043-6262\",\"url\":\"https://dx.doi.org/10.1088/2043-6254/aa5957\",\"doi\":\"10.1088/2043-6254/aa5957\",\"abstract\":\"Double-walled carbon nanotubes (DWNT) are made of two concentric and weakly van der Waals coupled single-walled carbon nanotubes (SWNT). DWNTs are the simplest systems for studying the mechanical and electronic interactions between concentric carbon layers. In this paper we review recent results concerning the intrinsic features of phonons of DWNTs obtained from Raman experiments performed on index-identified DWNTs. The effect of the interlayer distance on the strength of the mechanical and electronic coupling between the layers, and thus on the frequencies of the Raman-active modes, namely the radial breathing-like modes (RBLMs) and G-modes, are evidenced and discussed.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Advances in Natural Sciences: Nanoscience and Nanotechnology\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Tran\"],\"firstnames\":[\"H.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Levshov\"],\"firstnames\":[\"D.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nguyen\"],\"firstnames\":[\"V.\",\"C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Paillet\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Arenal\"],\"firstnames\":[\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Than\"],\"firstnames\":[\"X.\",\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zahab\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Y.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Phan\"],\"firstnames\":[\"N.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sauvajol\"],\"firstnames\":[\"J.-L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Michel\"],\"firstnames\":[\"T.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2017\",\"note\":\"Publisher: IOP Publishing\",\"pages\":\"015018\",\"file\":\"IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\5JJ685FU\\\\\\\\Tran и др. - 2017 - Intrinsic phonon properties of double-walled carbo.pdf:application/pdf\",\"bibtex\":\"@article{tran_intrinsic_2017,\\n\\ttitle = {Intrinsic phonon properties of double-walled carbon nanotubes*},\\n\\tvolume = {8},\\n\\tissn = {2043-6262},\\n\\turl = {https://dx.doi.org/10.1088/2043-6254/aa5957},\\n\\tdoi = {10.1088/2043-6254/aa5957},\\n\\tabstract = {Double-walled carbon nanotubes (DWNT) are made of two concentric and weakly van der Waals coupled single-walled carbon nanotubes (SWNT). DWNTs are the simplest systems for studying the mechanical and electronic interactions between concentric carbon layers. In this paper we review recent results concerning the intrinsic features of phonons of DWNTs obtained from Raman experiments performed on index-identified DWNTs. The effect of the interlayer distance on the strength of the mechanical and electronic coupling between the layers, and thus on the frequencies of the Raman-active modes, namely the radial breathing-like modes (RBLMs) and G-modes, are evidenced and discussed.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Advances in Natural Sciences: Nanoscience and Nanotechnology},\\n\\tauthor = {Tran, H. N. and Levshov, D. I. and Nguyen, V. C. and Paillet, M. and Arenal, R. and Than, X. T. and Zahab, A. A. and Yuzyuk, Y. I. and Phan, N. M. and Sauvajol, J.-L. and Michel, T.},\\n\\tmonth = mar,\\n\\tyear = {2017},\\n\\tnote = {Publisher: IOP Publishing},\\n\\tpages = {015018},\\n\\tfile = {IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\5JJ685FU\\\\\\\\Tran и др. - 2017 - Intrinsic phonon properties of double-walled carbo.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Tran, H. N.\",\"Levshov, D. I.\",\"Nguyen, V. C.\",\"Paillet, M.\",\"Arenal, R.\",\"Than, X. T.\",\"Zahab, A. A.\",\"Yuzyuk, Y. I.\",\"Phan, N. M.\",\"Sauvajol, J.\",\"Michel, T.\"],\"key\":\"tran_intrinsic_2017\",\"id\":\"tran_intrinsic_2017\",\"bibbaseid\":\"tran-levshov-nguyen-paillet-arenal-than-zahab-yuzyuk-etal-intrinsicphononpropertiesofdoublewalledcarbonnanotubes-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/2043-6254/aa5957\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Tunable pyroelectric properties of barium strontium titanate thin films\",\"volume\":\"29\",\"issn\":\"0953-8984\",\"url\":\"https://dx.doi.org/10.1088/1361-648X/aa5711\",\"doi\":\"10.1088/1361-648X/aa5711\",\"abstract\":\"We studied the influence of the induced strain and applied electric field on the ground state of ferroelectric Ba0.7Sr0.3TiO3 thin films, deposited on the cubic (0 0 1) substrate. The dependence of the pyroelectric coefficient on the applied field is calculated for the different values of the induced strain. We found that tuning of the misfit strain in the film under the dielectric bolometer mode by the proper selection of substrate makes it possible to create the structures with very large values of the pyroelectric coefficient.\",\"language\":\"en\",\"number\":\"18\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics: Condensed Matter\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu\",\"I.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2017\",\"note\":\"Publisher: IOP Publishing\",\"pages\":\"185701\",\"bibtex\":\"@article{shirokov_tunable_2017,\\n\\ttitle = {Tunable pyroelectric properties of barium strontium titanate thin films},\\n\\tvolume = {29},\\n\\tissn = {0953-8984},\\n\\turl = {https://dx.doi.org/10.1088/1361-648X/aa5711},\\n\\tdoi = {10.1088/1361-648X/aa5711},\\n\\tabstract = {We studied the influence of the induced strain and applied electric field on the ground state of ferroelectric Ba0.7Sr0.3TiO3 thin films, deposited on the cubic (0 0 1) substrate. The dependence of the pyroelectric coefficient on the applied field is calculated for the different values of the induced strain. We found that tuning of the misfit strain in the film under the dielectric bolometer mode by the proper selection of substrate makes it possible to create the structures with very large values of the pyroelectric coefficient.},\\n\\tlanguage = {en},\\n\\tnumber = {18},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics: Condensed Matter},\\n\\tauthor = {Shirokov, V. B. and Razumnaya, A. G. and Yuzyuk, Yu I.},\\n\\tmonth = mar,\\n\\tyear = {2017},\\n\\tnote = {Publisher: IOP Publishing},\\n\\tpages = {185701},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Razumnaya, A. G.\",\"Yuzyuk, Y. I.\"],\"key\":\"shirokov_tunable_2017\",\"id\":\"shirokov_tunable_2017\",\"bibbaseid\":\"shirokov-razumnaya-yuzyuk-tunablepyroelectricpropertiesofbariumstrontiumtitanatethinfilms-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/1361-648X/aa5711\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Use of multiple acoustic reflections to enhance SAW UV photo-detector sensitivity\",\"volume\":\"26\",\"issn\":\"0964-1726\",\"url\":\"https://dx.doi.org/10.1088/1361-665X/26/3/035029\",\"doi\":\"10.1088/1361-665X/26/3/035029\",\"abstract\":\"A new approach to enhance the sensitivity of existing SAW UV-visible photo-detectors based on the monitoring of the multiple reflections of the acoustic waves in the Fourier transform of the frequency response (S21) is demonstrated. By using this concept, it is possible to monitor the UV-visible light in a wide intensity range from very high to ultralow. We present a strategy to obtain an ultrafast SAW UV photo-detector with millisecond response by tuning the deposition conditions of the ZnO film and using the multiple-reflections concept.\",\"language\":\"en\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Smart Materials and Structures\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Karapetyan\"],\"firstnames\":[\"G.\",\"Y.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaydashev\"],\"firstnames\":[\"V.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhilin\"],\"firstnames\":[\"D.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Minasyan\"],\"firstnames\":[\"T.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Abdulvakhidov\"],\"firstnames\":[\"K.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2017\",\"note\":\"Publisher: IOP Publishing\",\"pages\":\"035029\",\"bibtex\":\"@article{karapetyan_use_2017,\\n\\ttitle = {Use of multiple acoustic reflections to enhance {SAW} {UV} photo-detector sensitivity},\\n\\tvolume = {26},\\n\\tissn = {0964-1726},\\n\\turl = {https://dx.doi.org/10.1088/1361-665X/26/3/035029},\\n\\tdoi = {10.1088/1361-665X/26/3/035029},\\n\\tabstract = {A new approach to enhance the sensitivity of existing SAW UV-visible photo-detectors based on the monitoring of the multiple reflections of the acoustic waves in the Fourier transform of the frequency response (S21) is demonstrated. By using this concept, it is possible to monitor the UV-visible light in a wide intensity range from very high to ultralow. We present a strategy to obtain an ultrafast SAW UV photo-detector with millisecond response by tuning the deposition conditions of the ZnO film and using the multiple-reflections concept.},\\n\\tlanguage = {en},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Smart Materials and Structures},\\n\\tauthor = {Karapetyan, G. Y. and Kaydashev, V. E. and Zhilin, D. A. and Minasyan, T. A. and Abdulvakhidov, K. G. and Kaidashev, E. M.},\\n\\tmonth = feb,\\n\\tyear = {2017},\\n\\tnote = {Publisher: IOP Publishing},\\n\\tpages = {035029},\\n}\\n\\n\",\"author_short\":[\"Karapetyan, G. Y.\",\"Kaydashev, V. E.\",\"Zhilin, D. A.\",\"Minasyan, T. A.\",\"Abdulvakhidov, K. G.\",\"Kaidashev, E. M.\"],\"key\":\"karapetyan_use_2017\",\"id\":\"karapetyan_use_2017\",\"bibbaseid\":\"karapetyan-kaydashev-zhilin-minasyan-abdulvakhidov-kaidashev-useofmultipleacousticreflectionstoenhancesawuvphotodetectorsensitivity-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/1361-665X/26/3/035029\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Thermal expansion coefficient of carbon-supported Pt nanoparticles: In-situ X-ray diffraction study\",\"volume\":\"254\",\"copyright\":\"© 2017 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim\",\"issn\":\"1521-3951\",\"shorttitle\":\"Thermal expansion coefficient of carbon-supported Pt nanoparticles\",\"url\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201600695\",\"doi\":\"10.1002/pssb.201600695\",\"abstract\":\"The thermal expansion of carbon-supported Pt nanoparticles with different particle size has been studied in-situ via X-ray diffraction at temperatures from 100 to 300 K. The thermal expansion coefficient (TEC) of investigated Pt/C nanoparticles is always superior to that of bulk Pt. When the grain size D decreases from 11 to 3 nm, the TEC nonlinearly increases by about 1.66 × 10−6 K−1 which corresponds to a variation of ∼20% from bulk Pt. The obtained experimental dependence of TEC for Pt/C nanoparticles has been interpreted using different theoretical approaches. A comparison of the considered models with the experimental data reveals the best agreement from the binding order–length–strength model with the size dependence of TEC experimentally found in carbon-supported Pt nanoparticles.\",\"language\":\"en\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"physica status solidi (b)\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kulbakov\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Allix\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rakhmatullin\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"A.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"O.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"N.\",\"V.\"],\"suffixes\":[]}],\"year\":\"2017\",\"note\":\"_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201600695\",\"keywords\":\"X-ray diffraction, platinum, nanoparticles, surface relaxation, thermal expansion\",\"pages\":\"1600695\",\"bibtex\":\"@article{leontyev_thermal_2017,\\n\\ttitle = {Thermal expansion coefficient of carbon-supported {Pt} nanoparticles: {In}-situ {X}-ray diffraction study},\\n\\tvolume = {254},\\n\\tcopyright = {© 2017 WILEY-VCH Verlag GmbH \\\\& Co. KGaA, Weinheim},\\n\\tissn = {1521-3951},\\n\\tshorttitle = {Thermal expansion coefficient of carbon-supported {Pt} nanoparticles},\\n\\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201600695},\\n\\tdoi = {10.1002/pssb.201600695},\\n\\tabstract = {The thermal expansion of carbon-supported Pt nanoparticles with different particle size has been studied in-situ via X-ray diffraction at temperatures from 100 to 300 K. The thermal expansion coefficient (TEC) of investigated Pt/C nanoparticles is always superior to that of bulk Pt. When the grain size D decreases from 11 to 3 nm, the TEC nonlinearly increases by about 1.66 × 10−6 K−1 which corresponds to a variation of ∼20\\\\% from bulk Pt. The obtained experimental dependence of TEC for Pt/C nanoparticles has been interpreted using different theoretical approaches. A comparison of the considered models with the experimental data reveals the best agreement from the binding order–length–strength model with the size dependence of TEC experimentally found in carbon-supported Pt nanoparticles.},\\n\\tlanguage = {en},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {physica status solidi (b)},\\n\\tauthor = {Leontyev, I. N. and Kulbakov, A. A. and Allix, M. and Rakhmatullin, A. and Kuriganova, A. B. and Maslova, O. A. and Smirnova, N. V.},\\n\\tyear = {2017},\\n\\tnote = {\\\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201600695},\\n\\tkeywords = {X-ray diffraction, platinum, nanoparticles, surface relaxation, thermal expansion},\\n\\tpages = {1600695},\\n}\\n\\n\",\"author_short\":[\"Leontyev, I. N.\",\"Kulbakov, A. A.\",\"Allix, M.\",\"Rakhmatullin, A.\",\"Kuriganova, A. B.\",\"Maslova, O. A.\",\"Smirnova, N. V.\"],\"key\":\"leontyev_thermal_2017\",\"id\":\"leontyev_thermal_2017\",\"bibbaseid\":\"leontyev-kulbakov-allix-rakhmatullin-kuriganova-maslova-smirnova-thermalexpansioncoefficientofcarbonsupportedptnanoparticlesinsituxraydiffractionstudy-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201600695\"},\"keyword\":[\"X-ray diffraction\",\"platinum\",\"nanoparticles\",\"surface relaxation\",\"thermal expansion\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Unexpectedly high Curie temperature in weakly strained ferroelectric film\",\"volume\":\"254\",\"copyright\":\"© 2016 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim\",\"issn\":\"1521-3951\",\"url\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201600413\",\"doi\":\"10.1002/pssb.201600413\",\"abstract\":\"Polarized Raman spectra of the epitaxial Ba0.4Sr0.6TiO3 film grown on MgO substrate with thickness of 600 nm were studied in a broad temperature range of 80–600 K and the phase transition from paraelectric to tetragonal ferroelectric phase was observed at about 500 K. This critical temperature is substantially higher than that calculated from the lattice-mismatch strain theory. In addition, the predicted from the theory low-temperature orthorhombic and rhombohedral phases were not observed. We ascribe the strengthening of the tetragonal ferroelectric phase to the effect of the interface-induced build-in electric field resulted from the interface-accumulated charges.\",\"language\":\"en\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"physica status solidi (b)\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"Anna\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"Alexey\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lukyanchuk\"],\"firstnames\":[\"Igor\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"Vladimir\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golovko\"],\"firstnames\":[\"Yury\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mukhortov\"],\"firstnames\":[\"Vladimir\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Marssi\"],\"firstnames\":[\"Mimoun\",\"El\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yury\",\"I.\"],\"suffixes\":[]}],\"year\":\"2017\",\"note\":\"_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201600413\",\"keywords\":\"thin films, Raman spectroscopy, strain, BaTiO3, soft mode, Curie temperature, ferroelectric transition\",\"pages\":\"1600413\",\"bibtex\":\"@article{razumnaya_unexpectedly_2017,\\n\\ttitle = {Unexpectedly high {Curie} temperature in weakly strained ferroelectric film},\\n\\tvolume = {254},\\n\\tcopyright = {© 2016 WILEY-VCH Verlag GmbH \\\\& Co. KGaA, Weinheim},\\n\\tissn = {1521-3951},\\n\\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201600413},\\n\\tdoi = {10.1002/pssb.201600413},\\n\\tabstract = {Polarized Raman spectra of the epitaxial Ba0.4Sr0.6TiO3 film grown on MgO substrate with thickness of 600 nm were studied in a broad temperature range of 80–600 K and the phase transition from paraelectric to tetragonal ferroelectric phase was observed at about 500 K. This critical temperature is substantially higher than that calculated from the lattice-mismatch strain theory. In addition, the predicted from the theory low-temperature orthorhombic and rhombohedral phases were not observed. We ascribe the strengthening of the tetragonal ferroelectric phase to the effect of the interface-induced build-in electric field resulted from the interface-accumulated charges.},\\n\\tlanguage = {en},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {physica status solidi (b)},\\n\\tauthor = {Razumnaya, Anna G. and Mikheykin, Alexey S. and Lukyanchuk, Igor A. and Shirokov, Vladimir B. and Golovko, Yury I. and Mukhortov, Vladimir M. and Marssi, Mimoun El and Yuzyuk, Yury I.},\\n\\tyear = {2017},\\n\\tnote = {\\\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201600413},\\n\\tkeywords = {thin films, Raman spectroscopy, strain, BaTiO3, soft mode, Curie temperature, ferroelectric transition},\\n\\tpages = {1600413},\\n}\\n\\n\",\"author_short\":[\"Razumnaya, A. G.\",\"Mikheykin, A. S.\",\"Lukyanchuk, I. A.\",\"Shirokov, V. B.\",\"Golovko, Y. I.\",\"Mukhortov, V. M.\",\"Marssi, M. E.\",\"Yuzyuk, Y. I.\"],\"key\":\"razumnaya_unexpectedly_2017\",\"id\":\"razumnaya_unexpectedly_2017\",\"bibbaseid\":\"razumnaya-mikheykin-lukyanchuk-shirokov-golovko-mukhortov-marssi-yuzyuk-unexpectedlyhighcurietemperatureinweaklystrainedferroelectricfilm-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201600413\"},\"keyword\":[\"thin films\",\"Raman spectroscopy\",\"strain\",\"BaTiO3\",\"soft mode\",\"Curie temperature\",\"ferroelectric transition\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Interlayer Interaction Effects on the G Modes in Double-Walled Carbon Nanotubes With Different Electronic Configurations\",\"volume\":\"254\",\"copyright\":\"© 2017 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim\",\"issn\":\"1521-3951\",\"url\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201700251\",\"doi\":\"10.1002/pssb.201700251\",\"abstract\":\"We present experimental measurements of the features of G band in individual index-identified free-standing double-walled carbon nanotubes. We examine Raman spectra of different electronic configurations of DWNTs, namely: SC@SC, SC@M, M@SC, M@M, and clearly establish that, as in SWNTs, the profile of LO G-mode of each layer is broad (narrow) when the layer is metallic (semiconducting). The dependence of G-modes on the diameter and inter-layer distance in several SC@SC, SC@M, M@SC, M@M index-identified DWNTs is reported. We find, that, independently of the metallic or semiconducting nature of the layers, the frequencies of LO and TO G-mode of the inner and outer layers shift significantly with respect to the frequencies of the same modes in the constituent SWNTs.\",\"language\":\"en\",\"number\":\"11\",\"urldate\":\"2023-11-11\",\"journal\":\"physica status solidi (b)\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Levshov\"],\"firstnames\":[\"Dmitry\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tran\"],\"firstnames\":[\"Huy-Nam\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Michel\"],\"firstnames\":[\"Thierry\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Cao\"],\"firstnames\":[\"Thi\",\"Thanh\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nguyen\"],\"firstnames\":[\"Van\",\"Chuc\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Arenal\"],\"firstnames\":[\"Raul\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Popov\"],\"firstnames\":[\"Valentin\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sauvajol\"],\"firstnames\":[\"Jean-Louis\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zahab\"],\"firstnames\":[\"Ahmed-Azmi\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Paillet\"],\"firstnames\":[\"Matthieu\"],\"suffixes\":[]}],\"year\":\"2017\",\"note\":\"_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201700251\",\"keywords\":\"Raman spectroscopy, double-walled carbon nanotubes, interlayer interaction\",\"pages\":\"1700251\",\"bibtex\":\"@article{levshov_interlayer_2017,\\n\\ttitle = {Interlayer {Interaction} {Effects} on the {G} {Modes} in {Double}-{Walled} {Carbon} {Nanotubes} {With} {Different} {Electronic} {Configurations}},\\n\\tvolume = {254},\\n\\tcopyright = {© 2017 WILEY-VCH Verlag GmbH \\\\& Co. KGaA, Weinheim},\\n\\tissn = {1521-3951},\\n\\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201700251},\\n\\tdoi = {10.1002/pssb.201700251},\\n\\tabstract = {We present experimental measurements of the features of G band in individual index-identified free-standing double-walled carbon nanotubes. We examine Raman spectra of different electronic configurations of DWNTs, namely: SC@SC, SC@M, M@SC, M@M, and clearly establish that, as in SWNTs, the profile of LO G-mode of each layer is broad (narrow) when the layer is metallic (semiconducting). The dependence of G-modes on the diameter and inter-layer distance in several SC@SC, SC@M, M@SC, M@M index-identified DWNTs is reported. We find, that, independently of the metallic or semiconducting nature of the layers, the frequencies of LO and TO G-mode of the inner and outer layers shift significantly with respect to the frequencies of the same modes in the constituent SWNTs.},\\n\\tlanguage = {en},\\n\\tnumber = {11},\\n\\turldate = {2023-11-11},\\n\\tjournal = {physica status solidi (b)},\\n\\tauthor = {Levshov, Dmitry I. and Tran, Huy-Nam and Michel, Thierry and Cao, Thi Thanh and Nguyen, Van Chuc and Arenal, Raul and Popov, Valentin N. and Sauvajol, Jean-Louis and Zahab, Ahmed-Azmi and Paillet, Matthieu},\\n\\tyear = {2017},\\n\\tnote = {\\\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201700251},\\n\\tkeywords = {Raman spectroscopy, double-walled carbon nanotubes, interlayer interaction},\\n\\tpages = {1700251},\\n}\\n\\n\",\"author_short\":[\"Levshov, D. I.\",\"Tran, H.\",\"Michel, T.\",\"Cao, T. T.\",\"Nguyen, V. C.\",\"Arenal, R.\",\"Popov, V. N.\",\"Sauvajol, J.\",\"Zahab, A.\",\"Paillet, M.\"],\"key\":\"levshov_interlayer_2017\",\"id\":\"levshov_interlayer_2017\",\"bibbaseid\":\"levshov-tran-michel-cao-nguyen-arenal-popov-sauvajol-etal-interlayerinteractioneffectsonthegmodesindoublewalledcarbonnanotubeswithdifferentelectronicconfigurations-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201700251\"},\"keyword\":[\"Raman spectroscopy\",\"double-walled carbon nanotubes\",\"interlayer interaction\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"One-step Simultaneous Synthesis of Graphene and Pt Nanoparticles under the Action of Pulsed Alternating Current and Electrochemical Performance of Pt/Graphene Catalysts\",\"volume\":\"2\",\"copyright\":\"© 2017 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim\",\"issn\":\"2365-6549\",\"url\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201701186\",\"doi\":\"10.1002/slct.201701186\",\"abstract\":\"Pt/graphene electrocatalyst for fuel elements has been obtained via the simultaneously electrochemical dispersion of Pt foil and expanded graphite by applying the alternating current. Raman spectroscopy and transmission electron microscopy (TEM) have revealed multilayered structure of graphene (3-5 layers) with linear defects of graphene sheets near 1 μm. The microstructural characteristics and catalytic activity of synthesized Pt/graphene catalyst have been compared with those of Pt/Vulcan catalyst prepared under the same conditions. Pt nanoparticles of Pt/Graphene catalyst exhibit smaller average dimensions and narrower particle size distribution. It follows from the electrochemical study that the electrochemical surface area of Pt/graphene catalyst is 2.5 times higher than for Pt/Vulcan. Besides this, the activity in the electrooxidation of methanol and the stability of Pt/graphene catalyst are found to be superior to the analogous parameters of Pt/Vulcan specimen.\",\"language\":\"en\",\"number\":\"24\",\"urldate\":\"2023-11-11\",\"journal\":\"ChemistrySelect\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"Alexandra\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Avramenko\"],\"firstnames\":[\"Marina\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Popov\"],\"firstnames\":[\"Yuri\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"Olga\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Koval\"],\"firstnames\":[\"Olga\",\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\",\"V.\"],\"suffixes\":[]}],\"year\":\"2017\",\"note\":\"_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/slct.201701186\",\"keywords\":\"electrochemical dispersion, fuel cell, platinum, Graphene, Pt/graphene catalysts\",\"pages\":\"6979–6983\",\"bibtex\":\"@article{kuriganova_one-step_2017,\\n\\ttitle = {One-step {Simultaneous} {Synthesis} of {Graphene} and {Pt} {Nanoparticles} under the {Action} of {Pulsed} {Alternating} {Current} and {Electrochemical} {Performance} of {Pt}/{Graphene} {Catalysts}},\\n\\tvolume = {2},\\n\\tcopyright = {© 2017 Wiley-VCH Verlag GmbH \\\\& Co. KGaA, Weinheim},\\n\\tissn = {2365-6549},\\n\\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201701186},\\n\\tdoi = {10.1002/slct.201701186},\\n\\tabstract = {Pt/graphene electrocatalyst for fuel elements has been obtained via the simultaneously electrochemical dispersion of Pt foil and expanded graphite by applying the alternating current. Raman spectroscopy and transmission electron microscopy (TEM) have revealed multilayered structure of graphene (3-5 layers) with linear defects of graphene sheets near 1 μm. The microstructural characteristics and catalytic activity of synthesized Pt/graphene catalyst have been compared with those of Pt/Vulcan catalyst prepared under the same conditions. Pt nanoparticles of Pt/Graphene catalyst exhibit smaller average dimensions and narrower particle size distribution. It follows from the electrochemical study that the electrochemical surface area of Pt/graphene catalyst is 2.5 times higher than for Pt/Vulcan. Besides this, the activity in the electrooxidation of methanol and the stability of Pt/graphene catalyst are found to be superior to the analogous parameters of Pt/Vulcan specimen.},\\n\\tlanguage = {en},\\n\\tnumber = {24},\\n\\turldate = {2023-11-11},\\n\\tjournal = {ChemistrySelect},\\n\\tauthor = {Kuriganova, Alexandra B. and Leontyev, Igor N. and Avramenko, Marina V. and Popov, Yuri and Maslova, Olga A. and Koval, Olga Yu. and Smirnova, Nina V.},\\n\\tyear = {2017},\\n\\tnote = {\\\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/slct.201701186},\\n\\tkeywords = {electrochemical dispersion, fuel cell, platinum, Graphene, Pt/graphene catalysts},\\n\\tpages = {6979--6983},\\n}\\n\\n\",\"author_short\":[\"Kuriganova, A. B.\",\"Leontyev, I. N.\",\"Avramenko, M. V.\",\"Popov, Y.\",\"Maslova, O. A.\",\"Koval, O. Y.\",\"Smirnova, N. V.\"],\"key\":\"kuriganova_one-step_2017\",\"id\":\"kuriganova_one-step_2017\",\"bibbaseid\":\"kuriganova-leontyev-avramenko-popov-maslova-koval-smirnova-onestepsimultaneoussynthesisofgrapheneandptnanoparticlesundertheactionofpulsedalternatingcurrentandelectrochemicalperformanceofptgraphenecatalysts-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201701186\"},\"keyword\":[\"electrochemical dispersion\",\"fuel cell\",\"platinum\",\"Graphene\",\"Pt/graphene catalysts\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Формирование магнитных никелевых наночастиц и изменения матрицы фталоцианина никеля при допировании натрием\",\"volume\":\"87\",\"issn\":\"0044-4642\",\"url\":\"http://journals.ioffe.ru/articles/44998\",\"doi\":\"10.21883/JTF.2017.10.44998.2149\",\"language\":\"ru\",\"number\":\"10\",\"urldate\":\"2023-11-11\",\"journal\":\"Журнал технической физики\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Колпачева\"],\"firstnames\":[\"Н.А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Авраменко\"],\"firstnames\":[\"М.В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Авакян\"],\"firstnames\":[\"Л.А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Зубавичус\"],\"firstnames\":[\"Я.В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мирзаханян\"],\"firstnames\":[\"А.А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Манукян\"],\"firstnames\":[\"А.С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Шароян\"],\"firstnames\":[\"Э.Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бугаев\"],\"firstnames\":[\"Л.А.\"],\"suffixes\":[]}],\"year\":\"2017\",\"pages\":\"1532\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\EXHSE7C9\\\\\\\\Колпачева и др. - 2017 - Формирование магнитных никелевых наночастиц и изме.pdf:application/pdf\",\"bibtex\":\"@article{__2017,\\n\\ttitle = {Формирование магнитных никелевых наночастиц и изменения матрицы фталоцианина никеля при допировании натрием},\\n\\tvolume = {87},\\n\\tissn = {0044-4642},\\n\\turl = {http://journals.ioffe.ru/articles/44998},\\n\\tdoi = {10.21883/JTF.2017.10.44998.2149},\\n\\tlanguage = {ru},\\n\\tnumber = {10},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Журнал технической физики},\\n\\tauthor = {Колпачева, Н.А. and Авраменко, М.В. and Авакян, Л.А. and Зубавичус, Я.В. and Мирзаханян, А.А. and Манукян, А.С. and Шароян, Э.Г. and Бугаев, Л.А.},\\n\\tyear = {2017},\\n\\tpages = {1532},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\EXHSE7C9\\\\\\\\Колпачева и др. - 2017 - Формирование магнитных никелевых наночастиц и изме.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Колпачева, Н.\",\"Авраменко, М.\",\"Авакян, Л.\",\"Зубавичус, Я.\",\"Мирзаханян, А.\",\"Манукян, А.\",\"Шароян, Э.\",\"Бугаев, Л.\"],\"key\":\"__2017\",\"id\":\"__2017\",\"bibbaseid\":\"---------2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/44998\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Экспериментальное исследование динамики решетки индивидуальных полупроводниковых двустенных углеродных нанотрубок: тангенциальные G-моды\",\"volume\":\"59\",\"issn\":\"0367-3294\",\"shorttitle\":\"Экспериментальное исследование динамики решетки индивидуальных полупроводниковых двустенных углеродных нанотрубок\",\"url\":\"https://journals.ioffe.ru/articles/44057\",\"doi\":\"10.21883/FTT.2017.02.44057.274\",\"abstract\":\"Проведены исследования тангенциальных G-мод индивидуальных полупроводниковых двустенных углеродных нанотрубок методом резонансной спектроскопии комбинационного рассеяния света в широком диапазоне длин волн лазерного возбуждения. Индивидуальные подвешенные нанотрубки синтезированы методом химического осаждения из парогазовой фазы. Индексы хиральности (n,m) нанотрубок определялись методами электронной дифракции и просвечивающей электронной микроскопии высокого разрешения. В спектрах комбинационного рассеяния двустенных нанотрубок наблюдается существенный сдвиг тангенциальных мод в сравнении с аналогичными модами одностенных нанотрубок. Показано, что величина сдвига зависит от межслойного расстояния и от величины ван-дер-ваальсова взаимодействия между слоями двустенной нанотрубки. Исследование выполнено за счет гранта Российского фонда фундаментальных исследований (проект N 15-02-08340). DOI: 10.21883/FTT.2017.02.44057.274\",\"language\":\"ru\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Левшов\"],\"firstnames\":[\"Д.И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tran\"],\"firstnames\":[\"H.N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Слабодян\"],\"firstnames\":[\"Ю.С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Осадчий\"],\"firstnames\":[\"А.В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Рошаль\"],\"firstnames\":[\"С.Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.И.\"],\"suffixes\":[]}],\"year\":\"2017\",\"pages\":\"328\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\CPU38V3F\\\\\\\\Левшов и др. - 2017 - Экспериментальное исследование динамики решетки ин.pdf:application/pdf\",\"bibtex\":\"@article{__2017-1,\\n\\ttitle = {Экспериментальное исследование динамики решетки индивидуальных полупроводниковых двустенных углеродных нанотрубок: тангенциальные {G}-моды},\\n\\tvolume = {59},\\n\\tissn = {0367-3294},\\n\\tshorttitle = {Экспериментальное исследование динамики решетки индивидуальных полупроводниковых двустенных углеродных нанотрубок},\\n\\turl = {https://journals.ioffe.ru/articles/44057},\\n\\tdoi = {10.21883/FTT.2017.02.44057.274},\\n\\tabstract = {Проведены исследования тангенциальных G-мод индивидуальных полупроводниковых двустенных углеродных нанотрубок методом резонансной спектроскопии комбинационного рассеяния света в широком диапазоне длин волн лазерного возбуждения. Индивидуальные подвешенные нанотрубки синтезированы методом химического осаждения из парогазовой фазы. Индексы хиральности (n,m) нанотрубок определялись методами электронной дифракции и просвечивающей электронной микроскопии высокого разрешения. В спектрах комбинационного рассеяния двустенных нанотрубок наблюдается существенный сдвиг тангенциальных мод в сравнении с аналогичными модами одностенных нанотрубок. Показано, что величина сдвига зависит от межслойного расстояния и от величины ван-дер-ваальсова взаимодействия между слоями двустенной нанотрубки. Исследование выполнено за счет гранта Российского фонда фундаментальных исследований (проект N 15-02-08340). DOI: 10.21883/FTT.2017.02.44057.274},\\n\\tlanguage = {ru},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Левшов, Д.И. and Tran, H.N. and Слабодян, Ю.С. and Осадчий, А.В. and Рошаль, С.Б. and Юзюк, Ю.И.},\\n\\tyear = {2017},\\n\\tpages = {328},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\CPU38V3F\\\\\\\\Левшов и др. - 2017 - Экспериментальное исследование динамики решетки ин.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Левшов, Д.\",\"Tran, H.\",\"Слабодян, Ю.\",\"Осадчий, А.\",\"Рошаль, С.\",\"Юзюк, Ю.\"],\"key\":\"__2017-1\",\"id\":\"__2017-1\",\"bibbaseid\":\"-tran-----g-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/44057\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Electrochemical Synthesis and Photocatalytic Activity of Differently Shaped CuOx Particles\",\"volume\":\"13\",\"issn\":\"2297-3400\",\"url\":\"https://www.scientific.net/NHC.13.330\",\"doi\":\"10.4028/www.scientific.net/NHC.13.330\",\"abstract\":\"CuOx powders with diff erently shaped particles were firstly prepared via an electrochemical method by oxidation and dispersion of copper electrodes in an electrolyte solution under pulse alternating current (PAC). By means of X-ray diffraction (XRD) and scanning electron microscopy (SEM) the current density is found to have an influence on the morphology and composition of CuOx particles. Photocatalytic efficiency of CuOx towards methyl orange (MO) degradation under visible light was investigated. The prepared polyhedral particles show the best photocatalytic activity of 81 % towards MO comparing to octahedral and spherical particles with 70 and 61 %, respectively.\",\"language\":\"en\",\"urldate\":\"2023-11-11\",\"journal\":\"Nano Hybrids and Composites\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Ulyankina\"],\"firstnames\":[\"Anna\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\",\"V.\"],\"suffixes\":[]}],\"year\":\"2017\",\"note\":\"Publisher: Trans Tech Publications Ltd\",\"pages\":\"330–333\",\"bibtex\":\"@article{ulyankina_electrochemical_2017,\\n\\ttitle = {Electrochemical {Synthesis} and {Photocatalytic} {Activity} of {Differently} {Shaped} {CuOx} {Particles}},\\n\\tvolume = {13},\\n\\tissn = {2297-3400},\\n\\turl = {https://www.scientific.net/NHC.13.330},\\n\\tdoi = {10.4028/www.scientific.net/NHC.13.330},\\n\\tabstract = {CuOx powders with diff erently shaped particles were firstly prepared via an electrochemical method by oxidation and dispersion of copper electrodes in an electrolyte solution under pulse alternating current (PAC). By means of X-ray diffraction (XRD) and scanning electron microscopy (SEM) the current density is found to have an influence on the morphology and composition of CuOx particles. Photocatalytic efficiency of CuOx towards methyl orange (MO) degradation under visible light was investigated. The prepared polyhedral particles show the best photocatalytic activity of 81 \\\\% towards MO comparing to octahedral and spherical particles with 70 and 61 \\\\%, respectively.},\\n\\tlanguage = {en},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Nano Hybrids and Composites},\\n\\tauthor = {Ulyankina, Anna and Leontyev, Igor and Smirnova, Nina V.},\\n\\tyear = {2017},\\n\\tnote = {Publisher: Trans Tech Publications Ltd},\\n\\tpages = {330--333},\\n}\\n\\n\",\"author_short\":[\"Ulyankina, A.\",\"Leontyev, I.\",\"Smirnova, N. V.\"],\"key\":\"ulyankina_electrochemical_2017\",\"id\":\"ulyankina_electrochemical_2017\",\"bibbaseid\":\"ulyankina-leontyev-smirnova-electrochemicalsynthesisandphotocatalyticactivityofdifferentlyshapedcuoxparticles-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.scientific.net/NHC.13.330\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Особенности тангенциальных мод в спектрах комбинационного рассеяния света одностенных полупроводниковых углеродных нанотрубок большого диаметра\",\"volume\":\"59\",\"issn\":\"0367-3294\",\"url\":\"https://journals.ioffe.ru/articles/44173\",\"doi\":\"10.21883/FTT.2017.03.44173.137\",\"abstract\":\"Методом резонансной спектроскопии комбинационного рассеяния света в широком диапазоне длин волн лазерного возбуждения исследована динамика решетки и оптические свойства индивидуальных полупроводниковых одностенных углеродных нанотрубок с диаметрами более 2.0 nm. Индивидуальные подвешенные нанотрубки синтезированы методом химического осаждения из парогазовой фазы. Индексы хиральности (n,m) нанотрубок определялись методом электронной дифракции. Обнаружена зависимость отношения абсолютных интенсивностей поперечной и продольной оптических тангенциальных мод как от энергии возбуждения, так и от структурных параметров нанотрубок (диаметра и хирального угла). Наблюдаемые зависимости отличаются от спектральных данных, полученных ранее для индивидуальных полупроводниковых структурно идентифицированных нанотрубок с диаметрами менее 1.1 nm. Работа выполнена за счет гранта Российского научного фонда (проект N 15-12-10004). DOI: 10.21883/FTT.2017.03.44173.137\",\"language\":\"ru\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Левшов\"],\"firstnames\":[\"Д.И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Слабодян\"],\"firstnames\":[\"Ю.С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Тонких\"],\"firstnames\":[\"А.А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Michel\"],\"firstnames\":[\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Рошаль\"],\"firstnames\":[\"С.Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.И.\"],\"suffixes\":[]}],\"year\":\"2017\",\"pages\":\"575\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\RFCMW9MW\\\\\\\\Левшов и др. - 2017 - Особенности тангенциальных мод в спектрах комбинац.pdf:application/pdf\",\"bibtex\":\"@article{__2017-2,\\n\\ttitle = {Особенности тангенциальных мод в спектрах комбинационного рассеяния света одностенных полупроводниковых углеродных нанотрубок большого диаметра},\\n\\tvolume = {59},\\n\\tissn = {0367-3294},\\n\\turl = {https://journals.ioffe.ru/articles/44173},\\n\\tdoi = {10.21883/FTT.2017.03.44173.137},\\n\\tabstract = {Методом резонансной спектроскопии комбинационного рассеяния света в широком диапазоне длин волн лазерного возбуждения исследована динамика решетки и оптические свойства индивидуальных полупроводниковых одностенных углеродных нанотрубок с диаметрами более 2.0 nm. Индивидуальные подвешенные нанотрубки синтезированы методом химического осаждения из парогазовой фазы. Индексы хиральности (n,m) нанотрубок определялись методом электронной дифракции. Обнаружена зависимость отношения абсолютных интенсивностей поперечной и продольной оптических тангенциальных мод как от энергии возбуждения, так и от структурных параметров нанотрубок (диаметра и хирального угла). Наблюдаемые зависимости отличаются от спектральных данных, полученных ранее для индивидуальных полупроводниковых структурно идентифицированных нанотрубок с диаметрами менее 1.1 nm. Работа выполнена за счет гранта Российского научного фонда (проект N 15-12-10004). DOI: 10.21883/FTT.2017.03.44173.137},\\n\\tlanguage = {ru},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Левшов, Д.И. and Слабодян, Ю.С. and Тонких, А.А. and Michel, T. and Рошаль, С.Б. and Юзюк, Ю.И.},\\n\\tyear = {2017},\\n\\tpages = {575},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\RFCMW9MW\\\\\\\\Левшов и др. - 2017 - Особенности тангенциальных мод в спектрах комбинац.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Левшов, Д.\",\"Слабодян, Ю.\",\"Тонких, А.\",\"Michel, T.\",\"Рошаль, С.\",\"Юзюк, Ю.\"],\"key\":\"__2017-2\",\"id\":\"__2017-2\",\"bibbaseid\":\"---michel----2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/44173\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Investigation of the Wireless Reading from Signal Passive SAW Sensors with Reflective Interdigital Transducers\",\"url\":\"https://elibrary.ru/item.asp?id=43958874\",\"language\":\"en\",\"urldate\":\"2023-11-11\",\"author\":[{\"firstnames\":[\"Karapetyan\"],\"propositions\":[],\"lastnames\":[\"G.ya.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dneprovsky\"],\"firstnames\":[\"V.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]}],\"year\":\"2016\",\"note\":\"Publisher: Южный федеральный университет\",\"bibtex\":\"@article{karapetyan_gya_investigation_2016,\\n\\ttitle = {Investigation of the {Wireless} {Reading} from {Signal} {Passive} {SAW} {Sensors} with {Reflective} {Interdigital} {Transducers}},\\n\\turl = {https://elibrary.ru/item.asp?id=43958874},\\n\\tlanguage = {en},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Karapetyan G.ya. and Dneprovsky, V. G. and Kaidashev, E. M.},\\n\\tyear = {2016},\\n\\tnote = {Publisher: Южный федеральный университет},\\n}\\n\\n\",\"author_short\":[\"G.ya., K.\",\"Dneprovsky, V. G.\",\"Kaidashev, E. M.\"],\"key\":\"karapetyan_gya_investigation_2016\",\"id\":\"karapetyan_gya_investigation_2016\",\"bibbaseid\":\"gya-dneprovsky-kaidashev-investigationofthewirelessreadingfromsignalpassivesawsensorswithreflectiveinterdigitaltransducers-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=43958874\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Design of Construction Elements for Piezoelectric Resonators and Chemisensors Based on Zinc Oxide Nanorods\",\"url\":\"https://elibrary.ru/item.asp?id=44011645\",\"language\":\"en\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Nikolaev\"],\"firstnames\":[\"A.\",\"L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kazmina\"],\"firstnames\":[\"M.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Minasyan\"],\"firstnames\":[\"T.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"V.\",\"E.\"],\"suffixes\":[]},{\"firstnames\":[\"Karapetyan\"],\"propositions\":[],\"lastnames\":[\"G.ya.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]}],\"year\":\"2016\",\"note\":\"Publisher: Южный федеральный университет\",\"bibtex\":\"@article{nikolaev_design_2016,\\n\\ttitle = {Design of {Construction} {Elements} for {Piezoelectric} {Resonators} and {Chemisensors} {Based} on {Zinc} {Oxide} {Nanorods}},\\n\\turl = {https://elibrary.ru/item.asp?id=44011645},\\n\\tlanguage = {en},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Nikolaev, A. L. and Kazmina, M. A. and Minasyan, T. A. and Kaidashev, V. E. and Karapetyan G.ya. and Kaidashev, E. M.},\\n\\tyear = {2016},\\n\\tnote = {Publisher: Южный федеральный университет},\\n}\\n\\n\",\"author_short\":[\"Nikolaev, A. L.\",\"Kazmina, M. A.\",\"Minasyan, T. A.\",\"Kaidashev, V. E.\",\"G.ya., K.\",\"Kaidashev, E. M.\"],\"key\":\"nikolaev_design_2016\",\"id\":\"nikolaev_design_2016\",\"bibbaseid\":\"nikolaev-kazmina-minasyan-kaidashev-gya-kaidashev-designofconstructionelementsforpiezoelectricresonatorsandchemisensorsbasedonzincoxidenanorods-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=44011645\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Refractive Properties of Nanorod-Type 2D Photonic Crystals\",\"url\":\"https://elibrary.ru/item.asp?id=43962934\",\"language\":\"en\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Lerer\"],\"firstnames\":[\"A.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golovacheva\"],\"firstnames\":[\"E.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]}],\"year\":\"2016\",\"note\":\"Publisher: Южный федеральный университет\",\"bibtex\":\"@article{lerer_refractive_2016,\\n\\ttitle = {Refractive {Properties} of {Nanorod}-{Type} {2D} {Photonic} {Crystals}},\\n\\turl = {https://elibrary.ru/item.asp?id=43962934},\\n\\tlanguage = {en},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Lerer, A. M. and Timoshenko, P. E. and Golovacheva, E. V. and Kaidashev, E. M.},\\n\\tyear = {2016},\\n\\tnote = {Publisher: Южный федеральный университет},\\n}\\n\\n\",\"author_short\":[\"Lerer, A. M.\",\"Timoshenko, P. E.\",\"Golovacheva, E. V.\",\"Kaidashev, E. M.\"],\"key\":\"lerer_refractive_2016\",\"id\":\"lerer_refractive_2016\",\"bibbaseid\":\"lerer-timoshenko-golovacheva-kaidashev-refractivepropertiesofnanorodtype2dphotoniccrystals-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=43962934\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"patent\",\"type\":\"patent\",\"title\":\"Способ измерения физических величин с помощью датчиков на поверхностных акустических волнах\",\"url\":\"https://findpatent.ru/patent/262/2629892.html\",\"number\":\"RU 2629892\",\"author\":[{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Минасян Тигран Арменович (RU)\"],\"suffixes\":[]},{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Кайдашев Евгений Михайлович (RU)\"],\"suffixes\":[]},{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Кайдашев Владимир Евгеньевич (RU)\"],\"suffixes\":[]},{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Карапетьян Геворк Яковлевич (RU)\"],\"suffixes\":[]}],\"bibtex\":\"@patent{___ru__nodate,\\n\\ttitle = {Способ измерения физических величин с помощью датчиков на поверхностных акустических волнах},\\n\\turl = {https://findpatent.ru/patent/262/2629892.html},\\n\\tnumber = {RU 2629892},\\n\\tauthor = {{Минасян Тигран Арменович (RU)} and {Кайдашев Евгений Михайлович (RU)} and {Кайдашев Владимир Евгеньевич (RU)} and {Карапетьян Геворк Яковлевич (RU)}},\\n}\\n\\n\",\"author_short\":[\"Минасян Тигран Арменович (RU)\",\"Кайдашев Евгений Михайлович (RU)\",\"Кайдашев Владимир Евгеньевич (RU)\",\"Карапетьян Геворк Яковлевич (RU)\"],\"key\":\"___ru__nodate\",\"id\":\"___ru__nodate\",\"bibbaseid\":\"ru-ru-ru-ru-\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://findpatent.ru/patent/262/2629892.html\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Accurate determination of the chiral indices of individual carbon nanotubes by combining electron diffraction and Resonant Raman spectroscopy\",\"volume\":\"114\",\"issn\":\"0008-6223\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0008622316310570\",\"doi\":\"10.1016/j.carbon.2016.11.076\",\"abstract\":\"The experimental approach combining high resolution transmission electron microscopy (HRTEM), electron diffraction (ED) and resonant Raman spectroscopy (RRS) on the same free-standing individual carbon nanotubes (CNT) is the most efficient method to determine unambiguously the intrinsic features of the Raman-active phonons. In this paper, we review the main results obtained by the approach regarding the intrinsic features of the phonons of single-walled (SWNT) and double-walled carbon nanotubes (DWNT). First, we detail the different methods to identify the structure of SWNTs and DWNTs from the analysis of their electron diffraction patterns (EDP). In the following, we remind the principal features of the Raman response of SWNTs, unambiguously index-identified by ED. A special attention is devoted to the effect of the inter-layer interaction on the frequencies of the Raman-active phonons in index-identified DWNTs. The information obtained on index-identified SWNT and DWNT allows us to propose Raman criteria, which help identifying CNT when the ED fails to propose a single assignment. The efficiency of the Raman criteria as the complement to the ED information for the index-assignment of a few SWNTs and DWNTs is shown. The same approach to index-assign a triple-walled carbon nanotube (TWNT), by combining ED and RRS information, is reported.\",\"urldate\":\"2023-11-11\",\"journal\":\"Carbon\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Levshov\"],\"firstnames\":[\"D.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tran\"],\"firstnames\":[\"H.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Paillet\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Arenal\"],\"firstnames\":[\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Than\"],\"firstnames\":[\"X.\",\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zahab\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Y.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sauvajol\"],\"firstnames\":[\"J.\",\"-L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Michel\"],\"firstnames\":[\"T.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2017\",\"pages\":\"141–159\",\"file\":\"Принятая версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\2BU26V7I\\\\Łevshov и др. - 2017 - Accurate determination of the chiral indices of in.pdf:application/pdf;Принятая версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\75XGRBXA\\\\Łevshov и др. - 2017 - Accurate determination of the chiral indices of in.pdf:application/pdf\",\"bibtex\":\"@article{levshov_accurate_2017,\\n\\ttitle = {Accurate determination of the chiral indices of individual carbon nanotubes by combining electron diffraction and {Resonant} {Raman} spectroscopy},\\n\\tvolume = {114},\\n\\tissn = {0008-6223},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0008622316310570},\\n\\tdoi = {10.1016/j.carbon.2016.11.076},\\n\\tabstract = {The experimental approach combining high resolution transmission electron microscopy (HRTEM), electron diffraction (ED) and resonant Raman spectroscopy (RRS) on the same free-standing individual carbon nanotubes (CNT) is the most efficient method to determine unambiguously the intrinsic features of the Raman-active phonons. In this paper, we review the main results obtained by the approach regarding the intrinsic features of the phonons of single-walled (SWNT) and double-walled carbon nanotubes (DWNT). First, we detail the different methods to identify the structure of SWNTs and DWNTs from the analysis of their electron diffraction patterns (EDP). In the following, we remind the principal features of the Raman response of SWNTs, unambiguously index-identified by ED. A special attention is devoted to the effect of the inter-layer interaction on the frequencies of the Raman-active phonons in index-identified DWNTs. The information obtained on index-identified SWNT and DWNT allows us to propose Raman criteria, which help identifying CNT when the ED fails to propose a single assignment. The efficiency of the Raman criteria as the complement to the ED information for the index-assignment of a few SWNTs and DWNTs is shown. The same approach to index-assign a triple-walled carbon nanotube (TWNT), by combining ED and RRS information, is reported.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Carbon},\\n\\tauthor = {Levshov, D. I. and Tran, H. N. and Paillet, M. and Arenal, R. and Than, X. T. and Zahab, A. A. and Yuzyuk, Y. I. and Sauvajol, J. -L. and Michel, T.},\\n\\tmonth = apr,\\n\\tyear = {2017},\\n\\tpages = {141--159},\\n\\tfile = {Принятая версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\2BU26V7I\\\\\\\\Levshov и др. - 2017 - Accurate determination of the chiral indices of in.pdf:application/pdf;Принятая версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\75XGRBXA\\\\\\\\Levshov и др. - 2017 - Accurate determination of the chiral indices of in.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Levshov, D. I.\",\"Tran, H. N.\",\"Paillet, M.\",\"Arenal, R.\",\"Than, X. T.\",\"Zahab, A. A.\",\"Yuzyuk, Y. I.\",\"Sauvajol, J. -.\",\"Michel, T.\"],\"key\":\"levshov_accurate_2017\",\"id\":\"levshov_accurate_2017\",\"bibbaseid\":\"levshov-tran-paillet-arenal-than-zahab-yuzyuk-sauvajol-etal-accuratedeterminationofthechiralindicesofindividualcarbonnanotubesbycombiningelectrondiffractionandresonantramanspectroscopy-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0008622316310570\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Crucial influence of crystal site disorder on dynamical spectral response in artificial magnetoplumbites\",\"volume\":\"62\",\"issn\":\"1293-2558\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S1293255816305465\",\"doi\":\"10.1016/j.solidstatesciences.2016.10.012\",\"abstract\":\"High quality PbFe12O19 single crystals were grown by a solution-melt crystallization technique and characterized by synchrotron radiation diffraction structural studies, Mössbauer, Raman and infrared spectral measurements. In the terahertz and sub-terahertz range two absorption bands are observed, which are associated with the dynamics of structurally disordered lead and iron ions. We develop a structural model that comprises Fe2+ ions at the (1/2 × 4e) (0, 0, z) position with bipyramidal oxygen environment, and Pb ions at the (24l) (x, y, z) position with generic strongly distorted 12 vertex polyhedron of oxygen. The atomic displacement ellipsoids of the oxygen surrounding the lead ion are stretched towards the Pb ion within the plane perpendicular to the hexagonal axis. The suggested model is in full agreement with the local symmetry of the Fe2 and Pb ions and with the chemical composition of the sample determined by X-ray analysis.\",\"urldate\":\"2023-11-11\",\"journal\":\"Solid State Sciences\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"E.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bush\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sashin\"],\"firstnames\":[\"A.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"B.\",\"P.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2016\",\"keywords\":\"X-ray diffraction, Hexaferrites, Magnetoplumbite, Single crystal, Terahertz-infrared spectroscopy\",\"pages\":\"13–21\",\"bibtex\":\"@article{zhukova_crucial_2016,\\n\\ttitle = {Crucial influence of crystal site disorder on dynamical spectral response in artificial magnetoplumbites},\\n\\tvolume = {62},\\n\\tissn = {1293-2558},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S1293255816305465},\\n\\tdoi = {10.1016/j.solidstatesciences.2016.10.012},\\n\\tabstract = {High quality PbFe12O19 single crystals were grown by a solution-melt crystallization technique and characterized by synchrotron radiation diffraction structural studies, Mössbauer, Raman and infrared spectral measurements. In the terahertz and sub-terahertz range two absorption bands are observed, which are associated with the dynamics of structurally disordered lead and iron ions. We develop a structural model that comprises Fe2+ ions at the (1/2 × 4e) (0, 0, z) position with bipyramidal oxygen environment, and Pb ions at the (24l) (x, y, z) position with generic strongly distorted 12 vertex polyhedron of oxygen. The atomic displacement ellipsoids of the oxygen surrounding the lead ion are stretched towards the Pb ion within the plane perpendicular to the hexagonal axis. The suggested model is in full agreement with the local symmetry of the Fe2 and Pb ions and with the chemical composition of the sample determined by X-ray analysis.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Solid State Sciences},\\n\\tauthor = {Zhukova, E. S. and Mikheykin, A. S. and Torgashev, V. I. and Bush, A. A. and Yuzyuk, Yu. I. and Sashin, A. E. and Prokhorov, A. S. and Dressel, M. and Gorshunov, B. P.},\\n\\tmonth = dec,\\n\\tyear = {2016},\\n\\tkeywords = {X-ray diffraction, Hexaferrites, Magnetoplumbite, Single crystal, Terahertz-infrared spectroscopy},\\n\\tpages = {13--21},\\n}\\n\\n\",\"author_short\":[\"Zhukova, E. S.\",\"Mikheykin, A. S.\",\"Torgashev, V. I.\",\"Bush, A. A.\",\"Yuzyuk, Y. I.\",\"Sashin, A. E.\",\"Prokhorov, A. S.\",\"Dressel, M.\",\"Gorshunov, B. P.\"],\"key\":\"zhukova_crucial_2016\",\"id\":\"zhukova_crucial_2016\",\"bibbaseid\":\"zhukova-mikheykin-torgashev-bush-yuzyuk-sashin-prokhorov-dressel-etal-crucialinfluenceofcrystalsitedisorderondynamicalspectralresponseinartificialmagnetoplumbites-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S1293255816305465\"},\"keyword\":[\"X-ray diffraction\",\"Hexaferrites\",\"Magnetoplumbite\",\"Single crystal\",\"Terahertz-infrared spectroscopy\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Assembly of the most topologically regular two-dimensional micro and nanocrystals with spherical, conical, and tubular shapes\",\"volume\":\"94\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevE.94.052605\",\"doi\":\"10.1103/PhysRevE.94.052605\",\"abstract\":\"We consider how to control the extension of curvature-induced defects in the hexagonal order covering different curved surfaces. In these frames we propose a physical mechanism for improving structures of two-dimensional spherical colloidal crystals (SCCs). For any SCC comprising of about 300 or less particles the mechanism transforms all extended topological defects (ETDs) in the hexagonal order into the point disclinations. Perfecting the structure is carried out by successive cycles of the particle implantation and subsequent relaxation of the crystal. The mechanism is potentially suitable for obtaining colloidosomes with better selective permeability. Our approach enables modeling the most topologically regular tubular and conical two-dimensional nanocrystals including various possible polymorphic forms of the HIV viral capsid. Different HIV-like shells with an arbitrary number of structural units (SUs) and desired geometrical parameters are easily formed. Faceting of the obtained structures is performed by minimizing the suggested elastic energy.\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review E\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Roshal\"],\"firstnames\":[\"D.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Konevtsova\"],\"firstnames\":[\"O.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Myasnikova\"],\"firstnames\":[\"A.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2016\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"052605\",\"bibtex\":\"@article{roshal_assembly_2016,\\n\\ttitle = {Assembly of the most topologically regular two-dimensional micro and nanocrystals with spherical, conical, and tubular shapes},\\n\\tvolume = {94},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevE.94.052605},\\n\\tdoi = {10.1103/PhysRevE.94.052605},\\n\\tabstract = {We consider how to control the extension of curvature-induced defects in the hexagonal order covering different curved surfaces. In these frames we propose a physical mechanism for improving structures of two-dimensional spherical colloidal crystals (SCCs). For any SCC comprising of about 300 or less particles the mechanism transforms all extended topological defects (ETDs) in the hexagonal order into the point disclinations. Perfecting the structure is carried out by successive cycles of the particle implantation and subsequent relaxation of the crystal. The mechanism is potentially suitable for obtaining colloidosomes with better selective permeability. Our approach enables modeling the most topologically regular tubular and conical two-dimensional nanocrystals including various possible polymorphic forms of the HIV viral capsid. Different HIV-like shells with an arbitrary number of structural units (SUs) and desired geometrical parameters are easily formed. Faceting of the obtained structures is performed by minimizing the suggested elastic energy.},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review E},\\n\\tauthor = {Roshal, D. S. and Konevtsova, O. V. and Myasnikova, A. E. and Rochal, S. B.},\\n\\tmonth = nov,\\n\\tyear = {2016},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {052605},\\n}\\n\\n\",\"author_short\":[\"Roshal, D. S.\",\"Konevtsova, O. V.\",\"Myasnikova, A. E.\",\"Rochal, S. B.\"],\"key\":\"roshal_assembly_2016\",\"id\":\"roshal_assembly_2016\",\"bibbaseid\":\"roshal-konevtsova-myasnikova-rochal-assemblyofthemosttopologicallyregulartwodimensionalmicroandnanocrystalswithsphericalconicalandtubularshapes-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevE.94.052605\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Optical properties and charge transfer effects in single-walled carbon nanotubes filled with functionalized adamantane molecules\",\"volume\":\"109\",\"issn\":\"0008-6223\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0008622316306261\",\"doi\":\"10.1016/j.carbon.2016.07.053\",\"abstract\":\"The filling of single-walled carbon nanotube films with 1-adamantanemethanol and 1-bromoadamantane molecules was carried out by a gas-phase procedure. Optical absorption and Raman spectroscopies revealed the effects of charge transfer for samples treated with 1-bromoadamantane. Using density functional simulations we show that the charge transfer takes place when bromine is detached from the carbon cage and accepts electrons as free-standing atoms or as polybromide structures. Transmission electron microscope images confirm the presence of individual bromine atoms inside carbon nanotubes, treated with 1-bromoadamantane molecules. The observed charge transfer is, therefore, a marker of the dehalogenization reaction, a critical step in the synthesis process of narrow 1D sp3 nanostructures.\",\"urldate\":\"2023-11-11\",\"journal\":\"Carbon\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Tonkikh\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rybkovskiy\"],\"firstnames\":[\"D.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Orekhov\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chernov\"],\"firstnames\":[\"A.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Khomich\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ewels\"],\"firstnames\":[\"C.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kauppinen\"],\"firstnames\":[\"E.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chuvilin\"],\"firstnames\":[\"A.\",\"L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Obraztsova\"],\"firstnames\":[\"E.\",\"D.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2016\",\"pages\":\"87–97\",\"bibtex\":\"@article{tonkikh_optical_2016,\\n\\ttitle = {Optical properties and charge transfer effects in single-walled carbon nanotubes filled with functionalized adamantane molecules},\\n\\tvolume = {109},\\n\\tissn = {0008-6223},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0008622316306261},\\n\\tdoi = {10.1016/j.carbon.2016.07.053},\\n\\tabstract = {The filling of single-walled carbon nanotube films with 1-adamantanemethanol and 1-bromoadamantane molecules was carried out by a gas-phase procedure. Optical absorption and Raman spectroscopies revealed the effects of charge transfer for samples treated with 1-bromoadamantane. Using density functional simulations we show that the charge transfer takes place when bromine is detached from the carbon cage and accepts electrons as free-standing atoms or as polybromide structures. Transmission electron microscope images confirm the presence of individual bromine atoms inside carbon nanotubes, treated with 1-bromoadamantane molecules. The observed charge transfer is, therefore, a marker of the dehalogenization reaction, a critical step in the synthesis process of narrow 1D sp3 nanostructures.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Carbon},\\n\\tauthor = {Tonkikh, A. A. and Rybkovskiy, D. V. and Orekhov, A. S. and Chernov, A. I. and Khomich, A. A. and Ewels, C. P. and Kauppinen, E. I. and Rochal, S. B. and Chuvilin, A. L. and Obraztsova, E. D.},\\n\\tmonth = nov,\\n\\tyear = {2016},\\n\\tpages = {87--97},\\n}\\n\\n\",\"author_short\":[\"Tonkikh, A. A.\",\"Rybkovskiy, D. V.\",\"Orekhov, A. S.\",\"Chernov, A. I.\",\"Khomich, A. A.\",\"Ewels, C. P.\",\"Kauppinen, E. I.\",\"Rochal, S. B.\",\"Chuvilin, A. L.\",\"Obraztsova, E. D.\"],\"key\":\"tonkikh_optical_2016\",\"id\":\"tonkikh_optical_2016\",\"bibbaseid\":\"tonkikh-rybkovskiy-orekhov-chernov-khomich-ewels-kauppinen-rochal-etal-opticalpropertiesandchargetransfereffectsinsinglewalledcarbonnanotubesfilledwithfunctionalizedadamantanemolecules-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0008622316306261\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Pre-transitional evolution of central peaks and transverse acoustic phonon branch in single crystal lead zirconate titanate with Ti concentration 0.7%\",\"volume\":\"769\",\"issn\":\"1742-6596\",\"url\":\"https://dx.doi.org/10.1088/1742-6596/769/1/012070\",\"doi\":\"10.1088/1742-6596/769/1/012070\",\"abstract\":\"Inelastic X-ray scattering measurements have been done to study the lattice dynamics in lead zirconate titanate solid solution with 0.7% of PbTiO3. The temperature evolution of central peak and low-energy transverse phonon branches has been traced. Temperature dependent in-plane transverse polarized acoustic phonon branch in \\\\textless1 1 0\\\\textgreater direction has been revealed. The central peaks of two types have been found. The central peak at small wave vectors can be attributed to the relaxational-type soft ferroelectric mode, while the latter at Q = (1.5 -0.5 0) could be linked to the formation of M-superstructure in the intermediate ferroelectric phase.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics: Conference Series\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Andronikova\"],\"firstnames\":[\"D.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bronwald\"],\"firstnames\":[\"I.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Burkovsky\"],\"firstnames\":[\"R.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontiev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontiev\"],\"firstnames\":[\"N.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bosak\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Filimonov\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vakhrushev\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2016\",\"note\":\"Publisher: IOP Publishing\",\"pages\":\"012070\",\"file\":\"IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\77XA23P4\\\\\\\\Andronikova и др. - 2016 - Pre-transitional evolution of central peaks and tr.pdf:application/pdf\",\"bibtex\":\"@article{andronikova_pre-transitional_2016,\\n\\ttitle = {Pre-transitional evolution of central peaks and transverse acoustic phonon branch in single crystal lead zirconate titanate with {Ti} concentration 0.7\\\\%},\\n\\tvolume = {769},\\n\\tissn = {1742-6596},\\n\\turl = {https://dx.doi.org/10.1088/1742-6596/769/1/012070},\\n\\tdoi = {10.1088/1742-6596/769/1/012070},\\n\\tabstract = {Inelastic X-ray scattering measurements have been done to study the lattice dynamics in lead zirconate titanate solid solution with 0.7\\\\% of PbTiO3. The temperature evolution of central peak and low-energy transverse phonon branches has been traced. Temperature dependent in-plane transverse polarized acoustic phonon branch in {\\\\textless}1 1 0{\\\\textgreater} direction has been revealed. The central peaks of two types have been found. The central peak at small wave vectors can be attributed to the relaxational-type soft ferroelectric mode, while the latter at Q = (1.5 -0.5 0) could be linked to the formation of M-superstructure in the intermediate ferroelectric phase.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics: Conference Series},\\n\\tauthor = {Andronikova, D. A. and Bronwald, I. A. and Burkovsky, R. G. and Leontiev, I. N. and Leontiev, N. G. and Bosak, A. A. and Filimonov, A. V. and Vakhrushev, S. B.},\\n\\tmonth = nov,\\n\\tyear = {2016},\\n\\tnote = {Publisher: IOP Publishing},\\n\\tpages = {012070},\\n\\tfile = {IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\77XA23P4\\\\\\\\Andronikova и др. - 2016 - Pre-transitional evolution of central peaks and tr.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Andronikova, D. A.\",\"Bronwald, I. A.\",\"Burkovsky, R. G.\",\"Leontiev, I. N.\",\"Leontiev, N. G.\",\"Bosak, A. A.\",\"Filimonov, A. V.\",\"Vakhrushev, S. B.\"],\"key\":\"andronikova_pre-transitional_2016\",\"id\":\"andronikova_pre-transitional_2016\",\"bibbaseid\":\"andronikova-bronwald-burkovsky-leontiev-leontiev-bosak-filimonov-vakhrushev-pretransitionalevolutionofcentralpeaksandtransverseacousticphononbranchinsinglecrystalleadzirconatetitanatewithticoncentration07-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/1742-6596/769/1/012070\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Hidden symmetry of small spherical viruses and organization principles in “anomalous” and double-shelled capsid nanoassemblies\",\"volume\":\"8\",\"issn\":\"2040-3372\",\"url\":\"https://pubs.rsc.org/en/content/articlelanding/2016/nr/c6nr04930c\",\"doi\":\"10.1039/C6NR04930C\",\"abstract\":\"We propose the principles of structural organization in spherical nanoassemblies with icosahedral symmetry constituted by asymmetric protein molecules. The approach modifies the paradigmatic geometrical Caspar and Klug (CK) model of icosahedral viral capsids and demonstrates the common origin of both the “anomalous” and conventional capsid structures. In contrast to all previous models of “anomalous” viral capsids the proposed modified model conserves the basic structural principles of the CK approach and reveals the common hidden symmetry underlying all small viral shells. We demonstrate the common genesis of the “anomalous” and conventional capsids and explain their structures in the same frame. The organization principles are derived from the group theory analysis of the positional order on the spherical surface. The relationship between the modified CK geometrical model and the theory of two-dimensional spherical crystallization is discussed. We also apply the proposed approach to complex double-shelled capsids and capsids with protruding knob-like proteins. The introduced notion of commensurability for the concentric nanoshells explains the peculiarities of their organization and helps to predict analogous, but yet undiscovered, double-shelled viral capsid nanostructures.\",\"language\":\"en\",\"number\":\"38\",\"urldate\":\"2023-11-11\",\"journal\":\"Nanoscale\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Konevtsova\"],\"firstnames\":[\"O.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Myasnikova\"],\"firstnames\":[\"A.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorman\"],\"firstnames\":[\"V.\",\"L.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2016\",\"note\":\"Publisher: The Royal Society of Chemistry\",\"pages\":\"16976–16988\",\"bibtex\":\"@article{rochal_hidden_2016,\\n\\ttitle = {Hidden symmetry of small spherical viruses and organization principles in “anomalous” and double-shelled capsid nanoassemblies},\\n\\tvolume = {8},\\n\\tissn = {2040-3372},\\n\\turl = {https://pubs.rsc.org/en/content/articlelanding/2016/nr/c6nr04930c},\\n\\tdoi = {10.1039/C6NR04930C},\\n\\tabstract = {We propose the principles of structural organization in spherical nanoassemblies with icosahedral symmetry constituted by asymmetric protein molecules. The approach modifies the paradigmatic geometrical Caspar and Klug (CK) model of icosahedral viral capsids and demonstrates the common origin of both the “anomalous” and conventional capsid structures. In contrast to all previous models of “anomalous” viral capsids the proposed modified model conserves the basic structural principles of the CK approach and reveals the common hidden symmetry underlying all small viral shells. We demonstrate the common genesis of the “anomalous” and conventional capsids and explain their structures in the same frame. The organization principles are derived from the group theory analysis of the positional order on the spherical surface. The relationship between the modified CK geometrical model and the theory of two-dimensional spherical crystallization is discussed. We also apply the proposed approach to complex double-shelled capsids and capsids with protruding knob-like proteins. The introduced notion of commensurability for the concentric nanoshells explains the peculiarities of their organization and helps to predict analogous, but yet undiscovered, double-shelled viral capsid nanostructures.},\\n\\tlanguage = {en},\\n\\tnumber = {38},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Nanoscale},\\n\\tauthor = {Rochal, S. B. and Konevtsova, O. V. and Myasnikova, A. E. and Lorman, V. L.},\\n\\tmonth = sep,\\n\\tyear = {2016},\\n\\tnote = {Publisher: The Royal Society of Chemistry},\\n\\tpages = {16976--16988},\\n}\\n\\n\",\"author_short\":[\"Rochal, S. B.\",\"Konevtsova, O. V.\",\"Myasnikova, A. E.\",\"Lorman, V. L.\"],\"key\":\"rochal_hidden_2016\",\"id\":\"rochal_hidden_2016\",\"bibbaseid\":\"rochal-konevtsova-myasnikova-lorman-hiddensymmetryofsmallsphericalvirusesandorganizationprinciplesinanomalousanddoubleshelledcapsidnanoassemblies-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://pubs.rsc.org/en/content/articlelanding/2016/nr/c6nr04930c\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Phase transitions in barium–strontium titanate films on MgO substrates with various orientations\",\"volume\":\"58\",\"issn\":\"1090-6460\",\"url\":\"https://doi.org/10.1134/S1063783416100048\",\"doi\":\"10.1134/S1063783416100048\",\"abstract\":\"A comparative study of the lattice dynamic upon phase transitions in a polycrystalline Ba0.8Sr0.2TiO3 (BST) film on a Pt substrate and in epitaxial BST films grown on various sections of an MgO substrate has been performed by Raman spectroscopy. It has been found that different sequences of phase transitions take place in these films. The BST/Pt films demonstrate the same sequence of phase transitions that is observed in the bulk ceramics. The hardening of a soft mode in BST/(001)MgO and BST/Pt films shows that the transition from the tetragonal ferroelectric phase to the paraelectric phase has features of the displacement-type phase transition and also the order–disorder phase transition. When approaching the ferroelectric transition temperature, the soft mode in the BST/(111)MgO film is softened, following the Cockran law, which indicates the displacement-type phase transition.\",\"language\":\"en\",\"number\":\"10\",\"urldate\":\"2023-11-11\",\"journal\":\"Physics of the Solid State\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Anokhin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golovko\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mukhortov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2016\",\"pages\":\"2027–2034\",\"bibtex\":\"@article{anokhin_phase_2016,\\n\\ttitle = {Phase transitions in barium–strontium titanate films on {MgO} substrates with various orientations},\\n\\tvolume = {58},\\n\\tissn = {1090-6460},\\n\\turl = {https://doi.org/10.1134/S1063783416100048},\\n\\tdoi = {10.1134/S1063783416100048},\\n\\tabstract = {A comparative study of the lattice dynamic upon phase transitions in a polycrystalline Ba0.8Sr0.2TiO3 (BST) film on a Pt substrate and in epitaxial BST films grown on various sections of an MgO substrate has been performed by Raman spectroscopy. It has been found that different sequences of phase transitions take place in these films. The BST/Pt films demonstrate the same sequence of phase transitions that is observed in the bulk ceramics. The hardening of a soft mode in BST/(001)MgO and BST/Pt films shows that the transition from the tetragonal ferroelectric phase to the paraelectric phase has features of the displacement-type phase transition and also the order–disorder phase transition. When approaching the ferroelectric transition temperature, the soft mode in the BST/(111)MgO film is softened, following the Cockran law, which indicates the displacement-type phase transition.},\\n\\tlanguage = {en},\\n\\tnumber = {10},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physics of the Solid State},\\n\\tauthor = {Anokhin, A. S. and Razumnaya, A. G. and Yuzyuk, Yu. I. and Golovko, Yu. I. and Mukhortov, V. M.},\\n\\tmonth = oct,\\n\\tyear = {2016},\\n\\tpages = {2027--2034},\\n}\\n\\n\",\"author_short\":[\"Anokhin, A. S.\",\"Razumnaya, A. G.\",\"Yuzyuk, Y. I.\",\"Golovko, Y. I.\",\"Mukhortov, V. M.\"],\"key\":\"anokhin_phase_2016\",\"id\":\"anokhin_phase_2016\",\"bibbaseid\":\"anokhin-razumnaya-yuzyuk-golovko-mukhortov-phasetransitionsinbariumstrontiumtitanatefilmsonmgosubstrateswithvariousorientations-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1063783416100048\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Incipient ferroelectricity of water molecules confined to nano-channels of beryl\",\"volume\":\"7\",\"copyright\":\"2016 The Author(s)\",\"issn\":\"2041-1723\",\"url\":\"https://www.nature.com/articles/ncomms12842\",\"doi\":\"10.1038/ncomms12842\",\"abstract\":\"Water is characterized by large molecular electric dipole moments and strong interactions between molecules; however, hydrogen bonds screen the dipole–dipole coupling and suppress the ferroelectric order. The situation changes drastically when water is confined: in this case ordering of the molecular dipoles has been predicted, but never unambiguously detected experimentally. In the present study we place separate H2O molecules in the structural channels of a beryl single crystal so that they are located far enough to prevent hydrogen bonding, but close enough to keep the dipole–dipole interaction, resulting in incipient ferroelectricity in the water molecular subsystem. We observe a ferroelectric soft mode that causes Curie–Weiss behaviour of the static permittivity, which saturates below 10 K due to quantum fluctuations. The ferroelectricity of water molecules may play a key role in the functioning of biological systems and find applications in fuel and memory cells, light emitters and other nanoscale electronic devices.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Nature Communications\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"B.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"E.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Thomas\"],\"firstnames\":[\"V.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Belyanchikov\"],\"firstnames\":[\"M.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kadlec\"],\"firstnames\":[\"C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kadlec\"],\"firstnames\":[\"F.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Savinov\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ostapchuk\"],\"firstnames\":[\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Petzelt\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokleška\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tomas\"],\"firstnames\":[\"P.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pestrjakov\"],\"firstnames\":[\"E.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fursenko\"],\"firstnames\":[\"D.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shakurov\"],\"firstnames\":[\"G.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorelik\"],\"firstnames\":[\"V.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kadyrov\"],\"firstnames\":[\"L.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Uskov\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kremer\"],\"firstnames\":[\"R.\",\"K.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2016\",\"note\":\"Number: 1 Publisher: Nature Publishing Group\",\"keywords\":\"Ferroelectrics and multiferroics, Electronic devices, Electronic properties and materials\",\"pages\":\"12842\",\"file\":\"Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\QJNV8X4R\\\\\\\\Gorshunov и др. - 2016 - Incipient ferroelectricity of water molecules conf.pdf:application/pdf\",\"bibtex\":\"@article{gorshunov_incipient_2016,\\n\\ttitle = {Incipient ferroelectricity of water molecules confined to nano-channels of beryl},\\n\\tvolume = {7},\\n\\tcopyright = {2016 The Author(s)},\\n\\tissn = {2041-1723},\\n\\turl = {https://www.nature.com/articles/ncomms12842},\\n\\tdoi = {10.1038/ncomms12842},\\n\\tabstract = {Water is characterized by large molecular electric dipole moments and strong interactions between molecules; however, hydrogen bonds screen the dipole–dipole coupling and suppress the ferroelectric order. The situation changes drastically when water is confined: in this case ordering of the molecular dipoles has been predicted, but never unambiguously detected experimentally. In the present study we place separate H2O molecules in the structural channels of a beryl single crystal so that they are located far enough to prevent hydrogen bonding, but close enough to keep the dipole–dipole interaction, resulting in incipient ferroelectricity in the water molecular subsystem. We observe a ferroelectric soft mode that causes Curie–Weiss behaviour of the static permittivity, which saturates below 10 K due to quantum fluctuations. The ferroelectricity of water molecules may play a key role in the functioning of biological systems and find applications in fuel and memory cells, light emitters and other nanoscale electronic devices.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Nature Communications},\\n\\tauthor = {Gorshunov, B. P. and Torgashev, V. I. and Zhukova, E. S. and Thomas, V. G. and Belyanchikov, M. A. and Kadlec, C. and Kadlec, F. and Savinov, M. and Ostapchuk, T. and Petzelt, J. and Prokleška, J. and Tomas, P. V. and Pestrjakov, E. V. and Fursenko, D. A. and Shakurov, G. S. and Prokhorov, A. S. and Gorelik, V. S. and Kadyrov, L. S. and Uskov, V. V. and Kremer, R. K. and Dressel, M.},\\n\\tmonth = sep,\\n\\tyear = {2016},\\n\\tnote = {Number: 1\\nPublisher: Nature Publishing Group},\\n\\tkeywords = {Ferroelectrics and multiferroics, Electronic devices, Electronic properties and materials},\\n\\tpages = {12842},\\n\\tfile = {Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\QJNV8X4R\\\\\\\\Gorshunov и др. - 2016 - Incipient ferroelectricity of water molecules conf.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Gorshunov, B. P.\",\"Torgashev, V. I.\",\"Zhukova, E. S.\",\"Thomas, V. G.\",\"Belyanchikov, M. A.\",\"Kadlec, C.\",\"Kadlec, F.\",\"Savinov, M.\",\"Ostapchuk, T.\",\"Petzelt, J.\",\"Prokleška, J.\",\"Tomas, P. V.\",\"Pestrjakov, E. V.\",\"Fursenko, D. A.\",\"Shakurov, G. S.\",\"Prokhorov, A. S.\",\"Gorelik, V. S.\",\"Kadyrov, L. S.\",\"Uskov, V. V.\",\"Kremer, R. K.\",\"Dressel, M.\"],\"key\":\"gorshunov_incipient_2016\",\"id\":\"gorshunov_incipient_2016\",\"bibbaseid\":\"gorshunov-torgashev-zhukova-thomas-belyanchikov-kadlec-kadlec-savinov-etal-incipientferroelectricityofwatermoleculesconfinedtonanochannelsofberyl-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.nature.com/articles/ncomms12842\"},\"keyword\":[\"Ferroelectrics and multiferroics\",\"Electronic devices\",\"Electronic properties and materials\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Dispersion characteristics of optical waveguides based on ZnO nanorods\",\"volume\":\"61\",\"issn\":\"1555-6557\",\"url\":\"https://doi.org/10.1134/S1064226916060140\",\"doi\":\"10.1134/S1064226916060140\",\"abstract\":\"Using the method of separation of variables in the cylindrical coordinate system, the problem of propagation of electromagnetic waves in a 2D periodic lattice of ZnO nanwaveguides covered with a thin metal film is solved. Comparison of calculation results with results of simulation with the use of the COMSOL Multiphysics™ package based on the finite-element method is performed. The obtained results are used for forecasting the resonance wavelengths of a 2D periodic lattice of ZnO nanorods grown on a dielectric substrate.\",\"language\":\"en\",\"number\":\"6\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Communications Technology and Electronics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Lerer\"],\"firstnames\":[\"A.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chernikova\"],\"firstnames\":[\"T.\",\"Yu.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2016\",\"pages\":\"619–623\",\"bibtex\":\"@article{lerer_dispersion_2016,\\n\\ttitle = {Dispersion characteristics of optical waveguides based on {ZnO} nanorods},\\n\\tvolume = {61},\\n\\tissn = {1555-6557},\\n\\turl = {https://doi.org/10.1134/S1064226916060140},\\n\\tdoi = {10.1134/S1064226916060140},\\n\\tabstract = {Using the method of separation of variables in the cylindrical coordinate system, the problem of propagation of electromagnetic waves in a 2D periodic lattice of ZnO nanwaveguides covered with a thin metal film is solved. Comparison of calculation results with results of simulation with the use of the COMSOL Multiphysics™ package based on the finite-element method is performed. The obtained results are used for forecasting the resonance wavelengths of a 2D periodic lattice of ZnO nanorods grown on a dielectric substrate.},\\n\\tlanguage = {en},\\n\\tnumber = {6},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Communications Technology and Electronics},\\n\\tauthor = {Lerer, A. M. and Timoshenko, P. E. and Chernikova, T. Yu.},\\n\\tmonth = jun,\\n\\tyear = {2016},\\n\\tpages = {619--623},\\n}\\n\\n\",\"author_short\":[\"Lerer, A. M.\",\"Timoshenko, P. E.\",\"Chernikova, T. Y.\"],\"key\":\"lerer_dispersion_2016\",\"id\":\"lerer_dispersion_2016\",\"bibbaseid\":\"lerer-timoshenko-chernikova-dispersioncharacteristicsofopticalwaveguidesbasedonznonanorods-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1064226916060140\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"Terahertz dynamics of nanoconfined water molecules\",\"url\":\"https://ieeexplore.ieee.org/document/7758778\",\"doi\":\"10.1109/IRMMW-THz.2016.7758778\",\"abstract\":\"We performed spectroscopic studies of water-containing beryl crystals. At terahertz frequencies, we observed a strongly temperature-dependent spectral feature, corresponding to a collective excitation caused by dipole-dipole interactions between separate H2O molecules. We associate the excitation with a soft mode signaling an incipient ferroelectric state within the water molecular subsystem. Single-particle excitations of nanocaged H2O molecules are also observed at terahertz and infrared frequencies; using DFT analysis, their origin is assigned to translational and librational vibrational states.\",\"urldate\":\"2023-11-11\",\"booktitle\":\"2016 41st International Conference on Infrared, Millimeter, and Terahertz waves (IRMMW-THz)\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"Elena\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Belyanchikov\"],\"firstnames\":[\"Mikhail\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"Victor\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Thomas\"],\"firstnames\":[\"Victor\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Savinov\"],\"firstnames\":[\"Maksim\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kadlec\"],\"firstnames\":[\"Christelle\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kadlec\"],\"firstnames\":[\"Filip\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"Anatoly\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kadyrov\"],\"firstnames\":[\"Lenar\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Petzelt\"],\"firstnames\":[\"Jan\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ostapchuk\"],\"firstnames\":[\"Tatyana\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fursenko\"],\"firstnames\":[\"Dmitry\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Thomas\"],\"firstnames\":[\"Pavel\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shakurov\"],\"firstnames\":[\"Gilman\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"Martin\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"Boris\",\"P.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2016\",\"note\":\"ISSN: 2162-2035\",\"pages\":\"1–2\",\"bibtex\":\"@inproceedings{zhukova_terahertz_2016,\\n\\ttitle = {Terahertz dynamics of nanoconfined water molecules},\\n\\turl = {https://ieeexplore.ieee.org/document/7758778},\\n\\tdoi = {10.1109/IRMMW-THz.2016.7758778},\\n\\tabstract = {We performed spectroscopic studies of water-containing beryl crystals. At terahertz frequencies, we observed a strongly temperature-dependent spectral feature, corresponding to a collective excitation caused by dipole-dipole interactions between separate H2O molecules. We associate the excitation with a soft mode signaling an incipient ferroelectric state within the water molecular subsystem. Single-particle excitations of nanocaged H2O molecules are also observed at terahertz and infrared frequencies; using DFT analysis, their origin is assigned to translational and librational vibrational states.},\\n\\turldate = {2023-11-11},\\n\\tbooktitle = {2016 41st {International} {Conference} on {Infrared}, {Millimeter}, and {Terahertz} waves ({IRMMW}-{THz})},\\n\\tauthor = {Zhukova, Elena S. and Belyanchikov, Mikhail A. and Torgashev, Victor I. and Thomas, Victor G. and Savinov, Maksim and Kadlec, Christelle and Kadlec, Filip and Prokhorov, Anatoly S. and Kadyrov, Lenar S. and Petzelt, Jan and Ostapchuk, Tatyana and Fursenko, Dmitry A. and Thomas, Pavel V. and Shakurov, Gilman S. and Dressel, Martin and Gorshunov, Boris P.},\\n\\tmonth = sep,\\n\\tyear = {2016},\\n\\tnote = {ISSN: 2162-2035},\\n\\tpages = {1--2},\\n}\\n\\n\",\"author_short\":[\"Zhukova, E. S.\",\"Belyanchikov, M. A.\",\"Torgashev, V. I.\",\"Thomas, V. G.\",\"Savinov, M.\",\"Kadlec, C.\",\"Kadlec, F.\",\"Prokhorov, A. S.\",\"Kadyrov, L. S.\",\"Petzelt, J.\",\"Ostapchuk, T.\",\"Fursenko, D. A.\",\"Thomas, P. V.\",\"Shakurov, G. S.\",\"Dressel, M.\",\"Gorshunov, B. P.\"],\"key\":\"zhukova_terahertz_2016\",\"id\":\"zhukova_terahertz_2016\",\"bibbaseid\":\"zhukova-belyanchikov-torgashev-thomas-savinov-kadlec-kadlec-prokhorov-etal-terahertzdynamicsofnanoconfinedwatermolecules-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://ieeexplore.ieee.org/document/7758778\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"On the issue of universal dielectric responses in proteins\",\"url\":\"https://ieeexplore.ieee.org/document/7758865\",\"doi\":\"10.1109/IRMMW-THz.2016.7758865\",\"abstract\":\"Ac conductivity and dielectric permittivity of bovine serum albumin, cytochrome c and extracellular matrix synthesized by electrogenic bacteria Shewanella oneidensis MR-1 are measured at frequencies 1-1012 Hz and temperatures 10-300 K. Two types of conductivity mechanisms are observed as well as nearly constant loss (NCL) phenomenon, universal dielectric response (UDR) and signatures of boson peak depending on the temperature and water/ion contents in the samples.\",\"urldate\":\"2023-11-11\",\"booktitle\":\"2016 41st International Conference on Infrared, Millimeter, and Terahertz waves (IRMMW-THz)\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Motovilov\"],\"firstnames\":[\"Konstantin\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pronin\"],\"firstnames\":[\"Aleksei\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"Elena\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gagkaeva\"],\"firstnames\":[\"Zarina\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"Victor\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Savinov\"],\"firstnames\":[\"Maxim\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grinenko\"],\"firstnames\":[\"Vadim\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Belyanchikov\"],\"firstnames\":[\"Mikhail\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grebenko\"],\"firstnames\":[\"Artem\",\"K.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sidoruk\"],\"firstnames\":[\"Konstantin\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"Martin\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"Boris\",\"P.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2016\",\"note\":\"ISSN: 2162-2035\",\"pages\":\"1–1\",\"bibtex\":\"@inproceedings{motovilov_issue_2016,\\n\\ttitle = {On the issue of universal dielectric responses in proteins},\\n\\turl = {https://ieeexplore.ieee.org/document/7758865},\\n\\tdoi = {10.1109/IRMMW-THz.2016.7758865},\\n\\tabstract = {Ac conductivity and dielectric permittivity of bovine serum albumin, cytochrome c and extracellular matrix synthesized by electrogenic bacteria Shewanella oneidensis MR-1 are measured at frequencies 1-1012 Hz and temperatures 10-300 K. Two types of conductivity mechanisms are observed as well as nearly constant loss (NCL) phenomenon, universal dielectric response (UDR) and signatures of boson peak depending on the temperature and water/ion contents in the samples.},\\n\\turldate = {2023-11-11},\\n\\tbooktitle = {2016 41st {International} {Conference} on {Infrared}, {Millimeter}, and {Terahertz} waves ({IRMMW}-{THz})},\\n\\tauthor = {Motovilov, Konstantin A. and Pronin, Aleksei A. and Zhukova, Elena S. and Gagkaeva, Zarina V. and Torgashev, Victor I. and Savinov, Maxim and Grinenko, Vadim and Belyanchikov, Mikhail A. and Grebenko, Artem K. and Sidoruk, Konstantin V. and Dressel, Martin and Gorshunov, Boris P.},\\n\\tmonth = sep,\\n\\tyear = {2016},\\n\\tnote = {ISSN: 2162-2035},\\n\\tpages = {1--1},\\n}\\n\\n\",\"author_short\":[\"Motovilov, K. A.\",\"Pronin, A. A.\",\"Zhukova, E. S.\",\"Gagkaeva, Z. V.\",\"Torgashev, V. I.\",\"Savinov, M.\",\"Grinenko, V.\",\"Belyanchikov, M. A.\",\"Grebenko, A. K.\",\"Sidoruk, K. V.\",\"Dressel, M.\",\"Gorshunov, B. P.\"],\"key\":\"motovilov_issue_2016\",\"id\":\"motovilov_issue_2016\",\"bibbaseid\":\"motovilov-pronin-zhukova-gagkaeva-torgashev-savinov-grinenko-belyanchikov-etal-ontheissueofuniversaldielectricresponsesinproteins-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://ieeexplore.ieee.org/document/7758865\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Optical Nanowaveguides Based on Zinc Oxide Plasmonic Materials\",\"volume\":\"741\",\"issn\":\"1742-6596\",\"url\":\"https://dx.doi.org/10.1088/1742-6596/741/1/012159\",\"doi\":\"10.1088/1742-6596/741/1/012159\",\"abstract\":\"The numerical study of nanowaveguides containing ZO, AZO, GZO and other materials are studied in infrared range. The dispersion relation for the waveguides contained an arbitrary number of layers are solved numerically. The integral-differential equations in vector form of the electromagnetic waves propagation in nanowaveguides containing a finite width plasmon films are calculated by the Galerkin’ method and the effective dielectric constants method. The opportunity of surface plasmon-polariton propagation with a large deceleration ratio are shown.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics: Conference Series\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Lerer\"],\"firstnames\":[\"A.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chernikova\"],\"firstnames\":[\"T.\",\"Yu\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Puzanov\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2016\",\"note\":\"Publisher: IOP Publishing\",\"pages\":\"012159\",\"file\":\"IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\V8WUEVR3\\\\Łerer и др. - 2016 - Optical Nanowaveguides Based on Zinc Oxide Plasmon.pdf:application/pdf\",\"bibtex\":\"@article{lerer_optical_2016,\\n\\ttitle = {Optical {Nanowaveguides} {Based} on {Zinc} {Oxide} {Plasmonic} {Materials}},\\n\\tvolume = {741},\\n\\tissn = {1742-6596},\\n\\turl = {https://dx.doi.org/10.1088/1742-6596/741/1/012159},\\n\\tdoi = {10.1088/1742-6596/741/1/012159},\\n\\tabstract = {The numerical study of nanowaveguides containing ZO, AZO, GZO and other materials are studied in infrared range. The dispersion relation for the waveguides contained an arbitrary number of layers are solved numerically. The integral-differential equations in vector form of the electromagnetic waves propagation in nanowaveguides containing a finite width plasmon films are calculated by the Galerkin’ method and the effective dielectric constants method. The opportunity of surface plasmon-polariton propagation with a large deceleration ratio are shown.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics: Conference Series},\\n\\tauthor = {Lerer, A. M. and Timoshenko, P. E. and Chernikova, T. Yu and Kaidashev, E. M. and Puzanov, A. S.},\\n\\tmonth = aug,\\n\\tyear = {2016},\\n\\tnote = {Publisher: IOP Publishing},\\n\\tpages = {012159},\\n\\tfile = {IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\V8WUEVR3\\\\\\\\Lerer и др. - 2016 - Optical Nanowaveguides Based on Zinc Oxide Plasmon.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Lerer, A. M.\",\"Timoshenko, P. E.\",\"Chernikova, T. Y.\",\"Kaidashev, E. M.\",\"Puzanov, A. S.\"],\"key\":\"lerer_optical_2016\",\"id\":\"lerer_optical_2016\",\"bibbaseid\":\"lerer-timoshenko-chernikova-kaidashev-puzanov-opticalnanowaveguidesbasedonzincoxideplasmonicmaterials-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/1742-6596/741/1/012159\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Phenomenological theory of uniaxial relaxor ferroelectrics\",\"volume\":\"28\",\"issn\":\"0953-8984\",\"url\":\"https://dx.doi.org/10.1088/0953-8984/28/39/395902\",\"doi\":\"10.1088/0953-8984/28/39/395902\",\"abstract\":\"A phenomenological thermodynamic theory of uniaxial relaxor strontium barium niobate is developed using the Landau–Devonshire approach with two order parameters. The fourth-order thermodynamic potential allowed to explain the shape of the polarization hysteresis loops experimentally observed at different temperatures. We show that the broad maximum of the dielectric permittivity is not related to the phase transition and arise due to the coupling between polarization and true order parameter which has antiferroelectric nature. We found that the phase transition temperature is much higher than the maximum of the dielectric permittivity and very likely corresponds to so-called Burn’s temperature. True order parameter has no simple relation with polar modes.\",\"language\":\"en\",\"number\":\"39\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics: Condensed Matter\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pavlenko\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu\",\"I.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2016\",\"note\":\"Publisher: IOP Publishing\",\"pages\":\"395902\",\"bibtex\":\"@article{shirokov_phenomenological_2016,\\n\\ttitle = {Phenomenological theory of uniaxial relaxor ferroelectrics},\\n\\tvolume = {28},\\n\\tissn = {0953-8984},\\n\\turl = {https://dx.doi.org/10.1088/0953-8984/28/39/395902},\\n\\tdoi = {10.1088/0953-8984/28/39/395902},\\n\\tabstract = {A phenomenological thermodynamic theory of uniaxial relaxor strontium barium niobate is developed using the Landau–Devonshire approach with two order parameters. The fourth-order thermodynamic potential allowed to explain the shape of the polarization hysteresis loops experimentally observed at different temperatures. We show that the broad maximum of the dielectric permittivity is not related to the phase transition and arise due to the coupling between polarization and true order parameter which has antiferroelectric nature. We found that the phase transition temperature is much higher than the maximum of the dielectric permittivity and very likely corresponds to so-called Burn’s temperature. True order parameter has no simple relation with polar modes.},\\n\\tlanguage = {en},\\n\\tnumber = {39},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics: Condensed Matter},\\n\\tauthor = {Shirokov, V. B. and Pavlenko, A. V. and Yuzyuk, Yu I.},\\n\\tmonth = aug,\\n\\tyear = {2016},\\n\\tnote = {Publisher: IOP Publishing},\\n\\tpages = {395902},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Pavlenko, A. V.\",\"Yuzyuk, Y. I.\"],\"key\":\"shirokov_phenomenological_2016\",\"id\":\"shirokov_phenomenological_2016\",\"bibbaseid\":\"shirokov-pavlenko-yuzyuk-phenomenologicaltheoryofuniaxialrelaxorferroelectrics-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/0953-8984/28/39/395902\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Physical states and properties of barium titanate films in a plane electric field\",\"volume\":\"61\",\"issn\":\"1090-6525\",\"url\":\"https://doi.org/10.1134/S1063784216070240\",\"doi\":\"10.1134/S1063784216070240\",\"abstract\":\"The influence of a plane electric field on the phase states of barium titanate thin films under the conditions of forced deformation has been studied. The field dependence of a complete set of material constants has been taken in the region of the c-phase, where polarization losses are absent. The material constants are calculated using equations of the piezoelectric effect derived by linearizing the nonlinear equations of state from the phenomenological; theory for barium titanate. It has been shown that there is a critical value of the field at which the electromechanical coupling coefficient reaches a maximum.\",\"language\":\"en\",\"number\":\"7\",\"urldate\":\"2023-11-11\",\"journal\":\"Technical Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kalinchuk\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shakhovoi\"],\"firstnames\":[\"R.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2016\",\"pages\":\"1073–1078\",\"bibtex\":\"@article{shirokov_physical_2016,\\n\\ttitle = {Physical states and properties of barium titanate films in a plane electric field},\\n\\tvolume = {61},\\n\\tissn = {1090-6525},\\n\\turl = {https://doi.org/10.1134/S1063784216070240},\\n\\tdoi = {10.1134/S1063784216070240},\\n\\tabstract = {The influence of a plane electric field on the phase states of barium titanate thin films under the conditions of forced deformation has been studied. The field dependence of a complete set of material constants has been taken in the region of the c-phase, where polarization losses are absent. The material constants are calculated using equations of the piezoelectric effect derived by linearizing the nonlinear equations of state from the phenomenological; theory for barium titanate. It has been shown that there is a critical value of the field at which the electromechanical coupling coefficient reaches a maximum.},\\n\\tlanguage = {en},\\n\\tnumber = {7},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Technical Physics},\\n\\tauthor = {Shirokov, V. B. and Kalinchuk, V. V. and Shakhovoi, R. A. and Yuzyuk, Yu. I.},\\n\\tmonth = jul,\\n\\tyear = {2016},\\n\\tpages = {1073--1078},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Kalinchuk, V. V.\",\"Shakhovoi, R. A.\",\"Yuzyuk, Y. I.\"],\"key\":\"shirokov_physical_2016\",\"id\":\"shirokov_physical_2016\",\"bibbaseid\":\"shirokov-kalinchuk-shakhovoi-yuzyuk-physicalstatesandpropertiesofbariumtitanatefilmsinaplaneelectricfield-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1063784216070240\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Theory of morphological transformation of viral capsid shell during the maturation process in the HK97 bacteriophage and similar viruses\",\"volume\":\"93\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevE.93.052412\",\"doi\":\"10.1103/PhysRevE.93.052412\",\"abstract\":\"We consider the symmetry and physical origin of collective displacement modes playing a crucial role in the morphological transformation during the maturation of the HK97 bacteriophage and similar viruses. It is shown that the experimentally observed hexamer deformation and pentamer twist in the HK97 procapsid correspond to the simplest irreducible shear strain mode of a spherical shell. We also show that the icosahedral faceting of the bacteriophage capsid shell is driven by the simplest irreducible radial displacement field. The shear field has the rotational icosahedral symmetry group I while the radial field has the full icosahedral symmetry Ih. This difference makes their actions independent. The radial field sign discriminates between the icosahedral and the dodecahedral shapes of the faceted capsid shell, thus making the approach relevant not only for the HK97-like viruses but also for the parvovirus family. In the frame of the Landau-Ginzburg formalism we propose a simple phenomenological model valid for the first reversible step of the HK97 maturation process. The calculated phase diagram illustrates the discontinuous character of the virus shape transformation. The characteristics of the virus shell faceting and expansion obtained in the in vitro and in vivo experiments are related to the decrease in the capsid shell thickness and to the increase of the internal capsid pressure.\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review E\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Konevtsova\"],\"firstnames\":[\"O.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorman\"],\"firstnames\":[\"V.\",\"L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2016\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"052412\",\"file\":\"Принятая версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\UA4NGX4T\\\\\\\\Konevtsova и др. - 2016 - Theory of morphological transformation of viral ca.pdf:application/pdf\",\"bibtex\":\"@article{konevtsova_theory_2016,\\n\\ttitle = {Theory of morphological transformation of viral capsid shell during the maturation process in the {HK97} bacteriophage and similar viruses},\\n\\tvolume = {93},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevE.93.052412},\\n\\tdoi = {10.1103/PhysRevE.93.052412},\\n\\tabstract = {We consider the symmetry and physical origin of collective displacement modes playing a crucial role in the morphological transformation during the maturation of the HK97 bacteriophage and similar viruses. It is shown that the experimentally observed hexamer deformation and pentamer twist in the HK97 procapsid correspond to the simplest irreducible shear strain mode of a spherical shell. We also show that the icosahedral faceting of the bacteriophage capsid shell is driven by the simplest irreducible radial displacement field. The shear field has the rotational icosahedral symmetry group I while the radial field has the full icosahedral symmetry Ih. This difference makes their actions independent. The radial field sign discriminates between the icosahedral and the dodecahedral shapes of the faceted capsid shell, thus making the approach relevant not only for the HK97-like viruses but also for the parvovirus family. In the frame of the Landau-Ginzburg formalism we propose a simple phenomenological model valid for the first reversible step of the HK97 maturation process. The calculated phase diagram illustrates the discontinuous character of the virus shape transformation. The characteristics of the virus shell faceting and expansion obtained in the in vitro and in vivo experiments are related to the decrease in the capsid shell thickness and to the increase of the internal capsid pressure.},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review E},\\n\\tauthor = {Konevtsova, O. V. and Lorman, V. L. and Rochal, S. B.},\\n\\tmonth = may,\\n\\tyear = {2016},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {052412},\\n\\tfile = {Принятая версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\UA4NGX4T\\\\\\\\Konevtsova и др. - 2016 - Theory of morphological transformation of viral ca.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Konevtsova, O. V.\",\"Lorman, V. L.\",\"Rochal, S. B.\"],\"key\":\"konevtsova_theory_2016\",\"id\":\"konevtsova_theory_2016\",\"bibbaseid\":\"konevtsova-lorman-rochal-theoryofmorphologicaltransformationofviralcapsidshellduringthematurationprocessinthehk97bacteriophageandsimilarviruses-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevE.93.052412\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Phenomenological thermodynamics and the structure formation mechanism of the CuTi2S4 rhombohedral phase\",\"volume\":\"18\",\"issn\":\"1463-9084\",\"url\":\"https://pubs.rsc.org/en/content/articlelanding/2016/cp/c6cp00387g\",\"doi\":\"10.1039/C6CP00387G\",\"abstract\":\"The theory of structural phase transition in CuTi2S4 is proposed. The symmetry of order parameters, thermodynamics and the mechanism of the atomic structure formation of the rhombohedral Cu–Ti–thiospinel have been studied. The critical order parameter inducing the phase transition has been found. Within the Landau theory of phase transitions, it is shown that the phase state may change from the high-symmetry cubic disordered Fdm phase to the low-symmetry ordered rhombohedral Rm phase as a result of phase transition of the first order close to the second order. It is shown that the rhombohedral structure of CuTi2S4 is formed as a result of the displacements of all types of atoms and the ordering of Cu-atoms (1 : 1 order type in tetrahedral spinel sites), Ti-atoms (1 : 1 : 6 order type in octahedral spinel sites), and S-atoms (1 : 1 : 3 : 3 order type). The Cu- and Ti-atoms form metal nanoclusters which are named a “bunch” of dimers. The “bunch” of dimers in CuTi2S4 is a new type of self-organization of atoms in frustrated spinel-like structures. It is shown that Ti-atoms also form other types of metal nanoclusters: trimers and tetrahedra.\",\"language\":\"en\",\"number\":\"15\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Chemistry Chemical Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"Michail\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"Vladimir\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"Valery\",\"M.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2016\",\"note\":\"Publisher: The Royal Society of Chemistry\",\"pages\":\"10600–10606\",\"file\":\"Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\IESXZ2EA\\\\\\\\Talanov и др. - 2016 - Phenomenological thermodynamics and the structure .pdf:application/pdf\",\"bibtex\":\"@article{talanov_phenomenological_2016,\\n\\ttitle = {Phenomenological thermodynamics and the structure formation mechanism of the {CuTi2S4} rhombohedral phase},\\n\\tvolume = {18},\\n\\tissn = {1463-9084},\\n\\turl = {https://pubs.rsc.org/en/content/articlelanding/2016/cp/c6cp00387g},\\n\\tdoi = {10.1039/C6CP00387G},\\n\\tabstract = {The theory of structural phase transition in CuTi2S4 is proposed. The symmetry of order parameters, thermodynamics and the mechanism of the atomic structure formation of the rhombohedral Cu–Ti–thiospinel have been studied. The critical order parameter inducing the phase transition has been found. Within the Landau theory of phase transitions, it is shown that the phase state may change from the high-symmetry cubic disordered Fdm phase to the low-symmetry ordered rhombohedral Rm phase as a result of phase transition of the first order close to the second order. It is shown that the rhombohedral structure of CuTi2S4 is formed as a result of the displacements of all types of atoms and the ordering of Cu-atoms (1 : 1 order type in tetrahedral spinel sites), Ti-atoms (1 : 1 : 6 order type in octahedral spinel sites), and S-atoms (1 : 1 : 3 : 3 order type). The Cu- and Ti-atoms form metal nanoclusters which are named a “bunch” of dimers. The “bunch” of dimers in CuTi2S4 is a new type of self-organization of atoms in frustrated spinel-like structures. It is shown that Ti-atoms also form other types of metal nanoclusters: trimers and tetrahedra.},\\n\\tlanguage = {en},\\n\\tnumber = {15},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Chemistry Chemical Physics},\\n\\tauthor = {Talanov, Michail V. and Shirokov, Vladimir B. and Talanov, Valery M.},\\n\\tmonth = apr,\\n\\tyear = {2016},\\n\\tnote = {Publisher: The Royal Society of Chemistry},\\n\\tpages = {10600--10606},\\n\\tfile = {Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\IESXZ2EA\\\\\\\\Talanov и др. - 2016 - Phenomenological thermodynamics and the structure .pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Talanov, M. V.\",\"Shirokov, V. B.\",\"Talanov, V. M.\"],\"key\":\"talanov_phenomenological_2016\",\"id\":\"talanov_phenomenological_2016\",\"bibbaseid\":\"talanov-shirokov-talanov-phenomenologicalthermodynamicsandthestructureformationmechanismofthecuti2s4rhombohedralphase-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://pubs.rsc.org/en/content/articlelanding/2016/cp/c6cp00387g\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Characterization of zinc and zinc cyanide nanoparticles in carbon matrices prepared by solid-phase pyrolysis of zinc-phthalocyanine\",\"volume\":\"51\",\"issn\":\"1934-9378\",\"url\":\"https://doi.org/10.3103/S1068337216020134\",\"doi\":\"10.3103/S1068337216020134\",\"abstract\":\"Using solid-phase pyrolysis of Zn-phthalocyanine (ZnC32H16N8), we have prepared zinc and zinc cyanide nanoparticles in carbon matrices with a zinc concentration of 3 at %. The structure and composition of samples were investigated by the methods of scanning electron microscopy, X-ray diffraction, and Raman spectroscopy. It is shown that at low pyrolysis temperature (700°C) only the Zn nanoparticles are formed, whereas at higher temperature (900°C) a certain amount of Zn(CN)2 nanoparticles are also synthesized. The mean diameter of nanoparticles is about 150 nm, and their size distribution has a logarithmically normal shape.\",\"language\":\"en\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Contemporary Physics (Armenian Academy of Sciences)\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Mirzakhanyan\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Manukyan\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gyulasaryan\"],\"firstnames\":[\"H.\",\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ginoyan\"],\"firstnames\":[\"A.\",\"K.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nurijanyan\"],\"firstnames\":[\"M.\",\"Kh.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaniukov\"],\"firstnames\":[\"E.\",\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sharoyan\"],\"firstnames\":[\"E.\",\"G.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2016\",\"keywords\":\"X-ray diffraction, Raman shift, SEM images, size distribution, solid-phase pyrolysis, zinc and zinc cyanide nanoparticles\",\"pages\":\"191–195\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\MAWN25GC\\\\\\\\Mirzakhanyan и др. - 2016 - Characterization of zinc and zinc cyanide nanopart.pdf:application/pdf\",\"bibtex\":\"@article{mirzakhanyan_characterization_2016,\\n\\ttitle = {Characterization of zinc and zinc cyanide nanoparticles in carbon matrices prepared by solid-phase pyrolysis of zinc-phthalocyanine},\\n\\tvolume = {51},\\n\\tissn = {1934-9378},\\n\\turl = {https://doi.org/10.3103/S1068337216020134},\\n\\tdoi = {10.3103/S1068337216020134},\\n\\tabstract = {Using solid-phase pyrolysis of Zn-phthalocyanine (ZnC32H16N8), we have prepared zinc and zinc cyanide nanoparticles in carbon matrices with a zinc concentration of 3 at \\\\%. The structure and composition of samples were investigated by the methods of scanning electron microscopy, X-ray diffraction, and Raman spectroscopy. It is shown that at low pyrolysis temperature (700°C) only the Zn nanoparticles are formed, whereas at higher temperature (900°C) a certain amount of Zn(CN)2 nanoparticles are also synthesized. The mean diameter of nanoparticles is about 150 nm, and their size distribution has a logarithmically normal shape.},\\n\\tlanguage = {en},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Contemporary Physics (Armenian Academy of Sciences)},\\n\\tauthor = {Mirzakhanyan, A. A. and Manukyan, A. S. and Gyulasaryan, H. T. and Ginoyan, A. K. and Nurijanyan, M. Kh. and Yuzyuk, Yu. I. and Kaniukov, E. Yu. and Sharoyan, E. G.},\\n\\tmonth = apr,\\n\\tyear = {2016},\\n\\tkeywords = {X-ray diffraction, Raman shift, SEM images, size distribution, solid-phase pyrolysis, zinc and zinc cyanide nanoparticles},\\n\\tpages = {191--195},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\MAWN25GC\\\\\\\\Mirzakhanyan и др. - 2016 - Characterization of zinc and zinc cyanide nanopart.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Mirzakhanyan, A. A.\",\"Manukyan, A. S.\",\"Gyulasaryan, H. T.\",\"Ginoyan, A. K.\",\"Nurijanyan, M. K.\",\"Yuzyuk, Y. I.\",\"Kaniukov, E. Y.\",\"Sharoyan, E. G.\"],\"key\":\"mirzakhanyan_characterization_2016\",\"id\":\"mirzakhanyan_characterization_2016\",\"bibbaseid\":\"mirzakhanyan-manukyan-gyulasaryan-ginoyan-nurijanyan-yuzyuk-kaniukov-sharoyan-characterizationofzincandzinccyanidenanoparticlesincarbonmatricespreparedbysolidphasepyrolysisofzincphthalocyanine-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.3103/S1068337216020134\"},\"keyword\":[\"X-ray diffraction\",\"Raman shift\",\"SEM images\",\"size distribution\",\"solid-phase pyrolysis\",\"zinc and zinc cyanide nanoparticles\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Investigation of defectiveness of multiwalled carbon nanotubes produced with Fe–Co catalysts of different composition\",\"volume\":\"10\",\"issn\":\"1934-2608, 1934-2608\",\"url\":\"https://www.spiedigitallibrary.org/journals/journal-of-nanophotonics/volume-10/issue-1/012526/Investigation-of-defectiveness-of-multiwalled-carbon-nanotubes-produced-with-FeCo/10.1117/1.JNP.10.012526.full\",\"doi\":\"10.1117/1.JNP.10.012526\",\"abstract\":\"We have performed a study of CVD multiwalled carbon nanotubes (MWCNTs) produced with Fe–Co catalysts with a variable ratio of active metals. The Raman data were considered in combination with the temperature dependence of MWCNT conductivity. The data analysis is based on the point that the value of I2D/ID ratio correlates with the graphene fragment size. The fragments are considered as building blocks of MWCNTs. We showed that MWCNT defectiveness depends on the ratio of bimetallic active components in the Fe–Co catalyst. Thus, the ratio of I2D/ID increases and the D-mode intensity decreases while the Fe content in the catalyst increases. This also points to the reduction of defect number in the bigger graphene fragments. These results correlate with the data on conductivity temperature dependence. Namely, the increase of Fe content in the active component of the Fe–Co catalyst results in the increase of charge carrier concentration, which, in turn, indicates a decrease in MWCNT defectiveness.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Nanophotonics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Bokova-Sirosh\"],\"firstnames\":[\"Sofya\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kuznetsov\"],\"firstnames\":[\"Vladimir\",\"L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Romanenko\"],\"firstnames\":[\"Anatoly\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kazakova\"],\"firstnames\":[\"Mariya\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Krasnikov\"],\"firstnames\":[\"Dmitry\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tkachev\"],\"firstnames\":[\"Evgeniy\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yuri\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Obraztsova\"],\"firstnames\":[\"Elena\",\"D.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2016\",\"note\":\"Publisher: SPIE\",\"pages\":\"012526\",\"bibtex\":\"@article{bokova-sirosh_investigation_2016,\\n\\ttitle = {Investigation of defectiveness of multiwalled carbon nanotubes produced with {Fe}–{Co} catalysts of different composition},\\n\\tvolume = {10},\\n\\tissn = {1934-2608, 1934-2608},\\n\\turl = {https://www.spiedigitallibrary.org/journals/journal-of-nanophotonics/volume-10/issue-1/012526/Investigation-of-defectiveness-of-multiwalled-carbon-nanotubes-produced-with-FeCo/10.1117/1.JNP.10.012526.full},\\n\\tdoi = {10.1117/1.JNP.10.012526},\\n\\tabstract = {We have performed a study of CVD multiwalled carbon nanotubes (MWCNTs) produced with Fe–Co catalysts with a variable ratio of active metals. The Raman data were considered in combination with the temperature dependence of MWCNT conductivity. The data analysis is based on the point that the value of I2D/ID ratio correlates with the graphene fragment size. The fragments are considered as building blocks of MWCNTs. We showed that MWCNT defectiveness depends on the ratio of bimetallic active components in the Fe–Co catalyst. Thus, the ratio of I2D/ID increases and the D-mode intensity decreases while the Fe content in the catalyst increases. This also points to the reduction of defect number in the bigger graphene fragments. These results correlate with the data on conductivity temperature dependence. Namely, the increase of Fe content in the active component of the Fe–Co catalyst results in the increase of charge carrier concentration, which, in turn, indicates a decrease in MWCNT defectiveness.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Nanophotonics},\\n\\tauthor = {Bokova-Sirosh, Sofya N. and Kuznetsov, Vladimir L. and Romanenko, Anatoly I. and Kazakova, Mariya A. and Krasnikov, Dmitry V. and Tkachev, Evgeniy N. and Yuzyuk, Yuri I. and Obraztsova, Elena D.},\\n\\tmonth = mar,\\n\\tyear = {2016},\\n\\tnote = {Publisher: SPIE},\\n\\tpages = {012526},\\n}\\n\\n\",\"author_short\":[\"Bokova-Sirosh, S. N.\",\"Kuznetsov, V. L.\",\"Romanenko, A. I.\",\"Kazakova, M. A.\",\"Krasnikov, D. V.\",\"Tkachev, E. N.\",\"Yuzyuk, Y. I.\",\"Obraztsova, E. D.\"],\"key\":\"bokova-sirosh_investigation_2016\",\"id\":\"bokova-sirosh_investigation_2016\",\"bibbaseid\":\"bokovasirosh-kuznetsov-romanenko-kazakova-krasnikov-tkachev-yuzyuk-obraztsova-investigationofdefectivenessofmultiwalledcarbonnanotubesproducedwithfecocatalystsofdifferentcomposition-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.spiedigitallibrary.org/journals/journal-of-nanophotonics/volume-10/issue-1/012526/Investigation-of-defectiveness-of-multiwalled-carbon-nanotubes-produced-with-FeCo/10.1117/1.JNP.10.012526.full\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Soft spherical nanostructures with a dodecagonal quasicrystal-like order\",\"volume\":\"12\",\"issn\":\"1744-6848\",\"url\":\"https://pubs.rsc.org/en/content/articlelanding/2016/sm/c5sm02265g\",\"doi\":\"10.1039/C5SM02265G\",\"abstract\":\"We develop a theory which predicts curvature-related structural peculiarities of soft spherical nanostructures with a dodecagonal local arrangement of subunits. Spherical templates coated with a thin film of a soft quasicrystal (QC)-forming material constitute the most promising direction to realize these nanostructures. Disordered and perfect spherical nanostructures are simulated using two approaches. The first of them models a random QC-like spherical nanostructure with extended curvature-induced topological defects similar to scars in colloidal spherical crystals. The second approach is inspired by the physics of viral capsids. It deals with the most regular spherical nanostructures with a local QC-like order derived from three well-known planar dodecagonal tilings. We explain how the additional QC-like degrees of freedom assist the nanostructure stabilization and determine the point defect number and location without extended scar formation. Unusual for nanoassemblies snub cube geometry is shown to be the most energetically favorable global organization of these spherical QC nanostructures.\",\"language\":\"en\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Soft Matter\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Konevtsova\"],\"firstnames\":[\"O.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shevchenko\"],\"firstnames\":[\"I.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorman\"],\"firstnames\":[\"V.\",\"L.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2016\",\"note\":\"Publisher: The Royal Society of Chemistry\",\"pages\":\"1238–1247\",\"bibtex\":\"@article{rochal_soft_2016,\\n\\ttitle = {Soft spherical nanostructures with a dodecagonal quasicrystal-like order},\\n\\tvolume = {12},\\n\\tissn = {1744-6848},\\n\\turl = {https://pubs.rsc.org/en/content/articlelanding/2016/sm/c5sm02265g},\\n\\tdoi = {10.1039/C5SM02265G},\\n\\tabstract = {We develop a theory which predicts curvature-related structural peculiarities of soft spherical nanostructures with a dodecagonal local arrangement of subunits. Spherical templates coated with a thin film of a soft quasicrystal (QC)-forming material constitute the most promising direction to realize these nanostructures. Disordered and perfect spherical nanostructures are simulated using two approaches. The first of them models a random QC-like spherical nanostructure with extended curvature-induced topological defects similar to scars in colloidal spherical crystals. The second approach is inspired by the physics of viral capsids. It deals with the most regular spherical nanostructures with a local QC-like order derived from three well-known planar dodecagonal tilings. We explain how the additional QC-like degrees of freedom assist the nanostructure stabilization and determine the point defect number and location without extended scar formation. Unusual for nanoassemblies snub cube geometry is shown to be the most energetically favorable global organization of these spherical QC nanostructures.},\\n\\tlanguage = {en},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Soft Matter},\\n\\tauthor = {Rochal, S. B. and Konevtsova, O. V. and Shevchenko, I. A. and Lorman, V. L.},\\n\\tmonth = jan,\\n\\tyear = {2016},\\n\\tnote = {Publisher: The Royal Society of Chemistry},\\n\\tpages = {1238--1247},\\n}\\n\\n\",\"author_short\":[\"Rochal, S. B.\",\"Konevtsova, O. V.\",\"Shevchenko, I. A.\",\"Lorman, V. L.\"],\"key\":\"rochal_soft_2016\",\"id\":\"rochal_soft_2016\",\"bibbaseid\":\"rochal-konevtsova-shevchenko-lorman-softsphericalnanostructureswithadodecagonalquasicrystallikeorder-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://pubs.rsc.org/en/content/articlelanding/2016/sm/c5sm02265g\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Effect of growth mechanisms on the deformation of a unit cell and polarization reversal in barium–strontium titanate heterostructures on magnesium oxide\",\"volume\":\"61\",\"issn\":\"1090-6525\",\"url\":\"https://doi.org/10.1134/S106378421601014X\",\"doi\":\"10.1134/S106378421601014X\",\"abstract\":\"The effect of a growth mechanism on the unit cell strain and the related change in the properties of single-crystal Ba0.8Sr0.2TiO3 films grown on MgO substrates according to the Frank–van der Merwe and Volmer–Weber growth mechanisms is studied. The unit cell strain is shown to depend substantially on the film thickness and the growth mechanism. It is found that the same film–substrate pair can be used to vary stresses in the film from two-dimensional tensile to compressive stresses due to a change in the growth mechanism and the film thickness.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Technical Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Mukhortov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golovko\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Biryukov\"],\"firstnames\":[\"S.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Anokhin\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2016\",\"keywords\":\"Strontium Titanate, Growth Mechanism, Paraelectric Phase, Remanent Polarization, Substrate Plane\",\"pages\":\"91–96\",\"bibtex\":\"@article{mukhortov_effect_2016,\\n\\ttitle = {Effect of growth mechanisms on the deformation of a unit cell and polarization reversal in barium–strontium titanate heterostructures on magnesium oxide},\\n\\tvolume = {61},\\n\\tissn = {1090-6525},\\n\\turl = {https://doi.org/10.1134/S106378421601014X},\\n\\tdoi = {10.1134/S106378421601014X},\\n\\tabstract = {The effect of a growth mechanism on the unit cell strain and the related change in the properties of single-crystal Ba0.8Sr0.2TiO3 films grown on MgO substrates according to the Frank–van der Merwe and Volmer–Weber growth mechanisms is studied. The unit cell strain is shown to depend substantially on the film thickness and the growth mechanism. It is found that the same film–substrate pair can be used to vary stresses in the film from two-dimensional tensile to compressive stresses due to a change in the growth mechanism and the film thickness.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Technical Physics},\\n\\tauthor = {Mukhortov, V. M. and Golovko, Yu. I. and Biryukov, S. V. and Anokhin, A. and Yuzyuk, Yu. I.},\\n\\tmonth = jan,\\n\\tyear = {2016},\\n\\tkeywords = {Strontium Titanate, Growth Mechanism, Paraelectric Phase, Remanent Polarization, Substrate Plane},\\n\\tpages = {91--96},\\n}\\n\\n\",\"author_short\":[\"Mukhortov, V. M.\",\"Golovko, Y. I.\",\"Biryukov, S. V.\",\"Anokhin, A.\",\"Yuzyuk, Y. I.\"],\"key\":\"mukhortov_effect_2016\",\"id\":\"mukhortov_effect_2016\",\"bibbaseid\":\"mukhortov-golovko-biryukov-anokhin-yuzyuk-effectofgrowthmechanismsonthedeformationofaunitcellandpolarizationreversalinbariumstrontiumtitanateheterostructuresonmagnesiumoxide-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S106378421601014X\"},\"keyword\":[\"Strontium Titanate\",\"Growth Mechanism\",\"Paraelectric Phase\",\"Remanent Polarization\",\"Substrate Plane\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Relaxation of interstitials in spherical colloidal crystals\",\"volume\":\"75\",\"issn\":\"1386-9477\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S1386947715302174\",\"doi\":\"10.1016/j.physe.2015.09.036\",\"abstract\":\"Spherical colloidal crystals (CCs) self-assemble on the interface between two liquids. These 2D structures unconventionally combine local hexagonal order and spherical geometry. Nowadays CCs are actively studied by altering their structures. However, the statistical analysis of such experiments results is limited by uniqueness of self-assembled structures and their short lifetime. Here we perform numerical experiments to investigate pathways of CC structure relaxation after the intrusion of interstitial. The process is simulated in the frames of overdamped molecular dynamics method. The relaxation occurs due to interaction with extended topological defects (ETDs) mandatory induced in spherical CCs by their intrinsic Gaussian curvature. Types of relaxation pathways are classified and their probabilities are estimated in the low-temperature region. To analyze the structural changes during the relaxation we use a parent phase approach allowing us to describe the global organization of spherical order. This organization is preserved by only the most typical relaxation pathway resulting in filling one of vacancies integrated inside the ETD areas. In contrast with this pathway the other ones shift the ETDs centers and can strongly reconstruct the internal structure of ETDs. Temperature dependence of the relaxation processes and the mechanism of dislocation unbinding are discussed. Common peculiarities in relaxation of spherical structures and particular fragments of planar hexagonal lattice are found.\",\"urldate\":\"2023-11-11\",\"journal\":\"Physica E: Low-dimensional Systems and Nanostructures\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Roshal\"],\"firstnames\":[\"D.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Myasnikova\"],\"firstnames\":[\"A.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2016\",\"keywords\":\"Topological defects, Self-assembly, Interstitial, Parent phase, Relaxation, Spherical colloidal crystals\",\"pages\":\"295–301\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\BC5X78BR\\\\\\\\Roshal и др. - 2016 - Relaxation of interstitials in spherical colloidal.pdf:application/pdf\",\"bibtex\":\"@article{roshal_relaxation_2016,\\n\\ttitle = {Relaxation of interstitials in spherical colloidal crystals},\\n\\tvolume = {75},\\n\\tissn = {1386-9477},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S1386947715302174},\\n\\tdoi = {10.1016/j.physe.2015.09.036},\\n\\tabstract = {Spherical colloidal crystals (CCs) self-assemble on the interface between two liquids. These 2D structures unconventionally combine local hexagonal order and spherical geometry. Nowadays CCs are actively studied by altering their structures. However, the statistical analysis of such experiments results is limited by uniqueness of self-assembled structures and their short lifetime. Here we perform numerical experiments to investigate pathways of CC structure relaxation after the intrusion of interstitial. The process is simulated in the frames of overdamped molecular dynamics method. The relaxation occurs due to interaction with extended topological defects (ETDs) mandatory induced in spherical CCs by their intrinsic Gaussian curvature. Types of relaxation pathways are classified and their probabilities are estimated in the low-temperature region. To analyze the structural changes during the relaxation we use a parent phase approach allowing us to describe the global organization of spherical order. This organization is preserved by only the most typical relaxation pathway resulting in filling one of vacancies integrated inside the ETD areas. In contrast with this pathway the other ones shift the ETDs centers and can strongly reconstruct the internal structure of ETDs. Temperature dependence of the relaxation processes and the mechanism of dislocation unbinding are discussed. Common peculiarities in relaxation of spherical structures and particular fragments of planar hexagonal lattice are found.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physica E: Low-dimensional Systems and Nanostructures},\\n\\tauthor = {Roshal, D. S. and Myasnikova, A. E. and Rochal, S. B.},\\n\\tmonth = jan,\\n\\tyear = {2016},\\n\\tkeywords = {Topological defects, Self-assembly, Interstitial, Parent phase, Relaxation, Spherical colloidal crystals},\\n\\tpages = {295--301},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\BC5X78BR\\\\\\\\Roshal и др. - 2016 - Relaxation of interstitials in spherical colloidal.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Roshal, D. S.\",\"Myasnikova, A. E.\",\"Rochal, S. B.\"],\"key\":\"roshal_relaxation_2016\",\"id\":\"roshal_relaxation_2016\",\"bibbaseid\":\"roshal-myasnikova-rochal-relaxationofinterstitialsinsphericalcolloidalcrystals-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S1386947715302174\"},\"keyword\":[\"Topological defects\",\"Self-assembly\",\"Interstitial\",\"Parent phase\",\"Relaxation\",\"Spherical colloidal crystals\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Электрофизические свойства шестикомпонентного состава сегнетомягкой керамики на основе ЦТС\",\"volume\":\"80\",\"issn\":\"0367-6765\",\"url\":\"https://elibrary.ru/item.asp?doi=10.7868/S0367676516090039\",\"doi\":\"10.7868/S0367676516090039\",\"abstract\":\"Изучены свойства шестикомпонентного состава сегнетомягкой керамики на основе ЦТС. Установлено, что этот состав проявляет свойства сегнетоэлектрика-релаксора. В сегнетоэлекрической фазе материала обнаружен фазовый переход между двумя ромбоэдрическими фазами R3c → R3m. Поляризация образцов постоянным электрическим полем при охлаждении через точку Кюри расширяет температурный интервал существования фазы R3m по сравнению с поляризацией при комнатной температуре.\",\"language\":\"ru\",\"number\":\"9\",\"urldate\":\"2023-11-11\",\"journal\":\"Известия Российской Академии Наук. Серия Физическая\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Акбаева\"],\"firstnames\":[\"Г.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гавриляченко\"],\"firstnames\":[\"В.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Захаров\"],\"firstnames\":[\"Ю.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лутохин\"],\"firstnames\":[\"А.\",\"Г.\"],\"suffixes\":[]}],\"year\":\"2016\",\"pages\":\"1179–1182\",\"bibtex\":\"@article{__2016,\\n\\ttitle = {Электрофизические свойства шестикомпонентного состава сегнетомягкой керамики на основе ЦТС},\\n\\tvolume = {80},\\n\\tissn = {0367-6765},\\n\\turl = {https://elibrary.ru/item.asp?doi=10.7868/S0367676516090039},\\n\\tdoi = {10.7868/S0367676516090039},\\n\\tabstract = {Изучены свойства шестикомпонентного состава сегнетомягкой керамики на основе ЦТС. Установлено, что этот состав проявляет свойства сегнетоэлектрика-релаксора. В сегнетоэлекрической фазе материала обнаружен фазовый переход между двумя ромбоэдрическими фазами R3c → R3m. Поляризация образцов постоянным электрическим полем при охлаждении через точку Кюри расширяет температурный интервал существования фазы R3m по сравнению с поляризацией при комнатной температуре.},\\n\\tlanguage = {ru},\\n\\tnumber = {9},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Известия Российской Академии Наук. Серия Физическая},\\n\\tauthor = {Акбаева, Г. М. and Гавриляченко, В. Г. and Захаров, Ю. Н. and Лутохин, А. Г.},\\n\\tyear = {2016},\\n\\tpages = {1179--1182},\\n}\\n\\n\",\"author_short\":[\"Акбаева, Г. М.\",\"Гавриляченко, В. Г.\",\"Захаров, Ю. Н.\",\"Лутохин, А. Г.\"],\"key\":\"__2016\",\"id\":\"__2016\",\"bibbaseid\":\"-----2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?doi=10.7868/S0367676516090039\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":1,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Study of collective radial breathing-like modes in double-walled carbon nanotubes: combination of continuous two-dimensional membrane theory and Raman spectroscopy\",\"volume\":\"10\",\"issn\":\"1934-2608, 1934-2608\",\"shorttitle\":\"Study of collective radial breathing-like modes in double-walled carbon nanotubes\",\"url\":\"https://www.spiedigitallibrary.org/journals/journal-of-nanophotonics/volume-10/issue-1/012502/Study-of-collective-radial-breathing-like-modes-in-double-walled/10.1117/1.JNP.10.012502.full\",\"doi\":\"10.1117/1.JNP.10.012502\",\"abstract\":\"Radial breathing modes (RBMs) are widely used for the atomic structure characterization and index assignment of single-walled carbon nanotubes (SWNTs) from resonant Raman spectroscopy. However, for double-walled carbon nanotubes (DWNTs), the use of conventional ωRBM(d) formulas is complicated due to the van der Waals interaction between the layers, which strongly affects the frequencies of radial modes and leads to new collective vibrations. This paper presents an alternative way to theoretically study the collective radial breathing-like modes (RBLMs) of DWNTs and to account for interlayer interaction, namely the continuous two-dimensional membrane theory. We obtain an analytical ωRBLM(do,di) relation, being the equivalent of the conventional ωRBM(d) expressions, established for SWNTs. We compare our theoretical predictions with Raman data, measured on individual index-identified suspended DWNTs, and find a good agreement between experiment and theory. Moreover, we show that the interlayer coupling in individual DWNTs strongly depends on the interlayer distance, which is manifested in the frequency shifts of the RBLMs with respect to the RBMs of the individual inner and outer tubes. In terms of characterization, this means that the combination of Raman spectroscopy data and predictions of continuous membrane theory may give additional criteria for the index identification of DWNTs, namely the interlayer distance.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Nanophotonics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Levshov\"],\"firstnames\":[\"Dmitry\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Avramenko\"],\"firstnames\":[\"Marina\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Than\"],\"firstnames\":[\"Xuan-Tinh\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Michel\"],\"firstnames\":[\"Thierry\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Arenal\"],\"firstnames\":[\"Raul\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Paillet\"],\"firstnames\":[\"Matthieu\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rybkovskiy\"],\"firstnames\":[\"Dmitry\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Osadchy\"],\"firstnames\":[\"Alexander\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergei\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yuri\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sauvajol\"],\"firstnames\":[\"Jean-Louis\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2015\",\"note\":\"Publisher: SPIE\",\"pages\":\"012502\",\"bibtex\":\"@article{levshov_study_2015,\\n\\ttitle = {Study of collective radial breathing-like modes in double-walled carbon nanotubes: combination of continuous two-dimensional membrane theory and {Raman} spectroscopy},\\n\\tvolume = {10},\\n\\tissn = {1934-2608, 1934-2608},\\n\\tshorttitle = {Study of collective radial breathing-like modes in double-walled carbon nanotubes},\\n\\turl = {https://www.spiedigitallibrary.org/journals/journal-of-nanophotonics/volume-10/issue-1/012502/Study-of-collective-radial-breathing-like-modes-in-double-walled/10.1117/1.JNP.10.012502.full},\\n\\tdoi = {10.1117/1.JNP.10.012502},\\n\\tabstract = {Radial breathing modes (RBMs) are widely used for the atomic structure characterization and index assignment of single-walled carbon nanotubes (SWNTs) from resonant Raman spectroscopy. However, for double-walled carbon nanotubes (DWNTs), the use of conventional ωRBM(d) formulas is complicated due to the van der Waals interaction between the layers, which strongly affects the frequencies of radial modes and leads to new collective vibrations. This paper presents an alternative way to theoretically study the collective radial breathing-like modes (RBLMs) of DWNTs and to account for interlayer interaction, namely the continuous two-dimensional membrane theory. We obtain an analytical ωRBLM(do,di) relation, being the equivalent of the conventional ωRBM(d) expressions, established for SWNTs. We compare our theoretical predictions with Raman data, measured on individual index-identified suspended DWNTs, and find a good agreement between experiment and theory. Moreover, we show that the interlayer coupling in individual DWNTs strongly depends on the interlayer distance, which is manifested in the frequency shifts of the RBLMs with respect to the RBMs of the individual inner and outer tubes. In terms of characterization, this means that the combination of Raman spectroscopy data and predictions of continuous membrane theory may give additional criteria for the index identification of DWNTs, namely the interlayer distance.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Nanophotonics},\\n\\tauthor = {Levshov, Dmitry I. and Avramenko, Marina V. and Than, Xuan-Tinh and Michel, Thierry and Arenal, Raul and Paillet, Matthieu and Rybkovskiy, Dmitry V. and Osadchy, Alexander V. and Rochal, Sergei B. and Yuzyuk, Yuri I. and Sauvajol, Jean-Louis},\\n\\tmonth = sep,\\n\\tyear = {2015},\\n\\tnote = {Publisher: SPIE},\\n\\tpages = {012502},\\n}\\n\\n\",\"author_short\":[\"Levshov, D. I.\",\"Avramenko, M. V.\",\"Than, X.\",\"Michel, T.\",\"Arenal, R.\",\"Paillet, M.\",\"Rybkovskiy, D. V.\",\"Osadchy, A. V.\",\"Rochal, S. B.\",\"Yuzyuk, Y. I.\",\"Sauvajol, J.\"],\"key\":\"levshov_study_2015\",\"id\":\"levshov_study_2015\",\"bibbaseid\":\"levshov-avramenko-than-michel-arenal-paillet-rybkovskiy-osadchy-etal-studyofcollectiveradialbreathinglikemodesindoublewalledcarbonnanotubescombinationofcontinuoustwodimensionalmembranetheoryandramanspectroscopy-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.spiedigitallibrary.org/journals/journal-of-nanophotonics/volume-10/issue-1/012502/Study-of-collective-radial-breathing-like-modes-in-double-walled/10.1117/1.JNP.10.012502.full\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Novel nanostructures of ZnO for nanoscale photonics, optoelectronics, piezoelectricity, and sensing\",\"volume\":\"88\",\"issn\":\"0947-8396, 1432-0630\",\"url\":\"http://link.springer.com/10.1007/s00339-007-3942-8\",\"doi\":\"10.1007/s00339-007-3942-8\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Applied Physics A\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Wang\"],\"firstnames\":[\"Z.L.\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2007\",\"pages\":\"7–15\",\"bibtex\":\"@article{wang_novel_2007,\\n\\ttitle = {Novel nanostructures of {ZnO} for nanoscale photonics, optoelectronics, piezoelectricity, and sensing},\\n\\tvolume = {88},\\n\\tissn = {0947-8396, 1432-0630},\\n\\turl = {http://link.springer.com/10.1007/s00339-007-3942-8},\\n\\tdoi = {10.1007/s00339-007-3942-8},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Applied Physics A},\\n\\tauthor = {Wang, Z.L.},\\n\\tmonth = may,\\n\\tyear = {2007},\\n\\tpages = {7--15},\\n}\\n\\n\",\"author_short\":[\"Wang, Z.\"],\"key\":\"wang_novel_2007\",\"id\":\"wang_novel_2007\",\"bibbaseid\":\"wang-novelnanostructuresofznofornanoscalephotonicsoptoelectronicspiezoelectricityandsensing-2007\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://link.springer.com/10.1007/s00339-007-3942-8\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"address\":\"Cham\",\"series\":\"Springer Proceedings in Physics\",\"title\":\"Dispersion Characteristics of Zinc Oxide Nanorods Coated with Thin Silver Layer and Organized in Two-Dimensional Uniform Arrays\",\"isbn\":\"978-3-319-26324-3\",\"doi\":\"10.1007/978-3-319-26324-3_22\",\"abstract\":\"The problem on electromagnetic waves propagation in a two-dimensional periodic array of zinc oxide nano-waveguides covered with a thin metal film is solved by the method of variables separationMethod of variables separationin cylindrical coordinates. The numerical results obtained by the method are in good agreement with the results computed by the commercial software COMSOL MultiphysicsTM over all optical range and have minor deviations for the wavelength range close to the critical wavelength. Resonances located at the amplitude-frequency characteristics of optical nano-antennas may be interpreted as resonances of circular bilayer nano-wave-guide segments with the ZnO core covered with thin metal shell. The results may also be used to predict the resonance wavelength of two-dimensional periodic arrays of ZnO nanorodsZnO nanorods, coated with a thin metal layer and grown on a dielectric substrate.\",\"language\":\"en\",\"booktitle\":\"Advanced Materials\",\"publisher\":\"Springer International Publishing\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Lerer\"],\"firstnames\":[\"A.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Puzanov\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chernikova\"],\"firstnames\":[\"T.\",\"Y.\"],\"suffixes\":[]}],\"editor\":[{\"propositions\":[],\"lastnames\":[\"Parinov\"],\"firstnames\":[\"Ivan\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chang\"],\"firstnames\":[\"Shun-Hsyung\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Topolov\"],\"firstnames\":[\"Vitaly\",\"Yu.\"],\"suffixes\":[]}],\"year\":\"2016\",\"keywords\":\"Complex Dielectric Constant, Critical Wavelength, Resonant Wavelength, Thin Metal Film, Unknown Coefficient\",\"pages\":\"317–327\",\"bibtex\":\"@inproceedings{lerer_dispersion_2016-1,\\n\\taddress = {Cham},\\n\\tseries = {Springer {Proceedings} in {Physics}},\\n\\ttitle = {Dispersion {Characteristics} of {Zinc} {Oxide} {Nanorods} {Coated} with {Thin} {Silver} {Layer} and {Organized} in {Two}-{Dimensional} {Uniform} {Arrays}},\\n\\tisbn = {978-3-319-26324-3},\\n\\tdoi = {10.1007/978-3-319-26324-3_22},\\n\\tabstract = {The problem on electromagnetic waves propagation in a two-dimensional periodic array of zinc oxide nano-waveguides covered with a thin metal film is solved by the method of variables separationMethod of variables separationin cylindrical coordinates. The numerical results obtained by the method are in good agreement with the results computed by the commercial software COMSOL MultiphysicsTM over all optical range and have minor deviations for the wavelength range close to the critical wavelength. Resonances located at the amplitude-frequency characteristics of optical nano-antennas may be interpreted as resonances of circular bilayer nano-wave-guide segments with the ZnO core covered with thin metal shell. The results may also be used to predict the resonance wavelength of two-dimensional periodic arrays of ZnO nanorodsZnO nanorods, coated with a thin metal layer and grown on a dielectric substrate.},\\n\\tlanguage = {en},\\n\\tbooktitle = {Advanced {Materials}},\\n\\tpublisher = {Springer International Publishing},\\n\\tauthor = {Lerer, A. M. and Timoshenko, P. E. and Kaidashev, E. M. and Puzanov, A. S. and Chernikova, T. Y.},\\n\\teditor = {Parinov, Ivan A. and Chang, Shun-Hsyung and Topolov, Vitaly Yu.},\\n\\tyear = {2016},\\n\\tkeywords = {Complex Dielectric Constant, Critical Wavelength, Resonant Wavelength, Thin Metal Film, Unknown Coefficient},\\n\\tpages = {317--327},\\n}\\n\\n\",\"author_short\":[\"Lerer, A. M.\",\"Timoshenko, P. E.\",\"Kaidashev, E. M.\",\"Puzanov, A. S.\",\"Chernikova, T. Y.\"],\"editor_short\":[\"Parinov, I. A.\",\"Chang, S.\",\"Topolov, V. Y.\"],\"key\":\"lerer_dispersion_2016-1\",\"id\":\"lerer_dispersion_2016-1\",\"bibbaseid\":\"lerer-timoshenko-kaidashev-puzanov-chernikova-dispersioncharacteristicsofzincoxidenanorodscoatedwiththinsilverlayerandorganizedintwodimensionaluniformarrays-2016\",\"role\":\"author\",\"urls\":{},\"keyword\":[\"Complex Dielectric Constant\",\"Critical Wavelength\",\"Resonant Wavelength\",\"Thin Metal Film\",\"Unknown Coefficient\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Anomalous change in the material moduli of thin films of barium titanate\",\"volume\":\"56\",\"issn\":\"1573-8620\",\"url\":\"https://doi.org/10.1134/S0021894415060218\",\"doi\":\"10.1134/S0021894415060218\",\"abstract\":\"A method is proposed to determine the moduli of thin ferroelectric films subjected to forced deformation due to the mismatch between the crystal lattice sizes of the film and substrate materials and the difference of their thermal expansion coefficients. Models of single-crystal films of barium titanate are studied using the eighth-degree Landau thermodynamic potential. It is shown that in the considered range of forced strain of the barium titanate film, three main states exist: a tetragonal phase (c phase) of 4mm symmetry with spontaneous polarization directed along the normal to the film plane; an orthorhombic phase (aa phase) of 2 mm symmetry with polarization oriented along the diagonal plane of the film; monoclinic phase (r phase) of Cmsymmetry with the intermediate direction of polarization. All phases are separated by the lines of transitions of the second kind. Dependences of the elastic, electric and piezoelectric moduli on the magnitude of forced strain are plotted. It is shown that at the phase boundaries there is an anomalous change in the constants of the ferroelectric film and in the region of existence of the r phase, some moduli reach extreme values.\",\"language\":\"en\",\"number\":\"6\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Applied Mechanics and Technical Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kalinchuk\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shakhovoi\"],\"firstnames\":[\"R.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2015\",\"keywords\":\"thin films, elastic moduli, ferroelectrics, forced strain, material constants, piezoelectric moduli\",\"pages\":\"1103–1110\",\"bibtex\":\"@article{shirokov_anomalous_2015,\\n\\ttitle = {Anomalous change in the material moduli of thin films of barium titanate},\\n\\tvolume = {56},\\n\\tissn = {1573-8620},\\n\\turl = {https://doi.org/10.1134/S0021894415060218},\\n\\tdoi = {10.1134/S0021894415060218},\\n\\tabstract = {A method is proposed to determine the moduli of thin ferroelectric films subjected to forced deformation due to the mismatch between the crystal lattice sizes of the film and substrate materials and the difference of their thermal expansion coefficients. Models of single-crystal films of barium titanate are studied using the eighth-degree Landau thermodynamic potential. It is shown that in the considered range of forced strain of the barium titanate film, three main states exist: a tetragonal phase (c phase) of 4mm symmetry with spontaneous polarization directed along the normal to the film plane; an orthorhombic phase (aa phase) of 2 mm symmetry with polarization oriented along the diagonal plane of the film; monoclinic phase (r phase) of Cmsymmetry with the intermediate direction of polarization. All phases are separated by the lines of transitions of the second kind. Dependences of the elastic, electric and piezoelectric moduli on the magnitude of forced strain are plotted. It is shown that at the phase boundaries there is an anomalous change in the constants of the ferroelectric film and in the region of existence of the r phase, some moduli reach extreme values.},\\n\\tlanguage = {en},\\n\\tnumber = {6},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Applied Mechanics and Technical Physics},\\n\\tauthor = {Shirokov, V. B. and Kalinchuk, V. V. and Shakhovoi, R. A. and Yuzyuk, Yu. I.},\\n\\tmonth = nov,\\n\\tyear = {2015},\\n\\tkeywords = {thin films, elastic moduli, ferroelectrics, forced strain, material constants, piezoelectric moduli},\\n\\tpages = {1103--1110},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Kalinchuk, V. V.\",\"Shakhovoi, R. A.\",\"Yuzyuk, Y. I.\"],\"key\":\"shirokov_anomalous_2015\",\"id\":\"shirokov_anomalous_2015\",\"bibbaseid\":\"shirokov-kalinchuk-shakhovoi-yuzyuk-anomalouschangeinthematerialmoduliofthinfilmsofbariumtitanate-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S0021894415060218\"},\"keyword\":[\"thin films\",\"elastic moduli\",\"ferroelectrics\",\"forced strain\",\"material constants\",\"piezoelectric moduli\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Characterization of the electrocatalytic activity of carbon-supported platinum-based catalysts by thermal gravimetric analysis\",\"volume\":\"25\",\"issn\":\"0959-9436\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0959943615002229\",\"doi\":\"10.1016/j.mencom.2015.11.024\",\"abstract\":\"Investigations of carbon-supported Pt, Pt3Co, and Pt3Ni electrocatalysts using thermal gravimetric analysis (TGA) in combination with electrochemical measurements of the membrane electrode assemblies (MEA) for proton exchange membrane fuel cells have demonstrated that the onset temperature of the carbon support thermal oxidation and apparent activation energy of this reaction decrease in the following orders: Pt(20%)/C \\\\textgreater Pt(35%)/C \\\\textgreater Pt(46%)/C and Pt3Ni/C \\\\textgreater Pt3Co/C \\\\textgreater Pt/C, while MEA power density increases. Thus, TGA can be used as a simple and express technique for analysis of the electrocatalytic activity of carbon-supported Pt-based catalysts for proton exchange membrane fuel cells.\",\"number\":\"6\",\"urldate\":\"2023-11-11\",\"journal\":\"Mendeleev Communications\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyeva\"],\"firstnames\":[\"Daria\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"Alexandra\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Popov\"],\"firstnames\":[\"Yurii\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"Olga\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Glebova\"],\"firstnames\":[\"Nadezhda\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nechitailov\"],\"firstnames\":[\"Andrei\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zelenina\"],\"firstnames\":[\"Natalia\",\"K.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tomasov\"],\"firstnames\":[\"Alexander\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hennet\"],\"firstnames\":[\"Louis\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\",\"V.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2015\",\"pages\":\"468–469\",\"bibtex\":\"@article{leontyev_characterization_2015,\\n\\ttitle = {Characterization of the electrocatalytic activity of carbon-supported platinum-based catalysts by thermal gravimetric analysis},\\n\\tvolume = {25},\\n\\tissn = {0959-9436},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0959943615002229},\\n\\tdoi = {10.1016/j.mencom.2015.11.024},\\n\\tabstract = {Investigations of carbon-supported Pt, Pt3Co, and Pt3Ni electrocatalysts using thermal gravimetric analysis (TGA) in combination with electrochemical measurements of the membrane electrode assemblies (MEA) for proton exchange membrane fuel cells have demonstrated that the onset temperature of the carbon support thermal oxidation and apparent activation energy of this reaction decrease in the following orders: Pt(20\\\\%)/C {\\\\textgreater} Pt(35\\\\%)/C {\\\\textgreater} Pt(46\\\\%)/C and Pt3Ni/C {\\\\textgreater} Pt3Co/C {\\\\textgreater} Pt/C, while MEA power density increases. Thus, TGA can be used as a simple and express technique for analysis of the electrocatalytic activity of carbon-supported Pt-based catalysts for proton exchange membrane fuel cells.},\\n\\tnumber = {6},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Mendeleev Communications},\\n\\tauthor = {Leontyev, Igor N. and Leontyeva, Daria V. and Kuriganova, Alexandra B. and Popov, Yurii V. and Maslova, Olga A. and Glebova, Nadezhda V. and Nechitailov, Andrei A. and Zelenina, Natalia K. and Tomasov, Alexander A. and Hennet, Louis and Smirnova, Nina V.},\\n\\tmonth = nov,\\n\\tyear = {2015},\\n\\tpages = {468--469},\\n}\\n\\n\",\"author_short\":[\"Leontyev, I. N.\",\"Leontyeva, D. V.\",\"Kuriganova, A. B.\",\"Popov, Y. V.\",\"Maslova, O. A.\",\"Glebova, N. V.\",\"Nechitailov, A. A.\",\"Zelenina, N. K.\",\"Tomasov, A. A.\",\"Hennet, L.\",\"Smirnova, N. V.\"],\"key\":\"leontyev_characterization_2015\",\"id\":\"leontyev_characterization_2015\",\"bibbaseid\":\"leontyev-leontyeva-kuriganova-popov-maslova-glebova-nechitailov-zelenina-etal-characterizationoftheelectrocatalyticactivityofcarbonsupportedplatinumbasedcatalystsbythermalgravimetricanalysis-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0959943615002229\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Complex instability of axially compressed tubular lipid membrane with controlled spontaneous curvature\",\"volume\":\"38\",\"issn\":\"1292-895X\",\"url\":\"https://doi.org/10.1140/epje/i2015-15112-6\",\"doi\":\"10.1140/epje/i2015-15112-6\",\"abstract\":\"Tubular lipid membranes (TLMs) are formed by an external pulling force from artificial or biological bilayer vesicles and can be subsequently stabilized by incorporating proteins or amphiphilic polymers into the lipid bilayer. The arising spontaneous curvature of the lipid sheet allows switching off the pulling force without TLM destabilization. However, here we show that during this process two different thermal fluctuation modes drastically increase their amplitudes making fluctuations of the TLM much greater than its radius. Due to the system’s proximity to the critical fluctuation point, a weak axial compressive force is sufficient to destabilize the TLM. Its absolute value is shown to be much smaller than that of the pulling force required for the initial lipid nanotube formation. Induced complex instability was studied in the frame of Landau phase transition theory. The process involves two consecutive second-order phase transitions and leads to the tube deformation combining annular corrugation with completely unconventional chiral buckling.\",\"language\":\"en\",\"number\":\"10\",\"urldate\":\"2023-11-11\",\"journal\":\"The European Physical Journal E\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Golushko\"],\"firstnames\":[\"I.\",\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorman\"],\"firstnames\":[\"V.\",\"L.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2015\",\"keywords\":\"Living systems: Biological Matter\",\"pages\":\"112\",\"bibtex\":\"@article{golushko_complex_2015,\\n\\ttitle = {Complex instability of axially compressed tubular lipid membrane with controlled spontaneous curvature},\\n\\tvolume = {38},\\n\\tissn = {1292-895X},\\n\\turl = {https://doi.org/10.1140/epje/i2015-15112-6},\\n\\tdoi = {10.1140/epje/i2015-15112-6},\\n\\tabstract = {Tubular lipid membranes (TLMs) are formed by an external pulling force from artificial or biological bilayer vesicles and can be subsequently stabilized by incorporating proteins or amphiphilic polymers into the lipid bilayer. The arising spontaneous curvature of the lipid sheet allows switching off the pulling force without TLM destabilization. However, here we show that during this process two different thermal fluctuation modes drastically increase their amplitudes making fluctuations of the TLM much greater than its radius. Due to the system’s proximity to the critical fluctuation point, a weak axial compressive force is sufficient to destabilize the TLM. Its absolute value is shown to be much smaller than that of the pulling force required for the initial lipid nanotube formation. Induced complex instability was studied in the frame of Landau phase transition theory. The process involves two consecutive second-order phase transitions and leads to the tube deformation combining annular corrugation with completely unconventional chiral buckling.},\\n\\tlanguage = {en},\\n\\tnumber = {10},\\n\\turldate = {2023-11-11},\\n\\tjournal = {The European Physical Journal E},\\n\\tauthor = {Golushko, I. Yu. and Rochal, S. B. and Lorman, V. L.},\\n\\tmonth = oct,\\n\\tyear = {2015},\\n\\tkeywords = {Living systems: Biological Matter},\\n\\tpages = {112},\\n}\\n\\n\",\"author_short\":[\"Golushko, I. Y.\",\"Rochal, S. B.\",\"Lorman, V. L.\"],\"key\":\"golushko_complex_2015\",\"id\":\"golushko_complex_2015\",\"bibbaseid\":\"golushko-rochal-lorman-complexinstabilityofaxiallycompressedtubularlipidmembranewithcontrolledspontaneouscurvature-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1140/epje/i2015-15112-6\"},\"keyword\":[\"Living systems: Biological Matter\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Interlayer Dependence of G-Modes in Semiconducting Double-Walled Carbon Nanotubes\",\"volume\":\"119\",\"issn\":\"1932-7447\",\"url\":\"https://doi.org/10.1021/acs.jpcc.5b05888\",\"doi\":\"10.1021/acs.jpcc.5b05888\",\"abstract\":\"A double-walled carbon nanotube (DWNT), a coaxial composite of two single-walled carbon nanotubes (SWNT), provides a unique model to study interactions between the two constituent SWNTs. Combining high resolution transmission electron microscopy (HRTEM), electron diffraction (ED), and resonant Raman scattering (RRS) experiments on the same individual suspended DWNT is the ultimate way to relate unambiguously its atomic structure, defined by the chiral indices of the coaxial outer/inner SWNTs, and its Raman-active vibration modes. This approach is used to investigate the intertube distance dependence of the G-modes of individual index-identified DWNTs composed of two semiconducting SWNTs. We state the main features of the dependence of the G-mode frequencies on the distance between the inner and outer layers: (i) When the interlayer distance is larger than the nominal van der Waals distance (close to 0.34 nm), a downshift of the inner-layer G-modes with respect to the G-modes in the equivalent SWNTs is measured. (ii) The amplitude of the downshift depends on the interlayer distance, or in other words, on the negative pressure felt by the inner layer in DWNT. (iii) No shift is observed for an intertube distance close to 0.34 nm.\",\"number\":\"40\",\"urldate\":\"2023-11-11\",\"journal\":\"The Journal of Physical Chemistry C\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Levshov\"],\"firstnames\":[\"D.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Michel\"],\"firstnames\":[\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Arenal\"],\"firstnames\":[\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tran\"],\"firstnames\":[\"H.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Than\"],\"firstnames\":[\"T.\",\"X.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Paillet\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sauvajol\"],\"firstnames\":[\"J.-L.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2015\",\"note\":\"Publisher: American Chemical Society\",\"pages\":\"23196–23202\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\M5V5TPZR\\\\Łevshov и др. - 2015 - Interlayer Dependence of G-Modes in Semiconducting.pdf:application/pdf\",\"bibtex\":\"@article{levshov_interlayer_2015,\\n\\ttitle = {Interlayer {Dependence} of {G}-{Modes} in {Semiconducting} {Double}-{Walled} {Carbon} {Nanotubes}},\\n\\tvolume = {119},\\n\\tissn = {1932-7447},\\n\\turl = {https://doi.org/10.1021/acs.jpcc.5b05888},\\n\\tdoi = {10.1021/acs.jpcc.5b05888},\\n\\tabstract = {A double-walled carbon nanotube (DWNT), a coaxial composite of two single-walled carbon nanotubes (SWNT), provides a unique model to study interactions between the two constituent SWNTs. Combining high resolution transmission electron microscopy (HRTEM), electron diffraction (ED), and resonant Raman scattering (RRS) experiments on the same individual suspended DWNT is the ultimate way to relate unambiguously its atomic structure, defined by the chiral indices of the coaxial outer/inner SWNTs, and its Raman-active vibration modes. This approach is used to investigate the intertube distance dependence of the G-modes of individual index-identified DWNTs composed of two semiconducting SWNTs. We state the main features of the dependence of the G-mode frequencies on the distance between the inner and outer layers: (i) When the interlayer distance is larger than the nominal van der Waals distance (close to 0.34 nm), a downshift of the inner-layer G-modes with respect to the G-modes in the equivalent SWNTs is measured. (ii) The amplitude of the downshift depends on the interlayer distance, or in other words, on the negative pressure felt by the inner layer in DWNT. (iii) No shift is observed for an intertube distance close to 0.34 nm.},\\n\\tnumber = {40},\\n\\turldate = {2023-11-11},\\n\\tjournal = {The Journal of Physical Chemistry C},\\n\\tauthor = {Levshov, D. I. and Michel, T. and Arenal, R. and Tran, H. N. and Than, T. X. and Paillet, M. and Yuzyuk, Yu. I. and Sauvajol, J.-L.},\\n\\tmonth = oct,\\n\\tyear = {2015},\\n\\tnote = {Publisher: American Chemical Society},\\n\\tpages = {23196--23202},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\M5V5TPZR\\\\\\\\Levshov и др. - 2015 - Interlayer Dependence of G-Modes in Semiconducting.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Levshov, D. I.\",\"Michel, T.\",\"Arenal, R.\",\"Tran, H. N.\",\"Than, T. X.\",\"Paillet, M.\",\"Yuzyuk, Y. I.\",\"Sauvajol, J.\"],\"key\":\"levshov_interlayer_2015\",\"id\":\"levshov_interlayer_2015\",\"bibbaseid\":\"levshov-michel-arenal-tran-than-paillet-yuzyuk-sauvajol-interlayerdependenceofgmodesinsemiconductingdoublewalledcarbonnanotubes-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1021/acs.jpcc.5b05888\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"The problem of determining elastic constants of thin ferroelectric films\",\"volume\":\"60\",\"issn\":\"1562-6903\",\"url\":\"https://doi.org/10.1134/S1028335815080108\",\"doi\":\"10.1134/S1028335815080108\",\"abstract\":\"A method of determining the constants of the linear equations of the piezoelectric effect dependent on the external conditions is proposed for thin ferroelectric films on the basis of the Landau potential of the phenomenological theory of phase transitions. By the example of single-crystalline barium—titanate thin films, the behavior of material constants is investigated in dependence on the value of the misfit strain. The investigation of material equations is implemented on the basis of the Landau potential of the eighth degree at room temperature. The substantial difference in the elastic, electric, and piezoelectric properties of a thin film from those of a bulk material is shown; the anomalous behavior of constants on the phase boundaries and the extremal behavior inside the r-phase is revealed.\",\"language\":\"en\",\"number\":\"8\",\"urldate\":\"2023-11-11\",\"journal\":\"Doklady Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kalinchuk\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shakhovoy\"],\"firstnames\":[\"R.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2015\",\"keywords\":\"Barium Titanate, DOKLADY Physic, Elastic Constant, Misfit Strain, Piezoelectric Effect\",\"pages\":\"349–354\",\"bibtex\":\"@article{shirokov_problem_2015,\\n\\ttitle = {The problem of determining elastic constants of thin ferroelectric films},\\n\\tvolume = {60},\\n\\tissn = {1562-6903},\\n\\turl = {https://doi.org/10.1134/S1028335815080108},\\n\\tdoi = {10.1134/S1028335815080108},\\n\\tabstract = {A method of determining the constants of the linear equations of the piezoelectric effect dependent on the external conditions is proposed for thin ferroelectric films on the basis of the Landau potential of the phenomenological theory of phase transitions. By the example of single-crystalline barium—titanate thin films, the behavior of material constants is investigated in dependence on the value of the misfit strain. The investigation of material equations is implemented on the basis of the Landau potential of the eighth degree at room temperature. The substantial difference in the elastic, electric, and piezoelectric properties of a thin film from those of a bulk material is shown; the anomalous behavior of constants on the phase boundaries and the extremal behavior inside the r-phase is revealed.},\\n\\tlanguage = {en},\\n\\tnumber = {8},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Doklady Physics},\\n\\tauthor = {Shirokov, V. B. and Kalinchuk, V. V. and Shakhovoy, R. A. and Yuzyuk, Yu. I.},\\n\\tmonth = aug,\\n\\tyear = {2015},\\n\\tkeywords = {Barium Titanate, DOKLADY Physic, Elastic Constant, Misfit Strain, Piezoelectric Effect},\\n\\tpages = {349--354},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Kalinchuk, V. V.\",\"Shakhovoy, R. A.\",\"Yuzyuk, Y. I.\"],\"key\":\"shirokov_problem_2015\",\"id\":\"shirokov_problem_2015\",\"bibbaseid\":\"shirokov-kalinchuk-shakhovoy-yuzyuk-theproblemofdeterminingelasticconstantsofthinferroelectricfilms-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1028335815080108\"},\"keyword\":[\"Barium Titanate\",\"DOKLADY Physic\",\"Elastic Constant\",\"Misfit Strain\",\"Piezoelectric Effect\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"Terahertz and infrared spectroscopy of bacterial nanofilaments\",\"url\":\"https://ieeexplore.ieee.org/document/7327875\",\"doi\":\"10.1109/IRMMW-THz.2015.7327875\",\"abstract\":\"By means of terahertz and infrared (THz, IR) spectroscopies we have measured the dielectric response of nano-filaments of electrogenic bacteria Shewanella oneidensis MR-1 in a wide frequency and temperature ranges. THz-far-IR spectra are dominated by absorption due to bound water. At helium temperatures and at sub-THz frequencies a boson-peak-like excitation is detected that is typical for disordered materials. The observation is in agreement with the heat capacity measurements.\",\"urldate\":\"2023-11-11\",\"booktitle\":\"2015 40th International Conference on Infrared, Millimeter, and Terahertz waves (IRMMW-THz)\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Motovilov\"],\"firstnames\":[\"Konstantin\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gagkaeva\"],\"firstnames\":[\"Zarina\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kadyrov\"],\"firstnames\":[\"Lenar\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"Elena\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tobokhova\"],\"firstnames\":[\"Aiyyna\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"Victor\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Savinov\"],\"firstnames\":[\"Maxim\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grinenko\"],\"firstnames\":[\"Vadim\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Belyanchikov\"],\"firstnames\":[\"Mikhail\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sidoruk\"],\"firstnames\":[\"Konstantin\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"Martin\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"Boris\",\"P.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2015\",\"note\":\"ISSN: 2162-2035\",\"pages\":\"1–2\",\"bibtex\":\"@inproceedings{motovilov_terahertz_2015,\\n\\ttitle = {Terahertz and infrared spectroscopy of bacterial nanofilaments},\\n\\turl = {https://ieeexplore.ieee.org/document/7327875},\\n\\tdoi = {10.1109/IRMMW-THz.2015.7327875},\\n\\tabstract = {By means of terahertz and infrared (THz, IR) spectroscopies we have measured the dielectric response of nano-filaments of electrogenic bacteria Shewanella oneidensis MR-1 in a wide frequency and temperature ranges. THz-far-IR spectra are dominated by absorption due to bound water. At helium temperatures and at sub-THz frequencies a boson-peak-like excitation is detected that is typical for disordered materials. The observation is in agreement with the heat capacity measurements.},\\n\\turldate = {2023-11-11},\\n\\tbooktitle = {2015 40th {International} {Conference} on {Infrared}, {Millimeter}, and {Terahertz} waves ({IRMMW}-{THz})},\\n\\tauthor = {Motovilov, Konstantin A. and Gagkaeva, Zarina V. and Kadyrov, Lenar S. and Zhukova, Elena S. and Tobokhova, Aiyyna S. and Torgashev, Victor I. and Savinov, Maxim and Grinenko, Vadim and Belyanchikov, Mikhail A. and Sidoruk, Konstantin V. and Dressel, Martin and Gorshunov, Boris P.},\\n\\tmonth = aug,\\n\\tyear = {2015},\\n\\tnote = {ISSN: 2162-2035},\\n\\tpages = {1--2},\\n}\\n\\n\",\"author_short\":[\"Motovilov, K. A.\",\"Gagkaeva, Z. V.\",\"Kadyrov, L. S.\",\"Zhukova, E. S.\",\"Tobokhova, A. S.\",\"Torgashev, V. I.\",\"Savinov, M.\",\"Grinenko, V.\",\"Belyanchikov, M. A.\",\"Sidoruk, K. V.\",\"Dressel, M.\",\"Gorshunov, B. P.\"],\"key\":\"motovilov_terahertz_2015\",\"id\":\"motovilov_terahertz_2015\",\"bibbaseid\":\"motovilov-gagkaeva-kadyrov-zhukova-tobokhova-torgashev-savinov-grinenko-etal-terahertzandinfraredspectroscopyofbacterialnanofilaments-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://ieeexplore.ieee.org/document/7327875\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Effect of ethylene glycol on electrochemical and morphological features of platinum electrodeposits from chloroplatinic acid\",\"volume\":\"45\",\"issn\":\"1572-8838\",\"url\":\"https://doi.org/10.1007/s10800-015-0820-5\",\"doi\":\"10.1007/s10800-015-0820-5\",\"abstract\":\"The aim of this work was to investigate the morphology, average size, and the electrochemical behavior of platinum nanoparticles electrodeposited from water and mixed water–ethylene glycol solutions of the electrolyte of H2PtCl6 and H2SO4 at a rotating disk electrode coated with Vulcan XC-72 carbon powder. Cyclic voltammetry and linear sweep voltammetry were used to determine the electrochemically active surface area (ESA) and oxygen reduction reaction (ORR) activity of the prepared Pt/C materials, respectively. XRD and scanning electron microscopy were used to study the influence of the electrodeposition methods applied on the morphology of platinum particles deposited in water and mixed water–ethylene glycol solutions. The average size of Pt crystallites was in the range of ca. 6–10 nm, and the average size of deposited Pt particles was in the range of ca. 30–150 nm. It was found that the presence of ethylene glycol in the electrolyte solution increased the overpotential of electrodeposition and it also strongly affected the morphology of Pt deposits when constant current electrodeposition was employed. Moreover, it was shown that pulse current electrodeposition is a more effective method compared to constant current electrodeposition method for the preparation of the Pt/Vulcan electrode with high ESA of Pt and enhanced catalytic activity toward ORR. The results obtained concerning the morphology and the spatial distribution of platinum particles electrodeposited on the surface of carbon support at different conditions demonstrate new possibilities to improve synthesis of Pt/C by electrodeposition methods.\",\"language\":\"en\",\"number\":\"6\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Applied Electrochemistry\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Yohannes\"],\"firstnames\":[\"Weldegebriel\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Belenov\"],\"firstnames\":[\"S.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Guterman\"],\"firstnames\":[\"V.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Skibina\"],\"firstnames\":[\"L.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Volotchaev\"],\"firstnames\":[\"V.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lyanguzov\"],\"firstnames\":[\"N.\",\"V.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2015\",\"keywords\":\"Platinum, Electrocatalyst, Galvanostatic electrodeposition, ORR, Vulcan XC-72\",\"pages\":\"623–633\",\"bibtex\":\"@article{yohannes_effect_2015,\\n\\ttitle = {Effect of ethylene glycol on electrochemical and morphological features of platinum electrodeposits from chloroplatinic acid},\\n\\tvolume = {45},\\n\\tissn = {1572-8838},\\n\\turl = {https://doi.org/10.1007/s10800-015-0820-5},\\n\\tdoi = {10.1007/s10800-015-0820-5},\\n\\tabstract = {The aim of this work was to investigate the morphology, average size, and the electrochemical behavior of platinum nanoparticles electrodeposited from water and mixed water–ethylene glycol solutions of the electrolyte of H2PtCl6 and H2SO4 at a rotating disk electrode coated with Vulcan XC-72 carbon powder. Cyclic voltammetry and linear sweep voltammetry were used to determine the electrochemically active surface area (ESA) and oxygen reduction reaction (ORR) activity of the prepared Pt/C materials, respectively. XRD and scanning electron microscopy were used to study the influence of the electrodeposition methods applied on the morphology of platinum particles deposited in water and mixed water–ethylene glycol solutions. The average size of Pt crystallites was in the range of ca. 6–10 nm, and the average size of deposited Pt particles was in the range of ca. 30–150 nm. It was found that the presence of ethylene glycol in the electrolyte solution increased the overpotential of electrodeposition and it also strongly affected the morphology of Pt deposits when constant current electrodeposition was employed. Moreover, it was shown that pulse current electrodeposition is a more effective method compared to constant current electrodeposition method for the preparation of the Pt/Vulcan electrode with high ESA of Pt and enhanced catalytic activity toward ORR. The results obtained concerning the morphology and the spatial distribution of platinum particles electrodeposited on the surface of carbon support at different conditions demonstrate new possibilities to improve synthesis of Pt/C by electrodeposition methods.},\\n\\tlanguage = {en},\\n\\tnumber = {6},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Applied Electrochemistry},\\n\\tauthor = {Yohannes, Weldegebriel and Belenov, S. V. and Guterman, V. E. and Skibina, L. M. and Volotchaev, V. A. and Lyanguzov, N. V.},\\n\\tmonth = jun,\\n\\tyear = {2015},\\n\\tkeywords = {Platinum, Electrocatalyst, Galvanostatic electrodeposition, ORR, Vulcan XC-72},\\n\\tpages = {623--633},\\n}\\n\\n\",\"author_short\":[\"Yohannes, W.\",\"Belenov, S. V.\",\"Guterman, V. E.\",\"Skibina, L. M.\",\"Volotchaev, V. A.\",\"Lyanguzov, N. V.\"],\"key\":\"yohannes_effect_2015\",\"id\":\"yohannes_effect_2015\",\"bibbaseid\":\"yohannes-belenov-guterman-skibina-volotchaev-lyanguzov-effectofethyleneglycolonelectrochemicalandmorphologicalfeaturesofplatinumelectrodepositsfromchloroplatinicacid-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1007/s10800-015-0820-5\"},\"keyword\":[\"Platinum\",\"Electrocatalyst\",\"Galvanostatic electrodeposition\",\"ORR\",\"Vulcan XC-72\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Vibrational heat capacity of carbon nanotubes at low and ultra-low temperatures\",\"volume\":\"68\",\"issn\":\"1386-9477\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S138694771400472X\",\"doi\":\"10.1016/j.physe.2014.12.033\",\"abstract\":\"To measure a heat capacity of a single carbon nanotube is impossible nowadays and experiments are performed with the nanotubes bundles. However, the existing theories of carbon nanotubes heat capacity do not take into account an interaction between an individual nanotube and its environment. Here we show that due to this fact the known theories overestimate the heat capacity in the ultra-low temperature limit. In this region the main contribution to heat capacity of a single free nanotube is caused by the bending phonon mode with a quadratic dispersion. At T=1K different known models of the phonon dynamics lead to the theoretical specific heat which is at least 10 times greater than the experimentally measured value. To overcome this contradiction we take into account the interaction between an individual nanotube and its environment. As a result, the nanotube loses its Goldstone degrees of freedom and essential reconstruction of the lowest-energy part of its phonon spectrum occurs. The theory proposed explains experimental data on thermal capacity in the ultra-low temperature range and simultaneously demonstrates better agreement with experiments in the region 2.5K\\\\textlessT\\\\textless40K than the preceding models.\",\"urldate\":\"2023-11-11\",\"journal\":\"Physica E: Low-dimensional Systems and Nanostructures\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Avramenko\"],\"firstnames\":[\"M.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golushko\"],\"firstnames\":[\"I.\",\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Myasnikova\"],\"firstnames\":[\"A.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2015\",\"keywords\":\"2D membranes, Carbon nanotubes, Heat capacity, Low temperatures, Phonon spectrum, Pinning\",\"pages\":\"133–139\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\QUQ3BBJ9\\\\\\\\Avramenko и др. - 2015 - Vibrational heat capacity of carbon nanotubes at l.pdf:application/pdf\",\"bibtex\":\"@article{avramenko_vibrational_2015,\\n\\ttitle = {Vibrational heat capacity of carbon nanotubes at low and ultra-low temperatures},\\n\\tvolume = {68},\\n\\tissn = {1386-9477},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S138694771400472X},\\n\\tdoi = {10.1016/j.physe.2014.12.033},\\n\\tabstract = {To measure a heat capacity of a single carbon nanotube is impossible nowadays and experiments are performed with the nanotubes bundles. However, the existing theories of carbon nanotubes heat capacity do not take into account an interaction between an individual nanotube and its environment. Here we show that due to this fact the known theories overestimate the heat capacity in the ultra-low temperature limit. In this region the main contribution to heat capacity of a single free nanotube is caused by the bending phonon mode with a quadratic dispersion. At T=1K different known models of the phonon dynamics lead to the theoretical specific heat which is at least 10 times greater than the experimentally measured value. To overcome this contradiction we take into account the interaction between an individual nanotube and its environment. As a result, the nanotube loses its Goldstone degrees of freedom and essential reconstruction of the lowest-energy part of its phonon spectrum occurs. The theory proposed explains experimental data on thermal capacity in the ultra-low temperature range and simultaneously demonstrates better agreement with experiments in the region 2.5K{\\\\textless}T{\\\\textless}40K than the preceding models.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physica E: Low-dimensional Systems and Nanostructures},\\n\\tauthor = {Avramenko, M. V. and Golushko, I. Yu. and Myasnikova, A. E. and Rochal, S. B.},\\n\\tmonth = apr,\\n\\tyear = {2015},\\n\\tkeywords = {2D membranes, Carbon nanotubes, Heat capacity, Low temperatures, Phonon spectrum, Pinning},\\n\\tpages = {133--139},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\QUQ3BBJ9\\\\\\\\Avramenko и др. - 2015 - Vibrational heat capacity of carbon nanotubes at l.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Avramenko, M. V.\",\"Golushko, I. Y.\",\"Myasnikova, A. E.\",\"Rochal, S. B.\"],\"key\":\"avramenko_vibrational_2015\",\"id\":\"avramenko_vibrational_2015\",\"bibbaseid\":\"avramenko-golushko-myasnikova-rochal-vibrationalheatcapacityofcarbonnanotubesatlowandultralowtemperatures-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S138694771400472X\"},\"keyword\":[\"2D membranes\",\"Carbon nanotubes\",\"Heat capacity\",\"Low temperatures\",\"Phonon spectrum\",\"Pinning\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Synthesis and structure of interaction products of quinoline-2(1H)-thione with molecular iodine\",\"volume\":\"139\",\"issn\":\"1386-1425\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S1386142514018551\",\"doi\":\"10.1016/j.saa.2014.12.075\",\"abstract\":\"The behavior of quinoline-2(1H)-thione, which is a potential antithyroid drug toward molecular iodine, was investigated. The ability of quinoline-2(1H)-thione to form the outer-sphere charge-transfer complex C9H7NS·I2 with iodine molecular in dilute chloroform solution has been studied by UV–vis spectroscopy (lgβ=3.85). The crystal structure of the new salt 2-(quinoline-2-yldisulfanyl)quinolinium triiodide – product of irreversible oxidation of quinoline-2(1H)-thione was determined by X-ray diffraction. The 2-(quinoline-2-yldisulfanyl)quinolinium cations form dimers through π–π–stacking interaction between quinoline rings. Strong intramolecular interactions are observed between iodine – sulfur atoms and iodine – hydrogen atoms with shortened contacts (less of sum of van der Waals contacts). It is noteworthy that two perfectly centrosymmetrical anions I3− form a very short contact I(3)⋯I(3′) 3.7550(5) so we can state the formation of the dianion I62−. Therefore the formation and topology of polyiodide species depend on the characteristics, such as shape, size and charge, etc., of the counter cation, 2-(quinoline-2-yldisulfanyl)quinolinium, which is considered as templating agent.\",\"urldate\":\"2023-11-11\",\"journal\":\"Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Chernov’yants\"],\"firstnames\":[\"Margarita\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Starikova\"],\"firstnames\":[\"Zoya\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kolesnikova\"],\"firstnames\":[\"Tatiana\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Karginova\"],\"firstnames\":[\"Anastasia\",\"O.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lyanguzov\"],\"firstnames\":[\"Nikolay\",\"V.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2015\",\"keywords\":\"X-ray diffraction, Raman spectroscopy, 2-(quinoline-2-yldisulfanyl)quinolinium triiodide, Charge-transfer complex, IR, Quinoline-2(1)-thione\",\"pages\":\"533–538\",\"bibtex\":\"@article{chernovyants_synthesis_2015,\\n\\ttitle = {Synthesis and structure of interaction products of quinoline-2({1H})-thione with molecular iodine},\\n\\tvolume = {139},\\n\\tissn = {1386-1425},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S1386142514018551},\\n\\tdoi = {10.1016/j.saa.2014.12.075},\\n\\tabstract = {The behavior of quinoline-2(1H)-thione, which is a potential antithyroid drug toward molecular iodine, was investigated. The ability of quinoline-2(1H)-thione to form the outer-sphere charge-transfer complex C9H7NS·I2 with iodine molecular in dilute chloroform solution has been studied by UV–vis spectroscopy (lgβ=3.85). The crystal structure of the new salt 2-(quinoline-2-yldisulfanyl)quinolinium triiodide – product of irreversible oxidation of quinoline-2(1H)-thione was determined by X-ray diffraction. The 2-(quinoline-2-yldisulfanyl)quinolinium cations form dimers through π–π–stacking interaction between quinoline rings. Strong intramolecular interactions are observed between iodine – sulfur atoms and iodine – hydrogen atoms with shortened contacts (less of sum of van der Waals contacts). It is noteworthy that two perfectly centrosymmetrical anions I3− form a very short contact I(3)⋯I(3′) 3.7550(5) so we can state the formation of the dianion I62−. Therefore the formation and topology of polyiodide species depend on the characteristics, such as shape, size and charge, etc., of the counter cation, 2-(quinoline-2-yldisulfanyl)quinolinium, which is considered as templating agent.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy},\\n\\tauthor = {Chernov’yants, Margarita S. and Starikova, Zoya A. and Kolesnikova, Tatiana S. and Karginova, Anastasia O. and Lyanguzov, Nikolay V.},\\n\\tmonth = mar,\\n\\tyear = {2015},\\n\\tkeywords = {X-ray diffraction, Raman spectroscopy, 2-(quinoline-2-yldisulfanyl)quinolinium triiodide, Charge-transfer complex, IR, Quinoline-2(1)-thione},\\n\\tpages = {533--538},\\n}\\n\\n\",\"author_short\":[\"Chernov’yants, M. S.\",\"Starikova, Z. A.\",\"Kolesnikova, T. S.\",\"Karginova, A. O.\",\"Lyanguzov, N. V.\"],\"key\":\"chernovyants_synthesis_2015\",\"id\":\"chernovyants_synthesis_2015\",\"bibbaseid\":\"chernovyants-starikova-kolesnikova-karginova-lyanguzov-synthesisandstructureofinteractionproductsofquinoline21hthionewithmoleculariodine-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S1386142514018551\"},\"keyword\":[\"X-ray diffraction\",\"Raman spectroscopy\",\"2-(quinoline-2-yldisulfanyl)quinolinium triiodide\",\"Charge-transfer complex\",\"IR\",\"Quinoline-2(1)-thione\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Slightly broken icosahedral symmetry advances Thomson problem\",\"volume\":\"379\",\"issn\":\"0375-9601\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0375960114011682\",\"doi\":\"10.1016/j.physleta.2014.11.039\",\"abstract\":\"To advance Thomson problem we generalize physical principles suggested by Caspar and Klug (CK) to model icosahedral capsids. Proposed simplest distortions of the CK spherical arrangements yield new-type trial structures very close to the lowest energy ones. In the region 600≤N≤1000, where N is the number of particles in the structure, we found 40 new spherical crystals with the lowest ever seen energies and curvature-induced topological defects being not the well-known elongated scars but flatten pentagons. These crystals have N values prohibited in the CK model and demonstrate a new way to combine the local hexagonal order and spherical geometry.\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Physics Letters A\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Roshal\"],\"firstnames\":[\"D.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Myasnikova\"],\"firstnames\":[\"A.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2015\",\"keywords\":\"Topological defects, Caspar and Klug theory, Self-assembly, Spherical crystals, Thomson problem, Viral capsids\",\"pages\":\"372–376\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\I3PW53KV\\\\\\\\Roshal и др. - 2015 - Slightly broken icosahedral symmetry advances Thom.pdf:application/pdf\",\"bibtex\":\"@article{roshal_slightly_2015,\\n\\ttitle = {Slightly broken icosahedral symmetry advances {Thomson} problem},\\n\\tvolume = {379},\\n\\tissn = {0375-9601},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0375960114011682},\\n\\tdoi = {10.1016/j.physleta.2014.11.039},\\n\\tabstract = {To advance Thomson problem we generalize physical principles suggested by Caspar and Klug (CK) to model icosahedral capsids. Proposed simplest distortions of the CK spherical arrangements yield new-type trial structures very close to the lowest energy ones. In the region 600≤N≤1000, where N is the number of particles in the structure, we found 40 new spherical crystals with the lowest ever seen energies and curvature-induced topological defects being not the well-known elongated scars but flatten pentagons. These crystals have N values prohibited in the CK model and demonstrate a new way to combine the local hexagonal order and spherical geometry.},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physics Letters A},\\n\\tauthor = {Roshal, D. S. and Myasnikova, A. E. and Rochal, S. B.},\\n\\tmonth = feb,\\n\\tyear = {2015},\\n\\tkeywords = {Topological defects, Caspar and Klug theory, Self-assembly, Spherical crystals, Thomson problem, Viral capsids},\\n\\tpages = {372--376},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\I3PW53KV\\\\\\\\Roshal и др. - 2015 - Slightly broken icosahedral symmetry advances Thom.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Roshal, D. S.\",\"Myasnikova, A. E.\",\"Rochal, S. B.\"],\"key\":\"roshal_slightly_2015\",\"id\":\"roshal_slightly_2015\",\"bibbaseid\":\"roshal-myasnikova-rochal-slightlybrokenicosahedralsymmetryadvancesthomsonproblem-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0375960114011682\"},\"keyword\":[\"Topological defects\",\"Caspar and Klug theory\",\"Self-assembly\",\"Spherical crystals\",\"Thomson problem\",\"Viral capsids\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Difference Raman spectroscopy of DNA molecules\",\"volume\":\"584\",\"issn\":\"1742-6596\",\"url\":\"https://dx.doi.org/10.1088/1742-6596/584/1/012022\",\"doi\":\"10.1088/1742-6596/584/1/012022\",\"abstract\":\"In this paper the micro-Raman spectra of calf DNA for different points of DNA sample have been recorded. The Raman spectra were made with help of difference Raman spectroscopy technique. Raman spectra were recorded with high spatial resolution from different points of the wet and dry samples in different spectral range (100÷4000cm−1) using two lasers: argon (514.5 nm) and helium -neon (632.8 nm). The significant differences in the Raman spectra for dry and wet DNA and for different points of DNA molecules were observed. The obtained data on difference Raman scattering spectra of DNA molecules may be used for identification of DNA types and for analysis of genetic information associated with the molecular structure of this molecule.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics: Conference Series\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Anokhin\"],\"firstnames\":[\"Andrey\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorelik\"],\"firstnames\":[\"Vladimir\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dovbeshko\"],\"firstnames\":[\"Galina\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pyatyshev\"],\"firstnames\":[\"Alexander\",\"Yu\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yury\",\"I.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2015\",\"pages\":\"012022\",\"file\":\"IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\B6MCEJV5\\\\\\\\Anokhin и др. - 2015 - Difference Raman spectroscopy of DNA molecules.pdf:application/pdf\",\"bibtex\":\"@article{anokhin_difference_2015,\\n\\ttitle = {Difference {Raman} spectroscopy of {DNA} molecules},\\n\\tvolume = {584},\\n\\tissn = {1742-6596},\\n\\turl = {https://dx.doi.org/10.1088/1742-6596/584/1/012022},\\n\\tdoi = {10.1088/1742-6596/584/1/012022},\\n\\tabstract = {In this paper the micro-Raman spectra of calf DNA for different points of DNA sample have been recorded. The Raman spectra were made with help of difference Raman spectroscopy technique. Raman spectra were recorded with high spatial resolution from different points of the wet and dry samples in different spectral range (100÷4000cm−1) using two lasers: argon (514.5 nm) and helium -neon (632.8 nm). The significant differences in the Raman spectra for dry and wet DNA and for different points of DNA molecules were observed. The obtained data on difference Raman scattering spectra of DNA molecules may be used for identification of DNA types and for analysis of genetic information associated with the molecular structure of this molecule.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics: Conference Series},\\n\\tauthor = {Anokhin, Andrey S. and Gorelik, Vladimir S. and Dovbeshko, Galina I. and Pyatyshev, Alexander Yu and Yuzyuk, Yury I.},\\n\\tmonth = jan,\\n\\tyear = {2015},\\n\\tpages = {012022},\\n\\tfile = {IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\B6MCEJV5\\\\\\\\Anokhin и др. - 2015 - Difference Raman spectroscopy of DNA molecules.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Anokhin, A. S.\",\"Gorelik, V. S.\",\"Dovbeshko, G. I.\",\"Pyatyshev, A. Y.\",\"Yuzyuk, Y. I.\"],\"key\":\"anokhin_difference_2015\",\"id\":\"anokhin_difference_2015\",\"bibbaseid\":\"anokhin-gorelik-dovbeshko-pyatyshev-yuzyuk-differenceramanspectroscopyofdnamolecules-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/1742-6596/584/1/012022\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Anomalies of piezoelectric coefficients in barium titanate thin films\",\"volume\":\"108\",\"issn\":\"0295-5075\",\"url\":\"https://dx.doi.org/10.1209/0295-5075/108/47008\",\"doi\":\"10.1209/0295-5075/108/47008\",\"abstract\":\"Modeling of electromechanical devices involves the use of different material coefficients, whose measurement is a difficult task, especially when the problem concerns thin films. Required coefficients of thin films could be found theoretically, using known values of the bulk constants. Electromechanical coefficients of barium titanate thin films are still unknown; therefore, it is expedient to carry out their calculations. We give here the full set of electromechanical coefficients of barium titanate thin films for the whole range of technologically available misfit strains. In the present paper, piezoelectric coefficients as functions of a misfit strain were calculated. It was revealed that piezoelectric coefficients exhibit anomalies at phase boundaries and inside the monoclinic r-phase as well. The obtained results allow finding the required values of the thin-film parameters, varying the misfit strain.\",\"language\":\"en\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Europhysics Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"Vladimir\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kalinchuk\"],\"firstnames\":[\"Valery\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shakhovoy\"],\"firstnames\":[\"Roman\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yury\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2014\",\"note\":\"Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica\",\"pages\":\"47008\",\"bibtex\":\"@article{shirokov_anomalies_2014,\\n\\ttitle = {Anomalies of piezoelectric coefficients in barium titanate thin films},\\n\\tvolume = {108},\\n\\tissn = {0295-5075},\\n\\turl = {https://dx.doi.org/10.1209/0295-5075/108/47008},\\n\\tdoi = {10.1209/0295-5075/108/47008},\\n\\tabstract = {Modeling of electromechanical devices involves the use of different material coefficients, whose measurement is a difficult task, especially when the problem concerns thin films. Required coefficients of thin films could be found theoretically, using known values of the bulk constants. Electromechanical coefficients of barium titanate thin films are still unknown; therefore, it is expedient to carry out their calculations. We give here the full set of electromechanical coefficients of barium titanate thin films for the whole range of technologically available misfit strains. In the present paper, piezoelectric coefficients as functions of a misfit strain were calculated. It was revealed that piezoelectric coefficients exhibit anomalies at phase boundaries and inside the monoclinic r-phase as well. The obtained results allow finding the required values of the thin-film parameters, varying the misfit strain.},\\n\\tlanguage = {en},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Europhysics Letters},\\n\\tauthor = {Shirokov, Vladimir and Kalinchuk, Valery and Shakhovoy, Roman and Yuzyuk, Yury},\\n\\tmonth = nov,\\n\\tyear = {2014},\\n\\tnote = {Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica},\\n\\tpages = {47008},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V.\",\"Kalinchuk, V.\",\"Shakhovoy, R.\",\"Yuzyuk, Y.\"],\"key\":\"shirokov_anomalies_2014\",\"id\":\"shirokov_anomalies_2014\",\"bibbaseid\":\"shirokov-kalinchuk-shakhovoy-yuzyuk-anomaliesofpiezoelectriccoefficientsinbariumtitanatethinfilms-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1209/0295-5075/108/47008\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":1,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"THz–IR spectroscopy of single H2O molecules confined in nanocage of beryl crystal lattice\",\"volume\":\"87\",\"issn\":\"0141-1594\",\"url\":\"https://doi.org/10.1080/01411594.2014.954247\",\"doi\":\"10.1080/01411594.2014.954247\",\"abstract\":\"We have measured the terahertz–infrared (3–7000 cm−1) spectra of the optical conductivity of iron-doped single crystals of beryl, (Mn,Fe):Be3Al2Si6O18, that contain lone water molecules isolated within nanometer-sized cages formed by the ions of beryl crystal lattice. By comparing the spectra with those of dehydrated crystals, we exclude phonon resonances and reconstruct the spectra determined exclusively by vibrations of the water molecules. At liquid-helium temperatures, well-known intramolecular H2O modes are observed above 1000 cm−1 and accompanied with satellite resonances that are combinations of intramolecular and external vibrations of H2O molecules. At terahertz frequencies, a broad bump centred around 20 cm−1 (at 5 K) is observed with three rather narrow resonances at its high-frequency shoulder (38, 42 and 46 cm−1). The origin of these low-energy excitations is discussed.\",\"number\":\"10-11\",\"urldate\":\"2023-11-11\",\"journal\":\"Phase Transitions\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"Boris\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"Elena\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"Victor\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Motovilova\"],\"firstnames\":[\"Elizaveta\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lebedev\"],\"firstnames\":[\"Vladimir\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"Anatoly\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shakurov\"],\"firstnames\":[\"Gil’man\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kremer\"],\"firstnames\":[\"Reinhard\",\"K.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Uskov\"],\"firstnames\":[\"Vladimir\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pestrjakov\"],\"firstnames\":[\"Efim\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Thomas\"],\"firstnames\":[\"Victor\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fursenko\"],\"firstnames\":[\"Dimitri\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kadlec\"],\"firstnames\":[\"Christelle\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kadlec\"],\"firstnames\":[\"Filip\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"Martin\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2014\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/01411594.2014.954247\",\"keywords\":\"nano-confined water molecule, terahertz spectroscopy\",\"pages\":\"966–972\",\"bibtex\":\"@article{gorshunov_thzir_2014,\\n\\ttitle = {{THz}–{IR} spectroscopy of single {H2O} molecules confined in nanocage of beryl crystal lattice},\\n\\tvolume = {87},\\n\\tissn = {0141-1594},\\n\\turl = {https://doi.org/10.1080/01411594.2014.954247},\\n\\tdoi = {10.1080/01411594.2014.954247},\\n\\tabstract = {We have measured the terahertz–infrared (3–7000 cm−1) spectra of the optical conductivity of iron-doped single crystals of beryl, (Mn,Fe):Be3Al2Si6O18, that contain lone water molecules isolated within nanometer-sized cages formed by the ions of beryl crystal lattice. By comparing the spectra with those of dehydrated crystals, we exclude phonon resonances and reconstruct the spectra determined exclusively by vibrations of the water molecules. At liquid-helium temperatures, well-known intramolecular H2O modes are observed above 1000 cm−1 and accompanied with satellite resonances that are combinations of intramolecular and external vibrations of H2O molecules. At terahertz frequencies, a broad bump centred around 20 cm−1 (at 5 K) is observed with three rather narrow resonances at its high-frequency shoulder (38, 42 and 46 cm−1). The origin of these low-energy excitations is discussed.},\\n\\tnumber = {10-11},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Phase Transitions},\\n\\tauthor = {Gorshunov, Boris P. and Zhukova, Elena S. and Torgashev, Victor I. and Motovilova, Elizaveta A. and Lebedev, Vladimir V. and Prokhorov, Anatoly S. and Shakurov, Gil’man S. and Kremer, Reinhard K. and Uskov, Vladimir V. and Pestrjakov, Efim V. and Thomas, Victor G. and Fursenko, Dimitri A. and Kadlec, Christelle and Kadlec, Filip and Dressel, Martin},\\n\\tmonth = nov,\\n\\tyear = {2014},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/01411594.2014.954247},\\n\\tkeywords = {nano-confined water molecule, terahertz spectroscopy},\\n\\tpages = {966--972},\\n}\\n\\n\",\"author_short\":[\"Gorshunov, B. P.\",\"Zhukova, E. S.\",\"Torgashev, V. I.\",\"Motovilova, E. A.\",\"Lebedev, V. V.\",\"Prokhorov, A. S.\",\"Shakurov, G. S.\",\"Kremer, R. K.\",\"Uskov, V. V.\",\"Pestrjakov, E. V.\",\"Thomas, V. G.\",\"Fursenko, D. A.\",\"Kadlec, C.\",\"Kadlec, F.\",\"Dressel, M.\"],\"key\":\"gorshunov_thzir_2014\",\"id\":\"gorshunov_thzir_2014\",\"bibbaseid\":\"gorshunov-zhukova-torgashev-motovilova-lebedev-prokhorov-shakurov-kremer-etal-thzirspectroscopyofsingleh2omoleculesconfinedinnanocageofberylcrystallattice-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/01411594.2014.954247\"},\"keyword\":[\"nano-confined water molecule\",\"terahertz spectroscopy\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"High pressure x-ray diffraction study of nickel–copper chromites solid solutions\",\"volume\":\"26\",\"issn\":\"0953-8984\",\"url\":\"https://dx.doi.org/10.1088/0953-8984/26/50/505401\",\"doi\":\"10.1088/0953-8984/26/50/505401\",\"abstract\":\"A high-pressure synchrotron radiation diffraction study has been carried out on Ni1−xCuxCr2O4 solid solutions. Observed pressure-controlled phase transitions, along with data previously collected for temperature-induced phase transitions, are analyzed in the framework of the unified phenomenological model that results in mapping of the generic phase diagram for the whole family of Ni1−xCuxCr2O4 solid solutions.\",\"language\":\"en\",\"number\":\"50\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics: Condensed Matter\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bush\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chernyshov\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"I.\",\"Yu\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dmitriev\"],\"firstnames\":[\"V.\",\"P.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2014\",\"note\":\"Publisher: IOP Publishing\",\"pages\":\"505401\",\"bibtex\":\"@article{mikheykin_high_2014,\\n\\ttitle = {High pressure x-ray diffraction study of nickel–copper chromites solid solutions},\\n\\tvolume = {26},\\n\\tissn = {0953-8984},\\n\\turl = {https://dx.doi.org/10.1088/0953-8984/26/50/505401},\\n\\tdoi = {10.1088/0953-8984/26/50/505401},\\n\\tabstract = {A high-pressure synchrotron radiation diffraction study has been carried out on Ni1−xCuxCr2O4 solid solutions. Observed pressure-controlled phase transitions, along with data previously collected for temperature-induced phase transitions, are analyzed in the framework of the unified phenomenological model that results in mapping of the generic phase diagram for the whole family of Ni1−xCuxCr2O4 solid solutions.},\\n\\tlanguage = {en},\\n\\tnumber = {50},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics: Condensed Matter},\\n\\tauthor = {Mikheykin, A. S. and Torgashev, V. I. and Talanov, V. M. and Bush, A. A. and Chernyshov, D. and Yuzyuk, I. Yu and Dmitriev, V. P.},\\n\\tmonth = nov,\\n\\tyear = {2014},\\n\\tnote = {Publisher: IOP Publishing},\\n\\tpages = {505401},\\n}\\n\\n\",\"author_short\":[\"Mikheykin, A. S.\",\"Torgashev, V. I.\",\"Talanov, V. M.\",\"Bush, A. A.\",\"Chernyshov, D.\",\"Yuzyuk, I. Y.\",\"Dmitriev, V. P.\"],\"key\":\"mikheykin_high_2014\",\"id\":\"mikheykin_high_2014\",\"bibbaseid\":\"mikheykin-torgashev-talanov-bush-chernyshov-yuzyuk-dmitriev-highpressurexraydiffractionstudyofnickelcopperchromitessolidsolutions-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/0953-8984/26/50/505401\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Photoelectric properties of MSM structure based on ZnO nanorods, received by thermal evaporation and carbothermal syntesis\",\"volume\":\"541\",\"issn\":\"1742-6596\",\"url\":\"https://dx.doi.org/10.1088/1742-6596/541/1/012038\",\"doi\":\"10.1088/1742-6596/541/1/012038\",\"abstract\":\"Photoelectric characteristics of metal-semiconductor-metal (MSM) structures: Au/ZnO(nanorods)/ZnO(film)/ZnO(nanorods)/Au were investigated. Synthesis of ZnO nanorods (NR's) was carried out by two different methods, such as catalyst-free carbothermal synthesis (t = 950°C, precursor – ZnO:C) and catalyst-free thermal evaporation of metallic Zn (t = 600°C, precursor Zn). Photoluminescence spectra have shown that the ZnO NR's obtained by means of thermal evaporation technique have a lower concentration of point defects related with oxygen vacancies, than ZnO NR's prepared by carbothermal synthesis. MSM structure with ZnO NR's obtained by thermal evaporation technique have photosensitivity 97 mA/W at 325 nm illumination and 44 mA/W at 518 nm illumination at a bias 5V. For MSM structure with ZnO NR's obtained by method of carbothermal synthesis, the photosensitivity values were 22 mA/W, and 103 mA/W, respectively.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics: Conference Series\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Zhilin\"],\"firstnames\":[\"D.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lyanguzov\"],\"firstnames\":[\"N.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nikolaev\"],\"firstnames\":[\"L.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pushkariov\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2014\",\"pages\":\"012038\",\"file\":\"IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\49KV5PK9\\\\\\\\Zhilin и др. - 2014 - Photoelectric properties of MSM structure based on.pdf:application/pdf\",\"bibtex\":\"@article{zhilin_photoelectric_2014,\\n\\ttitle = {Photoelectric properties of {MSM} structure based on {ZnO} nanorods, received by thermal evaporation and carbothermal syntesis},\\n\\tvolume = {541},\\n\\tissn = {1742-6596},\\n\\turl = {https://dx.doi.org/10.1088/1742-6596/541/1/012038},\\n\\tdoi = {10.1088/1742-6596/541/1/012038},\\n\\tabstract = {Photoelectric characteristics of metal-semiconductor-metal (MSM) structures: Au/ZnO(nanorods)/ZnO(film)/ZnO(nanorods)/Au were investigated. Synthesis of ZnO nanorods (NR's) was carried out by two different methods, such as catalyst-free carbothermal synthesis (t = 950°C, precursor – ZnO:C) and catalyst-free thermal evaporation of metallic Zn (t = 600°C, precursor Zn). Photoluminescence spectra have shown that the ZnO NR's obtained by means of thermal evaporation technique have a lower concentration of point defects related with oxygen vacancies, than ZnO NR's prepared by carbothermal synthesis. MSM structure with ZnO NR's obtained by thermal evaporation technique have photosensitivity 97 mA/W at 325 nm illumination and 44 mA/W at 518 nm illumination at a bias 5V. For MSM structure with ZnO NR's obtained by method of carbothermal synthesis, the photosensitivity values were 22 mA/W, and 103 mA/W, respectively.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics: Conference Series},\\n\\tauthor = {Zhilin, D. A. and Lyanguzov, N. V. and Nikolaev, L. A. and Pushkariov, V. I. and Kaidashev, E. M.},\\n\\tmonth = oct,\\n\\tyear = {2014},\\n\\tpages = {012038},\\n\\tfile = {IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\49KV5PK9\\\\\\\\Zhilin и др. - 2014 - Photoelectric properties of MSM structure based on.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Zhilin, D. A.\",\"Lyanguzov, N. V.\",\"Nikolaev, L. A.\",\"Pushkariov, V. I.\",\"Kaidashev, E. M.\"],\"key\":\"zhilin_photoelectric_2014\",\"id\":\"zhilin_photoelectric_2014\",\"bibbaseid\":\"zhilin-lyanguzov-nikolaev-pushkariov-kaidashev-photoelectricpropertiesofmsmstructurebasedonznonanorodsreceivedbythermalevaporationandcarbothermalsyntesis-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/1742-6596/541/1/012038\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Combined atomic ordering in the A and B sublattices of perovskite structure\",\"volume\":\"59\",\"issn\":\"1562-689X\",\"url\":\"https://doi.org/10.1134/S1063774514050198\",\"doi\":\"10.1134/S1063774514050198\",\"abstract\":\"The simultaneous ordering of cations in the A and B sublattices of cubic perovskite structure has been investigated by the group-theoretical method. It is found that 147 ordered phases may exist. Among them, there may be 121 phases with simultaneous cation ordering in the 1(a)- and 1(c) positions of perovskite structure. It is shown that 53 phases are described by improper order parameters related to cation ordering, the formation of 56 phases is related to improper rotations of octahedra, and 15 phases are improper ferroelectrics. Calculated structures of some types of ordered low-symmetry perovskite modifications are presented.\",\"language\":\"en\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Crystallography Reports\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"M.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2014\",\"keywords\":\"Crystallography Report, Group Theoretical Method, Permutation Representation, Perovskite, Perovskite Structure\",\"pages\":\"662–678\",\"bibtex\":\"@article{talanov_combined_2014,\\n\\ttitle = {Combined atomic ordering in the {A} and {B} sublattices of perovskite structure},\\n\\tvolume = {59},\\n\\tissn = {1562-689X},\\n\\turl = {https://doi.org/10.1134/S1063774514050198},\\n\\tdoi = {10.1134/S1063774514050198},\\n\\tabstract = {The simultaneous ordering of cations in the A and B sublattices of cubic perovskite structure has been investigated by the group-theoretical method. It is found that 147 ordered phases may exist. Among them, there may be 121 phases with simultaneous cation ordering in the 1(a)- and 1(c) positions of perovskite structure. It is shown that 53 phases are described by improper order parameters related to cation ordering, the formation of 56 phases is related to improper rotations of octahedra, and 15 phases are improper ferroelectrics. Calculated structures of some types of ordered low-symmetry perovskite modifications are presented.},\\n\\tlanguage = {en},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Crystallography Reports},\\n\\tauthor = {Talanov, M. V. and Shirokov, V. B. and Talanov, V. M.},\\n\\tmonth = sep,\\n\\tyear = {2014},\\n\\tkeywords = {Crystallography Report, Group Theoretical Method, Permutation Representation, Perovskite, Perovskite Structure},\\n\\tpages = {662--678},\\n}\\n\\n\",\"author_short\":[\"Talanov, M. V.\",\"Shirokov, V. B.\",\"Talanov, V. M.\"],\"key\":\"talanov_combined_2014\",\"id\":\"talanov_combined_2014\",\"bibbaseid\":\"talanov-shirokov-talanov-combinedatomicorderingintheaandbsublatticesofperovskitestructure-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1063774514050198\"},\"keyword\":[\"Crystallography Report\",\"Group Theoretical Method\",\"Permutation Representation\",\"Perovskite\",\"Perovskite Structure\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Group-theoretical study of cationic ordering in perovskite structure\",\"volume\":\"59\",\"issn\":\"1562-689X\",\"url\":\"https://doi.org/10.1134/S1063774514050186\",\"doi\":\"10.1134/S1063774514050186\",\"abstract\":\"Atomic ordering in the structure of cubic perovskite has been investigated by the group-theoretical method. The possibility of existence of 13 ordered phases in the 1(a) position (including four binary, two ternary, and five quaternary cationic superstructures) and 13 phases with different types of ordering in the 1(b) position (including four binary, two ternary, and five quaternary cationic superstructures) is established. Calculated structures of some types of ordered low-symmetry perovskite modifications are reported.\",\"language\":\"en\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Crystallography Reports\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"M.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2014\",\"keywords\":\"Crystallography Report, Perovskite, Perovskite Structure, CaCu, Central Atom\",\"pages\":\"650–661\",\"bibtex\":\"@article{talanov_group-theoretical_2014,\\n\\ttitle = {Group-theoretical study of cationic ordering in perovskite structure},\\n\\tvolume = {59},\\n\\tissn = {1562-689X},\\n\\turl = {https://doi.org/10.1134/S1063774514050186},\\n\\tdoi = {10.1134/S1063774514050186},\\n\\tabstract = {Atomic ordering in the structure of cubic perovskite has been investigated by the group-theoretical method. The possibility of existence of 13 ordered phases in the 1(a) position (including four binary, two ternary, and five quaternary cationic superstructures) and 13 phases with different types of ordering in the 1(b) position (including four binary, two ternary, and five quaternary cationic superstructures) is established. Calculated structures of some types of ordered low-symmetry perovskite modifications are reported.},\\n\\tlanguage = {en},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Crystallography Reports},\\n\\tauthor = {Talanov, V. M. and Talanov, M. V. and Shirokov, V. B.},\\n\\tmonth = sep,\\n\\tyear = {2014},\\n\\tkeywords = {Crystallography Report, Perovskite, Perovskite Structure, CaCu, Central Atom},\\n\\tpages = {650--661},\\n}\\n\\n\",\"author_short\":[\"Talanov, V. M.\",\"Talanov, M. V.\",\"Shirokov, V. B.\"],\"key\":\"talanov_group-theoretical_2014\",\"id\":\"talanov_group-theoretical_2014\",\"bibbaseid\":\"talanov-talanov-shirokov-grouptheoreticalstudyofcationicorderinginperovskitestructure-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1063774514050186\"},\"keyword\":[\"Crystallography Report\",\"Perovskite\",\"Perovskite Structure\",\"CaCu\",\"Central Atom\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"Scattering of magnetostatic waves by defects of the surface of a ferromagnetic film\",\"volume\":\"1\",\"url\":\"https://ieeexplore.ieee.org/document/6958761\",\"doi\":\"10.1109/APEDE.2014.6958761\",\"abstract\":\"The solution for the diffraction problem of scattering of magnetostatic waves by an arbitrary shallow defect situated under the surface of a ferromagnetic film magnetized at an arbitrary angle is obtained in the quasi-static approximation. Expressions for the energy flux density of scattered magnetostatic waves in the far-field zone are found.\",\"urldate\":\"2023-11-11\",\"booktitle\":\"2014 International Conference on Actual Problems of Electron Devices Engineering (APEDE)\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Babichev\"],\"firstnames\":[\"R.\",\"K.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vyatkina\"],\"firstnames\":[\"S.\",\"A.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2014\",\"pages\":\"279–283\",\"bibtex\":\"@inproceedings{timoshenko_scattering_2014,\\n\\ttitle = {Scattering of magnetostatic waves by defects of the surface of a ferromagnetic film},\\n\\tvolume = {1},\\n\\turl = {https://ieeexplore.ieee.org/document/6958761},\\n\\tdoi = {10.1109/APEDE.2014.6958761},\\n\\tabstract = {The solution for the diffraction problem of scattering of magnetostatic waves by an arbitrary shallow defect situated under the surface of a ferromagnetic film magnetized at an arbitrary angle is obtained in the quasi-static approximation. Expressions for the energy flux density of scattered magnetostatic waves in the far-field zone are found.},\\n\\turldate = {2023-11-11},\\n\\tbooktitle = {2014 {International} {Conference} on {Actual} {Problems} of {Electron} {Devices} {Engineering} ({APEDE})},\\n\\tauthor = {Timoshenko, P. E. and Babichev, R. K. and Vyatkina, S. A.},\\n\\tmonth = sep,\\n\\tyear = {2014},\\n\\tpages = {279--283},\\n}\\n\\n\",\"author_short\":[\"Timoshenko, P. E.\",\"Babichev, R. K.\",\"Vyatkina, S. A.\"],\"key\":\"timoshenko_scattering_2014\",\"id\":\"timoshenko_scattering_2014\",\"bibbaseid\":\"timoshenko-babichev-vyatkina-scatteringofmagnetostaticwavesbydefectsofthesurfaceofaferromagneticfilm-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://ieeexplore.ieee.org/document/6958761\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"Finite element simulation of surface acoustic waves excited in barium-strontium titanate films fabricated on magnesium oxide substrate by interdigital transducers\",\"volume\":\"1\",\"url\":\"https://ieeexplore.ieee.org/document/6958762\",\"doi\":\"10.1109/APEDE.2014.6958762\",\"abstract\":\"In this paper, we present study on surface acoustic waves excited in barium — strontium titanate films fabricated on magnesium oxide substrate by interdigital transducers. The surface acoustic waves propagation was simulated by using COMSOL Multiphysics™. The presence of bias, since the oscillations are not considered as sagittal polarized, is the principal difference between considered problem and standard problem that implemented in many finite element packages. The calculations of mechanic displacement and electric field potential for the first Eigen frequencies for different planes are shown. The methods of modeling in COMSOL Multiphysics™ software package are presented in this paper can be used for calculations of other systems that have different complex configuration.\",\"urldate\":\"2023-11-11\",\"booktitle\":\"2014 International Conference on Actual Problems of Electron Devices Engineering (APEDE)\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kalinchuk\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Levi\"],\"firstnames\":[\"M.\",\"O.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pan'kin\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Donets\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2014\",\"pages\":\"283–289\",\"bibtex\":\"@inproceedings{timoshenko_finite_2014,\\n\\ttitle = {Finite element simulation of surface acoustic waves excited in barium-strontium titanate films fabricated on magnesium oxide substrate by interdigital transducers},\\n\\tvolume = {1},\\n\\turl = {https://ieeexplore.ieee.org/document/6958762},\\n\\tdoi = {10.1109/APEDE.2014.6958762},\\n\\tabstract = {In this paper, we present study on surface acoustic waves excited in barium — strontium titanate films fabricated on magnesium oxide substrate by interdigital transducers. The surface acoustic waves propagation was simulated by using COMSOL Multiphysics™. The presence of bias, since the oscillations are not considered as sagittal polarized, is the principal difference between considered problem and standard problem that implemented in many finite element packages. The calculations of mechanic displacement and electric field potential for the first Eigen frequencies for different planes are shown. The methods of modeling in COMSOL Multiphysics™ software package are presented in this paper can be used for calculations of other systems that have different complex configuration.},\\n\\turldate = {2023-11-11},\\n\\tbooktitle = {2014 {International} {Conference} on {Actual} {Problems} of {Electron} {Devices} {Engineering} ({APEDE})},\\n\\tauthor = {Timoshenko, P. E. and Kalinchuk, V. V. and Shirokov, V. B. and Levi, M. O. and Pan'kin, A. V. and Donets, A. V.},\\n\\tmonth = sep,\\n\\tyear = {2014},\\n\\tpages = {283--289},\\n}\\n\\n\",\"author_short\":[\"Timoshenko, P. E.\",\"Kalinchuk, V. V.\",\"Shirokov, V. B.\",\"Levi, M. O.\",\"Pan'kin, A. V.\",\"Donets, A. V.\"],\"key\":\"timoshenko_finite_2014\",\"id\":\"timoshenko_finite_2014\",\"bibbaseid\":\"timoshenko-kalinchuk-shirokov-levi-pankin-donets-finiteelementsimulationofsurfaceacousticwavesexcitedinbariumstrontiumtitanatefilmsfabricatedonmagnesiumoxidesubstratebyinterdigitaltransducers-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://ieeexplore.ieee.org/document/6958762\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Synthesis and characterization of ZnO nanorods obtained by catalyst-free thermal technique\",\"volume\":\"541\",\"issn\":\"1742-6596\",\"url\":\"https://dx.doi.org/10.1088/1742-6596/541/1/012031\",\"doi\":\"10.1088/1742-6596/541/1/012031\",\"abstract\":\"ZnO nanorod arrays have been synthesized on silicon wafers by catalyst free thermal vapor deposition with different temperature values. Vertical-aligned ZnO nanostructures were grown at the quite low temperatures by this method. Modification of the method allowed to place silicon substrates in areas with different ratios of concentrations Ar and O2 molecules in the vapor phase. Photoluminescence spectroscopy and electron microscopy studies have shown that morphologies and optical properties of nanorods depends on different ratios of concentrations of the molecules in the vapor phase.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics: Conference Series\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Pushkariov\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nikolaev\"],\"firstnames\":[\"A.\",\"L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2014\",\"pages\":\"012031\",\"file\":\"IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\7WR58HGN\\\\¶ushkariov и др. - 2014 - Synthesis and characterization of ZnO nanorods obt.pdf:application/pdf\",\"bibtex\":\"@article{pushkariov_synthesis_2014,\\n\\ttitle = {Synthesis and characterization of {ZnO} nanorods obtained by catalyst-free thermal technique},\\n\\tvolume = {541},\\n\\tissn = {1742-6596},\\n\\turl = {https://dx.doi.org/10.1088/1742-6596/541/1/012031},\\n\\tdoi = {10.1088/1742-6596/541/1/012031},\\n\\tabstract = {ZnO nanorod arrays have been synthesized on silicon wafers by catalyst free thermal vapor deposition with different temperature values. Vertical-aligned ZnO nanostructures were grown at the quite low temperatures by this method. Modification of the method allowed to place silicon substrates in areas with different ratios of concentrations Ar and O2 molecules in the vapor phase. Photoluminescence spectroscopy and electron microscopy studies have shown that morphologies and optical properties of nanorods depends on different ratios of concentrations of the molecules in the vapor phase.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics: Conference Series},\\n\\tauthor = {Pushkariov, V. I. and Nikolaev, A. L. and Kaidashev, E. M.},\\n\\tmonth = oct,\\n\\tyear = {2014},\\n\\tpages = {012031},\\n\\tfile = {IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\7WR58HGN\\\\\\\\Pushkariov и др. - 2014 - Synthesis and characterization of ZnO nanorods obt.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Pushkariov, V. I.\",\"Nikolaev, A. L.\",\"Kaidashev, E. M.\"],\"key\":\"pushkariov_synthesis_2014\",\"id\":\"pushkariov_synthesis_2014\",\"bibbaseid\":\"pushkariov-nikolaev-kaidashev-synthesisandcharacterizationofznonanorodsobtainedbycatalystfreethermaltechnique-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/1742-6596/541/1/012031\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Pulsed laser deposition and investigation of antimony-doped ZnO films\",\"volume\":\"541\",\"issn\":\"1742-6596\",\"url\":\"https://dx.doi.org/10.1088/1742-6596/541/1/012004\",\"doi\":\"10.1088/1742-6596/541/1/012004\",\"abstract\":\"We have investigated the influence of oxygen partial pressure, temperature of synthesis and annealing conditions on nanocsrystallineSb-doped thin films, grown by pulsed laser deposition. It is shown that the minimum resistivity ( 8·10−3Ω·cm) and the maximum carriers density ( 2·1019 cm-3) corresponds to the pressure range 5·10−3-7·10−3 mbar, to the temperature 550 ° C and in situ annealing at 700 °C.Also we show the features of the crystal lattice's dynamics, which are found in the Raman research.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics: Conference Series\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Puzikov\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lyanguzov\"],\"firstnames\":[\"N.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2014\",\"pages\":\"012004\",\"file\":\"IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\6̋J3GSQ8\\\\¶uzikov и др. - 2014 - Pulsed laser deposition and investigation of antim.pdf:application/pdf\",\"bibtex\":\"@article{puzikov_pulsed_2014,\\n\\ttitle = {Pulsed laser deposition and investigation of antimony-doped {ZnO} films},\\n\\tvolume = {541},\\n\\tissn = {1742-6596},\\n\\turl = {https://dx.doi.org/10.1088/1742-6596/541/1/012004},\\n\\tdoi = {10.1088/1742-6596/541/1/012004},\\n\\tabstract = {We have investigated the influence of oxygen partial pressure, temperature of synthesis and annealing conditions on nanocsrystallineSb-doped thin films, grown by pulsed laser deposition. It is shown that the minimum resistivity ( 8·10−3Ω·cm) and the maximum carriers density ( 2·1019 cm-3) corresponds to the pressure range 5·10−3-7·10−3 mbar, to the temperature 550 ° C and in situ annealing at 700 °C.Also we show the features of the crystal lattice's dynamics, which are found in the Raman research.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics: Conference Series},\\n\\tauthor = {Puzikov, A. S. and Lyanguzov, N. V. and Kaidashev, E. M.},\\n\\tmonth = oct,\\n\\tyear = {2014},\\n\\tpages = {012004},\\n\\tfile = {IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\H6J3GSQ8\\\\\\\\Puzikov и др. - 2014 - Pulsed laser deposition and investigation of antim.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Puzikov, A. S.\",\"Lyanguzov, N. V.\",\"Kaidashev, E. M.\"],\"key\":\"puzikov_pulsed_2014\",\"id\":\"puzikov_pulsed_2014\",\"bibbaseid\":\"puzikov-lyanguzov-kaidashev-pulsedlaserdepositionandinvestigationofantimonydopedznofilms-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/1742-6596/541/1/012004\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"Experimental investigation of magnetostatic backward volume waves excited by the narrow transducer\",\"volume\":\"1\",\"url\":\"https://ieeexplore.ieee.org/document/6958745\",\"doi\":\"10.1109/APEDE.2014.6958745\",\"abstract\":\"The results of experimental investigation of diffraction profiles of magnetostatic backward volume waves (MSBVW) exited by the linear transducer with finite length located at the surface of ferrite-dielectric structure are presented. The comparison of experimental data obtained and theoretical calculations is reported.\",\"urldate\":\"2023-11-11\",\"booktitle\":\"2014 International Conference on Actual Problems of Electron Devices Engineering (APEDE)\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Nistratov\"],\"firstnames\":[\"N.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vyatkina\"],\"firstnames\":[\"S.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Babichev\"],\"firstnames\":[\"R.\",\"K.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2014\",\"pages\":\"199–204\",\"bibtex\":\"@inproceedings{nistratov_experimental_2014,\\n\\ttitle = {Experimental investigation of magnetostatic backward volume waves excited by the narrow transducer},\\n\\tvolume = {1},\\n\\turl = {https://ieeexplore.ieee.org/document/6958745},\\n\\tdoi = {10.1109/APEDE.2014.6958745},\\n\\tabstract = {The results of experimental investigation of diffraction profiles of magnetostatic backward volume waves (MSBVW) exited by the linear transducer with finite length located at the surface of ferrite-dielectric structure are presented. The comparison of experimental data obtained and theoretical calculations is reported.},\\n\\turldate = {2023-11-11},\\n\\tbooktitle = {2014 {International} {Conference} on {Actual} {Problems} of {Electron} {Devices} {Engineering} ({APEDE})},\\n\\tauthor = {Nistratov, N. P. and Vyatkina, S. A. and Babichev, R. K. and Timoshenko, P. E.},\\n\\tmonth = sep,\\n\\tyear = {2014},\\n\\tpages = {199--204},\\n}\\n\\n\",\"author_short\":[\"Nistratov, N. P.\",\"Vyatkina, S. A.\",\"Babichev, R. K.\",\"Timoshenko, P. E.\"],\"key\":\"nistratov_experimental_2014\",\"id\":\"nistratov_experimental_2014\",\"bibbaseid\":\"nistratov-vyatkina-babichev-timoshenko-experimentalinvestigationofmagnetostaticbackwardvolumewavesexcitedbythenarrowtransducer-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://ieeexplore.ieee.org/document/6958745\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Vibrational states of a water molecule in a nano-cavity of beryl crystal lattice\",\"volume\":\"140\",\"issn\":\"0021-9606\",\"url\":\"https://doi.org/10.1063/1.4882062\",\"doi\":\"10.1063/1.4882062\",\"abstract\":\"Low-energy excitations of a single water molecule are studied when confined within a nano-size cavity formed by the ionic crystal lattice. Optical spectra are measured of manganese doped beryl single crystal Mn:Be3Al2Si6O18, that contains water molecules individually isolated in 0.51 nm diameter voids within the crystal lattice. Two types of orientation are distinguished: water-I molecules have their dipole moments aligned perpendicular to the c axis and dipole moments of water-II molecules are parallel to the c-axis. The optical conductivity σ(ν) and permittivity ɛ′(ν) spectra are recorded in terahertz and infrared ranges, at frequencies from several wavenumbers up to ν = 7000 cm−1, at temperatures 5–300 K and for two polarizations, when the electric vector E of the radiation is parallel and perpendicular to the c-axis. Comparative experiments on as-grown and on dehydrated samples allow to identify the spectra of σ(ν) and ɛ′(ν) caused exclusively by water molecules. In the infrared range, well-known internal modes ν1, ν2, and ν3 of the H2O molecule are observed for both polarizations, indicating the presence of water-I and water-II molecules in the crystal. Spectra recorded below 1000 cm−1 reveal a rich set of highly anisotropic features in the low-energy response of H2O molecule in a crystalline nano-cavity. While for E∥c only two absorption peaks are detected, at ∼90 cm−1 and ∼160 cm−1, several absorption bands are discovered for E⊥c, each consisting of narrower resonances. The bands are assigned to librational (400–500 cm−1) and translational (150–200 cm−1) vibrations of water-I molecule that is weakly coupled to the nano-cavity “walls.” A model is presented that explains the “fine structure” of the bands by a splitting of the energy levels due to quantum tunneling between the minima in a six-well potential relief felt by a molecule within the cavity.\",\"number\":\"22\",\"urldate\":\"2023-11-11\",\"journal\":\"The Journal of Chemical Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"Elena\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"Victor\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"Boris\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lebedev\"],\"firstnames\":[\"Vladimir\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shakurov\"],\"firstnames\":[\"Gil'man\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kremer\"],\"firstnames\":[\"Reinhard\",\"K.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pestrjakov\"],\"firstnames\":[\"Efim\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Thomas\"],\"firstnames\":[\"Victor\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fursenko\"],\"firstnames\":[\"Dimitry\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"Anatoly\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"Martin\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2014\",\"pages\":\"224317\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\776RNGVS\\\\\\\\Zhukova и др. - 2014 - Vibrational states of a water molecule in a nano-c.pdf:application/pdf\",\"bibtex\":\"@article{zhukova_vibrational_2014,\\n\\ttitle = {Vibrational states of a water molecule in a nano-cavity of beryl crystal lattice},\\n\\tvolume = {140},\\n\\tissn = {0021-9606},\\n\\turl = {https://doi.org/10.1063/1.4882062},\\n\\tdoi = {10.1063/1.4882062},\\n\\tabstract = {Low-energy excitations of a single water molecule are studied when confined within a nano-size cavity formed by the ionic crystal lattice. Optical spectra are measured of manganese doped beryl single crystal Mn:Be3Al2Si6O18, that contains water molecules individually isolated in 0.51 nm diameter voids within the crystal lattice. Two types of orientation are distinguished: water-I molecules have their dipole moments aligned perpendicular to the c axis and dipole moments of water-II molecules are parallel to the c-axis. The optical conductivity σ(ν) and permittivity ɛ′(ν) spectra are recorded in terahertz and infrared ranges, at frequencies from several wavenumbers up to ν = 7000 cm−1, at temperatures 5–300 K and for two polarizations, when the electric vector E of the radiation is parallel and perpendicular to the c-axis. Comparative experiments on as-grown and on dehydrated samples allow to identify the spectra of σ(ν) and ɛ′(ν) caused exclusively by water molecules. In the infrared range, well-known internal modes ν1, ν2, and ν3 of the H2O molecule are observed for both polarizations, indicating the presence of water-I and water-II molecules in the crystal. Spectra recorded below 1000 cm−1 reveal a rich set of highly anisotropic features in the low-energy response of H2O molecule in a crystalline nano-cavity. While for E∥c only two absorption peaks are detected, at ∼90 cm−1 and ∼160 cm−1, several absorption bands are discovered for E⊥c, each consisting of narrower resonances. The bands are assigned to librational (400–500 cm−1) and translational (150–200 cm−1) vibrations of water-I molecule that is weakly coupled to the nano-cavity “walls.” A model is presented that explains the “fine structure” of the bands by a splitting of the energy levels due to quantum tunneling between the minima in a six-well potential relief felt by a molecule within the cavity.},\\n\\tnumber = {22},\\n\\turldate = {2023-11-11},\\n\\tjournal = {The Journal of Chemical Physics},\\n\\tauthor = {Zhukova, Elena S. and Torgashev, Victor I. and Gorshunov, Boris P. and Lebedev, Vladimir V. and Shakurov, Gil'man S. and Kremer, Reinhard K. and Pestrjakov, Efim V. and Thomas, Victor G. and Fursenko, Dimitry A. and Prokhorov, Anatoly S. and Dressel, Martin},\\n\\tmonth = jun,\\n\\tyear = {2014},\\n\\tpages = {224317},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\776RNGVS\\\\\\\\Zhukova и др. - 2014 - Vibrational states of a water molecule in a nano-c.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Zhukova, E. S.\",\"Torgashev, V. I.\",\"Gorshunov, B. P.\",\"Lebedev, V. V.\",\"Shakurov, G. S.\",\"Kremer, R. K.\",\"Pestrjakov, E. V.\",\"Thomas, V. G.\",\"Fursenko, D. A.\",\"Prokhorov, A. S.\",\"Dressel, M.\"],\"key\":\"zhukova_vibrational_2014\",\"id\":\"zhukova_vibrational_2014\",\"bibbaseid\":\"zhukova-torgashev-gorshunov-lebedev-shakurov-kremer-pestrjakov-thomas-etal-vibrationalstatesofawatermoleculeinananocavityofberylcrystallattice-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.4882062\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Size dependence of the lattice parameters of carbon supported platinum nanoparticles: X-ray diffraction analysis and theoretical considerations\",\"volume\":\"4\",\"issn\":\"2046-2069\",\"shorttitle\":\"Size dependence of the lattice parameters of carbon supported platinum nanoparticles\",\"url\":\"https://pubs.rsc.org/en/content/articlelanding/2014/ra/c4ra04809a\",\"doi\":\"10.1039/C4RA04809A\",\"abstract\":\"Carbon supported Pt nanoparticles with diameters ranging from 2 to 28 nm have been studied using X-ray diffraction. The unit cell parameter of synthesized Pt/C nanoparticles is always lower than that of bulk Pt. By decreasing the average particle size D to approximately 2 nm, the unit cell parameter a nonlinearly decreases by about 0.03 Å which corresponds to a variation of 0.7% in comparison to bulk Pt, and the size effect is predominant for sizes ranging from 2 to 10 nm. The dependence a(1/D) is approximated well using a straight line with a slope of −0.0555 ± 0.0067 nm−1 and an intercept of −3.9230 ± 0.0017 Å. For interpreting the obtained experimental dependence of the unit cell parameter of Pt/C nanoparticles, four different theoretical approaches such as the thermal vacancy mechanism, continuous-medium model, Laplace pressure, and bond order–length–strength correlation mechanism, were used. Comparison of the calculated dependencies, based on the above models, with the experimental ones, shows that the continuous-medium model agrees best with the experimentally found unit cell parameter dependence of our carbon supported Pt nanoparticles.\",\"language\":\"en\",\"number\":\"68\",\"urldate\":\"2023-11-11\",\"journal\":\"RSC Advances\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"A.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"N.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hennet\"],\"firstnames\":[\"L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rakhmatullin\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"N.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dmitriev\"],\"firstnames\":[\"V.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2014\",\"note\":\"Publisher: The Royal Society of Chemistry\",\"pages\":\"35959–35965\",\"bibtex\":\"@article{leontyev_size_2014,\\n\\ttitle = {Size dependence of the lattice parameters of carbon supported platinum nanoparticles: {X}-ray diffraction analysis and theoretical considerations},\\n\\tvolume = {4},\\n\\tissn = {2046-2069},\\n\\tshorttitle = {Size dependence of the lattice parameters of carbon supported platinum nanoparticles},\\n\\turl = {https://pubs.rsc.org/en/content/articlelanding/2014/ra/c4ra04809a},\\n\\tdoi = {10.1039/C4RA04809A},\\n\\tabstract = {Carbon supported Pt nanoparticles with diameters ranging from 2 to 28 nm have been studied using X-ray diffraction. The unit cell parameter of synthesized Pt/C nanoparticles is always lower than that of bulk Pt. By decreasing the average particle size D to approximately 2 nm, the unit cell parameter a nonlinearly decreases by about 0.03 Å which corresponds to a variation of 0.7\\\\% in comparison to bulk Pt, and the size effect is predominant for sizes ranging from 2 to 10 nm. The dependence a(1/D) is approximated well using a straight line with a slope of −0.0555 ± 0.0067 nm−1 and an intercept of −3.9230 ± 0.0017 Å. For interpreting the obtained experimental dependence of the unit cell parameter of Pt/C nanoparticles, four different theoretical approaches such as the thermal vacancy mechanism, continuous-medium model, Laplace pressure, and bond order–length–strength correlation mechanism, were used. Comparison of the calculated dependencies, based on the above models, with the experimental ones, shows that the continuous-medium model agrees best with the experimentally found unit cell parameter dependence of our carbon supported Pt nanoparticles.},\\n\\tlanguage = {en},\\n\\tnumber = {68},\\n\\turldate = {2023-11-11},\\n\\tjournal = {RSC Advances},\\n\\tauthor = {Leontyev, I. N. and Kuriganova, A. B. and Leontyev, N. G. and Hennet, L. and Rakhmatullin, A. and Smirnova, N. V. and Dmitriev, V.},\\n\\tmonth = aug,\\n\\tyear = {2014},\\n\\tnote = {Publisher: The Royal Society of Chemistry},\\n\\tpages = {35959--35965},\\n}\\n\\n\",\"author_short\":[\"Leontyev, I. N.\",\"Kuriganova, A. B.\",\"Leontyev, N. G.\",\"Hennet, L.\",\"Rakhmatullin, A.\",\"Smirnova, N. V.\",\"Dmitriev, V.\"],\"key\":\"leontyev_size_2014\",\"id\":\"leontyev_size_2014\",\"bibbaseid\":\"leontyev-kuriganova-leontyev-hennet-rakhmatullin-smirnova-dmitriev-sizedependenceofthelatticeparametersofcarbonsupportedplatinumnanoparticlesxraydiffractionanalysisandtheoreticalconsiderations-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://pubs.rsc.org/en/content/articlelanding/2014/ra/c4ra04809a\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Strain engineering of perovskite thin films using a single substrate\",\"volume\":\"26\",\"issn\":\"0953-8984\",\"url\":\"https://dx.doi.org/10.1088/0953-8984/26/29/292201\",\"doi\":\"10.1088/0953-8984/26/29/292201\",\"abstract\":\"Combining temperature-dependent x-ray diffraction, Raman spectroscopy and first-principles-based effective Hamiltonian calculations, we show that varying the thickness of (Ba0.8Sr0.2)TiO3 (BST) thin films deposited on the same single substrate (namely, MgO) enables us to change not only the magnitude but also the sign of the misfit strain. Such previously overlooked control of the strain allows several properties of these films (e.g. Curie temperature, symmetry of ferroelectric phases, dielectric response) to be tuned and even optimized. Surprisingly, such desired control of the strain (and of the resulting properties) originates from an effect that is commonly believed to be detrimental to functionalities of films, namely the existence of misfit dislocations. The present study therefore provides a novel route to strain engineering, as well as leading us to revisit common beliefs.\",\"language\":\"en\",\"number\":\"29\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics: Condensed Matter\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Janolin\"],\"firstnames\":[\"P.-E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Anokhin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gui\"],\"firstnames\":[\"Z.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mukhortov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golovko\"],\"firstnames\":[\"Yu\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Guiblin\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ravy\"],\"firstnames\":[\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Marssi\"],\"firstnames\":[\"M.\",\"El\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bellaiche\"],\"firstnames\":[\"L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dkhil\"],\"firstnames\":[\"B.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2014\",\"note\":\"Publisher: IOP Publishing\",\"pages\":\"292201\",\"bibtex\":\"@article{janolin_strain_2014,\\n\\ttitle = {Strain engineering of perovskite thin films using a single substrate},\\n\\tvolume = {26},\\n\\tissn = {0953-8984},\\n\\turl = {https://dx.doi.org/10.1088/0953-8984/26/29/292201},\\n\\tdoi = {10.1088/0953-8984/26/29/292201},\\n\\tabstract = {Combining temperature-dependent x-ray diffraction, Raman spectroscopy and first-principles-based effective Hamiltonian calculations, we show that varying the thickness of (Ba0.8Sr0.2)TiO3 (BST) thin films deposited on the same single substrate (namely, MgO) enables us to change not only the magnitude but also the sign of the misfit strain. Such previously overlooked control of the strain allows several properties of these films (e.g. Curie temperature, symmetry of ferroelectric phases, dielectric response) to be tuned and even optimized. Surprisingly, such desired control of the strain (and of the resulting properties) originates from an effect that is commonly believed to be detrimental to functionalities of films, namely the existence of misfit dislocations. The present study therefore provides a novel route to strain engineering, as well as leading us to revisit common beliefs.},\\n\\tlanguage = {en},\\n\\tnumber = {29},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics: Condensed Matter},\\n\\tauthor = {Janolin, P.-E. and Anokhin, A. S. and Gui, Z. and Mukhortov, V. M. and Golovko, Yu I. and Guiblin, N. and Ravy, S. and Marssi, M. El and Yuzyuk, Yu I. and Bellaiche, L. and Dkhil, B.},\\n\\tmonth = jun,\\n\\tyear = {2014},\\n\\tnote = {Publisher: IOP Publishing},\\n\\tpages = {292201},\\n}\\n\\n\",\"author_short\":[\"Janolin, P.\",\"Anokhin, A. S.\",\"Gui, Z.\",\"Mukhortov, V. M.\",\"Golovko, Y. I.\",\"Guiblin, N.\",\"Ravy, S.\",\"Marssi, M. E.\",\"Yuzyuk, Y. I.\",\"Bellaiche, L.\",\"Dkhil, B.\"],\"key\":\"janolin_strain_2014\",\"id\":\"janolin_strain_2014\",\"bibbaseid\":\"janolin-anokhin-gui-mukhortov-golovko-guiblin-ravy-marssi-etal-strainengineeringofperovskitethinfilmsusingasinglesubstrate-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/0953-8984/26/29/292201\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Extended topological defects as sources and outlets of dislocations in spherical hexagonal crystals\",\"volume\":\"378\",\"issn\":\"0375-9601\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0375960114002941\",\"doi\":\"10.1016/j.physleta.2014.03.037\",\"abstract\":\"Extended topological defects (ETDs) arising in spherical hexagonal crystals due to their curvature are considered. These prevalent defects carry a unit total topological charge and are surrounded by scalene pentagonal boundaries. Topological peculiarities of reactions between ETDs and dislocations are considered. Similarly to boundaries of the usual planar crystalline order the ETDs emit and absorb the dislocations without preservation of their dislocational charge. Dislocations located inside the ETD area lose it and the enforced ETD decay can proceed in different ways without conservation of the total Burgers vector of the dislocations emitted.\",\"number\":\"21\",\"urldate\":\"2023-11-11\",\"journal\":\"Physics Letters A\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Roshal\"],\"firstnames\":[\"D.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Petrov\"],\"firstnames\":[\"K.\",\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Myasnikova\"],\"firstnames\":[\"A.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2014\",\"keywords\":\"Colloidal crystals, Curvature, Disclinations, Dislocations, Spherical structures, Topological defects\",\"pages\":\"1548–1552\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\VVC82RZB\\\\\\\\Roshal и др. - 2014 - Extended topological defects as sources and outlet.pdf:application/pdf\",\"bibtex\":\"@article{roshal_extended_2014,\\n\\ttitle = {Extended topological defects as sources and outlets of dislocations in spherical hexagonal crystals},\\n\\tvolume = {378},\\n\\tissn = {0375-9601},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0375960114002941},\\n\\tdoi = {10.1016/j.physleta.2014.03.037},\\n\\tabstract = {Extended topological defects (ETDs) arising in spherical hexagonal crystals due to their curvature are considered. These prevalent defects carry a unit total topological charge and are surrounded by scalene pentagonal boundaries. Topological peculiarities of reactions between ETDs and dislocations are considered. Similarly to boundaries of the usual planar crystalline order the ETDs emit and absorb the dislocations without preservation of their dislocational charge. Dislocations located inside the ETD area lose it and the enforced ETD decay can proceed in different ways without conservation of the total Burgers vector of the dislocations emitted.},\\n\\tnumber = {21},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physics Letters A},\\n\\tauthor = {Roshal, D. S. and Petrov, K. Yu. and Myasnikova, A. E. and Rochal, S. B.},\\n\\tmonth = apr,\\n\\tyear = {2014},\\n\\tkeywords = {Colloidal crystals, Curvature, Disclinations, Dislocations, Spherical structures, Topological defects},\\n\\tpages = {1548--1552},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\VVC82RZB\\\\\\\\Roshal и др. - 2014 - Extended topological defects as sources and outlet.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Roshal, D. S.\",\"Petrov, K. Y.\",\"Myasnikova, A. E.\",\"Rochal, S. B.\"],\"key\":\"roshal_extended_2014\",\"id\":\"roshal_extended_2014\",\"bibbaseid\":\"roshal-petrov-myasnikova-rochal-extendedtopologicaldefectsassourcesandoutletsofdislocationsinsphericalhexagonalcrystals-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0375960114002941\"},\"keyword\":[\"Colloidal crystals\",\"Curvature\",\"Disclinations\",\"Dislocations\",\"Spherical structures\",\"Topological defects\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Longitudinal and Transversal Polarization Switching in Strained Ferroelectrics\",\"volume\":\"461\",\"issn\":\"0015-0193\",\"url\":\"https://doi.org/10.1080/00150193.2014.889528\",\"doi\":\"10.1080/00150193.2014.889528\",\"abstract\":\"Using the multicomponent Landau-Devonshire functional we study the field-induced polarization switching in c-oriented ferroelectric phase of epitaxial perovskite film and found that two different regimes are possible: (i) longitudinal switching with change of the polarization modulus and (ii) transversal switching with virtual admixing of the a-component of polarization. The results are specified for the case of barium titanate oxide BaTiO3where the crossover line between two types of switching is found at strain-temperature phase diagram.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Baudry\"],\"firstnames\":[\"L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Luk’yanchuk\"],\"firstnames\":[\"I.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2014\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2014.889528\",\"keywords\":\"Ferroelectric thin films, strain, switching\",\"pages\":\"22–28\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\XAP4K9W5\\\\\\\\Baudry и др. - 2014 - Longitudinal and Transversal Polarization Switchin.pdf:application/pdf\",\"bibtex\":\"@article{baudry_longitudinal_2014,\\n\\ttitle = {Longitudinal and {Transversal} {Polarization} {Switching} in {Strained} {Ferroelectrics}},\\n\\tvolume = {461},\\n\\tissn = {0015-0193},\\n\\turl = {https://doi.org/10.1080/00150193.2014.889528},\\n\\tdoi = {10.1080/00150193.2014.889528},\\n\\tabstract = {Using the multicomponent Landau-Devonshire functional we study the field-induced polarization switching in c-oriented ferroelectric phase of epitaxial perovskite film and found that two different regimes are possible: (i) longitudinal switching with change of the polarization modulus and (ii) transversal switching with virtual admixing of the a-component of polarization. The results are specified for the case of barium titanate oxide BaTiO3where the crossover line between two types of switching is found at strain-temperature phase diagram.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Baudry, L. and Luk’yanchuk, I. A. and Razumnaya, A.},\\n\\tmonth = mar,\\n\\tyear = {2014},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/00150193.2014.889528},\\n\\tkeywords = {Ferroelectric thin films, strain, switching},\\n\\tpages = {22--28},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\XAP4K9W5\\\\\\\\Baudry и др. - 2014 - Longitudinal and Transversal Polarization Switchin.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Baudry, L.\",\"Luk’yanchuk, I. A.\",\"Razumnaya, A.\"],\"key\":\"baudry_longitudinal_2014\",\"id\":\"baudry_longitudinal_2014\",\"bibbaseid\":\"baudry-lukyanchuk-razumnaya-longitudinalandtransversalpolarizationswitchinginstrainedferroelectrics-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/00150193.2014.889528\"},\"keyword\":[\"Ferroelectric thin films\",\"strain\",\"switching\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Quantum behaviour of water molecule in gemstone: terahertz fingerprints\",\"volume\":\"486\",\"issn\":\"1742-6596\",\"shorttitle\":\"Quantum behaviour of water molecule in gemstone\",\"url\":\"https://dx.doi.org/10.1088/1742-6596/486/1/012019\",\"doi\":\"10.1088/1742-6596/486/1/012019\",\"abstract\":\"We have shown that a weak interaction of a lone H2O molecule with the ‘‘walls’’ of nano-sized crystalline cage of gemstone (beryl) results in emergence of a rich set of molecular vibrational states. By analogy with translational and librational bands in liquid water and ice corresponding absorption bands are explained as due to translational (T) and librational (L) movements of the H2O molecule which is hydrogen bonded to the cage walls. In beryl crystal lattice, however, the six-fold symmetry of the cage brings about additional effect of splitting of the T and L bands into fine structure due to tunnelling within the six-well potential relief. The presented results will be of use for analysis of more complicated systems with confined water molecules like H2O chains in carbon nano-tubes, molecular clusters in e.g. zeolites, clays, silica gels and other natural or synthetic frameworks, as well as for interfacial water in biological systems.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics: Conference Series\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"Elena\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"Boris\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"Victor\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lebedev\"],\"firstnames\":[\"Vladimir\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shakurov\"],\"firstnames\":[\"Gil'man\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kremer\"],\"firstnames\":[\"Reinhard\",\"K.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pestrjakov\"],\"firstnames\":[\"Efim\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Thomas\"],\"firstnames\":[\"Victor\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fursenko\"],\"firstnames\":[\"Dimitry\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"Martin\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2014\",\"pages\":\"012019\",\"file\":\"IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\E6MX2SN9\\\\\\\\Zhukova и др. - 2014 - Quantum behaviour of water molecule in gemstone t.pdf:application/pdf\",\"bibtex\":\"@article{zhukova_quantum_2014,\\n\\ttitle = {Quantum behaviour of water molecule in gemstone: terahertz fingerprints},\\n\\tvolume = {486},\\n\\tissn = {1742-6596},\\n\\tshorttitle = {Quantum behaviour of water molecule in gemstone},\\n\\turl = {https://dx.doi.org/10.1088/1742-6596/486/1/012019},\\n\\tdoi = {10.1088/1742-6596/486/1/012019},\\n\\tabstract = {We have shown that a weak interaction of a lone H2O molecule with the ‘‘walls’’ of nano-sized crystalline cage of gemstone (beryl) results in emergence of a rich set of molecular vibrational states. By analogy with translational and librational bands in liquid water and ice corresponding absorption bands are explained as due to translational (T) and librational (L) movements of the H2O molecule which is hydrogen bonded to the cage walls. In beryl crystal lattice, however, the six-fold symmetry of the cage brings about additional effect of splitting of the T and L bands into fine structure due to tunnelling within the six-well potential relief. The presented results will be of use for analysis of more complicated systems with confined water molecules like H2O chains in carbon nano-tubes, molecular clusters in e.g. zeolites, clays, silica gels and other natural or synthetic frameworks, as well as for interfacial water in biological systems.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics: Conference Series},\\n\\tauthor = {Zhukova, Elena S. and Gorshunov, Boris P. and Torgashev, Victor I. and Lebedev, Vladimir V. and Shakurov, Gil'man S. and Kremer, Reinhard K. and Pestrjakov, Efim V. and Thomas, Victor G. and Fursenko, Dimitry A. and Dressel, Martin},\\n\\tmonth = mar,\\n\\tyear = {2014},\\n\\tpages = {012019},\\n\\tfile = {IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\E6MX2SN9\\\\\\\\Zhukova и др. - 2014 - Quantum behaviour of water molecule in gemstone t.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Zhukova, E. S.\",\"Gorshunov, B. P.\",\"Torgashev, V. I.\",\"Lebedev, V. V.\",\"Shakurov, G. S.\",\"Kremer, R. K.\",\"Pestrjakov, E. V.\",\"Thomas, V. G.\",\"Fursenko, D. A.\",\"Dressel, M.\"],\"key\":\"zhukova_quantum_2014\",\"id\":\"zhukova_quantum_2014\",\"bibbaseid\":\"zhukova-gorshunov-torgashev-lebedev-shakurov-kremer-pestrjakov-thomas-etal-quantumbehaviourofwatermoleculeingemstoneterahertzfingerprints-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/1742-6596/486/1/012019\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Atomic order in the spinel structure – a group-theoretical analysis\",\"volume\":\"70\",\"copyright\":\"Copyright (c) 2014 International Union of Crystallography\",\"issn\":\"2053-2733\",\"url\":\"http://scripts.iucr.org/cgi-bin/paper?kx5021\",\"doi\":\"10.1107/S2053273313027605\",\"abstract\":\"Group-theoretical methods of the Landau theory of phase transitions are used to investigate the structures of ordered spinels. The possibility of the existence is determined of 305 phases with different types of order in Wyckoff position 8a (including seven binary and seven ternary cation substructures), 537 phases in Wyckoff position 16d (including eight binary and 11 ternary cation substructures), 595 phases in Wyckoff position 32e (including seven binary and four ternary anion substructures) and 549 phases with simultaneous ordering in Wyckoff positions 8a and 16d (including five substructures with binary order in tetrahedral and octahedral sublattices, two substructures with ternary order in both spinel sublattices, and nine substructures with different combined types of binary and ternary order). Theoretical results and experimental data are compared. Calculated structures of the spread types of ordered low-symmetry spinel modifications are given.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Acta Crystallographica Section A: Foundations and Advances\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2014\",\"note\":\"Number: 1 Publisher: International Union of Crystallography\",\"pages\":\"49–63\",\"bibtex\":\"@article{talanov_atomic_2014,\\n\\ttitle = {Atomic order in the spinel structure – a group-theoretical analysis},\\n\\tvolume = {70},\\n\\tcopyright = {Copyright (c) 2014 International Union of Crystallography},\\n\\tissn = {2053-2733},\\n\\turl = {http://scripts.iucr.org/cgi-bin/paper?kx5021},\\n\\tdoi = {10.1107/S2053273313027605},\\n\\tabstract = {Group-theoretical methods of the Landau theory of phase transitions are used to investigate the structures of ordered spinels. The possibility of the existence is determined of 305 phases with different types of order in Wyckoff position 8a (including seven binary and seven ternary cation substructures), 537 phases in Wyckoff position 16d (including eight binary and 11 ternary cation substructures), 595 phases in Wyckoff position 32e (including seven binary and four ternary anion substructures) and 549 phases with simultaneous ordering in Wyckoff positions 8a and 16d (including five substructures with binary order in tetrahedral and octahedral sublattices, two substructures with ternary order in both spinel sublattices, and nine substructures with different combined types of binary and ternary order). Theoretical results and experimental data are compared. Calculated structures of the spread types of ordered low-symmetry spinel modifications are given.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Acta Crystallographica Section A: Foundations and Advances},\\n\\tauthor = {Talanov, V. M. and Shirokov, V. B.},\\n\\tmonth = jan,\\n\\tyear = {2014},\\n\\tnote = {Number: 1\\nPublisher: International Union of Crystallography},\\n\\tpages = {49--63},\\n}\\n\\n\",\"author_short\":[\"Talanov, V. M.\",\"Shirokov, V. B.\"],\"key\":\"talanov_atomic_2014\",\"id\":\"talanov_atomic_2014\",\"bibbaseid\":\"talanov-shirokov-atomicorderinthespinelstructureagrouptheoreticalanalysis-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://scripts.iucr.org/cgi-bin/paper?kx5021\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Effect of thermal annealing on the surface of sol-gel prepared oxide film studied by atomic force microscopy and Raman spectroscopy\",\"volume\":\"40\",\"issn\":\"1608-313X\",\"url\":\"https://doi.org/10.1134/S1087659614010192\",\"doi\":\"10.1134/S1087659614010192\",\"abstract\":\"In this work, we have investigated the surface topography evolution of sol-gel deposited SiO2-SnO2 nanocomposite films annealed in the temperature range 200–600°C. The fractal dimension of atomic force microscopy images of the films was determined by the cube counting method and the triangulation method. The fractal dimension was shown to be an appropriate and easy to use tool for the characterization of nanosized thin film structures. Raman spectroscopy revealed the formation of a SiO2 cage-like structure at 400°C and SnO2 crystallization above 500°C.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Glass Physics and Chemistry\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Ponomareva\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Moshnikov\"],\"firstnames\":[\"V.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"O.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Suchaneck\"],\"firstnames\":[\"G.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2014\",\"keywords\":\"nanocomposite SiO2-SnO2, the sol-gel method\",\"pages\":\"99–105\",\"bibtex\":\"@article{ponomareva_effect_2014,\\n\\ttitle = {Effect of thermal annealing on the surface of sol-gel prepared oxide film studied by atomic force microscopy and {Raman} spectroscopy},\\n\\tvolume = {40},\\n\\tissn = {1608-313X},\\n\\turl = {https://doi.org/10.1134/S1087659614010192},\\n\\tdoi = {10.1134/S1087659614010192},\\n\\tabstract = {In this work, we have investigated the surface topography evolution of sol-gel deposited SiO2-SnO2 nanocomposite films annealed in the temperature range 200–600°C. The fractal dimension of atomic force microscopy images of the films was determined by the cube counting method and the triangulation method. The fractal dimension was shown to be an appropriate and easy to use tool for the characterization of nanosized thin film structures. Raman spectroscopy revealed the formation of a SiO2 cage-like structure at 400°C and SnO2 crystallization above 500°C.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Glass Physics and Chemistry},\\n\\tauthor = {Ponomareva, A. A. and Moshnikov, V. A. and Maslova, O. A. and Yuzyuk, Yu. I. and Suchaneck, G.},\\n\\tmonth = jan,\\n\\tyear = {2014},\\n\\tkeywords = {nanocomposite SiO2-SnO2, the sol-gel method},\\n\\tpages = {99--105},\\n}\\n\\n\",\"author_short\":[\"Ponomareva, A. A.\",\"Moshnikov, V. A.\",\"Maslova, O. A.\",\"Yuzyuk, Y. I.\",\"Suchaneck, G.\"],\"key\":\"ponomareva_effect_2014\",\"id\":\"ponomareva_effect_2014\",\"bibbaseid\":\"ponomareva-moshnikov-maslova-yuzyuk-suchaneck-effectofthermalannealingonthesurfaceofsolgelpreparedoxidefilmstudiedbyatomicforcemicroscopyandramanspectroscopy-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1087659614010192\"},\"keyword\":[\"nanocomposite SiO2-SnO2\",\"the sol-gel method\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Boson peak in manganites\",\"volume\":\"486\",\"issn\":\"1742-6596\",\"url\":\"https://dx.doi.org/10.1088/1742-6596/486/1/012001\",\"doi\":\"10.1088/1742-6596/486/1/012001\",\"abstract\":\"After the phase transition occurs in manganites La1-xCaxMnO3 (x ≥ 0.5) into a dielectric phase with charge order, right below the corresponding temperature of TCO = 240 K a series of absorption lines appear in the terahertz spectral range, only in case of commensurate x values. We show that the lines originate from acoustic phonons that become optically active by folding of the Brillouin zone. At even lower temperatures, a strongly asymmetric extra absorption band develops at frequencies around 20 cm−1 – 30 cm−1 corresponding to the position of the lowest-energy van Hove singularity in the reduced Brillouin zone. The band is assigned to the Boson Peak, i.e. to the excess of lattice vibrational states over the standard Debye contribution. The folded phonons and the boson peak do not show up for incommensurate calcium.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics: Conference Series\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"Boris\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"Elena\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"Victor\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kadyrov\"],\"firstnames\":[\"Lenar\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Motovilova\"],\"firstnames\":[\"Elizaveta\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fischgrabe\"],\"firstnames\":[\"Florian\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Moshnyaga\"],\"firstnames\":[\"Vasiliy\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhang\"],\"firstnames\":[\"Tao\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kremer\"],\"firstnames\":[\"Reinhard\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pracht\"],\"firstnames\":[\"Uwe\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zapf\"],\"firstnames\":[\"Sina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"Martin\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2014\",\"pages\":\"012001\",\"file\":\"IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\MKBKK4JA\\\\\\\\Gorshunov и др. - 2014 - Boson peak in manganites.pdf:application/pdf\",\"bibtex\":\"@article{gorshunov_boson_2014,\\n\\ttitle = {Boson peak in manganites},\\n\\tvolume = {486},\\n\\tissn = {1742-6596},\\n\\turl = {https://dx.doi.org/10.1088/1742-6596/486/1/012001},\\n\\tdoi = {10.1088/1742-6596/486/1/012001},\\n\\tabstract = {After the phase transition occurs in manganites La1-xCaxMnO3 (x ≥ 0.5) into a dielectric phase with charge order, right below the corresponding temperature of TCO = 240 K a series of absorption lines appear in the terahertz spectral range, only in case of commensurate x values. We show that the lines originate from acoustic phonons that become optically active by folding of the Brillouin zone. At even lower temperatures, a strongly asymmetric extra absorption band develops at frequencies around 20 cm−1 – 30 cm−1 corresponding to the position of the lowest-energy van Hove singularity in the reduced Brillouin zone. The band is assigned to the Boson Peak, i.e. to the excess of lattice vibrational states over the standard Debye contribution. The folded phonons and the boson peak do not show up for incommensurate calcium.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics: Conference Series},\\n\\tauthor = {Gorshunov, Boris P. and Zhukova, Elena S. and Torgashev, Victor I. and Kadyrov, Lenar S. and Motovilova, Elizaveta A. and Fischgrabe, Florian and Moshnyaga, Vasiliy and Zhang, Tao and Kremer, Reinhard and Pracht, Uwe and Zapf, Sina and Dressel, Martin},\\n\\tmonth = mar,\\n\\tyear = {2014},\\n\\tpages = {012001},\\n\\tfile = {IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\MKBKK4JA\\\\\\\\Gorshunov и др. - 2014 - Boson peak in manganites.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Gorshunov, B. P.\",\"Zhukova, E. S.\",\"Torgashev, V. I.\",\"Kadyrov, L. S.\",\"Motovilova, E. A.\",\"Fischgrabe, F.\",\"Moshnyaga, V.\",\"Zhang, T.\",\"Kremer, R.\",\"Pracht, U.\",\"Zapf, S.\",\"Dressel, M.\"],\"key\":\"gorshunov_boson_2014\",\"id\":\"gorshunov_boson_2014\",\"bibbaseid\":\"gorshunov-zhukova-torgashev-kadyrov-motovilova-fischgrabe-moshnyaga-zhang-etal-bosonpeakinmanganites-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/1742-6596/486/1/012001\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Coupled Vibrations in Index-Identified Carbon Nanotubes\",\"volume\":\"1700\",\"issn\":\"0272-9172, 1946-4274\",\"url\":\"https://www.cambridge.org/core/journals/mrs-online-proceedings-library-archive/article/abs/coupled-vibrations-in-indexidentified-carbon-nanotubes/2DD3B289A28698521E4E64C11E70F0DB\",\"doi\":\"10.1557/opl.2014.574\",\"abstract\":\"Combining high resolution transmission electron spectroscopy, electron diffraction, and resonant Raman spectroscopy experiments on the same suspended (free-standing) individual carbon nanotubes is the ultimate approach to relate unambiguously the structure and the intrinsic phonon features of these nano-systems.By using this approach, the effect of coupling between nanotubes on the phonons is investigated in two model nano-systems: (i) a bundle of two non-identical SWNTs (inhomogeneous dimer), (ii) double-walled carbon nanotubes.\",\"language\":\"en\",\"urldate\":\"2023-11-11\",\"journal\":\"MRS Online Proceedings Library (OPL)\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Levshov\"],\"firstnames\":[\"Dmitry\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Michel\"],\"firstnames\":[\"Thierry\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Paillet\"],\"firstnames\":[\"Matthieu\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Than\"],\"firstnames\":[\"Xuan\",\"Tinh\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tran\"],\"firstnames\":[\"Huy\",\"Nam\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Arenal\"],\"firstnames\":[\"Raul\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rahmani\"],\"firstnames\":[\"Abdelali\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Boutahir\"],\"firstnames\":[\"Mourad\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zahab\"],\"firstnames\":[\"Ahmed-Azmi\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sauvajol\"],\"firstnames\":[\"Jean-Louis\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2014\",\"note\":\"Publisher: Cambridge University Press\",\"keywords\":\"C, nanoscale, Raman spectroscopy\",\"pages\":\"69–77\",\"bibtex\":\"@article{levshov_coupled_2014,\\n\\ttitle = {Coupled {Vibrations} in {Index}-{Identified} {Carbon} {Nanotubes}},\\n\\tvolume = {1700},\\n\\tissn = {0272-9172, 1946-4274},\\n\\turl = {https://www.cambridge.org/core/journals/mrs-online-proceedings-library-archive/article/abs/coupled-vibrations-in-indexidentified-carbon-nanotubes/2DD3B289A28698521E4E64C11E70F0DB},\\n\\tdoi = {10.1557/opl.2014.574},\\n\\tabstract = {Combining high resolution transmission electron spectroscopy, electron diffraction, and resonant Raman spectroscopy experiments on the same suspended (free-standing) individual carbon nanotubes is the ultimate approach to relate unambiguously the structure and the intrinsic phonon features of these nano-systems.By using this approach, the effect of coupling between nanotubes on the phonons is investigated in two model nano-systems: (i) a bundle of two non-identical SWNTs (inhomogeneous dimer), (ii) double-walled carbon nanotubes.},\\n\\tlanguage = {en},\\n\\turldate = {2023-11-11},\\n\\tjournal = {MRS Online Proceedings Library (OPL)},\\n\\tauthor = {Levshov, Dmitry and Michel, Thierry and Paillet, Matthieu and Than, Xuan Tinh and Tran, Huy Nam and Arenal, Raul and Rahmani, Abdelali and Boutahir, Mourad and Zahab, Ahmed-Azmi and Sauvajol, Jean-Louis},\\n\\tmonth = jan,\\n\\tyear = {2014},\\n\\tnote = {Publisher: Cambridge University Press},\\n\\tkeywords = {C, nanoscale, Raman spectroscopy},\\n\\tpages = {69--77},\\n}\\n\\n\",\"author_short\":[\"Levshov, D.\",\"Michel, T.\",\"Paillet, M.\",\"Than, X. T.\",\"Tran, H. N.\",\"Arenal, R.\",\"Rahmani, A.\",\"Boutahir, M.\",\"Zahab, A.\",\"Sauvajol, J.\"],\"key\":\"levshov_coupled_2014\",\"id\":\"levshov_coupled_2014\",\"bibbaseid\":\"levshov-michel-paillet-than-tran-arenal-rahmani-boutahir-etal-coupledvibrationsinindexidentifiedcarbonnanotubes-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.cambridge.org/core/journals/mrs-online-proceedings-library-archive/article/abs/coupled-vibrations-in-indexidentified-carbon-nanotubes/2DD3B289A28698521E4E64C11E70F0DB\"},\"keyword\":[\"C\",\"nanoscale\",\"Raman spectroscopy\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Two-dimensional elasticity determines the low-frequency dynamics of single- and double-walled carbon nanotubes\",\"volume\":\"88\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.88.235435\",\"doi\":\"10.1103/PhysRevB.88.235435\",\"abstract\":\"We develop a continuous theory of low-frequency dynamics for nanotubes with walls constituted by single-atom monolayer, the topological elasticity of which is not related to its vanishing macroscopic thickness. The applicability region of the theory proposed includes all truly two-dimensional materials such as graphene and MoS2. New comprehensive interpretation and analytical expressions for low-frequency modes in single-walled carbon nanotube (SWCNT) are given. The theory unambiguously relates the radial breathing modes of SWCNT and breathinglike modes of the double-walled carbon nanotube (DWCNT). The existing Raman data on DWCNTs are fitted better than in the frame of previous models.\",\"number\":\"23\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorman\"],\"firstnames\":[\"V.\",\"L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2013\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"235435\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\IBZ3DB87\\\\\\\\Rochal и др. - 2013 - Two-dimensional elasticity determines the low-freq.pdf:application/pdf\",\"bibtex\":\"@article{rochal_two-dimensional_2013,\\n\\ttitle = {Two-dimensional elasticity determines the low-frequency dynamics of single- and double-walled carbon nanotubes},\\n\\tvolume = {88},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.88.235435},\\n\\tdoi = {10.1103/PhysRevB.88.235435},\\n\\tabstract = {We develop a continuous theory of low-frequency dynamics for nanotubes with walls constituted by single-atom monolayer, the topological elasticity of which is not related to its vanishing macroscopic thickness. The applicability region of the theory proposed includes all truly two-dimensional materials such as graphene and MoS2. New comprehensive interpretation and analytical expressions for low-frequency modes in single-walled carbon nanotube (SWCNT) are given. The theory unambiguously relates the radial breathing modes of SWCNT and breathinglike modes of the double-walled carbon nanotube (DWCNT). The existing Raman data on DWCNTs are fitted better than in the frame of previous models.},\\n\\tnumber = {23},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Rochal, S. B. and Lorman, V. L. and Yuzyuk, Yu. I.},\\n\\tmonth = dec,\\n\\tyear = {2013},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {235435},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\IBZ3DB87\\\\\\\\Rochal и др. - 2013 - Two-dimensional elasticity determines the low-freq.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Rochal, S. B.\",\"Lorman, V. L.\",\"Yuzyuk, Y. I.\"],\"key\":\"rochal_two-dimensional_2013\",\"id\":\"rochal_two-dimensional_2013\",\"bibbaseid\":\"rochal-lorman-yuzyuk-twodimensionalelasticitydeterminesthelowfrequencydynamicsofsingleanddoublewalledcarbonnanotubes-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.88.235435\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Electrochemical dispergation as a simple and effective technique toward preparation of NiO based nanocomposite for supercapacitor application\",\"volume\":\"114\",\"issn\":\"0013-4686\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0013468613019725\",\"doi\":\"10.1016/j.electacta.2013.10.031\",\"abstract\":\"NiO/C nanocomposite was prepared directly by means a one-step electrochemical technique based on electrochemical dispergation of nickel by the alternating current. The prepared material was well characterized using different analytical techniques such as X-ray diffraction, Raman spectroscopy, scanning electron microscopy, and N2 adsorption/desorption. The X-ray diffraction and Raman scattering investigations of the freshly prepared sample confirmed the formation of β-NiO. The morphology of synthesized NiO/C can be described as dispersed on carbon support nano-leaves consisting of tightly packed array of nanoparticles (around 10nm in diam) with length of 500–2000nm and ∼20nm thick. NiO/C composite possesses high specific surface area of 137m2g−1 and a micro–meso–macroporous structure with a distribution of the pore size from 1 to 200nm. The electrochemical properties of the nanostructured NiO/C were investigated using cyclic voltammetry (CV) and galvanostatic charge-discharge tests. The synthesized NiO/C composite exhibited pseudo-capacitive behavior with the mass capacitance value as high as 1012Fg−1 and 750Fg−1 measured from CV and discharge curves, respectively. Compared with the theoretical specific capacitance of NiO 2573Fg−1, the degree of electrochemical utilization is 97% for NiO in the synthesized NiO/C composite. The superior electrochemical performance is attributed to the hierarchically porous structure of the synthesized NiO/C, its with a high specific surface area as well as a wide pore size distribution. Considering the excellent performance and facile preparation, this NiO/C composite should have great potential for application in energy storage and conversion devices.\",\"urldate\":\"2023-11-11\",\"journal\":\"Electrochimica Acta\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Leontyeva\"],\"firstnames\":[\"D.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Avramenko\"],\"firstnames\":[\"M.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kukushkina\"],\"firstnames\":[\"Yu.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"N.\",\"V.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2013\",\"keywords\":\"Electrochemical capacitors, Nanoplatelets, Nanostructured materials, Nickel oxide\",\"pages\":\"356–362\",\"bibtex\":\"@article{leontyeva_electrochemical_2013,\\n\\ttitle = {Electrochemical dispergation as a simple and effective technique toward preparation of {NiO} based nanocomposite for supercapacitor application},\\n\\tvolume = {114},\\n\\tissn = {0013-4686},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0013468613019725},\\n\\tdoi = {10.1016/j.electacta.2013.10.031},\\n\\tabstract = {NiO/C nanocomposite was prepared directly by means a one-step electrochemical technique based on electrochemical dispergation of nickel by the alternating current. The prepared material was well characterized using different analytical techniques such as X-ray diffraction, Raman spectroscopy, scanning electron microscopy, and N2 adsorption/desorption. The X-ray diffraction and Raman scattering investigations of the freshly prepared sample confirmed the formation of β-NiO. The morphology of synthesized NiO/C can be described as dispersed on carbon support nano-leaves consisting of tightly packed array of nanoparticles (around 10nm in diam) with length of 500–2000nm and ∼20nm thick. NiO/C composite possesses high specific surface area of 137m2g−1 and a micro–meso–macroporous structure with a distribution of the pore size from 1 to 200nm. The electrochemical properties of the nanostructured NiO/C were investigated using cyclic voltammetry (CV) and galvanostatic charge-discharge tests. The synthesized NiO/C composite exhibited pseudo-capacitive behavior with the mass capacitance value as high as 1012Fg−1 and 750Fg−1 measured from CV and discharge curves, respectively. Compared with the theoretical specific capacitance of NiO 2573Fg−1, the degree of electrochemical utilization is 97\\\\% for NiO in the synthesized NiO/C composite. The superior electrochemical performance is attributed to the hierarchically porous structure of the synthesized NiO/C, its with a high specific surface area as well as a wide pore size distribution. Considering the excellent performance and facile preparation, this NiO/C composite should have great potential for application in energy storage and conversion devices.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Electrochimica Acta},\\n\\tauthor = {Leontyeva, D. V. and Leontyev, I. N. and Avramenko, M. V. and Yuzyuk, Yu. I. and Kukushkina, Yu. A. and Smirnova, N. V.},\\n\\tmonth = dec,\\n\\tyear = {2013},\\n\\tkeywords = {Electrochemical capacitors, Nanoplatelets, Nanostructured materials, Nickel oxide},\\n\\tpages = {356--362},\\n}\\n\\n\",\"author_short\":[\"Leontyeva, D. V.\",\"Leontyev, I. N.\",\"Avramenko, M. V.\",\"Yuzyuk, Y. I.\",\"Kukushkina, Y. A.\",\"Smirnova, N. V.\"],\"key\":\"leontyeva_electrochemical_2013\",\"id\":\"leontyeva_electrochemical_2013\",\"bibbaseid\":\"leontyeva-leontyev-avramenko-yuzyuk-kukushkina-smirnova-electrochemicaldispergationasasimpleandeffectivetechniquetowardpreparationofniobasednanocompositeforsupercapacitorapplication-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0013468613019725\"},\"keyword\":[\"Electrochemical capacitors\",\"Nanoplatelets\",\"Nanostructured materials\",\"Nickel oxide\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"УФ фотоприемник на основе наностержней и пленок оксида цинка\",\"url\":\"http://www.ivdon.ru/magazine/archive/n4y2013/1883\",\"abstract\":\"Сетевой научный журнал «Инженерный вестник Дона»\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Жилин\"],\"firstnames\":[\"Д.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2013\",\"bibtex\":\"@article{__2013,\\n\\ttitle = {{УФ} фотоприемник на основе наностержней и пленок оксида цинка},\\n\\turl = {http://www.ivdon.ru/magazine/archive/n4y2013/1883},\\n\\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Жилин, Д. А. and Лянгузов, Н. В. and Кайдашев, Е. М.},\\n\\tmonth = aug,\\n\\tyear = {2013},\\n}\\n\\n\",\"author_short\":[\"Жилин, Д. А.\",\"Лянгузов, Н. В.\",\"Кайдашев, Е. М.\"],\"key\":\"__2013\",\"id\":\"__2013\",\"bibbaseid\":\"----2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://www.ivdon.ru/magazine/archive/n4y2013/1883\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":3,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Импульсное лазерное напыление наноструктур\",\"url\":\"http://www.ivdon.ru/magazine/archive/n4y2013/1885\",\"abstract\":\"Сетевой научный журнал «Инженерный вестник Дона»\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Несветаев\"],\"firstnames\":[\"Д.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Пузиков\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2013\",\"bibtex\":\"@article{__2013-1,\\n\\ttitle = {Импульсное лазерное напыление наноструктур},\\n\\turl = {http://www.ivdon.ru/magazine/archive/n4y2013/1885},\\n\\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Несветаев, Д. Г. and Кайдашев, Е. М. and Пузиков, А. С.},\\n\\tmonth = aug,\\n\\tyear = {2013},\\n}\\n\\n\",\"author_short\":[\"Несветаев, Д. Г.\",\"Кайдашев, Е. М.\",\"Пузиков, А. С.\"],\"key\":\"__2013-1\",\"id\":\"__2013-1\",\"bibbaseid\":\"----2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://www.ivdon.ru/magazine/archive/n4y2013/1885\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":3,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Unconventional Landau theory of quasicrystalline structure formation\",\"volume\":\"377\",\"issn\":\"0375-9601\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0375960113002417\",\"doi\":\"10.1016/j.physleta.2013.03.006\",\"abstract\":\"We propose an unconventional theory which unifies the description of quasicrystal thermodynamics and quasicrystal structure formation by combining the Landau theory of crystallization and the cluster approach to quasicrystals. The theory is illustrated on the example of pentagonal Penrose quasilattice. It employs the notion of non-linear order parameter dependent on the atomic coordinates which was developed in the theory of reconstructive phase transitions. The coordinates of the quasilattice nodes are calculated by minimizing the Landau free energy with the constraint imposed by internal organization of clusters. The correspondence is shown between the theory proposed and the conventional projection method.\",\"number\":\"16\",\"urldate\":\"2023-11-11\",\"journal\":\"Physics Letters A\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Konevtsova\"],\"firstnames\":[\"O.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorman\"],\"firstnames\":[\"V.\",\"L.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2013\",\"keywords\":\"Cluster approach, Constrained minimization, Landau crystallization theory, Non-linear order parameter, Quasicrystal\",\"pages\":\"1215–1220\",\"bibtex\":\"@article{konevtsova_unconventional_2013,\\n\\ttitle = {Unconventional {Landau} theory of quasicrystalline structure formation},\\n\\tvolume = {377},\\n\\tissn = {0375-9601},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0375960113002417},\\n\\tdoi = {10.1016/j.physleta.2013.03.006},\\n\\tabstract = {We propose an unconventional theory which unifies the description of quasicrystal thermodynamics and quasicrystal structure formation by combining the Landau theory of crystallization and the cluster approach to quasicrystals. The theory is illustrated on the example of pentagonal Penrose quasilattice. It employs the notion of non-linear order parameter dependent on the atomic coordinates which was developed in the theory of reconstructive phase transitions. The coordinates of the quasilattice nodes are calculated by minimizing the Landau free energy with the constraint imposed by internal organization of clusters. The correspondence is shown between the theory proposed and the conventional projection method.},\\n\\tnumber = {16},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physics Letters A},\\n\\tauthor = {Konevtsova, O. V. and Rochal, S. B. and Lorman, V. L.},\\n\\tmonth = jul,\\n\\tyear = {2013},\\n\\tkeywords = {Cluster approach, Constrained minimization, Landau crystallization theory, Non-linear order parameter, Quasicrystal},\\n\\tpages = {1215--1220},\\n}\\n\\n\",\"author_short\":[\"Konevtsova, O. V.\",\"Rochal, S. B.\",\"Lorman, V. L.\"],\"key\":\"konevtsova_unconventional_2013\",\"id\":\"konevtsova_unconventional_2013\",\"bibbaseid\":\"konevtsova-rochal-lorman-unconventionallandautheoryofquasicrystallinestructureformation-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0375960113002417\"},\"keyword\":[\"Cluster approach\",\"Constrained minimization\",\"Landau crystallization theory\",\"Non-linear order parameter\",\"Quasicrystal\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Quantum Behavior of Water Molecules Confined to Nanocavities in Gemstones\",\"volume\":\"4\",\"url\":\"https://doi.org/10.1021/jz400782j\",\"doi\":\"10.1021/jz400782j\",\"abstract\":\"When water is confined to nanocavities, its quantum mechanical behavior can be revealed by terahertz spectroscopy. We place H2O molecules in the nanopores of a beryl crystal lattice and observe a rich and highly anisotropic set of absorption lines in the terahertz spectral range. Two bands can be identified, which originate from translational and librational motions of the water molecule isolated within the cage; they correspond to the analogous broad bands in liquid water and ice. In the present case of well-defined and highly symmetric nanocavities, the observed fine structure can be explained by macroscopic tunneling of the H2O molecules within a six-fold potential caused by the interaction of the molecule with the cavity walls.\",\"number\":\"12\",\"urldate\":\"2023-11-11\",\"journal\":\"The Journal of Physical Chemistry Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"Boris\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"Elena\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"Victor\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lebedev\"],\"firstnames\":[\"Vladimir\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shakurov\"],\"firstnames\":[\"Gil’man\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kremer\"],\"firstnames\":[\"Reinhard\",\"K.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pestrjakov\"],\"firstnames\":[\"Efim\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Thomas\"],\"firstnames\":[\"Victor\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fursenko\"],\"firstnames\":[\"Dimitry\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"Martin\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2013\",\"note\":\"Publisher: American Chemical Society\",\"pages\":\"2015–2020\",\"bibtex\":\"@article{gorshunov_quantum_2013,\\n\\ttitle = {Quantum {Behavior} of {Water} {Molecules} {Confined} to {Nanocavities} in {Gemstones}},\\n\\tvolume = {4},\\n\\turl = {https://doi.org/10.1021/jz400782j},\\n\\tdoi = {10.1021/jz400782j},\\n\\tabstract = {When water is confined to nanocavities, its quantum mechanical behavior can be revealed by terahertz spectroscopy. We place H2O molecules in the nanopores of a beryl crystal lattice and observe a rich and highly anisotropic set of absorption lines in the terahertz spectral range. Two bands can be identified, which originate from translational and librational motions of the water molecule isolated within the cage; they correspond to the analogous broad bands in liquid water and ice. In the present case of well-defined and highly symmetric nanocavities, the observed fine structure can be explained by macroscopic tunneling of the H2O molecules within a six-fold potential caused by the interaction of the molecule with the cavity walls.},\\n\\tnumber = {12},\\n\\turldate = {2023-11-11},\\n\\tjournal = {The Journal of Physical Chemistry Letters},\\n\\tauthor = {Gorshunov, Boris P. and Zhukova, Elena S. and Torgashev, Victor I. and Lebedev, Vladimir V. and Shakurov, Gil’man S. and Kremer, Reinhard K. and Pestrjakov, Efim V. and Thomas, Victor G. and Fursenko, Dimitry A. and Dressel, Martin},\\n\\tmonth = jun,\\n\\tyear = {2013},\\n\\tnote = {Publisher: American Chemical Society},\\n\\tpages = {2015--2020},\\n}\\n\\n\",\"author_short\":[\"Gorshunov, B. P.\",\"Zhukova, E. S.\",\"Torgashev, V. I.\",\"Lebedev, V. V.\",\"Shakurov, G. S.\",\"Kremer, R. K.\",\"Pestrjakov, E. V.\",\"Thomas, V. G.\",\"Fursenko, D. A.\",\"Dressel, M.\"],\"key\":\"gorshunov_quantum_2013\",\"id\":\"gorshunov_quantum_2013\",\"bibbaseid\":\"gorshunov-zhukova-torgashev-lebedev-shakurov-kremer-pestrjakov-thomas-etal-quantumbehaviorofwatermoleculesconfinedtonanocavitiesingemstones-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1021/jz400782j\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Электронные методы структурного анализа индивидуальных углеродных нанотрубок\",\"url\":\"http://www.ivdon.ru/magazine/archive/n4y2013/2006\",\"abstract\":\"Сетевой научный журнал «Инженерный вестник Дона»\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Левшов\"],\"firstnames\":[\"Д.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Авраменко\"],\"firstnames\":[\"М.\",\"В.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2013\",\"bibtex\":\"@article{__2013-2,\\n\\ttitle = {Электронные методы структурного анализа индивидуальных углеродных нанотрубок},\\n\\turl = {http://www.ivdon.ru/magazine/archive/n4y2013/2006},\\n\\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Левшов, Д. И. and Авраменко, М. В.},\\n\\tmonth = jun,\\n\\tyear = {2013},\\n}\\n\\n\",\"author_short\":[\"Левшов, Д. И.\",\"Авраменко, М. В.\"],\"key\":\"__2013-2\",\"id\":\"__2013-2\",\"bibbaseid\":\"---2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://www.ivdon.ru/magazine/archive/n4y2013/2006\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Топологические дефекты в двумерных сферических кристаллах\",\"url\":\"http://www.ivdon.ru/magazine/archive/n3y2013/1844\",\"abstract\":\"Сетевой научный журнал «Инженерный вестник Дона»\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Петров\"],\"firstnames\":[\"К.\",\"Ю.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Шевченко\"],\"firstnames\":[\"И.\",\"А.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2013\",\"bibtex\":\"@article{__2013-3,\\n\\ttitle = {Топологические дефекты в двумерных сферических кристаллах},\\n\\turl = {http://www.ivdon.ru/magazine/archive/n3y2013/1844},\\n\\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Петров, К. Ю. and Шевченко, И. А.},\\n\\tmonth = apr,\\n\\tyear = {2013},\\n}\\n\\n\",\"author_short\":[\"Петров, К. Ю.\",\"Шевченко, И. А.\"],\"key\":\"__2013-3\",\"id\":\"__2013-3\",\"bibbaseid\":\"---2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://www.ivdon.ru/magazine/archive/n3y2013/1844\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Symmetry of the carbon nanotube modes and their origin from the phonon branches of graphene\",\"volume\":\"87\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.87.035407\",\"doi\":\"10.1103/PhysRevB.87.035407\",\"abstract\":\"A group-theory method to relate the spectra of tubular and parent planar structures is elaborated. The spectra correlation is obtained using a virtual intermediate planar periodic structure, which has a local symmetry coinciding with that of the tube surface. The method is applied to deduce the zone-center phonon modes of carbon nanotubes from the dispersion branches of the graphene monolayer. The results obtained open an additional way for experimental indexing of the carbon nanotubes by means of Raman spectroscopy, and the origin of the Raman-active modes in the achiral nanotubes is determined. We demonstrate that the number of modes in the G band and the relation between their frequencies are governed by the nanotube type. The proposed theory can be easily explored to understand the phonon and electron spectra of many other tubular structures (boron nitride, transition metal dichalcogenides) which have emerged in the past decade.\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Avramenko\"],\"firstnames\":[\"M.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2013\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"035407\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\§37AE8AD\\\\\\\\Avramenko и др. - 2013 - Symmetry of the carbon nanotube modes and their or.pdf:application/pdf\",\"bibtex\":\"@article{avramenko_symmetry_2013,\\n\\ttitle = {Symmetry of the carbon nanotube modes and their origin from the phonon branches of graphene},\\n\\tvolume = {87},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.87.035407},\\n\\tdoi = {10.1103/PhysRevB.87.035407},\\n\\tabstract = {A group-theory method to relate the spectra of tubular and parent planar structures is elaborated. The spectra correlation is obtained using a virtual intermediate planar periodic structure, which has a local symmetry coinciding with that of the tube surface. The method is applied to deduce the zone-center phonon modes of carbon nanotubes from the dispersion branches of the graphene monolayer. The results obtained open an additional way for experimental indexing of the carbon nanotubes by means of Raman spectroscopy, and the origin of the Raman-active modes in the achiral nanotubes is determined. We demonstrate that the number of modes in the G band and the relation between their frequencies are governed by the nanotube type. The proposed theory can be easily explored to understand the phonon and electron spectra of many other tubular structures (boron nitride, transition metal dichalcogenides) which have emerged in the past decade.},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Avramenko, M. V. and Rochal, S. B. and Yuzyuk, Yu. I.},\\n\\tmonth = jan,\\n\\tyear = {2013},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {035407},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\S37AE8AD\\\\\\\\Avramenko и др. - 2013 - Symmetry of the carbon nanotube modes and their or.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Avramenko, M. V.\",\"Rochal, S. B.\",\"Yuzyuk, Y. I.\"],\"key\":\"avramenko_symmetry_2013\",\"id\":\"avramenko_symmetry_2013\",\"bibbaseid\":\"avramenko-rochal-yuzyuk-symmetryofthecarbonnanotubemodesandtheiroriginfromthephononbranchesofgraphene-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.87.035407\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Resistive Switching Hysteresis in Thin Films of Bismuth Ferrite\",\"volume\":\"444\",\"issn\":\"0015-0193\",\"url\":\"https://doi.org/10.1080/00150193.2013.790759\",\"doi\":\"10.1080/00150193.2013.790759\",\"abstract\":\"We have studied the resistive switching (RS) phenomenon in series of BiFeO3 thin films of thickness of 40 – 154 nm deposited by PLD technique on conducting Nb-doped substrate of SrTiO3 and with Pt top electrodes. It was found that 154 nm film demonstrates the interface-provided I–V characteristic of Schottky diode when the applied voltage does not exceed the threshold value Vd = 1.3 V. The RS phenomenon appears as the current hysteresis loop during the 0 → Vm → 0 → −Vm → 0 voltage sweep cycle, provided that the maximal stop-voltage Vm is larger than Vd. For thinner films neither diode-like I–V behavior nor substantial RS effect were observed. The results are interpreted in terms of the filamentary model of the mobile oxygen vacancies.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gagou\"],\"firstnames\":[\"Y.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bouyanfif\"],\"firstnames\":[\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Carcan\"],\"firstnames\":[\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Allouche\"],\"firstnames\":[\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Wolfman\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Autret-Lambert\"],\"firstnames\":[\"C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Marssi\"],\"firstnames\":[\"M.\",\"El\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzane\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Luk'yanchuk\"],\"firstnames\":[\"I.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2013\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2013.790759\",\"keywords\":\"multiferroics, oxides, Resistive switching, thin films\",\"pages\":\"183–189\",\"bibtex\":\"@article{razumnaya_resistive_2013,\\n\\ttitle = {Resistive {Switching} {Hysteresis} in {Thin} {Films} of {Bismuth} {Ferrite}},\\n\\tvolume = {444},\\n\\tissn = {0015-0193},\\n\\turl = {https://doi.org/10.1080/00150193.2013.790759},\\n\\tdoi = {10.1080/00150193.2013.790759},\\n\\tabstract = {We have studied the resistive switching (RS) phenomenon in series of BiFeO3 thin films of thickness of 40 – 154 nm deposited by PLD technique on conducting Nb-doped substrate of SrTiO3 and with Pt top electrodes. It was found that 154 nm film demonstrates the interface-provided I–V characteristic of Schottky diode when the applied voltage does not exceed the threshold value Vd = 1.3 V. The RS phenomenon appears as the current hysteresis loop during the 0 → Vm → 0 → −Vm → 0 voltage sweep cycle, provided that the maximal stop-voltage Vm is larger than Vd. For thinner films neither diode-like I–V behavior nor substantial RS effect were observed. The results are interpreted in terms of the filamentary model of the mobile oxygen vacancies.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Razumnaya, A. and Gagou, Y. and Bouyanfif, H. and Carcan, B. and Allouche, B. and Wolfman, J. and Autret-Lambert, C. and Marssi, M. El and Mezzane, D. and Luk'yanchuk, I.},\\n\\tmonth = jan,\\n\\tyear = {2013},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/00150193.2013.790759},\\n\\tkeywords = {multiferroics, oxides, Resistive switching, thin films},\\n\\tpages = {183--189},\\n}\\n\\n\",\"author_short\":[\"Razumnaya, A.\",\"Gagou, Y.\",\"Bouyanfif, H.\",\"Carcan, B.\",\"Allouche, B.\",\"Wolfman, J.\",\"Autret-Lambert, C.\",\"Marssi, M. E.\",\"Mezzane, D.\",\"Luk'yanchuk, I.\"],\"key\":\"razumnaya_resistive_2013\",\"id\":\"razumnaya_resistive_2013\",\"bibbaseid\":\"razumnaya-gagou-bouyanfif-carcan-allouche-wolfman-autretlambert-marssi-etal-resistiveswitchinghysteresisinthinfilmsofbismuthferrite-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/00150193.2013.790759\"},\"keyword\":[\"multiferroics\",\"oxides\",\"Resistive switching\",\"thin films\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Phase States in Multicomponent PZT-Based Materials Depending on Poling Conditions\",\"volume\":\"443\",\"issn\":\"0015-0193\",\"url\":\"https://doi.org/10.1080/00150193.2013.778616\",\"doi\":\"10.1080/00150193.2013.778616\",\"abstract\":\"Phase states of the PZT-based multicomponent solid solutions belonging to the rhombohedral area of the phase х-Т diagram with low coercive field values are considered. The solid-solution samples in the initial state are proved to be heterophase (R3c and P4mm mixtures) and reveal relaxor properties. The anomalies of dielectric characteristics obtained in poled samples are due to the R3c→R3m phase transition. The manifestations of relaxor properties above the temperature of the dielectric permittivity maximum are caused by the R3m phase in the P4mm and Pm3m phase mixture.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Akbaeva\"],\"firstnames\":[\"G.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kabirov\"],\"firstnames\":[\"Yu.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Milov\"],\"firstnames\":[\"E.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gavrilyachenko\"],\"firstnames\":[\"V.\",\"G.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2013\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2013.778616\",\"keywords\":\"phase transition, X-ray diffraction, Phase state, poling condition\",\"pages\":\"57–62\",\"bibtex\":\"@article{akbaeva_phase_2013,\\n\\ttitle = {Phase {States} in {Multicomponent} {PZT}-{Based} {Materials} {Depending} on {Poling} {Conditions}},\\n\\tvolume = {443},\\n\\tissn = {0015-0193},\\n\\turl = {https://doi.org/10.1080/00150193.2013.778616},\\n\\tdoi = {10.1080/00150193.2013.778616},\\n\\tabstract = {Phase states of the PZT-based multicomponent solid solutions belonging to the rhombohedral area of the phase х-Т diagram with low coercive field values are considered. The solid-solution samples in the initial state are proved to be heterophase (R3c and P4mm mixtures) and reveal relaxor properties. The anomalies of dielectric characteristics obtained in poled samples are due to the R3c→R3m phase transition. The manifestations of relaxor properties above the temperature of the dielectric permittivity maximum are caused by the R3m phase in the P4mm and Pm3m phase mixture.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Akbaeva, G. M. and Kabirov, Yu. V. and Milov, E. V. and Gavrilyachenko, V. G.},\\n\\tmonth = jan,\\n\\tyear = {2013},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/00150193.2013.778616},\\n\\tkeywords = {phase transition, X-ray diffraction, Phase state, poling condition},\\n\\tpages = {57--62},\\n}\\n\\n\",\"author_short\":[\"Akbaeva, G. M.\",\"Kabirov, Y. V.\",\"Milov, E. V.\",\"Gavrilyachenko, V. G.\"],\"key\":\"akbaeva_phase_2013\",\"id\":\"akbaeva_phase_2013\",\"bibbaseid\":\"akbaeva-kabirov-milov-gavrilyachenko-phasestatesinmulticomponentpztbasedmaterialsdependingonpolingconditions-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/00150193.2013.778616\"},\"keyword\":[\"phase transition\",\"X-ray diffraction\",\"Phase state\",\"poling condition\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Comparative Raman Study of Individual Double-Walled Carbon Nanotubes and Single-Walled Carbon Nanotubes\",\"volume\":\"8\",\"doi\":\"10.1166/jno.2013.1423\",\"abstract\":\"In this paper, we compare the Raman responses obtained on individual suspended Single-Walled Carbon Nanotubes (SWNTs) and Double-Walled Carbon Nanotubes (DWNTs). We focus on the comparison of the frequencies, line widths, intensities and resonance conditions of the main Raman active modes measured on an index-identified DWNT with those measured on SWNTs having atomic structures close to the inner and outer tubes of the DWNT. By this way, we state that the relation between the radial breathing mode frequencies and the diameters established for SWNTs do not work in DWNTs. We found that resonance of only one tube can be sufficient to observe the response of the coupled layers in DWNTs. These results are understood in terms of mechanical coupling between the layers in DWNTs. We evidence that the spectral line widths of the Raman active modes are systematically narrower for DWNTs compared to the corresponding SWNTs. Finally, we present the measurements of the G modes of two different DWNTs which behave in a different way. For the first one, the frequencies of the G modes are not significantly affected by the interaction between the layers, while for the second one we evidence a downward shift of the LO and TO bands arising from the inner layer.\",\"number\":\"1\",\"journal\":\"Journal of Nanoelectronics and Optoelectronics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Levshov\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Michel\"],\"firstnames\":[\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Than\"],\"firstnames\":[\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Paillet\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Arenal\"],\"firstnames\":[\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Jourdain\"],\"firstnames\":[\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sauvajol\"],\"firstnames\":[\"J.-L.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2013\",\"keywords\":\"ELECTRON DIFFRACTION, INDIVIDUAL DOUBLE-WALLED CARBON NANOTUBES, INDIVIDUAL SINGLE-WALLED CARBON NANOTUBES, RAMAN SPECTROSCOPY\",\"pages\":\"9–15\",\"bibtex\":\"@article{levshov_comparative_2013,\\n\\ttitle = {Comparative {Raman} {Study} of {Individual} {Double}-{Walled} {Carbon} {Nanotubes} and {Single}-{Walled} {Carbon} {Nanotubes}},\\n\\tvolume = {8},\\n\\tdoi = {10.1166/jno.2013.1423},\\n\\tabstract = {In this paper, we compare the Raman responses obtained on individual suspended Single-Walled Carbon Nanotubes (SWNTs) and Double-Walled Carbon Nanotubes (DWNTs). We focus on the comparison of the frequencies, line widths, intensities and resonance conditions of the main Raman active\\nmodes measured on an index-identified DWNT with those measured on SWNTs having atomic structures close to the inner and outer tubes of the DWNT. By this way, we state that the relation between the radial breathing mode frequencies and the diameters established for SWNTs do not work in DWNTs.\\nWe found that resonance of only one tube can be sufficient to observe the response of the coupled layers in DWNTs. These results are understood in terms of mechanical coupling between the layers in DWNTs. We evidence that the spectral line widths of the Raman active modes are systematically\\nnarrower for DWNTs compared to the corresponding SWNTs. Finally, we present the measurements of the G modes of two different DWNTs which behave in a different way. For the first one, the frequencies of the G modes are not significantly affected by the interaction between the\\nlayers, while for the second one we evidence a downward shift of the LO and TO bands arising from the inner layer.},\\n\\tnumber = {1},\\n\\tjournal = {Journal of Nanoelectronics and Optoelectronics},\\n\\tauthor = {Levshov, D. and Michel, T. and Than, T. and Paillet, M. and Arenal, R. and Jourdain, V. and Yuzyuk, Yu. I. and Sauvajol, J.-L.},\\n\\tmonth = jan,\\n\\tyear = {2013},\\n\\tkeywords = {ELECTRON DIFFRACTION, INDIVIDUAL DOUBLE-WALLED CARBON NANOTUBES, INDIVIDUAL SINGLE-WALLED CARBON NANOTUBES, RAMAN SPECTROSCOPY},\\n\\tpages = {9--15},\\n}\\n\\n\",\"author_short\":[\"Levshov, D.\",\"Michel, T.\",\"Than, T.\",\"Paillet, M.\",\"Arenal, R.\",\"Jourdain, V.\",\"Yuzyuk, Y. I.\",\"Sauvajol, J.\"],\"key\":\"levshov_comparative_2013\",\"id\":\"levshov_comparative_2013\",\"bibbaseid\":\"levshov-michel-than-paillet-arenal-jourdain-yuzyuk-sauvajol-comparativeramanstudyofindividualdoublewalledcarbonnanotubesandsinglewalledcarbonnanotubes-2013\",\"role\":\"author\",\"urls\":{},\"keyword\":[\"ELECTRON DIFFRACTION\",\"INDIVIDUAL DOUBLE-WALLED CARBON NANOTUBES\",\"INDIVIDUAL SINGLE-WALLED CARBON NANOTUBES\",\"RAMAN SPECTROSCOPY\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"Структурные и электрокаталитические свойства катализаторов Pt/C и Pt–Ni/C, полученных методом электрохимического диспергирования\",\"volume\":\"54\",\"url\":\"http://www.maikonline.com/maik/showArticle.do?auid=VAHEB686WM&lang=ru\",\"doi\":\"10.7868/S0453881113020147\",\"abstract\":\"Semantic Scholar extracted view of \\\"Структурные и электрокаталитические свойства катализаторов Pt/C и Pt–Ni/C, полученных методом электрохимического диспергирования\\\" by Наталья Владимировна Смирнова et al.\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"booktitle\":\"Кинетика и катализ\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Смирнова\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Куриганова\"],\"firstnames\":[\"А.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Леонтьева\"],\"firstnames\":[\"Д.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Леонтьев\"],\"firstnames\":[\"И.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Михейкин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]}],\"year\":\"2013\",\"note\":\"ISSN: 0453-8811 Issue: 2 Journal Abbreviation: Кинет. и катал.\",\"pages\":\"265–272\",\"bibtex\":\"@inproceedings{__2013-4,\\n\\ttitle = {Структурные и электрокаталитические свойства катализаторов {Pt}/{C} и {Pt}–{Ni}/{C}, полученных методом электрохимического диспергирования},\\n\\tvolume = {54},\\n\\turl = {http://www.maikonline.com/maik/showArticle.do?auid=VAHEB686WM&lang=ru},\\n\\tdoi = {10.7868/S0453881113020147},\\n\\tabstract = {Semantic Scholar extracted view of \\\"Структурные и электрокаталитические свойства катализаторов Pt/C и Pt–Ni/C, полученных методом электрохимического диспергирования\\\" by Наталья Владимировна Смирнова et al.},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tbooktitle = {Кинетика и катализ},\\n\\tauthor = {Смирнова, Н. В. and Куриганова, А. Б. and Леонтьева, Д. В. and Леонтьев, И. Н. and Михейкин, А. С.},\\n\\tyear = {2013},\\n\\tnote = {ISSN: 0453-8811\\nIssue: 2\\nJournal Abbreviation: Кинет. и катал.},\\n\\tpages = {265--272},\\n}\\n\\n\",\"author_short\":[\"Смирнова, Н. В.\",\"Куриганова, А. Б.\",\"Леонтьева, Д. В.\",\"Леонтьев, И. Н.\",\"Михейкин, А. С.\"],\"key\":\"__2013-4\",\"id\":\"__2013-4\",\"bibbaseid\":\"-----ptcptnic-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://www.maikonline.com/maik/showArticle.do?auid=VAHEB686WM&lang=ru\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Синтез и свойства метаматериалов со структурой оболочка-ядро\",\"issn\":\"2073-2562\",\"url\":\"https://elibrary.ru/item.asp?id=18944350\",\"abstract\":\"Синтезированы поликристаллические и керамические композитные материалы (КМ) Pt ( PbZrO 3 ) и CaCu 3 Ti 4 O 12 ( SrFe 12 O 19 ), архитектурно представляющие собой структуру оболочка—ядро. В первых из них обнаружен парамагнетизм, обусловленный появлением парамагнитных центров при взаимодействии атомов платины и матрицы. Композитная керамика на основе гексаферрита стронция SrFe 12 O 19, структурированная по типу оболочка—ядро материалом с колоссальным значением диэлектрической проницаемости CaCu 3 Ti 4 O 12, приготовлена с использованием традиционной керамической технологии. Приведены результаты электронно-микроскопических и электрофизических исследований объектов\",\"language\":\"ru\",\"number\":\"2 (130)\",\"urldate\":\"2023-11-11\",\"journal\":\"Конструкции Из Композиционных Материалов\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Кабиров\"],\"firstnames\":[\"Ю.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гавриляченко\"],\"firstnames\":[\"В.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гутерман\"],\"firstnames\":[\"В.\",\"Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Залетов\"],\"firstnames\":[\"В.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Сидоренко\"],\"firstnames\":[\"Е.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Панченко\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]}],\"year\":\"2013\",\"keywords\":\"Гексаферрит Стронция, Композиты, Метаматериалы\",\"pages\":\"37–42\",\"bibtex\":\"@article{__2013-5,\\n\\ttitle = {Синтез и свойства метаматериалов со структурой оболочка-ядро},\\n\\tissn = {2073-2562},\\n\\turl = {https://elibrary.ru/item.asp?id=18944350},\\n\\tabstract = {Синтезированы поликристаллические и керамические композитные материалы (КМ) Pt ( PbZrO 3 ) и CaCu 3 Ti 4 O 12 ( SrFe 12 O 19 ), архитектурно представляющие собой структуру оболочка—ядро. В первых из них обнаружен парамагнетизм, обусловленный появлением парамагнитных центров при взаимодействии атомов платины и матрицы. Композитная керамика на основе гексаферрита стронция SrFe 12 O 19, структурированная по типу оболочка—ядро материалом с колоссальным значением диэлектрической проницаемости CaCu 3 Ti 4 O 12, приготовлена с использованием традиционной керамической технологии. Приведены результаты электронно-микроскопических и электрофизических исследований объектов},\\n\\tlanguage = {ru},\\n\\tnumber = {2 (130)},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Конструкции Из Композиционных Материалов},\\n\\tauthor = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Гутерман, В. Е. and Залетов, В. Г. and Сидоренко, Е. Н. and Лянгузов, Н. В. and Панченко, Е. М.},\\n\\tyear = {2013},\\n\\tkeywords = {Гексаферрит Стронция, Композиты, Метаматериалы},\\n\\tpages = {37--42},\\n}\\n\\n\",\"author_short\":[\"Кабиров, Ю. В.\",\"Гавриляченко, В. Г.\",\"Гутерман, В. Е.\",\"Залетов, В. Г.\",\"Сидоренко, Е. Н.\",\"Лянгузов, Н. В.\",\"Панченко, Е. М.\"],\"key\":\"__2013-5\",\"id\":\"__2013-5\",\"bibbaseid\":\"--------2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=18944350\"},\"keyword\":[\"Гексаферрит Стронция\",\"Композиты\",\"Метаматериалы\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"The compressibility of nanocrystalline Pt\",\"volume\":\"101\",\"issn\":\"0003-6951\",\"url\":\"https://doi.org/10.1063/1.4758000\",\"doi\":\"10.1063/1.4758000\",\"abstract\":\"High-pressure behavior of carbon supported Pt nanoparticles (Pt/C) with an average particle size of 10.6 nm was investigated by in situ high-pressure synchrotron radiation x-ray diffraction up to 14 GPa at ambient temperature. Our results show that the compressibility of Pt/C nanoparticles decreases substantially as the particle size decreases. An interpretation based upon the available mechanisms of structural compliance in nanoscale vs bulk materials was proposed.\",\"number\":\"17\",\"urldate\":\"2023-11-11\",\"journal\":\"Applied Physics Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dmitriev\"],\"firstnames\":[\"V.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chagovets\"],\"firstnames\":[\"S.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"A.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"N.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2012\",\"pages\":\"173111\",\"bibtex\":\"@article{mikheykin_compressibility_2012,\\n\\ttitle = {The compressibility of nanocrystalline {Pt}},\\n\\tvolume = {101},\\n\\tissn = {0003-6951},\\n\\turl = {https://doi.org/10.1063/1.4758000},\\n\\tdoi = {10.1063/1.4758000},\\n\\tabstract = {High-pressure behavior of carbon supported Pt nanoparticles (Pt/C) with an average particle size of 10.6 nm was investigated by in situ high-pressure synchrotron radiation x-ray diffraction up to 14 GPa at ambient temperature. Our results show that the compressibility of Pt/C nanoparticles decreases substantially as the particle size decreases. An interpretation based upon the available mechanisms of structural compliance in nanoscale vs bulk materials was proposed.},\\n\\tnumber = {17},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Applied Physics Letters},\\n\\tauthor = {Mikheykin, A. S. and Dmitriev, V. P. and Chagovets, S. V. and Kuriganova, A. B. and Smirnova, N. V. and Leontyev, I. N.},\\n\\tmonth = oct,\\n\\tyear = {2012},\\n\\tpages = {173111},\\n}\\n\\n\",\"author_short\":[\"Mikheykin, A. S.\",\"Dmitriev, V. P.\",\"Chagovets, S. V.\",\"Kuriganova, A. B.\",\"Smirnova, N. V.\",\"Leontyev, I. N.\"],\"key\":\"mikheykin_compressibility_2012\",\"id\":\"mikheykin_compressibility_2012\",\"bibbaseid\":\"mikheykin-dmitriev-chagovets-kuriganova-smirnova-leontyev-thecompressibilityofnanocrystallinept-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.4758000\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Исследование наностержней оксида цинка методом фотолюминесценции для оптимизации характеристик чувствительного элемента ПАВ сенсора\",\"url\":\"http://ivdon.ru/magazine/archive/n4p1y2012/1178\",\"abstract\":\"Сетевой научный журнал «Инженерный вестник Дона»\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Несветаев\"],\"firstnames\":[\"Д.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Николаев\"],\"firstnames\":[\"А.\",\"Л.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2012\",\"bibtex\":\"@article{__2012,\\n\\ttitle = {Исследование наностержней оксида цинка методом фотолюминесценции для оптимизации характеристик чувствительного элемента ПАВ сенсора},\\n\\turl = {http://ivdon.ru/magazine/archive/n4p1y2012/1178},\\n\\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Несветаев, Д. Г. and Лянгузов, Н. В. and Николаев, А. Л. and Кайдашев, Е. М.},\\n\\tmonth = aug,\\n\\tyear = {2012},\\n}\\n\\n\",\"author_short\":[\"Несветаев, Д. Г.\",\"Лянгузов, Н. В.\",\"Николаев, А. Л.\",\"Кайдашев, Е. М.\"],\"key\":\"__2012\",\"id\":\"__2012\",\"bibbaseid\":\"-----2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://ivdon.ru/magazine/archive/n4p1y2012/1178\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"New life of a forgotten method: Electrochemical route toward highly efficient Pt/C catalysts for low-temperature fuel cells\",\"volume\":\"431-432\",\"issn\":\"0926-860X\",\"shorttitle\":\"New life of a forgotten method\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0926860X12002268\",\"doi\":\"10.1016/j.apcata.2012.04.025\",\"abstract\":\"Driven by global environmental concerns, great efforts are currently made to develop novel, cheap and practical means for producing highly efficient electrocatalysts, specifically for the low-temperature fuel-cell applications. Employing an old but yet unexplored method based on electrochemical dispergation of platinum by the alternating current, we show that the freshly prepared Pt/C catalysts exhibit greatly enhanced catalytic activity (up to 350% for oxygen reduction and up to 200% for ethylene glycol oxidation) as compared with that of a commercially available counterpart (E-TEK). A key role in these reactions is attributed to a specific nanoparticle morphology. These findings should provide a revival of an ancient but simple and efficient electrochemical process and motivate further researches in the field.\",\"urldate\":\"2023-11-11\",\"journal\":\"Applied Catalysis A: General\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"Aleksandra\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kudryavtsev\"],\"firstnames\":[\"Yuri\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dkhil\"],\"firstnames\":[\"Brahim\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2012\",\"keywords\":\"Electrocatalysis, Oxygen reduction reaction (ORR), X-ray diffraction (XRD), Low-temperature fuel cell, Platinum nanoparticles, Shape\",\"pages\":\"120–125\",\"bibtex\":\"@article{leontyev_new_2012,\\n\\ttitle = {New life of a forgotten method: {Electrochemical} route toward highly efficient {Pt}/{C} catalysts for low-temperature fuel cells},\\n\\tvolume = {431-432},\\n\\tissn = {0926-860X},\\n\\tshorttitle = {New life of a forgotten method},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0926860X12002268},\\n\\tdoi = {10.1016/j.apcata.2012.04.025},\\n\\tabstract = {Driven by global environmental concerns, great efforts are currently made to develop novel, cheap and practical means for producing highly efficient electrocatalysts, specifically for the low-temperature fuel-cell applications. Employing an old but yet unexplored method based on electrochemical dispergation of platinum by the alternating current, we show that the freshly prepared Pt/C catalysts exhibit greatly enhanced catalytic activity (up to 350\\\\% for oxygen reduction and up to 200\\\\% for ethylene glycol oxidation) as compared with that of a commercially available counterpart (E-TEK). A key role in these reactions is attributed to a specific nanoparticle morphology. These findings should provide a revival of an ancient but simple and efficient electrochemical process and motivate further researches in the field.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Applied Catalysis A: General},\\n\\tauthor = {Leontyev, Igor and Kuriganova, Aleksandra and Kudryavtsev, Yuri and Dkhil, Brahim and Smirnova, Nina},\\n\\tmonth = jul,\\n\\tyear = {2012},\\n\\tkeywords = {Electrocatalysis, Oxygen reduction reaction (ORR), X-ray diffraction (XRD), Low-temperature fuel cell, Platinum nanoparticles, Shape},\\n\\tpages = {120--125},\\n}\\n\\n\",\"author_short\":[\"Leontyev, I.\",\"Kuriganova, A.\",\"Kudryavtsev, Y.\",\"Dkhil, B.\",\"Smirnova, N.\"],\"key\":\"leontyev_new_2012\",\"id\":\"leontyev_new_2012\",\"bibbaseid\":\"leontyev-kuriganova-kudryavtsev-dkhil-smirnova-newlifeofaforgottenmethodelectrochemicalroutetowardhighlyefficientptccatalystsforlowtemperaturefuelcells-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0926860X12002268\"},\"keyword\":[\"Electrocatalysis\",\"Oxygen reduction reaction (ORR)\",\"X-ray diffraction (XRD)\",\"Low-temperature fuel cell\",\"Platinum nanoparticles\",\"Shape\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Исследование влияния адсорбции моноокиси углерода на характеристики линии задержки на ПАВ с чувствительным элементом из наностержней оксида цинка\",\"url\":\"http://ivdon.ru/ru/magazine/archive/n4p1y2012/1189\",\"abstract\":\"Сетевой научный журнал «Инженерный вестник Дона»\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Карапетьян\"],\"firstnames\":[\"Г.\",\"Я.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Николаев\"],\"firstnames\":[\"А.\",\"Л.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Несветаев\"],\"firstnames\":[\"Д.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2012\",\"bibtex\":\"@article{__2012-1,\\n\\ttitle = {Исследование влияния адсорбции моноокиси углерода на характеристики линии задержки на ПАВ с чувствительным элементом из наностержней оксида цинка},\\n\\turl = {http://ivdon.ru/ru/magazine/archive/n4p1y2012/1189},\\n\\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Карапетьян, Г. Я. and Николаев, А. Л. and Лянгузов, Н. В. and Несветаев, Д. Г. and Кайдашев, Е. М.},\\n\\tmonth = jul,\\n\\tyear = {2012},\\n}\\n\\n\",\"author_short\":[\"Карапетьян, Г. Я.\",\"Николаев, А. Л.\",\"Лянгузов, Н. В.\",\"Несветаев, Д. Г.\",\"Кайдашев, Е. М.\"],\"key\":\"__2012-1\",\"id\":\"__2012-1\",\"bibbaseid\":\"------2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://ivdon.ru/ru/magazine/archive/n4p1y2012/1189\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":1,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Diffraction of surface magnetostatic waves by surface cavities on ferromagnetic film\",\"volume\":\"57\",\"issn\":\"1555-6557\",\"url\":\"https://doi.org/10.1134/S1064226912060137\",\"doi\":\"10.1134/S1064226912060137\",\"abstract\":\"The diffraction problem of the scattering of surface magnetostatic waves by shallow rectangular and circular cavities on the surface of a ferromagnetic film that is tangentially magnetized with respect to the surface is numerically analyzed in the magnetostatic approximation.\",\"language\":\"en\",\"number\":\"7\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Communications Technology and Electronics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ivanov\"],\"firstnames\":[\"V.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Babichev\"],\"firstnames\":[\"R.\",\"K.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shloma\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2012\",\"keywords\":\"Circular Cavity, Lower Lobe, Rectangular Cavity, Reflection Coefficient, Surface Cavity\",\"pages\":\"726–733\",\"bibtex\":\"@article{timoshenko_diffraction_2012,\\n\\ttitle = {Diffraction of surface magnetostatic waves by surface cavities on ferromagnetic film},\\n\\tvolume = {57},\\n\\tissn = {1555-6557},\\n\\turl = {https://doi.org/10.1134/S1064226912060137},\\n\\tdoi = {10.1134/S1064226912060137},\\n\\tabstract = {The diffraction problem of the scattering of surface magnetostatic waves by shallow rectangular and circular cavities on the surface of a ferromagnetic film that is tangentially magnetized with respect to the surface is numerically analyzed in the magnetostatic approximation.},\\n\\tlanguage = {en},\\n\\tnumber = {7},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Communications Technology and Electronics},\\n\\tauthor = {Timoshenko, P. E. and Ivanov, V. N. and Babichev, R. K. and Shloma, A. V.},\\n\\tmonth = jul,\\n\\tyear = {2012},\\n\\tkeywords = {Circular Cavity, Lower Lobe, Rectangular Cavity, Reflection Coefficient, Surface Cavity},\\n\\tpages = {726--733},\\n}\\n\\n\",\"author_short\":[\"Timoshenko, P. E.\",\"Ivanov, V. N.\",\"Babichev, R. K.\",\"Shloma, A. V.\"],\"key\":\"timoshenko_diffraction_2012\",\"id\":\"timoshenko_diffraction_2012\",\"bibbaseid\":\"timoshenko-ivanov-babichev-shloma-diffractionofsurfacemagnetostaticwavesbysurfacecavitiesonferromagneticfilm-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1064226912060137\"},\"keyword\":[\"Circular Cavity\",\"Lower Lobe\",\"Rectangular Cavity\",\"Reflection Coefficient\",\"Surface Cavity\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Nickel nanoparticles in carbon structures prepared by solid-phase pyrolysis of nickel-phthalocyanine\",\"volume\":\"14\",\"issn\":\"1572-896X\",\"url\":\"https://doi.org/10.1007/s11051-012-0982-6\",\"doi\":\"10.1007/s11051-012-0982-6\",\"abstract\":\"By using a modified method of solid-phase pyrolysis of metal-phthalocyanines, we have synthesized ferromagnetic Ni nanoparticles in different carbon structures: amorphous carbon plates, multiwall carbon nanotubes, carbon fibers, and graphitized capsules. The composition, structure and morphology of prepared composite materials have been studied by energy dispersive X-ray microanalysis, scanning and transmission electron microscopy, and X-ray diffraction technique. It has been found that the sizes of nickel nanoparticles (10–500 nm) and the type of carbon structures strongly depend on the pyrolysis conditions. By using the X-band ferromagnetic resonance measurements, we have revealed features of the temperature dependence of resonance spectra of single-domain and multi-domain Ni nanoparticles in Ni/C composites.\",\"language\":\"en\",\"number\":\"7\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Nanoparticle Research\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Manukyan\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mirzakhanyan\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Badalyan\"],\"firstnames\":[\"G.\",\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirinyan\"],\"firstnames\":[\"G.\",\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fedorenko\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lianguzov\"],\"firstnames\":[\"N.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bugaev\"],\"firstnames\":[\"L.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sharoyan\"],\"firstnames\":[\"E.\",\"G.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2012\",\"keywords\":\"Carbon nanostructures, Magnetic properties, Nickel nanoparticles, Nickel-phthalocyanine, Solid-phase pyrolysis\",\"pages\":\"982\",\"bibtex\":\"@article{manukyan_nickel_2012,\\n\\ttitle = {Nickel nanoparticles in carbon structures prepared by solid-phase pyrolysis of nickel-phthalocyanine},\\n\\tvolume = {14},\\n\\tissn = {1572-896X},\\n\\turl = {https://doi.org/10.1007/s11051-012-0982-6},\\n\\tdoi = {10.1007/s11051-012-0982-6},\\n\\tabstract = {By using a modified method of solid-phase pyrolysis of metal-phthalocyanines, we have synthesized ferromagnetic Ni nanoparticles in different carbon structures: amorphous carbon plates, multiwall carbon nanotubes, carbon fibers, and graphitized capsules. The composition, structure and morphology of prepared composite materials have been studied by energy dispersive X-ray microanalysis, scanning and transmission electron microscopy, and X-ray diffraction technique. It has been found that the sizes of nickel nanoparticles (10–500 nm) and the type of carbon structures strongly depend on the pyrolysis conditions. By using the X-band ferromagnetic resonance measurements, we have revealed features of the temperature dependence of resonance spectra of single-domain and multi-domain Ni nanoparticles in Ni/C composites.},\\n\\tlanguage = {en},\\n\\tnumber = {7},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Nanoparticle Research},\\n\\tauthor = {Manukyan, A. S. and Mirzakhanyan, A. A. and Badalyan, G. R. and Shirinyan, G. H. and Fedorenko, A. G. and Lianguzov, N. V. and Yuzyuk, Yu I. and Bugaev, L. A. and Sharoyan, E. G.},\\n\\tmonth = jun,\\n\\tyear = {2012},\\n\\tkeywords = {Carbon nanostructures, Magnetic properties, Nickel nanoparticles, Nickel-phthalocyanine, Solid-phase pyrolysis},\\n\\tpages = {982},\\n}\\n\\n\",\"author_short\":[\"Manukyan, A. S.\",\"Mirzakhanyan, A. A.\",\"Badalyan, G. R.\",\"Shirinyan, G. H.\",\"Fedorenko, A. G.\",\"Lianguzov, N. V.\",\"Yuzyuk, Y. I.\",\"Bugaev, L. A.\",\"Sharoyan, E. G.\"],\"key\":\"manukyan_nickel_2012\",\"id\":\"manukyan_nickel_2012\",\"bibbaseid\":\"manukyan-mirzakhanyan-badalyan-shirinyan-fedorenko-lianguzov-yuzyuk-bugaev-etal-nickelnanoparticlesincarbonstructurespreparedbysolidphasepyrolysisofnickelphthalocyanine-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1007/s11051-012-0982-6\"},\"keyword\":[\"Carbon nanostructures\",\"Magnetic properties\",\"Nickel nanoparticles\",\"Nickel-phthalocyanine\",\"Solid-phase pyrolysis\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Пассивный беспроводный датчик на поверхностных акустических волнах для измерения параметров газовых и жидких сред\",\"url\":\"http://ivdon.ru/magazine/archive/n2y2012/770\",\"abstract\":\"Сетевой научный журнал «Инженерный вестник Дона»\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Карапетьян\"],\"firstnames\":[\"Г.\",\"Я.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Днепровский\"],\"firstnames\":[\"В.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Багдасарян\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Багдасарян\"],\"firstnames\":[\"С.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Николаев\"],\"firstnames\":[\"А.\",\"Л.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2012\",\"bibtex\":\"@article{__2012-2,\\n\\ttitle = {Пассивный беспроводный датчик на поверхностных акустических волнах для измерения параметров газовых и жидких сред},\\n\\turl = {http://ivdon.ru/magazine/archive/n2y2012/770},\\n\\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Карапетьян, Г. Я. and Днепровский, В. Г. and Багдасарян, А. С. and Багдасарян, С. А. and Николаев, А. Л. and Кайдашев, Е. М.},\\n\\tmonth = mar,\\n\\tyear = {2012},\\n}\\n\\n\",\"author_short\":[\"Карапетьян, Г. Я.\",\"Днепровский, В. Г.\",\"Багдасарян, А. С.\",\"Багдасарян, С. А.\",\"Николаев, А. Л.\",\"Кайдашев, Е. М.\"],\"key\":\"__2012-2\",\"id\":\"__2012-2\",\"bibbaseid\":\"-------2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://ivdon.ru/magazine/archive/n2y2012/770\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Тригональная хиральная и гексагональная двумерные квазикристаллические укладки\",\"url\":\"http://ivdon.ru/magazine/archive/n2y2012/816\",\"abstract\":\"Сетевой научный журнал «Инженерный вестник Дона»\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Рошаль\"],\"firstnames\":[\"Д.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Рошаль\"],\"firstnames\":[\"С.\",\"Б.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2012\",\"bibtex\":\"@article{__2012-3,\\n\\ttitle = {Тригональная хиральная и гексагональная двумерные квазикристаллические укладки},\\n\\turl = {http://ivdon.ru/magazine/archive/n2y2012/816},\\n\\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Рошаль, Д. С. and Рошаль, С. Б.},\\n\\tmonth = jan,\\n\\tyear = {2012},\\n}\\n\\n\",\"author_short\":[\"Рошаль, Д. С.\",\"Рошаль, С. Б.\"],\"key\":\"__2012-3\",\"id\":\"__2012-3\",\"bibbaseid\":\"---2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://ivdon.ru/magazine/archive/n2y2012/816\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Chiral Quasicrystalline Order and Dodecahedral Geometry in Exceptional Families of Viruses\",\"volume\":\"108\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevLett.108.038102\",\"doi\":\"10.1103/PhysRevLett.108.038102\",\"abstract\":\"On the example of exceptional families of viruses we (i) show the existence of a completely new type of matter organization in nanoparticles, in which the regions with a chiral pentagonal quasicrystalline order of protein positions are arranged in a structure commensurate with the spherical topology and dodecahedral geometry, (ii) generalize the classical theory of quasicrystals (QCs) to explain this organization, and (iii) establish the relation between local chiral QC order and nonzero curvature of the dodecahedral capsid faces.\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Konevtsova\"],\"firstnames\":[\"O.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorman\"],\"firstnames\":[\"V.\",\"L.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2012\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"038102\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\T2BMSVJV\\\\\\\\Konevtsova и др. - 2012 - Chiral Quasicrystalline Order and Dodecahedral Geo.pdf:application/pdf\",\"bibtex\":\"@article{konevtsova_chiral_2012,\\n\\ttitle = {Chiral {Quasicrystalline} {Order} and {Dodecahedral} {Geometry} in {Exceptional} {Families} of {Viruses}},\\n\\tvolume = {108},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevLett.108.038102},\\n\\tdoi = {10.1103/PhysRevLett.108.038102},\\n\\tabstract = {On the example of exceptional families of viruses we (i) show the existence of a completely new type of matter organization in nanoparticles, in which the regions with a chiral pentagonal quasicrystalline order of protein positions are arranged in a structure commensurate with the spherical topology and dodecahedral geometry, (ii) generalize the classical theory of quasicrystals (QCs) to explain this organization, and (iii) establish the relation between local chiral QC order and nonzero curvature of the dodecahedral capsid faces.},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review Letters},\\n\\tauthor = {Konevtsova, O. V. and Rochal, S. B. and Lorman, V. L.},\\n\\tmonth = jan,\\n\\tyear = {2012},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {038102},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\T2BMSVJV\\\\\\\\Konevtsova и др. - 2012 - Chiral Quasicrystalline Order and Dodecahedral Geo.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Konevtsova, O. V.\",\"Rochal, S. B.\",\"Lorman, V. L.\"],\"key\":\"konevtsova_chiral_2012\",\"id\":\"konevtsova_chiral_2012\",\"bibbaseid\":\"konevtsova-rochal-lorman-chiralquasicrystallineorderanddodecahedralgeometryinexceptionalfamiliesofviruses-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevLett.108.038102\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Femtosecond Infrared Laser Annealing of PZT Films on a Metal Substrate\",\"volume\":\"433\",\"issn\":\"0015-0193\",\"url\":\"https://doi.org/10.1080/00150193.2012.696459\",\"doi\":\"10.1080/00150193.2012.696459\",\"abstract\":\"The quazi-amorphous PbZrTiO2 (PZT) precursor film on a platinized silicon substrate is annealed by femtosecond laser at the wavelength falling into transparency band of PZT. Two areas are found within the laser spot: ferroelectric perovskite revealing strong hysteresis and coercivity in piezoelectric response and paraelectric with low piezoresponse and the absence of hysteresis and coercivity. Annealing takes place through platinum absorbing laser irradiation and acting as a heat source for transparent film on top of it.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Firsova\"],\"firstnames\":[\"N.\",\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mishina\"],\"firstnames\":[\"E.\",\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sigov\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Senkevich\"],\"firstnames\":[\"S.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pronin\"],\"firstnames\":[\"I.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kholkin\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bdikin\"],\"firstnames\":[\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2012\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2012.696459\",\"keywords\":\"thin films, Raman scattering, ferroelectric, femtosecond laser annealing, piezoelectric, second harmonic generation, Sol-gel\",\"pages\":\"164–169\",\"bibtex\":\"@article{firsova_femtosecond_2012,\\n\\ttitle = {Femtosecond {Infrared} {Laser} {Annealing} of {PZT} {Films} on a {Metal} {Substrate}},\\n\\tvolume = {433},\\n\\tissn = {0015-0193},\\n\\turl = {https://doi.org/10.1080/00150193.2012.696459},\\n\\tdoi = {10.1080/00150193.2012.696459},\\n\\tabstract = {The quazi-amorphous PbZrTiO2 (PZT) precursor film on a platinized silicon substrate is annealed by femtosecond laser at the wavelength falling into transparency band of PZT. Two areas are found within the laser spot: ferroelectric perovskite revealing strong hysteresis and coercivity in piezoelectric response and paraelectric with low piezoresponse and the absence of hysteresis and coercivity. Annealing takes place through platinum absorbing laser irradiation and acting as a heat source for transparent film on top of it.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Firsova, N. Yu. and Mishina, E. D. and Sigov, A. S. and Senkevich, S. V. and Pronin, I. P. and Kholkin, A. and Bdikin, I. and Yuzyuk, Yu. I.},\\n\\tmonth = jan,\\n\\tyear = {2012},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/00150193.2012.696459},\\n\\tkeywords = {thin films, Raman scattering, ferroelectric, femtosecond laser annealing, piezoelectric, second harmonic generation, Sol-gel},\\n\\tpages = {164--169},\\n}\\n\\n\",\"author_short\":[\"Firsova, N. Y.\",\"Mishina, E. D.\",\"Sigov, A. S.\",\"Senkevich, S. V.\",\"Pronin, I. P.\",\"Kholkin, A.\",\"Bdikin, I.\",\"Yuzyuk, Y. I.\"],\"key\":\"firsova_femtosecond_2012\",\"id\":\"firsova_femtosecond_2012\",\"bibbaseid\":\"firsova-mishina-sigov-senkevich-pronin-kholkin-bdikin-yuzyuk-femtosecondinfraredlaserannealingofpztfilmsonametalsubstrate-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/00150193.2012.696459\"},\"keyword\":[\"thin films\",\"Raman scattering\",\"ferroelectric\",\"femtosecond laser annealing\",\"piezoelectric\",\"second harmonic generation\",\"Sol-gel\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Diagnostics of Carbonaceous Nanomaterial “Taunit” by Raman Spectroscopy\",\"volume\":\"7\",\"doi\":\"10.1166/jno.2012.1225\",\"abstract\":\"Crystalline structure perfection of carbonaceous nanomaterial (CNM) “Taunit” which constitutes the multi-walled nanotubes was studied using a Raman spectroscopy technique. CNM “Taunit” was synthesized by MOCVD method. The pristine material, the samples annealed at different temperatures and the samples functionalized by Pt-catalyst nanoparticles were investigated. It has been found that “Taunit” belongs to the poorly organized carbon materials but its crystalline structure was observed to order while the annealing temperature increased. D1 and G Raman band (at 1350 and 1580 cm–1, respectively) intensity ratios were calculated to estimate the crystal structure ordering of CNM “Taunit”. The investigation of the influence of functionalization by the catalyst nanoparticles shows that Pt-catalyst precipitation on the surface of MWNTs leads to the increase of the defect band intensity due to an appearance of lattice defects.\",\"number\":\"1\",\"journal\":\"Journal of Nanoelectronics and Optoelectronics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"O.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontiev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tkachev\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2012\",\"keywords\":\"RAMAN SPECTROSCOPY, CRYSTALLINE STRUCTURE ORDERING, D- AND G-BAND INTENSITIES RATIOS, MULTI-WALLED CARBON NANOTUBES, PT-CATALYST NANOPARTICLES\",\"pages\":\"95–98\",\"bibtex\":\"@article{maslova_diagnostics_2012,\\n\\ttitle = {Diagnostics of {Carbonaceous} {Nanomaterial} “{Taunit}” by {Raman} {Spectroscopy}},\\n\\tvolume = {7},\\n\\tdoi = {10.1166/jno.2012.1225},\\n\\tabstract = {Crystalline structure perfection of carbonaceous nanomaterial (CNM) “Taunit” which constitutes the multi-walled nanotubes was studied using a Raman spectroscopy technique. CNM “Taunit” was synthesized by MOCVD method. The pristine material, the samples annealed\\nat different temperatures and the samples functionalized by Pt-catalyst nanoparticles were investigated. It has been found that “Taunit” belongs to the poorly organized carbon materials but its crystalline structure was observed to order while the annealing temperature increased.\\nD1 and G Raman band (at 1350 and 1580 cm–1, respectively) intensity ratios were calculated to estimate the crystal structure ordering of CNM “Taunit”. The investigation of the influence of functionalization by the catalyst nanoparticles shows that Pt-catalyst\\nprecipitation on the surface of MWNTs leads to the increase of the defect band intensity due to an appearance of lattice defects.},\\n\\tnumber = {1},\\n\\tjournal = {Journal of Nanoelectronics and Optoelectronics},\\n\\tauthor = {Maslova, O. A. and Mikheykin, A. S. and Leontiev, I. N. and Yuzyuk, Yu. I. and Tkachev, A. G.},\\n\\tmonth = jan,\\n\\tyear = {2012},\\n\\tkeywords = {RAMAN SPECTROSCOPY, CRYSTALLINE STRUCTURE ORDERING, D- AND G-BAND INTENSITIES RATIOS, MULTI-WALLED CARBON NANOTUBES, PT-CATALYST NANOPARTICLES},\\n\\tpages = {95--98},\\n}\\n\\n\",\"author_short\":[\"Maslova, O. A.\",\"Mikheykin, A. S.\",\"Leontiev, I. N.\",\"Yuzyuk, Y. I.\",\"Tkachev, A. G.\"],\"key\":\"maslova_diagnostics_2012\",\"id\":\"maslova_diagnostics_2012\",\"bibbaseid\":\"maslova-mikheykin-leontiev-yuzyuk-tkachev-diagnosticsofcarbonaceousnanomaterialtaunitbyramanspectroscopy-2012\",\"role\":\"author\",\"urls\":{},\"keyword\":[\"RAMAN SPECTROSCOPY\",\"CRYSTALLINE STRUCTURE ORDERING\",\"D- AND G-BAND INTENSITIES RATIOS\",\"MULTI-WALLED CARBON NANOTUBES\",\"PT-CATALYST NANOPARTICLES\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Raman Study of Uniaxial Strain in Individual Single-Wall Carbon Nanotubes Induced by Temperature Changes\",\"volume\":\"7\",\"doi\":\"10.1166/jno.2012.1221\",\"abstract\":\"We report the temperature dependence of the Raman spectra of a gelatine-based composite material doped with single-walled carbon nanotubes (SWNT@gelatin). On decreasing the temperature from 290 to 20 K a significant up-shift of the G-mode and no changes in the radial breathing modes are observed. This behaviour cannot be understood by pure thermal effects. We explain these results in terms of an uniaxial strain of the nanotubes induced by the thermal expansion mismatch between the nanotubes and the surrounding matrix.\",\"number\":\"1\",\"journal\":\"Journal of Nanoelectronics and Optoelectronics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Levshov\"],\"firstnames\":[\"D.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Michel\"],\"firstnames\":[\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Voisin\"],\"firstnames\":[\"C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Alvarez\"],\"firstnames\":[\"L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Berger\"],\"firstnames\":[\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Roussignol\"],\"firstnames\":[\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sauvajol\"],\"firstnames\":[\"J.-L.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2012\",\"keywords\":\"RAMAN SPECTROSCOPY, COMPOSITES, SINGLE-WALLED CARBON NANOTUBES, UNIAXIAL STRAIN\",\"pages\":\"77–80\",\"bibtex\":\"@article{levshov_raman_2012,\\n\\ttitle = {Raman {Study} of {Uniaxial} {Strain} in {Individual} {Single}-{Wall} {Carbon} {Nanotubes} {Induced} by {Temperature} {Changes}},\\n\\tvolume = {7},\\n\\tdoi = {10.1166/jno.2012.1221},\\n\\tabstract = {We report the temperature dependence of the Raman spectra of a gelatine-based composite material doped with single-walled carbon nanotubes (SWNT@gelatin). On decreasing the temperature from 290 to 20 K a significant up-shift of the G-mode and no changes in the radial breathing modes\\nare observed. This behaviour cannot be understood by pure thermal effects. We explain these results in terms of an uniaxial strain of the nanotubes induced by the thermal expansion mismatch between the nanotubes and the surrounding matrix.},\\n\\tnumber = {1},\\n\\tjournal = {Journal of Nanoelectronics and Optoelectronics},\\n\\tauthor = {Levshov, D. I. and Yuzyuk, Yu. I. and Michel, T. and Voisin, C. and Alvarez, L. and Berger, S. and Roussignol, P. and Sauvajol, J.-L.},\\n\\tmonth = jan,\\n\\tyear = {2012},\\n\\tkeywords = {RAMAN SPECTROSCOPY, COMPOSITES, SINGLE-WALLED CARBON NANOTUBES, UNIAXIAL STRAIN},\\n\\tpages = {77--80},\\n}\\n\\n\",\"author_short\":[\"Levshov, D. I.\",\"Yuzyuk, Y. I.\",\"Michel, T.\",\"Voisin, C.\",\"Alvarez, L.\",\"Berger, S.\",\"Roussignol, P.\",\"Sauvajol, J.\"],\"key\":\"levshov_raman_2012\",\"id\":\"levshov_raman_2012\",\"bibbaseid\":\"levshov-yuzyuk-michel-voisin-alvarez-berger-roussignol-sauvajol-ramanstudyofuniaxialstraininindividualsinglewallcarbonnanotubesinducedbytemperaturechanges-2012\",\"role\":\"author\",\"urls\":{},\"keyword\":[\"RAMAN SPECTROSCOPY\",\"COMPOSITES\",\"SINGLE-WALLED CARBON NANOTUBES\",\"UNIAXIAL STRAIN\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Enhanced Magnetization and Ferroelectric Switching in Multiferroic BST/BNFO Superstructures\",\"volume\":\"433\",\"issn\":\"0015-0193\",\"url\":\"https://doi.org/10.1080/00150193.2012.696448\",\"doi\":\"10.1080/00150193.2012.696448\",\"abstract\":\"Multiferroic BaSrTiO3/NdBiFeO3 (BST/BNFO) mulilayers with 3 nm and 6 nm layer thickness demonstrate superlattice structure in the XRD patterns. The break of the spin cycloide and interface strain results in ferromagnetic behavior and enhancement of magnetization. The total thickness of BNFO is varied in the range of 50–60 nm, and saturation magnetization is varied in the range of 50-60 emu/cm3, which is an order of magnitude higher than reported for BaTiO3/BiFeO3 superstructure [1]. Polarization hysteresis loop were obtained by second harmonic generation technique and show significant electro-optical switchability. Both magnetization and ferroelectric polarization possess bulk rather than interface localization.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Ivanov\"],\"firstnames\":[\"M.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sherstyuk\"],\"firstnames\":[\"N.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mishina\"],\"firstnames\":[\"E.\",\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sigov\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mukhortov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Moshnyaga\"],\"firstnames\":[\"V.\",\"T.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2012\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2012.696448\",\"keywords\":\"thin films, superlattice, polarization, Multiferroic, second harmonic generation, magnetization\",\"pages\":\"158–163\",\"bibtex\":\"@article{ivanov_enhanced_2012,\\n\\ttitle = {Enhanced {Magnetization} and {Ferroelectric} {Switching} in {Multiferroic} {BST}/{BNFO} {Superstructures}},\\n\\tvolume = {433},\\n\\tissn = {0015-0193},\\n\\turl = {https://doi.org/10.1080/00150193.2012.696448},\\n\\tdoi = {10.1080/00150193.2012.696448},\\n\\tabstract = {Multiferroic BaSrTiO3/NdBiFeO3 (BST/BNFO) mulilayers with 3 nm and 6 nm layer thickness demonstrate superlattice structure in the XRD patterns. The break of the spin cycloide and interface strain results in ferromagnetic behavior and enhancement of magnetization. The total thickness of BNFO is varied in the range of 50–60 nm, and saturation magnetization is varied in the range of 50-60 emu/cm3, which is an order of magnitude higher than reported for BaTiO3/BiFeO3 superstructure [1]. Polarization hysteresis loop were obtained by second harmonic generation technique and show significant electro-optical switchability. Both magnetization and ferroelectric polarization possess bulk rather than interface localization.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Ivanov, M. S. and Sherstyuk, N. E. and Mishina, E. D. and Sigov, A. S. and Mukhortov, V. M. and Moshnyaga, V. T.},\\n\\tmonth = jan,\\n\\tyear = {2012},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/00150193.2012.696448},\\n\\tkeywords = {thin films, superlattice, polarization, Multiferroic, second harmonic generation, magnetization},\\n\\tpages = {158--163},\\n}\\n\\n\",\"author_short\":[\"Ivanov, M. S.\",\"Sherstyuk, N. E.\",\"Mishina, E. D.\",\"Sigov, A. S.\",\"Mukhortov, V. M.\",\"Moshnyaga, V. T.\"],\"key\":\"ivanov_enhanced_2012\",\"id\":\"ivanov_enhanced_2012\",\"bibbaseid\":\"ivanov-sherstyuk-mishina-sigov-mukhortov-moshnyaga-enhancedmagnetizationandferroelectricswitchinginmultiferroicbstbnfosuperstructures-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/00150193.2012.696448\"},\"keyword\":[\"thin films\",\"superlattice\",\"polarization\",\"Multiferroic\",\"second harmonic generation\",\"magnetization\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Селективный рост массивов наностержней гидротермальным методом на кремнии\",\"url\":\"http://ivdon.ru/magazine/archive/n1y2012/684\",\"abstract\":\"Сетевой научный журнал «Инженерный вестник Дона»\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Ступко\"],\"firstnames\":[\"М.\",\"Ю.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Николаев\"],\"firstnames\":[\"А.\",\"Л.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2011\",\"bibtex\":\"@article{__2011,\\n\\ttitle = {Селективный рост массивов наностержней гидротермальным методом на кремнии},\\n\\turl = {http://ivdon.ru/magazine/archive/n1y2012/684},\\n\\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Ступко, М. Ю. and Лянгузов, Н. В. and Николаев, А. Л. and Кайдашев, Е. М.},\\n\\tmonth = dec,\\n\\tyear = {2011},\\n}\\n\\n\",\"author_short\":[\"Ступко, М. Ю.\",\"Лянгузов, Н. В.\",\"Николаев, А. Л.\",\"Кайдашев, Е. 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a\":\"https://www.klassphil.hu-berlin.de/de/personen/andrea-beyer\",\"bluestein, d\":\"https://www.bme.stonybrook.edu/labs/dbluestein/aaapatient.html\",\"sabattini, l\":\"https://883789326-atari-embeds.googleusercontent.com/embeds/16cb204cf3a9d4d223a0a3fd8b0eec5d/inner-frame-minified.html\"}},\"downloads\":9,\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"Raman spectra of nickel-carbon nanocomposites\",\"volume\":\"7998\",\"url\":\"https://www.spiedigitallibrary.org/conference-proceedings-of-spie/7998/79981B/Raman-spectra-of-nickel-carbon-nanocomposites/10.1117/12.890940.full\",\"doi\":\"10.1117/12.890940\",\"abstract\":\"By using the solid-phase pyrolysis of phthalocyanines the nickel-carbon nanocomposites have been synthesized. The composition, structure, and morphology of samples were investigated by scanning electron microscopy and Raman spectroscopy. The first-order Raman shifts of prepared materials were measured with laser excitation at 514.5 nm in the frequency range from 900 to 2000 cm$^{\\\\textrm{-1}}$. It is shown that the degree of graphitization in nanocomposites essentially depends on the pyrolysis temperature. By analyzing the intensity ratio of Raman D- and G-bands the mean sizes of graphitic nanocrystallites in prepared samples were estimated.\",\"urldate\":\"2023-11-11\",\"booktitle\":\"International Conference on Laser Physics 2010\",\"publisher\":\"SPIE\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Mirzakhanyan\"],\"firstnames\":[\"Armen\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Manukyan\"],\"firstnames\":[\"Aram\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Badalyan\"],\"firstnames\":[\"George\",\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Khachatryan\"],\"firstnames\":[\"Tatevik\",\"K.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"Olga\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yurii\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bugaev\"],\"firstnames\":[\"Lusegen\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sharoyan\"],\"firstnames\":[\"Eduard\",\"G.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2011\",\"pages\":\"346–349\",\"bibtex\":\"@inproceedings{mirzakhanyan_raman_2011,\\n\\ttitle = {Raman spectra of nickel-carbon nanocomposites},\\n\\tvolume = {7998},\\n\\turl = {https://www.spiedigitallibrary.org/conference-proceedings-of-spie/7998/79981B/Raman-spectra-of-nickel-carbon-nanocomposites/10.1117/12.890940.full},\\n\\tdoi = {10.1117/12.890940},\\n\\tabstract = {By using the solid-phase pyrolysis of phthalocyanines the nickel-carbon nanocomposites have been synthesized. The composition, structure, and morphology of samples were investigated by scanning electron microscopy and Raman spectroscopy. The first-order Raman shifts of prepared materials were measured with laser excitation at 514.5 nm in the frequency range from 900 to 2000 cm$^{\\\\textrm{-1}}$. It is shown that the degree of graphitization in nanocomposites essentially depends on the pyrolysis temperature. By analyzing the intensity ratio of Raman D- and G-bands the mean sizes of graphitic nanocrystallites in prepared samples were estimated.},\\n\\turldate = {2023-11-11},\\n\\tbooktitle = {International {Conference} on {Laser} {Physics} 2010},\\n\\tpublisher = {SPIE},\\n\\tauthor = {Mirzakhanyan, Armen A. and Manukyan, Aram S. and Badalyan, George R. and Khachatryan, Tatevik K. and Maslova, Olga A. and Yuzyuk, Yurii I. and Bugaev, Lusegen A. and Sharoyan, Eduard G.},\\n\\tmonth = mar,\\n\\tyear = {2011},\\n\\tpages = {346--349},\\n}\\n\\n\",\"author_short\":[\"Mirzakhanyan, A. A.\",\"Manukyan, A. S.\",\"Badalyan, G. R.\",\"Khachatryan, T. K.\",\"Maslova, O. A.\",\"Yuzyuk, Y. I.\",\"Bugaev, L. A.\",\"Sharoyan, E. G.\"],\"key\":\"mirzakhanyan_raman_2011\",\"id\":\"mirzakhanyan_raman_2011\",\"bibbaseid\":\"mirzakhanyan-manukyan-badalyan-khachatryan-maslova-yuzyuk-bugaev-sharoyan-ramanspectraofnickelcarbonnanocomposites-2011\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.spiedigitallibrary.org/conference-proceedings-of-spie/7998/79981B/Raman-spectra-of-nickel-carbon-nanocomposites/10.1117/12.890940.full\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Experimental Evidence of a Mechanical Coupling between Layers in an Individual Double-Walled Carbon Nanotube\",\"volume\":\"11\",\"issn\":\"1530-6984\",\"url\":\"https://doi.org/10.1021/nl2026234\",\"doi\":\"10.1021/nl2026234\",\"abstract\":\"We perform transmission electron microscopy, electron diffraction, and Raman scattering experiments on an individual suspended double-walled carbon nanotube (DWCNT). The first two techniques allow the unambiguous determination of the DWCNT structure: (12,8)@(16,14). However, the low-frequency features in the Raman spectra cannot be connected to the derived layer diameters d by means of the 1/d power law, widely used for the diameter dependence of the radial-breathing mode of single-walled nanotubes. We discuss this disagreement in terms of mechanical coupling between the layers of the DWCNT, which results in collective vibrational modes. Theoretical predictions for the breathing-like modes of the DWCNT, originating from the radial-breathing modes of the layers, are in a very good agreement with the observed Raman spectra. Moreover, the mechanical coupling qualitatively explains the observation of Raman lines of breathing-like modes, whenever only one of the layers is in resonance with the laser energy.\",\"number\":\"11\",\"urldate\":\"2023-11-11\",\"journal\":\"Nano Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Levshov\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Than\"],\"firstnames\":[\"T.\",\"X.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Arenal\"],\"firstnames\":[\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Popov\"],\"firstnames\":[\"V.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Parret\"],\"firstnames\":[\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Paillet\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Jourdain\"],\"firstnames\":[\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zahab\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Michel\"],\"firstnames\":[\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sauvajol\"],\"firstnames\":[\"J.-L.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2011\",\"note\":\"Publisher: American Chemical Society\",\"pages\":\"4800–4804\",\"bibtex\":\"@article{levshov_experimental_2011,\\n\\ttitle = {Experimental {Evidence} of a {Mechanical} {Coupling} between {Layers} in an {Individual} {Double}-{Walled} {Carbon} {Nanotube}},\\n\\tvolume = {11},\\n\\tissn = {1530-6984},\\n\\turl = {https://doi.org/10.1021/nl2026234},\\n\\tdoi = {10.1021/nl2026234},\\n\\tabstract = {We perform transmission electron microscopy, electron diffraction, and Raman scattering experiments on an individual suspended double-walled carbon nanotube (DWCNT). The first two techniques allow the unambiguous determination of the DWCNT structure: (12,8)@(16,14). However, the low-frequency features in the Raman spectra cannot be connected to the derived layer diameters d by means of the 1/d power law, widely used for the diameter dependence of the radial-breathing mode of single-walled nanotubes. We discuss this disagreement in terms of mechanical coupling between the layers of the DWCNT, which results in collective vibrational modes. Theoretical predictions for the breathing-like modes of the DWCNT, originating from the radial-breathing modes of the layers, are in a very good agreement with the observed Raman spectra. Moreover, the mechanical coupling qualitatively explains the observation of Raman lines of breathing-like modes, whenever only one of the layers is in resonance with the laser energy.},\\n\\tnumber = {11},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Nano Letters},\\n\\tauthor = {Levshov, D. and Than, T. X. and Arenal, R. and Popov, V. N. and Parret, R. and Paillet, M. and Jourdain, V. and Zahab, A. A. and Michel, T. and Yuzyuk, Yu. I. and Sauvajol, J.-L.},\\n\\tmonth = nov,\\n\\tyear = {2011},\\n\\tnote = {Publisher: American Chemical Society},\\n\\tpages = {4800--4804},\\n}\\n\\n\",\"author_short\":[\"Levshov, D.\",\"Than, T. X.\",\"Arenal, R.\",\"Popov, V. N.\",\"Parret, R.\",\"Paillet, M.\",\"Jourdain, V.\",\"Zahab, A. A.\",\"Michel, T.\",\"Yuzyuk, Y. I.\",\"Sauvajol, J.\"],\"key\":\"levshov_experimental_2011\",\"id\":\"levshov_experimental_2011\",\"bibbaseid\":\"levshov-than-arenal-popov-parret-paillet-jourdain-zahab-etal-experimentalevidenceofamechanicalcouplingbetweenlayersinanindividualdoublewalledcarbonnanotube-2011\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1021/nl2026234\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Catalytic Activity of Carbon-Supported Pt Nanoelectrocatalysts. Why Reducing the Size of Pt Nanoparticles is Not Always Beneficial\",\"volume\":\"115\",\"issn\":\"1932-7447\",\"url\":\"https://doi.org/10.1021/jp1109477\",\"doi\":\"10.1021/jp1109477\",\"abstract\":\"Carbon-supported Pt catalysts prepared by the impregnation method in water−dimethyl sulfoxide (DMSO) solutions were investigated. Using X-ray diffraction (XRD) technique for estimation of the particle size and shapes, we show that morphology of the Pt/C catalysts depends strongly on the DMSO content in the solutions. The average particles size reduces and a shape of the Pt nanocrystals changes from a truncated octahedron to a cuboctahedron and eventually to a truncated cube with increasing DMSO concentration in the reaction mixture. Antibate effects of the size and shape cause nonmonotonic dependence of the catalytic activity for the oxygen reduction reaction (ORR) with electric current maximum at an average particle size of 2.7 nm.\",\"number\":\"13\",\"urldate\":\"2023-11-11\",\"journal\":\"The Journal of Physical Chemistry C\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Belenov\"],\"firstnames\":[\"S.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Guterman\"],\"firstnames\":[\"V.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Haghi-Ashtiani\"],\"firstnames\":[\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shaganov\"],\"firstnames\":[\"A.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dkhil\"],\"firstnames\":[\"B.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2011\",\"note\":\"Publisher: American Chemical Society\",\"pages\":\"5429–5434\",\"bibtex\":\"@article{leontyev_catalytic_2011,\\n\\ttitle = {Catalytic {Activity} of {Carbon}-{Supported} {Pt} {Nanoelectrocatalysts}. {Why} {Reducing} the {Size} of {Pt} {Nanoparticles} is {Not} {Always} {Beneficial}},\\n\\tvolume = {115},\\n\\tissn = {1932-7447},\\n\\turl = {https://doi.org/10.1021/jp1109477},\\n\\tdoi = {10.1021/jp1109477},\\n\\tabstract = {Carbon-supported Pt catalysts prepared by the impregnation method in water−dimethyl sulfoxide (DMSO) solutions were investigated. Using X-ray diffraction (XRD) technique for estimation of the particle size and shapes, we show that morphology of the Pt/C catalysts depends strongly on the DMSO content in the solutions. The average particles size reduces and a shape of the Pt nanocrystals changes from a truncated octahedron to a cuboctahedron and eventually to a truncated cube with increasing DMSO concentration in the reaction mixture. Antibate effects of the size and shape cause nonmonotonic dependence of the catalytic activity for the oxygen reduction reaction (ORR) with electric current maximum at an average particle size of 2.7 nm.},\\n\\tnumber = {13},\\n\\turldate = {2023-11-11},\\n\\tjournal = {The Journal of Physical Chemistry C},\\n\\tauthor = {Leontyev, I. N. and Belenov, S. V. and Guterman, V. E. and Haghi-Ashtiani, P. and Shaganov, A. P. and Dkhil, B.},\\n\\tmonth = apr,\\n\\tyear = {2011},\\n\\tnote = {Publisher: American Chemical Society},\\n\\tpages = {5429--5434},\\n}\\n\\n\",\"author_short\":[\"Leontyev, I. N.\",\"Belenov, S. V.\",\"Guterman, V. E.\",\"Haghi-Ashtiani, P.\",\"Shaganov, A. P.\",\"Dkhil, B.\"],\"key\":\"leontyev_catalytic_2011\",\"id\":\"leontyev_catalytic_2011\",\"bibbaseid\":\"leontyev-belenov-guterman-haghiashtiani-shaganov-dkhil-catalyticactivityofcarbonsupportedptnanoelectrocatalystswhyreducingthesizeofptnanoparticlesisnotalwaysbeneficial-2011\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1021/jp1109477\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Наноразмерные сегнетоэлектрические пленки Ba$_{\\\\textrm{0.8}}$Sr$_{\\\\textrm{0.2}}$TiO$_{\\\\textrm{3}}$ на подложках MgO\",\"volume\":\"12\",\"issn\":\"1999-8465\",\"url\":\"https://www.elibrary.ru/item.asp?id=16220258\",\"abstract\":\"Методом просвечивающей электронной микроскопии высокого разрешения проведены исследования и анализ дефектной микроструктуры монокристаллических сегнетоэлектрических наноразмерных пленок Ba0.8Sr0.2TiO3, выращенных методом магнетронного распыления мишени на подложках MgO. Выявлено в пленке наличие дислокаций с векторами Бюргерса \\\\textless100\\\\textgreaterи 1/2\\\\textless110\\\\textgreater и границы блоков.\",\"language\":\"ru\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Наукоемкие Технологии\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Жигалина\"],\"firstnames\":[\"О.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Чувилин\"],\"firstnames\":[\"A.\",\"Л.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кускова\"],\"firstnames\":[\"А.\",\"Н.\"],\"suffixes\":[]}],\"year\":\"2011\",\"keywords\":\"Тонкие Сегнетоэлектрические Пленки, Электронная Микроскопия Высокого Разрешения\",\"pages\":\"23–25\",\"bibtex\":\"@article{__2011-2,\\n\\ttitle = {Наноразмерные сегнетоэлектрические пленки {Ba}$_{\\\\textrm{0.8}}${Sr}$_{\\\\textrm{0.2}}${TiO}$_{\\\\textrm{3}}$ на подложках {MgO}},\\n\\tvolume = {12},\\n\\tissn = {1999-8465},\\n\\turl = {https://www.elibrary.ru/item.asp?id=16220258},\\n\\tabstract = {Методом просвечивающей электронной микроскопии высокого разрешения проведены исследования и анализ дефектной микроструктуры монокристаллических сегнетоэлектрических наноразмерных пленок Ba0.8Sr0.2TiO3, выращенных методом магнетронного распыления мишени на подложках MgO. Выявлено в пленке наличие дислокаций с векторами Бюргерса {\\\\textless}100{\\\\textgreater}и 1/2{\\\\textless}110{\\\\textgreater} и границы блоков.},\\n\\tlanguage = {ru},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Наукоемкие Технологии},\\n\\tauthor = {Жигалина, О. М. and Мухортов, В. М. and Головко, Ю. И. and Чувилин, A. Л. and Кускова, А. Н.},\\n\\tyear = {2011},\\n\\tkeywords = {Тонкие Сегнетоэлектрические Пленки, Электронная Микроскопия Высокого Разрешения},\\n\\tpages = {23--25},\\n}\\n\\n\",\"author_short\":[\"Жигалина, О. М.\",\"Мухортов, В. М.\",\"Головко, Ю. И.\",\"Чувилин, A. Л.\",\"Кускова, А. Н.\"],\"key\":\"__2011-2\",\"id\":\"__2011-2\",\"bibbaseid\":\"-----batextrm08srtextrm02tiotextrm3mgo-2011\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.elibrary.ru/item.asp?id=16220258\"},\"keyword\":[\"Тонкие Сегнетоэлектрические Пленки\",\"Электронная Микроскопия Высокого Разрешения\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Coherent optical phonons of ZnO under near resonant photoexcitation\",\"volume\":\"22\",\"issn\":\"0953-8984\",\"url\":\"https://dx.doi.org/10.1088/0953-8984/22/46/465803\",\"doi\":\"10.1088/0953-8984/22/46/465803\",\"abstract\":\"Ultrafast electron–phonon coupling dynamics in ZnO are investigated by degenerate pump–probe reflectivity measurements using near resonant 400 nm light. Because of the below-gap excitation, photocarriers are excited primarily from deep levels of intrinsic point defects. At least six coherent phonon modes, including two E2 modes and their combination, longitudinal optical (LO) mode and its overtone (2LO), are observed. Unlike the previous resonant Raman studies using 325 nm light, the intensity of the polar LO phonons is only moderately enhanced by the Fröhlich interaction. The non-polar E2 phonons decay considerably faster than under visible excitation, indicative of strong deformation potential interaction with photocarriers. The overdamped oscillation centered at around 20 THz is tentatively attributed to the upper branch of the plasmon–phonon coupled mode. The pump-polarization dependence of the phonon amplitudes is consistent with the impulsive Raman generation.\",\"language\":\"en\",\"number\":\"46\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics: Condensed Matter\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Ishioka\"],\"firstnames\":[\"K.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Petek\"],\"firstnames\":[\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaydashev\"],\"firstnames\":[\"V.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Misochko\"],\"firstnames\":[\"O.\",\"V.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2010\",\"pages\":\"465803\",\"bibtex\":\"@article{ishioka_coherent_2010,\\n\\ttitle = {Coherent optical phonons of {ZnO} under near resonant photoexcitation},\\n\\tvolume = {22},\\n\\tissn = {0953-8984},\\n\\turl = {https://dx.doi.org/10.1088/0953-8984/22/46/465803},\\n\\tdoi = {10.1088/0953-8984/22/46/465803},\\n\\tabstract = {Ultrafast electron–phonon coupling dynamics in ZnO are investigated by degenerate pump–probe reflectivity measurements using near resonant 400 nm light. Because of the below-gap excitation, photocarriers are excited primarily from deep levels of intrinsic point defects. At least six coherent phonon modes, including two E2 modes and their combination, longitudinal optical (LO) mode and its overtone (2LO), are observed. Unlike the previous resonant Raman studies using 325 nm light, the intensity of the polar LO phonons is only moderately enhanced by the Fröhlich interaction. The non-polar E2 phonons decay considerably faster than under visible excitation, indicative of strong deformation potential interaction with photocarriers. The overdamped oscillation centered at around 20 THz is tentatively attributed to the upper branch of the plasmon–phonon coupled mode. The pump-polarization dependence of the phonon amplitudes is consistent with the impulsive Raman generation.},\\n\\tlanguage = {en},\\n\\tnumber = {46},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics: Condensed Matter},\\n\\tauthor = {Ishioka, K. and Petek, H. and Kaydashev, V. E. and Kaidashev, E. M. and Misochko, O. V.},\\n\\tmonth = nov,\\n\\tyear = {2010},\\n\\tpages = {465803},\\n}\\n\\n\",\"author_short\":[\"Ishioka, K.\",\"Petek, H.\",\"Kaydashev, V. E.\",\"Kaidashev, E. M.\",\"Misochko, O. V.\"],\"key\":\"ishioka_coherent_2010\",\"id\":\"ishioka_coherent_2010\",\"bibbaseid\":\"ishioka-petek-kaydashev-kaidashev-misochko-coherentopticalphononsofznoundernearresonantphotoexcitation-2010\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/0953-8984/22/46/465803\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Long-Range Protein Coupling Mediated by Critical Low-Energy Modes of Tubular Lipid Membranes\",\"volume\":\"105\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevLett.105.028102\",\"doi\":\"10.1103/PhysRevLett.105.028102\",\"abstract\":\"We develop a theory of a resonant effect in protein-membrane coupling taking place in the vicinity of instabilities in tubular lipid membranes (TLMs) under longitudinal force and pressure difference constraints. Two critical low-energy modes defining the stability domain boundaries are found. We show that these modes mediate long-range TLM-protein coupling and interactions between absorbed proteins. Besides, TLM mechanical instabilities strongly influence protein desorption and protein cluster nucleation on TLMs. Model predictions can be tested over a large spectrum of mechanochemical conditions.\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Monnier\"],\"firstnames\":[\"Sylvain\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergei\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Parmeggiani\"],\"firstnames\":[\"Andrea\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorman\"],\"firstnames\":[\"Vladimir\",\"L.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2010\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"028102\",\"file\":\"APS Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\22HMBNIH\\\\¶hysRevLett.105.html:text/html\",\"bibtex\":\"@article{monnier_long-range_2010,\\n\\ttitle = {Long-{Range} {Protein} {Coupling} {Mediated} by {Critical} {Low}-{Energy} {Modes} of {Tubular} {Lipid} {Membranes}},\\n\\tvolume = {105},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevLett.105.028102},\\n\\tdoi = {10.1103/PhysRevLett.105.028102},\\n\\tabstract = {We develop a theory of a resonant effect in protein-membrane coupling taking place in the vicinity of instabilities in tubular lipid membranes (TLMs) under longitudinal force and pressure difference constraints. Two critical low-energy modes defining the stability domain boundaries are found. We show that these modes mediate long-range TLM-protein coupling and interactions between absorbed proteins. Besides, TLM mechanical instabilities strongly influence protein desorption and protein cluster nucleation on TLMs. Model predictions can be tested over a large spectrum of mechanochemical conditions.},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review Letters},\\n\\tauthor = {Monnier, Sylvain and Rochal, Sergei B. and Parmeggiani, Andrea and Lorman, Vladimir L.},\\n\\tmonth = jul,\\n\\tyear = {2010},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {028102},\\n\\tfile = {APS Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\22HMBNIH\\\\\\\\PhysRevLett.105.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Monnier, S.\",\"Rochal, S. B.\",\"Parmeggiani, A.\",\"Lorman, V. L.\"],\"key\":\"monnier_long-range_2010\",\"id\":\"monnier_long-range_2010\",\"bibbaseid\":\"monnier-rochal-parmeggiani-lorman-longrangeproteincouplingmediatedbycriticallowenergymodesoftubularlipidmembranes-2010\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevLett.105.028102\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Спектры комбинационного рассеяния углеродного наноматериала \\\"Таунит\\\"\",\"volume\":\"5\",\"issn\":\"1992-7223, 1993-4068\",\"url\":\"https://www.elibrary.ru/item.asp?id=15271362\",\"abstract\":\"Изучены спектры комбинационного рассеяния света (КРС) образцов углеродного наноматериала (УНМ) «Таунит», отожженных при различных температурах. Кроме того, исследовалось влияние наночастиц катализатора Pt с размерами 3-6 нм на спектры КРС УНМ «Таунит». Было обнаружено, что «Таунит» относится к углеродным материалам с нарушенной степенью организации, однако с ростом температуры отжига наблюдалось упорядочение его кристаллической структуры. Показано, что осаждение частиц платинового катализатора на поверхность УНМ «Таунит» приводит к увеличению интенсивности дефектной полосы в спектрах КРС из-за появления некоторого количества дефектов кристаллической решеткиRaman spectra of carbonaceous nanomaterial (CNM) «Taunit» samples annealed at different temperatures were studied. Also influence Pt-catalyst nanoparticles with the size distribution 3-6 nm on the Raman spectra of CNM «Taunit» was studied. It was found that «Taunit» belonged to poorly organized CNM but the its crystalline structure ordering was observed with increasing of annealing temperature. It is shown that Pt-catalyst precipitation on the surface of CNM «Taunit» leads to increasing of the defect band intensity due to appearance of some crystal lattice defects.\",\"language\":\"ru\",\"number\":\"9-10\",\"urldate\":\"2023-11-11\",\"journal\":\"Российские Нанотехнологии\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Маслова\"],\"firstnames\":[\"О.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Михейкин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Леонтьев\"],\"firstnames\":[\"И.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ткачев\"],\"firstnames\":[\"А.\",\"Г.\"],\"suffixes\":[]}],\"year\":\"2010\",\"pages\":\"89–93\",\"bibtex\":\"@article{__2010,\\n\\ttitle = {Спектры комбинационного рассеяния углеродного наноматериала \\\"Таунит\\\"},\\n\\tvolume = {5},\\n\\tissn = {1992-7223, 1993-4068},\\n\\turl = {https://www.elibrary.ru/item.asp?id=15271362},\\n\\tabstract = {Изучены спектры комбинационного рассеяния света (КРС) образцов углеродного наноматериала (УНМ) «Таунит», отожженных при различных температурах. Кроме того, исследовалось влияние наночастиц катализатора Pt с размерами 3-6 нм на спектры КРС УНМ «Таунит». Было обнаружено, что «Таунит» относится к углеродным материалам с нарушенной степенью организации, однако с ростом температуры отжига наблюдалось упорядочение его кристаллической структуры. Показано, что осаждение частиц платинового катализатора на поверхность УНМ «Таунит» приводит к увеличению интенсивности дефектной полосы в спектрах КРС из-за появления некоторого количества дефектов кристаллической решеткиRaman spectra of carbonaceous nanomaterial (CNM) «Taunit» samples annealed at different temperatures were studied. Also influence Pt-catalyst nanoparticles with the size distribution 3-6 nm on the Raman spectra of CNM «Taunit» was studied. It was found that «Taunit» belonged to poorly organized CNM but the its crystalline structure ordering was observed with increasing of annealing temperature. It is shown that Pt-catalyst precipitation on the surface of CNM «Taunit» leads to increasing of the defect band intensity due to appearance of some crystal lattice defects.},\\n\\tlanguage = {ru},\\n\\tnumber = {9-10},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Российские Нанотехнологии},\\n\\tauthor = {Маслова, О. А. and Михейкин, А. С. and Леонтьев, И. Н. and Юзюк, Ю. И. and Ткачев, А. Г.},\\n\\tyear = {2010},\\n\\tpages = {89--93},\\n}\\n\\n\",\"author_short\":[\"Маслова, О. А.\",\"Михейкин, А. С.\",\"Леонтьев, И. Н.\",\"Юзюк, Ю. И.\",\"Ткачев, А. Г.\"],\"key\":\"__2010\",\"id\":\"__2010\",\"bibbaseid\":\"------2010\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.elibrary.ru/item.asp?id=15271362\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"XRD and electrochemical investigation of particle size effects in platinum-cobalt cathode electrocatalysts for oxygen reduction\",\"volume\":\"500\",\"issn\":\"0925-8388\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0925838810008091\",\"doi\":\"10.1016/j.jallcom.2010.04.018\",\"abstract\":\"Pt-Co/C electrocatalysts with Pt loadings close to 30wt.% prepared by the impregnation method in water–ethylene glycol solutions were investigated by X-ray diffraction and correlated with electrochemical measurements. We show that composition of the binary solvent controls the average particle size and its distribution. The unit cell parameter of the Pt3Co alloy decreases nonlinearly with decreasing particle size. The ORR activity of the prepared Pt-Co/C catalysts in H2SO4 solution enhances with decreasing particle size and unit cell parameter as well as with narrowing of the particle size distribution. Corrosion treatment of the synthesized Pt-Co/C materials brings about an increase of ca. 1nm in the average grain size accompanied by broadening of the grain size distribution and a decrease in the Co content. All of the synthesized Pt-Co/C materials show higher ORR activities compared with commercial Pt/C electrocatalysts.\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Alloys and Compounds\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Guterman\"],\"firstnames\":[\"V.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pakhomova\"],\"firstnames\":[\"E.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]},{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"A.V.Guterman\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zakharchenko\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Petin\"],\"firstnames\":[\"G.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dkhil\"],\"firstnames\":[\"B.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2010\",\"keywords\":\"Grain size distribution, Electrocatalysis, Oxygen reduction reaction (ORR), Platinum alloy, X-ray diffraction (XRD)\",\"pages\":\"241–246\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\RVNSSP3Z\\\\Łeontyev и др. - 2010 - XRD and electrochemical investigation of particle .pdf:application/pdf;ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\VESEAEDH\\\\§0925838810008091.html:text/html\",\"bibtex\":\"@article{leontyev_xrd_2010,\\n\\ttitle = {{XRD} and electrochemical investigation of particle size effects in platinum-cobalt cathode electrocatalysts for oxygen reduction},\\n\\tvolume = {500},\\n\\tissn = {0925-8388},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0925838810008091},\\n\\tdoi = {10.1016/j.jallcom.2010.04.018},\\n\\tabstract = {Pt-Co/C electrocatalysts with Pt loadings close to 30wt.\\\\% prepared by the impregnation method in water–ethylene glycol solutions were investigated by X-ray diffraction and correlated with electrochemical measurements. We show that composition of the binary solvent controls the average particle size and its distribution. The unit cell parameter of the Pt3Co alloy decreases nonlinearly with decreasing particle size. The ORR activity of the prepared Pt-Co/C catalysts in H2SO4 solution enhances with decreasing particle size and unit cell parameter as well as with narrowing of the particle size distribution. Corrosion treatment of the synthesized Pt-Co/C materials brings about an increase of ca. 1nm in the average grain size accompanied by broadening of the grain size distribution and a decrease in the Co content. All of the synthesized Pt-Co/C materials show higher ORR activities compared with commercial Pt/C electrocatalysts.},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Alloys and Compounds},\\n\\tauthor = {Leontyev, I. N. and Guterman, V. E. and Pakhomova, E. B. and Timoshenko, P. E. and {A.V.Guterman} and Zakharchenko, I. N. and Petin, G. P. and Dkhil, B.},\\n\\tmonth = jun,\\n\\tyear = {2010},\\n\\tkeywords = {Grain size distribution, Electrocatalysis, Oxygen reduction reaction (ORR), Platinum alloy, X-ray diffraction (XRD)},\\n\\tpages = {241--246},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\RVNSSP3Z\\\\\\\\Leontyev и др. - 2010 - XRD and electrochemical investigation of particle .pdf:application/pdf;ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\VESEAEDH\\\\\\\\S0925838810008091.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Leontyev, I. N.\",\"Guterman, V. E.\",\"Pakhomova, E. B.\",\"Timoshenko, P. E.\",\"A.V.Guterman\",\"Zakharchenko, I. N.\",\"Petin, G. P.\",\"Dkhil, B.\"],\"key\":\"leontyev_xrd_2010\",\"id\":\"leontyev_xrd_2010\",\"bibbaseid\":\"leontyev-guterman-pakhomova-timoshenko-avguterman-zakharchenko-petin-dkhil-xrdandelectrochemicalinvestigationofparticlesizeeffectsinplatinumcobaltcathodeelectrocatalystsforoxygenreduction-2010\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0925838810008091\"},\"keyword\":[\"Grain size distribution\",\"Electrocatalysis\",\"Oxygen reduction reaction (ORR)\",\"Platinum alloy\",\"X-ray diffraction (XRD)\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Self-organized growth of ZnO-based nano- and microstructures\",\"volume\":\"247\",\"copyright\":\"Copyright © 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim\",\"issn\":\"1521-3951\",\"url\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.200945514\",\"doi\":\"10.1002/pssb.200945514\",\"abstract\":\"ZnO-based nano- and micro-structures with controlled orientation, size, and lateral density were grown by specially designed two-step pulsed laser deposition and direct carbothermal growth, respectively. Different substrate orientations and nucleation layers allow well-defined tuning of growth direction and lateral arrangement of the wires. As a result, axial MgZnOZnO nano quantum dots and homogeneous radial nano core-shell quantum well structures are demonstrated. Donor and acceptor doping of nano- and microwires influence considerably both electrical characteristics as well as morphology including branching. Field effect transistors with n- and p-type wire channel and nanowire p–n junctions seem to prove a reproducible p-type conductivity of phosphorous-doped ZnO wires. Single ZnO wire (309 nm thick, 3.99 µm high) grown on pyramidal base with controlled lateral density by tuning the ZnO template layer in a two-step PLD process.\",\"language\":\"en\",\"number\":\"6\",\"urldate\":\"2023-11-11\",\"journal\":\"physica status solidi (b)\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"Michael\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rahm\"],\"firstnames\":[\"Andreas\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Cao\"],\"firstnames\":[\"Bingqiang\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zúñiga-Pérez\"],\"firstnames\":[\"Jesús\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"Evgeni\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhakarov\"],\"firstnames\":[\"Nikolai\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Wagner\"],\"firstnames\":[\"Gerald\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nobis\"],\"firstnames\":[\"Thomas\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Czekalla\"],\"firstnames\":[\"Christian\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zimmermann\"],\"firstnames\":[\"Gregor\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"Marius\"],\"suffixes\":[]}],\"year\":\"2010\",\"note\":\"_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.200945514\",\"keywords\":\"72.80.Ey, 73.21.Fg, 78.67.Bf, 81.05.Dz, 81.16.Dn, 81.16.Mk\",\"pages\":\"1265–1281\",\"file\":\"Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\6WSS5J7I\\\\\\\\pssb.html:text/html\",\"bibtex\":\"@article{lorenz_self-organized_2010,\\n\\ttitle = {Self-organized growth of {ZnO}-based nano- and microstructures},\\n\\tvolume = {247},\\n\\tcopyright = {Copyright © 2010 WILEY-VCH Verlag GmbH \\\\& Co. KGaA, Weinheim},\\n\\tissn = {1521-3951},\\n\\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.200945514},\\n\\tdoi = {10.1002/pssb.200945514},\\n\\tabstract = {ZnO-based nano- and micro-structures with controlled orientation, size, and lateral density were grown by specially designed two-step pulsed laser deposition and direct carbothermal growth, respectively. Different substrate orientations and nucleation layers allow well-defined tuning of growth direction and lateral arrangement of the wires. As a result, axial MgZnOZnO nano quantum dots and homogeneous radial nano core-shell quantum well structures are demonstrated. Donor and acceptor doping of nano- and microwires influence considerably both electrical characteristics as well as morphology including branching. Field effect transistors with n- and p-type wire channel and nanowire p–n junctions seem to prove a reproducible p-type conductivity of phosphorous-doped ZnO wires. Single ZnO wire (309 nm thick, 3.99 µm high) grown on pyramidal base with controlled lateral density by tuning the ZnO template layer in a two-step PLD process.},\\n\\tlanguage = {en},\\n\\tnumber = {6},\\n\\turldate = {2023-11-11},\\n\\tjournal = {physica status solidi (b)},\\n\\tauthor = {Lorenz, Michael and Rahm, Andreas and Cao, Bingqiang and Zúñiga-Pérez, Jesús and Kaidashev, Evgeni M. and Zhakarov, Nikolai and Wagner, Gerald and Nobis, Thomas and Czekalla, Christian and Zimmermann, Gregor and Grundmann, Marius},\\n\\tyear = {2010},\\n\\tnote = {\\\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.200945514},\\n\\tkeywords = {72.80.Ey, 73.21.Fg, 78.67.Bf, 81.05.Dz, 81.16.Dn, 81.16.Mk},\\n\\tpages = {1265--1281},\\n\\tfile = {Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\6WSS5J7I\\\\\\\\pssb.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Lorenz, M.\",\"Rahm, A.\",\"Cao, B.\",\"Zúñiga-Pérez, J.\",\"Kaidashev, E. M.\",\"Zhakarov, N.\",\"Wagner, G.\",\"Nobis, T.\",\"Czekalla, C.\",\"Zimmermann, G.\",\"Grundmann, M.\"],\"key\":\"lorenz_self-organized_2010\",\"id\":\"lorenz_self-organized_2010\",\"bibbaseid\":\"lorenz-rahm-cao-zigaprez-kaidashev-zhakarov-wagner-nobis-etal-selforganizedgrowthofznobasednanoandmicrostructures-2010\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.200945514\"},\"keyword\":[\"72.80.Ey\",\"73.21.Fg\",\"78.67.Bf\",\"81.05.Dz\",\"81.16.Dn\",\"81.16.Mk\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Impedance of the microstrip line for magnetostatic backward volume waves\",\"volume\":\"52\",\"issn\":\"1573-9120\",\"url\":\"https://doi.org/10.1007/s11141-010-9197-9\",\"doi\":\"10.1007/s11141-010-9197-9\",\"abstract\":\"We study excitation of magnetostatic backward volume waves on the microstrip line. The relation between the current density in the line and the normal component of the magnetic induction is found. The impedance of the line per unit length, i.e., its reactance and radiation resistance per unit length, is represented as a functional of the current density. The dependence of the operating-wave radiation resistance on the transverse size of the line and the width of the dielectric gap is studied. The radiation resistances of multistrip array and meander-type converters of magnetostatic backward volume waves are calculated\",\"language\":\"en\",\"number\":\"12\",\"urldate\":\"2023-11-11\",\"journal\":\"Radiophysics and Quantum Electronics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Babicheva\"],\"firstnames\":[\"E.\",\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ivanov\"],\"firstnames\":[\"V.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zubkov\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2009\",\"keywords\":\"Ferrite, Frequency Dependence, Radiation Resistance, Side Lobe, Unit Length\",\"pages\":\"892–899\",\"bibtex\":\"@article{timoshenko_impedance_2009,\\n\\ttitle = {Impedance of the microstrip line for magnetostatic backward volume waves},\\n\\tvolume = {52},\\n\\tissn = {1573-9120},\\n\\turl = {https://doi.org/10.1007/s11141-010-9197-9},\\n\\tdoi = {10.1007/s11141-010-9197-9},\\n\\tabstract = {We study excitation of magnetostatic backward volume waves on the microstrip line. The relation between the current density in the line and the normal component of the magnetic induction is found. The impedance of the line per unit length, i.e., its reactance and radiation resistance per unit length, is represented as a functional of the current density. The dependence of the operating-wave radiation resistance on the transverse size of the line and the width of the dielectric gap is studied. The radiation resistances of multistrip array and meander-type converters of magnetostatic backward volume waves are calculated},\\n\\tlanguage = {en},\\n\\tnumber = {12},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Radiophysics and Quantum Electronics},\\n\\tauthor = {Timoshenko, P. E. and Babicheva, E. R. and Ivanov, V. N. and Zubkov, V. I.},\\n\\tmonth = dec,\\n\\tyear = {2009},\\n\\tkeywords = {Ferrite, Frequency Dependence, Radiation Resistance, Side Lobe, Unit Length},\\n\\tpages = {892--899},\\n}\\n\\n\",\"author_short\":[\"Timoshenko, P. E.\",\"Babicheva, E. R.\",\"Ivanov, V. N.\",\"Zubkov, V. I.\"],\"key\":\"timoshenko_impedance_2009\",\"id\":\"timoshenko_impedance_2009\",\"bibbaseid\":\"timoshenko-babicheva-ivanov-zubkov-impedanceofthemicrostriplineformagnetostaticbackwardvolumewaves-2009\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1007/s11141-010-9197-9\"},\"keyword\":[\"Ferrite\",\"Frequency Dependence\",\"Radiation Resistance\",\"Side Lobe\",\"Unit Length\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Theory of a reconstructive structural transformation in capsids of icosahedral viruses\",\"volume\":\"80\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevE.80.051905\",\"doi\":\"10.1103/PhysRevE.80.051905\",\"abstract\":\"A theory of a reconstructive structural transformation in icosahedral capsid shells is developed for a whole family of virulent human viruses. It is shown that the reversible rearrangement of proteins during the virus maturation transformation is driven by the variation in the wave number l associated with the protein density distribution function. The collective displacement field of protein centers from their positions in the initial (procapsid) and the final (capsid) two-dimensional icosahderal structures is derived. The amplitude of the displacement field is shown to be small and it minimizes the calculated free energy of the transformation. The theory allows us to propose a continuous thermodynamical mechanism of the reconstructive procapsid-to-capsid transformation. In the frame of the density-wave approach, we also propose to take an equivalent plane-wave vector as a common structural feature for different icosahedral capsid shells formed by the same proteins. Using these characteristics, we explain the relation between the radii of the procapsid and capsid shells and generalize it to the case of the viral capsid polymorphism.\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review E\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorman\"],\"firstnames\":[\"V.\",\"L.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2009\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"051905\",\"bibtex\":\"@article{rochal_theory_2009,\\n\\ttitle = {Theory of a reconstructive structural transformation in capsids of icosahedral viruses},\\n\\tvolume = {80},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevE.80.051905},\\n\\tdoi = {10.1103/PhysRevE.80.051905},\\n\\tabstract = {A theory of a reconstructive structural transformation in icosahedral capsid shells is developed for a whole family of virulent human viruses. It is shown that the reversible rearrangement of proteins during the virus maturation transformation is driven by the variation in the wave number l associated with the protein density distribution function. The collective displacement field of protein centers from their positions in the initial (procapsid) and the final (capsid) two-dimensional icosahderal structures is derived. The amplitude of the displacement field is shown to be small and it minimizes the calculated free energy of the transformation. The theory allows us to propose a continuous thermodynamical mechanism of the reconstructive procapsid-to-capsid transformation. In the frame of the density-wave approach, we also propose to take an equivalent plane-wave vector as a common structural feature for different icosahedral capsid shells formed by the same proteins. Using these characteristics, we explain the relation between the radii of the procapsid and capsid shells and generalize it to the case of the viral capsid polymorphism.},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review E},\\n\\tauthor = {Rochal, S. B. and Lorman, V. L.},\\n\\tmonth = nov,\\n\\tyear = {2009},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {051905},\\n}\\n\\n\",\"author_short\":[\"Rochal, S. B.\",\"Lorman, V. L.\"],\"key\":\"rochal_theory_2009\",\"id\":\"rochal_theory_2009\",\"bibbaseid\":\"rochal-lorman-theoryofareconstructivestructuraltransformationincapsidsoficosahedralviruses-2009\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevE.80.051905\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Particle size effect in carbon supported Pt–Co alloy electrocatalysts prepared by the borohydride method: XRD characterization\",\"volume\":\"357\",\"issn\":\"0926-860X\",\"shorttitle\":\"Particle size effect in carbon supported Pt–Co alloy electrocatalysts prepared by the borohydride method\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0926860X08007874\",\"doi\":\"10.1016/j.apcata.2008.12.023\",\"abstract\":\"Pt3Co/C electrocatalysts prepared by wet synthesis method from water–ethylene glycol solutions of Pt and Co precursors were investigated by X-ray diffraction in conjunction with electrochemical measurements. It was shown that varying the binary solvent composition is an effective means of control over the average nanoparticle size and the grain size distribution. It was found that unit cell parameter of the Pt3Co/C electrocatalysts decreases nonlinearly with decreasing particle size. The activity of the prepared Pt3Co/C catalysts for the oxygen reduction reaction (ORR) in H2SO4 solution enhances with decrease in the particle size, the unit cell parameter, and the dispersion of the grain size distribution. All samples studied show higher catalytic activities in comparison with the commercial Pt/C materials.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Applied Catalysis A: General\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chernyshov\"],\"firstnames\":[\"D.\",\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Guterman\"],\"firstnames\":[\"V.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pakhomova\"],\"firstnames\":[\"E.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Guterman\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2009\",\"keywords\":\"X-ray diffraction, Grain size distribution, Oxygen reduction, Pt–Co alloy, Size effects\",\"pages\":\"1–4\",\"file\":\"ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\356CZ2CX\\\\§0926860X08007874.html:text/html\",\"bibtex\":\"@article{leontyev_particle_2009,\\n\\ttitle = {Particle size effect in carbon supported {Pt}–{Co} alloy electrocatalysts prepared by the borohydride method: {XRD} characterization},\\n\\tvolume = {357},\\n\\tissn = {0926-860X},\\n\\tshorttitle = {Particle size effect in carbon supported {Pt}–{Co} alloy electrocatalysts prepared by the borohydride method},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0926860X08007874},\\n\\tdoi = {10.1016/j.apcata.2008.12.023},\\n\\tabstract = {Pt3Co/C electrocatalysts prepared by wet synthesis method from water–ethylene glycol solutions of Pt and Co precursors were investigated by X-ray diffraction in conjunction with electrochemical measurements. It was shown that varying the binary solvent composition is an effective means of control over the average nanoparticle size and the grain size distribution. It was found that unit cell parameter of the Pt3Co/C electrocatalysts decreases nonlinearly with decreasing particle size. The activity of the prepared Pt3Co/C catalysts for the oxygen reduction reaction (ORR) in H2SO4 solution enhances with decrease in the particle size, the unit cell parameter, and the dispersion of the grain size distribution. All samples studied show higher catalytic activities in comparison with the commercial Pt/C materials.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Applied Catalysis A: General},\\n\\tauthor = {Leontyev, I. N. and Chernyshov, D. Yu. and Guterman, V. E. and Pakhomova, E. V. and Guterman, A. V.},\\n\\tmonth = mar,\\n\\tyear = {2009},\\n\\tkeywords = {X-ray diffraction, Grain size distribution, Oxygen reduction, Pt–Co alloy, Size effects},\\n\\tpages = {1--4},\\n\\tfile = {ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\356CZ2CX\\\\\\\\S0926860X08007874.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Leontyev, I. N.\",\"Chernyshov, D. Y.\",\"Guterman, V. E.\",\"Pakhomova, E. V.\",\"Guterman, A. V.\"],\"key\":\"leontyev_particle_2009\",\"id\":\"leontyev_particle_2009\",\"bibbaseid\":\"leontyev-chernyshov-guterman-pakhomova-guterman-particlesizeeffectincarbonsupportedptcoalloyelectrocatalystspreparedbytheborohydridemethodxrdcharacterization-2009\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0926860X08007874\"},\"keyword\":[\"X-ray diffraction\",\"Grain size distribution\",\"Oxygen reduction\",\"Pt–Co alloy\",\"Size effects\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Topological Control of Life and Death in Non-Proliferative Epithelia\",\"volume\":\"4\",\"issn\":\"1932-6203\",\"url\":\"https://journals.plos.org/plosone/article?id=10.1371/journal.pone.0004202\",\"doi\":\"10.1371/journal.pone.0004202\",\"abstract\":\"Programmed cell death is one of the most fascinating demonstrations of the plasticity of biological systems. It is classically described to act upstream of and govern major developmental patterning processes (e.g. inter-digitations in vertebrates, ommatidia in Drosophila). We show here the first evidence that massive apoptosis can also be controlled and coordinated by a pre-established pattern of a specific ‘master cell’ population. This new concept is supported by the development and validation of an original model of cell patterning. Ciona intestinalis eggs are surrounded by a three-layered follicular organization composed of 60 elongated floating extensions made of as many outer and inner cells, and indirectly spread through an extracellular matrix over 1200 test cells. Experimental and selective ablation of outer and inner cells results in the abrogation of apoptosis in respective remaining neighbouring test cells. In addition incubation of outer/inner follicular cell-depleted eggs with a soluble extract of apoptotic outer/inner cells partially restores apoptosis to apoptotic-defective test cells. The 60 inner follicular cells were thus identified as ‘apoptotic master’ cells which collectively are induction sites for programmed cell death of the underlying test cells. The position of apoptotic master cells is controlled by topological constraints exhibiting a tetrahedral symmetry, and each cell spreads over and can control the destiny of 20 smaller test cells, which leads to optimized apoptosis signalling.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"PLOS ONE\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Martinand-Mari\"],\"firstnames\":[\"Camille\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maury\"],\"firstnames\":[\"Benoit\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rousset\"],\"firstnames\":[\"François\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sahuquet\"],\"firstnames\":[\"Alain\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mennessier\"],\"firstnames\":[\"Gérard\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergei\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorman\"],\"firstnames\":[\"Vladimir\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mangeat\"],\"firstnames\":[\"Paul\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Baghdiguian\"],\"firstnames\":[\"Stephen\"],\"suffixes\":[]}],\"year\":\"2009\",\"note\":\"Publisher: Public Library of Science\",\"keywords\":\"Apoptosis, Apoptotic signaling cascade, Chorion, Ciona intestinalis, Eggs, Fertilization, Ova, Symmetry\",\"pages\":\"e4202\",\"file\":\"Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\U26F6JVM\\\\\\\\Martinand-Mari и др. - 2009 - Topological Control of Life and Death in Non-Proli.pdf:application/pdf\",\"bibtex\":\"@article{martinand-mari_topological_2009,\\n\\ttitle = {Topological {Control} of {Life} and {Death} in {Non}-{Proliferative} {Epithelia}},\\n\\tvolume = {4},\\n\\tissn = {1932-6203},\\n\\turl = {https://journals.plos.org/plosone/article?id=10.1371/journal.pone.0004202},\\n\\tdoi = {10.1371/journal.pone.0004202},\\n\\tabstract = {Programmed cell death is one of the most fascinating demonstrations of the plasticity of biological systems. It is classically described to act upstream of and govern major developmental patterning processes (e.g. inter-digitations in vertebrates, ommatidia in Drosophila). We show here the first evidence that massive apoptosis can also be controlled and coordinated by a pre-established pattern of a specific ‘master cell’ population. This new concept is supported by the development and validation of an original model of cell patterning. Ciona intestinalis eggs are surrounded by a three-layered follicular organization composed of 60 elongated floating extensions made of as many outer and inner cells, and indirectly spread through an extracellular matrix over 1200 test cells. Experimental and selective ablation of outer and inner cells results in the abrogation of apoptosis in respective remaining neighbouring test cells. In addition incubation of outer/inner follicular cell-depleted eggs with a soluble extract of apoptotic outer/inner cells partially restores apoptosis to apoptotic-defective test cells. The 60 inner follicular cells were thus identified as ‘apoptotic master’ cells which collectively are induction sites for programmed cell death of the underlying test cells. The position of apoptotic master cells is controlled by topological constraints exhibiting a tetrahedral symmetry, and each cell spreads over and can control the destiny of 20 smaller test cells, which leads to optimized apoptosis signalling.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {PLOS ONE},\\n\\tauthor = {Martinand-Mari, Camille and Maury, Benoit and Rousset, François and Sahuquet, Alain and Mennessier, Gérard and Rochal, Sergei and Lorman, Vladimir and Mangeat, Paul and Baghdiguian, Stephen},\\n\\tyear = {2009},\\n\\tnote = {Publisher: Public Library of Science},\\n\\tkeywords = {Apoptosis, Apoptotic signaling cascade, Chorion, Ciona intestinalis, Eggs, Fertilization, Ova, Symmetry},\\n\\tpages = {e4202},\\n\\tfile = {Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\U26F6JVM\\\\\\\\Martinand-Mari и др. - 2009 - Topological Control of Life and Death in Non-Proli.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Martinand-Mari, C.\",\"Maury, B.\",\"Rousset, F.\",\"Sahuquet, A.\",\"Mennessier, G.\",\"Rochal, S.\",\"Lorman, V.\",\"Mangeat, P.\",\"Baghdiguian, S.\"],\"key\":\"martinand-mari_topological_2009\",\"id\":\"martinand-mari_topological_2009\",\"bibbaseid\":\"martinandmari-maury-rousset-sahuquet-mennessier-rochal-lorman-mangeat-etal-topologicalcontroloflifeanddeathinnonproliferativeepithelia-2009\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.plos.org/plosone/article?id=10.1371/journal.pone.0004202\"},\"keyword\":[\"Apoptosis\",\"Apoptotic signaling cascade\",\"Chorion\",\"Ciona intestinalis\",\"Eggs\",\"Fertilization\",\"Ova\",\"Symmetry\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Magnetic and structural properties of transition metal doped zinc-oxide nanostructures\",\"volume\":\"246\",\"copyright\":\"Copyright © 2009 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim\",\"issn\":\"1521-3951\",\"url\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.200880581\",\"doi\":\"10.1002/pssb.200880581\",\"abstract\":\"We report on the magnetic and structural properties of two types of nanostructures doped with Co or Mn, namely, ZnO nanowires and colloidal ZnO nanocrystals. Electron paramagnetic resonance (EPR) spectra have been measured and analysed to extract information on the incorporation of the ions in the lattice. A detailed analysis by means of simulations of the experimental EPR spectra confirms that the transition metal (TM) ions were mainly incorporated as TM2+, occupying the Zn2+ sites in the wurtzite structure of ZnO. Furthermore, for both types of nanostructures, the EPR spectra are composed of more than one signal, revealing locally distorted environments or core-shell structures, proved by surface modifications via inorganic coatings. (© 2009 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)\",\"language\":\"en\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"physica status solidi (b)\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Ankiewicz\"],\"firstnames\":[\"Amélia\",\"O.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gehlhoff\"],\"firstnames\":[\"Wolfgang\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Martins\"],\"firstnames\":[\"Joana\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pereira\"],\"firstnames\":[\"Ângela\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pereira\"],\"firstnames\":[\"Sérgio\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hoffmann\"],\"firstnames\":[\"Axel\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"Evgeni\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rahm\"],\"firstnames\":[\"Andreas\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"Michael\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"Marius\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Carmo\"],\"firstnames\":[\"Maria\",\"C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Trindade\"],\"firstnames\":[\"Tito\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sobolev\"],\"firstnames\":[\"Nikolai\",\"A.\"],\"suffixes\":[]}],\"year\":\"2009\",\"note\":\"_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.200880581\",\"keywords\":\"61.72.Vv, 68.65.La, 75.50.Pp, 76.30.Fc, 81.07.Bc\",\"pages\":\"766–770\",\"bibtex\":\"@article{ankiewicz_magnetic_2009,\\n\\ttitle = {Magnetic and structural properties of transition metal doped zinc-oxide nanostructures},\\n\\tvolume = {246},\\n\\tcopyright = {Copyright © 2009 WILEY-VCH Verlag GmbH \\\\& Co. KGaA, Weinheim},\\n\\tissn = {1521-3951},\\n\\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.200880581},\\n\\tdoi = {10.1002/pssb.200880581},\\n\\tabstract = {We report on the magnetic and structural properties of two types of nanostructures doped with Co or Mn, namely, ZnO nanowires and colloidal ZnO nanocrystals. Electron paramagnetic resonance (EPR) spectra have been measured and analysed to extract information on the incorporation of the ions in the lattice. A detailed analysis by means of simulations of the experimental EPR spectra confirms that the transition metal (TM) ions were mainly incorporated as TM2+, occupying the Zn2+ sites in the wurtzite structure of ZnO. Furthermore, for both types of nanostructures, the EPR spectra are composed of more than one signal, revealing locally distorted environments or core-shell structures, proved by surface modifications via inorganic coatings. (© 2009 WILEY-VCH Verlag GmbH \\\\& Co. KGaA, Weinheim)},\\n\\tlanguage = {en},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {physica status solidi (b)},\\n\\tauthor = {Ankiewicz, Amélia O. and Gehlhoff, Wolfgang and Martins, Joana S. and Pereira, Ângela S. and Pereira, Sérgio and Hoffmann, Axel and Kaidashev, Evgeni M. and Rahm, Andreas and Lorenz, Michael and Grundmann, Marius and Carmo, Maria C. and Trindade, Tito and Sobolev, Nikolai A.},\\n\\tyear = {2009},\\n\\tnote = {\\\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.200880581},\\n\\tkeywords = {61.72.Vv, 68.65.La, 75.50.Pp, 76.30.Fc, 81.07.Bc},\\n\\tpages = {766--770},\\n}\\n\\n\",\"author_short\":[\"Ankiewicz, A. O.\",\"Gehlhoff, W.\",\"Martins, J. S.\",\"Pereira, Â. S.\",\"Pereira, S.\",\"Hoffmann, A.\",\"Kaidashev, E. M.\",\"Rahm, A.\",\"Lorenz, M.\",\"Grundmann, M.\",\"Carmo, M. C.\",\"Trindade, T.\",\"Sobolev, N. A.\"],\"key\":\"ankiewicz_magnetic_2009\",\"id\":\"ankiewicz_magnetic_2009\",\"bibbaseid\":\"ankiewicz-gehlhoff-martins-pereira-pereira-hoffmann-kaidashev-rahm-etal-magneticandstructuralpropertiesoftransitionmetaldopedzincoxidenanostructures-2009\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.200880581\"},\"keyword\":[\"61.72.Vv\",\"68.65.La\",\"75.50.Pp\",\"76.30.Fc\",\"81.07.Bc\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"book\",\"type\":\"book\",\"title\":\"Обработка и визуализация данных физических экспериментов с помощью пакета Origin\",\"isbn\":\"978-5-397-00183-0\",\"url\":\"https://urss.ru/cgi-bin/db.pl?lang=Ru&blang=ru&page=Book&id=81481&list=Found\",\"abstract\":\"Настоящее учебно-методическое пособие на конкретных примерах учит приемам обработки спектров с помощью пакета Origin. Рассматриваются типичные задачи, наиболее часто встречающиеся на практике. Пособие может использоваться при изучении дисциплин общего и специального физического практикума студентами направлений \\\"Нанотехнология\\\", \\\"Физика\\\" и других физических направлений и специальностей. Оно будет полезно всем, кому по роду своей деятельности приходится иметь дело с анализом спектров.\",\"author\":[{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Исакова О.П.\"],\"suffixes\":[]},{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Тарасевич Ю.Ю.\"],\"suffixes\":[]},{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Юзюк Ю.И.\"],\"suffixes\":[]}],\"year\":\"2009\",\"bibtex\":\"@book{___2009,\\n\\ttitle = {Обработка и визуализация данных физических экспериментов с помощью пакета {Origin}},\\n\\tisbn = {978-5-397-00183-0},\\n\\turl = {https://urss.ru/cgi-bin/db.pl?lang=Ru&blang=ru&page=Book&id=81481&list=Found},\\n\\tabstract = {Настоящее учебно-методическое пособие на конкретных примерах учит приемам обработки спектров с помощью пакета Origin. Рассматриваются типичные задачи, наиболее часто встречающиеся на практике.\\n\\nПособие может использоваться при изучении дисциплин общего и специального физического практикума студентами направлений \\\"Нанотехнология\\\", \\\"Физика\\\" и других физических направлений и специальностей. Оно будет полезно всем, кому по роду своей деятельности приходится иметь дело с анализом спектров.},\\n\\tauthor = {{Исакова О.П.} and {Тарасевич Ю.Ю.} and {Юзюк Ю.И.}},\\n\\tyear = {2009},\\n}\\n\\n\",\"author_short\":[\"Исакова О.П.\",\"Тарасевич Ю.Ю.\",\"Юзюк Ю.И.\"],\"key\":\"___2009\",\"id\":\"___2009\",\"bibbaseid\":\"---origin-2009\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://urss.ru/cgi-bin/db.pl?lang=Ru&blang=ru&page=Book&id=81481&list=Found\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Spatial fluctuations of optical emission from single ZnO/MgZnO nanowire quantum wells\",\"volume\":\"19\",\"issn\":\"0957-4484\",\"url\":\"https://dx.doi.org/10.1088/0957-4484/19/11/115202\",\"doi\":\"10.1088/0957-4484/19/11/115202\",\"abstract\":\"MgZnO/ZnO quantum wells on top of ZnO nanowires were grown by pulsed laser deposition. Ensembles of spatially fluctuating and narrow cathodoluminescence peaks with single widths down to 1 meV were found at the spectral position of the quantum well emission at 4 K. In addition, the number of these narrow QW peaks increases with increasing excitation power in micro-photoluminescence, thus pointing to quantum-dot-like emission centers. Indeed, laterally strained areas of about 5 nm diameter were identified at the quantum well positions on top of the nanowires by high-resolution transmission electron microscopy.\",\"language\":\"en\",\"number\":\"11\",\"urldate\":\"2023-11-11\",\"journal\":\"Nanotechnology\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Czekalla\"],\"firstnames\":[\"C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Guinard\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hanisch\"],\"firstnames\":[\"C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Cao\"],\"firstnames\":[\"B.\",\"Q.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Boukos\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Travlos\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Renard\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gayral\"],\"firstnames\":[\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dang\"],\"firstnames\":[\"D.\",\"Le\",\"Si\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2008\",\"pages\":\"115202\",\"bibtex\":\"@article{czekalla_spatial_2008,\\n\\ttitle = {Spatial fluctuations of optical emission from single {ZnO}/{MgZnO} nanowire quantum wells},\\n\\tvolume = {19},\\n\\tissn = {0957-4484},\\n\\turl = {https://dx.doi.org/10.1088/0957-4484/19/11/115202},\\n\\tdoi = {10.1088/0957-4484/19/11/115202},\\n\\tabstract = {MgZnO/ZnO quantum wells on top of ZnO nanowires were grown by pulsed laser deposition. Ensembles of spatially fluctuating and narrow cathodoluminescence peaks with single widths down to 1 meV were found at the spectral position of the quantum well emission at 4 K. In addition, the number of these narrow QW peaks increases with increasing excitation power in micro-photoluminescence, thus pointing to quantum-dot-like emission centers. Indeed, laterally strained areas of about 5 nm diameter were identified at the quantum well positions on top of the nanowires by high-resolution transmission electron microscopy.},\\n\\tlanguage = {en},\\n\\tnumber = {11},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Nanotechnology},\\n\\tauthor = {Czekalla, C. and Guinard, J. and Hanisch, C. and Cao, B. Q. and Kaidashev, E. M. and Boukos, N. and Travlos, A. and Renard, J. and Gayral, B. and Dang, D. Le Si and Lorenz, M. and Grundmann, M.},\\n\\tmonth = feb,\\n\\tyear = {2008},\\n\\tpages = {115202},\\n}\\n\\n\",\"author_short\":[\"Czekalla, C.\",\"Guinard, J.\",\"Hanisch, C.\",\"Cao, B. Q.\",\"Kaidashev, E. M.\",\"Boukos, N.\",\"Travlos, A.\",\"Renard, J.\",\"Gayral, B.\",\"Dang, D. L. S.\",\"Lorenz, M.\",\"Grundmann, M.\"],\"key\":\"czekalla_spatial_2008\",\"id\":\"czekalla_spatial_2008\",\"bibbaseid\":\"czekalla-guinard-hanisch-cao-kaidashev-boukos-travlos-renard-etal-spatialfluctuationsofopticalemissionfromsingleznomgznonanowirequantumwells-2008\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/0957-4484/19/11/115202\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Structure and optical properties of ZnO nanowires fabricated by pulsed laser deposition on GaN/Si(111) films with the use of Au and NiO catalysts\",\"volume\":\"72\",\"issn\":\"1062-8738, 1934-9432\",\"url\":\"http://link.springer.com/10.3103/S1062873808080315\",\"doi\":\"10.3103/S1062873808080315\",\"language\":\"en\",\"number\":\"8\",\"urldate\":\"2023-11-11\",\"journal\":\"Bulletin of the Russian Academy of Sciences: Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lenzner\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ramm\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nobis\"],\"firstnames\":[\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zakharov\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kozakov\"],\"firstnames\":[\"A.\",\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shevtsova\"],\"firstnames\":[\"S.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Abdulvakhidov\"],\"firstnames\":[\"K.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"V.\",\"E.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2008\",\"pages\":\"1129–1131\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\TPG4HECU\\\\\\\\Kaidashev и др. - 2008 - Structure and optical properties of ZnO nanowires .pdf:application/pdf\",\"bibtex\":\"@article{kaidashev_structure_2008,\\n\\ttitle = {Structure and optical properties of {ZnO} nanowires fabricated by pulsed laser deposition on {GaN}/{Si}(111) films with the use of {Au} and {NiO} catalysts},\\n\\tvolume = {72},\\n\\tissn = {1062-8738, 1934-9432},\\n\\turl = {http://link.springer.com/10.3103/S1062873808080315},\\n\\tdoi = {10.3103/S1062873808080315},\\n\\tlanguage = {en},\\n\\tnumber = {8},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Bulletin of the Russian Academy of Sciences: Physics},\\n\\tauthor = {Kaidashev, E. M. and Lorenz, M. and Lenzner, J. and Ramm, A. and Nobis, T. and Grundmann, M. and Zakharov, N. and Kozakov, A. T. and Shevtsova, S. I. and Abdulvakhidov, K. G. and Kaidashev, V. E.},\\n\\tmonth = aug,\\n\\tyear = {2008},\\n\\tpages = {1129--1131},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\TPG4HECU\\\\\\\\Kaidashev и др. - 2008 - Structure and optical properties of ZnO nanowires .pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Kaidashev, E. M.\",\"Lorenz, M.\",\"Lenzner, J.\",\"Ramm, A.\",\"Nobis, T.\",\"Grundmann, M.\",\"Zakharov, N.\",\"Kozakov, A. T.\",\"Shevtsova, S. I.\",\"Abdulvakhidov, K. G.\",\"Kaidashev, V. E.\"],\"key\":\"kaidashev_structure_2008\",\"id\":\"kaidashev_structure_2008\",\"bibbaseid\":\"kaidashev-lorenz-lenzner-ramm-nobis-grundmann-zakharov-kozakov-etal-structureandopticalpropertiesofznonanowiresfabricatedbypulsedlaserdepositionongansi111filmswiththeuseofauandniocatalysts-2008\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://link.springer.com/10.3103/S1062873808080315\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Vacuum Ultraviolet Dielectric Function and Band Structure of ZnO\",\"volume\":\"53\",\"issn\":\"0374-4884\",\"url\":\"http://www.jkps.or.kr/journal/DOIx.php?id=10.3938/jkps.53.88\",\"doi\":\"10.3938/jkps.53.88\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of the Korean Physical Society\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Schmidt-Grund\"],\"firstnames\":[\"Rüdiger\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rheinländer\"],\"firstnames\":[\"Bernd\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"Evgeni\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"Michael\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"Marius\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fritsch\"],\"firstnames\":[\"Daniel\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Schubert\"],\"firstnames\":[\"Mathias\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Schmidt\"],\"firstnames\":[\"Heidemarie\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Herzinger\"],\"firstnames\":[\"Craig\",\"M.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2008\",\"pages\":\"88–93\",\"bibtex\":\"@article{schmidt-grund_vacuum_2008,\\n\\ttitle = {Vacuum {Ultraviolet} {Dielectric} {Function} and {Band} {Structure} of {ZnO}},\\n\\tvolume = {53},\\n\\tissn = {0374-4884},\\n\\turl = {http://www.jkps.or.kr/journal/DOIx.php?id=10.3938/jkps.53.88},\\n\\tdoi = {10.3938/jkps.53.88},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of the Korean Physical Society},\\n\\tauthor = {Schmidt-Grund, Rüdiger and Rheinländer, Bernd and Kaidashev, Evgeni M. and Lorenz, Michael and Grundmann, Marius and Fritsch, Daniel and Schubert, Mathias M. and Schmidt, Heidemarie and Herzinger, Craig M.},\\n\\tmonth = jul,\\n\\tyear = {2008},\\n\\tpages = {88--93},\\n}\\n\\n\",\"author_short\":[\"Schmidt-Grund, R.\",\"Rheinländer, B.\",\"Kaidashev, E. M.\",\"Lorenz, M.\",\"Grundmann, M.\",\"Fritsch, D.\",\"Schubert, M. M.\",\"Schmidt, H.\",\"Herzinger, C. M.\"],\"key\":\"schmidt-grund_vacuum_2008\",\"id\":\"schmidt-grund_vacuum_2008\",\"bibbaseid\":\"schmidtgrund-rheinlnder-kaidashev-lorenz-grundmann-fritsch-schubert-schmidt-etal-vacuumultravioletdielectricfunctionandbandstructureofzno-2008\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://www.jkps.or.kr/journal/DOIx.php?id=10.3938/jkps.53.88\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"incollection\",\"type\":\"incollection\",\"title\":\"Growth and Characterization of ZnO Nano- and Microstructures\",\"isbn\":\"978-0-08-046325-4\",\"url\":\"https://linkinghub.elsevier.com/retrieve/pii/B9780080463254000098\",\"language\":\"en\",\"urldate\":\"2023-11-11\",\"booktitle\":\"Handbook of Self Assembled Semiconductor Nanostructures for Novel Devices in Photonics and Electronics\",\"publisher\":\"Elsevier\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"Marius\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rahm\"],\"firstnames\":[\"Andreas\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nobis\"],\"firstnames\":[\"Thomas\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"Michael\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Czekalla\"],\"firstnames\":[\"Christian\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"Evgeni\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lenzner\"],\"firstnames\":[\"Jörg\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Boukos\"],\"firstnames\":[\"Nikos\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Travlos\"],\"firstnames\":[\"Anastasios\"],\"suffixes\":[]}],\"year\":\"2008\",\"doi\":\"10.1016/B978-0-08-046325-4.00009-8\",\"pages\":\"293–323\",\"bibtex\":\"@incollection{grundmann_growth_2008,\\n\\ttitle = {Growth and {Characterization} of {ZnO} {Nano}- and {Microstructures}},\\n\\tisbn = {978-0-08-046325-4},\\n\\turl = {https://linkinghub.elsevier.com/retrieve/pii/B9780080463254000098},\\n\\tlanguage = {en},\\n\\turldate = {2023-11-11},\\n\\tbooktitle = {Handbook of {Self} {Assembled} {Semiconductor} {Nanostructures} for {Novel} {Devices} in {Photonics} and {Electronics}},\\n\\tpublisher = {Elsevier},\\n\\tauthor = {Grundmann, Marius and Rahm, Andreas and Nobis, Thomas and Lorenz, Michael and Czekalla, Christian and Kaidashev, Evgeni M. and Lenzner, Jörg and Boukos, Nikos and Travlos, Anastasios},\\n\\tyear = {2008},\\n\\tdoi = {10.1016/B978-0-08-046325-4.00009-8},\\n\\tpages = {293--323},\\n}\\n\\n\",\"author_short\":[\"Grundmann, M.\",\"Rahm, A.\",\"Nobis, T.\",\"Lorenz, M.\",\"Czekalla, C.\",\"Kaidashev, E. M.\",\"Lenzner, J.\",\"Boukos, N.\",\"Travlos, A.\"],\"key\":\"grundmann_growth_2008\",\"id\":\"grundmann_growth_2008\",\"bibbaseid\":\"grundmann-rahm-nobis-lorenz-czekalla-kaidashev-lenzner-boukos-etal-growthandcharacterizationofznonanoandmicrostructures-2008\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://linkinghub.elsevier.com/retrieve/pii/B9780080463254000098\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"book\",\"type\":\"book\",\"title\":\"Введение в химию и физику наноструктур и наноструктурированных материалов\",\"isbn\":\"978-5-91327-029-0\",\"publisher\":\"Москва: Академия Естествознания\",\"author\":[{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Таланов В.М.\"],\"suffixes\":[]},{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Ерейская Г.П.\"],\"suffixes\":[]},{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Юзюк Ю.И.\"],\"suffixes\":[]}],\"year\":\"2008\",\"bibtex\":\"@book{___2008,\\n\\ttitle = {Введение в химию и физику наноструктур и наноструктурированных материалов},\\n\\tisbn = {978-5-91327-029-0},\\n\\tpublisher = {Москва: Академия Естествознания},\\n\\tauthor = {{Таланов В.М.} and {Ерейская Г.П.} and {Юзюк Ю.И.}},\\n\\tyear = {2008},\\n}\\n\\n\",\"author_short\":[\"Таланов В.М.\",\"Ерейская Г.П.\",\"Юзюк Ю.И.\"],\"key\":\"___2008\",\"id\":\"___2008\",\"bibbaseid\":\"----2008\",\"role\":\"author\",\"urls\":{},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Switchable nonlinear metalloferroelectric photonic crystals\",\"volume\":\"91\",\"issn\":\"0003-6951\",\"url\":\"https://doi.org/10.1063/1.2762284\",\"doi\":\"10.1063/1.2762284\",\"abstract\":\"Two types of low-voltage electroswitchable nonlinear photonic crystals were fabricated providing spatial-frequency control of second harmonic generation radiation of visible light. A two-dimensional photonic crystal was fabricated by focused ion beam etching of a ferroelectric BaSrTiO3 thin film and switched by an electric field applied by an interdigital electrode system, which simultaneously acted as a one-dimensional photonic crystal. The fabricated device operated at a second harmonic wavelength around 400nm with an efficiency incomparably higher than in the case of linear optics.\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Applied Physics Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Mishina\"],\"firstnames\":[\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zaitsev\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ilyin\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sherstyuk\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sigov\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golovko\"],\"firstnames\":[\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Muhortov\"],\"firstnames\":[\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kolesnikov\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lozovik\"],\"firstnames\":[\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yemtsova\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rasing\"],\"firstnames\":[\"Th.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2007\",\"pages\":\"041107\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\UJII4ECH\\\\\\\\Mishina и др. - 2007 - Switchable nonlinear metalloferroelectric photonic.pdf:application/pdf\",\"bibtex\":\"@article{mishina_switchable_2007,\\n\\ttitle = {Switchable nonlinear metalloferroelectric photonic crystals},\\n\\tvolume = {91},\\n\\tissn = {0003-6951},\\n\\turl = {https://doi.org/10.1063/1.2762284},\\n\\tdoi = {10.1063/1.2762284},\\n\\tabstract = {Two types of low-voltage electroswitchable nonlinear photonic crystals were fabricated providing spatial-frequency control of second harmonic generation radiation of visible light. A two-dimensional photonic crystal was fabricated by focused ion beam etching of a ferroelectric BaSrTiO3 thin film and switched by an electric field applied by an interdigital electrode system, which simultaneously acted as a one-dimensional photonic crystal. The fabricated device operated at a second harmonic wavelength around 400nm with an efficiency incomparably higher than in the case of linear optics.},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Applied Physics Letters},\\n\\tauthor = {Mishina, E. and Zaitsev, A. and Ilyin, N. and Sherstyuk, N. and Sigov, A. and Golovko, Yu. and Muhortov, V. and Kolesnikov, A. and Lozovik, Yu. and Yemtsova, M. and Rasing, Th.},\\n\\tmonth = jul,\\n\\tyear = {2007},\\n\\tpages = {041107},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\UJII4ECH\\\\\\\\Mishina и др. - 2007 - Switchable nonlinear metalloferroelectric photonic.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Mishina, E.\",\"Zaitsev, A.\",\"Ilyin, N.\",\"Sherstyuk, N.\",\"Sigov, A.\",\"Golovko, Y.\",\"Muhortov, V.\",\"Kolesnikov, A.\",\"Lozovik, Y.\",\"Yemtsova, M.\",\"Rasing, T.\"],\"key\":\"mishina_switchable_2007\",\"id\":\"mishina_switchable_2007\",\"bibbaseid\":\"mishina-zaitsev-ilyin-sherstyuk-sigov-golovko-muhortov-kolesnikov-etal-switchablenonlinearmetalloferroelectricphotoniccrystals-2007\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.2762284\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Growth and characterization of Mn- and Co-doped ZnO nanowires\",\"volume\":\"156\",\"issn\":\"1436-5073\",\"url\":\"https://doi.org/10.1007/s00604-006-0602-1\",\"doi\":\"10.1007/s00604-006-0602-1\",\"abstract\":\"We report on the high-pressure pulsed laser deposition growth of zinc oxide nanowires containing about 0.2 at.% Co and 0.5 at.% Mn by NiO and Au catalyst. Scanning electron microscopy and X-ray diffraction measurements revealed arrays of parallel-standing nanowires with hexagonal cross section and uniform in-plane epitaxial relations without rotational domains. Elemental analysis was carried out using particle induced X-ray emission and Q-band electron spin resonance. The valence of the incorporated Mn was determined to be 2+. Atomic and magnetic force microscopy measurements indicate that Mn is incorporated preferentially at the nanowire boundaries.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Microchimica Acta\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Rahm\"],\"firstnames\":[\"Andreas\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"Evgeni\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Schmidt\"],\"firstnames\":[\"Heidemarie\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Diaconu\"],\"firstnames\":[\"Mariana\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pöppl\"],\"firstnames\":[\"Andreas\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Böttcher\"],\"firstnames\":[\"Rolf\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Meinecke\"],\"firstnames\":[\"Christoph\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Butz\"],\"firstnames\":[\"Tilman\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"Michael\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"Marius\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2006\",\"keywords\":\"Key words: Zinc oxide; pulsed laser deposition; nanowire; transition metal.\",\"pages\":\"21–25\",\"bibtex\":\"@article{rahm_growth_2006,\\n\\ttitle = {Growth and characterization of {Mn}- and {Co}-doped {ZnO} nanowires},\\n\\tvolume = {156},\\n\\tissn = {1436-5073},\\n\\turl = {https://doi.org/10.1007/s00604-006-0602-1},\\n\\tdoi = {10.1007/s00604-006-0602-1},\\n\\tabstract = {We report on the high-pressure pulsed laser deposition growth of zinc oxide nanowires containing about 0.2 at.\\\\% Co and 0.5 at.\\\\% Mn by NiO and Au catalyst. Scanning electron microscopy and X-ray diffraction measurements revealed arrays of parallel-standing nanowires with hexagonal cross section and uniform in-plane epitaxial relations without rotational domains. Elemental analysis was carried out using particle induced X-ray emission and Q-band electron spin resonance. The valence of the incorporated Mn was determined to be 2+. Atomic and magnetic force microscopy measurements indicate that Mn is incorporated preferentially at the nanowire boundaries.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Microchimica Acta},\\n\\tauthor = {Rahm, Andreas and Kaidashev, Evgeni M. and Schmidt, Heidemarie and Diaconu, Mariana and Pöppl, Andreas and Böttcher, Rolf and Meinecke, Christoph and Butz, Tilman and Lorenz, Michael and Grundmann, Marius},\\n\\tmonth = nov,\\n\\tyear = {2006},\\n\\tkeywords = {Key words: Zinc oxide; pulsed laser deposition; nanowire; transition metal.},\\n\\tpages = {21--25},\\n}\\n\\n\",\"author_short\":[\"Rahm, A.\",\"Kaidashev, E. M.\",\"Schmidt, H.\",\"Diaconu, M.\",\"Pöppl, A.\",\"Böttcher, R.\",\"Meinecke, C.\",\"Butz, T.\",\"Lorenz, M.\",\"Grundmann, M.\"],\"key\":\"rahm_growth_2006\",\"id\":\"rahm_growth_2006\",\"bibbaseid\":\"rahm-kaidashev-schmidt-diaconu-pppl-bttcher-meinecke-butz-etal-growthandcharacterizationofmnandcodopedznonanowires-2006\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1007/s00604-006-0602-1\"},\"keyword\":[\"Key words: Zinc oxide; pulsed laser deposition; nanowire; transition metal.\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"address\":\"Dordrecht\",\"series\":\"NATO Science Series II: Mathematics, Physics and Chemistry\",\"title\":\"Whispering Gallery Modes in Hexagonal Zinc Oxide Micro- and Nanocrystals\",\"isbn\":\"978-1-4020-3475-6\",\"doi\":\"10.1007/1-4020-3475-X_8\",\"abstract\":\"The resonator properties of zinc oxide (ZnO) micro- and nanocrystals grown by a novel high pressure pulsed laser deposition process have been investigated at room temperature by cathodoluminescence (CL), spatially resolved CL-imaging and polarization resolved micro-photoluminescence (μ-PL) within the visible spectral range. The spectra exhibit a series of comparatively sharp and almost equidistant resonance lines. Using a simple plane wave interference model and taking into account the spectral characteristic n(ω) of the refractive index of ZnO, we can unambiguously attribute those lines to whispering gallery modes (WGMs) of a two dimensional hexagonal resonator. The predicted resonator diameters agree well with the measured crystal sizes. Tapered, high aspect ratio ZnO nanoneedles furthermore allow systematic investigations of the WGMs as a function of cavity diameter D down to zero. Hence, the transition from a multi-mode to a single mode cavity is directly observed. μ-PL experiments demonstrate that the WGMs are mainly TM polarized.\",\"language\":\"en\",\"booktitle\":\"Zinc Oxide — A Material for Micro- and Optoelectronic Applications\",\"publisher\":\"Springer Netherlands\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Nobis\"],\"firstnames\":[\"Thomas\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"Evgeni\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rahm\"],\"firstnames\":[\"Andreas\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"Michael\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"Marius\"],\"suffixes\":[]}],\"editor\":[{\"propositions\":[],\"lastnames\":[\"Nickel\"],\"firstnames\":[\"Norbert\",\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Terukov\"],\"firstnames\":[\"Evgenii\"],\"suffixes\":[]}],\"year\":\"2005\",\"keywords\":\"microcrystal, nanocavity, nanostructure, polarization, Whispering gallery modes\",\"pages\":\"83–98\",\"bibtex\":\"@inproceedings{nobis_whispering_2005,\\n\\taddress = {Dordrecht},\\n\\tseries = {{NATO} {Science} {Series} {II}: {Mathematics}, {Physics} and {Chemistry}},\\n\\ttitle = {Whispering {Gallery} {Modes} in {Hexagonal} {Zinc} {Oxide} {Micro}- and {Nanocrystals}},\\n\\tisbn = {978-1-4020-3475-6},\\n\\tdoi = {10.1007/1-4020-3475-X_8},\\n\\tabstract = {The resonator properties of zinc oxide (ZnO) micro- and nanocrystals grown by a novel high pressure pulsed laser deposition process have been investigated at room temperature by cathodoluminescence (CL), spatially resolved CL-imaging and polarization resolved micro-photoluminescence (μ-PL) within the visible spectral range. The spectra exhibit a series of comparatively sharp and almost equidistant resonance lines. Using a simple plane wave interference model and taking into account the spectral characteristic n(ω) of the refractive index of ZnO, we can unambiguously attribute those lines to whispering gallery modes (WGMs) of a two dimensional hexagonal resonator. The predicted resonator diameters agree well with the measured crystal sizes. Tapered, high aspect ratio ZnO nanoneedles furthermore allow systematic investigations of the WGMs as a function of cavity diameter D down to zero. Hence, the transition from a multi-mode to a single mode cavity is directly observed. μ-PL experiments demonstrate that the WGMs are mainly TM polarized.},\\n\\tlanguage = {en},\\n\\tbooktitle = {Zinc {Oxide} — {A} {Material} for {Micro}- and {Optoelectronic} {Applications}},\\n\\tpublisher = {Springer Netherlands},\\n\\tauthor = {Nobis, Thomas and Kaidashev, Evgeni M. and Rahm, Andreas and Lorenz, Michael and Grundmann, Marius},\\n\\teditor = {Nickel, Norbert H. and Terukov, Evgenii},\\n\\tyear = {2005},\\n\\tkeywords = {microcrystal, nanocavity, nanostructure, polarization, Whispering gallery modes},\\n\\tpages = {83--98},\\n}\\n\\n\",\"author_short\":[\"Nobis, T.\",\"Kaidashev, E. M.\",\"Rahm, A.\",\"Lorenz, M.\",\"Grundmann, M.\"],\"editor_short\":[\"Nickel, N. H.\",\"Terukov, E.\"],\"key\":\"nobis_whispering_2005\",\"id\":\"nobis_whispering_2005\",\"bibbaseid\":\"nobis-kaidashev-rahm-lorenz-grundmann-whisperinggallerymodesinhexagonalzincoxidemicroandnanocrystals-2005\",\"role\":\"author\",\"urls\":{},\"keyword\":[\"microcrystal\",\"nanocavity\",\"nanostructure\",\"polarization\",\"Whispering gallery modes\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Whispering Gallery Modes in Nanosized Dielectric Resonators with Hexagonal Cross Section\",\"volume\":\"93\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevLett.93.103903\",\"doi\":\"10.1103/PhysRevLett.93.103903\",\"abstract\":\"The size dependence of whispering gallery modes in dielectric resonators with hexagonal cross section has been observed within the visible spectral range for cavity diameters comparable to the light wavelength. As a model system single, tapered, high aspect ratio zinc oxide nanoneedles were analyzed. They enable systematic investigations as a function of the resonator diameter down to the nanometer regime. A simple plane wave interference model without free parameter describes the spectral positions and the linewidths of the modes in good agreement with the experiment.\",\"number\":\"10\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Nobis\"],\"firstnames\":[\"Thomas\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"Evgeni\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rahm\"],\"firstnames\":[\"Andreas\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"Michael\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"Marius\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2004\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"103903\",\"bibtex\":\"@article{nobis_whispering_2004,\\n\\ttitle = {Whispering {Gallery} {Modes} in {Nanosized} {Dielectric} {Resonators} with {Hexagonal} {Cross} {Section}},\\n\\tvolume = {93},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevLett.93.103903},\\n\\tdoi = {10.1103/PhysRevLett.93.103903},\\n\\tabstract = {The size dependence of whispering gallery modes in dielectric resonators with hexagonal cross section has been observed within the visible spectral range for cavity diameters comparable to the light wavelength. As a model system single, tapered, high aspect ratio zinc oxide nanoneedles were analyzed. They enable systematic investigations as a function of the resonator diameter down to the nanometer regime. A simple plane wave interference model without free parameter describes the spectral positions and the linewidths of the modes in good agreement with the experiment.},\\n\\tnumber = {10},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review Letters},\\n\\tauthor = {Nobis, Thomas and Kaidashev, Evgeni M. and Rahm, Andreas and Lorenz, Michael and Grundmann, Marius},\\n\\tmonth = sep,\\n\\tyear = {2004},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {103903},\\n}\\n\\n\",\"author_short\":[\"Nobis, T.\",\"Kaidashev, E. M.\",\"Rahm, A.\",\"Lorenz, M.\",\"Grundmann, M.\"],\"key\":\"nobis_whispering_2004\",\"id\":\"nobis_whispering_2004\",\"bibbaseid\":\"nobis-kaidashev-rahm-lorenz-grundmann-whisperinggallerymodesinnanosizeddielectricresonatorswithhexagonalcrosssection-2004\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevLett.93.103903\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Spatially Inhomogeneous Impurity Distribution in ZnO Micropillars\",\"volume\":\"4\",\"issn\":\"1530-6984\",\"url\":\"https://doi.org/10.1021/nl049889y\",\"doi\":\"10.1021/nl049889y\",\"abstract\":\"Using ZnO a variety of micro- and nanostructures can be fabricated. We investigate hexagonal micropillars grown by high pressure pulsed laser deposition on sapphire with spatially and spectrally resolved cathodoluminescence. We demonstrate that the impurity and defect incorporation is strongly inhomogeneous, at least under the present growth conditions, dramatically influencing the optical properties.\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Nano Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Nobis\"],\"firstnames\":[\"Thomas\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"Evgeni\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rahm\"],\"firstnames\":[\"Andreas\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"Michael\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lenzner\"],\"firstnames\":[\"Jörg\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"Marius\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2004\",\"note\":\"Publisher: American Chemical Society\",\"pages\":\"797–800\",\"bibtex\":\"@article{nobis_spatially_2004,\\n\\ttitle = {Spatially {Inhomogeneous} {Impurity} {Distribution} in {ZnO} {Micropillars}},\\n\\tvolume = {4},\\n\\tissn = {1530-6984},\\n\\turl = {https://doi.org/10.1021/nl049889y},\\n\\tdoi = {10.1021/nl049889y},\\n\\tabstract = {Using ZnO a variety of micro- and nanostructures can be fabricated. We investigate hexagonal micropillars grown by high pressure pulsed laser deposition on sapphire with spatially and spectrally resolved cathodoluminescence. We demonstrate that the impurity and defect incorporation is strongly inhomogeneous, at least under the present growth conditions, dramatically influencing the optical properties.},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Nano Letters},\\n\\tauthor = {Nobis, Thomas and Kaidashev, Evgeni M. and Rahm, Andreas and Lorenz, Michael and Lenzner, Jörg and Grundmann, Marius},\\n\\tmonth = may,\\n\\tyear = {2004},\\n\\tnote = {Publisher: American Chemical Society},\\n\\tpages = {797--800},\\n}\\n\\n\",\"author_short\":[\"Nobis, T.\",\"Kaidashev, E. M.\",\"Rahm, A.\",\"Lorenz, M.\",\"Lenzner, J.\",\"Grundmann, M.\"],\"key\":\"nobis_spatially_2004\",\"id\":\"nobis_spatially_2004\",\"bibbaseid\":\"nobis-kaidashev-rahm-lorenz-lenzner-grundmann-spatiallyinhomogeneousimpuritydistributioninznomicropillars-2004\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1021/nl049889y\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"series\":\"The 3rd International Conference on Spectroscopic Ellipsometry\",\"title\":\"Infrared dielectric functions and crystal orientation of a-plane ZnO thin films on r-plane sapphire determined by generalized ellipsometry\",\"volume\":\"455-456\",\"issn\":\"0040-6090\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0040609003018285\",\"doi\":\"10.1016/j.tsf.2003.11.226\",\"abstract\":\"Generalized infrared spectroscopic ellipsometry for wave numbers from 370 to 1200 cm−1 was applied to study the anisotropic dielectric response of wurtzite-type ZnO thin films grown on r-plane sapphire. Combined wavelength-by-wavelength analysis of data measured at multiple sample in-plane orientations allows for simultaneous extraction of the dielectric function (DF) tensor, the film thickness and the respective ZnO c-axis orientation, specifically in relation to the sapphire substrate. For anisotropic materials and use of generalized ellipsometry, the correlation problem between thickness and DF does not exist. Subsequent line shape analysis of ordinary and extraordinary DFs provides complete A1- and E1-symmetry longitudinal and transverse optical phonon-mode and broadening parameters, together with the static dielectric constants. The epitaxial relations from the ellipsometry data analysis are (11−20)ZnO∣∣(01−12)sapphire and [0001]ZnO∣∣[0−111]sapphire, which was confirmed by XRD measurements.\",\"urldate\":\"2023-11-11\",\"journal\":\"Thin Solid Films\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Bundesmann\"],\"firstnames\":[\"C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ashkenov\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Schubert\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rahm\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Wenckstern\"],\"firstnames\":[\"H.\",\"v.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2004\",\"keywords\":\"-Plane ZnO, Epitaxial relation, Generalized infrared spectroscopic ellipsometry, Phonon modes\",\"pages\":\"161–166\",\"bibtex\":\"@article{bundesmann_infrared_2004,\\n\\tseries = {The 3rd {International} {Conference} on {Spectroscopic} {Ellipsometry}},\\n\\ttitle = {Infrared dielectric functions and crystal orientation of a-plane {ZnO} thin films on r-plane sapphire determined by generalized ellipsometry},\\n\\tvolume = {455-456},\\n\\tissn = {0040-6090},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0040609003018285},\\n\\tdoi = {10.1016/j.tsf.2003.11.226},\\n\\tabstract = {Generalized infrared spectroscopic ellipsometry for wave numbers from 370 to 1200 cm−1 was applied to study the anisotropic dielectric response of wurtzite-type ZnO thin films grown on r-plane sapphire. Combined wavelength-by-wavelength analysis of data measured at multiple sample in-plane orientations allows for simultaneous extraction of the dielectric function (DF) tensor, the film thickness and the respective ZnO c-axis orientation, specifically in relation to the sapphire substrate. For anisotropic materials and use of generalized ellipsometry, the correlation problem between thickness and DF does not exist. Subsequent line shape analysis of ordinary and extraordinary DFs provides complete A1- and E1-symmetry longitudinal and transverse optical phonon-mode and broadening parameters, together with the static dielectric constants. The epitaxial relations from the ellipsometry data analysis are (11−20)ZnO∣∣(01−12)sapphire and [0001]ZnO∣∣[0−111]sapphire, which was confirmed by XRD measurements.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Thin Solid Films},\\n\\tauthor = {Bundesmann, C. and Ashkenov, N. and Schubert, M. and Rahm, A. and Wenckstern, H. v. and Kaidashev, E. M. and Lorenz, M. and Grundmann, M.},\\n\\tmonth = may,\\n\\tyear = {2004},\\n\\tkeywords = {-Plane ZnO, Epitaxial relation, Generalized infrared spectroscopic ellipsometry, Phonon modes},\\n\\tpages = {161--166},\\n}\\n\\n\",\"author_short\":[\"Bundesmann, C.\",\"Ashkenov, N.\",\"Schubert, M.\",\"Rahm, A.\",\"Wenckstern, H. v.\",\"Kaidashev, E. M.\",\"Lorenz, M.\",\"Grundmann, M.\"],\"key\":\"bundesmann_infrared_2004\",\"id\":\"bundesmann_infrared_2004\",\"bibbaseid\":\"bundesmann-ashkenov-schubert-rahm-wenckstern-kaidashev-lorenz-grundmann-infrareddielectricfunctionsandcrystalorientationofaplaneznothinfilmsonrplanesapphiredeterminedbygeneralizedellipsometry-2004\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0040609003018285\"},\"keyword\":[\"-Plane ZnO\",\"Epitaxial relation\",\"Generalized infrared spectroscopic ellipsometry\",\"Phonon modes\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Lateral homogeneity of Schottky contacts on n-type ZnO\",\"volume\":\"84\",\"issn\":\"0003-6951\",\"url\":\"https://doi.org/10.1063/1.1638898\",\"doi\":\"10.1063/1.1638898\",\"abstract\":\"The electrical properties of Schottky contacts (SCs) produced ex situ on n-type ZnO single crystals and epitaxial thin films were investigated. Electron beam induced current imaging was used to study lateral variations of the current induced in the space charge region of the SC. Further, the effective barrier height was determined by current–voltage and capacitance–voltage measurements. Pd contacts prepared on ZnO thin films that had undergone treatment in a plasma-enhanced chemical vapor deposition with nitrous oxide (N2O) as ambient gas are laterally homogeneous with an effective barrier height of (600±30) meV.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Applied Physics Letters\",\"author\":[{\"propositions\":[\"von\"],\"lastnames\":[\"Wenckstern\"],\"firstnames\":[\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hochmuth\"],\"firstnames\":[\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Biehne\"],\"firstnames\":[\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lenzner\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gottschalch\"],\"firstnames\":[\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pickenhain\"],\"firstnames\":[\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2003\",\"pages\":\"79–81\",\"bibtex\":\"@article{von_wenckstern_lateral_2003,\\n\\ttitle = {Lateral homogeneity of {Schottky} contacts on n-type {ZnO}},\\n\\tvolume = {84},\\n\\tissn = {0003-6951},\\n\\turl = {https://doi.org/10.1063/1.1638898},\\n\\tdoi = {10.1063/1.1638898},\\n\\tabstract = {The electrical properties of Schottky contacts (SCs) produced ex situ on n-type ZnO single crystals and epitaxial thin films were investigated. Electron beam induced current imaging was used to study lateral variations of the current induced in the space charge region of the SC. Further, the effective barrier height was determined by current–voltage and capacitance–voltage measurements. Pd contacts prepared on ZnO thin films that had undergone treatment in a plasma-enhanced chemical vapor deposition with nitrous oxide (N2O) as ambient gas are laterally homogeneous with an effective barrier height of (600±30) meV.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Applied Physics Letters},\\n\\tauthor = {von Wenckstern, H. and Kaidashev, E. M. and Lorenz, M. and Hochmuth, H. and Biehne, G. and Lenzner, J. and Gottschalch, V. and Pickenhain, R. and Grundmann, M.},\\n\\tmonth = dec,\\n\\tyear = {2003},\\n\\tpages = {79--81},\\n}\\n\\n\",\"author_short\":[\"von Wenckstern, H.\",\"Kaidashev, E. M.\",\"Lorenz, M.\",\"Hochmuth, H.\",\"Biehne, G.\",\"Lenzner, J.\",\"Gottschalch, V.\",\"Pickenhain, R.\",\"Grundmann, M.\"],\"key\":\"von_wenckstern_lateral_2003\",\"id\":\"von_wenckstern_lateral_2003\",\"bibbaseid\":\"vonwenckstern-kaidashev-lorenz-hochmuth-biehne-lenzner-gottschalch-pickenhain-etal-lateralhomogeneityofschottkycontactsonntypezno-2003\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.1638898\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Raman scattering in ZnO thin films doped with Fe, Sb, Al, Ga, and Li\",\"volume\":\"83\",\"issn\":\"0003-6951\",\"url\":\"https://doi.org/10.1063/1.1609251\",\"doi\":\"10.1063/1.1609251\",\"abstract\":\"Polarized micro-Raman measurements were performed to study the phonon modes of Fe, Sb, Al, Ga, and Li doped ZnO thin films, grown by pulsed-laser deposition on c-plane sapphire substrates. Additional modes at about 277, 511, 583, and 644 cm−1, recently assigned to N incorporation [A. Kaschner et al., Appl. Phys. Lett. 80, 1909 (2002)], were observed for Fe, Sb, and Al doped films, intentionally grown without N. The mode at 277 cm−1 occurs also for Ga doped films. These modes thus cannot be related directly to N incorporation. Instead, we suggest host lattice defects as their origin. Further additional modes at 531, 631, and 720 cm−1 seem specific for the Sb, Ga, and Fe dopants, respectively. Li doped ZnO did not reveal additional modes.\",\"number\":\"10\",\"urldate\":\"2023-11-11\",\"journal\":\"Applied Physics Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Bundesmann\"],\"firstnames\":[\"C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ashkenov\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Schubert\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Spemann\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Butz\"],\"firstnames\":[\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2003\",\"pages\":\"1974–1976\",\"bibtex\":\"@article{bundesmann_raman_2003,\\n\\ttitle = {Raman scattering in {ZnO} thin films doped with {Fe}, {Sb}, {Al}, {Ga}, and {Li}},\\n\\tvolume = {83},\\n\\tissn = {0003-6951},\\n\\turl = {https://doi.org/10.1063/1.1609251},\\n\\tdoi = {10.1063/1.1609251},\\n\\tabstract = {Polarized micro-Raman measurements were performed to study the phonon modes of Fe, Sb, Al, Ga, and Li doped ZnO thin films, grown by pulsed-laser deposition on c-plane sapphire substrates. Additional modes at about 277, 511, 583, and 644 cm−1, recently assigned to N incorporation [A. Kaschner et al., Appl. Phys. Lett. 80, 1909 (2002)], were observed for Fe, Sb, and Al doped films, intentionally grown without N. The mode at 277 cm−1 occurs also for Ga doped films. These modes thus cannot be related directly to N incorporation. Instead, we suggest host lattice defects as their origin. Further additional modes at 531, 631, and 720 cm−1 seem specific for the Sb, Ga, and Fe dopants, respectively. Li doped ZnO did not reveal additional modes.},\\n\\tnumber = {10},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Applied Physics Letters},\\n\\tauthor = {Bundesmann, C. and Ashkenov, N. and Schubert, M. and Spemann, D. and Butz, T. and Kaidashev, E. M. and Lorenz, M. and Grundmann, M.},\\n\\tmonth = sep,\\n\\tyear = {2003},\\n\\tpages = {1974--1976},\\n}\\n\\n\",\"author_short\":[\"Bundesmann, C.\",\"Ashkenov, N.\",\"Schubert, M.\",\"Spemann, D.\",\"Butz, T.\",\"Kaidashev, E. M.\",\"Lorenz, M.\",\"Grundmann, M.\"],\"key\":\"bundesmann_raman_2003\",\"id\":\"bundesmann_raman_2003\",\"bibbaseid\":\"bundesmann-ashkenov-schubert-spemann-butz-kaidashev-lorenz-grundmann-ramanscatteringinznothinfilmsdopedwithfesbalgaandli-2003\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.1609251\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Infrared dielectric functions and phonon modes of high-quality ZnO films\",\"volume\":\"93\",\"issn\":\"0021-8979\",\"url\":\"https://doi.org/10.1063/1.1526935\",\"doi\":\"10.1063/1.1526935\",\"abstract\":\"Infrared dielectric function spectra and phonon modes of high-quality, single crystalline, and highly resistive wurtzite ZnO films were obtained from infrared (300–1200 cm−1) spectroscopic ellipsometry and Raman scattering studies. The ZnO films were deposited by pulsed-laser deposition on c-plane sapphire substrates and investigated by high-resolution x-ray diffraction, high-resolution transmission electron microscopy, and Rutherford backscattering experiments. The crystal structure, phonon modes, and dielectric functions are compared to those obtained from a single-crystal ZnO bulk sample. The film ZnO phonon mode frequencies are highly consistent with those of the bulk material. A small redshift of the longitudinal optical phonon mode frequencies of the ZnO films with respect to the bulk material is observed. This is tentatively assigned to the existence of vacancy point defects within the films. Accurate long-wavelength dielectric constant limits of ZnO are obtained from the infrared ellipsometry analysis and compared with previously measured near-band-gap index-of-refraction data using the Lyddane–Sachs–Teller relation. The ZnO model dielectric function spectra will become useful for future infrared ellipsometry analysis of free-carrier parameters in complex ZnO-based heterostructures.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Applied Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Ashkenov\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mbenkum\"],\"firstnames\":[\"B.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bundesmann\"],\"firstnames\":[\"C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Riede\"],\"firstnames\":[\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Spemann\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kasic\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Schubert\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Wagner\"],\"firstnames\":[\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Neumann\"],\"firstnames\":[\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Darakchieva\"],\"firstnames\":[\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Arwin\"],\"firstnames\":[\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Monemar\"],\"firstnames\":[\"B.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2002\",\"pages\":\"126–133\",\"bibtex\":\"@article{ashkenov_infrared_2002,\\n\\ttitle = {Infrared dielectric functions and phonon modes of high-quality {ZnO} films},\\n\\tvolume = {93},\\n\\tissn = {0021-8979},\\n\\turl = {https://doi.org/10.1063/1.1526935},\\n\\tdoi = {10.1063/1.1526935},\\n\\tabstract = {Infrared dielectric function spectra and phonon modes of high-quality, single crystalline, and highly resistive wurtzite ZnO films were obtained from infrared (300–1200 cm−1) spectroscopic ellipsometry and Raman scattering studies. The ZnO films were deposited by pulsed-laser deposition on c-plane sapphire substrates and investigated by high-resolution x-ray diffraction, high-resolution transmission electron microscopy, and Rutherford backscattering experiments. The crystal structure, phonon modes, and dielectric functions are compared to those obtained from a single-crystal ZnO bulk sample. The film ZnO phonon mode frequencies are highly consistent with those of the bulk material. A small redshift of the longitudinal optical phonon mode frequencies of the ZnO films with respect to the bulk material is observed. This is tentatively assigned to the existence of vacancy point defects within the films. Accurate long-wavelength dielectric constant limits of ZnO are obtained from the infrared ellipsometry analysis and compared with previously measured near-band-gap index-of-refraction data using the Lyddane–Sachs–Teller relation. The ZnO model dielectric function spectra will become useful for future infrared ellipsometry analysis of free-carrier parameters in complex ZnO-based heterostructures.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Applied Physics},\\n\\tauthor = {Ashkenov, N. and Mbenkum, B. N. and Bundesmann, C. and Riede, V. and Lorenz, M. and Spemann, D. and Kaidashev, E. M. and Kasic, A. and Schubert, M. and Grundmann, M. and Wagner, G. and Neumann, H. and Darakchieva, V. and Arwin, H. and Monemar, B.},\\n\\tmonth = dec,\\n\\tyear = {2002},\\n\\tpages = {126--133},\\n}\\n\\n\",\"author_short\":[\"Ashkenov, N.\",\"Mbenkum, B. N.\",\"Bundesmann, C.\",\"Riede, V.\",\"Lorenz, M.\",\"Spemann, D.\",\"Kaidashev, E. M.\",\"Kasic, A.\",\"Schubert, M.\",\"Grundmann, M.\",\"Wagner, G.\",\"Neumann, H.\",\"Darakchieva, V.\",\"Arwin, H.\",\"Monemar, B.\"],\"key\":\"ashkenov_infrared_2002\",\"id\":\"ashkenov_infrared_2002\",\"bibbaseid\":\"ashkenov-mbenkum-bundesmann-riede-lorenz-spemann-kaidashev-kasic-etal-infrareddielectricfunctionsandphononmodesofhighqualityznofilms-2002\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.1526935\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"High electron mobility of epitaxial ZnO thin films on c-plane sapphire grown by multistep pulsed-laser deposition\",\"volume\":\"82\",\"issn\":\"0003-6951\",\"url\":\"https://doi.org/10.1063/1.1578694\",\"doi\":\"10.1063/1.1578694\",\"abstract\":\"A multistep pulsed-laser deposition (PLD) process is presented for epitaxial, nominally undoped ZnO thin films of total thickness of 1 to 2 μm on c-plane sapphire substrates. We obtain reproducibly high electron mobilities from 115 up to 155 cm2/V s at 300 K in a narrow carrier concentration range from 2 to 5×1016 cm−3. The key issue of the multistep PLD process is the insertion of 30-nm-thin ZnO relaxation layers deposited at reduced substrate temperature. The high-mobility samples show atomically flat surface structure with grain size of about 0.5–1 μm, whereas the surfaces of low-mobility films consist of clearly resolved hexagonally faceted columnar grains of only 200-nm size, as shown by atomic force microscopy. Structurally optimized PLD ZnO thin films show narrow high-resolution x-ray diffraction peak widths of the ZnO(0002) ω- and 2Θ-scans as low as 151 and 43 arcsec, respectively, and narrow photoluminescence linewidths of donor-bound excitons of 1.7 meV at 2 K.\",\"number\":\"22\",\"urldate\":\"2023-11-11\",\"journal\":\"Applied Physics Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[\"von\"],\"lastnames\":[\"Wenckstern\"],\"firstnames\":[\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rahm\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Semmelhack\"],\"firstnames\":[\"H.-C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Han\"],\"firstnames\":[\"K.-H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Benndorf\"],\"firstnames\":[\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bundesmann\"],\"firstnames\":[\"C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hochmuth\"],\"firstnames\":[\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2003\",\"pages\":\"3901–3903\",\"bibtex\":\"@article{kaidashev_high_2003,\\n\\ttitle = {High electron mobility of epitaxial {ZnO} thin films on c-plane sapphire grown by multistep pulsed-laser deposition},\\n\\tvolume = {82},\\n\\tissn = {0003-6951},\\n\\turl = {https://doi.org/10.1063/1.1578694},\\n\\tdoi = {10.1063/1.1578694},\\n\\tabstract = {A multistep pulsed-laser deposition (PLD) process is presented for epitaxial, nominally undoped ZnO thin films of total thickness of 1 to 2 μm on c-plane sapphire substrates. We obtain reproducibly high electron mobilities from 115 up to 155 cm2/V s at 300 K in a narrow carrier concentration range from 2 to 5×1016 cm−3. The key issue of the multistep PLD process is the insertion of 30-nm-thin ZnO relaxation layers deposited at reduced substrate temperature. The high-mobility samples show atomically flat surface structure with grain size of about 0.5–1 μm, whereas the surfaces of low-mobility films consist of clearly resolved hexagonally faceted columnar grains of only 200-nm size, as shown by atomic force microscopy. Structurally optimized PLD ZnO thin films show narrow high-resolution x-ray diffraction peak widths of the ZnO(0002) ω- and 2Θ-scans as low as 151 and 43 arcsec, respectively, and narrow photoluminescence linewidths of donor-bound excitons of 1.7 meV at 2 K.},\\n\\tnumber = {22},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Applied Physics Letters},\\n\\tauthor = {Kaidashev, E. M. and Lorenz, M. and von Wenckstern, H. and Rahm, A. and Semmelhack, H.-C. and Han, K.-H. and Benndorf, G. and Bundesmann, C. and Hochmuth, H. and Grundmann, M.},\\n\\tmonth = may,\\n\\tyear = {2003},\\n\\tpages = {3901--3903},\\n}\\n\\n\",\"author_short\":[\"Kaidashev, E. M.\",\"Lorenz, M.\",\"von Wenckstern, H.\",\"Rahm, A.\",\"Semmelhack, H.\",\"Han, K.\",\"Benndorf, G.\",\"Bundesmann, C.\",\"Hochmuth, H.\",\"Grundmann, M.\"],\"key\":\"kaidashev_high_2003\",\"id\":\"kaidashev_high_2003\",\"bibbaseid\":\"kaidashev-lorenz-vonwenckstern-rahm-semmelhack-han-benndorf-bundesmann-etal-highelectronmobilityofepitaxialznothinfilmsoncplanesapphiregrownbymultisteppulsedlaserdeposition-2003\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.1578694\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Fabrication of nano-In$_{\\\\textrm{2}}$O$_{\\\\textrm{3}}$ phase junction by pulse alternating current synthesis for enhanced photoelectrochemical performance: Unravelling the role of synthetic conditions\",\"volume\":\"49\",\"issn\":\"02728842\",\"shorttitle\":\"Fabrication of nano-In2O3 phase junction by pulse alternating current synthesis for enhanced photoelectrochemical performance\",\"url\":\"https://linkinghub.elsevier.com/retrieve/pii/S0272884222043309\",\"doi\":\"10.1016/j.ceramint.2022.11.293\",\"language\":\"en\",\"number\":\"7\",\"urldate\":\"2023-11-11\",\"journal\":\"Ceramics International\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Molodtsova\"],\"firstnames\":[\"Tatyana\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshenkov\"],\"firstnames\":[\"Mikhail\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kolesnikov\"],\"firstnames\":[\"Evgeny\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaichev\"],\"firstnames\":[\"Vasily\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhigunov\"],\"firstnames\":[\"Denis\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Faddeev\"],\"firstnames\":[\"Nikita\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"Alexandra\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2023\",\"keywords\":\"Q1\",\"pages\":\"10986–10992\",\"bibtex\":\"@article{molodtsova_fabrication_2023,\\n\\ttitle = {Fabrication of nano-{In}$_{\\\\textrm{2}}${O}$_{\\\\textrm{3}}$ phase junction by pulse alternating current synthesis for enhanced photoelectrochemical performance: {Unravelling} the role of synthetic conditions},\\n\\tvolume = {49},\\n\\tissn = {02728842},\\n\\tshorttitle = {Fabrication of nano-{In2O3} phase junction by pulse alternating current synthesis for enhanced photoelectrochemical performance},\\n\\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0272884222043309},\\n\\tdoi = {10.1016/j.ceramint.2022.11.293},\\n\\tlanguage = {en},\\n\\tnumber = {7},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ceramics International},\\n\\tauthor = {Molodtsova, Tatyana and Gorshenkov, Mikhail and Kolesnikov, Evgeny and Leontyev, Igor and Kaichev, Vasily and Zhigunov, Denis and Faddeev, Nikita and Kuriganova, Alexandra and Smirnova, Nina},\\n\\tmonth = apr,\\n\\tyear = {2023},\\n\\tkeywords = {Q1},\\n\\tpages = {10986--10992},\\n}\\n\\n\",\"author_short\":[\"Molodtsova, T.\",\"Gorshenkov, M.\",\"Kolesnikov, E.\",\"Leontyev, I.\",\"Kaichev, V.\",\"Zhigunov, D.\",\"Faddeev, N.\",\"Kuriganova, A.\",\"Smirnova, N.\"],\"key\":\"molodtsova_fabrication_2023\",\"id\":\"molodtsova_fabrication_2023\",\"bibbaseid\":\"molodtsova-gorshenkov-kolesnikov-leontyev-kaichev-zhigunov-faddeev-kuriganova-etal-fabricationofnanointextrm2otextrm3phasejunctionbypulsealternatingcurrentsynthesisforenhancedphotoelectrochemicalperformanceunravellingtheroleofsyntheticconditions-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://linkinghub.elsevier.com/retrieve/pii/S0272884222043309\"},\"keyword\":[\"Q1\"],\"metadata\":{\"authorlinks\":{}},\"downloads\":2,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Pulse Electrolysis Technique for Preparation of Bimetal Tin-Containing Electrocatalytic Materials\",\"volume\":\"12\",\"issn\":\"2073-4344\",\"url\":\"https://www.mdpi.com/2073-4344/12/11/1444\",\"doi\":\"10.3390/catal12111444\",\"abstract\":\"Platinum–tin-containing materials are the most popular catalysts for processes occurring in fuel cells with direct ethanol oxidation. Pulse electrolysis based on the electrochemical dispersion of platinum electrodes under the influence of alternating pulse current in an alkaline electrolyte made it possible to introduce the tin component into the catalyst in the form of a dopant, an alloy with platinum, and in the form of an oxide phase and evaluate the effect of the form in which tin is present in the catalyst on its microstructural and electrocatalytic characteristics. The introduction of tin into the catalyst generally increases the rate of ethanol electrooxidation; however, with the most prominent effect observed when tin is present in form of an oxide.\",\"language\":\"en\",\"number\":\"11\",\"urldate\":\"2023-11-11\",\"journal\":\"Catalysts\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"Alexandra\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kubanova\"],\"firstnames\":[\"Marina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Molodtsova\"],\"firstnames\":[\"Tatiana\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2022\",\"pages\":\"1444\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\BTS2JHFX\\\\\\\\Kuriganova и др. - 2022 - Pulse Electrolysis Technique for Preparation of Bi.pdf:application/pdf\",\"bibtex\":\"@article{kuriganova_pulse_2022,\\n\\ttitle = {Pulse {Electrolysis} {Technique} for {Preparation} of {Bimetal} {Tin}-{Containing} {Electrocatalytic} {Materials}},\\n\\tvolume = {12},\\n\\tissn = {2073-4344},\\n\\turl = {https://www.mdpi.com/2073-4344/12/11/1444},\\n\\tdoi = {10.3390/catal12111444},\\n\\tabstract = {Platinum–tin-containing materials are the most popular catalysts for processes occurring in fuel cells with direct ethanol oxidation. Pulse electrolysis based on the electrochemical dispersion of platinum electrodes under the influence of alternating pulse current in an alkaline electrolyte made it possible to introduce the tin component into the catalyst in the form of a dopant, an alloy with platinum, and in the form of an oxide phase and evaluate the effect of the form in which tin is present in the catalyst on its microstructural and electrocatalytic characteristics. The introduction of tin into the catalyst generally increases the rate of ethanol electrooxidation; however, with the most prominent effect observed when tin is present in form of an oxide.},\\n\\tlanguage = {en},\\n\\tnumber = {11},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Catalysts},\\n\\tauthor = {Kuriganova, Alexandra and Kubanova, Marina and Leontyev, Igor and Molodtsova, Tatiana and Smirnova, Nina},\\n\\tmonth = nov,\\n\\tyear = {2022},\\n\\tpages = {1444},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\BTS2JHFX\\\\\\\\Kuriganova и др. - 2022 - Pulse Electrolysis Technique for Preparation of Bi.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Kuriganova, A.\",\"Kubanova, M.\",\"Leontyev, I.\",\"Molodtsova, T.\",\"Smirnova, N.\"],\"key\":\"kuriganova_pulse_2022\",\"id\":\"kuriganova_pulse_2022\",\"bibbaseid\":\"kuriganova-kubanova-leontyev-molodtsova-smirnova-pulseelectrolysistechniqueforpreparationofbimetaltincontainingelectrocatalyticmaterials-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.mdpi.com/2073-4344/12/11/1444\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Role of the Potential Range during Stress Testing of Platinum-Containing Electrocatalysts at Elevated Temperature\",\"volume\":\"12\",\"issn\":\"2073-4344\",\"url\":\"https://www.mdpi.com/2073-4344/12/10/1179\",\"doi\":\"10.3390/catal12101179\",\"abstract\":\"The durability of low temperature proton exchange membrane fuel cell (PEMFC) catalysts crucially affects their lifetime. The choice of carbon support is important in terms of increasing the stability of catalysts. In this research, Pt/C samples were obtained using the polyol synthesis method on two types of carbon supports: the standard support, Vulcan XC-72, and carbon support with a high degree of graphitization, ECS-002402. One method for assessing structural characteristics is through transmission electron microscopy (TEM), according to which materials G1 and G2 showed an average nanoparticle size of 3.7 and 4.2 nm, respectively. On all catalysts, the oxygen reduction reaction proceeded according to the four electron mechanism. Durability was assessed by changes in ESA and activity in the ORR after 1000 cycles, with changes in the upper potential values: 0.7; 1.0; 1.2; and 1.4 V. After accelerated stress testing, the G1 material showed the greatest residual activity at a potential of 1.4 V (165 A/g (Pt). Based on the results of comparing various ADT protocols, the optimal mode of 0.4 and 1.4 V was chosen, and should be used for further studies comparing the durability of Pt/C catalysts.\",\"language\":\"en\",\"number\":\"10\",\"urldate\":\"2023-11-11\",\"journal\":\"Catalysts\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Gerasimova\"],\"firstnames\":[\"Irina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Belenov\"],\"firstnames\":[\"Sergey\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lyanguzov\"],\"firstnames\":[\"Nikolai\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pankov\"],\"firstnames\":[\"Ilya\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tolstunov\"],\"firstnames\":[\"Mikhail\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pavlets\"],\"firstnames\":[\"Angelina\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2022\",\"pages\":\"1179\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\IERK75HA\\\\\\\\Gerasimova и др. - 2022 - Role of the Potential Range during Stress Testing .pdf:application/pdf;Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\G3CGGG63\\\\\\\\Gerasimova и др. - 2022 - Role of the Potential Range during Stress Testing .pdf:application/pdf\",\"bibtex\":\"@article{gerasimova_role_2022,\\n\\ttitle = {Role of the {Potential} {Range} during {Stress} {Testing} of {Platinum}-{Containing} {Electrocatalysts} at {Elevated} {Temperature}},\\n\\tvolume = {12},\\n\\tissn = {2073-4344},\\n\\turl = {https://www.mdpi.com/2073-4344/12/10/1179},\\n\\tdoi = {10.3390/catal12101179},\\n\\tabstract = {The durability of low temperature proton exchange membrane fuel cell (PEMFC) catalysts crucially affects their lifetime. The choice of carbon support is important in terms of increasing the stability of catalysts. In this research, Pt/C samples were obtained using the polyol synthesis method on two types of carbon supports: the standard support, Vulcan XC-72, and carbon support with a high degree of graphitization, ECS-002402. One method for assessing structural characteristics is through transmission electron microscopy (TEM), according to which materials G1 and G2 showed an average nanoparticle size of 3.7 and 4.2 nm, respectively. On all catalysts, the oxygen reduction reaction proceeded according to the four electron mechanism. Durability was assessed by changes in ESA and activity in the ORR after 1000 cycles, with changes in the upper potential values: 0.7; 1.0; 1.2; and 1.4 V. After accelerated stress testing, the G1 material showed the greatest residual activity at a potential of 1.4 V (165 A/g (Pt). Based on the results of comparing various ADT protocols, the optimal mode of 0.4 and 1.4 V was chosen, and should be used for further studies comparing the durability of Pt/C catalysts.},\\n\\tlanguage = {en},\\n\\tnumber = {10},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Catalysts},\\n\\tauthor = {Gerasimova, Irina and Belenov, Sergey and Lyanguzov, Nikolai and Pankov, Ilya and Tolstunov, Mikhail and Pavlets, Angelina},\\n\\tmonth = oct,\\n\\tyear = {2022},\\n\\tpages = {1179},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\IERK75HA\\\\\\\\Gerasimova и др. - 2022 - Role of the Potential Range during Stress Testing .pdf:application/pdf;Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\G3CGGG63\\\\\\\\Gerasimova и др. - 2022 - Role of the Potential Range during Stress Testing .pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Gerasimova, I.\",\"Belenov, S.\",\"Lyanguzov, N.\",\"Pankov, I.\",\"Tolstunov, M.\",\"Pavlets, A.\"],\"key\":\"gerasimova_role_2022\",\"id\":\"gerasimova_role_2022\",\"bibbaseid\":\"gerasimova-belenov-lyanguzov-pankov-tolstunov-pavlets-roleofthepotentialrangeduringstresstestingofplatinumcontainingelectrocatalystsatelevatedtemperature-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.mdpi.com/2073-4344/12/10/1179\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"The Influence of the Elemental Composition, Crystal Structure, and Grain Structure of the Ferro-Piezoceramics of Various Degrees of the Ferro-Hardness on the Stability of the Polarized State\",\"volume\":\"15\",\"issn\":\"1996-1944\",\"url\":\"https://www.mdpi.com/1996-1944/15/6/2118\",\"doi\":\"10.3390/ma15062118\",\"abstract\":\"Ferro-piezoceramic materials (FPCM) with different degrees of ferrohardness were fabricated by double solid-phase synthesis followed by the sintering technique using hot pressing method. The X-ray studies carried out in a wide temperature range showed that with increasing temperature, each of the studied FPCM undergoes a series of phase transformations, accompanied by a change in the symmetry of the unit cell. In this case, near the phase transition to the nonpolar cubic phase, in each of the FPCM, the formation of a fuzzy symmetry region is observed, which is characterized by weak distortions and temperature–time instability of the crystal structure. The study of the piezoelectric modulus d33 in the quasi-static regime as a function of temperature made it possible to reveal the different nature of its behavior in materials of various degrees of ferrohardness. It was shown that the conservation of the state in ferrosoft materials above the Curie temperature is associated with the relaxation nature of the change in their properties, the existence of a region of fuzzy symmetry (noncubic phase) in them above the Curie temperature, and increased inertia of the system. The expediency of taking into account the presented results in the development of electromechanical converters based on FPCM of various degrees of ferrohardness, operated under temperature effects, including cyclic ones, was shown.\",\"language\":\"en\",\"number\":\"6\",\"urldate\":\"2023-11-11\",\"journal\":\"Materials\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Andryushin\"],\"firstnames\":[\"Konstantin\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dudkina\"],\"firstnames\":[\"Svetlana\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sahoo\"],\"firstnames\":[\"Sushrisangita\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shilkina\"],\"firstnames\":[\"Lidiya\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Alyoshin\"],\"firstnames\":[\"Vladimir\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Triger\"],\"firstnames\":[\"Ekaterina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Andryushina\"],\"firstnames\":[\"Inna\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Verbenko\"],\"firstnames\":[\"Iliya\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudskiy\"],\"firstnames\":[\"Daniil\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudskaya\"],\"firstnames\":[\"Angela\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Reznichenko\"],\"firstnames\":[\"Larisa\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2022\",\"pages\":\"2118\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\G8H4F7ND\\\\\\\\Andryushin и др. - 2022 - The Influence of the Elemental Composition, Crysta.pdf:application/pdf;Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\J7PHWKJD\\\\\\\\Andryushin и др. - 2022 - The Influence of the Elemental Composition, Crysta.pdf:application/pdf\",\"bibtex\":\"@article{andryushin_influence_2022,\\n\\ttitle = {The {Influence} of the {Elemental} {Composition}, {Crystal} {Structure}, and {Grain} {Structure} of the {Ferro}-{Piezoceramics} of {Various} {Degrees} of the {Ferro}-{Hardness} on the {Stability} of the {Polarized} {State}},\\n\\tvolume = {15},\\n\\tissn = {1996-1944},\\n\\turl = {https://www.mdpi.com/1996-1944/15/6/2118},\\n\\tdoi = {10.3390/ma15062118},\\n\\tabstract = {Ferro-piezoceramic materials (FPCM) with different degrees of ferrohardness were fabricated by double solid-phase synthesis followed by the sintering technique using hot pressing method. The X-ray studies carried out in a wide temperature range showed that with increasing temperature, each of the studied FPCM undergoes a series of phase transformations, accompanied by a change in the symmetry of the unit cell. In this case, near the phase transition to the nonpolar cubic phase, in each of the FPCM, the formation of a fuzzy symmetry region is observed, which is characterized by weak distortions and temperature–time instability of the crystal structure. The study of the piezoelectric modulus d33 in the quasi-static regime as a function of temperature made it possible to reveal the different nature of its behavior in materials of various degrees of ferrohardness. It was shown that the conservation of the state in ferrosoft materials above the Curie temperature is associated with the relaxation nature of the change in their properties, the existence of a region of fuzzy symmetry (noncubic phase) in them above the Curie temperature, and increased inertia of the system. The expediency of taking into account the presented results in the development of electromechanical converters based on FPCM of various degrees of ferrohardness, operated under temperature effects, including cyclic ones, was shown.},\\n\\tlanguage = {en},\\n\\tnumber = {6},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Materials},\\n\\tauthor = {Andryushin, Konstantin and Dudkina, Svetlana and Sahoo, Sushrisangita and Shilkina, Lidiya and Alyoshin, Vladimir and Triger, Ekaterina and Andryushina, Inna and Verbenko, Iliya and Rudskiy, Daniil and Rudskaya, Angela and Reznichenko, Larisa},\\n\\tmonth = mar,\\n\\tyear = {2022},\\n\\tpages = {2118},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\G8H4F7ND\\\\\\\\Andryushin и др. - 2022 - The Influence of the Elemental Composition, Crysta.pdf:application/pdf;Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\J7PHWKJD\\\\\\\\Andryushin и др. - 2022 - The Influence of the Elemental Composition, Crysta.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Andryushin, K.\",\"Dudkina, S.\",\"Sahoo, S.\",\"Shilkina, L.\",\"Alyoshin, V.\",\"Triger, E.\",\"Andryushina, I.\",\"Verbenko, I.\",\"Rudskiy, D.\",\"Rudskaya, A.\",\"Reznichenko, L.\"],\"key\":\"andryushin_influence_2022\",\"id\":\"andryushin_influence_2022\",\"bibbaseid\":\"andryushin-dudkina-sahoo-shilkina-alyoshin-triger-andryushina-verbenko-etal-theinfluenceoftheelementalcompositioncrystalstructureandgrainstructureoftheferropiezoceramicsofvariousdegreesoftheferrohardnessonthestabilityofthepolarizedstate-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.mdpi.com/1996-1944/15/6/2118\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Moiré patterns and carbon nanotube sorting\",\"volume\":\"6\",\"issn\":\"2399-1984\",\"url\":\"https://iopscience.iop.org/article/10.1088/2399-1984/ac4a27\",\"doi\":\"10.1088/2399-1984/ac4a27\",\"abstract\":\"Abstract Moiré patterns (MPs), arising from the superposition of two lattices with close periods, are tightly related to the physicochemical properties of bilayer nanostructures. Here, we develop the theory of complex MPs emerging in twisted bilayer graphene and planar nets of double-walled nanotubes at significant relative twist and/or deformation of layers. The proposed theory clarifies the physicochemical regularities arising at sorting of single-walled carbon nanotubes (SWCNTs) by organic molecules, which self-assemble in regular coatings on both the tubes and planar graphene. We introduce and consider an outer tubular virtual lattice that is a parent structure for the deposited coating and due to this fact, its existence is crucial for the coating formation. As we show, such outer lattices exist only for successfully sorted SWCNTs and the superposition between the outer lattice and SWCNT forms a specific long-period MP. We explain known experimental results of SWCNT sorting by molecules of flavin group, poly(9,9-dioctylfluorene-2,7-diyl), and poly [(m-phenylenevinylene)-alt-(p-phenylenevinylene)]. Also, our approach points out other organic molecules and polymers suitable for effective carbon nanotube sorting.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Nano Futures\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Konevtsova\"],\"firstnames\":[\"Olga\",\"V\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Roshal\"],\"firstnames\":[\"Daria\",\"S\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergei\",\"B\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2022\",\"pages\":\"015005\",\"bibtex\":\"@article{konevtsova_moire_2022,\\n\\ttitle = {Moiré patterns and carbon nanotube sorting},\\n\\tvolume = {6},\\n\\tissn = {2399-1984},\\n\\turl = {https://iopscience.iop.org/article/10.1088/2399-1984/ac4a27},\\n\\tdoi = {10.1088/2399-1984/ac4a27},\\n\\tabstract = {Abstract\\n            Moiré patterns (MPs), arising from the superposition of two lattices with close periods, are tightly related to the physicochemical properties of bilayer nanostructures. Here, we develop the theory of complex MPs emerging in twisted bilayer graphene and planar nets of double-walled nanotubes at significant relative twist and/or deformation of layers. The proposed theory clarifies the physicochemical regularities arising at sorting of single-walled carbon nanotubes (SWCNTs) by organic molecules, which self-assemble in regular coatings on both the tubes and planar graphene. We introduce and consider an outer tubular virtual lattice that is a parent structure for the deposited coating and due to this fact, its existence is crucial for the coating formation. As we show, such outer lattices exist only for successfully sorted SWCNTs and the superposition between the outer lattice and SWCNT forms a specific long-period MP. We explain known experimental results of SWCNT sorting by molecules of flavin group, poly(9,9-dioctylfluorene-2,7-diyl), and poly [(m-phenylenevinylene)-alt-(p-phenylenevinylene)]. Also, our approach points out other organic molecules and polymers suitable for effective carbon nanotube sorting.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Nano Futures},\\n\\tauthor = {Konevtsova, Olga V and Roshal, Daria S and Rochal, Sergei B},\\n\\tmonth = mar,\\n\\tyear = {2022},\\n\\tpages = {015005},\\n}\\n\\n\",\"author_short\":[\"Konevtsova, O. V\",\"Roshal, D. S\",\"Rochal, S. B\"],\"key\":\"konevtsova_moire_2022\",\"id\":\"konevtsova_moire_2022\",\"bibbaseid\":\"konevtsova-roshal-rochal-moirpatternsandcarbonnanotubesorting-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://iopscience.iop.org/article/10.1088/2399-1984/ac4a27\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Tight-binding approximation for bilayer graphene and nanotube structures: From commensurability to incommensurability between the layers\",\"volume\":\"105\",\"issn\":\"2469-9950, 2469-9969\",\"shorttitle\":\"Tight-binding approximation for bilayer graphene and nanotube structures\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.105.045402\",\"doi\":\"10.1103/PhysRevB.105.045402\",\"language\":\"en\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Chalin\"],\"firstnames\":[\"D.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Levshov\"],\"firstnames\":[\"D.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Myasnikova\"],\"firstnames\":[\"A.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2022\",\"pages\":\"045402\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\MDNW4VT5\\\\\\\\Chalin и др. - 2022 - Tight-binding approximation for bilayer graphene a.pdf:application/pdf;Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\VM6EQJBB\\\\\\\\Chalin и др. - 2022 - Tight-binding approximation for bilayer graphene a.pdf:application/pdf\",\"bibtex\":\"@article{chalin_tight-binding_2022,\\n\\ttitle = {Tight-binding approximation for bilayer graphene and nanotube structures: {From} commensurability to incommensurability between the layers},\\n\\tvolume = {105},\\n\\tissn = {2469-9950, 2469-9969},\\n\\tshorttitle = {Tight-binding approximation for bilayer graphene and nanotube structures},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.105.045402},\\n\\tdoi = {10.1103/PhysRevB.105.045402},\\n\\tlanguage = {en},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Chalin, D. V. and Levshov, D. I. and Myasnikova, A. E. and Rochal, S. B.},\\n\\tmonth = jan,\\n\\tyear = {2022},\\n\\tpages = {045402},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\MDNW4VT5\\\\\\\\Chalin и др. - 2022 - Tight-binding approximation for bilayer graphene a.pdf:application/pdf;Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\VM6EQJBB\\\\\\\\Chalin и др. - 2022 - Tight-binding approximation for bilayer graphene a.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Chalin, D. V.\",\"Levshov, D. I.\",\"Myasnikova, A. E.\",\"Rochal, S. B.\"],\"key\":\"chalin_tight-binding_2022\",\"id\":\"chalin_tight-binding_2022\",\"bibbaseid\":\"chalin-levshov-myasnikova-rochal-tightbindingapproximationforbilayergrapheneandnanotubestructuresfromcommensurabilitytoincommensurabilitybetweenthelayers-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.105.045402\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Efficiency of Generation of Surface Acoustic Waves in Barium Strontium Titanate Thin Films\",\"volume\":\"69\",\"issn\":\"0885-3010, 1525-8955\",\"url\":\"https://ieeexplore.ieee.org/document/9744607/\",\"doi\":\"10.1109/TUFFC.2022.3163610\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"Vladimir\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"Pavel\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kalinchuk\"],\"firstnames\":[\"Valery\",\"V.\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2022\",\"pages\":\"1815–1820\",\"bibtex\":\"@article{shirokov_efficiency_2022,\\n\\ttitle = {Efficiency of {Generation} of {Surface} {Acoustic} {Waves} in {Barium} {Strontium} {Titanate} {Thin} {Films}},\\n\\tvolume = {69},\\n\\tissn = {0885-3010, 1525-8955},\\n\\turl = {https://ieeexplore.ieee.org/document/9744607/},\\n\\tdoi = {10.1109/TUFFC.2022.3163610},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control},\\n\\tauthor = {Shirokov, Vladimir B. and Timoshenko, Pavel E. and Kalinchuk, Valery V.},\\n\\tmonth = may,\\n\\tyear = {2022},\\n\\tpages = {1815--1820},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Timoshenko, P. E.\",\"Kalinchuk, V. V.\"],\"key\":\"shirokov_efficiency_2022\",\"id\":\"shirokov_efficiency_2022\",\"bibbaseid\":\"shirokov-timoshenko-kalinchuk-efficiencyofgenerationofsurfaceacousticwavesinbariumstrontiumtitanatethinfilms-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://ieeexplore.ieee.org/document/9744607/\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Random nature of epithelial cancer cell monolayers\",\"volume\":\"19\",\"issn\":\"1742-5662\",\"url\":\"https://royalsocietypublishing.org/doi/10.1098/rsif.2022.0026\",\"doi\":\"10.1098/rsif.2022.0026\",\"abstract\":\"Although the polygonal shape of epithelial cells has been drawing the attention of scientists for several centuries, only a decade and a half ago it was demonstrated that distributions of polygon types (DOPTs) are similar in proliferative epithelia of many different plant and animal species. In this study, we show that hyper-proliferation of cancer cells disrupts this universal paradigm and results in randomly organized epithelial structures. Examining non-synchronized and synchronized HeLa cervix cells, we suppose that the spread of cell sizes is the main parameter controlling the DOPT in the cancer cell monolayers. To test this hypothesis, we develop a theory of morphologically similar random polygonal packings. By analysing differences between tumoural and normal epithelial cell monolayers, we conclude that the latter have more ordered structures because of their lower proliferation rates and, consequently, more effective relaxation of mechanical stress associated with cell division and growth. To explain the structural features of normal proliferative epithelium, we take into account the spread of cell sizes in the monolayer. The proposed theory also rationalizes some highly ordered unconventional post-mitotic epithelia.\",\"language\":\"en\",\"number\":\"190\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of The Royal Society Interface\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Roshal\"],\"firstnames\":[\"Daria\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Martin\"],\"firstnames\":[\"Marianne\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fedorenko\"],\"firstnames\":[\"Kirill\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golushko\"],\"firstnames\":[\"Ivan\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Molle\"],\"firstnames\":[\"Virginie\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Baghdiguian\"],\"firstnames\":[\"Stephen\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergei\",\"B.\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2022\",\"pages\":\"20220026\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\9ZQ6KFAD\\\\\\\\Roshal и др. - 2022 - Random nature of epithelial cancer cell monolayers.pdf:application/pdf\",\"bibtex\":\"@article{roshal_random_2022,\\n\\ttitle = {Random nature of epithelial cancer cell monolayers},\\n\\tvolume = {19},\\n\\tissn = {1742-5662},\\n\\turl = {https://royalsocietypublishing.org/doi/10.1098/rsif.2022.0026},\\n\\tdoi = {10.1098/rsif.2022.0026},\\n\\tabstract = {Although the polygonal shape of epithelial cells has been drawing the attention of scientists for several centuries, only a decade and a half ago it was demonstrated that distributions of polygon types (DOPTs) are similar in proliferative epithelia of many different plant and animal species. In this study, we show that hyper-proliferation of cancer cells disrupts this universal paradigm and results in randomly organized epithelial structures. Examining non-synchronized and synchronized HeLa cervix cells, we suppose that the spread of cell sizes is the main parameter controlling the DOPT in the cancer cell monolayers. To test this hypothesis, we develop a theory of morphologically similar random polygonal packings. By analysing differences between tumoural and normal epithelial cell monolayers, we conclude that the latter have more ordered structures because of their lower proliferation rates and, consequently, more effective relaxation of mechanical stress associated with cell division and growth. To explain the structural features of normal proliferative epithelium, we take into account the spread of cell sizes in the monolayer. The proposed theory also rationalizes some highly ordered unconventional post-mitotic epithelia.},\\n\\tlanguage = {en},\\n\\tnumber = {190},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of The Royal Society Interface},\\n\\tauthor = {Roshal, Daria S. and Martin, Marianne and Fedorenko, Kirill and Golushko, Ivan and Molle, Virginie and Baghdiguian, Stephen and Rochal, Sergei B.},\\n\\tmonth = may,\\n\\tyear = {2022},\\n\\tpages = {20220026},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\9ZQ6KFAD\\\\\\\\Roshal и др. - 2022 - Random nature of epithelial cancer cell monolayers.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Roshal, D. S.\",\"Martin, M.\",\"Fedorenko, K.\",\"Golushko, I.\",\"Molle, V.\",\"Baghdiguian, S.\",\"Rochal, S. B.\"],\"key\":\"roshal_random_2022\",\"id\":\"roshal_random_2022\",\"bibbaseid\":\"roshal-martin-fedorenko-golushko-molle-baghdiguian-rochal-randomnatureofepithelialcancercellmonolayers-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://royalsocietypublishing.org/doi/10.1098/rsif.2022.0026\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":1,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"The effects of the modification of the BST-system solid solutions with rare earth elements\",\"volume\":\"48\",\"issn\":\"02728842\",\"url\":\"https://linkinghub.elsevier.com/retrieve/pii/S0272884221030534\",\"doi\":\"10.1016/j.ceramint.2021.09.243\",\"language\":\"en\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Ceramics International\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Andryushin\"],\"firstnames\":[\"K.P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shilkina\"],\"firstnames\":[\"L.A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Khasbulatov\"],\"firstnames\":[\"S.V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nagaenko\"],\"firstnames\":[\"A.V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dudkina\"],\"firstnames\":[\"S.I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Andryushina\"],\"firstnames\":[\"I.N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sadykov\"],\"firstnames\":[\"KhA.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Verbenko\"],\"firstnames\":[\"I.A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudskaya\"],\"firstnames\":[\"A.G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Reznichenko\"],\"firstnames\":[\"L.A.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2022\",\"pages\":\"1642–1658\",\"bibtex\":\"@article{andryushin_effects_2022,\\n\\ttitle = {The effects of the modification of the {BST}-system solid solutions with rare earth elements},\\n\\tvolume = {48},\\n\\tissn = {02728842},\\n\\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0272884221030534},\\n\\tdoi = {10.1016/j.ceramint.2021.09.243},\\n\\tlanguage = {en},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ceramics International},\\n\\tauthor = {Andryushin, K.P. and Shilkina, L.A. and Khasbulatov, S.V. and Nagaenko, A.V. and Dudkina, S.I. and Andryushina, I.N. and Sadykov, KhA. and Verbenko, I.A. and Rudskaya, A.G. and Reznichenko, L.A.},\\n\\tmonth = jan,\\n\\tyear = {2022},\\n\\tpages = {1642--1658},\\n}\\n\\n\",\"author_short\":[\"Andryushin, K.\",\"Shilkina, L.\",\"Khasbulatov, S.\",\"Nagaenko, A.\",\"Dudkina, S.\",\"Andryushina, I.\",\"Sadykov, K.\",\"Verbenko, I.\",\"Rudskaya, A.\",\"Reznichenko, L.\"],\"key\":\"andryushin_effects_2022\",\"id\":\"andryushin_effects_2022\",\"bibbaseid\":\"andryushin-shilkina-khasbulatov-nagaenko-dudkina-andryushina-sadykov-verbenko-etal-theeffectsofthemodificationofthebstsystemsolidsolutionswithrareearthelements-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://linkinghub.elsevier.com/retrieve/pii/S0272884221030534\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Hidden symmetry of the flavivirus protein shell and pH-controlled reconstruction of the viral surface\",\"volume\":\"11\",\"issn\":\"2047-4830, 2047-4849\",\"url\":\"http://xlink.rsc.org/?DOI=D2BM01562E\",\"doi\":\"10.1039/D2BM01562E\",\"abstract\":\"A pH-induced change in the charge distribution of proteins leads to a structural transformation of the outer flavivirus shell, which violates the hidden symmetry of the mutual arrangement of proteins located on opposite sides of the lipid membrane. , Using recent Zika virus structural data we reveal a hidden symmetry of protein order in immature and mature flavivirus shells, violating the Caspar–Klug paradigmatic model of capsid structures. We show that proteins of the outer immature shell layer exhibit trihexagonal tiling, while proteins from inner and outer layers conjointly form a double-shelled close-packed structure, based on a common triangular spherical lattice. Within the proposed structural model, we furthermore rationalize the structural organization of misassembled non-infectious subviral particles that have no inner capsid. We consider a pH-controlled structural reconstruction of the outer shell from the trimeric to the dimeric state, and demonstrate that this transition, occurring during the virus maturation, can be induced by changes in protein charges at lower pH, leading to a decrease in the electrostatic interaction free energy. This transition could also be assisted by electrostatic attraction of shell proteins to the interposed lipid membrane substrate separating the shells.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Biomaterials Science\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Konevtsova\"],\"firstnames\":[\"Olga\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golushko\"],\"firstnames\":[\"Ivan\",\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Podgornik\"],\"firstnames\":[\"Rudolf\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergei\",\"B.\"],\"suffixes\":[]}],\"year\":\"2023\",\"keywords\":\"Q1\",\"pages\":\"225–234\",\"bibtex\":\"@article{konevtsova_hidden_2023,\\n\\ttitle = {Hidden symmetry of the flavivirus protein shell and {pH}-controlled reconstruction of the viral surface},\\n\\tvolume = {11},\\n\\tissn = {2047-4830, 2047-4849},\\n\\turl = {http://xlink.rsc.org/?DOI=D2BM01562E},\\n\\tdoi = {10.1039/D2BM01562E},\\n\\tabstract = {A pH-induced change in the charge distribution of proteins leads to a structural transformation of the outer flavivirus shell, which violates the hidden symmetry of the mutual arrangement of proteins located on opposite sides of the lipid membrane.\\n          , \\n            Using recent Zika virus structural data we reveal a hidden symmetry of protein order in immature and mature flavivirus shells, violating the Caspar–Klug paradigmatic model of capsid structures. We show that proteins of the outer immature shell layer exhibit trihexagonal tiling, while proteins from inner and outer layers conjointly form a double-shelled close-packed structure, based on a common triangular spherical lattice. Within the proposed structural model, we furthermore rationalize the structural organization of misassembled non-infectious subviral particles that have no inner capsid. We consider a pH-controlled structural reconstruction of the outer shell from the trimeric to the dimeric state, and demonstrate that this transition, occurring during the virus maturation, can be induced by changes in protein charges at lower pH, leading to a decrease in the electrostatic interaction free energy. This transition could also be assisted by electrostatic attraction of shell proteins to the interposed lipid membrane substrate separating the shells.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Biomaterials Science},\\n\\tauthor = {Konevtsova, Olga V. and Golushko, Ivan Yu. and Podgornik, Rudolf and Rochal, Sergei B.},\\n\\tyear = {2023},\\n\\tkeywords = {Q1},\\n\\tpages = {225--234},\\n}\\n\\n\",\"author_short\":[\"Konevtsova, O. V.\",\"Golushko, I. Y.\",\"Podgornik, R.\",\"Rochal, S. B.\"],\"key\":\"konevtsova_hidden_2023\",\"id\":\"konevtsova_hidden_2023\",\"bibbaseid\":\"konevtsova-golushko-podgornik-rochal-hiddensymmetryoftheflavivirusproteinshellandphcontrolledreconstructionoftheviralsurface-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://xlink.rsc.org/?DOI=D2BM01562E\"},\"keyword\":[\"Q1\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Структура и динамика решетки твердых растворов (1-x)BiFeO$_{\\\\textrm{3}}$-xANbO$_{\\\\textrm{3}}$ (A-K, Na)\",\"volume\":\"56\",\"url\":\"http://journals.ioffe.ru/articles/40748\",\"abstract\":\"Методами рентгеновской порошковой дифракции и комбинационного рассеяния света изучены структуры и динамические характеристики решеток составов двух систем твердых растворов мультиферроика BiFeO3 с сегнетоэлектриком KNbO3 и антисегнетоэлектриком NaNbO3: (1-x)BiFeO3-xKNbO3 и (1-x)BiFeO3-xNaNbO3. Для этих систем в составах с x=0.3, 0.5 и 0.7 при комнатной температуре определены симметрия, параметры элементарных ячеек. Из анализа колебательных спектров установлены последовательности ротационных искажений при изменении концентраций в этих системах твердых растворов.\",\"language\":\"ru\",\"number\":\"9\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Тесленко\"],\"firstnames\":[\"П.\",\"Ю.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Разумная\"],\"firstnames\":[\"А.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Пономоренко\"],\"firstnames\":[\"В.\",\"О.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Рудская\"],\"firstnames\":[\"А.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Назаренко\"],\"firstnames\":[\"А.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Анохин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Авраменко\"],\"firstnames\":[\"М.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Левшов\"],\"firstnames\":[\"Д.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Куприянов\"],\"firstnames\":[\"М.\",\"Ф.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2014\",\"pages\":\"1804–18010\",\"bibtex\":\"@article{__2014,\\n\\ttitle = {Структура и динамика решетки твердых растворов (1-x){BiFeO}$_{\\\\textrm{3}}$-{xANbO}$_{\\\\textrm{3}}$ ({A}-{K}, {Na})},\\n\\tvolume = {56},\\n\\turl = {http://journals.ioffe.ru/articles/40748},\\n\\tabstract = {Методами рентгеновской порошковой дифракции и комбинационного рассеяния света изучены структуры и динамические характеристики решеток составов двух систем твердых растворов мультиферроика BiFeO3 с сегнетоэлектриком KNbO3 и антисегнетоэлектриком NaNbO3: (1-x)BiFeO3-xKNbO3 и (1-x)BiFeO3-xNaNbO3. Для этих систем в составах с x=0.3, 0.5 и 0.7 при комнатной температуре определены симметрия, параметры элементарных ячеек. Из анализа колебательных спектров установлены последовательности ротационных искажений при изменении концентраций в этих системах твердых растворов.},\\n\\tlanguage = {ru},\\n\\tnumber = {9},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Тесленко, П. Ю. and Разумная, А. Г. and Пономоренко, В. О. and Рудская, А. Г. and Назаренко, А. В. and Анохин, А. С. and Авраменко, М. В. and Левшов, Д. И. and Куприянов, М. Ф. and Юзюк, Ю. И.},\\n\\tmonth = aug,\\n\\tyear = {2014},\\n\\tpages = {1804--18010},\\n}\\n\\n\",\"author_short\":[\"Тесленко, П. Ю.\",\"Разумная, А. Г.\",\"Пономоренко, В. О.\",\"Рудская, А. Г.\",\"Назаренко, А. В.\",\"Анохин, А. С.\",\"Авраменко, М. В.\",\"Левшов, Д. И.\",\"Куприянов, М. Ф.\",\"Юзюк, Ю. И.\"],\"key\":\"__2014\",\"id\":\"__2014\",\"bibbaseid\":\"--------etal-1xbifeotextrm3xanbotextrm3akna-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/40748\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Спектроскопия комбинационного рассеяния света как метод диагностики структуры индивидуальных углеродных нанотрубок\",\"url\":\"http://www.ivdon.ru/magazine/archive/n4y2013/1972\",\"abstract\":\"Сетевой научный журнал «Инженерный вестник Дона»\",\"language\":\"ru\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Левшов\"],\"firstnames\":[\"Д.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Авраменко\"],\"firstnames\":[\"М.\",\"В.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2013\",\"bibtex\":\"@article{__2013-6,\\n\\ttitle = {Спектроскопия комбинационного рассеяния света как метод диагностики структуры индивидуальных углеродных нанотрубок},\\n\\turl = {http://www.ivdon.ru/magazine/archive/n4y2013/1972},\\n\\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\\n\\tlanguage = {ru},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Левшов, Д. И. and Авраменко, М. В.},\\n\\tmonth = jul,\\n\\tyear = {2013},\\n}\\n\\n\",\"author_short\":[\"Левшов, Д. И.\",\"Авраменко, М. В.\"],\"key\":\"__2013-6\",\"id\":\"__2013-6\",\"bibbaseid\":\"---2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://www.ivdon.ru/magazine/archive/n4y2013/1972\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Низкотемпературный термический синтез наностержней оксида цинка из паров цинка без катализатора\",\"url\":\"http://www.ivdon.ru/magazine/archive/n4y2013/1884\",\"abstract\":\"Сетевой научный журнал «Инженерный вестник Дона»\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Пушкарев\"],\"firstnames\":[\"В.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2013\",\"bibtex\":\"@article{__2013-7,\\n\\ttitle = {Низкотемпературный термический синтез наностержней оксида цинка из паров цинка без катализатора},\\n\\turl = {http://www.ivdon.ru/magazine/archive/n4y2013/1884},\\n\\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Пушкарев, В. И. and Лянгузов, Н. В. and Кайдашев, Е. М.},\\n\\tmonth = aug,\\n\\tyear = {2013},\\n}\\n\\n\",\"author_short\":[\"Пушкарев, В. И.\",\"Лянгузов, Н. В.\",\"Кайдашев, Е. М.\"],\"key\":\"__2013-7\",\"id\":\"__2013-7\",\"bibbaseid\":\"----2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://www.ivdon.ru/magazine/archive/n4y2013/1884\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":3,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Фазовращатель на щелевой линии, нагруженный варакторами на основе наноразмерных пленок титаната бария-стронция\",\"volume\":\"52\",\"issn\":\"0033-8494\",\"url\":\"http://naukarus.com/fazovraschatel-na-schelevoy-linii-nagruzhennoy-varaktorami-na-osnove-nanorazmernyh-plenok-titanata-bariya-strontsiya\",\"abstract\":\"Реализован монолитный фазовращатель на щелевой линии передачи, периодически нагруженной сегнетоэлектрическими варакторами на основе наноразмерных пленок Bа0.8Sr0.2TiO3. Установлено, что при уменьшении толщины наноразмерной сегнетоэлектрической пленки, на основе которой реализованы варакторы, от 36 до 18 нм коэффициент качества фазовращателя в полосе частот от 12 до 13.5 ГГц возрастает более чем в два раза.\",\"language\":\"ru\",\"number\":\"11\",\"urldate\":\"2023-11-11\",\"journal\":\"Радиотехника и электроника\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Масычев\"],\"firstnames\":[\"С.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"Вас.М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"Вл.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Чуб\"],\"firstnames\":[\"А.\",\"В.\"],\"suffixes\":[]}],\"year\":\"2007\",\"keywords\":\"⛔ No DOI found\",\"file\":\"Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\NC57SS3Z\\\\\\\\fazovraschatel-na-schelevoy-linii-nagruzhennoy-varaktorami-na-osnove-nanorazmernyh-plenok-titan.html:text/html\",\"bibtex\":\"@article{__2007,\\n\\ttitle = {Фазовращатель на щелевой линии, нагруженный варакторами на основе наноразмерных пленок титаната бария-стронция},\\n\\tvolume = {52},\\n\\tissn = {0033-8494},\\n\\turl = {http://naukarus.com/fazovraschatel-na-schelevoy-linii-nagruzhennoy-varaktorami-na-osnove-nanorazmernyh-plenok-titanata-bariya-strontsiya},\\n\\tabstract = {Реализован монолитный фазовращатель на щелевой линии передачи, периодически нагруженной сегнетоэлектрическими варакторами на основе наноразмерных пленок Bа0.8Sr0.2TiO3. Установлено, что при уменьшении толщины наноразмерной сегнетоэлектрической пленки, на основе которой реализованы варакторы, от 36 до 18 нм коэффициент качества фазовращателя в полосе частот от 12 до 13.5 ГГц возрастает более чем в два раза.},\\n\\tlanguage = {ru},\\n\\tnumber = {11},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Радиотехника и электроника},\\n\\tauthor = {Головко, Ю. И. and Масычев, С. И. and Мухортов, Вас.М. and Мухортов, Вл. М. and Чуб, А. В.},\\n\\tyear = {2007},\\n\\tkeywords = {⛔ No DOI found},\\n\\tfile = {Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\NC57SS3Z\\\\\\\\fazovraschatel-na-schelevoy-linii-nagruzhennoy-varaktorami-na-osnove-nanorazmernyh-plenok-titan.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Головко, Ю. И.\",\"Масычев, С. И.\",\"Мухортов, В.\",\"Мухортов, В. М.\",\"Чуб, А. В.\"],\"key\":\"__2007\",\"id\":\"__2007\",\"bibbaseid\":\"------2007\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://naukarus.com/fazovraschatel-na-schelevoy-linii-nagruzhennoy-varaktorami-na-osnove-nanorazmernyh-plenok-titanata-bariya-strontsiya\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Новый датчик динамической деформации на основе тонких пьезоэлектрических пленок, полученных ионноплазменным напылением\",\"volume\":\"58\",\"issn\":\"1999-9429\",\"url\":\"https://cyberleninka.ru/article/n/novyy-datchik-dinamicheskoy-deformatsii-na-osnove-tonkih-piezoelektricheskih-plenok-poluchennyh-ionnoplazmennym-napyleniem\",\"language\":\"ru\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Известия Южного федерального университета. Технические науки\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"Вл.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"Вас.М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бирюков\"],\"firstnames\":[\"С.\",\"В.\"],\"suffixes\":[]}],\"year\":\"2006\",\"note\":\"Number: 3 Place: Россия, Ростов-на-Дону Publisher: Федеральное государственное автономное образовательное учреждение высшего образования «Южный федеральный университет»\",\"keywords\":\"⛔ No DOI found\",\"pages\":\"221–227\",\"file\":\"Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\D4V7B898\\\\\\\\В.м и др. - 2006 - Новый датчик динамической деформации на основе тон.pdf:application/pdf\",\"bibtex\":\"@article{__2006,\\n\\ttitle = {Новый датчик динамической деформации на основе тонких пьезоэлектрических пленок, полученных ионноплазменным напылением},\\n\\tvolume = {58},\\n\\tissn = {1999-9429},\\n\\turl = {https://cyberleninka.ru/article/n/novyy-datchik-dinamicheskoy-deformatsii-na-osnove-tonkih-piezoelektricheskih-plenok-poluchennyh-ionnoplazmennym-napyleniem},\\n\\tlanguage = {ru},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Известия Южного федерального университета. Технические науки},\\n\\tauthor = {Мухортов, Вл. М. and Мухортов, Вас.М. and Бирюков, С. В.},\\n\\tyear = {2006},\\n\\tnote = {Number: 3\\nPlace: Россия, Ростов-на-Дону\\nPublisher: Федеральное государственное автономное образовательное учреждение высшего образования «Южный федеральный университет»},\\n\\tkeywords = {⛔ No DOI found},\\n\\tpages = {221--227},\\n\\tfile = {Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\D4V7B898\\\\\\\\В.м и др. - 2006 - Новый датчик динамической деформации на основе тон.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Мухортов, В. М.\",\"Мухортов, В.\",\"Бирюков, С. В.\"],\"key\":\"__2006\",\"id\":\"__2006\",\"bibbaseid\":\"----2006\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://cyberleninka.ru/article/n/novyy-datchik-dinamicheskoy-deformatsii-na-osnove-tonkih-piezoelektricheskih-plenok-poluchennyh-ionnoplazmennym-napyleniem\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Анализ атомной структуры углеродных нанотрубок методами спектроскопии комбинационного рассеяния света и электронной дифракции\",\"url\":\"http://www.ivdon.ru/ru/magazine/archive/N4y2014/2679\",\"abstract\":\"Сетевой научный журнал «Инженерный вестник Дона»\",\"language\":\"ru\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Инженерный Вестник Дона\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Левшов\"],\"firstnames\":[\"Д.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Авраменко\"],\"firstnames\":[\"М.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Пимонов\"],\"firstnames\":[\"В.\",\"В.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2014\",\"keywords\":\"⛔ No DOI found\",\"pages\":\"1–11\",\"file\":\"Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\8MAPFW2E\\\\\\\\2679.html:text/html\",\"bibtex\":\"@article{__2014-1,\\n\\ttitle = {Анализ атомной структуры углеродных нанотрубок методами спектроскопии комбинационного рассеяния света и электронной дифракции},\\n\\turl = {http://www.ivdon.ru/ru/magazine/archive/N4y2014/2679},\\n\\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\\n\\tlanguage = {ru},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Инженерный Вестник Дона},\\n\\tauthor = {Левшов, Д. И. and Авраменко, М. В. and Пимонов, В. В.},\\n\\tmonth = jun,\\n\\tyear = {2014},\\n\\tkeywords = {⛔ No DOI found},\\n\\tpages = {1--11},\\n\\tfile = {Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\8MAPFW2E\\\\\\\\2679.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Левшов, Д. И.\",\"Авраменко, М. В.\",\"Пимонов, В. В.\"],\"key\":\"__2014-1\",\"id\":\"__2014-1\",\"bibbaseid\":\"----2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://www.ivdon.ru/ru/magazine/archive/N4y2014/2679\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Влияние эффектов окружения на колебательные свойства индивидуальных углеродных нанотрубок\",\"url\":\"http://www.ivdon.ru/ru/magazine/archive/N4y2014/2680\",\"abstract\":\"Сетевой научный журнал «Инженерный вестник Дона»\",\"language\":\"ru\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Инженерный Вестник Дона\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Левшов\"],\"firstnames\":[\"Д.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Авраменко\"],\"firstnames\":[\"М.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Пимонов\"],\"firstnames\":[\"В.\",\"В.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2014\",\"keywords\":\"⛔ No DOI found\",\"pages\":\"1–14\",\"file\":\"Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\ZAP3J5ZW\\\\\\\\2680.html:text/html\",\"bibtex\":\"@article{__2014-2,\\n\\ttitle = {Влияние эффектов окружения на колебательные свойства индивидуальных углеродных нанотрубок},\\n\\turl = {http://www.ivdon.ru/ru/magazine/archive/N4y2014/2680},\\n\\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\\n\\tlanguage = {ru},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Инженерный Вестник Дона},\\n\\tauthor = {Левшов, Д. И. and Авраменко, М. В. and Пимонов, В. В.},\\n\\tmonth = jun,\\n\\tyear = {2014},\\n\\tkeywords = {⛔ No DOI found},\\n\\tpages = {1--14},\\n\\tfile = {Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\ZAP3J5ZW\\\\\\\\2680.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Левшов, Д. И.\",\"Авраменко, М. В.\",\"Пимонов, В. В.\"],\"key\":\"__2014-2\",\"id\":\"__2014-2\",\"bibbaseid\":\"----2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://www.ivdon.ru/ru/magazine/archive/N4y2014/2680\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Температурная зависимость двухмагнонных возбуждений в пленках феррита висмута легированного неодимом\",\"url\":\"http://www.ivdon.ru/ru/magazine/archive/N4y2014/2681\",\"abstract\":\"Сетевой научный журнал «Инженерный вестник Дона»\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Кхабири\"],\"firstnames\":[\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Разумная\"],\"firstnames\":[\"А.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2014\",\"keywords\":\"⛔ No DOI found\",\"file\":\"Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\NBC8JXKZ\\\\\\\\2681.html:text/html\",\"bibtex\":\"@article{__2014-3,\\n\\ttitle = {Температурная зависимость двухмагнонных возбуждений в пленках феррита висмута легированного неодимом},\\n\\turl = {http://www.ivdon.ru/ru/magazine/archive/N4y2014/2681},\\n\\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Кхабири, Г. and Разумная, А. Г. and Юзюк, Ю. И.},\\n\\tmonth = may,\\n\\tyear = {2014},\\n\\tkeywords = {⛔ No DOI found},\\n\\tfile = {Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\NBC8JXKZ\\\\\\\\2681.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Кхабири, Г.\",\"Разумная, А. Г.\",\"Юзюк, Ю. И.\"],\"key\":\"__2014-3\",\"id\":\"__2014-3\",\"bibbaseid\":\"----2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://www.ivdon.ru/ru/magazine/archive/N4y2014/2681\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Terahertz–infrared electrodynamics of overdoped manganites La$_{\\\\textrm{1–x}}$Ca$_{\\\\textrm{x}}$MnO$_{\\\\textrm{3}}$\",\"volume\":\"87\",\"issn\":\"0141-1594\",\"url\":\"https://doi.org/10.1080/01411594.2014.953508\",\"doi\":\"10.1080/01411594.2014.953508\",\"abstract\":\"We have measured low-temperature terahertz and infrared spectra of La1–xCa xMnO3 with x = 0.5; 0.6; 2/3, 0.7; 3/4, 0.85; 0.9; 0.95; 0.98 and x = 1 in the form of ceramics and epitaxial films. In the charge-ordered state for commensurate dopings (x = 2/3 and 3/4), we observed an absorption band at frequencies corresponding to the position of the lowest energy van Hove singularity in the folded Brillouin zone. The band is assigned to the boson peak. We observed qualitatively the same boson peak in Raman spectra of La1/3Ca2/3MnO3 ceramics. In antiferromagnetic phase, for the 0.5 ≤ x \\\\textless 0.85 range of doping, the conductivity mechanism gradually changes from a hopping-like transport at low temperatures to the Drude behavior at elevated temperatures in the paramagnetic phase. For 0.85 ≤ x \\\\textless 1 (canted antiferromagnetic phase), the electrons behave as Drude-like carriers in the whole temperature interval 5–300 K.\",\"number\":\"10-11\",\"urldate\":\"2023-11-11\",\"journal\":\"Phase Transitions\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kadyrov\"],\"firstnames\":[\"Lenar\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"Boris\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"Elena\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"Victor\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"Anatoly\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Motovilova\"],\"firstnames\":[\"Elizaveta\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fischgrabe\"],\"firstnames\":[\"Florian\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Moshnyaga\"],\"firstnames\":[\"Vasily\",\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhang\"],\"firstnames\":[\"Tao\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kremer\"],\"firstnames\":[\"Reinhard\",\"K.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pracht\"],\"firstnames\":[\"Uwe\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zapf\"],\"firstnames\":[\"Sina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pokorný\"],\"firstnames\":[\"Jan\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Untereiner\"],\"firstnames\":[\"Gabriele\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kamba\"],\"firstnames\":[\"Stanislav\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"Martin\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2014\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/01411594.2014.953508\",\"keywords\":\"manganites, terahertz\",\"pages\":\"1050–1059\",\"bibtex\":\"@article{kadyrov_terahertzinfrared_2014,\\n\\ttitle = {Terahertz–infrared electrodynamics of overdoped manganites {La}$_{\\\\textrm{1–x}}${Ca}$_{\\\\textrm{x}}${MnO}$_{\\\\textrm{3}}$},\\n\\tvolume = {87},\\n\\tissn = {0141-1594},\\n\\turl = {https://doi.org/10.1080/01411594.2014.953508},\\n\\tdoi = {10.1080/01411594.2014.953508},\\n\\tabstract = {We have measured low-temperature terahertz and infrared spectra of La1–xCa xMnO3 with x = 0.5; 0.6; 2/3, 0.7; 3/4, 0.85; 0.9; 0.95; 0.98 and x = 1 in the form of ceramics and epitaxial films. In the charge-ordered state for commensurate dopings (x = 2/3 and 3/4), we observed an absorption band at frequencies corresponding to the position of the lowest energy van Hove singularity in the folded Brillouin zone. The band is assigned to the boson peak. We observed qualitatively the same boson peak in Raman spectra of La1/3Ca2/3MnO3 ceramics. In antiferromagnetic phase, for the 0.5 ≤ x {\\\\textless} 0.85 range of doping, the conductivity mechanism gradually changes from a hopping-like transport at low temperatures to the Drude behavior at elevated temperatures in the paramagnetic phase. For 0.85 ≤ x {\\\\textless} 1 (canted antiferromagnetic phase), the electrons behave as Drude-like carriers in the whole temperature interval 5–300 K.},\\n\\tnumber = {10-11},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Phase Transitions},\\n\\tauthor = {Kadyrov, Lenar S. and Gorshunov, Boris P. and Zhukova, Elena S. and Torgashev, Victor I. and Prokhorov, Anatoly S. and Motovilova, Elizaveta A. and Fischgrabe, Florian and Moshnyaga, Vasily T. and Zhang, Tao and Kremer, Reinhard K. and Pracht, Uwe and Zapf, Sina and Pokorný, Jan and Untereiner, Gabriele and Kamba, Stanislav and Dressel, Martin},\\n\\tmonth = nov,\\n\\tyear = {2014},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/01411594.2014.953508},\\n\\tkeywords = {manganites, terahertz},\\n\\tpages = {1050--1059},\\n}\\n\\n\",\"author_short\":[\"Kadyrov, L. S.\",\"Gorshunov, B. P.\",\"Zhukova, E. S.\",\"Torgashev, V. I.\",\"Prokhorov, A. S.\",\"Motovilova, E. A.\",\"Fischgrabe, F.\",\"Moshnyaga, V. T.\",\"Zhang, T.\",\"Kremer, R. K.\",\"Pracht, U.\",\"Zapf, S.\",\"Pokorný, J.\",\"Untereiner, G.\",\"Kamba, S.\",\"Dressel, M.\"],\"key\":\"kadyrov_terahertzinfrared_2014\",\"id\":\"kadyrov_terahertzinfrared_2014\",\"bibbaseid\":\"kadyrov-gorshunov-zhukova-torgashev-prokhorov-motovilova-fischgrabe-moshnyaga-etal-terahertzinfraredelectrodynamicsofoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/01411594.2014.953508\"},\"keyword\":[\"manganites\",\"terahertz\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Phase transitions in BaTiO$_{\\\\textrm{3}}$ thin films and BaTiO$_{\\\\textrm{3}}$/BaZrO$_{\\\\textrm{3}}$ superlattices\",\"volume\":\"116\",\"issn\":\"0021-8979\",\"url\":\"https://doi.org/10.1063/1.4901207\",\"doi\":\"10.1063/1.4901207\",\"abstract\":\"Using pulsed laser deposition, we grew a ferroelectric [BaTiO3]Λ/2/[BaZrO3]Λ/2 (BT/BZ) superlattice with a stacking periodicity of Λ = 256 Å and a BT single film on a La1/2Sr1/2CoO3-buffered (001)MgO substrate, and then studied the phase transitions of these materials. At room temperature, the polarized Raman spectra of the BT film corresponded to a ferroelectric orthorhombic C2V14 phase with the polar axis oriented in the plane of the substrate. A ferroelectric-paraelectric phase transition in the BT film occurred at ∼450 K. Upon cooling to ∼300 K, a phase transition to the monoclinic Cs3 phase occurred. These experimental results agree well with a theoretical “temperature-misfit strain” phase diagram of the BT film. We found no evidence of phase transitions in the BT/BZ superlattice below room temperature. The phase transition to the paraelectric phase in the BT/BZ superlattice increased in temperature because of lattice mismatch between the BT and BZ layers. A desirable Curie temperature can be tailored rather precisely by varying the layer thicknesses or the BT/BZ ratio in the superlattice. The BT/BZ superlattices are very good for device applications because their ferroelectric phase with in-plane polarization can remain stable at least from 0 K up to 723 K, and even at higher temperatures in superlattices with smaller periodicities.\",\"number\":\"18\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Applied Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sakhovoy\"],\"firstnames\":[\"R.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"O.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zakharchenko\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Belhadi\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2014\",\"pages\":\"184102\",\"bibtex\":\"@article{yuzyuk_phase_2014,\\n\\ttitle = {Phase transitions in {BaTiO}$_{\\\\textrm{3}}$ thin films and {BaTiO}$_{\\\\textrm{3}}$/{BaZrO}$_{\\\\textrm{3}}$ superlattices},\\n\\tvolume = {116},\\n\\tissn = {0021-8979},\\n\\turl = {https://doi.org/10.1063/1.4901207},\\n\\tdoi = {10.1063/1.4901207},\\n\\tabstract = {Using pulsed laser deposition, we grew a ferroelectric [BaTiO3]Λ/2/[BaZrO3]Λ/2 (BT/BZ) superlattice with a stacking periodicity of Λ = 256 Å and a BT single film on a La1/2Sr1/2CoO3-buffered (001)MgO substrate, and then studied the phase transitions of these materials. At room temperature, the polarized Raman spectra of the BT film corresponded to a ferroelectric orthorhombic C2V14 phase with the polar axis oriented in the plane of the substrate. A ferroelectric-paraelectric phase transition in the BT film occurred at ∼450 K. Upon cooling to ∼300 K, a phase transition to the monoclinic Cs3 phase occurred. These experimental results agree well with a theoretical “temperature-misfit strain” phase diagram of the BT film. We found no evidence of phase transitions in the BT/BZ superlattice below room temperature. The phase transition to the paraelectric phase in the BT/BZ superlattice increased in temperature because of lattice mismatch between the BT and BZ layers. A desirable Curie temperature can be tailored rather precisely by varying the layer thicknesses or the BT/BZ ratio in the superlattice. The BT/BZ superlattices are very good for device applications because their ferroelectric phase with in-plane polarization can remain stable at least from 0 K up to 723 K, and even at higher temperatures in superlattices with smaller periodicities.},\\n\\tnumber = {18},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Applied Physics},\\n\\tauthor = {Yuzyuk, Yu. I. and Sakhovoy, R. A. and Maslova, O. A. and Shirokov, V. B. and Zakharchenko, I. N. and Belhadi, J. and El Marssi, M.},\\n\\tmonth = nov,\\n\\tyear = {2014},\\n\\tpages = {184102},\\n}\\n\\n\",\"author_short\":[\"Yuzyuk, Y. I.\",\"Sakhovoy, R. A.\",\"Maslova, O. A.\",\"Shirokov, V. B.\",\"Zakharchenko, I. N.\",\"Belhadi, J.\",\"El Marssi, M.\"],\"key\":\"yuzyuk_phase_2014\",\"id\":\"yuzyuk_phase_2014\",\"bibbaseid\":\"yuzyuk-sakhovoy-maslova-shirokov-zakharchenko-belhadi-elmarssi-phasetransitionsinbatiotextrm3thinfilmsandbatiotextrm3bazrotextrm3superlattices-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.4901207\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Optical properties of the Ba$_{\\\\textrm{0.8}}$Sr$_{\\\\textrm{0.2}}$TiO$_{\\\\textrm{3}}$/(Bi$_{\\\\textrm{0.82}}$, Nd$_{\\\\textrm{0.02}}$)FeO$_{\\\\textrm{3}}$ superlattice\",\"volume\":\"59\",\"issn\":\"1090-6525\",\"url\":\"https://doi.org/10.1134/S1063784214040239\",\"doi\":\"10.1134/S1063784214040239\",\"abstract\":\"A Ba0.8Sr0.2TiO3/(Bi0.82, Nd0.02)FeO3 multilayer heteroepitaxial structure is prepared by successively depositing 20 Ba0.8Sr0.2TiO3 and (Bi0.82, Nd0.02)FeO3 layers, each 4 nm thick, using the method of rf sputtering. The layers grow on a single-crystal MgO substrate following the layer-by-layer mechanism. The structural perfection of the layers is examined by X-ray diffraction. The optical transmission is studied in the wavelength interval 200–1100 nm. The spectra are processed using a dispersion formula for the permittivity represented as a superposition of two oscillators with regard to relaxation. Such an approach allows us to separate direct and indirect transitions. The absorption edge of the superlattice for direct transitions is 80 nm wide and is estimated to be 3.78 eV.\",\"language\":\"en\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Technical Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golovko\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mukhortov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Revinskii\"],\"firstnames\":[\"Yu.\",\"V.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2014\",\"keywords\":\"Barium Strontium, Barium Strontium Titanate, Multilayer Structure, Strontium Titanate, Wavelength Interval\",\"pages\":\"571–575\",\"bibtex\":\"@article{shirokov_optical_2014,\\n\\ttitle = {Optical properties of the {Ba}$_{\\\\textrm{0.8}}${Sr}$_{\\\\textrm{0.2}}${TiO}$_{\\\\textrm{3}}$/({Bi}$_{\\\\textrm{0.82}}$, {Nd}$_{\\\\textrm{0.02}}$){FeO}$_{\\\\textrm{3}}$ superlattice},\\n\\tvolume = {59},\\n\\tissn = {1090-6525},\\n\\turl = {https://doi.org/10.1134/S1063784214040239},\\n\\tdoi = {10.1134/S1063784214040239},\\n\\tabstract = {A Ba0.8Sr0.2TiO3/(Bi0.82, Nd0.02)FeO3 multilayer heteroepitaxial structure is prepared by successively depositing 20 Ba0.8Sr0.2TiO3 and (Bi0.82, Nd0.02)FeO3 layers, each 4 nm thick, using the method of rf sputtering. The layers grow on a single-crystal MgO substrate following the layer-by-layer mechanism. The structural perfection of the layers is examined by X-ray diffraction. The optical transmission is studied in the wavelength interval 200–1100 nm. The spectra are processed using a dispersion formula for the permittivity represented as a superposition of two oscillators with regard to relaxation. Such an approach allows us to separate direct and indirect transitions. The absorption edge of the superlattice for direct transitions is 80 nm wide and is estimated to be 3.78 eV.},\\n\\tlanguage = {en},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Technical Physics},\\n\\tauthor = {Shirokov, V. B. and Golovko, Yu. I. and Mukhortov, V. M. and Revinskii, Yu. V.},\\n\\tmonth = apr,\\n\\tyear = {2014},\\n\\tkeywords = {Barium Strontium, Barium Strontium Titanate, Multilayer Structure, Strontium Titanate, Wavelength Interval},\\n\\tpages = {571--575},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Golovko, Y. I.\",\"Mukhortov, V. M.\",\"Revinskii, Y. V.\"],\"key\":\"shirokov_optical_2014\",\"id\":\"shirokov_optical_2014\",\"bibbaseid\":\"shirokov-golovko-mukhortov-revinskii-opticalpropertiesofthebatextrm08srtextrm02tiotextrm3bitextrm082ndtextrm002feotextrm3superlattice-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1063784214040239\"},\"keyword\":[\"Barium Strontium\",\"Barium Strontium Titanate\",\"Multilayer Structure\",\"Strontium Titanate\",\"Wavelength Interval\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"On the nature of phase transitions in the tetragonal tungsten bronze GdK$_{\\\\textrm{2}}$Nb$_{\\\\textrm{5}}$O$_{\\\\textrm{15}}$ ceramics\",\"volume\":\"115\",\"issn\":\"0021-8979\",\"url\":\"https://doi.org/10.1063/1.4865741\",\"doi\":\"10.1063/1.4865741\",\"abstract\":\"Phase transitions in gadolinium potassium niobate GdK2Nb5O15 (GKN) ceramics have been investigated by x-ray diffraction, dielectric susceptibility, differential scanning calorimetry, and Raman scattering. The results of our complementary studies show that GKN exhibits two phase transitions at Tc1 = 238 °C and Tc2 = 375 °C attributed to the ferroelectric-antiferroelectric-paraelectric (FE-AFE-PE) phase transitions. According to the x-ray diffraction analysis, the FE and PE phases were refined in the polar P4bm and centrosymmetric P4/mbm space groups. For the intermediate phase, the structure is refined in the space group P4nc with doubling of the c unit cell parameter, which is compatible with an AFE phase. This result was confirmed by Raman spectroscopy since new low-frequency lines are activated in the AFE phase due to the Brillouin zone-folding effect, typical for the modulated phases. The presence of the AFE phase between the FE and PE phases and the complex nature of tetragonal tungsten bronze crystal structure can explain the large thermal hysteresis observed at the FE-AFE transition between heating and cooling cycle and the strong depression of the Curie-Weiss temperature T0. The semi-phenomenological Ising-like model based on the obtained experimental data is proposed to account for the observed FE-AFE-PE transition sequence.\",\"number\":\"6\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Applied Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Gagou\"],\"firstnames\":[\"Y.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Amira\"],\"firstnames\":[\"Y.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lukyanchuk\"],\"firstnames\":[\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzane\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Courty\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Masquelier\"],\"firstnames\":[\"C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2014\",\"pages\":\"064104\",\"file\":\"Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\4WTIXGZJ\\\\Øn-the-nature-of-phase-transitions-in-the.html:text/html\",\"bibtex\":\"@article{gagou_nature_2014,\\n\\ttitle = {On the nature of phase transitions in the tetragonal tungsten bronze {GdK}$_{\\\\textrm{2}}${Nb}$_{\\\\textrm{5}}${O}$_{\\\\textrm{15}}$ ceramics},\\n\\tvolume = {115},\\n\\tissn = {0021-8979},\\n\\turl = {https://doi.org/10.1063/1.4865741},\\n\\tdoi = {10.1063/1.4865741},\\n\\tabstract = {Phase transitions in gadolinium potassium niobate GdK2Nb5O15 (GKN) ceramics have been investigated by x-ray diffraction, dielectric susceptibility, differential scanning calorimetry, and Raman scattering. The results of our complementary studies show that GKN exhibits two phase transitions at Tc1 = 238 °C and Tc2 = 375 °C attributed to the ferroelectric-antiferroelectric-paraelectric (FE-AFE-PE) phase transitions. According to the x-ray diffraction analysis, the FE and PE phases were refined in the polar P4bm and centrosymmetric P4/mbm space groups. For the intermediate phase, the structure is refined in the space group P4nc with doubling of the c unit cell parameter, which is compatible with an AFE phase. This result was confirmed by Raman spectroscopy since new low-frequency lines are activated in the AFE phase due to the Brillouin zone-folding effect, typical for the modulated phases. The presence of the AFE phase between the FE and PE phases and the complex nature of tetragonal tungsten bronze crystal structure can explain the large thermal hysteresis observed at the FE-AFE transition between heating and cooling cycle and the strong depression of the Curie-Weiss temperature T0. The semi-phenomenological Ising-like model based on the obtained experimental data is proposed to account for the observed FE-AFE-PE transition sequence.},\\n\\tnumber = {6},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Applied Physics},\\n\\tauthor = {Gagou, Y. and Amira, Y. and Lukyanchuk, I. and Mezzane, D. and Courty, M. and Masquelier, C. and Yuzyuk, Yu. I. and El Marssi, M.},\\n\\tmonth = feb,\\n\\tyear = {2014},\\n\\tpages = {064104},\\n\\tfile = {Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\4WTIXGZJ\\\\\\\\On-the-nature-of-phase-transitions-in-the.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Gagou, Y.\",\"Amira, Y.\",\"Lukyanchuk, I.\",\"Mezzane, D.\",\"Courty, M.\",\"Masquelier, C.\",\"Yuzyuk, Y. I.\",\"El Marssi, M.\"],\"key\":\"gagou_nature_2014\",\"id\":\"gagou_nature_2014\",\"bibbaseid\":\"gagou-amira-lukyanchuk-mezzane-courty-masquelier-yuzyuk-elmarssi-onthenatureofphasetransitionsinthetetragonaltungstenbronzegdktextrm2nbtextrm5otextrm15ceramics-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.4865741\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Lattice anharmonicity and polar soft mode in ferrimagnetic M-type hexaferrite BaFe$_{\\\\textrm{12}}$O$_{\\\\textrm{19}}$ single crystal\",\"volume\":\"87\",\"issn\":\"1434-6036\",\"url\":\"https://doi.org/10.1140/epjb/e2014-50329-4\",\"doi\":\"10.1140/epjb/e2014-50329-4\",\"abstract\":\"The polar phonon modes in BaFe12O19 single crystal are studied in the temperature rangefrom 6 to 300 K by polarized infrared spectroscopy. The phonon spectrum of the crystal isstrongly anharmonic and unstable with respect to long-wavelength fluctuations ofthe dielectric permittivity along the hexagonal axis. Our results suggests that inBaFe12O19 hexaferrite symmetry lowering to the polar phase withthe space group P63mc can beexpected.\",\"language\":\"en\",\"number\":\"10\",\"urldate\":\"2023-11-11\",\"journal\":\"The European Physical Journal B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"Alexey\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"Elena\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"Viktor\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"Anna\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yury\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"Boris\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"Anatoly\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sashin\"],\"firstnames\":[\"Aleksandr\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bush\"],\"firstnames\":[\"Alexandr\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"Martin\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2014\",\"keywords\":\"Solid State and Materials\",\"pages\":\"232\",\"bibtex\":\"@article{mikheykin_lattice_2014,\\n\\ttitle = {Lattice anharmonicity and polar soft mode in ferrimagnetic {M}-type hexaferrite {BaFe}$_{\\\\textrm{12}}${O}$_{\\\\textrm{19}}$ single crystal},\\n\\tvolume = {87},\\n\\tissn = {1434-6036},\\n\\turl = {https://doi.org/10.1140/epjb/e2014-50329-4},\\n\\tdoi = {10.1140/epjb/e2014-50329-4},\\n\\tabstract = {The polar phonon modes in BaFe12O19 single crystal are studied in the temperature rangefrom 6 to 300 K by polarized infrared spectroscopy. The phonon spectrum of the crystal isstrongly anharmonic and unstable with respect to long-wavelength fluctuations ofthe dielectric permittivity along the hexagonal axis. Our results suggests that inBaFe12O19 hexaferrite symmetry lowering to the polar phase withthe space group P63mc can beexpected.},\\n\\tlanguage = {en},\\n\\tnumber = {10},\\n\\turldate = {2023-11-11},\\n\\tjournal = {The European Physical Journal B},\\n\\tauthor = {Mikheykin, Alexey S. and Zhukova, Elena S. and Torgashev, Viktor I. and Razumnaya, Anna G. and Yuzyuk, Yury I. and Gorshunov, Boris P. and Prokhorov, Anatoly S. and Sashin, Aleksandr E. and Bush, Alexandr A. and Dressel, Martin},\\n\\tmonth = oct,\\n\\tyear = {2014},\\n\\tkeywords = {Solid State and Materials},\\n\\tpages = {232},\\n}\\n\\n\",\"author_short\":[\"Mikheykin, A. S.\",\"Zhukova, E. S.\",\"Torgashev, V. I.\",\"Razumnaya, A. G.\",\"Yuzyuk, Y. I.\",\"Gorshunov, B. P.\",\"Prokhorov, A. S.\",\"Sashin, A. E.\",\"Bush, A. A.\",\"Dressel, M.\"],\"key\":\"mikheykin_lattice_2014\",\"id\":\"mikheykin_lattice_2014\",\"bibbaseid\":\"mikheykin-zhukova-torgashev-razumnaya-yuzyuk-gorshunov-prokhorov-sashin-etal-latticeanharmonicityandpolarsoftmodeinferrimagneticmtypehexaferritebafetextrm12otextrm19singlecrystal-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1140/epjb/e2014-50329-4\"},\"keyword\":[\"Solid State and Materials\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Investigations of Ba$_{\\\\textrm{x}}$Sr$_{\\\\textrm{1−x}}$TiO$_{\\\\textrm{3}}$ ceramics and powders prepared by direct current arc discharge technique\",\"volume\":\"105\",\"issn\":\"0003-6951\",\"url\":\"https://doi.org/10.1063/1.4894456\",\"doi\":\"10.1063/1.4894456\",\"abstract\":\"BaxSr1−xTiO3 ceramics with x ranging from 0 to 1 were prepared by direct current arc discharge technique and studied by means of x-ray diffraction (XRD) and Raman spectroscopy. The cubic-tetragonal ferroelectric phase transition in BaxSr1−xTiO3 ceramics was found to occur at x ≈ 0.75. XRD investigation of as-grown BaTiO3 ceramics revealed co-existence of tetragonal and hexagonal modifications with a small amount of impurity phase BaTi4O9. No evidences of hexagonal phase were observed in Raman spectra of as-grown BaTiO3 ceramics, while Raman peaks related to hexagonal phase were clearly observed in the spectrum of fine-grain powders prepared from the same ceramics. A core-shell model for BaTiO3 ceramics prepared by direct current arc discharge technique is proposed. Absence of the hexagonal phase in any BaxSr1−xTiO3 solid solution with x &lt; 1 is discussed in the frame of specific atomic arrangement.\",\"number\":\"9\",\"urldate\":\"2023-11-11\",\"journal\":\"Applied Physics Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Li\"],\"firstnames\":[\"Shuangbin\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yao\"],\"firstnames\":[\"Ying\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Jia\"],\"firstnames\":[\"Yongzhong\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Wang\"],\"firstnames\":[\"Xiaohan\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Xie\"],\"firstnames\":[\"Shaolei\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Jing\"],\"firstnames\":[\"Yan\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2014\",\"pages\":\"092901\",\"bibtex\":\"@article{li_investigations_2014,\\n\\ttitle = {Investigations of {Ba}$_{\\\\textrm{x}}${Sr}$_{\\\\textrm{1−x}}${TiO}$_{\\\\textrm{3}}$ ceramics and powders prepared by direct current arc discharge technique},\\n\\tvolume = {105},\\n\\tissn = {0003-6951},\\n\\turl = {https://doi.org/10.1063/1.4894456},\\n\\tdoi = {10.1063/1.4894456},\\n\\tabstract = {BaxSr1−xTiO3 ceramics with x ranging from 0 to 1 were prepared by direct current arc discharge technique and studied by means of x-ray diffraction (XRD) and Raman spectroscopy. The cubic-tetragonal ferroelectric phase transition in BaxSr1−xTiO3 ceramics was found to occur at x ≈ 0.75. XRD investigation of as-grown BaTiO3 ceramics revealed co-existence of tetragonal and hexagonal modifications with a small amount of impurity phase BaTi4O9. No evidences of hexagonal phase were observed in Raman spectra of as-grown BaTiO3 ceramics, while Raman peaks related to hexagonal phase were clearly observed in the spectrum of fine-grain powders prepared from the same ceramics. A core-shell model for BaTiO3 ceramics prepared by direct current arc discharge technique is proposed. Absence of the hexagonal phase in any BaxSr1−xTiO3 solid solution with x \\\\&lt; 1 is discussed in the frame of specific atomic arrangement.},\\n\\tnumber = {9},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Applied Physics Letters},\\n\\tauthor = {Li, Shuangbin and Yao, Ying and Yuzyuk, Yu. I. and Jia, Yongzhong and Wang, Xiaohan and Xie, Shaolei and Jing, Yan},\\n\\tmonth = sep,\\n\\tyear = {2014},\\n\\tpages = {092901},\\n}\\n\\n\",\"author_short\":[\"Li, S.\",\"Yao, Y.\",\"Yuzyuk, Y. I.\",\"Jia, Y.\",\"Wang, X.\",\"Xie, S.\",\"Jing, Y.\"],\"key\":\"li_investigations_2014\",\"id\":\"li_investigations_2014\",\"bibbaseid\":\"li-yao-yuzyuk-jia-wang-xie-jing-investigationsofbatextrmxsrtextrm1xtiotextrm3ceramicsandpowderspreparedbydirectcurrentarcdischargetechnique-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.4894456\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Highly constrained ferroelectric [BaTiO$_{\\\\textrm{3}}$]$_{\\\\textrm{(1−x)Λ}}$/[BaZrO$_{\\\\textrm{3}}$]$_{\\\\textrm{{xΛ}}}$ superlattices: X-ray diffraction and Raman spectroscopy\",\"volume\":\"116\",\"issn\":\"0021-8979\",\"shorttitle\":\"Highly constrained ferroelectric [BaTiO3](1−x)Λ/[BaZrO3]xΛ superlattices\",\"url\":\"https://doi.org/10.1063/1.4890513\",\"doi\":\"10.1063/1.4890513\",\"abstract\":\"We report an x-ray diffraction (XRD) and a Raman-scattering investigation of ferroelectric/paraelectric superlattices [BaTiO3] (1−x)Λ/[BaZrO3]xΛ for which the composition varied, 0.15 ≤ x ≤ 0.85, while the superlattice (SL) modulation period Λ was kept constant at about 100 Å. The samples were epitaxially grown by pulsed laser deposition on MgO substrates buffered with La0.5Sr0.5CoO3. Based on the XRD analysis and on polarized Raman spectra, we have showed that the large strain in SLs induced ferroelectricity in BaZrO3 (BZ) for all SLs, a material that is paraelectric in the bulk form at any temperature and in the single film. The induced polar axis in BZ layers is perpendicular to the plane of substrate while BaTiO3 (BT) layers exhibit in-plane polar orientation. Raman spectroscopy revealed a lattice ordering in SLs due to the misfit strain generated by the large lattice mismatch between the alternating BZ and BT layers. This strain induced a huge upward frequency of the lowest E(1TO) soft mode from 60 cm−1 in the BT single film to 215 cm−1 in the SL with x = 0.85. These results show that in spite of relatively large periodicity of SLs, they are highly constrained and the variation of BZ ratio allowed modifying strains between layers. The temperature dependence of the Raman spectra for BT0.3Λ/BZ0.7Λ and BT0.7Λ/BZ0.3Λ samples revealed giant shift of the ferroelectric phase transition. The phase transition temperature was found to be upshifted by about 300 °C with respect to BT single crystal.\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Applied Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Belhadi\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gagou\"],\"firstnames\":[\"Y.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Mendili\"],\"firstnames\":[\"Y.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Raevski\"],\"firstnames\":[\"I.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bouyanfif\"],\"firstnames\":[\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Wolfman\"],\"firstnames\":[\"J.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2014\",\"pages\":\"034108\",\"bibtex\":\"@article{belhadi_highly_2014,\\n\\ttitle = {Highly constrained ferroelectric [{BaTiO}$_{\\\\textrm{3}}$]$_{\\\\textrm{(1−x)Λ}}$/[{BaZrO}$_{\\\\textrm{3}}$]$_{\\\\textrm{{xΛ}}}$ superlattices: {X}-ray diffraction and {Raman} spectroscopy},\\n\\tvolume = {116},\\n\\tissn = {0021-8979},\\n\\tshorttitle = {Highly constrained ferroelectric [{BaTiO3}](1−x)Λ/[{BaZrO3}]{xΛ} superlattices},\\n\\turl = {https://doi.org/10.1063/1.4890513},\\n\\tdoi = {10.1063/1.4890513},\\n\\tabstract = {We report an x-ray diffraction (XRD) and a Raman-scattering investigation of ferroelectric/paraelectric superlattices [BaTiO3] (1−x)Λ/[BaZrO3]xΛ for which the composition varied, 0.15 ≤ x ≤ 0.85, while the superlattice (SL) modulation period Λ was kept constant at about 100 Å. The samples were epitaxially grown by pulsed laser deposition on MgO substrates buffered with La0.5Sr0.5CoO3. Based on the XRD analysis and on polarized Raman spectra, we have showed that the large strain in SLs induced ferroelectricity in BaZrO3 (BZ) for all SLs, a material that is paraelectric in the bulk form at any temperature and in the single film. The induced polar axis in BZ layers is perpendicular to the plane of substrate while BaTiO3 (BT) layers exhibit in-plane polar orientation. Raman spectroscopy revealed a lattice ordering in SLs due to the misfit strain generated by the large lattice mismatch between the alternating BZ and BT layers. This strain induced a huge upward frequency of the lowest E(1TO) soft mode from 60 cm−1 in the BT single film to 215 cm−1 in the SL with x = 0.85. These results show that in spite of relatively large periodicity of SLs, they are highly constrained and the variation of BZ ratio allowed modifying strains between layers. The temperature dependence of the Raman spectra for BT0.3Λ/BZ0.7Λ and BT0.7Λ/BZ0.3Λ samples revealed giant shift of the ferroelectric phase transition. The phase transition temperature was found to be upshifted by about 300 °C with respect to BT single crystal.},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Applied Physics},\\n\\tauthor = {Belhadi, J. and El Marssi, M. and Gagou, Y. and Yuzyuk, Yu. I. and El Mendili, Y. and Raevski, I. P. and Bouyanfif, H. and Wolfman, J.},\\n\\tmonth = jul,\\n\\tyear = {2014},\\n\\tpages = {034108},\\n}\\n\\n\",\"author_short\":[\"Belhadi, J.\",\"El Marssi, M.\",\"Gagou, Y.\",\"Yuzyuk, Y. I.\",\"El Mendili, Y.\",\"Raevski, I. P.\",\"Bouyanfif, H.\",\"Wolfman, J.\"],\"key\":\"belhadi_highly_2014\",\"id\":\"belhadi_highly_2014\",\"bibbaseid\":\"belhadi-elmarssi-gagou-yuzyuk-elmendili-raevski-bouyanfif-wolfman-highlyconstrainedferroelectricbatiotextrm3textrm1xbazrotextrm3textrmxsuperlatticesxraydiffractionandramanspectroscopy-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.4890513\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Giant increase of ferroelectric phase transition temperature in highly strained ferroelectric [BaTiO$_{\\\\textrm{3}}$]$_{\\\\textrm{0.{7Λ}}}$/[BaZrO$_{\\\\textrm{3}}$]$_{\\\\textrm{0.{3Λ}}}$ superlattice\",\"volume\":\"106\",\"issn\":\"0295-5075\",\"url\":\"https://dx.doi.org/10.1209/0295-5075/106/17004\",\"doi\":\"10.1209/0295-5075/106/17004\",\"abstract\":\"We report epitaxial strain effects in the lead-free ferroelectric/paraelectric superlattice (SL) for a modulation period Λ of about 100 Å. We have demonstrated that the large strain in SL induces ferroelectricity in BaZrO3 layers, a material that is paraelectric at any temperature in the bulk form. The induced polar axis in BaZrO3 layers is perpendicular to the plane of the substrate while BaTiO3 layers exhibit in-plane polar orientation. Raman spectroscopy revealed a lattice ordering in SL due to the misfit strain generated by the large lattice mismatch between the alternating BaZrO3 and BaTiO3 layers. Such strain induces a huge upward frequency shift of the lowest E(1TO) soft mode from in the BaTiO3 single film to in the SL. The temperature of the ferroelectric phase transition in the SL was found to be upshifted by about with respect to the BaTiO3 single crystal.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Europhysics Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Belhadi\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Marssi\"],\"firstnames\":[\"M.\",\"El\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gagou\"],\"firstnames\":[\"Y.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Raevski\"],\"firstnames\":[\"I.\",\"P.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2014\",\"note\":\"Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica\",\"pages\":\"17004\",\"bibtex\":\"@article{belhadi_giant_2014,\\n\\ttitle = {Giant increase of ferroelectric phase transition temperature in highly strained ferroelectric [{BaTiO}$_{\\\\textrm{3}}$]$_{\\\\textrm{0.{7Λ}}}$/[{BaZrO}$_{\\\\textrm{3}}$]$_{\\\\textrm{0.{3Λ}}}$ superlattice},\\n\\tvolume = {106},\\n\\tissn = {0295-5075},\\n\\turl = {https://dx.doi.org/10.1209/0295-5075/106/17004},\\n\\tdoi = {10.1209/0295-5075/106/17004},\\n\\tabstract = {We report epitaxial strain effects in the lead-free ferroelectric/paraelectric superlattice (SL) for a modulation period Λ of about 100 Å. We have demonstrated that the large strain in SL induces ferroelectricity in BaZrO3 layers, a material that is paraelectric at any temperature in the bulk form. The induced polar axis in BaZrO3 layers is perpendicular to the plane of the substrate while BaTiO3 layers exhibit in-plane polar orientation. Raman spectroscopy revealed a lattice ordering in SL due to the misfit strain generated by the large lattice mismatch between the alternating BaZrO3 and BaTiO3 layers. Such strain induces a huge upward frequency shift of the lowest E(1TO) soft mode from in the BaTiO3 single film to in the SL. The temperature of the ferroelectric phase transition in the SL was found to be upshifted by about with respect to the BaTiO3 single crystal.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Europhysics Letters},\\n\\tauthor = {Belhadi, J. and Marssi, M. El and Gagou, Y. and Yuzyuk, Yu I. and Raevski, I. P.},\\n\\tmonth = apr,\\n\\tyear = {2014},\\n\\tnote = {Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica},\\n\\tpages = {17004},\\n}\\n\\n\",\"author_short\":[\"Belhadi, J.\",\"Marssi, M. E.\",\"Gagou, Y.\",\"Yuzyuk, Y. I.\",\"Raevski, I. P.\"],\"key\":\"belhadi_giant_2014\",\"id\":\"belhadi_giant_2014\",\"bibbaseid\":\"belhadi-marssi-gagou-yuzyuk-raevski-giantincreaseofferroelectricphasetransitiontemperatureinhighlystrainedferroelectricbatiotextrm3textrm07bazrotextrm3textrm03superlattice-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1209/0295-5075/106/17004\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Chemical bonding and valence state of 3d-metal ions in Ni$_{\\\\textrm{1−x}}$Co$_{\\\\textrm{x}}$Cr$_{\\\\textrm{2}}$O$_{\\\\textrm{4}}$ spinels from X-ray diffraction and X-ray photoelectron spectroscopy data\",\"volume\":\"195\",\"issn\":\"0368-2048\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0368204814001583\",\"doi\":\"10.1016/j.elspec.2014.07.010\",\"abstract\":\"Ni1−xCoxCr2O4 solid solution samples with х=0, 0.005, 0.01, 0.02, 0.3, 0.5, 0.8 and 1 are studied by the methods of X-ray diffraction and X-ray photoelectron spectroscopy (XPS). Ni2p3/2,1/2, Co2p3/2,1/2, Cr2p3/2,1/2, and O1s spectra are measured. The spectra are calculated with allowance for multiplet splitting, crystal field, and charge-transfer effect. Ni2+ ions are found to be present in tetrahedral and octahedral positions. Relative numbers of Ni2+ ions in tetrahedral and octahedral sites are determined via fitting the experimental spectra with superposition of the spectra of Ni2+ ions calculated in tetrahedral and octahedral crystal field. Cobalt ions are bivalent and occupy mostly tetrahedral sites. Chromium ions are trivalent and occupy predominantly octahedral positions. However, due to a defective lattice, the samples may contain Cr ions in non-equivalent states, either chemically or structurally.\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Electron Spectroscopy and Related Phenomena\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kochur\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kozakov\"],\"firstnames\":[\"A.\",\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Googlev\"],\"firstnames\":[\"K.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bush\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nikolskii\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2014\",\"keywords\":\"X-ray diffraction, Crystal structure, NiCoCrO spinels, Valence state, XPS\",\"pages\":\"208–219\",\"bibtex\":\"@article{kochur_chemical_2014,\\n\\ttitle = {Chemical bonding and valence state of 3d-metal ions in {Ni}$_{\\\\textrm{1−x}}${Co}$_{\\\\textrm{x}}${Cr}$_{\\\\textrm{2}}${O}$_{\\\\textrm{4}}$ spinels from {X}-ray diffraction and {X}-ray photoelectron spectroscopy data},\\n\\tvolume = {195},\\n\\tissn = {0368-2048},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0368204814001583},\\n\\tdoi = {10.1016/j.elspec.2014.07.010},\\n\\tabstract = {Ni1−xCoxCr2O4 solid solution samples with х=0, 0.005, 0.01, 0.02, 0.3, 0.5, 0.8 and 1 are studied by the methods of X-ray diffraction and X-ray photoelectron spectroscopy (XPS). Ni2p3/2,1/2, Co2p3/2,1/2, Cr2p3/2,1/2, and O1s spectra are measured. The spectra are calculated with allowance for multiplet splitting, crystal field, and charge-transfer effect. Ni2+ ions are found to be present in tetrahedral and octahedral positions. Relative numbers of Ni2+ ions in tetrahedral and octahedral sites are determined via fitting the experimental spectra with superposition of the spectra of Ni2+ ions calculated in tetrahedral and octahedral crystal field. Cobalt ions are bivalent and occupy mostly tetrahedral sites. Chromium ions are trivalent and occupy predominantly octahedral positions. However, due to a defective lattice, the samples may contain Cr ions in non-equivalent states, either chemically or structurally.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Electron Spectroscopy and Related Phenomena},\\n\\tauthor = {Kochur, A. G. and Kozakov, A. T. and Googlev, K. A. and Mikheykin, A. S. and Torgashev, V. I. and Bush, A. A. and Nikolskii, A. V.},\\n\\tmonth = aug,\\n\\tyear = {2014},\\n\\tkeywords = {X-ray diffraction, Crystal structure, NiCoCrO spinels, Valence state, XPS},\\n\\tpages = {208--219},\\n}\\n\\n\",\"author_short\":[\"Kochur, A. G.\",\"Kozakov, A. T.\",\"Googlev, K. A.\",\"Mikheykin, A. S.\",\"Torgashev, V. I.\",\"Bush, A. A.\",\"Nikolskii, A. V.\"],\"key\":\"kochur_chemical_2014\",\"id\":\"kochur_chemical_2014\",\"bibbaseid\":\"kochur-kozakov-googlev-mikheykin-torgashev-bush-nikolskii-chemicalbondingandvalencestateof3dmetalionsinnitextrm1xcotextrmxcrtextrm2otextrm4spinelsfromxraydiffractionandxrayphotoelectronspectroscopydata-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0368204814001583\"},\"keyword\":[\"X-ray diffraction\",\"Crystal structure\",\"NiCoCrO spinels\",\"Valence state\",\"XPS\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Экспериментальное и теоретическое исследование массивов наностержней ZnO, покрытых пленкой серебра, как антенн оптического и ближнего ИК-диапазона\",\"volume\":\"40\",\"url\":\"http://journals.ioffe.ru/articles/27360\",\"abstract\":\"Предложена новая конструкция оптической антенны - наностержень ZnO, покрытый тонкой металлической пленкой. Методами карботермического синтеза и магнетронного напыления получены решетки высокоориентированных перпендикулярно подложке наностержней оксида цинка, покрытых тонкой пленкой серебра. Решены задачи дифракции электромагнитных волн на одиночном металлодиэлектрическом нановибраторе, расположенном на границе раздела диэлектриков и на двумерно-периодической решетке нановибраторов. Проведено сравнение расчетов электродинамических характеристик оптических наноантенн различной длины с экспериментально полученными.\",\"language\":\"ru\",\"number\":\"7\",\"urldate\":\"2023-11-11\",\"journal\":\"Письма в ЖТФ\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лерер\"],\"firstnames\":[\"А.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Распопова\"],\"firstnames\":[\"Е.\",\"А.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2014\",\"pages\":\"79–86\",\"bibtex\":\"@article{__2014-4,\\n\\ttitle = {Экспериментальное и теоретическое исследование массивов наностержней {ZnO}, покрытых пленкой серебра, как антенн оптического и ближнего ИК-диапазона},\\n\\tvolume = {40},\\n\\turl = {http://journals.ioffe.ru/articles/27360},\\n\\tabstract = {Предложена новая конструкция оптической антенны - наностержень ZnO, покрытый тонкой металлической пленкой. Методами карботермического синтеза и магнетронного напыления получены решетки высокоориентированных перпендикулярно подложке наностержней оксида цинка, покрытых тонкой пленкой серебра. Решены задачи дифракции электромагнитных волн на одиночном металлодиэлектрическом нановибраторе, расположенном на границе раздела диэлектриков и на двумерно-периодической решетке нановибраторов. Проведено сравнение расчетов электродинамических характеристик оптических наноантенн различной длины с экспериментально полученными.},\\n\\tlanguage = {ru},\\n\\tnumber = {7},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Письма в ЖТФ},\\n\\tauthor = {Кайдашев, Е. М. and Лянгузов, Н. В. and Лерер, А. М. and Распопова, Е. А.},\\n\\tmonth = mar,\\n\\tyear = {2014},\\n\\tpages = {79--86},\\n}\\n\\n\",\"author_short\":[\"Кайдашев, Е. М.\",\"Лянгузов, Н. В.\",\"Лерер, А. М.\",\"Распопова, Е. А.\"],\"key\":\"__2014-4\",\"id\":\"__2014-4\",\"bibbaseid\":\"----zno-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/27360\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Оптические свойства эпитаксиальных тонких пленок BiFeO3\",\"volume\":\"84\",\"url\":\"http://journals.ioffe.ru/articles/27131\",\"abstract\":\"Исследованы свойства наноразмерных пленок BiFeO3, допированных неодимом, на монокристаллических подложках оксида магния, полученных методом высокочастотного распыления по слоевому механизму роста. Структурное совершенство пленок изучено методами рентгеновской дифракции. Пропускание пленок различной толщины исследовано в диапазоне длин волн 200-1100 nm. Спектры обработаны с использованием дисперсионной формулы для диэлектрической проницаемости в виде суммы осцилляторов с учетом релаксации, что позволило выделить прямые и непрямые переходы. Край поглощения оценен для прямых переходов как 2.81 и 2.78 eV для пленок толщиной 14 и 60 nm соответственно.\",\"language\":\"ru\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Журнал технической физики\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2013\",\"pages\":\"104–108\",\"bibtex\":\"@article{__2013-8,\\n\\ttitle = {Оптические свойства эпитаксиальных тонких пленок {BiFeO3}},\\n\\tvolume = {84},\\n\\turl = {http://journals.ioffe.ru/articles/27131},\\n\\tabstract = {Исследованы свойства наноразмерных пленок BiFeO3, допированных неодимом, на монокристаллических подложках оксида магния, полученных методом высокочастотного распыления по слоевому механизму роста. Структурное совершенство пленок изучено методами рентгеновской дифракции. Пропускание пленок различной толщины исследовано в диапазоне длин волн 200-1100 nm. Спектры обработаны с использованием дисперсионной формулы для диэлектрической проницаемости в виде суммы осцилляторов с учетом релаксации, что позволило выделить прямые и непрямые переходы. Край поглощения оценен для прямых переходов как 2.81 и 2.78 eV для пленок толщиной 14 и 60 nm соответственно.},\\n\\tlanguage = {ru},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Журнал технической физики},\\n\\tauthor = {Широков, В. Б. and Головко, Ю. И. and Мухортов, В. М.},\\n\\tmonth = dec,\\n\\tyear = {2013},\\n\\tpages = {104--108},\\n}\\n\\n\",\"author_short\":[\"Широков, В. Б.\",\"Головко, Ю. И.\",\"Мухортов, В. М.\"],\"key\":\"__2013-8\",\"id\":\"__2013-8\",\"bibbaseid\":\"---bifeo3-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/27131\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"address\":\"Тула\",\"title\":\"Сферические упаковки в оболочках вирусов, эпителиальных монослоях и коллоидных кристаллах\",\"shorttitle\":\"Алгебра, теория чисел и дискретная геометрия\",\"url\":\"https://elibrary.ru/item.asp?id=39552125\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"booktitle\":\"Материалы XVI Международной конференции, посвященной 80-летию со дня рождения профессора Мишеля Деза\",\"publisher\":\"Тульский государственный педагогический университет им. Л.Н. Толстого\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Рошаль\"],\"firstnames\":[\"Д.\",\"С.\"],\"suffixes\":[]}],\"year\":\"2019\",\"pages\":\"2\",\"bibtex\":\"@inproceedings{__2019-1,\\n\\taddress = {Тула},\\n\\ttitle = {Сферические упаковки в оболочках вирусов, эпителиальных монослоях и коллоидных кристаллах},\\n\\tshorttitle = {Алгебра, теория чисел и дискретная геометрия},\\n\\turl = {https://elibrary.ru/item.asp?id=39552125},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tbooktitle = {Материалы {XVI} Международной конференции,  посвященной 80-летию со дня рождения  профессора Мишеля Деза},\\n\\tpublisher = {Тульский государственный педагогический университет им. Л.Н. Толстого},\\n\\tauthor = {Рошаль, Д. С.},\\n\\tyear = {2019},\\n\\tpages = {2},\\n}\\n\\n\",\"author_short\":[\"Рошаль, Д. С.\"],\"key\":\"__2019-1\",\"id\":\"__2019-1\",\"bibbaseid\":\"--2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=39552125\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":1,\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"address\":\"St. Petersburg, Russian Federation\",\"title\":\"Temperature Evolution of Inelastic Synchrotron Radiation Scattering in PbZr $_{\\\\textrm{0.985}}$Ti$_{\\\\textrm{0.015}}$O$_{\\\\textrm{3}}$ in the Vicinity of M-Point\",\"isbn\":\"978-1-66544-972-4\",\"url\":\"https://ieeexplore.ieee.org/document/9614882/\",\"doi\":\"10.1109/EExPolytech53083.2021.9614882\",\"urldate\":\"2023-11-10\",\"booktitle\":\"2021 International Conference on Electrical Engineering and Photonics (EExPolytech)\",\"publisher\":\"IEEE\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Vakhrushev\"],\"firstnames\":[\"Sergey\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bosak\"],\"firstnames\":[\"Alexey\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Udovenko\"],\"firstnames\":[\"Stanislav\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Petroukhno\"],\"firstnames\":[\"Konstantin\",\"A.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2021\",\"pages\":\"143–145\",\"bibtex\":\"@inproceedings{vakhrushev_temperature_2021,\\n\\taddress = {St. Petersburg, Russian Federation},\\n\\ttitle = {Temperature {Evolution} of {Inelastic} {Synchrotron} {Radiation} {Scattering} in {PbZr} $_{\\\\textrm{0.985}}${Ti}$_{\\\\textrm{0.015}}${O}$_{\\\\textrm{3}}$ in the {Vicinity} of {M}-{Point}},\\n\\tisbn = {978-1-66544-972-4},\\n\\turl = {https://ieeexplore.ieee.org/document/9614882/},\\n\\tdoi = {10.1109/EExPolytech53083.2021.9614882},\\n\\turldate = {2023-11-10},\\n\\tbooktitle = {2021 {International} {Conference} on {Electrical} {Engineering} and {Photonics} ({EExPolytech})},\\n\\tpublisher = {IEEE},\\n\\tauthor = {Vakhrushev, Sergey B. and Leontyev, Igor N. and Bosak, Alexey and Udovenko, Stanislav A. and Petroukhno, Konstantin A.},\\n\\tmonth = oct,\\n\\tyear = {2021},\\n\\tpages = {143--145},\\n}\\n\\n\",\"author_short\":[\"Vakhrushev, S. B.\",\"Leontyev, I. N.\",\"Bosak, A.\",\"Udovenko, S. A.\",\"Petroukhno, K. A.\"],\"key\":\"vakhrushev_temperature_2021\",\"id\":\"vakhrushev_temperature_2021\",\"bibbaseid\":\"vakhrushev-leontyev-bosak-udovenko-petroukhno-temperatureevolutionofinelasticsynchrotronradiationscatteringinpbzrtextrm0985titextrm0015otextrm3inthevicinityofmpoint-2021\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://ieeexplore.ieee.org/document/9614882/\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Characteristics of Carbon Nanotubes Synthesized from Methane and Acetylene in the Presence of a FeCl$_{\\\\textrm{3}}$ Catalyst\",\"volume\":\"66\",\"issn\":\"1063-7842, 1090-6525\",\"url\":\"http://link.springer.com/10.1134/S106378422103021X\",\"doi\":\"10.1134/S106378422103021X\",\"language\":\"en\",\"number\":\"3\",\"urldate\":\"2023-11-10\",\"journal\":\"Technical Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Redina\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Avramenko\"],\"firstnames\":[\"M.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lyanguzov\"],\"firstnames\":[\"N.\",\"V.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2021\",\"pages\":\"445–452\",\"bibtex\":\"@article{redina_characteristics_2021,\\n\\ttitle = {Characteristics of {Carbon} {Nanotubes} {Synthesized} from {Methane} and {Acetylene} in the {Presence} of a {FeCl}$_{\\\\textrm{3}}$ {Catalyst}},\\n\\tvolume = {66},\\n\\tissn = {1063-7842, 1090-6525},\\n\\turl = {http://link.springer.com/10.1134/S106378422103021X},\\n\\tdoi = {10.1134/S106378422103021X},\\n\\tlanguage = {en},\\n\\tnumber = {3},\\n\\turldate = {2023-11-10},\\n\\tjournal = {Technical Physics},\\n\\tauthor = {Redina, A. G. and Avramenko, M. V. and Lyanguzov, N. V.},\\n\\tmonth = mar,\\n\\tyear = {2021},\\n\\tpages = {445--452},\\n}\\n\\n\",\"author_short\":[\"Redina, A. G.\",\"Avramenko, M. V.\",\"Lyanguzov, N. V.\"],\"key\":\"redina_characteristics_2021\",\"id\":\"redina_characteristics_2021\",\"bibbaseid\":\"redina-avramenko-lyanguzov-characteristicsofcarbonnanotubessynthesizedfrommethaneandacetyleneinthepresenceofafecltextrm3catalyst-2021\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://link.springer.com/10.1134/S106378422103021X\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Исследование динамики решетки макро-, микро- и наноструктурированного титаната бария методом спектроскопии комбинационного рассеяния света\",\"volume\":\"56\",\"url\":\"http://journals.ioffe.ru/articles/26768\",\"language\":\"ru\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Маслова\"],\"firstnames\":[\"О.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Marssi\"],\"firstnames\":[\"M.\",\"El\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Jain\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ortega\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"R.\",\"S.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2014\",\"pages\":\"308–314\",\"bibtex\":\"@article{__2014-5,\\n\\ttitle = {Исследование динамики решетки макро-, микро- и наноструктурированного титаната бария методом спектроскопии комбинационного рассеяния света},\\n\\tvolume = {56},\\n\\turl = {http://journals.ioffe.ru/articles/26768},\\n\\tlanguage = {ru},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Маслова, О. А. and Широков, В. Б. and Юзюк, Ю. И. and Marssi, M. El and Jain, M. and Ortega, N. and Katiyar, R. S.},\\n\\tmonth = jan,\\n\\tyear = {2014},\\n\\tpages = {308--314},\\n}\\n\\n\",\"author_short\":[\"Маслова, О. А.\",\"Широков, В. Б.\",\"Юзюк, Ю. И.\",\"Marssi, M. E.\",\"Jain, M.\",\"Ortega, N.\",\"Katiyar, R. S.\"],\"key\":\"__2014-5\",\"id\":\"__2014-5\",\"bibbaseid\":\"---marssi-jain-ortega-katiyar--2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/26768\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Динамический спектральный отклик твердых растворов висмут-стронциевого феррита Bi$_{\\\\textrm{1-x}}$Sr$_{\\\\textrm{x}}$FeO$_{\\\\textrm{3-delta}}$ в диапазоне частот 0.3-200 THz\",\"volume\":\"55\",\"url\":\"http://journals.ioffe.ru/articles/1093\",\"language\":\"ru\",\"number\":\"7\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Анохин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Разумная\"],\"firstnames\":[\"А.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Торгашев\"],\"firstnames\":[\"В.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Троценко\"],\"firstnames\":[\"В.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Буш\"],\"firstnames\":[\"А.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Шкуратов\"],\"firstnames\":[\"В.\",\"Я.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Горшунов\"],\"firstnames\":[\"Б.\",\"П.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Жукова\"],\"firstnames\":[\"Е.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кадыров\"],\"firstnames\":[\"Л.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Командин\"],\"firstnames\":[\"Г.\",\"А.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2013\",\"pages\":\"1320–1332\",\"bibtex\":\"@article{__2013-9,\\n\\ttitle = {Динамический спектральный отклик твердых растворов висмут-стронциевого феррита {Bi}$_{\\\\textrm{1-x}}${Sr}$_{\\\\textrm{x}}${FeO}$_{\\\\textrm{3-delta}}$ в диапазоне частот 0.3-200 {THz}},\\n\\tvolume = {55},\\n\\turl = {http://journals.ioffe.ru/articles/1093},\\n\\tlanguage = {ru},\\n\\tnumber = {7},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Анохин, А. С. and Разумная, А. Г. and Торгашев, В. И. and Троценко, В. Г. and Юзюк, Ю. И. and Буш, А. А. and Шкуратов, В. Я. and Горшунов, Б. П. and Жукова, Е. С. and Кадыров, Л. С. and Командин, Г. А.},\\n\\tmonth = jun,\\n\\tyear = {2013},\\n\\tpages = {1320--1332},\\n}\\n\\n\",\"author_short\":[\"Анохин, А. С.\",\"Разумная, А. Г.\",\"Торгашев, В. И.\",\"Троценко, В. Г.\",\"Юзюк, Ю. И.\",\"Буш, А. А.\",\"Шкуратов, В. Я.\",\"Горшунов, Б. П.\",\"Жукова, Е. С.\",\"Кадыров, Л. С.\",\"Командин, Г. А.\"],\"key\":\"__2013-9\",\"id\":\"__2013-9\",\"bibbaseid\":\"--------etal-bitextrm1xsrtextrmxfeotextrm3delta03200thz-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/1093\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Теплоемкость наноструктурированной керамики BaTiO$_{\\\\textrm{3}}$\",\"volume\":\"55\",\"url\":\"http://journals.ioffe.ru/articles/1045\",\"abstract\":\"Исследована температурная зависимость теплоемкости наноструктурированной керамики BaTiO3, полученной твердофазным методом, спеканию которой предшествовала обработка при комнатной температуре синтезированной шихты в наковальнях Бриджмена силовым воздействием в сочетании со сдвиговой деформацией. Обнаружено существенное размытие сегнетоэлектрического перехода и нелинейное убывание температуры фазового перехода с увеличением приложенного давления. Показано, что дефектная структура играет доминирующую роль в формировании физических свойств керамики.\",\"language\":\"ru\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Каллаев\"],\"firstnames\":[\"С.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Омаров\"],\"firstnames\":[\"З.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бакмаев\"],\"firstnames\":[\"А.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Абдулвахидов\"],\"firstnames\":[\"К.\",\"Г.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2013\",\"pages\":\"1011–1013\",\"bibtex\":\"@article{__2013-10,\\n\\ttitle = {Теплоемкость наноструктурированной керамики {BaTiO}$_{\\\\textrm{3}}$},\\n\\tvolume = {55},\\n\\turl = {http://journals.ioffe.ru/articles/1045},\\n\\tabstract = {Исследована температурная зависимость теплоемкости наноструктурированной керамики BaTiO3, полученной твердофазным методом, спеканию которой предшествовала обработка при комнатной температуре синтезированной шихты в наковальнях Бриджмена силовым воздействием в сочетании со сдвиговой деформацией. Обнаружено существенное размытие сегнетоэлектрического перехода и нелинейное убывание температуры фазового перехода с увеличением приложенного давления. Показано, что дефектная структура играет доминирующую роль в формировании физических свойств керамики.},\\n\\tlanguage = {ru},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Каллаев, С. Н. and Омаров, З. М. and Бакмаев, А. Г. and Абдулвахидов, К. Г.},\\n\\tmonth = apr,\\n\\tyear = {2013},\\n\\tpages = {1011--1013},\\n}\\n\\n\",\"author_short\":[\"Каллаев, С. Н.\",\"Омаров, З. М.\",\"Бакмаев, А. Г.\",\"Абдулвахидов, К. Г.\"],\"key\":\"__2013-10\",\"id\":\"__2013-10\",\"bibbaseid\":\"----batiotextrm3-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/1045\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Материальные константы твердых растворов (Ba,Sr)TiO$_{\\\\textrm{3}}$\",\"volume\":\"55\",\"url\":\"http://journals.ioffe.ru/articles/998\",\"abstract\":\"Феноменологическая теория твердого раствора использована для вычисления поведения материальных констант (упругих податливостей, восприимчивостей, пьезоэлектрических модулей, пироэлектрических коэффициентов) твердого раствора BaxSr1-xTiO3 во всей области изменения концентраций x при комнатной температуре. Для выделенных концентраций приведены константы феноменологического потенциала и численные значения материальных констант.\",\"language\":\"ru\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Калинчук\"],\"firstnames\":[\"В.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Леманов\"],\"firstnames\":[\"В.\",\"В.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2013\",\"pages\":\"709–714\",\"bibtex\":\"@article{__2013-11,\\n\\ttitle = {Материальные константы твердых растворов ({Ba},{Sr}){TiO}$_{\\\\textrm{3}}$},\\n\\tvolume = {55},\\n\\turl = {http://journals.ioffe.ru/articles/998},\\n\\tabstract = {Феноменологическая теория твердого раствора использована для вычисления поведения материальных констант (упругих податливостей, восприимчивостей, пьезоэлектрических модулей, пироэлектрических коэффициентов) твердого раствора BaxSr1-xTiO3 во всей области изменения концентраций x при комнатной температуре. Для выделенных концентраций приведены константы феноменологического потенциала и численные значения материальных констант.},\\n\\tlanguage = {ru},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Широков, В. Б. and Юзюк, Ю. И. and Калинчук, В. В. and Леманов, В. В.},\\n\\tmonth = mar,\\n\\tyear = {2013},\\n\\tpages = {709--714},\\n}\\n\\n\",\"author_short\":[\"Широков, В. Б.\",\"Юзюк, Ю. И.\",\"Калинчук, В. В.\",\"Леманов, В. В.\"],\"key\":\"__2013-11\",\"id\":\"__2013-11\",\"bibbaseid\":\"----basrtiotextrm3-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/998\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Теория кристаллизации Ландау и самосборка октагональных квазикристаллов\",\"volume\":\"55\",\"url\":\"http://journals.ioffe.ru/articles/1117\",\"abstract\":\"Предложена теория кристаллизации квазикристаллических структур, не использующая для описания квазикристаллического порядка концепций многомерной кристаллографии. На примере структуры октагонального квазикристалла MnSiAl показано, что координаты узлов соответствующей квазикристаллической решетки (КР) можно рассчитать путем условной минимизации свободной энергии Ландау. Отказ от безусловной минимизации свободной энергии обосновывается особенностями локального атомного порядка в рассматриваемой структуре. Предложенная теория придает новый физический смысл традиционным понятиям многомерной кристаллографии и может быть также применена для объяснения образования квазикристаллических структур с другими КР.\",\"language\":\"ru\",\"number\":\"8\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Коневцова\"],\"firstnames\":[\"О.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Рошаль\"],\"firstnames\":[\"С.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лорман\"],\"firstnames\":[\"В.\",\"Л.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2013\",\"pages\":\"1488–1493\",\"bibtex\":\"@article{__2013-12,\\n\\ttitle = {Теория кристаллизации Ландау и самосборка октагональных квазикристаллов},\\n\\tvolume = {55},\\n\\turl = {http://journals.ioffe.ru/articles/1117},\\n\\tabstract = {Предложена теория кристаллизации квазикристаллических структур, не использующая для описания квазикристаллического порядка концепций многомерной кристаллографии. На примере структуры октагонального квазикристалла MnSiAl показано, что координаты узлов соответствующей квазикристаллической решетки (КР) можно рассчитать путем условной минимизации свободной энергии Ландау. Отказ от безусловной минимизации свободной энергии обосновывается особенностями локального атомного порядка в рассматриваемой структуре. Предложенная теория придает новый физический смысл традиционным понятиям многомерной кристаллографии и может быть также применена для объяснения образования квазикристаллических структур с другими КР.},\\n\\tlanguage = {ru},\\n\\tnumber = {8},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Коневцова, О. В. and Рошаль, С. Б. and Лорман, В. Л.},\\n\\tmonth = jul,\\n\\tyear = {2013},\\n\\tpages = {1488--1493},\\n}\\n\\n\",\"author_short\":[\"Коневцова, О. В.\",\"Рошаль, С. Б.\",\"Лорман, В. Л.\"],\"key\":\"__2013-12\",\"id\":\"__2013-12\",\"bibbaseid\":\"----2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/1117\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":3,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Особенности диэлектрического спектра CaCu$_{\\\\textrm{3}}$Ti$_{\\\\textrm{4}}$O$_{\\\\textrm{12}}$ в низкочастотном диапазоне\",\"volume\":\"55\",\"url\":\"http://journals.ioffe.ru/articles/1124\",\"abstract\":\"Представлены диэлектрические спектры керамики CaCu3Ti4O12, отличающейся гигантскими значениями диэлектрической проницаемости. В высокочастотной части спектра в области 106-107 Hz проявляется дисперсия дебаевского типа с энергией активации 0.075 eV, а также характерное плато в частотной зависимости диэлектрической проницаемости в области 104-105 Hz. В низкочастотной части спектра наблюдается значительное увеличение фактора потерь varepsilon'', а при частоте менее 10-2 Hz в некоторых образцах обнаружен переход от импеданса емкостного типа к индуктивному. Обсуждаются причины такого перехода.\",\"language\":\"ru\",\"number\":\"8\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Гавриляченко\"],\"firstnames\":[\"В.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кабиров\"],\"firstnames\":[\"Ю.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Панченко\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ситало\"],\"firstnames\":[\"Е.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гавриляченко\"],\"firstnames\":[\"Т.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Милов\"],\"firstnames\":[\"Е.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2013\",\"pages\":\"1540–1543\",\"bibtex\":\"@article{__2013-13,\\n\\ttitle = {Особенности диэлектрического спектра {CaCu}$_{\\\\textrm{3}}${Ti}$_{\\\\textrm{4}}${O}$_{\\\\textrm{12}}$ в низкочастотном диапазоне},\\n\\tvolume = {55},\\n\\turl = {http://journals.ioffe.ru/articles/1124},\\n\\tabstract = {Представлены диэлектрические спектры керамики CaCu3Ti4O12, отличающейся гигантскими значениями диэлектрической проницаемости. В высокочастотной части спектра в области 106-107 Hz проявляется дисперсия дебаевского типа с энергией активации 0.075 eV, а также характерное плато в частотной зависимости диэлектрической проницаемости в области 104-105 Hz. В низкочастотной части спектра наблюдается значительное увеличение фактора потерь varepsilon'', а при частоте менее 10-2 Hz в некоторых образцах обнаружен переход от импеданса емкостного типа к индуктивному. Обсуждаются причины такого перехода.},\\n\\tlanguage = {ru},\\n\\tnumber = {8},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Гавриляченко, В. Г. and Кабиров, Ю. В. and Панченко, Е. М. and Ситало, Е. И. and Гавриляченко, Т. В. and Милов, Е. В. and Лянгузов, Н. В.},\\n\\tmonth = jul,\\n\\tyear = {2013},\\n\\tpages = {1540--1543},\\n}\\n\\n\",\"author_short\":[\"Гавриляченко, В. Г.\",\"Кабиров, Ю. В.\",\"Панченко, Е. М.\",\"Ситало, Е. И.\",\"Гавриляченко, Т. В.\",\"Милов, Е. В.\",\"Лянгузов, Н. В.\"],\"key\":\"__2013-13\",\"id\":\"__2013-13\",\"bibbaseid\":\"-------cacutextrm3titextrm4otextrm12-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/1124\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Boson peak in overdoped manganites La$_{\\\\textrm{1-x}}$Ca$_{\\\\textrm{x}}$MnO$_{\\\\textrm{3}}$\",\"volume\":\"87\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.87.245124\",\"doi\":\"10.1103/PhysRevB.87.245124\",\"abstract\":\"In the charge-ordered phase of strongly doped manganites La1−xCaxMnO3 (x≥0.5) absorption lines appear in the terahertz spectral range for commensurate x values right below the charge-ordering temperature. They are connected to acoustic phonons that become optically active by folding of the Brillouin zone. At lower temperatures a strongly asymmetric extra absorption band develops at frequencies corresponding to the position of the lowest-energy van Hove singularity in the reduced Brillouin zone. The band is assigned to the boson peak, i.e., to the excess of lattice vibrational states over the standard Debye contribution. The folded phonons and the boson peak do not show up for incommensurate calcium contents when no distinct Brillouin zone folding exists.\",\"number\":\"24\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kadyrov\"],\"firstnames\":[\"L.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Motovilova\"],\"firstnames\":[\"E.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fischgrabe\"],\"firstnames\":[\"F.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Moshnyaga\"],\"firstnames\":[\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhang\"],\"firstnames\":[\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kremer\"],\"firstnames\":[\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pracht\"],\"firstnames\":[\"U.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zapf\"],\"firstnames\":[\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2013\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"245124\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\G3SEUD2M\\\\\\\\Gorshunov и др. - 2013 - Boson peak in overdoped manganites La$ _ 1ensure.pdf:application/pdf\",\"bibtex\":\"@article{gorshunov_boson_2013,\\n\\ttitle = {Boson peak in overdoped manganites {La}$_{\\\\textrm{1-x}}${Ca}$_{\\\\textrm{x}}${MnO}$_{\\\\textrm{3}}$},\\n\\tvolume = {87},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.87.245124},\\n\\tdoi = {10.1103/PhysRevB.87.245124},\\n\\tabstract = {In the charge-ordered phase of strongly doped manganites La1−xCaxMnO3 (x≥0.5) absorption lines appear in the terahertz spectral range for commensurate x values right below the charge-ordering temperature. They are connected to acoustic phonons that become optically active by folding of the Brillouin zone. At lower temperatures a strongly asymmetric extra absorption band develops at frequencies corresponding to the position of the lowest-energy van Hove singularity in the reduced Brillouin zone. The band is assigned to the boson peak, i.e., to the excess of lattice vibrational states over the standard Debye contribution. The folded phonons and the boson peak do not show up for incommensurate calcium contents when no distinct Brillouin zone folding exists.},\\n\\tnumber = {24},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Gorshunov, B. and Zhukova, E. and Torgashev, V. I. and Kadyrov, L. S. and Motovilova, E. A. and Fischgrabe, F. and Moshnyaga, V. and Zhang, T. and Kremer, R. and Pracht, U. and Zapf, S. and Dressel, M.},\\n\\tmonth = jun,\\n\\tyear = {2013},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {245124},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\G3SEUD2M\\\\\\\\Gorshunov и др. - 2013 - Boson peak in overdoped manganites La\\\\$ _ 1ensure.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Gorshunov, B.\",\"Zhukova, E.\",\"Torgashev, V. I.\",\"Kadyrov, L. S.\",\"Motovilova, E. A.\",\"Fischgrabe, F.\",\"Moshnyaga, V.\",\"Zhang, T.\",\"Kremer, R.\",\"Pracht, U.\",\"Zapf, S.\",\"Dressel, M.\"],\"key\":\"gorshunov_boson_2013\",\"id\":\"gorshunov_boson_2013\",\"bibbaseid\":\"gorshunov-zhukova-torgashev-kadyrov-motovilova-fischgrabe-moshnyaga-zhang-etal-bosonpeakinoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.87.245124\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Chemical bonding in the Bi$_{\\\\textrm{1−x}}$Sr$_{\\\\textrm{x}}$FeO$_{\\\\textrm{3±y}}$ system by X-ray photoelectron and Mössbauer spectroscopy\",\"volume\":\"189\",\"issn\":\"0368-2048\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0368204813001369\",\"doi\":\"10.1016/j.elspec.2013.08.006\",\"abstract\":\"Ceramic samples Bi1−xSrxFeO3±y are synthesized with 0≤x≤1 by the solid state reaction method. X-ray diffraction study of the samples is performed. Chemical bonding and the valence state of the Fe ions in the Bi1−xSrxFeO3±y ceramics are studied using X-ray photoelectron Fe2p-, Sr3d-, Bi4f-, and O1s-spectra, and Mössbauer spectroscopy. Fe2p-spectra for various ionic states of Fe are calculated in an isolated ion approximation. Considerable deviations of actual elemental compositions from nominal ones are discovered. Both Fe3+ and Fe4+ ions are found to be present in the samples with x\\\\textgreater0. Relative Fe3+/Fe4+ contents are determined by comparing the parameters of experimental and theoretical Fe2p-spectra. Concentration of Fe4+ ions in the samples correlates with that of the Sr atoms.\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Electron Spectroscopy and Related Phenomena\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kozakov\"],\"firstnames\":[\"A.\",\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kochur\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bush\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shkuratov\"],\"firstnames\":[\"V.\",\"Ya.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kubrin\"],\"firstnames\":[\"S.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nikolskii\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Googlev\"],\"firstnames\":[\"K.\",\"A.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2013\",\"keywords\":\"X-ray diffraction, BiSrFeO ceramics, Fe valence state, Mössbauer spectra, X-ray photoelectron spectra\",\"pages\":\"106–115\",\"bibtex\":\"@article{kozakov_chemical_2013,\\n\\ttitle = {Chemical bonding in the {Bi}$_{\\\\textrm{1−x}}${Sr}$_{\\\\textrm{x}}${FeO}$_{\\\\textrm{3±y}}$ system by {X}-ray photoelectron and {Mössbauer} spectroscopy},\\n\\tvolume = {189},\\n\\tissn = {0368-2048},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0368204813001369},\\n\\tdoi = {10.1016/j.elspec.2013.08.006},\\n\\tabstract = {Ceramic samples Bi1−xSrxFeO3±y are synthesized with 0≤x≤1 by the solid state reaction method. X-ray diffraction study of the samples is performed. Chemical bonding and the valence state of the Fe ions in the Bi1−xSrxFeO3±y ceramics are studied using X-ray photoelectron Fe2p-, Sr3d-, Bi4f-, and O1s-spectra, and Mössbauer spectroscopy. Fe2p-spectra for various ionic states of Fe are calculated in an isolated ion approximation. Considerable deviations of actual elemental compositions from nominal ones are discovered. Both Fe3+ and Fe4+ ions are found to be present in the samples with x{\\\\textgreater}0. Relative Fe3+/Fe4+ contents are determined by comparing the parameters of experimental and theoretical Fe2p-spectra. Concentration of Fe4+ ions in the samples correlates with that of the Sr atoms.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Electron Spectroscopy and Related Phenomena},\\n\\tauthor = {Kozakov, A. T. and Kochur, A. G. and Torgashev, V. I. and Bush, A. A. and Shkuratov, V. Ya. and Kubrin, S. P. and Nikolskii, A. V. and Googlev, K. A.},\\n\\tmonth = aug,\\n\\tyear = {2013},\\n\\tkeywords = {X-ray diffraction, BiSrFeO ceramics, Fe valence state, Mössbauer spectra, X-ray photoelectron spectra},\\n\\tpages = {106--115},\\n}\\n\\n\",\"author_short\":[\"Kozakov, A. T.\",\"Kochur, A. G.\",\"Torgashev, V. I.\",\"Bush, A. A.\",\"Shkuratov, V. Y.\",\"Kubrin, S. P.\",\"Nikolskii, A. V.\",\"Googlev, K. A.\"],\"key\":\"kozakov_chemical_2013\",\"id\":\"kozakov_chemical_2013\",\"bibbaseid\":\"kozakov-kochur-torgashev-bush-shkuratov-kubrin-nikolskii-googlev-chemicalbondinginthebitextrm1xsrtextrmxfeotextrm3ysystembyxrayphotoelectronandmssbauerspectroscopy-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0368204813001369\"},\"keyword\":[\"X-ray diffraction\",\"BiSrFeO ceramics\",\"Fe valence state\",\"Mössbauer spectra\",\"X-ray photoelectron spectra\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Compositional engineering of BaTiO$_{\\\\textrm{3}}$/(Ba,Sr)TiO$_{\\\\textrm{3}}$ ferroelectric superlattices\",\"volume\":\"114\",\"issn\":\"0021-8979\",\"url\":\"https://doi.org/10.1063/1.4820576\",\"doi\":\"10.1063/1.4820576\",\"abstract\":\"Epitaxial strain is one of the major factors influencing physical properties of artificial superlattice (SL) structures. One way to control the local stress in epitaxial films is altering the lattice parameters by doping. Superlattices of BT/Ba(1−x)SrxTiO3 (BT/BST) with x = (0, 0.3, 0.4, 0.5, 0.6, 0.7, 1) with a modulation period of about 80–90 Å were grown on La0.67Sr0.33MnO3 coated (100) MgO substrates by pulsed laser deposition technique. The modulated structure of the thin films was confirmed by x-ray diffraction, Raman spectroscopy, and transmission electron microscopy. The increase in Sr concentration in BST layers of the SLs results in an increase in in-plane (a) and out-plane (c) compressive/tensile misfit strains in the BT/BST layers, respectively. The highest value of the dielectric constant was obtained for BT/Ba0.3Sr0.7TiO3 (BT/BST3070) and BT/Ba0.7Sr0.3TiO3 (BT/BST7030) SLs. Slim, asymmetric, but well-saturated ferroelectric hysteresis loops were observed in all SLs. Additionally, BT/BST SLs exhibited exceptionally high electric field stress sustainability over a wide range of frequency (10 kHz) and temperature (80–350 K). Temperature-dependent dielectric and ferroelectric properties show a ferroelectric relaxor behavior when the Sr content is increased in the BST layer of the SLs. Analysis of polarization versus temperature data using Landau-Devonshire theory suggests a second-order ferroelectric phase transition in these SLs. This structure can therefore be attractive in the design of a new kind of dielectric device capable in both high power and high energy density applications.\",\"number\":\"10\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Applied Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Ortega\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kumar\"],\"firstnames\":[\"Ashok\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Resto\"],\"firstnames\":[\"Oscar\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"O.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Scott\"],\"firstnames\":[\"J.\",\"F.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"Ram\",\"S.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2013\",\"pages\":\"104102\",\"bibtex\":\"@article{ortega_compositional_2013,\\n\\ttitle = {Compositional engineering of {BaTiO}$_{\\\\textrm{3}}$/({Ba},{Sr}){TiO}$_{\\\\textrm{3}}$ ferroelectric superlattices},\\n\\tvolume = {114},\\n\\tissn = {0021-8979},\\n\\turl = {https://doi.org/10.1063/1.4820576},\\n\\tdoi = {10.1063/1.4820576},\\n\\tabstract = {Epitaxial strain is one of the major factors influencing physical properties of artificial superlattice (SL) structures. One way to control the local stress in epitaxial films is altering the lattice parameters by doping. Superlattices of BT/Ba(1−x)SrxTiO3 (BT/BST) with x = (0, 0.3, 0.4, 0.5, 0.6, 0.7, 1) with a modulation period of about 80–90 Å were grown on La0.67Sr0.33MnO3 coated (100) MgO substrates by pulsed laser deposition technique. The modulated structure of the thin films was confirmed by x-ray diffraction, Raman spectroscopy, and transmission electron microscopy. The increase in Sr concentration in BST layers of the SLs results in an increase in in-plane (a) and out-plane (c) compressive/tensile misfit strains in the BT/BST layers, respectively. The highest value of the dielectric constant was obtained for BT/Ba0.3Sr0.7TiO3 (BT/BST3070) and BT/Ba0.7Sr0.3TiO3 (BT/BST7030) SLs. Slim, asymmetric, but well-saturated ferroelectric hysteresis loops were observed in all SLs. Additionally, BT/BST SLs exhibited exceptionally high electric field stress sustainability over a wide range of frequency (10 kHz) and temperature (80–350 K). Temperature-dependent dielectric and ferroelectric properties show a ferroelectric relaxor behavior when the Sr content is increased in the BST layer of the SLs. Analysis of polarization versus temperature data using Landau-Devonshire theory suggests a second-order ferroelectric phase transition in these SLs. This structure can therefore be attractive in the design of a new kind of dielectric device capable in both high power and high energy density applications.},\\n\\tnumber = {10},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Applied Physics},\\n\\tauthor = {Ortega, N. and Kumar, Ashok and Resto, Oscar and Maslova, O. A. and Yuzyuk, Yu. I. and Scott, J. F. and Katiyar, Ram S.},\\n\\tmonth = sep,\\n\\tyear = {2013},\\n\\tpages = {104102},\\n}\\n\\n\",\"author_short\":[\"Ortega, N.\",\"Kumar, A.\",\"Resto, O.\",\"Maslova, O. A.\",\"Yuzyuk, Y. I.\",\"Scott, J. F.\",\"Katiyar, R. S.\"],\"key\":\"ortega_compositional_2013\",\"id\":\"ortega_compositional_2013\",\"bibbaseid\":\"ortega-kumar-resto-maslova-yuzyuk-scott-katiyar-compositionalengineeringofbatiotextrm3basrtiotextrm3ferroelectricsuperlattices-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.4820576\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Observation of an intersublattice exchange magnon in CoCr$_{\\\\textrm{2}}$O$_{\\\\textrm{4}}$ and analysis of magnetic ordering\",\"volume\":\"87\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.87.134423\",\"doi\":\"10.1103/PhysRevB.87.134423\",\"abstract\":\"We report on an investigation of optical properties of multiferroic CoCr2O4 at terahertz frequencies in magnetic fields up to 30 T. Below the ferrimagnetic transition (94 K), the terahertz response of CoCr2O4 is dominated by a magnon mode, which shows a steep magnetic-field dependence. We ascribe this mode to an exchange resonance between two magnetic sublattices with different g factors. In the framework of a simple two-sublattice model (the sublattices are formed by Co2+ and Cr3+ ions), we find the inter-sublattice coupling constant, λ=−(18±1) K, and trace the magnetization for each sublattice as a function of field. We show that the Curie temperature of the Cr3+ sublattice, Θ2 = (49±2) K, coincides with the temperature range, where anomalies of the dielectric and magnetic properties of CoCr2O4 have been reported in literature.\",\"number\":\"13\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kamenskyi\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Engelkamp\"],\"firstnames\":[\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fischer\"],\"firstnames\":[\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Uhlarz\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Wosnitza\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"B.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Komandin\"],\"firstnames\":[\"G.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bush\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pronin\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2013\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"134423\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\X6THP5XM\\\\\\\\Kamenskyi и др. - 2013 - Observation of an intersublattice exchange magnon .pdf:application/pdf;APS Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\3GBGXRM2\\\\¶hysRevB.87.html:text/html\",\"bibtex\":\"@article{kamenskyi_observation_2013,\\n\\ttitle = {Observation of an intersublattice exchange magnon in {CoCr}$_{\\\\textrm{2}}${O}$_{\\\\textrm{4}}$ and analysis of magnetic ordering},\\n\\tvolume = {87},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.87.134423},\\n\\tdoi = {10.1103/PhysRevB.87.134423},\\n\\tabstract = {We report on an investigation of optical properties of multiferroic CoCr2O4 at terahertz frequencies in magnetic fields up to 30 T. Below the ferrimagnetic transition (94 K), the terahertz response of CoCr2O4 is dominated by a magnon mode, which shows a steep magnetic-field dependence. We ascribe this mode to an exchange resonance between two magnetic sublattices with different g factors. In the framework of a simple two-sublattice model (the sublattices are formed by Co2+ and Cr3+ ions), we find the inter-sublattice coupling constant, λ=−(18±1) K, and trace the magnetization for each sublattice as a function of field. We show that the Curie temperature of the Cr3+ sublattice, Θ2 = (49±2) K, coincides with the temperature range, where anomalies of the dielectric and magnetic properties of CoCr2O4 have been reported in literature.},\\n\\tnumber = {13},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Kamenskyi, D. and Engelkamp, H. and Fischer, T. and Uhlarz, M. and Wosnitza, J. and Gorshunov, B. P. and Komandin, G. A. and Prokhorov, A. S. and Dressel, M. and Bush, A. A. and Torgashev, V. I. and Pronin, A. V.},\\n\\tmonth = apr,\\n\\tyear = {2013},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {134423},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\X6THP5XM\\\\\\\\Kamenskyi и др. - 2013 - Observation of an intersublattice exchange magnon .pdf:application/pdf;APS Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\3GBGXRM2\\\\\\\\PhysRevB.87.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Kamenskyi, D.\",\"Engelkamp, H.\",\"Fischer, T.\",\"Uhlarz, M.\",\"Wosnitza, J.\",\"Gorshunov, B. P.\",\"Komandin, G. A.\",\"Prokhorov, A. S.\",\"Dressel, M.\",\"Bush, A. A.\",\"Torgashev, V. I.\",\"Pronin, A. V.\"],\"key\":\"kamenskyi_observation_2013\",\"id\":\"kamenskyi_observation_2013\",\"bibbaseid\":\"kamenskyi-engelkamp-fischer-uhlarz-wosnitza-gorshunov-komandin-prokhorov-etal-observationofanintersublatticeexchangemagnonincocrtextrm2otextrm4andanalysisofmagneticordering-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.87.134423\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Phase Diagrams of BaTiO$_{\\\\textrm{3}}$/BaZrO$_{\\\\textrm{3}}$ Superlattices\",\"volume\":\"444\",\"issn\":\"0015-0193\",\"url\":\"https://doi.org/10.1080/10584587.2013.785795\",\"doi\":\"10.1080/10584587.2013.785795\",\"abstract\":\"Temperature-misfit strain phase diagrams of BaTiO3/BaZrO3 superlattices were developed and an alteration of the “misfit strain-temperature” phase diagrams against the changing of ferroelectric layers volume fraction was investigated. The topology of developed phase diagrams is similar to that of single BaTiO3 film, but phase transition lines exhibit substation shifts. According to our approach, the main reason of this shift is the electrostatic interaction between the layers. It is revealed that only one polar phase remains stable in superlattices with volume fraction of BaTiO3 being less than 70%.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shakhovoy\"],\"firstnames\":[\"R.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2013\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/10584587.2013.785795\",\"keywords\":\"ferroelectric superlattices, Phenomenological theory\",\"pages\":\"168–176\",\"bibtex\":\"@article{shakhovoy_phase_2013,\\n\\ttitle = {Phase {Diagrams} of {BaTiO}$_{\\\\textrm{3}}$/{BaZrO}$_{\\\\textrm{3}}$ {Superlattices}},\\n\\tvolume = {444},\\n\\tissn = {0015-0193},\\n\\turl = {https://doi.org/10.1080/10584587.2013.785795},\\n\\tdoi = {10.1080/10584587.2013.785795},\\n\\tabstract = {Temperature-misfit strain phase diagrams of BaTiO3/BaZrO3 superlattices were developed and an alteration of the “misfit strain-temperature” phase diagrams against the changing of ferroelectric layers volume fraction was investigated. The topology of developed phase diagrams is similar to that of single BaTiO3 film, but phase transition lines exhibit substation shifts. According to our approach, the main reason of this shift is the electrostatic interaction between the layers. It is revealed that only one polar phase remains stable in superlattices with volume fraction of BaTiO3 being less than 70\\\\%.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Shakhovoy, R. A. and Shirokov, V. B. and Yuzyuk, Yu. I.},\\n\\tmonth = jan,\\n\\tyear = {2013},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/10584587.2013.785795},\\n\\tkeywords = {ferroelectric superlattices, Phenomenological theory},\\n\\tpages = {168--176},\\n}\\n\\n\",\"author_short\":[\"Shakhovoy, R. A.\",\"Shirokov, V. B.\",\"Yuzyuk, Y. I.\"],\"key\":\"shakhovoy_phase_2013\",\"id\":\"shakhovoy_phase_2013\",\"bibbaseid\":\"shakhovoy-shirokov-yuzyuk-phasediagramsofbatiotextrm3bazrotextrm3superlattices-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/10584587.2013.785795\"},\"keyword\":[\"ferroelectric superlattices\",\"Phenomenological theory\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Raman and X-ray diffraction study of (Ba,Sr)TiO$_{\\\\textrm{3}}$/(Bi,Nd)FeO$_{\\\\textrm{3}}$ multilayer heterostructures\",\"volume\":\"545\",\"issn\":\"0040-6090\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0040609013013564\",\"doi\":\"10.1016/j.tsf.2013.08.057\",\"abstract\":\"We report synthesis, X-ray diffraction (XRD) and Raman scattering characterisation of epitaxial heterostructures containing alternating (Bi0.98Nd0.02)FeO3 (BNFO) and (Ba0.8Sr0.2TiO3) (BST) layers deposited on (100) MgO substrates. A significant shift of the BST soft mode and partial depolarisation in the Raman spectra of multilayer heterostructures caused by epitaxial strains were observed. Satellite peaks typical for superlattices were observed in the XRD patterns of multilayer heterostructures with layer thicknesses below 30nm. Raman spectra of the BNFO/BST superlattice with a modulation period of 10nm revealed hardening of the soft mode and a dominating symmetric-stretching mode at 705cm−1 due to distortion in FeO6 octahedra enforced by the epitaxial strain in the superlattice.\",\"urldate\":\"2023-11-11\",\"journal\":\"Thin Solid Films\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Anokhin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bunina\"],\"firstnames\":[\"O.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golovko\"],\"firstnames\":[\"Yu\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mukhortov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Simon\"],\"firstnames\":[\"P.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2013\",\"keywords\":\"Raman spectroscopy, Thin films, Multiferroics, Sputtering, X-ray diffraction superlattices\",\"pages\":\"267–271\",\"bibtex\":\"@article{anokhin_raman_2013,\\n\\ttitle = {Raman and {X}-ray diffraction study of ({Ba},{Sr}){TiO}$_{\\\\textrm{3}}$/({Bi},{Nd}){FeO}$_{\\\\textrm{3}}$ multilayer heterostructures},\\n\\tvolume = {545},\\n\\tissn = {0040-6090},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0040609013013564},\\n\\tdoi = {10.1016/j.tsf.2013.08.057},\\n\\tabstract = {We report synthesis, X-ray diffraction (XRD) and Raman scattering characterisation of epitaxial heterostructures containing alternating (Bi0.98Nd0.02)FeO3 (BNFO) and (Ba0.8Sr0.2TiO3) (BST) layers deposited on (100) MgO substrates. A significant shift of the BST soft mode and partial depolarisation in the Raman spectra of multilayer heterostructures caused by epitaxial strains were observed. Satellite peaks typical for superlattices were observed in the XRD patterns of multilayer heterostructures with layer thicknesses below 30nm. Raman spectra of the BNFO/BST superlattice with a modulation period of 10nm revealed hardening of the soft mode and a dominating symmetric-stretching mode at 705cm−1 due to distortion in FeO6 octahedra enforced by the epitaxial strain in the superlattice.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Thin Solid Films},\\n\\tauthor = {Anokhin, A. S. and Bunina, O. A. and Golovko, Yu I. and Mukhortov, V. M. and Yuzyuk, Yu I. and Simon, P.},\\n\\tmonth = oct,\\n\\tyear = {2013},\\n\\tkeywords = {Raman spectroscopy, Thin films, Multiferroics, Sputtering, X-ray diffraction superlattices},\\n\\tpages = {267--271},\\n}\\n\\n\",\"author_short\":[\"Anokhin, A. S.\",\"Bunina, O. A.\",\"Golovko, Y. I.\",\"Mukhortov, V. M.\",\"Yuzyuk, Y. I.\",\"Simon, P.\"],\"key\":\"anokhin_raman_2013\",\"id\":\"anokhin_raman_2013\",\"bibbaseid\":\"anokhin-bunina-golovko-mukhortov-yuzyuk-simon-ramanandxraydiffractionstudyofbasrtiotextrm3bindfeotextrm3multilayerheterostructures-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0040609013013564\"},\"keyword\":[\"Raman spectroscopy\",\"Thin films\",\"Multiferroics\",\"Sputtering\",\"X-ray diffraction superlattices\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Studies of Diffuse Phase Transition in Ferroelectric Solid Solution Pb$_{\\\\textrm{1-x}}$K$_{\\\\textrm{2x}}$Nb$_{\\\\textrm{2}}$O$_{\\\\textrm{6}}$ (x = 0.1, 0.2, 0.25 and 0.3)\",\"volume\":\"444\",\"issn\":\"0015-0193\",\"url\":\"https://doi.org/10.1080/00150193.2013.786619\",\"doi\":\"10.1080/00150193.2013.786619\",\"abstract\":\"New compositions of Tetragonal Tungsten Bronze (TTB) ferroelectrics Pb1-xK2xNb5O15 (PKN) with x = 0.1, 0.2, 0.25 and 0.3 were synthesized using the solid state reaction method. Structural and electrical properties were examined as a function of the ratio Pb/K using X-ray diffraction, Raman spectroscopy and dielectric measurements. The dielectric permittivity and the loss tangent of each composition have been measured in a frequency range 10 Hz–1 MH and in a temperatures range 25–600°C. It was shown that the Pb substitution induces the diffuse phase transition.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Belboukhari\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Abkhar\"],\"firstnames\":[\"Z.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Choukri\"],\"firstnames\":[\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gagou\"],\"firstnames\":[\"Y.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Abdelmoula\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Elmoznine\"],\"firstnames\":[\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzane\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Khemakhem\"],\"firstnames\":[\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Marssi\"],\"firstnames\":[\"M.\",\"El\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Raevski\"],\"firstnames\":[\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Luk'yanchuk\"],\"firstnames\":[\"I.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2013\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2013.786619\",\"keywords\":\"dielectric spectroscopy, Ferroelectrics, phase transition, TTB compounds\",\"pages\":\"116–124\",\"bibtex\":\"@article{belboukhari_studies_2013,\\n\\ttitle = {Studies of {Diffuse} {Phase} {Transition} in {Ferroelectric} {Solid} {Solution} {Pb}$_{\\\\textrm{1-x}}${K}$_{\\\\textrm{2x}}${Nb}$_{\\\\textrm{2}}${O}$_{\\\\textrm{6}}$ (x = 0.1, 0.2, 0.25 and 0.3)},\\n\\tvolume = {444},\\n\\tissn = {0015-0193},\\n\\turl = {https://doi.org/10.1080/00150193.2013.786619},\\n\\tdoi = {10.1080/00150193.2013.786619},\\n\\tabstract = {New compositions of Tetragonal Tungsten Bronze (TTB) ferroelectrics Pb1-xK2xNb5O15 (PKN) with x = 0.1, 0.2, 0.25 and 0.3 were synthesized using the solid state reaction method. Structural and electrical properties were examined as a function of the ratio Pb/K using X-ray diffraction, Raman spectroscopy and dielectric measurements. The dielectric permittivity and the loss tangent of each composition have been measured in a frequency range 10 Hz–1 MH and in a temperatures range 25–600°C. It was shown that the Pb substitution induces the diffuse phase transition.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Belboukhari, A. and Abkhar, Z. and Choukri, E. and Gagou, Y. and Abdelmoula, N. and Elmoznine, R. and Mezzane, D. and Khemakhem, H. and Marssi, M. El and Razumnaya, A. and Raevski, I. and Luk'yanchuk, I.},\\n\\tmonth = jan,\\n\\tyear = {2013},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/00150193.2013.786619},\\n\\tkeywords = {dielectric spectroscopy, Ferroelectrics, phase transition, TTB compounds},\\n\\tpages = {116--124},\\n}\\n\\n\",\"author_short\":[\"Belboukhari, A.\",\"Abkhar, Z.\",\"Choukri, E.\",\"Gagou, Y.\",\"Abdelmoula, N.\",\"Elmoznine, R.\",\"Mezzane, D.\",\"Khemakhem, H.\",\"Marssi, M. E.\",\"Razumnaya, A.\",\"Raevski, I.\",\"Luk'yanchuk, I.\"],\"key\":\"belboukhari_studies_2013\",\"id\":\"belboukhari_studies_2013\",\"bibbaseid\":\"belboukhari-abkhar-choukri-gagou-abdelmoula-elmoznine-mezzane-khemakhem-etal-studiesofdiffusephasetransitioninferroelectricsolidsolutionpbtextrm1xktextrm2xnbtextrm2otextrm6x0102025and03-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/00150193.2013.786619\"},\"keyword\":[\"dielectric spectroscopy\",\"Ferroelectrics\",\"phase transition\",\"TTB compounds\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Terahertz-infrared spectra of the rare-earth scandate DyScO$_{\\\\textrm{3}}$ single crystal\",\"volume\":\"114\",\"issn\":\"0021-8979\",\"url\":\"https://doi.org/10.1063/1.4813496\",\"doi\":\"10.1063/1.4813496\",\"abstract\":\"Terahertz and infrared spectra of the optical response of DyScO3 single crystal are measured at temperatures from 5 K to 300 K for two different polarizations E‖[1¯01] and E‖[010], i.e., along the two crystallographic directions of the DyScO3 substrates used for growing of thin films and heterostructures. Detailed reference data on the terahertz dielectric characteristics of the DyScO3 substrate are presented. We discuss the mechanisms responsible for electromagnetic absorption. Phonon spectra are analyzed along with the results of group-theoretical analysis of the crystal structure. Besides phonon modes, additional resonance absorptions are found and assigned to the electronic transitions between Kramers doublets in the three lowest-energy terms of the Dy3+ ion.\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Applied Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Komandin\"],\"firstnames\":[\"G.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"E.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Boris\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Boris\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Motovilova\"],\"firstnames\":[\"E.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kadyrov\"],\"firstnames\":[\"L.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"B.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2013\",\"pages\":\"024102\",\"bibtex\":\"@article{komandin_terahertz-infrared_2013,\\n\\ttitle = {Terahertz-infrared spectra of the rare-earth scandate {DyScO}$_{\\\\textrm{3}}$ single crystal},\\n\\tvolume = {114},\\n\\tissn = {0021-8979},\\n\\turl = {https://doi.org/10.1063/1.4813496},\\n\\tdoi = {10.1063/1.4813496},\\n\\tabstract = {Terahertz and infrared spectra of the optical response of DyScO3 single crystal are measured at temperatures from 5 K to 300 K for two different polarizations E‖[1¯01] and E‖[010], i.e., along the two crystallographic directions of the DyScO3 substrates used for growing of thin films and heterostructures. Detailed reference data on the terahertz dielectric characteristics of the DyScO3 substrate are presented. We discuss the mechanisms responsible for electromagnetic absorption. Phonon spectra are analyzed along with the results of group-theoretical analysis of the crystal structure. Besides phonon modes, additional resonance absorptions are found and assigned to the electronic transitions between Kramers doublets in the three lowest-energy terms of the Dy3+ ion.},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Applied Physics},\\n\\tauthor = {Komandin, G. A. and Zhukova, E. S. and Torgashev, V. I. and Boris, A. V. and Boris, A. A. and Motovilova, E. A. and Prokhorov, A. S. and Kadyrov, L. S. and Gorshunov, B. P. and Dressel, M.},\\n\\tmonth = jul,\\n\\tyear = {2013},\\n\\tpages = {024102},\\n}\\n\\n\",\"author_short\":[\"Komandin, G. A.\",\"Zhukova, E. S.\",\"Torgashev, V. I.\",\"Boris, A. V.\",\"Boris, A. A.\",\"Motovilova, E. A.\",\"Prokhorov, A. S.\",\"Kadyrov, L. S.\",\"Gorshunov, B. P.\",\"Dressel, M.\"],\"key\":\"komandin_terahertz-infrared_2013\",\"id\":\"komandin_terahertz-infrared_2013\",\"bibbaseid\":\"komandin-zhukova-torgashev-boris-boris-motovilova-prokhorov-kadyrov-etal-terahertzinfraredspectraoftherareearthscandatedyscotextrm3singlecrystal-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.4813496\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Индуцированный электрическим полем фазовый переход в релаксорной керамике на основе PMN–PT\",\"volume\":\"55\",\"url\":\"http://journals.ioffe.ru/articles/929\",\"abstract\":\"Методами рентгеновской дифрактометрии и атомно-силовой микроскопии проанализированы механизмы формирования плато на зависимостях реверсивной диэлектрической проницаемости от величины напряженности внешнего электрического поля в керамическом образце системы yPZN-mPMN-nPNN-xPT (x=0,3, y =0.0982, m = 0.4541, n = 0.1477). Показано, что в электрических полях, соответствующих аномалии диэлектрической проницаемости, происходит индуцированный фазовый переход из гетерофазного (тетрагонального+псевдокубического) в монофазное (тетрагональное) состояние. При этом наблюдаются значительные деформации тетрагональной ячейки (до 0.1%) и прекращение 90o-ных доменных переключений. Представлена качественная модель формирования наблюдаемой диэлектрической аномалии, основанная на выделении двух процессов, протекающих при увеличении напряженности электрического поля: роста полярных областей тетрагональной фазы и их переключения.\",\"language\":\"ru\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Таланов\"],\"firstnames\":[\"М.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бунина\"],\"firstnames\":[\"О.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бунин\"],\"firstnames\":[\"М.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Захарченко\"],\"firstnames\":[\"И.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Резниченко\"],\"firstnames\":[\"Л.\",\"А.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2013\",\"pages\":\"288–294\",\"bibtex\":\"@article{__2013-14,\\n\\ttitle = {Индуцированный электрическим полем фазовый переход в релаксорной керамике на основе {PMN}--{PT}},\\n\\tvolume = {55},\\n\\turl = {http://journals.ioffe.ru/articles/929},\\n\\tabstract = {Методами рентгеновской дифрактометрии и атомно-силовой микроскопии проанализированы механизмы формирования плато на зависимостях реверсивной диэлектрической проницаемости от величины напряженности внешнего электрического поля в керамическом образце системы yPZN-mPMN-nPNN-xPT (x=0,3, y =0.0982, m = 0.4541, n = 0.1477). Показано, что в электрических полях, соответствующих аномалии диэлектрической проницаемости, происходит индуцированный фазовый переход из гетерофазного (тетрагонального+псевдокубического) в монофазное (тетрагональное) состояние. При этом наблюдаются значительные деформации тетрагональной ячейки (до 0.1\\\\%) и прекращение 90o-ных доменных переключений. Представлена качественная модель формирования наблюдаемой диэлектрической аномалии, основанная на выделении двух процессов, протекающих при увеличении напряженности электрического поля: роста полярных областей тетрагональной фазы и их переключения.},\\n\\tlanguage = {ru},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Таланов, М. В. and Бунина, О. А. and Бунин, М. А. and Захарченко, И. Н. and Резниченко, Л. А.},\\n\\tmonth = jan,\\n\\tyear = {2013},\\n\\tpages = {288--294},\\n}\\n\\n\",\"author_short\":[\"Таланов, М. В.\",\"Бунина, О. А.\",\"Бунин, М. А.\",\"Захарченко, И. Н.\",\"Резниченко, Л. А.\"],\"key\":\"__2013-14\",\"id\":\"__2013-14\",\"bibbaseid\":\"-----pmnpt-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/929\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"X-ray Diffraction Study of BaTiO$_{\\\\textrm{3}}$/(Ba$_{\\\\textrm{1-x}}$Sr$_{\\\\textrm{x}}$)TiO$_{\\\\textrm{3}}$ Artificial Superlattices\",\"volume\":\"444\",\"issn\":\"0015-0193\",\"url\":\"https://doi.org/10.1080/00150193.2013.785833\",\"doi\":\"10.1080/00150193.2013.785833\",\"abstract\":\"We report x-ray diffraction investigation of two sets of artificial BaTiO3/Ba1-x Sr x TiO3 (BT/BST-x) superlattices (SLs) grown on MgO substrates. The first set of SLs was deposited with the constant periodicity (about 150 Å) and the variable Ba/Sr content in BST layers. In the second set, the modulation period Λ was varied between 30 Å \\\\textless Λ \\\\textless 110 Å while Ba content was equal 0 in BST layers. It is shown that, fabrication of the artificial SLs with variable composition of the constituting layers even with large modulation period may provide enhanced variation of the ferroelectric properties comparing to the SLs with variable layers thickness.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Zakharchenko\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bunina\"],\"firstnames\":[\"O.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"O.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ortega\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kumar\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"R.\",\"S.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2013\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2013.785833\",\"keywords\":\"ferroelectric superlattices, X-ray diffraction\",\"pages\":\"1–8\",\"bibtex\":\"@article{zakharchenko_x-ray_2013,\\n\\ttitle = {X-ray {Diffraction} {Study} of {BaTiO}$_{\\\\textrm{3}}$/({Ba}$_{\\\\textrm{1-x}}${Sr}$_{\\\\textrm{x}}$){TiO}$_{\\\\textrm{3}}$ {Artificial} {Superlattices}},\\n\\tvolume = {444},\\n\\tissn = {0015-0193},\\n\\turl = {https://doi.org/10.1080/00150193.2013.785833},\\n\\tdoi = {10.1080/00150193.2013.785833},\\n\\tabstract = {We report x-ray diffraction investigation of two sets of artificial BaTiO3/Ba1-x Sr x TiO3 (BT/BST-x) superlattices (SLs) grown on MgO substrates. The first set of SLs was deposited with the constant periodicity (about 150 Å) and the variable Ba/Sr content in BST layers. In the second set, the modulation period Λ was varied between 30 Å {\\\\textless} Λ {\\\\textless} 110 Å while Ba content was equal 0 in BST layers. It is shown that, fabrication of the artificial SLs with variable composition of the constituting layers even with large modulation period may provide enhanced variation of the ferroelectric properties comparing to the SLs with variable layers thickness.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Zakharchenko, I. N. and Bunina, O. A. and Maslova, O. A. and Yuzyuk, Yu. I. and Ortega, N. and Kumar, A. and Katiyar, R. S.},\\n\\tmonth = jan,\\n\\tyear = {2013},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/00150193.2013.785833},\\n\\tkeywords = {ferroelectric superlattices, X-ray diffraction},\\n\\tpages = {1--8},\\n}\\n\\n\",\"author_short\":[\"Zakharchenko, I. N.\",\"Bunina, O. A.\",\"Maslova, O. A.\",\"Yuzyuk, Y. I.\",\"Ortega, N.\",\"Kumar, A.\",\"Katiyar, R. S.\"],\"key\":\"zakharchenko_x-ray_2013\",\"id\":\"zakharchenko_x-ray_2013\",\"bibbaseid\":\"zakharchenko-bunina-maslova-yuzyuk-ortega-kumar-katiyar-xraydiffractionstudyofbatiotextrm3batextrm1xsrtextrmxtiotextrm3artificialsuperlattices-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/00150193.2013.785833\"},\"keyword\":[\"ferroelectric superlattices\",\"X-ray diffraction\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Методы синтеза LaMnO$_{\\\\textrm{3}}$ (обзор)\",\"url\":\"http://www.ivdon.ru/magazine/archive/n2y2013/1724\",\"abstract\":\"Сетевой научный журнал «Инженерный вестник Дона»\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Рудская\"],\"firstnames\":[\"А.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Власенко\"],\"firstnames\":[\"М.\",\"П.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Чаговец\"],\"firstnames\":[\"С.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Назаренко\"],\"firstnames\":[\"А.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Тесленко\"],\"firstnames\":[\"П.\",\"Ю.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Разумная\"],\"firstnames\":[\"А.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кофанова\"],\"firstnames\":[\"Н.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Куприянов\"],\"firstnames\":[\"М.\",\"Ф.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2013\",\"bibtex\":\"@article{__2013-15,\\n\\ttitle = {Методы синтеза {LaMnO}$_{\\\\textrm{3}}$ (обзор)},\\n\\turl = {http://www.ivdon.ru/magazine/archive/n2y2013/1724},\\n\\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Рудская, А. Г. and Власенко, М. П. and Чаговец, С. В. and Назаренко, А. В. and Тесленко, П. Ю. and Разумная, А. Г. and Кофанова, Н. Б. and Куприянов, М. Ф.},\\n\\tmonth = jan,\\n\\tyear = {2013},\\n}\\n\\n\",\"author_short\":[\"Рудская, А. Г.\",\"Власенко, М. П.\",\"Чаговец, С. В.\",\"Назаренко, А. В.\",\"Тесленко, П. Ю.\",\"Разумная, А. Г.\",\"Кофанова, Н. Б.\",\"Куприянов, М. Ф.\"],\"key\":\"__2013-15\",\"id\":\"__2013-15\",\"bibbaseid\":\"--------lamnotextrm3-2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://www.ivdon.ru/magazine/archive/n2y2013/1724\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Оптимизация карботермического синтеза массивов микро- и наностержней оксида цинка и их морфометрических параметров\",\"volume\":\"39\",\"url\":\"http://journals.ioffe.ru/articles/14597\",\"abstract\":\"Исследовано влияние буферного давления Ar и расстояния до источника вещества на морфометрические параметры массивов вертикально ориентированных нано- и микростержней ZnO, синтезированных карботермическим методом на подложках Si(100) с тонкопленочным подслоем ZnO. Проведены системные исследования бескаталитического роста, а также влияния катализаторов роста, таких как Au и Cu, на процесс формирования и размеры стержней. Продемонстрировано, что катализатор играет роль лишь на начальном этапе, и не участвует в дальнейшем росте стержней в применяемых условиях синтеза. Показана возможность управления средними диаметрами, длинами и плотностью поверхностного распределения стержней в диапазонах 100-300 nm, 1.5-9 mum и 2.8-5.3· 108 cm-2 соответственно.\",\"language\":\"ru\",\"number\":\"17\",\"urldate\":\"2023-11-11\",\"journal\":\"Письма в ЖТФ\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Захарченко\"],\"firstnames\":[\"И.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бунина\"],\"firstnames\":[\"О.\",\"А.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2013\",\"pages\":\"27–34\",\"bibtex\":\"@article{__2013-16,\\n\\ttitle = {Оптимизация карботермического синтеза массивов микро- и наностержней оксида цинка и их морфометрических параметров},\\n\\tvolume = {39},\\n\\turl = {http://journals.ioffe.ru/articles/14597},\\n\\tabstract = {Исследовано влияние буферного давления Ar и расстояния до источника вещества на морфометрические параметры массивов вертикально ориентированных нано- и микростержней ZnO, синтезированных карботермическим методом на подложках Si(100) с тонкопленочным подслоем ZnO. Проведены системные исследования бескаталитического роста, а также влияния катализаторов роста, таких как Au и Cu, на процесс формирования и размеры стержней. Продемонстрировано, что катализатор играет роль лишь на начальном этапе, и не участвует в дальнейшем росте стержней в применяемых условиях синтеза. Показана возможность управления средними диаметрами, длинами и плотностью поверхностного распределения стержней в диапазонах 100-300 nm, 1.5-9 mum и 2.8-5.3· 108 cm-2 соответственно.},\\n\\tlanguage = {ru},\\n\\tnumber = {17},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Письма в ЖТФ},\\n\\tauthor = {Лянгузов, Н. В. and Кайдашев, Е. М. and Захарченко, И. Н. and Бунина, О. А.},\\n\\tmonth = aug,\\n\\tyear = {2013},\\n\\tpages = {27--34},\\n}\\n\\n\",\"author_short\":[\"Лянгузов, Н. В.\",\"Кайдашев, Е. М.\",\"Захарченко, И. Н.\",\"Бунина, О. А.\"],\"key\":\"__2013-16\",\"id\":\"__2013-16\",\"bibbaseid\":\"-----2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/14597\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Структура и динамика решетки гетероструктур на основе феррита висмута и титаната бария-стронция\",\"volume\":\"55\",\"url\":\"http://journals.ioffe.ru/articles/1254\",\"abstract\":\"Исследования морфологии поверхности, параметров решетки и спектров комбинационного рассеяния выполнены на этапах последовательного формирования трехслойной гетероструктуры, состоящей из эпитаксиальных слоев Ba0.8Sr0.2TiO3 (BST) и (Bi0.98Nd0.02)FeO3 (BNFO). Методами рентгенографии определены структурные искажения, возникающие при последовательном осаждении слоев BST/BNFO/BST равной толщины. Обнаружено, что степень тетрагонального искажения пленки BST на MgO повышается после осаждения на ее поверхность пленки BNFO, что свидетельствует о появлении в BST сжимающих напряжений. На основании анализа поляризованных спектров КРС показано, что в слое BNFO наблюдается новое фазовое состояние, не реализующееся в объемных образцах. Показано, что в пленке BST, выращенной на поверхности BNFO степень тетрагональности оказывается выше, чем в такой же пленке, выращенной непосредственно на MgO.\",\"language\":\"ru\",\"number\":\"12\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Кхабири\"],\"firstnames\":[\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Анохин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бунина\"],\"firstnames\":[\"О.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Simon\"],\"firstnames\":[\"P.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2013\",\"pages\":\"2383–2391\",\"bibtex\":\"@article{__2013-17,\\n\\ttitle = {Структура и динамика решетки гетероструктур на основе феррита висмута и титаната бария-стронция},\\n\\tvolume = {55},\\n\\turl = {http://journals.ioffe.ru/articles/1254},\\n\\tabstract = {Исследования морфологии поверхности, параметров решетки и спектров комбинационного рассеяния выполнены на этапах последовательного формирования трехслойной гетероструктуры, состоящей из эпитаксиальных слоев Ba0.8Sr0.2TiO3 (BST) и (Bi0.98Nd0.02)FeO3 (BNFO). Методами рентгенографии определены структурные искажения, возникающие при последовательном осаждении слоев BST/BNFO/BST равной толщины. Обнаружено, что степень тетрагонального искажения пленки BST на MgO повышается после осаждения на ее поверхность пленки BNFO, что свидетельствует о появлении в BST сжимающих напряжений. На основании анализа поляризованных спектров КРС показано, что в слое BNFO наблюдается новое фазовое состояние, не реализующееся в объемных образцах. Показано, что в пленке BST, выращенной на поверхности BNFO степень тетрагональности оказывается выше, чем в такой же пленке, выращенной непосредственно на MgO.},\\n\\tlanguage = {ru},\\n\\tnumber = {12},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Кхабири, Г. and Анохин, А. С. and Бунина, О. А. and Головко, Ю. И. and Мухортов, В. М. and Широков, В. Б. and Юзюк, Ю. И. and Simon, P.},\\n\\tmonth = nov,\\n\\tyear = {2013},\\n\\tpages = {2383--2391},\\n}\\n\\n\",\"author_short\":[\"Кхабири, Г.\",\"Анохин, А. С.\",\"Бунина, О. А.\",\"Головко, Ю. И.\",\"Мухортов, В. М.\",\"Широков, В. Б.\",\"Юзюк, Ю. И.\",\"Simon, P.\"],\"key\":\"__2013-17\",\"id\":\"__2013-17\",\"bibbaseid\":\"-------simon--2013\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/1254\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Спектры комбинационного рассеяния керамик, пленок и сверхрешеток сегнетоэлектрических перовскитов (О б з о р)\",\"url\":\"http://journals.ioffe.ru/articles/598\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2012\",\"bibtex\":\"@article{__2012-4,\\n\\ttitle = {Спектры комбинационного рассеяния керамик, пленок и сверхрешеток сегнетоэлектрических перовскитов (О б з о р)},\\n\\turl = {http://journals.ioffe.ru/articles/598},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Юзюк, Ю. И.},\\n\\tmonth = apr,\\n\\tyear = {2012},\\n}\\n\\n\",\"author_short\":[\"Юзюк, Ю. И.\"],\"key\":\"__2012-4\",\"id\":\"__2012-4\",\"bibbaseid\":\"--2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/598\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Сравнительное исследование пленки BaTiO$_{\\\\textrm{3}}$ и сверхрешетки BaTiO$_{\\\\textrm{3}}$/(Ba$_{\\\\textrm{0.7}}$Sr$_{\\\\textrm{0.3}}$)TiO$_{\\\\textrm{3}}$ методами дифракции рентгеновских лучей и спектроскопии комбинационного рассеяния света\",\"volume\":\"54\",\"abstract\":\"Проведено сравнительное исследование эпитаксиальной пленки BaTiO3 и сверхрешетки состава BaTiO3/(Ba0.7Sr0.3)TiO3, изготовленных методом импульсного лазерного осаждения на подложках (100) MgO. На основе данных рентгеновской дифрактометрии установлена полная параллельная ориентация пленки и подложки, определены период модуляции сверхрешетки Lambda=28 nm, параметры ячейки, усредненной по периоду Lambda, и параметры ячеек слоев сверхрешетки. Согласно рентгенографическим данным, ячейка однокомпонентной пленки BaTiO3 и усредненная по периоду Lambda ячейка сверхрешетки являются псевдокубическими, однако анализ поляризационных характеристик спектров комбинационного рассеяния света позволил предположить моноклинную симметрию (Px=Py#0, Pz#0) в пленке и сверхрешетке. Обсуждается трансформация компонент мягкой моды, обусловленная деформацией эпитаксиальных слоев, образующих сверхрешетку.\",\"language\":\"ru\",\"number\":\"8\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Маслова\"],\"firstnames\":[\"О.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Захарченко\"],\"firstnames\":[\"И.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бунина\"],\"firstnames\":[\"О.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ortega\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kumar\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"R.\",\"S.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2012\",\"pages\":\"1526–1532\",\"bibtex\":\"@article{__2012-5,\\n\\ttitle = {Сравнительное исследование пленки {BaTiO}$_{\\\\textrm{3}}$ и сверхрешетки {BaTiO}$_{\\\\textrm{3}}$/({Ba}$_{\\\\textrm{0.7}}${Sr}$_{\\\\textrm{0.3}}$){TiO}$_{\\\\textrm{3}}$ методами дифракции рентгеновских лучей и спектроскопии комбинационного рассеяния света},\\n\\tvolume = {54},\\n\\tabstract = {Проведено сравнительное исследование эпитаксиальной пленки BaTiO3 и сверхрешетки состава BaTiO3/(Ba0.7Sr0.3)TiO3, изготовленных методом импульсного лазерного осаждения на подложках (100) MgO. На основе данных рентгеновской дифрактометрии установлена полная параллельная ориентация пленки и подложки, определены период модуляции сверхрешетки Lambda=28 nm, параметры ячейки, усредненной по периоду Lambda, и параметры ячеек слоев сверхрешетки. Согласно рентгенографическим данным, ячейка однокомпонентной пленки BaTiO3 и усредненная по периоду Lambda ячейка сверхрешетки являются псевдокубическими, однако анализ поляризационных характеристик спектров комбинационного рассеяния света позволил предположить моноклинную симметрию (Px=Py\\\\#0, Pz\\\\#0) в пленке и сверхрешетке. Обсуждается трансформация компонент мягкой моды, обусловленная деформацией эпитаксиальных слоев, образующих сверхрешетку.},\\n\\tlanguage = {ru},\\n\\tnumber = {8},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Маслова, О. А. and Захарченко, И. Н. and Бунина, О. А. and Юзюк, Ю. И. and Ortega, N. and Kumar, A. and Katiyar, R. S.},\\n\\tmonth = jul,\\n\\tyear = {2012},\\n\\tpages = {1526--1532},\\n}\\n\\n\",\"author_short\":[\"Маслова, О. А.\",\"Захарченко, И. Н.\",\"Бунина, О. А.\",\"Юзюк, Ю. И.\",\"Ortega, N.\",\"Kumar, A.\",\"Katiyar, R. S.\"],\"key\":\"__2012-5\",\"id\":\"__2012-5\",\"bibbaseid\":\"----ortega-kumar-katiyar-batiotextrm3batiotextrm3batextrm07srtextrm03tiotextrm3-2012\",\"role\":\"author\",\"urls\":{},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Влияние морфологии керамик BiFeO$_{\\\\textrm{3}}$ на электродинамические свойства в терагерцевом диапазоне частот\",\"volume\":\"54\",\"url\":\"http://journals.ioffe.ru/articles/623\",\"abstract\":\"Методами субмиллиметровой и инфракрасной Фурье-спектроскопии исследована природа вклада, дополнительного к фононному, в диэлектрическую проницаемость керамик феррита висмута. Выявлено, что его численное значение зависит от морфологических особенностей образцов, а природа обусловлена наличием дефектов и межкристаллитных границ. Отмечено влияние структурно-фазовых особенностей керамик феррита висмута на частоты линий антиферромагнитного резонанса.\",\"language\":\"ru\",\"number\":\"6\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Командин\"],\"firstnames\":[\"Г.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Торгашев\"],\"firstnames\":[\"В.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Волков\"],\"firstnames\":[\"А.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Породинков\"],\"firstnames\":[\"О.\",\"Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Пронин\"],\"firstnames\":[\"А.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Исхакова\"],\"firstnames\":[\"Л.\",\"Д.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Буш\"],\"firstnames\":[\"А.\",\"А.\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2012\",\"pages\":\"1120–1127\",\"bibtex\":\"@article{__2012-6,\\n\\ttitle = {Влияние морфологии керамик {BiFeO}$_{\\\\textrm{3}}$ на электродинамические свойства в терагерцевом диапазоне частот},\\n\\tvolume = {54},\\n\\turl = {http://journals.ioffe.ru/articles/623},\\n\\tabstract = {Методами субмиллиметровой и инфракрасной Фурье-спектроскопии исследована природа вклада, дополнительного к фононному, в диэлектрическую проницаемость керамик феррита висмута. Выявлено, что его численное значение зависит от морфологических особенностей образцов, а природа обусловлена наличием дефектов и межкристаллитных границ. Отмечено влияние структурно-фазовых особенностей керамик феррита висмута на частоты линий антиферромагнитного резонанса.},\\n\\tlanguage = {ru},\\n\\tnumber = {6},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Командин, Г. А. and Торгашев, В. И. and Волков, А. А. and Породинков, О. Е. and Пронин, А. А. and Исхакова, Л. Д. and Буш, А. А.},\\n\\tmonth = may,\\n\\tyear = {2012},\\n\\tpages = {1120--1127},\\n}\\n\\n\",\"author_short\":[\"Командин, Г. А.\",\"Торгашев, В. И.\",\"Волков, А. А.\",\"Породинков, О. Е.\",\"Пронин, А. А.\",\"Исхакова, Л. Д.\",\"Буш, А. А.\"],\"key\":\"__2012-6\",\"id\":\"__2012-6\",\"bibbaseid\":\"-------bifeotextrm3-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/623\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Магнитный и диэлектрический отклик кобальт-хромовой шпинели CoCr$_{\\\\textrm{2}}$O$_{\\\\textrm{4}}$ в терагерцевой области частот\",\"volume\":\"54\",\"url\":\"http://journals.ioffe.ru/articles/523\",\"abstract\":\"Методами субмиллиметровой спектроскопии и инфракрасной Фурье-спектроскопии исследована природа фононных и магнонных мод в мультиферроике CoCr2O4 со структурой кубической шпинели. Впервые измерена температурная эволюция обменного оптического магнона в ферримагнитной (TC=94 K) и двух низкосимметричных (TS~ 26 K, Tlock-in=14.5 K) фазах CoCr2O4 вплоть до T=5 K в нулевом магнитном поле. Показано, что зарегистрированный магнон не является ферримагнитным параметром порядка и, вероятнее всего, обусловлен прецессией спинов в подрешетках кобальта. В точках магнитных фазовых переходов осцилляторные параметры двух наиболее низкочастотных фононных мод проявляют аномальную температурную зависимость, что свидетельствует о значительном взаимодействии между магнитной и фононной подсистемами. На основании того, что параметр затухания фононной моды, обусловленной колебаниями тетраэдров CoO4, при переходе CoCr2O4 в состояние мультиферроика (T\\\\textlessTS) увеличивается на 25%, сделано предположение о структурных изменениях в решетке с потерей пространственной центросимметричности среды.\",\"language\":\"ru\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Торгашев\"],\"firstnames\":[\"В.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Прохоров\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Командин\"],\"firstnames\":[\"Г.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Жукова\"],\"firstnames\":[\"Е.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Анзин\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Таланов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Рабкин\"],\"firstnames\":[\"Л.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Буш\"],\"firstnames\":[\"А.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Горшунов\"],\"firstnames\":[\"Б.\",\"П.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2012\",\"pages\":\"330–339\",\"bibtex\":\"@article{__2012-7,\\n\\ttitle = {Магнитный и диэлектрический отклик кобальт-хромовой шпинели {CoCr}$_{\\\\textrm{2}}${O}$_{\\\\textrm{4}}$ в терагерцевой области частот},\\n\\tvolume = {54},\\n\\turl = {http://journals.ioffe.ru/articles/523},\\n\\tabstract = {Методами субмиллиметровой спектроскопии и инфракрасной Фурье-спектроскопии исследована природа фононных и магнонных мод в мультиферроике CoCr2O4 со структурой кубической шпинели. Впервые измерена температурная эволюция обменного оптического магнона в ферримагнитной (TC=94 K) и двух низкосимметричных (TS{\\\\textasciitilde} 26 K, Tlock-in=14.5 K) фазах CoCr2O4 вплоть до T=5 K в нулевом магнитном поле. Показано, что зарегистрированный магнон не является ферримагнитным параметром порядка и, вероятнее всего, обусловлен прецессией спинов в подрешетках кобальта. В точках магнитных фазовых переходов осцилляторные параметры двух наиболее низкочастотных фононных мод проявляют аномальную температурную зависимость, что свидетельствует о значительном взаимодействии между магнитной и фононной подсистемами. На основании того, что параметр затухания фононной моды, обусловленной колебаниями тетраэдров CoO4, при переходе CoCr2O4 в состояние мультиферроика (T{\\\\textless}TS) увеличивается на 25\\\\%, сделано предположение о структурных изменениях в решетке с потерей пространственной центросимметричности среды.},\\n\\tlanguage = {ru},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Торгашев, В. И. and Прохоров, А. С. and Командин, Г. А. and Жукова, Е. С. and Анзин, В. Б. and Таланов, В. М. and Рабкин, Л. М. and Буш, А. А. and Dressel, M. and Горшунов, Б. П.},\\n\\tmonth = jan,\\n\\tyear = {2012},\\n\\tpages = {330--339},\\n}\\n\\n\",\"author_short\":[\"Торгашев, В. И.\",\"Прохоров, А. С.\",\"Командин, Г. А.\",\"Жукова, Е. С.\",\"Анзин, В. Б.\",\"Таланов, В. М.\",\"Рабкин, Л. М.\",\"Буш, А. А.\",\"Dressel, M.\",\"Горшунов, Б. П.\"],\"key\":\"__2012-7\",\"id\":\"__2012-7\",\"bibbaseid\":\"--------etal-cocrtextrm2otextrm4-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/523\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Нелинейно-оптическая микроскопия и спектроскопия сегнетоэлектрических и мультиферроидных материалов\",\"volume\":\"54\",\"url\":\"http://journals.ioffe.ru/articles/840\",\"abstract\":\"Раcсмотрены особенности применения двухфотонной микроскопии и спектроскопии для исследования мультиферроидных и пьезоэлектрических наноразмерных структур. Для наноразмерных планарных мультислойных структур титанат бария-стронция/феррит висмута показано проявление в нелинейно-оптическом отклике локальных электроиндуцированного и магнитоиндуцированного вкладов в определенных спектральных диапазонах. Для пьезоэлектрических био-микротрубок пептидов показано, что максимальное значение интенсивности второй гармоники не меняется вдоль трубки, в то время как направление поляризации изменяется значительно.\",\"language\":\"ru\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Мишина\"],\"firstnames\":[\"Е.\",\"Д.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Семин\"],\"firstnames\":[\"С.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Швырков\"],\"firstnames\":[\"К.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кудрявцев\"],\"firstnames\":[\"А.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ильин\"],\"firstnames\":[\"Н.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Шерстюк\"],\"firstnames\":[\"Н.\",\"Э.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2012\",\"pages\":\"836–841\",\"bibtex\":\"@article{_-_2012,\\n\\ttitle = {Нелинейно-оптическая микроскопия и спектроскопия сегнетоэлектрических и мультиферроидных материалов},\\n\\tvolume = {54},\\n\\turl = {http://journals.ioffe.ru/articles/840},\\n\\tabstract = {Раcсмотрены особенности применения двухфотонной микроскопии и спектроскопии для исследования мультиферроидных и пьезоэлектрических наноразмерных структур. Для наноразмерных планарных мультислойных структур титанат бария-стронция/феррит висмута показано проявление в нелинейно-оптическом отклике локальных электроиндуцированного и магнитоиндуцированного вкладов в определенных спектральных диапазонах. Для пьезоэлектрических био-микротрубок пептидов показано, что максимальное значение интенсивности второй гармоники не меняется вдоль трубки, в то время как направление поляризации изменяется значительно.},\\n\\tlanguage = {ru},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Мишина, Е. Д. and Семин, С. В. and Швырков, К. В. and Кудрявцев, А. В. and Ильин, Н. А. and Шерстюк, Н. Э. and Мухортов, В. М.},\\n\\tmonth = apr,\\n\\tyear = {2012},\\n\\tpages = {836--841},\\n}\\n\\n\",\"author_short\":[\"Мишина, Е. Д.\",\"Семин, С. В.\",\"Швырков, К. В.\",\"Кудрявцев, А. В.\",\"Ильин, Н. А.\",\"Шерстюк, Н. Э.\",\"Мухортов, В. М.\"],\"key\":\"_-_2012\",\"id\":\"_-_2012\",\"bibbaseid\":\"--------2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/840\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Электропроводность и термо-э.д.с. кристаллов титаната свинца\",\"volume\":\"54\",\"url\":\"http://journals.ioffe.ru/articles/859\",\"abstract\":\"Исследованы температурные зависимости коэффициента термо-э.д.с. alpha и удельной объемной электропроводности sigmaV в температурном интервале 400-550 K, где в кристаллах титаната свинца наблюдаются аномалии диэлектрической проницаемости varepsilon, не связанные с фазовым переходом. Установлено, что в указанном интервале температур alpha имеет максимум и во многих кристаллах меняет знак, при этом sigmaV снижается. Сделано предположение о том, что аномалии alpha и sigmaV, коррелирующие с аномалиями varepsilon, обусловлены термоактивацией ловушек электронов, что приводит к компенсации проводимости p-типа. Определены концентрация свободных носителей заряда и их дрейфовая подвижность в парафазе вблизи точки Кюри. Эти данные указывают на возможность полного внутреннего экранирования связанного заряда Ps.\",\"language\":\"ru\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Гавриляченко\"],\"firstnames\":[\"В.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Семенчев\"],\"firstnames\":[\"А.\",\"Ф.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Авакян\"],\"firstnames\":[\"Е.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Панченко\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мартыщенко\"],\"firstnames\":[\"А.\",\"В.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2012\",\"pages\":\"901–902\",\"bibtex\":\"@article{__2012-8,\\n\\ttitle = {Электропроводность и термо-э.д.с. кристаллов титаната свинца},\\n\\tvolume = {54},\\n\\turl = {http://journals.ioffe.ru/articles/859},\\n\\tabstract = {Исследованы температурные зависимости коэффициента термо-э.д.с. alpha и удельной объемной электропроводности sigmaV в температурном интервале 400-550 K, где в кристаллах титаната свинца наблюдаются аномалии диэлектрической проницаемости varepsilon, не связанные с фазовым переходом. Установлено, что в указанном интервале температур alpha имеет максимум и во многих кристаллах меняет знак, при этом sigmaV снижается. Сделано предположение о том, что аномалии alpha и sigmaV, коррелирующие с аномалиями varepsilon, обусловлены термоактивацией ловушек электронов, что приводит к компенсации проводимости p-типа. Определены концентрация свободных носителей заряда и их дрейфовая подвижность в парафазе вблизи точки Кюри. Эти данные указывают на возможность полного внутреннего экранирования связанного заряда Ps.},\\n\\tlanguage = {ru},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Гавриляченко, В. Г. and Семенчев, А. Ф. and Авакян, Е. И. and Панченко, Е. М. and Мартыщенко, А. В.},\\n\\tmonth = apr,\\n\\tyear = {2012},\\n\\tpages = {901--902},\\n}\\n\\n\",\"author_short\":[\"Гавриляченко, В. Г.\",\"Семенчев, А. Ф.\",\"Авакян, Е. И.\",\"Панченко, Е. М.\",\"Мартыщенко, А. В.\"],\"key\":\"__2012-8\",\"id\":\"__2012-8\",\"bibbaseid\":\"------2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/859\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":1,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Электродинамические характеристики стекол составов LaBGeO$_{\\\\textrm{5}}$ и LaBSiO$_{\\\\textrm{5}}$ в терагерцевом и ИК-диапазонах\",\"volume\":\"54\",\"url\":\"http://journals.ioffe.ru/articles/780\",\"abstract\":\"Сравниваются методы расчета функций диэлектрического отклика разупорядоченных веществ по пропусканию (субмиллиметровый диапазон) и отражению (ИК диапазон) на примере функциональных стекол LaBGeO5 и LaBSiO5 со структурой стиллвеллита. В рамках четырехпараметрической факторизованной модели дисперсии определены диэлектрические параметры стекол LaBGeO5 и LaBSiO5 и выполнено соотнесение спектральных полос с фрагментами структуры.\",\"language\":\"ru\",\"number\":\"11\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Командин\"],\"firstnames\":[\"Г.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Сигаев\"],\"firstnames\":[\"В.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Торгашев\"],\"firstnames\":[\"В.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лотарев\"],\"firstnames\":[\"С.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Породинков\"],\"firstnames\":[\"О.\",\"Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Спектор\"],\"firstnames\":[\"И.\",\"Е.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2012\",\"pages\":\"2058–2065\",\"bibtex\":\"@article{__2012-9,\\n\\ttitle = {Электродинамические характеристики стекол составов {LaBGeO}$_{\\\\textrm{5}}$ и {LaBSiO}$_{\\\\textrm{5}}$ в терагерцевом и ИК-диапазонах},\\n\\tvolume = {54},\\n\\turl = {http://journals.ioffe.ru/articles/780},\\n\\tabstract = {Сравниваются методы расчета функций диэлектрического отклика разупорядоченных веществ по пропусканию (субмиллиметровый диапазон) и отражению (ИК диапазон) на примере функциональных стекол LaBGeO5 и LaBSiO5 со структурой стиллвеллита. В рамках четырехпараметрической факторизованной модели дисперсии определены диэлектрические параметры стекол LaBGeO5 и LaBSiO5 и выполнено соотнесение спектральных полос с фрагментами структуры.},\\n\\tlanguage = {ru},\\n\\tnumber = {11},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Командин, Г. А. and Сигаев, В. Н. and Торгашев, В. И. and Лотарев, С. В. and Породинков, О. Е. and Спектор, И. Е.},\\n\\tmonth = oct,\\n\\tyear = {2012},\\n\\tpages = {2058--2065},\\n}\\n\\n\",\"author_short\":[\"Командин, Г. А.\",\"Сигаев, В. Н.\",\"Торгашев, В. И.\",\"Лотарев, С. В.\",\"Породинков, О. Е.\",\"Спектор, И. Е.\"],\"key\":\"__2012-9\",\"id\":\"__2012-9\",\"bibbaseid\":\"------labgeotextrm5labsiotextrm5-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/780\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Исследование сверхрешеток BaTiO$_{\\\\textrm{3}}$/(Ba,Sr)TiO$_{\\\\textrm{3}}$ методом дифракции рентгеновских лучей\",\"volume\":\"54\",\"url\":\"http://journals.ioffe.ru/articles/878\",\"abstract\":\"Методом дифракции рентгеновских лучей проведено исследование образцов сверхрешеток BaTiO3/ (Ba1-xSrx)TiO3 (ВТ/BST-x). Установлена полная параллельная ориентация всех пленок и подложки, определены периоды модуляции Lambda сверхрешеток, параметры ячейки, усредненной по периоду Lambda, и параметры отдельных компонент сверхрешеток.\",\"language\":\"ru\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Маслова\"],\"firstnames\":[\"О.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Захарченко\"],\"firstnames\":[\"И.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бунина\"],\"firstnames\":[\"О.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ortega\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kumar\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"R.\",\"S.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2012\",\"pages\":\"953–955\",\"bibtex\":\"@article{__2012-10,\\n\\ttitle = {Исследование сверхрешеток {BaTiO}$_{\\\\textrm{3}}$/({Ba},{Sr}){TiO}$_{\\\\textrm{3}}$ методом дифракции рентгеновских лучей},\\n\\tvolume = {54},\\n\\turl = {http://journals.ioffe.ru/articles/878},\\n\\tabstract = {Методом дифракции рентгеновских лучей проведено исследование образцов сверхрешеток BaTiO3/ (Ba1-xSrx)TiO3 (ВТ/BST-x). Установлена полная параллельная ориентация всех пленок и подложки, определены периоды модуляции Lambda сверхрешеток, параметры ячейки, усредненной по периоду Lambda, и параметры отдельных компонент сверхрешеток.},\\n\\tlanguage = {ru},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Маслова, О. А. and Захарченко, И. Н. and Бунина, О. А. and Юзюк, Ю. И. and Ortega, N. and Kumar, A. and Katiyar, R. S.},\\n\\tmonth = apr,\\n\\tyear = {2012},\\n\\tpages = {953--955},\\n}\\n\\n\",\"author_short\":[\"Маслова, О. А.\",\"Захарченко, И. Н.\",\"Бунина, О. А.\",\"Юзюк, Ю. И.\",\"Ortega, N.\",\"Kumar, A.\",\"Katiyar, R. S.\"],\"key\":\"__2012-10\",\"id\":\"__2012-10\",\"bibbaseid\":\"----ortega-kumar-katiyar-batiotextrm3basrtiotextrm3-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/878\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Магнетронное и импульсное лазерное напыление наночастиц и несплошных пленок Ag и Au и исследование их оптических свойств\",\"volume\":\"82\",\"url\":\"http://journals.ioffe.ru/articles/10727\",\"abstract\":\"Исследованы различные режимы получения наночастиц Ag и Au методами магнетронного и импульсного лазерного напыления и особенности спектров поглощения, связанные с плазмонными резонансами. Для получения наночастиц серебра малых размеров (5-10 nm) с большой плотностью поверхностного распределения определен оптимальный режим получения: повышенное давление аргона (2.5·10-2 Torr) и малое напряжение разряда (100 V). Массивы наночастиц Au, полученные методом импульского лазерного напыления, проявляют более высокую однородность при напылении на подложки при температуре 200oC в вакууме, нежели при комнатной температуре в атмосфере аргона. Показано, что положение максимума плазмонного поглощения сдвигается в область меньших длин волн при снижении значения эквивалентной толщины пленок металлов и зависит не только от данного значения, но и от типа подложки, которая определяет морфологические характеристики массивов наночастиц.\",\"language\":\"ru\",\"number\":\"10\",\"urldate\":\"2023-11-11\",\"journal\":\"Журнал технической физики\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"В.\",\"Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2012\",\"pages\":\"90–95\",\"bibtex\":\"@article{__2012-11,\\n\\ttitle = {Магнетронное и импульсное лазерное напыление наночастиц и несплошных пленок {Ag} и {Au} и исследование их оптических свойств},\\n\\tvolume = {82},\\n\\turl = {http://journals.ioffe.ru/articles/10727},\\n\\tabstract = {Исследованы различные режимы получения наночастиц Ag и Au методами магнетронного и импульсного лазерного напыления и особенности спектров поглощения, связанные с плазмонными резонансами. Для получения наночастиц серебра малых размеров (5-10 nm) с большой плотностью поверхностного распределения определен оптимальный режим получения: повышенное давление аргона (2.5·10-2 Torr) и малое напряжение разряда (100 V). Массивы наночастиц Au, полученные методом импульского лазерного напыления, проявляют более высокую однородность при напылении на подложки при температуре 200oC в вакууме, нежели при комнатной температуре в атмосфере аргона. Показано, что положение максимума плазмонного поглощения сдвигается в область меньших длин волн при снижении значения эквивалентной толщины пленок металлов и зависит не только от данного значения, но и от типа подложки, которая определяет морфологические характеристики массивов наночастиц.},\\n\\tlanguage = {ru},\\n\\tnumber = {10},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Журнал технической физики},\\n\\tauthor = {Лянгузов, Н. В. and Кайдашев, В. Е. and Широков, В. Б. and Кайдашев, Е. М.},\\n\\tmonth = sep,\\n\\tyear = {2012},\\n\\tpages = {90--95},\\n}\\n\\n\",\"author_short\":[\"Лянгузов, Н. В.\",\"Кайдашев, В. Е.\",\"Широков, В. Б.\",\"Кайдашев, Е. М.\"],\"key\":\"__2012-11\",\"id\":\"__2012-11\",\"bibbaseid\":\"----agau-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/10727\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Фазовые переходы в поляризованных гетерофазных системах на основе цирконата-титаната свинца\",\"volume\":\"54\",\"url\":\"http://journals.ioffe.ru/articles/850\",\"abstract\":\"Исследованы зависимости токов деполяризации, определены фазовые превращения между фазами R3c, R3m, P4mm и Pm3m в образцах пятикомпонентной гетерофазной сегнетокерамики на основе цирконата-титаната свинца.\",\"language\":\"ru\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Милов\"],\"firstnames\":[\"Е.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Акбаева\"],\"firstnames\":[\"Г.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гавриляченко\"],\"firstnames\":[\"В.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Семенчев\"],\"firstnames\":[\"А.\",\"Ф.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2012\",\"pages\":\"878–879\",\"bibtex\":\"@article{__2012-12,\\n\\ttitle = {Фазовые переходы в поляризованных гетерофазных системах на основе цирконата-титаната свинца},\\n\\tvolume = {54},\\n\\turl = {http://journals.ioffe.ru/articles/850},\\n\\tabstract = {Исследованы зависимости токов деполяризации, определены фазовые превращения между фазами R3c, R3m, P4mm и Pm3m в образцах пятикомпонентной гетерофазной сегнетокерамики на основе цирконата-титаната свинца.},\\n\\tlanguage = {ru},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Милов, Е. В. and Акбаева, Г. М. and Гавриляченко, В. Г. and Семенчев, А. Ф.},\\n\\tmonth = apr,\\n\\tyear = {2012},\\n\\tpages = {878--879},\\n}\\n\\n\",\"author_short\":[\"Милов, Е. В.\",\"Акбаева, Г. М.\",\"Гавриляченко, В. Г.\",\"Семенчев, А. Ф.\"],\"key\":\"__2012-12\",\"id\":\"__2012-12\",\"bibbaseid\":\"-----2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/850\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Structural Properties of Composite Thin Films BiFeO$_{\\\\textrm{3}}$ - Ba$_{\\\\textrm{0.8}}$Sr$_{\\\\textrm{0.2}}$TiO$_{\\\\textrm{3}}$\",\"volume\":\"439\",\"issn\":\"0015-0193\",\"url\":\"https://doi.org/10.1080/00150193.2012.741920\",\"doi\":\"10.1080/00150193.2012.741920\",\"abstract\":\"The results of X-ray diffraction study of a new promising magnetoelectric composite films with alternating layers of barium strontium titanate and bismuth ferrite with layer thicknesses d = 6–200 nm are presented. All films show epitaxial growth on the MgO single crystals substrates. The 00L profiles for thick layered films (d \\\\textgreater 15 nm) consist of the two reflections corresponding to the separate coherent scattering regions of composite layers. The XRD patterns of thin layered films testify the formation of superlattice. The mean microstrain and mean size of coherent scattering regions were determined using the Willamson-Hall approach.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Bunina\"],\"firstnames\":[\"O.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zakharchenko\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golovko\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mukhortov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Stryukov\"],\"firstnames\":[\"D.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2012\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2012.741920\",\"keywords\":\"X-ray diffraction, superlattice, Thin films, magnetoelectric composite\",\"pages\":\"67–73\",\"bibtex\":\"@article{bunina_structural_2012,\\n\\ttitle = {Structural {Properties} of {Composite} {Thin} {Films} {BiFeO}$_{\\\\textrm{3}}$ - {Ba}$_{\\\\textrm{0.8}}${Sr}$_{\\\\textrm{0.2}}${TiO}$_{\\\\textrm{3}}$},\\n\\tvolume = {439},\\n\\tissn = {0015-0193},\\n\\turl = {https://doi.org/10.1080/00150193.2012.741920},\\n\\tdoi = {10.1080/00150193.2012.741920},\\n\\tabstract = {The results of X-ray diffraction study of a new promising magnetoelectric composite films with alternating layers of barium strontium titanate and bismuth ferrite with layer thicknesses d = 6–200 nm are presented. All films show epitaxial growth on the MgO single crystals substrates. The 00L profiles for thick layered films (d {\\\\textgreater} 15 nm) consist of the two reflections corresponding to the separate coherent scattering regions of composite layers. The XRD patterns of thin layered films testify the formation of superlattice. The mean microstrain and mean size of coherent scattering regions were determined using the Willamson-Hall approach.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Bunina, O. A. and Zakharchenko, I. N. and Golovko, Yu. I. and Mukhortov, V. M. and Stryukov, D. V. and Yuzyuk, Yu. I.},\\n\\tmonth = jan,\\n\\tyear = {2012},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/00150193.2012.741920},\\n\\tkeywords = {X-ray diffraction, superlattice, Thin films, magnetoelectric composite},\\n\\tpages = {67--73},\\n}\\n\\n\",\"author_short\":[\"Bunina, O. A.\",\"Zakharchenko, I. N.\",\"Golovko, Y. I.\",\"Mukhortov, V. M.\",\"Stryukov, D. V.\",\"Yuzyuk, Y. I.\"],\"key\":\"bunina_structural_2012\",\"id\":\"bunina_structural_2012\",\"bibbaseid\":\"bunina-zakharchenko-golovko-mukhortov-stryukov-yuzyuk-structuralpropertiesofcompositethinfilmsbifeotextrm3batextrm08srtextrm02tiotextrm3-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/00150193.2012.741920\"},\"keyword\":[\"X-ray diffraction\",\"superlattice\",\"Thin films\",\"magnetoelectric composite\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Ferroelectricity in spinel solid solution Co$_{\\\\textrm{0.8}}$Ni$_{\\\\textrm{0.2}}$Cr$_{\\\\textrm{2}}$O$_{\\\\textrm{4}}$\",\"volume\":\"85\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.85.214112\",\"doi\":\"10.1103/PhysRevB.85.214112\",\"abstract\":\"Temperature dependencies of dielectric permittivity and loss tangent (at frequencies 0.1–200 kHz) together with thermally stimulated depolarization currents, magnetization, and Mössbauer spectra of ceramic solid solutions Co1−xNixCr2O4 (x = 0, 0.2, 0.4, 0.6, 1.0) are studied at temperatures from 80 to 350 K. We find evidence of two reversible phase transitions located at T1 and T2 (220 and 245 K, respectively, for x = 0.2), of occurrence of pyroelectric properties below T2, as well as of a phase transition to magnetically ordered state of ferrimagnetic type (below 86 K for x = 0.2). The obtained results evidence that the compounds possess, additionally to magnetic, ferroelectric properties and are thus new members in the family of multiferroics.\",\"number\":\"21\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Bush\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shkuratov\"],\"firstnames\":[\"V.\",\"Ya.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kamentsev\"],\"firstnames\":[\"K.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"E.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"B.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2012\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"214112\",\"bibtex\":\"@article{bush_ferroelectricity_2012,\\n\\ttitle = {Ferroelectricity in spinel solid solution {Co}$_{\\\\textrm{0.8}}${Ni}$_{\\\\textrm{0.2}}${Cr}$_{\\\\textrm{2}}${O}$_{\\\\textrm{4}}$},\\n\\tvolume = {85},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.85.214112},\\n\\tdoi = {10.1103/PhysRevB.85.214112},\\n\\tabstract = {Temperature dependencies of dielectric permittivity and loss tangent (at frequencies 0.1–200 kHz) together with thermally stimulated depolarization currents, magnetization, and Mössbauer spectra of ceramic solid solutions Co1−xNixCr2O4 (x = 0, 0.2, 0.4, 0.6, 1.0) are studied at temperatures from 80 to 350 K. We find evidence of two reversible phase transitions located at T1 and T2 (220 and 245 K, respectively, for x = 0.2), of occurrence of pyroelectric properties below T2, as well as of a phase transition to magnetically ordered state of ferrimagnetic type (below 86 K for x = 0.2). The obtained results evidence that the compounds possess, additionally to magnetic, ferroelectric properties and are thus new members in the family of multiferroics.},\\n\\tnumber = {21},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Bush, A. A. and Shkuratov, V. Ya. and Kamentsev, K. E. and Prokhorov, A. S. and Zhukova, E. S. and Gorshunov, B. P. and Torgashev, V. I.},\\n\\tmonth = jun,\\n\\tyear = {2012},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {214112},\\n}\\n\\n\",\"author_short\":[\"Bush, A. A.\",\"Shkuratov, V. Y.\",\"Kamentsev, K. E.\",\"Prokhorov, A. S.\",\"Zhukova, E. S.\",\"Gorshunov, B. P.\",\"Torgashev, V. I.\"],\"key\":\"bush_ferroelectricity_2012\",\"id\":\"bush_ferroelectricity_2012\",\"bibbaseid\":\"bush-shkuratov-kamentsev-prokhorov-zhukova-gorshunov-torgashev-ferroelectricityinspinelsolidsolutioncotextrm08nitextrm02crtextrm2otextrm4-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.85.214112\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Raman Spectra of PbFe$_{\\\\textrm{0.5}}$Nb$_{\\\\textrm{0.5}}$O$_{\\\\textrm{3}}$Multiferroic Single Crystals and Ceramics\",\"volume\":\"438\",\"issn\":\"0015-0193\",\"url\":\"https://doi.org/10.1080/00150193.2012.747391\",\"doi\":\"10.1080/00150193.2012.747391\",\"abstract\":\"Room temperature Raman spectra of both PbFe0.5Nb0.5O3 (PFN) single crystal and ceramics were found to contain 14 bands, namely 64, 130, 200, 265, 427, 488, 560, 703, 785, 861, 971, 1123, 1236, and 1383 cm−1. For the first time distinct anomalies in the temperature dependences of frequency and/or full width at half maximum were observed for some lines in the Raman spectra of PFN single crystal at both antiferromagnetic (≈150 K) and ferroelectric (≈350 K) phase transitions.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Druzhinina\"],\"firstnames\":[\"N.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Raevski\"],\"firstnames\":[\"I.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Marssi\"],\"firstnames\":[\"M.\",\"El\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Laguta\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Raevskaya\"],\"firstnames\":[\"S.\",\"I.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2012\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2012.747391\",\"keywords\":\"phase transition, ferroelectric, lead iron niobate, multiferroic, Raman spectra\",\"pages\":\"107–114\",\"bibtex\":\"@article{druzhinina_raman_2012,\\n\\ttitle = {Raman {Spectra} of {PbFe}$_{\\\\textrm{0.5}}${Nb}$_{\\\\textrm{0.5}}${O}$_{\\\\textrm{3}}${Multiferroic} {Single} {Crystals} and {Ceramics}},\\n\\tvolume = {438},\\n\\tissn = {0015-0193},\\n\\turl = {https://doi.org/10.1080/00150193.2012.747391},\\n\\tdoi = {10.1080/00150193.2012.747391},\\n\\tabstract = {Room temperature Raman spectra of both PbFe0.5Nb0.5O3 (PFN) single crystal and ceramics were found to contain 14 bands, namely 64, 130, 200, 265, 427, 488, 560, 703, 785, 861, 971, 1123, 1236, and 1383 cm−1. For the first time distinct anomalies in the temperature dependences of frequency and/or full width at half maximum were observed for some lines in the Raman spectra of PFN single crystal at both antiferromagnetic (≈150 K) and ferroelectric (≈350 K) phase transitions.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Druzhinina, N. S. and Yuzyuk, Yu. I. and Raevski, I. P. and Marssi, M. El and Laguta, V. V. and Raevskaya, S. I.},\\n\\tmonth = jan,\\n\\tyear = {2012},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/00150193.2012.747391},\\n\\tkeywords = {phase transition, ferroelectric, lead iron niobate, multiferroic, Raman spectra},\\n\\tpages = {107--114},\\n}\\n\\n\",\"author_short\":[\"Druzhinina, N. S.\",\"Yuzyuk, Y. I.\",\"Raevski, I. P.\",\"Marssi, M. E.\",\"Laguta, V. V.\",\"Raevskaya, S. I.\"],\"key\":\"druzhinina_raman_2012\",\"id\":\"druzhinina_raman_2012\",\"bibbaseid\":\"druzhinina-yuzyuk-raevski-marssi-laguta-raevskaya-ramanspectraofpbfetextrm05nbtextrm05otextrm3multiferroicsinglecrystalsandceramics-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/00150193.2012.747391\"},\"keyword\":[\"phase transition\",\"ferroelectric\",\"lead iron niobate\",\"multiferroic\",\"Raman spectra\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Ferroelectric and Dielectric Properties of BaTiO$_{\\\\textrm{3}}$/Ba$_{\\\\textrm{0.30}}$Sr$_{\\\\textrm{0.70}}$TiO$_{\\\\textrm{3}}$ Superlattices\",\"volume\":\"134\",\"issn\":\"1058-4587\",\"url\":\"https://doi.org/10.1080/10584587.2012.673980\",\"doi\":\"10.1080/10584587.2012.673980\",\"abstract\":\"BaTiO3/Ba0.30Sr0.70TiO3 (BT/BST3070) artificial superlattice (SL) was fabricated by pulsed laser deposition on La0.67Sr0.33MnO3 (LSMO) coated (001) MgO substrates. Satellite reflections in X-ray diffraction are used to calculate the periodicity of SL structure indicates a period ∼14 nm. Cross polarized Raman spectra show upward shift of the E(1TO) soft mode, this is markedly changed with respect to its parent BT layer thin film. The BT/BST3070 SL illustrates high dielectric constant (1100-1300) and low loss tangent (\\\\textless0.1) below to 104 Hz. Polarization and dielectric constant show strong switching behavior under applied external electric field with well saturated hysteresis loop and high dielectric tunability.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Integrated Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Ortega\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kumar\"],\"firstnames\":[\"Ashok\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"YU.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Scott\"],\"firstnames\":[\"J.\",\"F.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"Rams.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2012\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/10584587.2012.673980\",\"keywords\":\"Superlattices, BT/BST, dielectric, ferroelectric, PLD\",\"pages\":\"139–145\",\"bibtex\":\"@article{ortega_ferroelectric_2012,\\n\\ttitle = {Ferroelectric and {Dielectric} {Properties} of {BaTiO}$_{\\\\textrm{3}}$/{Ba}$_{\\\\textrm{0.30}}${Sr}$_{\\\\textrm{0.70}}${TiO}$_{\\\\textrm{3}}$ {Superlattices}},\\n\\tvolume = {134},\\n\\tissn = {1058-4587},\\n\\turl = {https://doi.org/10.1080/10584587.2012.673980},\\n\\tdoi = {10.1080/10584587.2012.673980},\\n\\tabstract = {BaTiO3/Ba0.30Sr0.70TiO3 (BT/BST3070) artificial superlattice (SL) was fabricated by pulsed laser deposition on La0.67Sr0.33MnO3 (LSMO) coated (001) MgO substrates. Satellite reflections in X-ray diffraction are used to calculate the periodicity of SL structure indicates a period ∼14 nm. Cross polarized Raman spectra show upward shift of the E(1TO) soft mode, this is markedly changed with respect to its parent BT layer thin film. The BT/BST3070 SL illustrates high dielectric constant (1100-1300) and low loss tangent ({\\\\textless}0.1) below to 104 Hz. Polarization and dielectric constant show strong switching behavior under applied external electric field with well saturated hysteresis loop and high dielectric tunability.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Integrated Ferroelectrics},\\n\\tauthor = {Ortega, N. and Kumar, Ashok and Yuzyuk, YU. I. and Scott, J. F. and Katiyar, Rams.},\\n\\tmonth = jan,\\n\\tyear = {2012},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/10584587.2012.673980},\\n\\tkeywords = {Superlattices, BT/BST, dielectric, ferroelectric, PLD},\\n\\tpages = {139--145},\\n}\\n\\n\",\"author_short\":[\"Ortega, N.\",\"Kumar, A.\",\"Yuzyuk, Y. I.\",\"Scott, J. F.\",\"Katiyar, R.\"],\"key\":\"ortega_ferroelectric_2012\",\"id\":\"ortega_ferroelectric_2012\",\"bibbaseid\":\"ortega-kumar-yuzyuk-scott-katiyar-ferroelectricanddielectricpropertiesofbatiotextrm3batextrm030srtextrm070tiotextrm3superlattices-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/10584587.2012.673980\"},\"keyword\":[\"Superlattices\",\"BT/BST\",\"dielectric\",\"ferroelectric\",\"PLD\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Ferroelectric Q and antiferroelectric P phases' coexistence and local phase transitions in oxygen-deficient NaNb$_{\\\\textrm{3}}$ single crystal: micro-Raman, dielectric and dilatometric studies\",\"volume\":\"43\",\"copyright\":\"Copyright © 2012 John Wiley & Sons, Ltd.\",\"issn\":\"1097-4555\",\"shorttitle\":\"Ferroelectric Q and antiferroelectric P phases' coexistence and local phase transitions in oxygen-deficient NaNbO3 single crystal\",\"url\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/jrs.3140\",\"doi\":\"10.1002/jrs.3140\",\"abstract\":\"Micro-Raman studies of oxygen-deficient gray-colored NaNbO3 single crystals have shown that at room temperature both antiferroelectric P and ferroelectric Q phases are present simultaneously as separate regions tens of micrometers in size. Phase transitions in P and Q regions have been elucidated by dielectric, dilatometric and micro-Raman studies. For the first time, the sequence of phase transitions between antiferroelectric phase P and ferroelectric Q and N phases has been revealed. Copyright © 2012 John Wiley & Sons, Ltd.\",\"language\":\"en\",\"number\":\"8\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Raman Spectroscopy\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shakhovoy\"],\"firstnames\":[\"R.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Raevskaya\"],\"firstnames\":[\"S.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shakhovaya\"],\"firstnames\":[\"L.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Suzdalev\"],\"firstnames\":[\"D.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Raevski\"],\"firstnames\":[\"I.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Semenchev\"],\"firstnames\":[\"A.\",\"F.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"year\":\"2012\",\"note\":\"_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/jrs.3140\",\"keywords\":\"phase transition, ferroelectric, antiferroelectric, micro-Raman spectroscopy, sodium niobate\",\"pages\":\"1141–1145\",\"file\":\"Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\W̋T6QGGA\\\\\\\\jrs.html:text/html\",\"bibtex\":\"@article{shakhovoy_ferroelectric_2012,\\n\\ttitle = {Ferroelectric {Q} and antiferroelectric {P} phases' coexistence and local phase transitions in oxygen-deficient {NaNb}$_{\\\\textrm{3}}$ single crystal: micro-{Raman}, dielectric and dilatometric studies},\\n\\tvolume = {43},\\n\\tcopyright = {Copyright © 2012 John Wiley \\\\& Sons, Ltd.},\\n\\tissn = {1097-4555},\\n\\tshorttitle = {Ferroelectric {Q} and antiferroelectric {P} phases' coexistence and local phase transitions in oxygen-deficient {NaNbO3} single crystal},\\n\\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/jrs.3140},\\n\\tdoi = {10.1002/jrs.3140},\\n\\tabstract = {Micro-Raman studies of oxygen-deficient gray-colored NaNbO3 single crystals have shown that at room temperature both antiferroelectric P and ferroelectric Q phases are present simultaneously as separate regions tens of micrometers in size. Phase transitions in P and Q regions have been elucidated by dielectric, dilatometric and micro-Raman studies. For the first time, the sequence of phase transitions between antiferroelectric phase P and ferroelectric Q and N phases has been revealed. Copyright © 2012 John Wiley \\\\& Sons, Ltd.},\\n\\tlanguage = {en},\\n\\tnumber = {8},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Raman Spectroscopy},\\n\\tauthor = {Shakhovoy, R. A. and Raevskaya, S. I. and Shakhovaya, L. A. and Suzdalev, D. V. and Raevski, I. P. and Yuzyuk, Yu. I. and Semenchev, A. F. and El Marssi, M.},\\n\\tyear = {2012},\\n\\tnote = {\\\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/jrs.3140},\\n\\tkeywords = {phase transition, ferroelectric, antiferroelectric, micro-Raman spectroscopy, sodium niobate},\\n\\tpages = {1141--1145},\\n\\tfile = {Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\HWT6QGGA\\\\\\\\jrs.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Shakhovoy, R. A.\",\"Raevskaya, S. I.\",\"Shakhovaya, L. A.\",\"Suzdalev, D. V.\",\"Raevski, I. P.\",\"Yuzyuk, Y. I.\",\"Semenchev, A. F.\",\"El Marssi, M.\"],\"key\":\"shakhovoy_ferroelectric_2012\",\"id\":\"shakhovoy_ferroelectric_2012\",\"bibbaseid\":\"shakhovoy-raevskaya-shakhovaya-suzdalev-raevski-yuzyuk-semenchev-elmarssi-ferroelectricqandantiferroelectricpphasescoexistenceandlocalphasetransitionsinoxygendeficientnanbtextrm3singlecrystalmicroramandielectricanddilatometricstudies-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/jrs.3140\"},\"keyword\":[\"phase transition\",\"ferroelectric\",\"antiferroelectric\",\"micro-Raman spectroscopy\",\"sodium niobate\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Усиление комбинационного рассеяния локализованными плазмонами в наночастицах серебра на поверхности наностержней оксида цинка\",\"volume\":\"82\",\"url\":\"http://journals.ioffe.ru/articles/10726\",\"abstract\":\"Исследованы особенности процесса магнетронного напыления наночастиц Ag на массивы наностержней ZnO. Боковые грани наностержней покрываются наночастицами с гораздо меньшей плотностью, нежели плоские поверхности при аналогичных временах напыления. Повышенная плотность частиц Ag наблюдается на ребрах боковых граней наностержней. Максимум плазмонного поглощения в синтезированных массивах наностержней, покрытых изолированными наночастицами Ag, лежит в диапазоне 450-500 nm. Возникновение локальных плазмонных возбуждений приводит к усилению интенсивности многофононных процессов с участием полярных мод ZnO в спектрах комбинационного рассеяния. С увеличением эквивалентной толщины пленок Ag возрастает сечение резонансного комбинационного рассеяния для обертонов фонона A1(LO).\",\"language\":\"ru\",\"number\":\"10\",\"urldate\":\"2023-11-11\",\"journal\":\"Журнал технической физики\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"В.\",\"Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2012\",\"pages\":\"85–89\",\"bibtex\":\"@article{__2012-13,\\n\\ttitle = {Усиление комбинационного рассеяния локализованными плазмонами в наночастицах серебра на поверхности наностержней оксида цинка},\\n\\tvolume = {82},\\n\\turl = {http://journals.ioffe.ru/articles/10726},\\n\\tabstract = {Исследованы особенности процесса магнетронного напыления наночастиц Ag на массивы наностержней ZnO. Боковые грани наностержней покрываются наночастицами с гораздо меньшей плотностью, нежели плоские поверхности при аналогичных временах напыления. Повышенная плотность частиц Ag наблюдается на ребрах боковых граней наностержней. Максимум плазмонного поглощения в синтезированных массивах наностержней, покрытых изолированными наночастицами Ag, лежит в диапазоне 450-500 nm. Возникновение локальных плазмонных возбуждений приводит к усилению интенсивности многофононных процессов с участием полярных мод ZnO в спектрах комбинационного рассеяния. С увеличением эквивалентной толщины пленок Ag возрастает сечение резонансного комбинационного рассеяния для обертонов фонона A1(LO).},\\n\\tlanguage = {ru},\\n\\tnumber = {10},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Журнал технической физики},\\n\\tauthor = {Кайдашев, В. Е. and Лянгузов, Н. В. and Юзюк, Ю. И. and Кайдашев, Е. М.},\\n\\tmonth = sep,\\n\\tyear = {2012},\\n\\tpages = {85--89},\\n}\\n\\n\",\"author_short\":[\"Кайдашев, В. Е.\",\"Лянгузов, Н. В.\",\"Юзюк, Ю. И.\",\"Кайдашев, Е. М.\"],\"key\":\"__2012-13\",\"id\":\"__2012-13\",\"bibbaseid\":\"-----2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/10726\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Оптические свойства эпитаксиальных тонких пленок Ba$_{\\\\textrm{0.8}}$Sr$_{\\\\textrm{0.2}}$TiO$_{\\\\textrm{3}}$\",\"volume\":\"82\",\"url\":\"http://journals.ioffe.ru/articles/10654\",\"abstract\":\"Исследованы свойства наноразмерных пленок (Ba0.8,Sr0.2)TiO3 на монокристаллических подложках окиси магния. Пленки изготовлены по методу высокочастотного распыления при осаждении по слоевому механизму роста. Измерения параметров решетки выполнены с помощью методов рентгеновской дифракции. Пропускание пленок различной толщины исследовано в диапазоне длин волн 190-1100 nm. При анализе экспериментальных оптических характеристик для определения коэффициента преломления и поглощения в дисперсионной формуле использованы дополнительные, релаксационные слагаемые, отражающие конечное время жизни осциллятора, что позволило более точно провести аппроксимацию экспериментальных данных.\",\"language\":\"ru\",\"number\":\"7\",\"urldate\":\"2023-11-11\",\"journal\":\"Журнал технической физики\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2012\",\"pages\":\"79–84\",\"file\":\"Журнал технической физики:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\8NHTT9Q2\\\\\\\\10654.html:text/html\",\"bibtex\":\"@article{__2012-14,\\n\\ttitle = {Оптические свойства эпитаксиальных тонких пленок {Ba}$_{\\\\textrm{0.8}}${Sr}$_{\\\\textrm{0.2}}${TiO}$_{\\\\textrm{3}}$},\\n\\tvolume = {82},\\n\\turl = {http://journals.ioffe.ru/articles/10654},\\n\\tabstract = {Исследованы свойства наноразмерных пленок (Ba0.8,Sr0.2)TiO3 на монокристаллических подложках окиси магния. Пленки изготовлены по методу высокочастотного распыления при осаждении по слоевому механизму роста. Измерения параметров решетки выполнены с помощью методов рентгеновской дифракции. Пропускание пленок различной толщины исследовано в диапазоне длин волн 190-1100 nm. При анализе экспериментальных оптических характеристик для определения коэффициента преломления и поглощения в дисперсионной формуле использованы дополнительные, релаксационные слагаемые, отражающие конечное время жизни осциллятора, что позволило более точно провести аппроксимацию экспериментальных данных.},\\n\\tlanguage = {ru},\\n\\tnumber = {7},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Журнал технической физики},\\n\\tauthor = {Широков, В. Б. and Головко, Ю. И. and Мухортов, В. М.},\\n\\tmonth = jun,\\n\\tyear = {2012},\\n\\tpages = {79--84},\\n\\tfile = {Журнал технической физики:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\8NHTT9Q2\\\\\\\\10654.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Широков, В. Б.\",\"Головко, Ю. И.\",\"Мухортов, В. М.\"],\"key\":\"__2012-14\",\"id\":\"__2012-14\",\"bibbaseid\":\"---batextrm08srtextrm02tiotextrm3-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/10654\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Использование различных катализаторов роста для лазерного напыления микро- и наностержней ZnO\",\"volume\":\"82\",\"url\":\"http://journals.ioffe.ru/articles/10579\",\"abstract\":\"С помощью метода импульсного лазерного напыления получены микро- и наностержни ZnO с использованием различных катализаторов роста при температурах, близких к оптимальным для каждого типа катализатора. Сравнительный анализ оптических и структурных свойств полученных образцов показал, что при снижении температуры роста при использовании подложек Al2O3 (11-20) уменьшаются внутренние напряжения в стержнях, что приводит к улучшению структуры и оптических свойств. При использовании подложек GaN/Si такой эффект не наблюдается из-за сильных напряжений, вносимых разностью параметров решеток. При повышении температуры синтеза увеличиваются внутренние напряжения и концентрация точечных дефектов решетки, происходит релаксация правил отбора, и наблюдаются множественные обертоны фонона A1(LO). Получено качественное соответствие результатов расчетов деформаций кристаллической решетки, произведенных по параметру a элементарной ячейки и по сдвигу частоты фонона A1(LO). Исследование фотолюминесценции образцов показало, что снижение температуры синтеза уменьшает дефектность стержней ZnO и позволяет улучшить их оптические свойства для УФ-приложений.\",\"language\":\"ru\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Журнал технической физики\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"В.\",\"Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Захарченко\"],\"firstnames\":[\"И.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Куприна\"],\"firstnames\":[\"Ю.А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бунина\"],\"firstnames\":[\"О.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Киселев\"],\"firstnames\":[\"А.\",\"П.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2012\",\"pages\":\"108–116\",\"bibtex\":\"@article{__2012-15,\\n\\ttitle = {Использование различных катализаторов роста для лазерного напыления микро- и наностержней {ZnO}},\\n\\tvolume = {82},\\n\\turl = {http://journals.ioffe.ru/articles/10579},\\n\\tabstract = {С помощью метода импульсного лазерного напыления получены микро- и наностержни ZnO с использованием различных катализаторов роста при температурах, близких к оптимальным для каждого типа катализатора. Сравнительный анализ оптических и структурных свойств полученных образцов показал, что при снижении температуры роста при использовании подложек Al2O3 (11-20) уменьшаются внутренние напряжения в стержнях, что приводит к улучшению структуры и оптических свойств. При использовании подложек GaN/Si такой эффект не наблюдается из-за сильных напряжений, вносимых разностью параметров решеток. При повышении температуры синтеза увеличиваются внутренние напряжения и концентрация точечных дефектов решетки, происходит релаксация правил отбора, и наблюдаются множественные обертоны фонона A1(LO). Получено качественное соответствие результатов расчетов деформаций кристаллической решетки, произведенных по параметру a элементарной ячейки и по сдвигу частоты фонона A1(LO). Исследование фотолюминесценции образцов показало, что снижение температуры синтеза уменьшает дефектность стержней ZnO и позволяет улучшить их оптические свойства для УФ-приложений.},\\n\\tlanguage = {ru},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Журнал технической физики},\\n\\tauthor = {Лянгузов, Н. В. and Кайдашев, В. Е. and Захарченко, И. Н. and Куприна, Ю.А. and Бунина, О. А. and Юзюк, Ю. И. and Киселев, А. П. and Кайдашев, Е. М.},\\n\\tmonth = mar,\\n\\tyear = {2012},\\n\\tpages = {108--116},\\n}\\n\\n\",\"author_short\":[\"Лянгузов, Н. В.\",\"Кайдашев, В. Е.\",\"Захарченко, И. Н.\",\"Куприна, Ю.\",\"Бунина, О. А.\",\"Юзюк, Ю. И.\",\"Киселев, А. П.\",\"Кайдашев, Е. М.\"],\"key\":\"__2012-15\",\"id\":\"__2012-15\",\"bibbaseid\":\"--------zno-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/10579\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"A comparative Raman study of 0.65(PbMg$_{\\\\textrm{1/3}}$Nb$_{\\\\textrm{2/3}}$O$_{\\\\textrm{3}}$) -0.35(PbTiO$_{\\\\textrm{3}}$) single crystal and thin film\",\"volume\":\"85\",\"issn\":\"1434-6036\",\"url\":\"https://doi.org/10.1140/epjb/e2011-20484-3\",\"doi\":\"10.1140/epjb/e2011-20484-3\",\"abstract\":\"We report a comparative Raman study of 0.65(PbMg1/3Nb2/3O3)-0.35(PbTiO3) (PMN-0.35PT) single crystal and thin film. Raman spectra investigation indicates a change in bulk from the high temperature cubic to the tetragonal phase and then to the low temperature Mc monoclinic phase. The transition temperatures are in good agreement with the ones previously observed by dielectric measurements on the same sample. In contrast, we observe no phase transition to the monoclinic phase in the PMN-0.35PT 4000 Å thick film and only a cubic to tetragonal diffuse transition has been determined at high temperature. The enhanced stability of the tetragonal phase and the absence of low temperature monoclinic phase have been attributed to the in plane strain.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"The European Physical Journal B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Bouyanfif\"],\"firstnames\":[\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lemée\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Le\",\"Marrec\"],\"firstnames\":[\"F.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Karkut\"],\"firstnames\":[\"M.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dkhil\"],\"firstnames\":[\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2012\",\"keywords\":\"Solid State and Materials\",\"pages\":\"35\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\ZDGC57TN\\\\\\\\Bouyanfif и др. - 2012 - A comparative Raman study of 0.65(PbMg13Nb23O3) .pdf:application/pdf\",\"bibtex\":\"@article{bouyanfif_comparative_2012,\\n\\ttitle = {A comparative {Raman} study of 0.65({PbMg}$_{\\\\textrm{1/3}}${Nb}$_{\\\\textrm{2/3}}${O}$_{\\\\textrm{3}}$) -0.35({PbTiO}$_{\\\\textrm{3}}$) single crystal and thin film},\\n\\tvolume = {85},\\n\\tissn = {1434-6036},\\n\\turl = {https://doi.org/10.1140/epjb/e2011-20484-3},\\n\\tdoi = {10.1140/epjb/e2011-20484-3},\\n\\tabstract = {We report a comparative Raman study of 0.65(PbMg1/3Nb2/3O3)-0.35(PbTiO3) (PMN-0.35PT) single crystal and thin film. Raman spectra investigation indicates a change in bulk from the high temperature cubic to the tetragonal phase and then to the low temperature Mc monoclinic phase. The transition temperatures are in good agreement with the ones previously observed by dielectric measurements on the same sample. In contrast, we observe no phase transition to the monoclinic phase in the PMN-0.35PT 4000 Å thick film and only a cubic to tetragonal diffuse transition has been determined at high temperature. The enhanced stability of the tetragonal phase and the absence of low temperature monoclinic phase have been attributed to the in plane strain.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {The European Physical Journal B},\\n\\tauthor = {Bouyanfif, H. and El Marssi, M. and Lemée, N. and Le Marrec, F. and Karkut, M. G. and Dkhil, B. and Yuzyuk, Yu. I.},\\n\\tmonth = jan,\\n\\tyear = {2012},\\n\\tkeywords = {Solid State and Materials},\\n\\tpages = {35},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\ZDGC57TN\\\\\\\\Bouyanfif и др. - 2012 - A comparative Raman study of 0.65(PbMg13Nb23O3) .pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Bouyanfif, H.\",\"El Marssi, M.\",\"Lemée, N.\",\"Le Marrec, F.\",\"Karkut, M. G.\",\"Dkhil, B.\",\"Yuzyuk, Y. I.\"],\"key\":\"bouyanfif_comparative_2012\",\"id\":\"bouyanfif_comparative_2012\",\"bibbaseid\":\"bouyanfif-elmarssi-leme-lemarrec-karkut-dkhil-yuzyuk-acomparativeramanstudyof065pbmgtextrm13nbtextrm23otextrm3035pbtiotextrm3singlecrystalandthinfilm-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1140/epjb/e2011-20484-3\"},\"keyword\":[\"Solid State and Materials\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Структурные изменения в жидкотвердых сплавах Bi + 44% Cd и Bi + 43% Sn под действием постоянного электрического тока\",\"volume\":\"76\",\"issn\":\"0367-6765\",\"url\":\"https://elibrary.ru/item.asp?id=17845707\",\"abstract\":\"Исследовано влияние постоянного электрического тока на параметры ячеек компонентов в жидкотвердых сплавах Bi + 44% Cd и Bi + 43% Sn. Обнаружено изменение параметров ячеек, связанное со структурными эффектами.\",\"language\":\"ru\",\"number\":\"7\",\"urldate\":\"2023-11-11\",\"journal\":\"Известия Российской Академии Наук. Серия Физическая\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Афашоков\"],\"firstnames\":[\"В.\",\"З.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ахкубеков\"],\"firstnames\":[\"А.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кабиров\"],\"firstnames\":[\"Ю.\",\"В.\"],\"suffixes\":[]}],\"year\":\"2012\",\"pages\":\"851\",\"bibtex\":\"@article{__2012-16,\\n\\ttitle = {Структурные изменения в жидкотвердых сплавах {Bi} + 44\\\\% {Cd} и {Bi} + 43\\\\% {Sn} под действием постоянного электрического тока},\\n\\tvolume = {76},\\n\\tissn = {0367-6765},\\n\\turl = {https://elibrary.ru/item.asp?id=17845707},\\n\\tabstract = {Исследовано влияние постоянного электрического тока на параметры ячеек компонентов в жидкотвердых сплавах Bi + 44\\\\% Cd и Bi + 43\\\\% Sn. Обнаружено изменение параметров ячеек, связанное со структурными эффектами.},\\n\\tlanguage = {ru},\\n\\tnumber = {7},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Известия Российской Академии Наук. Серия Физическая},\\n\\tauthor = {Афашоков, В. З. and Ахкубеков, А. А. and Кабиров, Ю. В.},\\n\\tyear = {2012},\\n\\tpages = {851},\\n}\\n\\n\",\"author_short\":[\"Афашоков, В. З.\",\"Ахкубеков, А. А.\",\"Кабиров, Ю. В.\"],\"key\":\"__2012-16\",\"id\":\"__2012-16\",\"bibbaseid\":\"---bi44cdbi43sn-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=17845707\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Динамика решетки эпитаксиальной пленки титаната бария-стронция во внешнем электрическом поле\",\"volume\":\"8\",\"issn\":\"1813-4289\",\"url\":\"https://elibrary.ru/item.asp?id=18062877\",\"abstract\":\"Исследована динамика решетки тонкой гетероэпитаксиальной пленки (Ba0,8Sr0,2)TiO3 на кубиче- ской подложке MgO во внешнем электрическом поле. Приведено как феноменологическое описание поведения мягких мод на основе теории Ландау, так и подробный анализ данных комбинационного рассеяния света. Расщепление мягкой моды на компоненты и их частотная зависимость свидетель- ствуют о переходе в моноклинную фазу при приложении внешнего электрического поля в направле- нии, перпендикулярном спонтанной поляризации c-доменной пленки.\",\"language\":\"ru\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Вестник Южного Научного Центра Ран\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Анохин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]}],\"year\":\"2012\",\"keywords\":\"Мягкая Мода, Сегнетоэлектрические Тонкие Пленки, Сегнетоэлектричество, Спектры Комбинационного Рассеяния Света\",\"pages\":\"22–31\",\"bibtex\":\"@article{__2012-17,\\n\\ttitle = {Динамика решетки эпитаксиальной пленки титаната бария-стронция во внешнем электрическом поле},\\n\\tvolume = {8},\\n\\tissn = {1813-4289},\\n\\turl = {https://elibrary.ru/item.asp?id=18062877},\\n\\tabstract = {Исследована динамика решетки тонкой гетероэпитаксиальной пленки (Ba0,8Sr0,2)TiO3 на кубиче- ской подложке MgO во внешнем электрическом поле. Приведено как феноменологическое описание поведения мягких мод на основе теории Ландау, так и подробный анализ данных комбинационного рассеяния света. Расщепление мягкой моды на компоненты и их частотная зависимость свидетель- ствуют о переходе в моноклинную фазу при приложении внешнего электрического поля в направле- нии, перпендикулярном спонтанной поляризации c-доменной пленки.},\\n\\tlanguage = {ru},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Вестник Южного Научного Центра Ран},\\n\\tauthor = {Анохин, А. С. and Головко, Ю. И. and Широков, В. Б. and Мухортов, В. М. and Юзюк, Ю. И.},\\n\\tyear = {2012},\\n\\tkeywords = {Мягкая Мода, Сегнетоэлектрические Тонкие Пленки, Сегнетоэлектричество, Спектры Комбинационного Рассеяния Света},\\n\\tpages = {22--31},\\n}\\n\\n\",\"author_short\":[\"Анохин, А. С.\",\"Головко, Ю. И.\",\"Широков, В. Б.\",\"Мухортов, В. М.\",\"Юзюк, Ю. И.\"],\"key\":\"__2012-17\",\"id\":\"__2012-17\",\"bibbaseid\":\"------2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=18062877\"},\"keyword\":[\"Мягкая Мода\",\"Сегнетоэлектрические Тонкие Пленки\",\"Сегнетоэлектричество\",\"Спектры Комбинационного Рассеяния Света\"],\"metadata\":{\"authorlinks\":{}},\"downloads\":1,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"B-T phase diagram of CoCr$_{\\\\textrm{2}}$O$_{\\\\textrm{4}}$ in magnetic fields up to 14 T\",\"volume\":\"85\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.85.012101\",\"doi\":\"10.1103/PhysRevB.85.012101\",\"abstract\":\"We have measured the magnetization and specific heat of multiferroic CoCr2O4 in magnetic fields up to 14 T. The high-field magnetization measurements indicate a new phase transition at T∗=5–6 K. The phase between T∗ and the lock-in transition at 15 K is characterized by magnetic irreversibility. At higher magnetic fields, the irreversibility increases. Specific-heat measurements confirm the transition at T∗, and also show irreversible behavior. We construct a field-temperature phase diagram of CoCr2O4.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Pronin\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Uhlarz\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Beyer\"],\"firstnames\":[\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fischer\"],\"firstnames\":[\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Wosnitza\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"B.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Komandin\"],\"firstnames\":[\"G.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bush\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2012\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"012101\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\AZP2XD73\\\\¶ronin и др. - 2012 - $B$-$T$ phase diagram of CoCr$ _ 2 $O$ _ 4 $ in .pdf:application/pdf\",\"bibtex\":\"@article{pronin_b-t_2012,\\n\\ttitle = {B-{T} phase diagram of {CoCr}$_{\\\\textrm{2}}${O}$_{\\\\textrm{4}}$ in magnetic fields up to 14 {T}},\\n\\tvolume = {85},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.85.012101},\\n\\tdoi = {10.1103/PhysRevB.85.012101},\\n\\tabstract = {We have measured the magnetization and specific heat of multiferroic CoCr2O4 in magnetic fields up to 14 T. The high-field magnetization measurements indicate a new phase transition at T∗=5–6 K. The phase between T∗ and the lock-in transition at 15 K is characterized by magnetic irreversibility. At higher magnetic fields, the irreversibility increases. Specific-heat measurements confirm the transition at T∗, and also show irreversible behavior. We construct a field-temperature phase diagram of CoCr2O4.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Pronin, A. V. and Uhlarz, M. and Beyer, R. and Fischer, T. and Wosnitza, J. and Gorshunov, B. P. and Komandin, G. A. and Prokhorov, A. S. and Dressel, M. and Bush, A. A. and Torgashev, V. I.},\\n\\tmonth = jan,\\n\\tyear = {2012},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {012101},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\AZP2XD73\\\\\\\\Pronin и др. - 2012 - \\\\$B\\\\$-\\\\$T\\\\$ phase diagram of CoCr\\\\$ _ 2 \\\\$O\\\\$ _ 4 \\\\$ in .pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Pronin, A. V.\",\"Uhlarz, M.\",\"Beyer, R.\",\"Fischer, T.\",\"Wosnitza, J.\",\"Gorshunov, B. P.\",\"Komandin, G. A.\",\"Prokhorov, A. S.\",\"Dressel, M.\",\"Bush, A. A.\",\"Torgashev, V. I.\"],\"key\":\"pronin_b-t_2012\",\"id\":\"pronin_b-t_2012\",\"bibbaseid\":\"pronin-uhlarz-beyer-fischer-wosnitza-gorshunov-komandin-prokhorov-etal-btphasediagramofcocrtextrm2otextrm4inmagneticfieldsupto14t-2012\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.85.012101\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Effect of periodicity and composition in artificial BaTiO$_{\\\\textrm{3}}$/(Ba,Sr)TiO$_{\\\\textrm{3}}$ superlattices\",\"volume\":\"83\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.83.144108\",\"doi\":\"10.1103/PhysRevB.83.144108\",\"abstract\":\"We have prepared two series of BaTiO3/SrTiO3 (BT/ST) superlattices (SLs). In the first set, the modulation period (Λ) was varied from 136 to 16 Å, whereas in the second set ST was replaced with Ba(1−x)SrxTiO3 (BST) (0\\\\textlessx\\\\textless1) with constant periodicity of ∼ 136 Å. A total stack height of 10 000 Å (1 μm) was maintained for both systems. The compositional changes give large spectral changes at x = 40% where the lowest E mode in BT/BST SL becomes underdamped. X-ray-diffraction patterns and surface topography of the modulated period revealed a Stranski-Krastanov growth mechanism. The upward frequency shift of the E(1TO) in SLs with decrease in Λ or Ba concentration in the BST layer was attributed to the in-plane compressive stress induced by the lattice mismatch of the constituent layers. [N.B., here the notation E(1TO) or A1(2TO) simply designates the vibrational mode of E or A1 symmetry, with 1TO or 2TO designating the transverse optical branch that is lowest, 1, or second lowest, 2, in energy.] In the low-frequency region, the folded acoustic phonon doublets were observed. Since the low-frequency out-of-plane dielectric constant is directly related to the E(1TO) soft mode frequency, strain engineering in artificial SLs allowed us to modify their dielectric properties by varying either the Ba/Sr in BST sublayer concentration or the modulation periodicity in the superlattices.\",\"number\":\"14\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Ortega\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kumar\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"O.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Scott\"],\"firstnames\":[\"J.\",\"F.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"R.\",\"S.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2011\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"144108\",\"file\":\"Принятая версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\56AU3DQI\\\\Ørtega и др. - 2011 - Effect of periodicity and composition in artificia.pdf:application/pdf\",\"bibtex\":\"@article{ortega_effect_2011,\\n\\ttitle = {Effect of periodicity and composition in artificial {BaTiO}$_{\\\\textrm{3}}$/({Ba},{Sr}){TiO}$_{\\\\textrm{3}}$ superlattices},\\n\\tvolume = {83},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.83.144108},\\n\\tdoi = {10.1103/PhysRevB.83.144108},\\n\\tabstract = {We have prepared two series of BaTiO3/SrTiO3 (BT/ST) superlattices (SLs). In the first set, the modulation period (Λ) was varied from 136 to 16 Å, whereas in the second set ST was replaced with Ba(1−x)SrxTiO3 (BST) (0{\\\\textless}x{\\\\textless}1) with constant periodicity of ∼ 136 Å. A total stack height of 10 000 Å (1 μm) was maintained for both systems. The compositional changes give large spectral changes at x = 40\\\\% where the lowest E mode in BT/BST SL becomes underdamped. X-ray-diffraction patterns and surface topography of the modulated period revealed a Stranski-Krastanov growth mechanism. The upward frequency shift of the E(1TO) in SLs with decrease in Λ or Ba concentration in the BST layer was attributed to the in-plane compressive stress induced by the lattice mismatch of the constituent layers. [N.B., here the notation E(1TO) or A1(2TO) simply designates the vibrational mode of E or A1 symmetry, with 1TO or 2TO designating the transverse optical branch that is lowest, 1, or second lowest, 2, in energy.] In the low-frequency region, the folded acoustic phonon doublets were observed. Since the low-frequency out-of-plane dielectric constant is directly related to the E(1TO) soft mode frequency, strain engineering in artificial SLs allowed us to modify their dielectric properties by varying either the Ba/Sr in BST sublayer concentration or the modulation periodicity in the superlattices.},\\n\\tnumber = {14},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Ortega, N. and Kumar, A. and Maslova, O. A. and Yuzyuk, Yu. I. and Scott, J. F. and Katiyar, R. S.},\\n\\tmonth = apr,\\n\\tyear = {2011},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {144108},\\n\\tfile = {Принятая версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\56AU3DQI\\\\\\\\Ortega и др. - 2011 - Effect of periodicity and composition in artificia.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Ortega, N.\",\"Kumar, A.\",\"Maslova, O. A.\",\"Yuzyuk, Y. I.\",\"Scott, J. F.\",\"Katiyar, R. S.\"],\"key\":\"ortega_effect_2011\",\"id\":\"ortega_effect_2011\",\"bibbaseid\":\"ortega-kumar-maslova-yuzyuk-scott-katiyar-effectofperiodicityandcompositioninartificialbatiotextrm3basrtiotextrm3superlattices-2011\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.83.144108\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Electric-field-induced monoclinic phase in (Ba,Sr)TiO$_{\\\\textrm{3}}$ thin film\",\"volume\":\"109\",\"issn\":\"0021-8979\",\"url\":\"https://doi.org/10.1063/1.3573516\",\"doi\":\"10.1063/1.3573516\",\"abstract\":\"We have studied electric-field-induced symmetry lowering in the tetragonal (001)-oriented heteroepitaxial (Ba0.8Sr0.2)TiO3 thin film deposited on (001)MgO substrate. Polarized micro-Raman spectra were recorded from the film area in between two planar electrodes deposited on the film surface. Presence of c domains with polarization normal to the substrate was confirmed from polarized Raman study under zero field, while splitting and hardening of the E(TO) soft mode and polarization changes in the Raman spectra suggest monoclinic symmetry under external electric field.\",\"number\":\"7\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Applied Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Anokhin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golovko\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mukhortov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2011\",\"pages\":\"074111\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\R9PF7M4M\\\\\\\\Anokhin и др. - 2011 - Electric-field-induced monoclinic phase in (Ba,Sr).pdf:application/pdf\",\"bibtex\":\"@article{anokhin_electric-field-induced_2011,\\n\\ttitle = {Electric-field-induced monoclinic phase in ({Ba},{Sr}){TiO}$_{\\\\textrm{3}}$ thin film},\\n\\tvolume = {109},\\n\\tissn = {0021-8979},\\n\\turl = {https://doi.org/10.1063/1.3573516},\\n\\tdoi = {10.1063/1.3573516},\\n\\tabstract = {We have studied electric-field-induced symmetry lowering in the tetragonal (001)-oriented heteroepitaxial (Ba0.8Sr0.2)TiO3 thin film deposited on (001)MgO substrate. Polarized micro-Raman spectra were recorded from the film area in between two planar electrodes deposited on the film surface. Presence of c domains with polarization normal to the substrate was confirmed from polarized Raman study under zero field, while splitting and hardening of the E(TO) soft mode and polarization changes in the Raman spectra suggest monoclinic symmetry under external electric field.},\\n\\tnumber = {7},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Applied Physics},\\n\\tauthor = {Anokhin, A. S. and Yuzyuk, Yu. I. and Golovko, Yu. I. and Mukhortov, V. M. and El Marssi, M.},\\n\\tmonth = apr,\\n\\tyear = {2011},\\n\\tpages = {074111},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\R9PF7M4M\\\\\\\\Anokhin и др. - 2011 - Electric-field-induced monoclinic phase in (Ba,Sr).pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Anokhin, A. S.\",\"Yuzyuk, Y. I.\",\"Golovko, Y. I.\",\"Mukhortov, V. M.\",\"El Marssi, M.\"],\"key\":\"anokhin_electric-field-induced_2011\",\"id\":\"anokhin_electric-field-induced_2011\",\"bibbaseid\":\"anokhin-yuzyuk-golovko-mukhortov-elmarssi-electricfieldinducedmonoclinicphaseinbasrtiotextrm3thinfilm-2011\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.3573516\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Orthorhombic polar Nd-doped BiFeO$_{\\\\textrm{3}}$ thin film on MgO substrate\",\"volume\":\"23\",\"issn\":\"0953-8984\",\"url\":\"https://dx.doi.org/10.1088/0953-8984/23/33/332201\",\"doi\":\"10.1088/0953-8984/23/33/332201\",\"abstract\":\"A Nd-doped BiFeO3 thin film deposited on MgO substrate was studied by synchrotron diffraction. The ferroelectric nature of the film is proven by in-plane remanent polarization measurement. The highest possible symmetry of the film is determined to be orthorhombic, within the Fm2m space group. Such a structure is rotated by 45° with respect to the substrate and is consistent with tilts of oxygen octahedra doubling the unit cell. This polar structure presents a rather unusual strain-accommodation mechanism.\",\"language\":\"en\",\"number\":\"33\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics: Condensed Matter\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Janolin\"],\"firstnames\":[\"P.-E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El-Marssi\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chernyshov\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dmitriev\"],\"firstnames\":[\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golovko\"],\"firstnames\":[\"Yu\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mukhortov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dkhil\"],\"firstnames\":[\"B.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2011\",\"pages\":\"332201\",\"bibtex\":\"@article{leontyev_orthorhombic_2011,\\n\\ttitle = {Orthorhombic polar {Nd}-doped {BiFeO}$_{\\\\textrm{3}}$ thin film on {MgO} substrate},\\n\\tvolume = {23},\\n\\tissn = {0953-8984},\\n\\turl = {https://dx.doi.org/10.1088/0953-8984/23/33/332201},\\n\\tdoi = {10.1088/0953-8984/23/33/332201},\\n\\tabstract = {A Nd-doped BiFeO3 thin film deposited on MgO substrate was studied by synchrotron diffraction. The ferroelectric nature of the film is proven by in-plane remanent polarization measurement. The highest possible symmetry of the film is determined to be orthorhombic, within the Fm2m space group. Such a structure is rotated by 45° with respect to the substrate and is consistent with tilts of oxygen octahedra doubling the unit cell. This polar structure presents a rather unusual strain-accommodation mechanism.},\\n\\tlanguage = {en},\\n\\tnumber = {33},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics: Condensed Matter},\\n\\tauthor = {Leontyev, I. N. and Yuzyuk, Yu I. and Janolin, P.-E. and El-Marssi, M. and Chernyshov, D. and Dmitriev, V. and Golovko, Yu I. and Mukhortov, V. M. and Dkhil, B.},\\n\\tmonth = jul,\\n\\tyear = {2011},\\n\\tpages = {332201},\\n}\\n\\n\",\"author_short\":[\"Leontyev, I. N.\",\"Yuzyuk, Y. I.\",\"Janolin, P.\",\"El-Marssi, M.\",\"Chernyshov, D.\",\"Dmitriev, V.\",\"Golovko, Y. I.\",\"Mukhortov, V. M.\",\"Dkhil, B.\"],\"key\":\"leontyev_orthorhombic_2011\",\"id\":\"leontyev_orthorhombic_2011\",\"bibbaseid\":\"leontyev-yuzyuk-janolin-elmarssi-chernyshov-dmitriev-golovko-mukhortov-etal-orthorhombicpolarnddopedbifeotextrm3thinfilmonmgosubstrate-2011\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/0953-8984/23/33/332201\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Особенности структурных состояний в твердых растворах BiFeO$_{\\\\textrm{3}}$-YMnO$_{\\\\textrm{3}}$\",\"volume\":\"53\",\"url\":\"http://journals.ioffe.ru/articles/1518\",\"abstract\":\"Обнаружено, что в твердых растворах (1-x)BiFeO3-xYMnO3 наблюдается следующая последовательность изменений фаз с увеличением x: R3c-\\\\textgreater Pbnm-\\\\textgreater C2-\\\\textgreater Pnma-\\\\textgreater P63cm. Установлено, что фазы Pbnm и Pnma различаются ориентацией атомных смещений и могут иметь антисегнетоэлектрические свойства. Работа поддержана грантом РФФИ N 10-03-00189-a. А.Г. Разумная благодарит Фонд содействия развитию малых форм предприятий в научно-технической сфере по программе У.М.Н.И.К. N 10170.\",\"language\":\"ru\",\"number\":\"8\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Назаренко\"],\"firstnames\":[\"А.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Разумная\"],\"firstnames\":[\"А.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Куприянов\"],\"firstnames\":[\"М.\",\"Ф.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кабиров\"],\"firstnames\":[\"Ю.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Рудская\"],\"firstnames\":[\"А.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Тесленко\"],\"firstnames\":[\"П.\",\"Ю.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кофанова\"],\"firstnames\":[\"Н.\",\"Б.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2011\",\"pages\":\"1523–1525\",\"bibtex\":\"@article{__2011-3,\\n\\ttitle = {Особенности структурных состояний в твердых растворах {BiFeO}$_{\\\\textrm{3}}$-{YMnO}$_{\\\\textrm{3}}$},\\n\\tvolume = {53},\\n\\turl = {http://journals.ioffe.ru/articles/1518},\\n\\tabstract = {Обнаружено, что в твердых растворах (1-x)BiFeO3-xYMnO3 наблюдается следующая последовательность изменений фаз с увеличением x: R3c-{\\\\textgreater} Pbnm-{\\\\textgreater} C2-{\\\\textgreater} Pnma-{\\\\textgreater} P63cm. Установлено, что фазы Pbnm и Pnma различаются ориентацией атомных смещений и могут иметь антисегнетоэлектрические свойства. Работа поддержана грантом РФФИ N 10-03-00189-a. А.Г. Разумная благодарит Фонд содействия развитию малых форм предприятий в научно-технической сфере по программе У.М.Н.И.К. N 10170.},\\n\\tlanguage = {ru},\\n\\tnumber = {8},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Назаренко, А. В. and Разумная, А. Г. and Куприянов, М. Ф. and Кабиров, Ю. В. and Рудская, А. Г. and Тесленко, П. Ю. and Кофанова, Н. Б.},\\n\\tmonth = jul,\\n\\tyear = {2011},\\n\\tpages = {1523--1525},\\n}\\n\\n\",\"author_short\":[\"Назаренко, А. В.\",\"Разумная, А. Г.\",\"Куприянов, М. Ф.\",\"Кабиров, Ю. В.\",\"Рудская, А. Г.\",\"Тесленко, П. Ю.\",\"Кофанова, Н. Б.\"],\"key\":\"__2011-3\",\"id\":\"__2011-3\",\"bibbaseid\":\"-------bifeotextrm3ymnotextrm3-2011\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/1518\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Структура и фазовые переходы твердых растворов цирконата-гафната свинца\",\"volume\":\"53\",\"url\":\"http://journals.ioffe.ru/articles/1291\",\"abstract\":\"Методом твердофазного синтеза из простых оксидов приготовлены твердые растворы двух антисегнетоэлектриков - цирконата и гафната свинца PbZr1-xHfxO3, x=0, 0.3, 0.5, 0.7, 1. Элементный состав образцов и их структура изучены методами рентгенофлуоресцентного анализа и рентгеновской дифракции. Определены фазовые изменения твердых растворов в области температур 20\\\\textlesst\\\\textless300oC. Работа поддержана грантом РФФИ N 10-03-00189-a.\",\"language\":\"ru\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Кабиров\"],\"firstnames\":[\"Ю.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Куприянов\"],\"firstnames\":[\"М.\",\"Ф.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Петрович\"],\"firstnames\":[\"Э.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Дуймакаев\"],\"firstnames\":[\"Ш.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Пономоренко\"],\"firstnames\":[\"В.\",\"О.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2010\",\"pages\":\"110–113\",\"bibtex\":\"@article{__2010-1,\\n\\ttitle = {Структура и фазовые переходы твердых растворов цирконата-гафната свинца},\\n\\tvolume = {53},\\n\\turl = {http://journals.ioffe.ru/articles/1291},\\n\\tabstract = {Методом твердофазного синтеза из простых оксидов приготовлены твердые растворы двух антисегнетоэлектриков - цирконата и гафната свинца PbZr1-xHfxO3, x=0, 0.3, 0.5, 0.7, 1. Элементный состав образцов и их структура изучены методами рентгенофлуоресцентного анализа и рентгеновской дифракции. Определены фазовые изменения твердых растворов в области температур 20{\\\\textless}t{\\\\textless}300oC. Работа поддержана грантом РФФИ N 10-03-00189-a.},\\n\\tlanguage = {ru},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Кабиров, Ю. В. and Куприянов, М. Ф. and Петрович, Э. В. and Дуймакаев, Ш. И. and Пономоренко, В. О.},\\n\\tmonth = dec,\\n\\tyear = {2010},\\n\\tpages = {110--113},\\n}\\n\\n\",\"author_short\":[\"Кабиров, Ю. В.\",\"Куприянов, М. Ф.\",\"Петрович, Э. В.\",\"Дуймакаев, Ш. И.\",\"Пономоренко, В. О.\"],\"key\":\"__2010-1\",\"id\":\"__2010-1\",\"bibbaseid\":\"------2010\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/1291\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Спектры комбинационного рассеяния поликристаллических нанотрубок титаната висмута\",\"volume\":\"53\",\"url\":\"http://journals.ioffe.ru/articles/1557\",\"abstract\":\"Исследованы спектры комбинационного рассеяния света нанотрубок титаната висмута Bi4Ti3O12 синтезированных темплатным методом на мембранах Al2O3. Полученные образцы представляли собой массив ориентированных нанотрубок со сросшимися гладкими стенками длиной около 50 mum. Толщина стенок нанотрубок варьировалась от 20 до 50 nm, а внутренний диаметр составлял около 200 nm. В спектрах комбинационного рассеяния света нанотрубок наблюдалось уширение линий, соответствующих валентным и деформационным колебаниям TiO6 октаэдров, а в низкочастотной области спектра, соответствующей колебаниям ионов Bi относительно кислородных октаэдров, наблюдалась трансформация, обусловленная сильными механическими напряжениями, возникающими при формировании нанотрубок.\",\"language\":\"ru\",\"number\":\"9\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Анохин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Рошаль\"],\"firstnames\":[\"С.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Wang\"],\"firstnames\":[\"Wen\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2011\",\"pages\":\"1768–1772\",\"bibtex\":\"@article{__2011-4,\\n\\ttitle = {Спектры комбинационного рассеяния поликристаллических нанотрубок титаната висмута},\\n\\tvolume = {53},\\n\\turl = {http://journals.ioffe.ru/articles/1557},\\n\\tabstract = {Исследованы спектры комбинационного рассеяния света нанотрубок титаната висмута Bi4Ti3O12 синтезированных темплатным методом на мембранах Al2O3. Полученные образцы представляли собой массив ориентированных нанотрубок со сросшимися гладкими стенками длиной около 50 mum. Толщина стенок нанотрубок варьировалась от 20 до 50 nm, а внутренний диаметр составлял около 200 nm. В спектрах комбинационного рассеяния света нанотрубок наблюдалось уширение линий, соответствующих валентным и деформационным колебаниям TiO6 октаэдров, а в низкочастотной области спектра, соответствующей колебаниям ионов Bi относительно кислородных октаэдров, наблюдалась трансформация, обусловленная сильными механическими напряжениями, возникающими при формировании нанотрубок.},\\n\\tlanguage = {ru},\\n\\tnumber = {9},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Анохин, А. С. and Лянгузов, Н. В. and Рошаль, С. Б. and Юзюк, Ю. И. and Wang, Wen},\\n\\tmonth = sep,\\n\\tyear = {2011},\\n\\tpages = {1768--1772},\\n}\\n\\n\",\"author_short\":[\"Анохин, А. С.\",\"Лянгузов, Н. В.\",\"Рошаль, С. Б.\",\"Юзюк, Ю. И.\",\"Wang, W.\"],\"key\":\"__2011-4\",\"id\":\"__2011-4\",\"bibbaseid\":\"----wang--2011\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/1557\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Формирование физических свойств релаксорного сегнетоэлектрика Pb$_{\\\\textrm{2}}$ScNbO$_{\\\\textrm{6}}$ методом механоактивации\",\"volume\":\"37\",\"url\":\"http://journals.ioffe.ru/articles/14334\",\"abstract\":\"Изучен релаксорный сегнетоэлектрик Pb2ScNbO6 (PSN), полученный твердофазным методом, спеканию которого предшествовала обработка при комнатной температуре синтезированного порошка PSN в наковальнях Бриджмена силовым воздействием в сочетании со сдвиговой деформацией. Показано, что при интенсивных силовых воздействиях в сочетании со сдвиговой деформацией в PSN развиваются динамические рекристаллизационные процессы, вносящие существенный вклад в формирование физических свойств керамики.\",\"language\":\"ru\",\"number\":\"20\",\"urldate\":\"2023-11-11\",\"journal\":\"Письма в ЖТФ\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Убушаева\"],\"firstnames\":[\"Э.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лихушина\"],\"firstnames\":[\"Е.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Абдулвахидов\"],\"firstnames\":[\"К.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Витченко\"],\"firstnames\":[\"М.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Абулвахидов\"],\"firstnames\":[\"Б.\",\"К.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мардасова\"],\"firstnames\":[\"И.\",\"В.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2011\",\"pages\":\"23–30\",\"bibtex\":\"@article{__2011-5,\\n\\ttitle = {Формирование физических свойств релаксорного сегнетоэлектрика {Pb}$_{\\\\textrm{2}}${ScNbO}$_{\\\\textrm{6}}$ методом механоактивации},\\n\\tvolume = {37},\\n\\turl = {http://journals.ioffe.ru/articles/14334},\\n\\tabstract = {Изучен релаксорный сегнетоэлектрик Pb2ScNbO6 (PSN), полученный твердофазным методом, спеканию которого предшествовала обработка при комнатной температуре синтезированного порошка PSN в наковальнях Бриджмена силовым воздействием в сочетании со сдвиговой деформацией. Показано, что при интенсивных силовых воздействиях в сочетании со сдвиговой деформацией в PSN развиваются динамические рекристаллизационные процессы, вносящие существенный вклад в формирование физических свойств керамики.},\\n\\tlanguage = {ru},\\n\\tnumber = {20},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Письма в ЖТФ},\\n\\tauthor = {Убушаева, Э. Н. and Лихушина, Е. В. and Абдулвахидов, К. Г. and Витченко, М. А. and Абулвахидов, Б. К. and Широков, В. Б. and Лянгузов, Н. В. and Юзюк, Ю. И. and Кайдашев, Е. М. and Мардасова, И. В.},\\n\\tmonth = sep,\\n\\tyear = {2011},\\n\\tpages = {23--30},\\n}\\n\\n\",\"author_short\":[\"Убушаева, Э. Н.\",\"Лихушина, Е. В.\",\"Абдулвахидов, К. Г.\",\"Витченко, М. А.\",\"Абулвахидов, Б. К.\",\"Широков, В. Б.\",\"Лянгузов, Н. В.\",\"Юзюк, Ю. И.\",\"Кайдашев, Е. М.\",\"Мардасова, И. В.\"],\"key\":\"__2011-5\",\"id\":\"__2011-5\",\"bibbaseid\":\"--------etal-pbtextrm2scnbotextrm6-2011\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/14334\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Исследование влияния толщины медного катализатора и пленочного подслоя на морфологию наностержней ZnO\",\"volume\":\"37\",\"url\":\"http://journals.ioffe.ru/articles/12488\",\"abstract\":\"Исследовано влияние толщины пленочного подслоя ZnO, а также толщины пленок катализатора роста (Cu) на морфологию наностержней ZnO, выращенных на подложках a-Al2O3(11-20) карботермическим методом. Увеличение толщины пленки Cu приводит к увеличению диаметров, высоты и поверхностной плотности наностержней. Увеличение толщины пленочного подслоя ZnO приводит к возрастанию среднего диаметра и уменьшению длины и поверхностной плотности наностержней. Проведены исследования по влиянию температуры на процесс термического развала сверхтонких пленок меди, нанесенынх на подложки a-Al2O3. Исследованы фотолюминесцентные свойства массивов наностержней при высоких уровнях оптической накачки. Повышение плотности мощности накачки до 250-280 kW/cm2 приводит к сверхлюминесценции наностержней.\",\"language\":\"ru\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Письма в ЖТФ\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"В.\",\"Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Абдулвахидов\"],\"firstnames\":[\"К.\",\"Г.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2011\",\"pages\":\"1–8\",\"bibtex\":\"@article{__2011-6,\\n\\ttitle = {Исследование влияния толщины медного катализатора и пленочного подслоя на морфологию наностержней {ZnO}},\\n\\tvolume = {37},\\n\\turl = {http://journals.ioffe.ru/articles/12488},\\n\\tabstract = {Исследовано влияние толщины пленочного подслоя ZnO, а также толщины пленок катализатора роста (Cu) на морфологию наностержней ZnO, выращенных на подложках a-Al2O3(11-20) карботермическим методом. Увеличение толщины пленки Cu приводит к увеличению диаметров, высоты и поверхностной плотности наностержней. Увеличение толщины пленочного подслоя ZnO приводит к возрастанию среднего диаметра и уменьшению длины и поверхностной плотности наностержней. Проведены исследования по влиянию температуры на процесс термического развала сверхтонких пленок меди, нанесенынх на подложки a-Al2O3. Исследованы фотолюминесцентные свойства массивов наностержней при высоких уровнях оптической накачки. Повышение плотности мощности накачки до 250-280 kW/cm2 приводит к сверхлюминесценции наностержней.},\\n\\tlanguage = {ru},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Письма в ЖТФ},\\n\\tauthor = {Лянгузов, Н. В. and Кайдашев, В. Е. and Кайдашев, Е. М. and Абдулвахидов, К. Г.},\\n\\tmonth = feb,\\n\\tyear = {2011},\\n\\tpages = {1--8},\\n}\\n\\n\",\"author_short\":[\"Лянгузов, Н. В.\",\"Кайдашев, В. Е.\",\"Кайдашев, Е. М.\",\"Абдулвахидов, К. Г.\"],\"key\":\"__2011-6\",\"id\":\"__2011-6\",\"bibbaseid\":\"----zno-2011\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/12488\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Поверхностные акустические волны в тонких пленках титаната бария-стронция на подложках из оксида магния\",\"volume\":\"37\",\"url\":\"http://journals.ioffe.ru/articles/12492\",\"abstract\":\"Установлено, что при использовании в устройстве на поверхностных акустических волнах в качестве активного элемента тонкой пленки титаната бария-стронция на подложке из оксида магния можно вдвое повысить рабочую частоту преобразователя за счет формирования в пленке периодической доменной структуры. Показано, что в тонкой сегнетоэлектрической пленке при стандартной структуре электродов эффективно возбуждается вторая гармоника поверхностной акустической волны. Путем изменения внешнего поляризующего напряжения на электродах пленки можно создавать преобразователи с электрически регулируемым коэффициентом электромеханической связи.\",\"language\":\"ru\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Письма в ЖТФ\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бирюков\"],\"firstnames\":[\"С.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Карапетьян\"],\"firstnames\":[\"Г.\",\"Я.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Масычев\"],\"firstnames\":[\"С.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.М.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2011\",\"pages\":\"31–37\",\"bibtex\":\"@article{__2011-7,\\n\\ttitle = {Поверхностные акустические волны в тонких пленках титаната бария-стронция на подложках из оксида магния},\\n\\tvolume = {37},\\n\\turl = {http://journals.ioffe.ru/articles/12492},\\n\\tabstract = {Установлено, что при использовании в устройстве на поверхностных акустических волнах в качестве активного элемента тонкой пленки титаната бария-стронция на подложке из оксида магния можно вдвое повысить рабочую частоту преобразователя за счет формирования в пленке периодической доменной структуры. Показано, что в тонкой сегнетоэлектрической пленке при стандартной структуре электродов эффективно возбуждается вторая гармоника поверхностной акустической волны. Путем изменения внешнего поляризующего напряжения на электродах пленки можно создавать преобразователи с электрически регулируемым коэффициентом электромеханической связи.},\\n\\tlanguage = {ru},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Письма в ЖТФ},\\n\\tauthor = {Мухортов, В. М. and Бирюков, С. В. and Головко, Ю. И. and Карапетьян, Г. Я. and Масычев, С. И. and Мухортов, В.М.},\\n\\tmonth = feb,\\n\\tyear = {2011},\\n\\tpages = {31--37},\\n}\\n\\n\",\"author_short\":[\"Мухортов, В. М.\",\"Бирюков, С. В.\",\"Головко, Ю. И.\",\"Карапетьян, Г. Я.\",\"Масычев, С. И.\",\"Мухортов, В.\"],\"key\":\"__2011-7\",\"id\":\"__2011-7\",\"bibbaseid\":\"-------2011\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/12492\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Поляризация тонких пленок титаната бария-стронция при действии внешнего электрического поля\",\"volume\":\"81\",\"url\":\"http://journals.ioffe.ru/articles/10392\",\"abstract\":\"В рамках простой феноменологической модели описано поведение поляризации тонкой пленки Ba0.8Sr0.2TiO3 во внешнем электрическом поле при планарной геометрии электродов. Для согласования с экспериментальными данными введено \\\"поле Ван-дер-Ваальса\\\" Ez, формируемое подложкой в направлении нормали к плоскости пленки. Оценка величины поля дает значение Ez=1.1· 108 V/m. Проанализирована фазовая диаграмма пленки Ba0.8Sr0.2TiO3 в плоскости Ez - misfit strain при комнатной температуре\",\"language\":\"ru\",\"number\":\"8\",\"urldate\":\"2023-11-11\",\"journal\":\"Журнал технической физики\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бирюков\"],\"firstnames\":[\"С.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2011\",\"pages\":\"115–120\",\"bibtex\":\"@article{__2011-8,\\n\\ttitle = {Поляризация тонких пленок титаната бария-стронция при действии внешнего электрического поля},\\n\\tvolume = {81},\\n\\turl = {http://journals.ioffe.ru/articles/10392},\\n\\tabstract = {В рамках простой феноменологической модели описано поведение поляризации тонкой пленки Ba0.8Sr0.2TiO3 во внешнем электрическом поле при планарной геометрии электродов. Для согласования с экспериментальными данными введено \\\"поле Ван-дер-Ваальса\\\" Ez, формируемое подложкой в направлении нормали к плоскости пленки. Оценка величины поля дает значение Ez=1.1· 108 V/m. Проанализирована фазовая диаграмма пленки Ba0.8Sr0.2TiO3 в плоскости Ez - misfit strain при комнатной температуре},\\n\\tlanguage = {ru},\\n\\tnumber = {8},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Журнал технической физики},\\n\\tauthor = {Широков, В. Б. and Бирюков, С. В. and Мухортов, В. М. and Юзюк, Ю. И.},\\n\\tmonth = jul,\\n\\tyear = {2011},\\n\\tpages = {115--120},\\n}\\n\\n\",\"author_short\":[\"Широков, В. Б.\",\"Бирюков, С. В.\",\"Мухортов, В. М.\",\"Юзюк, Ю. И.\"],\"key\":\"__2011-8\",\"id\":\"__2011-8\",\"bibbaseid\":\"-----2011\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/10392\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Структура и динамика решетки гетероструктур на основе феррита висмута и титаната бария-стронция на подложке оксида магния\",\"volume\":\"52\",\"url\":\"https://journals.ioffe.ru/articles/1900\",\"abstract\":\"Пленки феррита висмута, легированные неодимом, получены на монокристаллических подложках MgO с эпитаксиальным тонким (1-2 nm) подслоем титаната бария-стронция методом высокочастотного распыления керамических мишеней при повышенном парциальном давлении кислорода при температурах ниже температур сегнетоэлектрического и магнитного переходов. Методами дифракции рентгеновских лучей и спектроскопии комбинационного рассеяния света установлено, что в этих пленках феррита висмута реализуется новая фаза, которая не наблюдается в объемных образцах. Симметрия такой фазы моноклинная, элементарная ячейка содержит две формульные единицы, а вектор спонтанной поляризации отклоняется от направления [111]cub и может иметь различные компоненты вдоль осей x, y и z.\",\"language\":\"ru\",\"number\":\"7\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бунина\"],\"firstnames\":[\"О.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Захарченко\"],\"firstnames\":[\"И.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Анохин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2010\",\"pages\":\"1336–1341\",\"file\":\"Физика твердого тела:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\3AQF2CGA\\\\\\\\1900.html:text/html\",\"bibtex\":\"@article{__2010-2,\\n\\ttitle = {Структура и динамика решетки гетероструктур на основе феррита висмута и титаната бария-стронция на подложке оксида магния},\\n\\tvolume = {52},\\n\\turl = {https://journals.ioffe.ru/articles/1900},\\n\\tabstract = {Пленки феррита висмута, легированные неодимом, получены на монокристаллических подложках MgO с эпитаксиальным тонким (1-2 nm) подслоем титаната бария-стронция методом высокочастотного распыления керамических мишеней при повышенном парциальном давлении кислорода при температурах ниже температур сегнетоэлектрического и магнитного переходов. Методами дифракции рентгеновских лучей и спектроскопии комбинационного рассеяния света установлено, что в этих пленках феррита висмута реализуется новая фаза, которая не наблюдается в объемных образцах. Симметрия такой фазы моноклинная, элементарная ячейка содержит две формульные единицы, а вектор спонтанной поляризации отклоняется от направления [111]cub и может иметь различные компоненты вдоль осей x, y и z.},\\n\\tlanguage = {ru},\\n\\tnumber = {7},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Головко, Ю. И. and Мухортов, В. М. and Бунина, О. А. and Захарченко, И. Н. and Анохин, А. С. and Широков, В. Б. and Юзюк, Ю. И.},\\n\\tmonth = jun,\\n\\tyear = {2010},\\n\\tpages = {1336--1341},\\n\\tfile = {Физика твердого тела:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\3AQF2CGA\\\\\\\\1900.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Головко, Ю. И.\",\"Мухортов, В. М.\",\"Бунина, О. А.\",\"Захарченко, И. Н.\",\"Анохин, А. С.\",\"Широков, В. Б.\",\"Юзюк, Ю. И.\"],\"key\":\"__2010-2\",\"id\":\"__2010-2\",\"bibbaseid\":\"--------2010\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/1900\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Тонкие сегнетоэлектрические пленки: получение и перспективы интеграции\",\"volume\":\"52\",\"url\":\"http://journals.ioffe.ru/articles/1789\",\"abstract\":\"ассматриваются свойства тонких пленок (Ba,Sr)TiO3 и BiFeO3 и наноструктур на их основе. Пленки изготавливаются методом высокочастотного распыления в атмосфере кислорода с повышенным давлением, наноструктуры - методом фокусированного ионного травления; электрическое поле прикладывается в планарной структуре встречно-штыревых электродов. Исследуются структура, диэлектрические, электро-оптические и нелинейно-оптические свойства полученных образцов в широком диапазоне толщин и частот электрического поля. Показана высокая эффективность планарного переключения и его влияния на оптические свойства полученных структур. Наноструктурирование позволяет изменять диэлектрические и оптические свойства исследуемых материалов и таким образом увеличивать диапазон переключения функциональных параметров.\",\"language\":\"ru\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Тонкие сегнетоэлектрические пленки: получение и перспективы интеграции\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Сигов\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мишина\"],\"firstnames\":[\"Е.\",\"Д.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2010\",\"pages\":\"709–717\",\"bibtex\":\"@article{__2010-3,\\n\\ttitle = {Тонкие сегнетоэлектрические пленки: получение и перспективы интеграции},\\n\\tvolume = {52},\\n\\turl = {http://journals.ioffe.ru/articles/1789},\\n\\tabstract = {ассматриваются свойства тонких пленок (Ba,Sr)TiO3 и BiFeO3 и наноструктур на их основе. Пленки изготавливаются методом высокочастотного распыления в атмосфере кислорода с повышенным давлением, наноструктуры - методом фокусированного ионного травления; электрическое поле прикладывается в планарной структуре встречно-штыревых электродов. Исследуются структура, диэлектрические, электро-оптические и нелинейно-оптические свойства полученных образцов в широком диапазоне толщин и частот электрического поля. Показана высокая эффективность планарного переключения и его влияния на оптические свойства полученных структур. Наноструктурирование позволяет изменять диэлектрические и оптические свойства исследуемых материалов и таким образом увеличивать диапазон переключения функциональных параметров.},\\n\\tlanguage = {ru},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Тонкие сегнетоэлектрические пленки: получение и перспективы интеграции},\\n\\tauthor = {Сигов, А. С. and Мишина, Е. Д. and Мухортов, В. М.},\\n\\tmonth = mar,\\n\\tyear = {2010},\\n\\tpages = {709--717},\\n}\\n\\n\",\"author_short\":[\"Сигов, А. С.\",\"Мишина, Е. Д.\",\"Мухортов, В. М.\"],\"key\":\"__2010-3\",\"id\":\"__2010-3\",\"bibbaseid\":\"----2010\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/1789\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":1,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Диэлектрические спектры тонких пленок мультиферроика Bi$_{\\\\textrm{0.98}}$Nd$_{\\\\textrm{0.02}}$FeO$_{\\\\textrm{3}}$ в терагерцевом диапазоне частот\",\"volume\":\"52\",\"url\":\"http://journals.ioffe.ru/articles/1956\",\"abstract\":\"етодами субмиллиметровой спектроскопии на основе ламп обратной волны (ЛОВ) и инфракрасной Фурье-спектроскопии в диапазоне частот 8-1000 cm-1 при комнатной температуре измерены спектры пропускания и отражения тонких пленок мультиферроика Bi0.98Nd0.02FeO3 на подложках монокристаллического MgO. В рамках модели слоистой среды рассчитаны спектры комплексной диэлектрической проницаемости пленок. Обнаружены мощный рост потерь в области 30 cm-1 при уменьшении толщины пленок и обусловленное им пятикратное увеличение статической диэлектрической проницаемости (до 500 в пленке толщиной 32 nm). Явление обсуждается в рамках феноменологической теории фазовых переходов.\",\"language\":\"ru\",\"number\":\"9\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Командин\"],\"firstnames\":[\"Г.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Торгашев\"],\"firstnames\":[\"В.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Волков\"],\"firstnames\":[\"А.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Породинков\"],\"firstnames\":[\"О.\",\"Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Спектор\"],\"firstnames\":[\"И.\",\"Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2010\",\"pages\":\"1717–1723\",\"file\":\"Физика твердого тела:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\NZQTPGVK\\\\\\\\1956.html:text/html\",\"bibtex\":\"@article{__2010-4,\\n\\ttitle = {Диэлектрические спектры тонких пленок мультиферроика {Bi}$_{\\\\textrm{0.98}}${Nd}$_{\\\\textrm{0.02}}${FeO}$_{\\\\textrm{3}}$ в терагерцевом диапазоне частот},\\n\\tvolume = {52},\\n\\turl = {http://journals.ioffe.ru/articles/1956},\\n\\tabstract = {етодами субмиллиметровой спектроскопии на основе ламп обратной волны (ЛОВ) и инфракрасной Фурье-спектроскопии в диапазоне частот 8-1000 cm-1 при комнатной температуре измерены спектры пропускания и отражения тонких пленок мультиферроика Bi0.98Nd0.02FeO3 на подложках монокристаллического MgO. В рамках модели слоистой среды рассчитаны спектры комплексной диэлектрической проницаемости пленок. Обнаружены мощный рост потерь в области 30 cm-1 при уменьшении толщины пленок и обусловленное им пятикратное увеличение статической диэлектрической проницаемости (до 500 в пленке толщиной 32 nm). Явление обсуждается в рамках феноменологической теории фазовых переходов.},\\n\\tlanguage = {ru},\\n\\tnumber = {9},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Командин, Г. А. and Торгашев, В. И. and Волков, А. А. and Породинков, О. Е. and Спектор, И. Е. and Мухортов, В. М.},\\n\\tmonth = sep,\\n\\tyear = {2010},\\n\\tpages = {1717--1723},\\n\\tfile = {Физика твердого тела:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\NZQTPGVK\\\\\\\\1956.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Командин, Г. А.\",\"Торгашев, В. И.\",\"Волков, А. А.\",\"Породинков, О. Е.\",\"Спектор, И. Е.\",\"Мухортов, В. М.\"],\"key\":\"__2010-4\",\"id\":\"__2010-4\",\"bibbaseid\":\"------bitextrm098ndtextrm002feotextrm3-2010\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/1956\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Спектры комбинационного рассеяния пленки титаната бария-стронция в электрических полях\",\"volume\":\"74\",\"issn\":\"0367-6765\",\"url\":\"https://www.elibrary.ru/item.asp?id=15249715\",\"abstract\":\"Исследованы поляризованные спектры комбинационного рассеяния гетероэпитаксиальной пленки титаната бария–стронция на подложке MgO во внешнем электрическом поле, приложенном перпендикулярно направлению спонтанной поляризации. Частичная деполяризация, наблюдающаяся в спектрах, свидетельствует об индуцированном полем понижении симметрии кристаллической решетки.\",\"language\":\"ru\",\"number\":\"9\",\"urldate\":\"2023-11-11\",\"journal\":\"Известия Российской Академии Наук. Серия Физическая\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Анохин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]}],\"year\":\"2010\",\"keywords\":\"⛔ No DOI found\",\"pages\":\"1282–1284\",\"bibtex\":\"@article{__2010-5,\\n\\ttitle = {Спектры комбинационного рассеяния пленки титаната бария-стронция в электрических полях},\\n\\tvolume = {74},\\n\\tissn = {0367-6765},\\n\\turl = {https://www.elibrary.ru/item.asp?id=15249715},\\n\\tabstract = {Исследованы поляризованные спектры комбинационного рассеяния гетероэпитаксиальной пленки титаната бария–стронция на подложке MgO во внешнем электрическом поле, приложенном перпендикулярно направлению спонтанной поляризации. Частичная деполяризация, наблюдающаяся в спектрах, свидетельствует об индуцированном полем понижении симметрии кристаллической решетки.},\\n\\tlanguage = {ru},\\n\\tnumber = {9},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Известия Российской Академии Наук. Серия Физическая},\\n\\tauthor = {Анохин, А. С. and Юзюк, Ю. И. and Головко, Ю. И. and Мухортов, В. М.},\\n\\tyear = {2010},\\n\\tkeywords = {⛔ No DOI found},\\n\\tpages = {1282--1284},\\n}\\n\\n\",\"author_short\":[\"Анохин, А. С.\",\"Юзюк, Ю. И.\",\"Головко, Ю. И.\",\"Мухортов, В. М.\"],\"key\":\"__2010-5\",\"id\":\"__2010-5\",\"bibbaseid\":\"-----2010\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.elibrary.ru/item.asp?id=15249715\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Сегнетоэлектрические тонкие пленки BiFeO$_{\\\\textrm{3}}$ с орторомбической структурой допированного Nd\",\"volume\":\"74\",\"issn\":\"0367-6765\",\"url\":\"https://www.elibrary.ru/item.asp?id=15142299\",\"abstract\":\"Методами дифракции рентгеновских лучей и рамановской спектроскопии определена орторомбическая симметрия (Fmm2, a = 7.914 A, b = 7.913 A и c = 7.937 A) эпитаксиальных пленок феррита висмута, допированного Nd, на подложках MgO.\",\"language\":\"ru\",\"number\":\"8\",\"urldate\":\"2023-11-11\",\"journal\":\"Известия Российской Академии Наук. Серия Физическая\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Леонтьев\"],\"firstnames\":[\"И.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Анохин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]}],\"year\":\"2010\",\"keywords\":\"⛔ No DOI found\",\"pages\":\"1163–1165\",\"bibtex\":\"@article{__2010-6,\\n\\ttitle = {Сегнетоэлектрические тонкие пленки {BiFeO}$_{\\\\textrm{3}}$ с орторомбической структурой допированного {Nd}},\\n\\tvolume = {74},\\n\\tissn = {0367-6765},\\n\\turl = {https://www.elibrary.ru/item.asp?id=15142299},\\n\\tabstract = {Методами дифракции рентгеновских лучей и рамановской спектроскопии определена орторомбическая симметрия (Fmm2, a = 7.914 A, b = 7.913 A и c = 7.937 A) эпитаксиальных пленок феррита висмута, допированного Nd, на подложках MgO.},\\n\\tlanguage = {ru},\\n\\tnumber = {8},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Известия Российской Академии Наук. Серия Физическая},\\n\\tauthor = {Леонтьев, И. Н. and Анохин, А. С. and Юзюк, Ю. И. and Головко, Ю. И. and Мухортов, В. М.},\\n\\tyear = {2010},\\n\\tkeywords = {⛔ No DOI found},\\n\\tpages = {1163--1165},\\n}\\n\\n\",\"author_short\":[\"Леонтьев, И. Н.\",\"Анохин, А. С.\",\"Юзюк, Ю. И.\",\"Головко, Ю. И.\",\"Мухортов, В. М.\"],\"key\":\"__2010-6\",\"id\":\"__2010-6\",\"bibbaseid\":\"-----bifeotextrm3nd-2010\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.elibrary.ru/item.asp?id=15142299\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Влияние внутренних деформационных полей на управляемость наноразмерных сегнетоэлектрических пленок в планарном конденсаторе\",\"volume\":\"80\",\"url\":\"http://journals.ioffe.ru/articles/9945\",\"abstract\":\"Рентгенодифракционными методами и просвечивающей электронной спектроскопией высокого разрешения исследованы наноразмерные сегнетоэлектрические гетероэпитаксиальные пленки Ba0.8Sr0.2TiO3, выращенные по слоевому механизму роста на подложках (100) MgO. Установлено, что при изменении толщины пленок релаксация напряжений происходит посредством образования дислокаций нсоответствия на границе раздела между пленкой и подложкой. Существует критическая толщина (~40 nm) пленок, ниже которой в пленках имеют место напряжения растяжения, а выше - напряжения сжатия. Приведены примеры влияния напряжений на диэлектрические характеристики пленок.\",\"language\":\"ru\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Журнал технической физики\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Маматов\"],\"firstnames\":[\"А.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Жигалина\"],\"firstnames\":[\"О.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кускова\"],\"firstnames\":[\"А.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Чувилин\"],\"firstnames\":[\"A.\",\"Л.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2010\",\"pages\":\"77–82\",\"bibtex\":\"@article{__2010-7,\\n\\ttitle = {Влияние внутренних деформационных полей на управляемость наноразмерных сегнетоэлектрических пленок в планарном конденсаторе},\\n\\tvolume = {80},\\n\\turl = {http://journals.ioffe.ru/articles/9945},\\n\\tabstract = {Рентгенодифракционными методами и просвечивающей электронной спектроскопией высокого разрешения исследованы наноразмерные сегнетоэлектрические гетероэпитаксиальные пленки Ba0.8Sr0.2TiO3, выращенные по слоевому механизму роста на подложках (100) MgO. Установлено, что при изменении толщины пленок релаксация напряжений происходит посредством образования дислокаций нсоответствия на границе раздела между пленкой и подложкой. Существует критическая толщина ({\\\\textasciitilde}40 nm) пленок, ниже которой в пленках имеют место напряжения растяжения, а выше - напряжения сжатия. Приведены примеры влияния напряжений на диэлектрические характеристики пленок.},\\n\\tlanguage = {ru},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Журнал технической физики},\\n\\tauthor = {Мухортов, В. М. and Головко, Ю. И. and Маматов, А. А. and Жигалина, О. М. and Кускова, А. Н. and Чувилин, A. Л.},\\n\\tmonth = feb,\\n\\tyear = {2010},\\n\\tpages = {77--82},\\n}\\n\\n\",\"author_short\":[\"Мухортов, В. М.\",\"Головко, Ю. И.\",\"Маматов, А. А.\",\"Жигалина, О. М.\",\"Кускова, А. Н.\",\"Чувилин, A. Л.\"],\"key\":\"__2010-7\",\"id\":\"__2010-7\",\"bibbaseid\":\"-------2010\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/9945\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Наноструктурированный мультиферроик PbFe$_{\\\\textrm{0.5}}$Nb$_{\\\\textrm{0.5}}$O$_{\\\\textrm{3}}$ и его физические свойства\",\"volume\":\"80\",\"url\":\"http://journals.ioffe.ru/articles/10151\",\"abstract\":\"Изучен поликристаллический мультиферроик PbFe0.5Nb0.5O3 (PEN), полученный твердофазным методом, спеканию которого предшествовала обработка при комнатной температуре синтезированного порошка PFN в наковальнях Бриджмена силовым воздействием в сочетании со сдвиговой деформацией (СВСД). Проведен сравнительный анализ электрофизических свойств и структурных параметров рабочих и эталонного образцов. Показано, что, начиная с величины СВСД, равной 200 MPa, доминирующую роль в формировании физических свойств играют точечные дефекты.\",\"language\":\"ru\",\"number\":\"11\",\"urldate\":\"2023-11-11\",\"journal\":\"Журнал технической физики\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Убушаева\"],\"firstnames\":[\"Э.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Абдулвахидов\"],\"firstnames\":[\"К.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мардасова\"],\"firstnames\":[\"И.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Абулвахидов\"],\"firstnames\":[\"Б.\",\"К.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Витченко\"],\"firstnames\":[\"М.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Амиров\"],\"firstnames\":[\"А.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Батдалов\"],\"firstnames\":[\"А.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гамзатов\"],\"firstnames\":[\"А.\",\"Г.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2010\",\"pages\":\"49–52\",\"file\":\"Журнал технической физики:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\26FX65HJ\\\\\\\\10151.html:text/html\",\"bibtex\":\"@article{__2010-8,\\n\\ttitle = {Наноструктурированный мультиферроик {PbFe}$_{\\\\textrm{0.5}}${Nb}$_{\\\\textrm{0.5}}${O}$_{\\\\textrm{3}}$ и его физические свойства},\\n\\tvolume = {80},\\n\\turl = {http://journals.ioffe.ru/articles/10151},\\n\\tabstract = {Изучен поликристаллический мультиферроик PbFe0.5Nb0.5O3 (PEN), полученный твердофазным методом, спеканию которого предшествовала обработка при комнатной температуре синтезированного порошка PFN в наковальнях Бриджмена силовым воздействием в сочетании со сдвиговой деформацией (СВСД). Проведен сравнительный анализ электрофизических свойств и структурных параметров рабочих и эталонного образцов. Показано, что, начиная с величины СВСД, равной 200 MPa, доминирующую роль в формировании физических свойств играют точечные дефекты.},\\n\\tlanguage = {ru},\\n\\tnumber = {11},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Журнал технической физики},\\n\\tauthor = {Убушаева, Э. Н. and Абдулвахидов, К. Г. and Мардасова, И. В. and Абулвахидов, Б. К. and Витченко, М. А. and Амиров, А. А. and Батдалов, А. Б. and Гамзатов, А. Г.},\\n\\tmonth = oct,\\n\\tyear = {2010},\\n\\tpages = {49--52},\\n\\tfile = {Журнал технической физики:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\26FX65HJ\\\\\\\\10151.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Убушаева, Э. Н.\",\"Абдулвахидов, К. Г.\",\"Мардасова, И. В.\",\"Абулвахидов, Б. К.\",\"Витченко, М. А.\",\"Амиров, А. А.\",\"Батдалов, А. Б.\",\"Гамзатов, А. Г.\"],\"key\":\"__2010-8\",\"id\":\"__2010-8\",\"bibbaseid\":\"--------pbfetextrm05nbtextrm05otextrm3-2010\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/10151\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Ferroelectric Q-phase in a NaNbO$_{\\\\textrm{3}}$ epitaxial thin film\",\"volume\":\"96\",\"issn\":\"0003-6951\",\"url\":\"https://doi.org/10.1063/1.3437090\",\"doi\":\"10.1063/1.3437090\",\"abstract\":\"Epitaxial NaNbO3 thin films have been grown by pulsed laser deposition on cubic (00l) MgO substrate with epitaxial (La0.5Sr0.5)CoO3 buffer layer. Micro-Raman spectroscopy studies revealed that the ferroelectric Q phase (Pmc21, Z=4) is stable in a 250-nm-thick film in contrast to the antiferroelectric phase P (Pbma, Z=8) known to exist in the bulk single crystals and ceramics of undoped stoichiometric NaNbO3. Temperature-dependent Raman spectra indicate that the Q phase is stable over a wide temperature range (at least from 80 to 600 K), while the low-temperature ferroelectric rhombohedral phase N, typical for NaNbO3 single crystals, is not observed.\",\"number\":\"22\",\"urldate\":\"2023-11-11\",\"journal\":\"Applied Physics Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shakhovoy\"],\"firstnames\":[\"R.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Raevskaya\"],\"firstnames\":[\"S.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Raevski\"],\"firstnames\":[\"I.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Karkut\"],\"firstnames\":[\"M.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Simon\"],\"firstnames\":[\"P.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2010\",\"pages\":\"222904\",\"bibtex\":\"@article{yuzyuk_ferroelectric_2010,\\n\\ttitle = {Ferroelectric {Q}-phase in a {NaNbO}$_{\\\\textrm{3}}$ epitaxial thin film},\\n\\tvolume = {96},\\n\\tissn = {0003-6951},\\n\\turl = {https://doi.org/10.1063/1.3437090},\\n\\tdoi = {10.1063/1.3437090},\\n\\tabstract = {Epitaxial NaNbO3 thin films have been grown by pulsed laser deposition on cubic (00l) MgO substrate with epitaxial (La0.5Sr0.5)CoO3 buffer layer. Micro-Raman spectroscopy studies revealed that the ferroelectric Q phase (Pmc21, Z=4) is stable in a 250-nm-thick film in contrast to the antiferroelectric phase P (Pbma, Z=8) known to exist in the bulk single crystals and ceramics of undoped stoichiometric NaNbO3. Temperature-dependent Raman spectra indicate that the Q phase is stable over a wide temperature range (at least from 80 to 600 K), while the low-temperature ferroelectric rhombohedral phase N, typical for NaNbO3 single crystals, is not observed.},\\n\\tnumber = {22},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Applied Physics Letters},\\n\\tauthor = {Yuzyuk, Yu. I. and Shakhovoy, R. A. and Raevskaya, S. I. and Raevski, I. P. and El Marssi, M. and Karkut, M. G. and Simon, P.},\\n\\tmonth = jun,\\n\\tyear = {2010},\\n\\tpages = {222904},\\n}\\n\\n\",\"author_short\":[\"Yuzyuk, Y. I.\",\"Shakhovoy, R. A.\",\"Raevskaya, S. I.\",\"Raevski, I. P.\",\"El Marssi, M.\",\"Karkut, M. G.\",\"Simon, P.\"],\"key\":\"yuzyuk_ferroelectric_2010\",\"id\":\"yuzyuk_ferroelectric_2010\",\"bibbaseid\":\"yuzyuk-shakhovoy-raevskaya-raevski-elmarssi-karkut-simon-ferroelectricqphaseinananbotextrm3epitaxialthinfilm-2010\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.3437090\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Ferroelectric BaTiO$_{\\\\textrm{3}}$/BaZrO$_{\\\\textrm{3}}$ superlattices: X-ray diffraction, Raman spectroscopy, and polarization hysteresis loops\",\"volume\":\"108\",\"issn\":\"0021-8979\",\"shorttitle\":\"Ferroelectric BaTiO3/BaZrO3 superlattices\",\"url\":\"https://doi.org/10.1063/1.3496620\",\"doi\":\"10.1063/1.3496620\",\"abstract\":\"Artificial superlattices (SLs) consisting of ferroelectric BaTiO3 (BT) and paraelectric BaZrO3 (BZ) have been growth by a pulsed laser deposition technique. The epitaxial BT and BZ layers with a periodicity from 16 Å to 1056 Å were sequentially deposited on (001) MgO substrate buffered with an oxide conducting layer of La1/2Sr1/2CoO3. The out-of-plane lattice parameters of the SLs constituents were determined by modeling of the x-ray diffractograms. The results indicate that the polar c-axis of the BT layers lies in the plane of the substrate and BZ layers exhibit enhanced tetragonal distortion which is induced by the mismatch between the alternating BZ and BT layers. The Raman data reinforces this interpretation and suggest a monoclinic phase in BT layers and polar phase in BZ layers. The Raman spectra give evidence of coupling between the constituent layers and a narrowing of the Raman peaks is attributed to a reduction in the disorder of the Ti4+ ions due to the epitaxial strain. This strain is responsible for the upward frequency shift in the soft modes, especially, the E(1TO) mode, which is markedly altered with respect to its analogs in BT-bulk crystal and BT thin film. Ferroelectric hysteresis loops measurements, confirmed the x-ray diffraction and Raman results, and revealed a clear ferroelectric behavior for the constrained SLs (32 Å≤Λ≤256 Å) while a weak ferroelectricity is observed for the large periods (Λ=500 Å and 1056 Å). This is attributed to the strain-induced ferroelectricity in BZ layers for the constrained SLs.\",\"number\":\"8\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Applied Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gagou\"],\"firstnames\":[\"Y.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Belhadi\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"De\",\"Guerville\"],\"firstnames\":[\"F.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Raevski\"],\"firstnames\":[\"I.\",\"P.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2010\",\"pages\":\"084104\",\"bibtex\":\"@article{el_marssi_ferroelectric_2010,\\n\\ttitle = {Ferroelectric {BaTiO}$_{\\\\textrm{3}}$/{BaZrO}$_{\\\\textrm{3}}$ superlattices: {X}-ray diffraction, {Raman} spectroscopy, and polarization hysteresis loops},\\n\\tvolume = {108},\\n\\tissn = {0021-8979},\\n\\tshorttitle = {Ferroelectric {BaTiO3}/{BaZrO3} superlattices},\\n\\turl = {https://doi.org/10.1063/1.3496620},\\n\\tdoi = {10.1063/1.3496620},\\n\\tabstract = {Artificial superlattices (SLs) consisting of ferroelectric BaTiO3 (BT) and paraelectric BaZrO3 (BZ) have been growth by a pulsed laser deposition technique. The epitaxial BT and BZ layers with a periodicity from 16 Å to 1056 Å were sequentially deposited on (001) MgO substrate buffered with an oxide conducting layer of La1/2Sr1/2CoO3. The out-of-plane lattice parameters of the SLs constituents were determined by modeling of the x-ray diffractograms. The results indicate that the polar c-axis of the BT layers lies in the plane of the substrate and BZ layers exhibit enhanced tetragonal distortion which is induced by the mismatch between the alternating BZ and BT layers. The Raman data reinforces this interpretation and suggest a monoclinic phase in BT layers and polar phase in BZ layers. The Raman spectra give evidence of coupling between the constituent layers and a narrowing of the Raman peaks is attributed to a reduction in the disorder of the Ti4+ ions due to the epitaxial strain. This strain is responsible for the upward frequency shift in the soft modes, especially, the E(1TO) mode, which is markedly altered with respect to its analogs in BT-bulk crystal and BT thin film. Ferroelectric hysteresis loops measurements, confirmed the x-ray diffraction and Raman results, and revealed a clear ferroelectric behavior for the constrained SLs (32 Å≤Λ≤256 Å) while a weak ferroelectricity is observed for the large periods (Λ=500 Å and 1056 Å). This is attributed to the strain-induced ferroelectricity in BZ layers for the constrained SLs.},\\n\\tnumber = {8},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Applied Physics},\\n\\tauthor = {El Marssi, M. and Gagou, Y. and Belhadi, J. and De Guerville, F. and Yuzyuk, Yu. I. and Raevski, I. P.},\\n\\tmonth = oct,\\n\\tyear = {2010},\\n\\tpages = {084104},\\n}\\n\\n\",\"author_short\":[\"El Marssi, M.\",\"Gagou, Y.\",\"Belhadi, J.\",\"De Guerville, F.\",\"Yuzyuk, Y. I.\",\"Raevski, I. P.\"],\"key\":\"el_marssi_ferroelectric_2010\",\"id\":\"el_marssi_ferroelectric_2010\",\"bibbaseid\":\"elmarssi-gagou-belhadi-deguerville-yuzyuk-raevski-ferroelectricbatiotextrm3bazrotextrm3superlatticesxraydiffractionramanspectroscopyandpolarizationhysteresisloops-2010\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.3496620\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Ferroelectric BaTiO$_{\\\\textrm{3}}$ single crystal under superstrong electric fields up to 55 MV/m: A comparative experimental and theoretical study\",\"volume\":\"96\",\"issn\":\"0003-6951\",\"shorttitle\":\"Ferroelectric BaTiO3 single crystal under superstrong electric fields up to 55 MV/m\",\"url\":\"https://doi.org/10.1063/1.3386537\",\"doi\":\"10.1063/1.3386537\",\"abstract\":\"We investigated the effect of huge electric field up to E=55 MV/m on tetragonal ferroelectric phase of BaTiO3 single crystal. Both lattice parameters and the dielectric susceptibility along the polar axis were determined. The induced polarization shows a continuous increase up to 20% of the spontaneous polarization. The longitudinal d33 and transverse d31 piezoelectric coefficients were also determined. The experimental data are described by a phenomenological approach. Interestingly, an intermediate critical electric field value of E∼25 MV/m was evidenced suggesting that the physics below and above this value are different.\",\"number\":\"14\",\"urldate\":\"2023-11-11\",\"journal\":\"Applied Physics Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fesenko\"],\"firstnames\":[\"O.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"N.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dkhil\"],\"firstnames\":[\"B.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2010\",\"pages\":\"142904\",\"file\":\"Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\ZP8445SF\\\\\\\\Ferroelectric-BaTiO3-single-crystal-under.html:text/html\",\"bibtex\":\"@article{leontyev_ferroelectric_2010,\\n\\ttitle = {Ferroelectric {BaTiO}$_{\\\\textrm{3}}$ single crystal under superstrong electric fields up to 55 {MV}/m: {A} comparative experimental and theoretical study},\\n\\tvolume = {96},\\n\\tissn = {0003-6951},\\n\\tshorttitle = {Ferroelectric {BaTiO3} single crystal under superstrong electric fields up to 55 {MV}/m},\\n\\turl = {https://doi.org/10.1063/1.3386537},\\n\\tdoi = {10.1063/1.3386537},\\n\\tabstract = {We investigated the effect of huge electric field up to E=55 MV/m on tetragonal ferroelectric phase of BaTiO3 single crystal. Both lattice parameters and the dielectric susceptibility along the polar axis were determined. The induced polarization shows a continuous increase up to 20\\\\% of the spontaneous polarization. The longitudinal d33 and transverse d31 piezoelectric coefficients were also determined. The experimental data are described by a phenomenological approach. Interestingly, an intermediate critical electric field value of E∼25 MV/m was evidenced suggesting that the physics below and above this value are different.},\\n\\tnumber = {14},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Applied Physics Letters},\\n\\tauthor = {Leontyev, I. N. and Fesenko, O. E. and Leontyev, N. G. and Dkhil, B.},\\n\\tmonth = apr,\\n\\tyear = {2010},\\n\\tpages = {142904},\\n\\tfile = {Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\ZP8445SF\\\\\\\\Ferroelectric-BaTiO3-single-crystal-under.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Leontyev, I. N.\",\"Fesenko, O. E.\",\"Leontyev, N. G.\",\"Dkhil, B.\"],\"key\":\"leontyev_ferroelectric_2010\",\"id\":\"leontyev_ferroelectric_2010\",\"bibbaseid\":\"leontyev-fesenko-leontyev-dkhil-ferroelectricbatiotextrm3singlecrystalundersuperstrongelectricfieldsupto55mvmacomparativeexperimentalandtheoreticalstudy-2010\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.3386537\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Фазовые переходы в PbSc$_{\\\\textrm{0.5}}$Ta$_{\\\\textrm{0.5}}$O$_{\\\\textrm{3}}$\",\"volume\":\"80\",\"url\":\"http://journals.ioffe.ru/articles/9965\",\"abstract\":\"Рентгенодифрактометрическим, электрофизическими и оптическими методами изучены разупорядоченные и частично упорядоченные сегнетоэлектрические монокристаллы PbSc0.5Ta0.5O3 в широком интервале значений температуры. В низкотемпературной области при T=-40oC обнаружен фазовый переход, который подтверждается как электрофизическими, так и рентгенодифрактометрическим методами.\",\"language\":\"ru\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Журнал технической физики\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Абдулвахидов\"],\"firstnames\":[\"К.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мардасова\"],\"firstnames\":[\"И.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мясникова\"],\"firstnames\":[\"Т.\",\"П.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Витченко\"],\"firstnames\":[\"М.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ошаева\"],\"firstnames\":[\"Э.\",\"Н.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2010\",\"pages\":\"81–83\",\"bibtex\":\"@article{__2010-9,\\n\\ttitle = {Фазовые переходы в {PbSc}$_{\\\\textrm{0.5}}${Ta}$_{\\\\textrm{0.5}}${O}$_{\\\\textrm{3}}$},\\n\\tvolume = {80},\\n\\turl = {http://journals.ioffe.ru/articles/9965},\\n\\tabstract = {Рентгенодифрактометрическим, электрофизическими и оптическими методами изучены разупорядоченные и частично упорядоченные сегнетоэлектрические монокристаллы PbSc0.5Ta0.5O3 в широком интервале значений температуры. В низкотемпературной области при T=-40oC обнаружен фазовый переход, который подтверждается как электрофизическими, так и рентгенодифрактометрическим методами.},\\n\\tlanguage = {ru},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Журнал технической физики},\\n\\tauthor = {Абдулвахидов, К. Г. and Мардасова, И. В. and Мясникова, Т. П. and Витченко, М. А. and Ошаева, Э. Н.},\\n\\tmonth = mar,\\n\\tyear = {2010},\\n\\tpages = {81--83},\\n}\\n\\n\",\"author_short\":[\"Абдулвахидов, К. Г.\",\"Мардасова, И. В.\",\"Мясникова, Т. П.\",\"Витченко, М. А.\",\"Ошаева, Э. Н.\"],\"key\":\"__2010-9\",\"id\":\"__2010-9\",\"bibbaseid\":\"-----pbsctextrm05tatextrm05otextrm3-2010\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/9965\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Терагерцевые диэлектрические спектры тонких пленок (Ba,Sr)TiO$_{\\\\textrm{3}}$\",\"volume\":\"51\",\"url\":\"https://journals.ioffe.ru/articles/2288\",\"abstract\":\"Измерены спектры отражения и пропускания пленок Ba0.7Sr0.3TiO3 с толщинами 36 и 800 mum на подложке из MgO на частотах 8-1000 cm-1 при комнатной температуре. Методом моделирования извлечены диэлектрические параметры материала пленок. Найдена зависимость диэлектрической проницаемости от толщины пленки. Выявлено сильное влияние спектра поглощения излучения в подложке на расчетные диэлектрические спектры материала пленки. Показана необходимость учета при моделировании подфононных диэлектрических потерь в подложке.\",\"language\":\"ru\",\"number\":\"7\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Командин\"],\"firstnames\":[\"Г.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Волков\"],\"firstnames\":[\"А.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Спектор\"],\"firstnames\":[\"И.\",\"Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Воротилов\"],\"firstnames\":[\"К.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2009\",\"pages\":\"1280–1283\",\"bibtex\":\"@article{__2009,\\n\\ttitle = {Терагерцевые диэлектрические спектры тонких пленок ({Ba},{Sr}){TiO}$_{\\\\textrm{3}}$},\\n\\tvolume = {51},\\n\\turl = {https://journals.ioffe.ru/articles/2288},\\n\\tabstract = {Измерены спектры отражения и пропускания пленок Ba0.7Sr0.3TiO3 с толщинами 36 и 800 mum на подложке из MgO на частотах 8-1000 cm-1 при комнатной температуре. Методом моделирования извлечены диэлектрические параметры материала пленок. Найдена зависимость диэлектрической проницаемости от толщины пленки. Выявлено сильное влияние спектра поглощения излучения в подложке на расчетные диэлектрические спектры материала пленки. Показана необходимость учета при моделировании подфононных диэлектрических потерь в подложке.},\\n\\tlanguage = {ru},\\n\\tnumber = {7},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Командин, Г. А. and Волков, А. А. and Спектор, И. Е. and Воротилов, К. А. and Мухортов, В. М.},\\n\\tmonth = jun,\\n\\tyear = {2009},\\n\\tpages = {1280--1283},\\n}\\n\\n\",\"author_short\":[\"Командин, Г. А.\",\"Волков, А. А.\",\"Спектор, И. Е.\",\"Воротилов, К. А.\",\"Мухортов, В. М.\"],\"key\":\"__2009\",\"id\":\"__2009\",\"bibbaseid\":\"-----basrtiotextrm3-2009\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/2288\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Феноменологическое описание тонких пленок SrTiO$_{\\\\textrm{3}}$\",\"volume\":\"51\",\"url\":\"https://journals.ioffe.ru/articles/2235\",\"abstract\":\"Проведено вычисление констант феноменологического потенциала SrTiO3 с учетом последних экспериментальных данных. По сравнению с ранее приведенными значениями константы alpha11,alpha12,t44 изменены более чем на порядок. Рассчитаны фазовые T-P-диаграммы при действии одноосных - [001] и [110] - нагрузок. Построена фазовая диаграмма температура-деформация (misfit strain) тонкой пленки SrTiO3, на которой чисто сегнетоэлектрические фазы существуют при низких температурах.\",\"language\":\"ru\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Леманов\"],\"firstnames\":[\"В.\",\"В.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2009\",\"pages\":\"972–978\",\"bibtex\":\"@article{__2009-1,\\n\\ttitle = {Феноменологическое описание тонких пленок {SrTiO}$_{\\\\textrm{3}}$},\\n\\tvolume = {51},\\n\\turl = {https://journals.ioffe.ru/articles/2235},\\n\\tabstract = {Проведено вычисление констант феноменологического потенциала SrTiO3 с учетом последних экспериментальных данных. По сравнению с ранее приведенными значениями константы alpha11,alpha12,t44 изменены более чем на порядок. Рассчитаны фазовые T-P-диаграммы при действии одноосных - [001] и [110] - нагрузок. Построена фазовая диаграмма температура-деформация (misfit strain) тонкой пленки SrTiO3, на которой чисто сегнетоэлектрические фазы существуют при низких температурах.},\\n\\tlanguage = {ru},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Широков, В. Б. and Юзюк, Ю. И. and Леманов, В. В.},\\n\\tmonth = apr,\\n\\tyear = {2009},\\n\\tpages = {972--978},\\n}\\n\\n\",\"author_short\":[\"Широков, В. Б.\",\"Юзюк, Ю. И.\",\"Леманов, В. В.\"],\"key\":\"__2009-1\",\"id\":\"__2009-1\",\"bibbaseid\":\"---srtiotextrm3-2009\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/2235\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Soft mode dynamics and the reduction of Ti$^{\\\\textrm{4+}}$ disorder in ferroelectric∕relaxor superlattices BaTiO$_{\\\\textrm{3}}$ / BaTi$_{\\\\textrm{0.68}}$Zr$_{\\\\textrm{0.32}}$O$_{\\\\textrm{3}}$\",\"volume\":\"74\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.74.064107\",\"doi\":\"10.1103/PhysRevB.74.064107\",\"abstract\":\"We used pulsed laser deposition to grow a series of [BaTiO3]Λ∕2/[BaTi0.68Zr0.32O3]Λ∕2 (BTZ∕BT) superlattices (SL’s) with a modulation period Λ that varies between 16Å⩽Λ⩽1008Å; the total thickness is kept constant at about 4000Å. We determine the out-of-plane lattice parameters of the SL constituents by modeling the x-ray diffractograms of the SL’s. The results indicate that the polar c axis of the BT layers lies in the plane of the film. The Raman data reinforces this interpretation. The Raman spectra of SL’s give evidence of coupling between BT and BTZ layers and a narrowing of the Raman peaks suggest a reduction of the disorder of the Ti4+ ions due to the strain. This strain resulting from the lattice mismatch between the constituent layers is responsible for the upward frequency shift of the soft modes, especially the E(1TO) mode, which is markedly altered with respect to its analogs in BT-bulk crystals and BT film. This soft-mode behavior as a function of Λ indicates that the crystal structure of all SL’s is more rigid than in BTZ and BT single thin films.\",\"language\":\"en\",\"number\":\"6\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"De\",\"Guerville\"],\"firstnames\":[\"F.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Raevski\"],\"firstnames\":[\"I.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Karkut\"],\"firstnames\":[\"M.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2006\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"064107\",\"bibtex\":\"@article{de_guerville_soft_2006,\\n\\ttitle = {Soft mode dynamics and the reduction of {Ti}$^{\\\\textrm{4+}}$ disorder in ferroelectric∕relaxor superlattices {BaTiO}$_{\\\\textrm{3}}$ / {BaTi}$_{\\\\textrm{0.68}}${Zr}$_{\\\\textrm{0.32}}${O}$_{\\\\textrm{3}}$},\\n\\tvolume = {74},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.74.064107},\\n\\tdoi = {10.1103/PhysRevB.74.064107},\\n\\tabstract = {We used pulsed laser deposition to grow a series of [BaTiO3]Λ∕2/[BaTi0.68Zr0.32O3]Λ∕2 (BTZ∕BT) superlattices (SL’s) with a modulation period Λ that varies between 16Å⩽Λ⩽1008Å; the total thickness is kept constant at about 4000Å. We determine the out-of-plane lattice parameters of the SL constituents by modeling the x-ray diffractograms of the SL’s. The results indicate that the polar c axis of the BT layers lies in the plane of the film. The Raman data reinforces this interpretation. The Raman spectra of SL’s give evidence of coupling between BT and BTZ layers and a narrowing of the Raman peaks suggest a reduction of the disorder of the Ti4+ ions due to the strain. This strain resulting from the lattice mismatch between the constituent layers is responsible for the upward frequency shift of the soft modes, especially the E(1TO) mode, which is markedly altered with respect to its analogs in BT-bulk crystals and BT film. This soft-mode behavior as a function of Λ indicates that the crystal structure of all SL’s is more rigid than in BTZ and BT single thin films.},\\n\\tlanguage = {en},\\n\\tnumber = {6},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {De Guerville, F. and El Marssi, M. and Raevski, I. P. and Karkut, M. G. and Yuzyuk, Yu. I.},\\n\\tmonth = aug,\\n\\tyear = {2006},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {064107},\\n}\\n\\n\",\"author_short\":[\"De Guerville, F.\",\"El Marssi, M.\",\"Raevski, I. P.\",\"Karkut, M. G.\",\"Yuzyuk, Y. I.\"],\"key\":\"de_guerville_soft_2006\",\"id\":\"de_guerville_soft_2006\",\"bibbaseid\":\"deguerville-elmarssi-raevski-karkut-yuzyuk-softmodedynamicsandthereductionoftitextrm4disorderinferroelectricrelaxorsuperlatticesbatiotextrm3batitextrm068zrtextrm032otextrm3-2006\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.74.064107\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Phenomenological theory of phase transitions in epitaxial Ba$_{\\\\textrm{x}}$Sr$_{\\\\textrm{1-x}}$TiO$_{\\\\textrm{3}}$ thin films\",\"volume\":\"79\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.79.144118\",\"doi\":\"10.1103/PhysRevB.79.144118\",\"abstract\":\"A phenomenological thermodynamic theory of BaxSr1−xTiO3 (BST-x) thin films epitaxially grown on cubic substrates is developed using the Landau-Devonshire approach. The eighth-order thermodynamic potential for BaTiO3 (BT) single crystal and modified fourth-order potential for SrTiO3 single crystal were used as starting potentials for the end members of the solid solution with the aim to develop potential of BST-x solid solution valid at high temperatures. Several coefficients of these potentials for BT were changed to obtain reasonable agreement between theory and experimental phase diagram for BST-x (x\\\\textgreater0.2) solid solutions. For low Ba content we constructed the specific phase diagram where five phases converge at the multiphase point (TN2=48 K, x=0.029) and all transitions are of the second order. The “concentration-misfit strain” phase diagrams for BST-x thin films at room temperature and “temperature-misfit strain” phase diagrams for particular concentrations are constructed and discussed. Near TN2 coupling between polarization and structural order parameter in the epitaxial film is modified considerably and large number of new phases not present in the bulk materials appear on the phase diagram.\",\"number\":\"14\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dkhil\"],\"firstnames\":[\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lemanov\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2009\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"144118\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\56FT9N2S\\\\§hirokov и др. - 2009 - Phenomenological theory of phase transitions in ep.pdf:application/pdf\",\"bibtex\":\"@article{shirokov_phenomenological_2009,\\n\\ttitle = {Phenomenological theory of phase transitions in epitaxial {Ba}$_{\\\\textrm{x}}${Sr}$_{\\\\textrm{1-x}}${TiO}$_{\\\\textrm{3}}$ thin films},\\n\\tvolume = {79},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.79.144118},\\n\\tdoi = {10.1103/PhysRevB.79.144118},\\n\\tabstract = {A phenomenological thermodynamic theory of BaxSr1−xTiO3 (BST-x) thin films epitaxially grown on cubic substrates is developed using the Landau-Devonshire approach. The eighth-order thermodynamic potential for BaTiO3 (BT) single crystal and modified fourth-order potential for SrTiO3 single crystal were used as starting potentials for the end members of the solid solution with the aim to develop potential of BST-x solid solution valid at high temperatures. Several coefficients of these potentials for BT were changed to obtain reasonable agreement between theory and experimental phase diagram for BST-x (x{\\\\textgreater}0.2) solid solutions. For low Ba content we constructed the specific phase diagram where five phases converge at the multiphase point (TN2=48 K, x=0.029) and all transitions are of the second order. The “concentration-misfit strain” phase diagrams for BST-x thin films at room temperature and “temperature-misfit strain” phase diagrams for particular concentrations are constructed and discussed. Near TN2 coupling between polarization and structural order parameter in the epitaxial film is modified considerably and large number of new phases not present in the bulk materials appear on the phase diagram.},\\n\\tnumber = {14},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Shirokov, V. B. and Yuzyuk, Yu. I. and Dkhil, B. and Lemanov, V. V.},\\n\\tmonth = apr,\\n\\tyear = {2009},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {144118},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\56FT9N2S\\\\\\\\Shirokov и др. - 2009 - Phenomenological theory of phase transitions in ep.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Yuzyuk, Y. I.\",\"Dkhil, B.\",\"Lemanov, V. V.\"],\"key\":\"shirokov_phenomenological_2009\",\"id\":\"shirokov_phenomenological_2009\",\"bibbaseid\":\"shirokov-yuzyuk-dkhil-lemanov-phenomenologicaltheoryofphasetransitionsinepitaxialbatextrmxsrtextrm1xtiotextrm3thinfilms-2009\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.79.144118\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Микрорамановский отклик и осцилляторные параметры фононов в твердых растворах Pb$_{\\\\textrm{1-x}}$Ca$_{\\\\textrm{x}}$TiO$_{\\\\textrm{3}}$ (0.40\\\\textlessx\\\\textless0.62)\",\"volume\":\"51\",\"url\":\"https://journals.ioffe.ru/articles/2094\",\"abstract\":\"Посредством температурных (295\\\\textlessT\\\\textless650 K) исследований поляризованных спектров комбинационного рассеяния света в области частот 10\\\\textlessnu\\\\textless1200 cm-1 на монокристаллическом образце твердого раствора Pb0.54Ca0.46TiO3 установлено существование по крейней мере одной особой температурной точки (Tc~392 K), в которой наблюдаются заметные аномалии осцилляторных параметров фононных мод. Аналогичные явления имеют место в растворах с 0.4\\\\textlessx\\\\textless0.5. Резкий рост интенсивности спектральных линий, соответствующих волнам поляризации, при температурах сразу ниже Tc позволяет сделать вывод о трансформации Pb1-xCaxTiO3 (0.4\\\\textlessx\\\\textless0.5) в полярное состояние, которое отсутствует в системе при концентрациях x\\\\textgreater0.5.\",\"language\":\"ru\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Чабанюк\"],\"firstnames\":[\"А.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Торгашев\"],\"firstnames\":[\"В.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Леманов\"],\"firstnames\":[\"В.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Simon\"],\"firstnames\":[\"P.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2008\",\"pages\":\"155–163\",\"bibtex\":\"@article{__2008,\\n\\ttitle = {Микрорамановский отклик и осцилляторные параметры фононов в твердых растворах {Pb}$_{\\\\textrm{1-x}}${Ca}$_{\\\\textrm{x}}${TiO}$_{\\\\textrm{3}}$ (0.40{\\\\textless}x{\\\\textless}0.62)},\\n\\tvolume = {51},\\n\\turl = {https://journals.ioffe.ru/articles/2094},\\n\\tabstract = {Посредством температурных (295{\\\\textless}T{\\\\textless}650 K) исследований поляризованных спектров комбинационного рассеяния света в области частот 10{\\\\textless}nu{\\\\textless}1200 cm-1 на монокристаллическом образце твердого раствора Pb0.54Ca0.46TiO3 установлено существование по крейней мере одной особой температурной точки (Tc{\\\\textasciitilde}392 K), в которой наблюдаются заметные аномалии осцилляторных параметров фононных мод. Аналогичные явления имеют место в растворах с 0.4{\\\\textless}x{\\\\textless}0.5. Резкий рост интенсивности спектральных линий, соответствующих волнам поляризации, при температурах сразу ниже Tc позволяет сделать вывод о трансформации Pb1-xCaxTiO3 (0.4{\\\\textless}x{\\\\textless}0.5) в полярное состояние, которое отсутствует в системе при концентрациях x{\\\\textgreater}0.5.},\\n\\tlanguage = {ru},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Чабанюк, А. Н. and Торгашев, В. И. and Юзюк, Ю. И. and Леманов, В. В. and Simon, P.},\\n\\tmonth = dec,\\n\\tyear = {2008},\\n\\tpages = {155--163},\\n}\\n\\n\",\"author_short\":[\"Чабанюк, А. Н.\",\"Торгашев, В. И.\",\"Юзюк, Ю. И.\",\"Леманов, В. В.\",\"Simon, P.\"],\"key\":\"__2008\",\"id\":\"__2008\",\"bibbaseid\":\"----simon-pbtextrm1xcatextrmxtiotextrm3040textlessxtextless062-2008\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/2094\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Оптические и структурные свойства наностержней ZnO, полученных методом импульсного лазерного напыления без катализатора\",\"volume\":\"79\",\"url\":\"https://journals.ioffe.ru/articles/9840\",\"abstract\":\"Методом импульсного лазерного напыления без использования катализатора на сапфире получены наностержни ZnO диаметром менее 10 nm. Исследованы структурные особенности наностержней методом комбинационного рассеяния при возбуждении в видимом и УФ-диапазонах. Изучены температурные зависимости экситонных спектров, а также поведение зеленой люминесценции в диапазоне 10-280 K. Интенсивность люминесценции полученных наностержней ZnO в экситонной области превышала зеленую люминесценцию в 7.8 раза при комнатной температуре.\",\"language\":\"ru\",\"number\":\"11\",\"urldate\":\"2023-11-11\",\"journal\":\"Журнал технической физики\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"В.\",\"Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Peres\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Monteiro\"],\"firstnames\":[\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Correira\"],\"firstnames\":[\"M.\",\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sobolev\"],\"firstnames\":[\"N.\",\"A.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2009\",\"pages\":\"45–49\",\"bibtex\":\"@article{__2009-2,\\n\\ttitle = {Оптические и структурные свойства наностержней {ZnO}, полученных методом импульсного лазерного напыления без катализатора},\\n\\tvolume = {79},\\n\\turl = {https://journals.ioffe.ru/articles/9840},\\n\\tabstract = {Методом импульсного лазерного напыления без использования катализатора на сапфире получены наностержни ZnO диаметром менее 10 nm. Исследованы структурные особенности наностержней методом комбинационного рассеяния при возбуждении в видимом и УФ-диапазонах. Изучены температурные зависимости экситонных спектров, а также поведение зеленой люминесценции в диапазоне 10-280 K. Интенсивность люминесценции полученных наностержней ZnO в экситонной области превышала зеленую люминесценцию в 7.8 раза при комнатной температуре.},\\n\\tlanguage = {ru},\\n\\tnumber = {11},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Журнал технической физики},\\n\\tauthor = {Кайдашев, В. Е. and Кайдашев, Е. М. and Peres, M. and Monteiro, T. and Correira, M. R. and Sobolev, N. A.},\\n\\tmonth = oct,\\n\\tyear = {2009},\\n\\tpages = {45--49},\\n}\\n\\n\",\"author_short\":[\"Кайдашев, В. Е.\",\"Кайдашев, Е. М.\",\"Peres, M.\",\"Monteiro, T.\",\"Correira, M. R.\",\"Sobolev, N. A.\"],\"key\":\"__2009-2\",\"id\":\"__2009-2\",\"bibbaseid\":\"--peres-monteiro-correira-sobolev-zno-2009\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/9840\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Исследование пьезоактивности тонких пленок цирконата-титаната свинца\",\"volume\":\"79\",\"url\":\"https://journals.ioffe.ru/articles/9770\",\"abstract\":\"зучены особенности проявления пьезоактивности тонких сегнетоэлектрических пленок цирконата-титаната свинца, полученных высокочастотным катодным распылением мишеней стехиометрического состава. Установлено, что пленки обладают естественной униполярностью. Обсуждаются возможные причины этого явления. Экспериментально построено семейство петель пьезоэлектрического гистерезиса при различных значениях частоты и напряженности внешнего смещающего поля. Полученные зависимости сравниваются с классическими петлями диэлектрического гистерезиса\",\"number\":\"8\",\"urldate\":\"2023-11-11\",\"journal\":\"Журнал технической физики\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Бирюков\"],\"firstnames\":[\"С.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Масычев\"],\"firstnames\":[\"С.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Шелепо\"],\"firstnames\":[\"А.\",\"П.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2009\",\"pages\":\"90–92\",\"bibtex\":\"@article{__2009-3,\\n\\ttitle = {Исследование пьезоактивности тонких пленок цирконата-титаната свинца},\\n\\tvolume = {79},\\n\\turl = {https://journals.ioffe.ru/articles/9770},\\n\\tabstract = {зучены особенности проявления пьезоактивности тонких сегнетоэлектрических пленок цирконата-титаната свинца, полученных высокочастотным катодным распылением мишеней стехиометрического состава. Установлено, что пленки обладают естественной униполярностью. Обсуждаются возможные причины этого явления. Экспериментально построено семейство петель пьезоэлектрического гистерезиса при различных значениях частоты и напряженности внешнего смещающего поля. Полученные зависимости сравниваются с классическими петлями диэлектрического гистерезиса},\\n\\tnumber = {8},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Журнал технической физики},\\n\\tauthor = {Бирюков, С. В. and Головко, Ю. И. and Масычев, С. И. and Мухортов, В. М. and Шелепо, А. П.},\\n\\tmonth = jul,\\n\\tyear = {2009},\\n\\tpages = {90--92},\\n}\\n\\n\",\"author_short\":[\"Бирюков, С. В.\",\"Головко, Ю. И.\",\"Масычев, С. И.\",\"Мухортов, В. М.\",\"Шелепо, А. П.\"],\"key\":\"__2009-3\",\"id\":\"__2009-3\",\"bibbaseid\":\"------2009\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/9770\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Феноменологическое описание фазовых переходов в тонких пленках BaTiO$_{\\\\textrm{3}}$\",\"volume\":\"50\",\"url\":\"https://journals.ioffe.ru/articles/2648\",\"abstract\":\"Проведено феноменологическое описание фазовых переходов в тонких эпитаксиальных пленках BaTiO3 на основе потенциалов Ландау шестой и восьмой степеней. Обнаружена зависимость вида фазовой диаграммы от величины электрострикционного коэффициента Q12. Для разных значений коэффициента Q12, известных из литературы, приведены качественно различные фазовые диаграммы. Определена зависимость деформации несоответствия (misfit strain) пленки от степени тетрагональности пленки при комнатной температуре, что позволяет определить термодинамический путь на фазовой диаграмме для конкретной пленки. Построены зависимости спонтанной поляризации и диэлектрической проницаемости пленки от деформации несоответствия при комнатной температуре.\",\"language\":\"ru\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dkhil\"],\"firstnames\":[\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Леманов\"],\"firstnames\":[\"В.\",\"В.\"],\"suffixes\":[]}],\"year\":\"2008\",\"pages\":\"889–896\",\"file\":\"Физика твердого тела:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\BKW4NGEV\\\\\\\\2648.html:text/html\",\"bibtex\":\"@article{__2008-1,\\n\\ttitle = {Феноменологическое описание фазовых переходов в тонких пленках {BaTiO}$_{\\\\textrm{3}}$},\\n\\tvolume = {50},\\n\\turl = {https://journals.ioffe.ru/articles/2648},\\n\\tabstract = {Проведено феноменологическое описание фазовых переходов в тонких эпитаксиальных пленках BaTiO3 на основе потенциалов Ландау шестой и восьмой степеней. Обнаружена зависимость вида фазовой диаграммы от величины электрострикционного коэффициента Q12. Для разных значений коэффициента Q12, известных из литературы, приведены качественно различные фазовые диаграммы. Определена зависимость деформации несоответствия (misfit strain) пленки от степени тетрагональности пленки при комнатной температуре, что позволяет определить термодинамический путь на фазовой диаграмме для конкретной пленки. Построены зависимости спонтанной поляризации и диэлектрической проницаемости пленки от деформации несоответствия при комнатной температуре.},\\n\\tlanguage = {ru},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Широков, В. Б. and Юзюк, Ю. И. and Dkhil, B. and Леманов, В. В.},\\n\\tyear = {2008},\\n\\tpages = {889--896},\\n\\tfile = {Физика твердого тела:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\BKW4NGEV\\\\\\\\2648.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Широков, В. Б.\",\"Юзюк, Ю. И.\",\"Dkhil, B.\",\"Леманов, В. В.\"],\"key\":\"__2008-1\",\"id\":\"__2008-1\",\"bibbaseid\":\"--dkhil--batiotextrm3-2008\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/2648\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Фазовые переходы в наноразмерных эпитаксиальных сегнетоэлектрических пленках титаната бария-стронция\",\"volume\":\"4\",\"issn\":\"1813-4289\",\"url\":\"http://naukarus.com/fazovye-perehody-v-nanorazmernyh-epitaksialnyh-segnetoelektricheskih-plenkah-titanata-bariya-strontsiya\",\"abstract\":\"С использованием дифракции рентгеновского излучения исследованы температурные зависимости параметров решетки в нормальном и тангенциальном к подложке направлении эиитакси-альных пленок титаната бария-стронция разной толщины (от 6 до 980 нм), выращенных по слоевому механизму высокочастотным катодным распылением при повышенном давлении кислорода. Выявлена критическая толщина пленок (-50 нм), ниже которой в пленках существуют сжимающие напряжения, а выше - растягивающие напряжения. Во всем интервале толщин при изменении температуры от 780 до 100 К в пленках наблюдаются два размытых структурных фазовых перехода второго рода.\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Вестник Южного научного центра РАН\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Маматов\"],\"firstnames\":[\"А.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]}],\"year\":\"2008\",\"keywords\":\"⛔ No DOI found\",\"file\":\"Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\¶WGKVDJ4\\\\\\\\fazovye-perehody-v-nanorazmernyh-epitaksialnyh-segnetoelektricheskih-plenkah-titanata-bariya-st.html:text/html\",\"bibtex\":\"@article{__2008-2,\\n\\ttitle = {Фазовые переходы в наноразмерных эпитаксиальных сегнетоэлектрических пленках титаната бария-стронция},\\n\\tvolume = {4},\\n\\tissn = {1813-4289},\\n\\turl = {http://naukarus.com/fazovye-perehody-v-nanorazmernyh-epitaksialnyh-segnetoelektricheskih-plenkah-titanata-bariya-strontsiya},\\n\\tabstract = {С использованием дифракции рентгеновского излучения исследованы температурные зависимости параметров решетки в нормальном и тангенциальном к подложке направлении эиитакси-альных пленок титаната бария-стронция разной толщины (от 6 до 980 нм), выращенных по слоевому механизму высокочастотным катодным распылением при повышенном давлении кислорода. Выявлена критическая толщина пленок (-50 нм), ниже которой в пленках существуют сжимающие напряжения, а выше - растягивающие напряжения. Во всем интервале толщин при изменении температуры от 780 до 100 К в пленках наблюдаются два размытых структурных фазовых перехода второго рода.},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Вестник Южного научного центра РАН},\\n\\tauthor = {Головко, Ю. И. and Маматов, А. А. and Мухортов, В. М.},\\n\\tyear = {2008},\\n\\tkeywords = {⛔ No DOI found},\\n\\tfile = {Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\PWGKVDJ4\\\\\\\\fazovye-perehody-v-nanorazmernyh-epitaksialnyh-segnetoelektricheskih-plenkah-titanata-bariya-st.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Головко, Ю. И.\",\"Маматов, А. А.\",\"Мухортов, В. М.\"],\"key\":\"__2008-2\",\"id\":\"__2008-2\",\"bibbaseid\":\"----2008\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://naukarus.com/fazovye-perehody-v-nanorazmernyh-epitaksialnyh-segnetoelektricheskih-plenkah-titanata-bariya-strontsiya\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Структурные фазовые переходы в наноразмерных сегнетоэлектрических пленках титаната бария–стронция\",\"volume\":\"50\",\"url\":\"https://journals.ioffe.ru/articles/2579\",\"abstract\":\"С использованием метода дифракции рентгеновского излучения исследованы температурные зависимости параметров решетки в нормальном и тангенциальном к подложке направлениях эпитаксиальных пленок титаната бария-стронция разной толщины (от 6 до 960 nm), выращенных по слоевому механизму высокочастотным катодным распылением при повышенном давлении кислорода. Выявлена критическая толщина пленок (~50 nm), ниже которой в пленках существуют сжимающие, а выше - растягивающие напряжения. Во всем интервале толщин при изменении температуры от 780 до 100 K в пленках наблюдаются два размытых структурных фазовых перехода второго рода. При растягивающих напряжениях переходы могут соответствовать переходам из тетрагональной параэлектрической фазы в aa-фазу и далее в r-фазу, в то время как при сжимающих напряжениях переходы происходят из тетрагональной параэлектрической фазы в сегнетоэлектрическую c-фазу, а при дальнейшем понижении температуры - в r-фазу. Работа проводилась при финансовой поддержке Российского фонда фундаментальных исследований (гранты N 05-02-17191 и 06-02-16271). PACS: 77.80.-e, 64.70.Nd, 77.55.+f\",\"language\":\"ru\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Janolin\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dkhil\"],\"firstnames\":[\"B.\"],\"suffixes\":[]}],\"year\":\"2008\",\"pages\":\"467–471\",\"file\":\"Физика твердого тела:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\GRNCX2XX\\\\\\\\2579.html:text/html\",\"bibtex\":\"@article{__2008-3,\\n\\ttitle = {Структурные фазовые переходы в наноразмерных сегнетоэлектрических пленках титаната бария--стронция},\\n\\tvolume = {50},\\n\\turl = {https://journals.ioffe.ru/articles/2579},\\n\\tabstract = {С использованием метода дифракции рентгеновского излучения исследованы температурные зависимости параметров решетки в нормальном и тангенциальном к подложке направлениях эпитаксиальных пленок титаната бария-стронция разной толщины (от 6 до 960 nm), выращенных по слоевому механизму высокочастотным катодным распылением при повышенном давлении кислорода. Выявлена критическая толщина пленок ({\\\\textasciitilde}50 nm), ниже которой в пленках существуют сжимающие, а выше - растягивающие напряжения. Во всем интервале толщин при изменении температуры от 780 до 100 K в пленках наблюдаются два размытых структурных фазовых перехода второго рода. При растягивающих напряжениях переходы могут соответствовать переходам из тетрагональной параэлектрической фазы в aa-фазу и далее в r-фазу, в то время как при сжимающих напряжениях переходы происходят из тетрагональной параэлектрической фазы в сегнетоэлектрическую c-фазу, а при дальнейшем понижении температуры - в r-фазу. Работа проводилась при финансовой поддержке Российского фонда фундаментальных исследований (гранты N 05-02-17191 и 06-02-16271). PACS: 77.80.-e, 64.70.Nd, 77.55.+f},\\n\\tlanguage = {ru},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Головко, Ю. И. and Мухортов, В. М. and Юзюк, Ю. И. and Janolin, P. E. and Dkhil, B.},\\n\\tyear = {2008},\\n\\tpages = {467--471},\\n\\tfile = {Физика твердого тела:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\GRNCX2XX\\\\\\\\2579.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Головко, Ю. И.\",\"Мухортов, В. М.\",\"Юзюк, Ю. И.\",\"Janolin, P. E.\",\"Dkhil, B.\"],\"key\":\"__2008-3\",\"id\":\"__2008-3\",\"bibbaseid\":\"---janolin-dkhil--2008\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/2579\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Особенности рамановских спектров и фазовых состояний в твердых растворах Pb$_{\\\\textrm{x}}$Sr$_{\\\\textrm{1}}$ $_{\\\\textrm{-}}$ $_{\\\\textrm{x}}$TiO$_{\\\\textrm{3}}$ с низким содержанием свинца\",\"volume\":\"72\",\"issn\":\"0367-6765\",\"url\":\"https://www.elibrary.ru/item.asp?id=9934183\",\"abstract\":\"Приведены результаты исследований микрорамановского спектрального отклика в твердых растворах PbxSr1 - xTiO3 (x = 0.005, 0.01, 0.02, 0.03, 0.04) в диапазоне частот 15–1200 см-1 при нескольких температурах между 10 и 300 К. Проведенное исследование позволило сделать вывод, что в твердых растворах PST область концентраций с x \\\\textless 0.04 скорее всего следует рассматривать как гетерофазную.\",\"language\":\"ru\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Известия Российской Академии Наук. Серия Физическая\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Торгашев\"],\"firstnames\":[\"В.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Чабанюк\"],\"firstnames\":[\"А.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Леманов\"],\"firstnames\":[\"В.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sauvajol\"],\"firstnames\":[\"J.\",\"L.\"],\"suffixes\":[]}],\"year\":\"2008\",\"keywords\":\"⛔ No DOI found\",\"pages\":\"569–571\",\"bibtex\":\"@article{__2008-4,\\n\\ttitle = {Особенности рамановских спектров и фазовых состояний в твердых растворах {Pb}$_{\\\\textrm{x}}${Sr}$_{\\\\textrm{1}}$ $_{\\\\textrm{-}}$ $_{\\\\textrm{x}}${TiO}$_{\\\\textrm{3}}$ с низким содержанием свинца},\\n\\tvolume = {72},\\n\\tissn = {0367-6765},\\n\\turl = {https://www.elibrary.ru/item.asp?id=9934183},\\n\\tabstract = {Приведены результаты исследований микрорамановского спектрального отклика в твердых растворах PbxSr1 - xTiO3 (x = 0.005, 0.01, 0.02, 0.03, 0.04) в диапазоне частот 15–1200 см-1 при нескольких температурах между 10 и 300 К. Проведенное исследование позволило сделать вывод, что в твердых растворах PST область концентраций с x {\\\\textless} 0.04 скорее всего следует рассматривать как гетерофазную.},\\n\\tlanguage = {ru},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Известия Российской Академии Наук. Серия Физическая},\\n\\tauthor = {Торгашев, В. И. and Чабанюк, А. Н. and Юзюк, Ю. И. and Леманов, В. В. and Sauvajol, J. L.},\\n\\tyear = {2008},\\n\\tkeywords = {⛔ No DOI found},\\n\\tpages = {569--571},\\n}\\n\\n\",\"author_short\":[\"Торгашев, В. И.\",\"Чабанюк, А. Н.\",\"Юзюк, Ю. И.\",\"Леманов, В. В.\",\"Sauvajol, J. L.\"],\"key\":\"__2008-4\",\"id\":\"__2008-4\",\"bibbaseid\":\"----sauvajol-pbtextrmxsrtextrm1textrmtextrmxtiotextrm3-2008\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.elibrary.ru/item.asp?id=9934183\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Диэлектрические свойства пленок титаната бария-стронция нанометровой толщины\",\"volume\":\"78\",\"url\":\"https://journals.ioffe.ru/articles/9548\",\"abstract\":\"Методами субмиллиметровой и инфракрасной спектроскопии в области частот 10\\\\textlessnu\\\\textless3000 cm-1 впервые измерены спектры отражения R(nu) и пропускания T(nu) гетероэпитаксиальных пленок титаната бария-стронция различной толщины на подложках MgO. Путем моделирования экспериментальных спектров френелевскими формулами для слоистых сред определены спектры комплексной диэлектрической проницаемости varepsilon*(nu)=varepsilon'(nu)+ivarepsilon''(nu) пленок. Показано, что при уменьшении толщины до 10 nm в пленках возникают растягивающие напряжения в направлении, параллельном плоскости подложки, вызывающие возрастание в несколько раз диэлектрического вклада низкочастотной мягкой моды. PACS: 77.22.Ch, 77.22.Gm, 78.20.Ci, 71.28.+d\",\"language\":\"ru\",\"number\":\"11\",\"urldate\":\"2023-11-11\",\"journal\":\"Журнал технической физики\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Мигунов\"],\"firstnames\":[\"С.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Волков\"],\"firstnames\":[\"А.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Командин\"],\"firstnames\":[\"Г.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лобанов\"],\"firstnames\":[\"А.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Горшунов\"],\"firstnames\":[\"Б.\",\"П.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]}],\"year\":\"2008\",\"pages\":\"99–103\",\"file\":\"Журнал технической физики:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\WZE458EK\\\\\\\\9548.html:text/html\",\"bibtex\":\"@article{__2008-5,\\n\\ttitle = {Диэлектрические свойства пленок титаната бария-стронция нанометровой толщины},\\n\\tvolume = {78},\\n\\turl = {https://journals.ioffe.ru/articles/9548},\\n\\tabstract = {Методами субмиллиметровой и инфракрасной спектроскопии в области частот 10{\\\\textless}nu{\\\\textless}3000 cm-1 впервые измерены спектры отражения R(nu) и пропускания T(nu) гетероэпитаксиальных пленок титаната бария-стронция различной толщины на подложках MgO. Путем моделирования экспериментальных спектров френелевскими формулами для слоистых сред определены спектры комплексной диэлектрической проницаемости varepsilon*(nu)=varepsilon'(nu)+ivarepsilon''(nu) пленок. Показано, что при уменьшении толщины до 10 nm в пленках возникают растягивающие напряжения в направлении, параллельном плоскости подложки, вызывающие возрастание в несколько раз диэлектрического вклада низкочастотной мягкой моды. PACS: 77.22.Ch, 77.22.Gm, 78.20.Ci, 71.28.+d},\\n\\tlanguage = {ru},\\n\\tnumber = {11},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Журнал технической физики},\\n\\tauthor = {Мигунов, С. Н. and Волков, А. А. and Командин, Г. А. and Лобанов, А. Н. and Горшунов, Б. П. and Головко, Ю. И. and Мухортов, В. М. and Юзюк, Ю. И.},\\n\\tyear = {2008},\\n\\tpages = {99--103},\\n\\tfile = {Журнал технической физики:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\WZE458EK\\\\\\\\9548.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Мигунов, С. Н.\",\"Волков, А. А.\",\"Командин, Г. А.\",\"Лобанов, А. Н.\",\"Горшунов, Б. П.\",\"Головко, Ю. И.\",\"Мухортов, В. М.\",\"Юзюк, Ю. И.\"],\"key\":\"__2008-5\",\"id\":\"__2008-5\",\"bibbaseid\":\"---------2008\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/9548\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Внутренние напряжения и деформационный фазовый переход в наноразмерных пленках титаната бария-стронция\",\"volume\":\"53\",\"issn\":\"0023-4761\",\"url\":\"https://www.elibrary.ru/item.asp?id=9955581\",\"abstract\":\"Установлено, что при изменении толщины гетероэпитаксиальных пленок Ba0.8Sr0.2TiO3, выращенных по слоевому механизму роста на подложках (100) MgO, существует критическая толщина пленок ( 50 нм), характерная тем, что внутренние деформационные поля в пленках толщиной ниже критической существенно меньше, чем в пленках толщиной выше критической. При толщине ниже критической имеют место напряжения растяжения, а при больших толщинах – напряжения сжатия. Существование критической толщины подтверждено рентгеноструктурными данными и рамановской спектроскопией.\",\"language\":\"ru\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Кристаллография\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Латуш\"],\"firstnames\":[\"Л.\",\"Т.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Жигалина\"],\"firstnames\":[\"О.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кускова\"],\"firstnames\":[\"А.\",\"Н.\"],\"suffixes\":[]}],\"year\":\"2008\",\"keywords\":\"⛔ No DOI found\",\"pages\":\"536–542\",\"bibtex\":\"@article{__2008-6,\\n\\ttitle = {Внутренние напряжения и деформационный фазовый переход в наноразмерных пленках титаната бария-стронция},\\n\\tvolume = {53},\\n\\tissn = {0023-4761},\\n\\turl = {https://www.elibrary.ru/item.asp?id=9955581},\\n\\tabstract = {Установлено, что при изменении толщины гетероэпитаксиальных пленок Ba0.8Sr0.2TiO3, выращенных по слоевому механизму роста на подложках (100) MgO, существует критическая толщина пленок ( 50 нм), характерная тем, что внутренние деформационные поля в пленках толщиной ниже критической существенно меньше, чем в пленках толщиной выше критической. При толщине ниже критической имеют место напряжения растяжения, а при больших толщинах – напряжения сжатия. Существование критической толщины подтверждено рентгеноструктурными данными и рамановской спектроскопией.},\\n\\tlanguage = {ru},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Кристаллография},\\n\\tauthor = {Мухортов, В. М. and Головко, Ю. И. and Юзюк, Ю. И. and Латуш, Л. Т. and Жигалина, О. М. and Кускова, А. Н.},\\n\\tyear = {2008},\\n\\tkeywords = {⛔ No DOI found},\\n\\tpages = {536--542},\\n}\\n\\n\",\"author_short\":[\"Мухортов, В. М.\",\"Головко, Ю. И.\",\"Юзюк, Ю. И.\",\"Латуш, Л. Т.\",\"Жигалина, О. М.\",\"Кускова, А. Н.\"],\"key\":\"__2008-6\",\"id\":\"__2008-6\",\"bibbaseid\":\"-------2008\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.elibrary.ru/item.asp?id=9955581\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"series\":\"Raman Spectroscopy Workshop 2006\",\"title\":\"Stress manipulation in ferroelectric thin films and superlattices\",\"volume\":\"45\",\"issn\":\"0924-2031\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0924203107000537\",\"doi\":\"10.1016/j.vibspec.2007.05.004\",\"abstract\":\"The integration of ferroelectric oxides into microelectronic devices requires a better understanding of stress and size effects onto ferroelectric properties of epitaxial thin films and superlattices which are generally imposed by the underlying substrate due to misfits in their lattice parameters and their thermal expansion coefficients. We have utilized polarized micro-Raman spectroscopy to investigate such stress effects in epitaxially grown Ba0.7Sr0.3TiO3 (BST-0.3) thin films and BaTiO3/SrTiO3 (BT/ST) superlattices with different periodicities as a function of temperature. In BST-0.3 films, the mismatch of the thermal expansion coefficients of the film and the substrate induces significant two-dimensional (2D) clamping and governs the domain structure formation. Moreover, the 2D stresses increase the Curie temperature remarkably and even change the phase-transition sequence in thin films, creating new phases, which were never observed in bulk materials. It is shown that in the epitaxial BST-0.3 films and BT/ST superlattices the E(TO) soft mode is very sensitive internal probe of 2D clamping and can be used for precise characterization.\",\"language\":\"en\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Vibrational Spectroscopy\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"R.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2007\",\"keywords\":\"Ferroelectrics, Raman spectroscopy, Superlattices\",\"pages\":\"108–111\",\"bibtex\":\"@article{katiyar_stress_2007,\\n\\tseries = {Raman {Spectroscopy} {Workshop} 2006},\\n\\ttitle = {Stress manipulation in ferroelectric thin films and superlattices},\\n\\tvolume = {45},\\n\\tissn = {0924-2031},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0924203107000537},\\n\\tdoi = {10.1016/j.vibspec.2007.05.004},\\n\\tabstract = {The integration of ferroelectric oxides into microelectronic devices requires a better understanding of stress and size effects onto ferroelectric properties of epitaxial thin films and superlattices which are generally imposed by the underlying substrate due to misfits in their lattice parameters and their thermal expansion coefficients. We have utilized polarized micro-Raman spectroscopy to investigate such stress effects in epitaxially grown Ba0.7Sr0.3TiO3 (BST-0.3) thin films and BaTiO3/SrTiO3 (BT/ST) superlattices with different periodicities as a function of temperature. In BST-0.3 films, the mismatch of the thermal expansion coefficients of the film and the substrate induces significant two-dimensional (2D) clamping and governs the domain structure formation. Moreover, the 2D stresses increase the Curie temperature remarkably and even change the phase-transition sequence in thin films, creating new phases, which were never observed in bulk materials. It is shown that in the epitaxial BST-0.3 films and BT/ST superlattices the E(TO) soft mode is very sensitive internal probe of 2D clamping and can be used for precise characterization.},\\n\\tlanguage = {en},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Vibrational Spectroscopy},\\n\\tauthor = {Katiyar, R. S. and Yuzyuk, Yu. I.},\\n\\tmonth = nov,\\n\\tyear = {2007},\\n\\tkeywords = {Ferroelectrics, Raman spectroscopy, Superlattices},\\n\\tpages = {108--111},\\n}\\n\\n\",\"author_short\":[\"Katiyar, R. S.\",\"Yuzyuk, Y. I.\"],\"key\":\"katiyar_stress_2007\",\"id\":\"katiyar_stress_2007\",\"bibbaseid\":\"katiyar-yuzyuk-stressmanipulationinferroelectricthinfilmsandsuperlattices-2007\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0924203107000537\"},\"keyword\":[\"Ferroelectrics\",\"Raman spectroscopy\",\"Superlattices\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Polarization Switching in Ferroelectric Thin Films Studied by Optical Second Harmonic Generation\",\"volume\":\"92\",\"issn\":\"1058-4587\",\"url\":\"https://doi.org/10.1080/10584580701746913\",\"doi\":\"10.1080/10584580701746913\",\"abstract\":\"Domain configuration during polarization switching in ferroelectric thin films was studied by optical second harmonic generation on different time scales: quasistatic (0.1 Hz), low-frequency (0.1–1 kHz) and fast (0.1 GHz). It is shown that within the electric pulses of several tenth of nanoseconds domain configuration may be different from the equilibrium.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Integrated Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Mishina\"],\"firstnames\":[\"Elena\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sherstyuk\"],\"firstnames\":[\"Nataliya\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golovko\"],\"firstnames\":[\"Yurii\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Muhortov\"],\"firstnames\":[\"Vladimir\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sigov\"],\"firstnames\":[\"Alexandr\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2007\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/10584580701746913\",\"pages\":\"65–76\",\"bibtex\":\"@article{mishina_polarization_2007,\\n\\ttitle = {Polarization {Switching} in {Ferroelectric} {Thin} {Films} {Studied} by {Optical} {Second} {Harmonic} {Generation}},\\n\\tvolume = {92},\\n\\tissn = {1058-4587},\\n\\turl = {https://doi.org/10.1080/10584580701746913},\\n\\tdoi = {10.1080/10584580701746913},\\n\\tabstract = {Domain configuration during polarization switching in ferroelectric thin films was studied by optical second harmonic generation on different time scales: quasistatic (0.1 Hz), low-frequency (0.1–1 kHz) and fast (0.1 GHz). It is shown that within the electric pulses of several tenth of nanoseconds domain configuration may be different from the equilibrium.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Integrated Ferroelectrics},\\n\\tauthor = {Mishina, Elena and Sherstyuk, Nataliya and Golovko, Yurii and Muhortov, Vladimir and Sigov, Alexandr},\\n\\tmonth = dec,\\n\\tyear = {2007},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/10584580701746913},\\n\\tpages = {65--76},\\n}\\n\\n\",\"author_short\":[\"Mishina, E.\",\"Sherstyuk, N.\",\"Golovko, Y.\",\"Muhortov, V.\",\"Sigov, A.\"],\"key\":\"mishina_polarization_2007\",\"id\":\"mishina_polarization_2007\",\"bibbaseid\":\"mishina-sherstyuk-golovko-muhortov-sigov-polarizationswitchinginferroelectricthinfilmsstudiedbyopticalsecondharmonicgeneration-2007\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/10584580701746913\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Phenomenological theory of phase transitions in epitaxial BaTiO$_{\\\\textrm{3}}$ thin films\",\"volume\":\"75\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.75.224116\",\"doi\":\"10.1103/PhysRevB.75.224116\",\"abstract\":\"We develop a phenomenological thermodynamic theory of ferroelectric BaTiO3 (BT) thin films epitaxially grown on cubic substrates using the Landau-Devonshire eight-order potential. The constructed “misfit-temperature” phase diagram is asymmetrical. We found that the overall view of the phase diagram depends on the values of compliances used in calculations and we provide two qualitatively different diagrams. A thermodynamic path for BT film grown onto a particular substrate can be found using a plot of the room-temperature tetragonal distortion (c−a)∕a as a function of misfit strain.\",\"language\":\"en\",\"number\":\"22\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dkhil\"],\"firstnames\":[\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lemanov\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2007\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"224116\",\"bibtex\":\"@article{shirokov_phenomenological_2007,\\n\\ttitle = {Phenomenological theory of phase transitions in epitaxial {BaTiO}$_{\\\\textrm{3}}$ thin films},\\n\\tvolume = {75},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.75.224116},\\n\\tdoi = {10.1103/PhysRevB.75.224116},\\n\\tabstract = {We develop a phenomenological thermodynamic theory of ferroelectric BaTiO3 (BT) thin films epitaxially grown on cubic substrates using the Landau-Devonshire eight-order potential. The constructed “misfit-temperature” phase diagram is asymmetrical. We found that the overall view of the phase diagram depends on the values of compliances used in calculations and we provide two qualitatively different diagrams. A thermodynamic path for BT film grown onto a particular substrate can be found using a plot of the room-temperature tetragonal distortion (c−a)∕a as a function of misfit strain.},\\n\\tlanguage = {en},\\n\\tnumber = {22},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Shirokov, V. B. and Yuzyuk, Yu. I. and Dkhil, B. and Lemanov, V. V.},\\n\\tmonth = jun,\\n\\tyear = {2007},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {224116},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Yuzyuk, Y. I.\",\"Dkhil, B.\",\"Lemanov, V. V.\"],\"key\":\"shirokov_phenomenological_2007\",\"id\":\"shirokov_phenomenological_2007\",\"bibbaseid\":\"shirokov-yuzyuk-dkhil-lemanov-phenomenologicaltheoryofphasetransitionsinepitaxialbatiotextrm3thinfilms-2007\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.75.224116\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Electron paramagnetic resonance in transition metal-doped ZnO nanowires\",\"volume\":\"101\",\"issn\":\"0021-8979\",\"url\":\"https://doi.org/10.1063/1.2402095\",\"doi\":\"10.1063/1.2402095\",\"abstract\":\"The wide-band-gap zinc oxide-based diluted magnetic semiconductors currently attract considerable attention due to their possible use in spintronic devices. In this work, we studied ZnO nanowire samples synthesized on 10×10 mm2 a-plane sapphire substrates by high-pressure pulsed laser deposition. The samples were characterized by scanning electron microscopy (SEM) and electron paramagnetic resonance (EPR) in the X-band (≃9.3 GHz) from T=4 to 300 K. According to the SEM pictures, the nanowires exhibit a length of about 1 μm and are aligned perpendicular to the substrate surface. The structures have a hexagonal cross section and their diameter ranges from 60 nm up to 150 nm. For the lowest nominal concentrations of xMn=3 at. % and xCo=5 at. %, we detect the anisotropic EPR spectra of isolated Mn2+ (3d5, S6) and Co2+ (3d7, F4), respectively, on Zn sites. The detection of the well-resolved anisotropic spectra proves a coherent crystallographic orientation of the nanowires. The linewidth was larger than the best values reported in the literature. Nevertheless, it was possible to identify two different components, A and B, of the reported spectra. From the temperature dependence of the EPR intensity, we found that both components exhibit paramagnetic behavior and are present in a concentration ratio of NB∕NA=1.4. In the case of the Mn-doped ZnO wires, the linewidth increases with increasing Mn concentration due to the dipole-dipole interaction of the paramagnetic ions. At the highest used nominal concentration, xMn=10 at. %, an additional broad single line is observed.\",\"language\":\"en\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Applied Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Ankiewicz\"],\"firstnames\":[\"A.\",\"O.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Carmo\"],\"firstnames\":[\"M.\",\"C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sobolev\"],\"firstnames\":[\"N.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gehlhoff\"],\"firstnames\":[\"W.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rahm\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2007\",\"pages\":\"024324\",\"bibtex\":\"@article{ankiewicz_electron_2007,\\n\\ttitle = {Electron paramagnetic resonance in transition metal-doped {ZnO} nanowires},\\n\\tvolume = {101},\\n\\tissn = {0021-8979},\\n\\turl = {https://doi.org/10.1063/1.2402095},\\n\\tdoi = {10.1063/1.2402095},\\n\\tabstract = {The wide-band-gap zinc oxide-based diluted magnetic semiconductors currently attract considerable attention due to their possible use in spintronic devices. In this work, we studied ZnO nanowire samples synthesized on 10×10 mm2 a-plane sapphire substrates by high-pressure pulsed laser deposition. The samples were characterized by scanning electron microscopy (SEM) and electron paramagnetic resonance (EPR) in the X-band (≃9.3 GHz) from T=4 to 300 K. According to the SEM pictures, the nanowires exhibit a length of about 1 μm and are aligned perpendicular to the substrate surface. The structures have a hexagonal cross section and their diameter ranges from 60 nm up to 150 nm. For the lowest nominal concentrations of xMn=3 at. \\\\% and xCo=5 at. \\\\%, we detect the anisotropic EPR spectra of isolated Mn2+ (3d5, S6) and Co2+ (3d7, F4), respectively, on Zn sites. The detection of the well-resolved anisotropic spectra proves a coherent crystallographic orientation of the nanowires. The linewidth was larger than the best values reported in the literature. Nevertheless, it was possible to identify two different components, A and B, of the reported spectra. From the temperature dependence of the EPR intensity, we found that both components exhibit paramagnetic behavior and are present in a concentration ratio of NB∕NA=1.4. In the case of the Mn-doped ZnO wires, the linewidth increases with increasing Mn concentration due to the dipole-dipole interaction of the paramagnetic ions. At the highest used nominal concentration, xMn=10 at. \\\\%, an additional broad single line is observed.},\\n\\tlanguage = {en},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Applied Physics},\\n\\tauthor = {Ankiewicz, A. O. and Carmo, M. C. and Sobolev, N. A. and Gehlhoff, W. and Kaidashev, E. M. and Rahm, A. and Lorenz, M. and Grundmann, M.},\\n\\tmonth = jan,\\n\\tyear = {2007},\\n\\tpages = {024324},\\n}\\n\\n\",\"author_short\":[\"Ankiewicz, A. O.\",\"Carmo, M. C.\",\"Sobolev, N. A.\",\"Gehlhoff, W.\",\"Kaidashev, E. M.\",\"Rahm, A.\",\"Lorenz, M.\",\"Grundmann, M.\"],\"key\":\"ankiewicz_electron_2007\",\"id\":\"ankiewicz_electron_2007\",\"bibbaseid\":\"ankiewicz-carmo-sobolev-gehlhoff-kaidashev-rahm-lorenz-grundmann-electronparamagneticresonanceintransitionmetaldopedznonanowires-2007\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.2402095\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Геометрические эффекты в наноразмерных эпитаксиальных пленках титаната бария-стронция\",\"volume\":\"77\",\"url\":\"https://journals.ioffe.ru/articles/9249\",\"abstract\":\"Исследованы наноразмерные (6−950 nm) эпитаксиальные пленки Ba0.8Sr0.2TiO3 на (001) MgO с целью изучения влияния толщины пленки на особенности проявления сегнетоэлектрических свойств. Данные комбинационного рассеяния света и рентгеновской дифрактометрии показывают, что при толщине пленки ∼ 70 nm происходит структурный фазовый переход, при котором резко изменяются параметры решетки пленки. Спектры комбинационного рассеяния света наноразмерных пленок подтвердили наличие в них сегне тоэлектрического состояния и изменение симметрии при переходе пленок через критическую толщину, что проявилось в резком смещении пиков, соответствующих A1 (TO) и E (TO) компонентам мягкой моды. В области толщины пленок \\\\textless 100 nm в зависимости диэлектрической проницаемости от толщины появляются два максимума при толщине ∼ 18 и ∼ 36 nm. Диэлектрическая нелинейность в области первого максимума существенно больше, чем в области второго.\",\"language\":\"ru\",\"number\":\"10\",\"urldate\":\"2023-11-11\",\"journal\":\"Журнал технической физики\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Колесников\"],\"firstnames\":[\"В.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бирюков\"],\"firstnames\":[\"С.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Маматов\"],\"firstnames\":[\"А.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]}],\"year\":\"2007\",\"keywords\":\"⛔ No DOI found\",\"pages\":\"97–102\",\"bibtex\":\"@article{__2007-1,\\n\\ttitle = {Геометрические эффекты в наноразмерных эпитаксиальных пленках титаната бария-стронция},\\n\\tvolume = {77},\\n\\turl = {https://journals.ioffe.ru/articles/9249},\\n\\tabstract = {Исследованы наноразмерные (6−950 nm) эпитаксиальные пленки Ba0.8Sr0.2TiO3 на (001) MgO с целью\\nизучения влияния толщины пленки на особенности проявления сегнетоэлектрических свойств. Данные\\nкомбинационного рассеяния света и рентгеновской дифрактометрии показывают, что при толщине пленки\\n∼ 70 nm происходит структурный фазовый переход, при котором резко изменяются параметры решетки\\nпленки.\\nСпектры комбинационного рассеяния света наноразмерных пленок подтвердили наличие в них сегне тоэлектрического состояния и изменение симметрии при переходе пленок через критическую толщину,\\nчто проявилось в резком смещении пиков, соответствующих A1 (TO) и E (TO) компонентам мягкой\\nмоды. В области толщины пленок {\\\\textless} 100 nm в зависимости диэлектрической проницаемости от толщины\\nпоявляются два максимума при толщине ∼ 18 и ∼ 36 nm. Диэлектрическая нелинейность в области первого\\nмаксимума существенно больше, чем в области второго.},\\n\\tlanguage = {ru},\\n\\tnumber = {10},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Журнал технической физики},\\n\\tauthor = {Мухортов, В. М. and Колесников, В. В. and Головко, Ю. И. and Бирюков, С. В. and Маматов, А. А. and Юзюк, Ю. И.},\\n\\tyear = {2007},\\n\\tkeywords = {⛔ No DOI found},\\n\\tpages = {97--102},\\n}\\n\\n\",\"author_short\":[\"Мухортов, В. М.\",\"Колесников, В. В.\",\"Головко, Ю. И.\",\"Бирюков, С. В.\",\"Маматов, А. А.\",\"Юзюк, Ю. И.\"],\"key\":\"__2007-1\",\"id\":\"__2007-1\",\"bibbaseid\":\"-------2007\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/9249\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Влияние механизма роста и термоупругих напряжений на динамику кристаллической решетки гетероэпитаксиальных пленок титаната бария-стронция\",\"volume\":\"49\",\"url\":\"https://journals.ioffe.ru/articles/3167\",\"language\":\"ru\",\"number\":\"9\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Захарченко\"],\"firstnames\":[\"И.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Алёшин\"],\"firstnames\":[\"В.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Леонтьев\"],\"firstnames\":[\"И.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Рабкин\"],\"firstnames\":[\"Л.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Simon\"],\"firstnames\":[\"P.\"],\"suffixes\":[]}],\"year\":\"2007\",\"keywords\":\"⛔ No DOI found\",\"pages\":\"1676–1682\",\"bibtex\":\"@article{__2007-2,\\n\\ttitle = {Влияние механизма роста и термоупругих напряжений на динамику кристаллической решетки гетероэпитаксиальных пленок титаната бария-стронция},\\n\\tvolume = {49},\\n\\turl = {https://journals.ioffe.ru/articles/3167},\\n\\tlanguage = {ru},\\n\\tnumber = {9},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Юзюк, Ю. И. and Захарченко, И. Н. and Алёшин, В. А. and Леонтьев, И. Н. and Рабкин, Л. М. and Мухортов, В. М. and Simon, P.},\\n\\tyear = {2007},\\n\\tkeywords = {⛔ No DOI found},\\n\\tpages = {1676--1682},\\n}\\n\\n\",\"author_short\":[\"Юзюк, Ю. И.\",\"Захарченко, И. Н.\",\"Алёшин, В. А.\",\"Леонтьев, И. Н.\",\"Рабкин, Л. М.\",\"Мухортов, В. М.\",\"Simon, P.\"],\"key\":\"__2007-2\",\"id\":\"__2007-2\",\"bibbaseid\":\"------simon--2007\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/3167\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"series\":\"Proceedings of the International Conference on Materials for Advanced Technologies (ICMAT 2005) Symposium N\",\"title\":\"Optical phonon modes in ZnO nanorods on Si prepared by pulsed laser deposition\",\"volume\":\"287\",\"issn\":\"0022-0248\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0022024805011619\",\"doi\":\"10.1016/j.jcrysgro.2005.10.039\",\"abstract\":\"An array of vertically aligned c-axis-oriented zinc oxide (ZnO) nanorods were fabricated at a low substrate temperature (500°C) without using any catalytic template on the Si substrate by pulsed laser deposition at a high pressure (1–5Torr). The successive deposition of ZnO nanoparticles one over the other during growth led to the formation of elongated and well-isolated nanorods with a diameter in the range 70–350nm and up to 14μm long. The influence of deposition parameters on the Raman phonon modes was investigated. The polarized Raman studies were carried out in the backward geometry with incident light (i) parallel and (ii) perpendicular to the nanorod length. The activation of lower and upper surface phonon modes were observed in the ZnO nanorods between the transverse optical (ωTO) and the longitudinal optical (ωLO) phonon frequencies. The lower surface mode observed at ∼475cm−1 is found to be predominant in the X(ZZ)X¯ configuration. The surface phonon modes were not found in the samples prepared at \\\\textgreater600°C due to the coalescence process resulting in a continuous film. The agreement of polarized Raman spectra with single crystal data indicates the growth of good quality ZnO nanorods, and allows direct integration on Si without introducing contamination at the interface due to any catalytic material.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Crystal Growth\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Gupta\"],\"firstnames\":[\"Vinay\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bhattacharya\"],\"firstnames\":[\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sreenivas\"],\"firstnames\":[\"K.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"R.\",\"S.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2006\",\"keywords\":\"A1. axis orientation, A1. Nanorods, A1. Raman scattering, A1. Surface phonon mode, A3. PLD, B2. Zinc oxide\",\"pages\":\"39–43\",\"file\":\"ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\R̋85BTQK\\\\§0022024805011619.html:text/html\",\"bibtex\":\"@article{gupta_optical_2006,\\n\\tseries = {Proceedings of the {International} {Conference} on {Materials} for {Advanced} {Technologies} ({ICMAT} 2005) {Symposium} {N}},\\n\\ttitle = {Optical phonon modes in {ZnO} nanorods on {Si} prepared by pulsed laser deposition},\\n\\tvolume = {287},\\n\\tissn = {0022-0248},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0022024805011619},\\n\\tdoi = {10.1016/j.jcrysgro.2005.10.039},\\n\\tabstract = {An array of vertically aligned c-axis-oriented zinc oxide (ZnO) nanorods were fabricated at a low substrate temperature (500°C) without using any catalytic template on the Si substrate by pulsed laser deposition at a high pressure (1–5Torr). The successive deposition of ZnO nanoparticles one over the other during growth led to the formation of elongated and well-isolated nanorods with a diameter in the range 70–350nm and up to 14μm long. The influence of deposition parameters on the Raman phonon modes was investigated. The polarized Raman studies were carried out in the backward geometry with incident light (i) parallel and (ii) perpendicular to the nanorod length. The activation of lower and upper surface phonon modes were observed in the ZnO nanorods between the transverse optical (ωTO) and the longitudinal optical (ωLO) phonon frequencies. The lower surface mode observed at ∼475cm−1 is found to be predominant in the X(ZZ)X¯ configuration. The surface phonon modes were not found in the samples prepared at {\\\\textgreater}600°C due to the coalescence process resulting in a continuous film. The agreement of polarized Raman spectra with single crystal data indicates the growth of good quality ZnO nanorods, and allows direct integration on Si without introducing contamination at the interface due to any catalytic material.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Crystal Growth},\\n\\tauthor = {Gupta, Vinay and Bhattacharya, P. and Yuzuk, Yu. I. and Sreenivas, K. and Katiyar, R. S.},\\n\\tmonth = jan,\\n\\tyear = {2006},\\n\\tkeywords = {A1. axis orientation, A1. Nanorods, A1. Raman scattering, A1. Surface phonon mode, A3. PLD, B2. Zinc oxide},\\n\\tpages = {39--43},\\n\\tfile = {ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\HR85BTQK\\\\\\\\S0022024805011619.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Gupta, V.\",\"Bhattacharya, P.\",\"Yuzuk, Y. I.\",\"Sreenivas, K.\",\"Katiyar, R. S.\"],\"key\":\"gupta_optical_2006\",\"id\":\"gupta_optical_2006\",\"bibbaseid\":\"gupta-bhattacharya-yuzuk-sreenivas-katiyar-opticalphononmodesinznonanorodsonsipreparedbypulsedlaserdeposition-2006\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0022024805011619\"},\"keyword\":[\"A1. axis orientation\",\"A1. Nanorods\",\"A1. Raman scattering\",\"A1. Surface phonon mode\",\"A3. PLD\",\"B2. Zinc oxide\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Ротационно-полярные структурные искажения в твердых растворах Pb$_{\\\\textrm{1-x}}$Ca$_{\\\\textrm{x}}$TiO$_{\\\\textrm{3}}$ на основе данных спектроскопии комбинационного рассеяния света\",\"volume\":\"48\",\"url\":\"https://journals.ioffe.ru/articles/3406\",\"abstract\":\"При проведении высокотемпературных (290−560 K) исследований поляризованных спектров комбинаци онного рассеяния света в области частот 6 \\\\textlessν\\\\textless 1200 cm−1 на монокристаллическом образце твердого раствора Pb0.55Ca0.45TiO3 установлено существование трех особых температурных точек, по крайней мере в двух из которых происходят структурные фазовые переходы. В рамках теории Ландау фазовых переходов второго рода обсуждается допустимая топология фазовых диаграмм, качественно верно отражающая экспериментальную ситуацию.\",\"language\":\"ru\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Торгашев\"],\"firstnames\":[\"В.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Леманов\"],\"firstnames\":[\"В.\",\"В.\"],\"suffixes\":[]}],\"year\":\"2006\",\"keywords\":\"⛔ No DOI found\",\"pages\":\"864–873\",\"bibtex\":\"@article{_-_2006,\\n\\ttitle = {Ротационно-полярные структурные искажения в твердых растворах {Pb}$_{\\\\textrm{1-x}}${Ca}$_{\\\\textrm{x}}${TiO}$_{\\\\textrm{3}}$ на основе данных спектроскопии комбинационного рассеяния света},\\n\\tvolume = {48},\\n\\turl = {https://journals.ioffe.ru/articles/3406},\\n\\tabstract = {При проведении высокотемпературных (290−560 K) исследований поляризованных спектров комбинаци онного рассеяния света в области частот 6 {\\\\textless}ν{\\\\textless} 1200 cm−1 на монокристаллическом образце твердого\\nраствора Pb0.55Ca0.45TiO3 установлено существование трех особых температурных точек, по крайней мере\\nв двух из которых происходят структурные фазовые переходы. В рамках теории Ландау фазовых переходов\\nвторого рода обсуждается допустимая топология фазовых диаграмм, качественно верно отражающая\\nэкспериментальную ситуацию.},\\n\\tlanguage = {ru},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Торгашев, В. И. and Юзюк, Ю. И. and Широков, В. Б. and Леманов, В. В.},\\n\\tyear = {2006},\\n\\tkeywords = {⛔ No DOI found},\\n\\tpages = {864--873},\\n}\\n\\n\",\"author_short\":[\"Торгашев, В. И.\",\"Юзюк, Ю. И.\",\"Широков, В. Б.\",\"Леманов, В. В.\"],\"key\":\"_-_2006\",\"id\":\"_-_2006\",\"bibbaseid\":\"----pbtextrm1xcatextrmxtiotextrm3-2006\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/3406\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Концентрационный фазовый переход в твердых растворах Pb$_{\\\\textrm{1-x}}$Ca$_{\\\\textrm{x}}$TiO$_{\\\\textrm{3}}$ по данным спектроскопии комбинационного рассеяния света\",\"volume\":\"48\",\"url\":\"https://journals.ioffe.ru/articles/3382\",\"abstract\":\"Впервые на монокристаллических образцах твердых перовскитных растворов Pb1−xCaxTiO3 (составы: x = 0, 0.03, 0.04, 0.15, 0.23, 0.28, 0.34, 0.38, 0.40, 0.45 и 0.50) получены поляризованные спектры комбинационного рассеяния света и ИК отражения в области частот 6 \\\\textlessν\\\\textless 1200 cm−1 и температурах 290–620 K. Основное внимание уделено низкочастотной динамике решетки, где установлено аномальное концентрационное поведение фононного спектрального отклика при 0.38 \\\\textless x \\\\textless 0.40. При комнатной температуре в области x \\\\textgreater 0.40 в твердых растворах Pb1−xCaxTiO3 реализуется новое фазовое состояние, которое, вероятно, является полярным\",\"language\":\"ru\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Торгашев\"],\"firstnames\":[\"В.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Леманов\"],\"firstnames\":[\"В.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kuntscher\"],\"firstnames\":[\"C.\",\"A.\"],\"suffixes\":[]}],\"year\":\"2006\",\"keywords\":\"⛔ No DOI found\",\"pages\":\"717–725\",\"bibtex\":\"@article{__2006-1,\\n\\ttitle = {Концентрационный фазовый переход в твердых растворах {Pb}$_{\\\\textrm{1-x}}${Ca}$_{\\\\textrm{x}}${TiO}$_{\\\\textrm{3}}$ по данным спектроскопии комбинационного рассеяния света},\\n\\tvolume = {48},\\n\\turl = {https://journals.ioffe.ru/articles/3382},\\n\\tabstract = {Впервые на монокристаллических образцах твердых перовскитных растворов Pb1−xCaxTiO3 (составы:\\nx = 0, 0.03, 0.04, 0.15, 0.23, 0.28, 0.34, 0.38, 0.40, 0.45 и 0.50) получены поляризованные спектры\\nкомбинационного рассеяния света и ИК отражения в области частот 6 {\\\\textless}ν{\\\\textless} 1200 cm−1 и температурах\\n290–620 K. Основное внимание уделено низкочастотной динамике решетки, где установлено аномальное\\nконцентрационное поведение фононного спектрального отклика при 0.38 {\\\\textless} x {\\\\textless} 0.40. При комнатной\\nтемпературе в области x {\\\\textgreater} 0.40 в твердых растворах Pb1−xCaxTiO3 реализуется новое фазовое состояние,\\nкоторое, вероятно, является полярным},\\n\\tlanguage = {ru},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Торгашев, В. И. and Юзюк, Ю. И. and Леманов, В. В. and Kuntscher, C. A.},\\n\\tyear = {2006},\\n\\tkeywords = {⛔ No DOI found},\\n\\tpages = {717--725},\\n}\\n\\n\",\"author_short\":[\"Торгашев, В. И.\",\"Юзюк, Ю. И.\",\"Леманов, В. В.\",\"Kuntscher, C. A.\"],\"key\":\"__2006-1\",\"id\":\"__2006-1\",\"bibbaseid\":\"---kuntscher-pbtextrm1xcatextrmxtiotextrm3-2006\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/3382\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Оптические свойства фотонных кристаллов на основе наностержней оксида цинка, покрытых тонкой пленкой плазмонного материала\",\"volume\":\"1\",\"url\":\"https://elibrary.ru/item.asp?id=39539483\",\"abstract\":\"В данной работе исследовались зависимости оптических свойств фотонных кристаллов, представляющих двумерно-периодическую решетку наностержней оксида цинка от геометрических параметров и типов их тонкопленочного покрытия плазмонными материалами (Au, Ag, Cu, AZO, GZO, AGZO и т. п.). В расчетах учтены свойства металлов и диэлектриков в оптическом диапазоне. Характеристики двухмерно-периодических структур, образованных бесконечно длинными слоистыми цилиндрами на основе ZnO, рассчитаны методом разделения переменных в цилиндрической системе координат. Проведено сравнение полученных численных данных с результатами конечноэлементного моделирования.\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"journal\":\"Электроника И Микроэлектроника Свч\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Лерер\"],\"firstnames\":[\"А.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Тимошенко\"],\"firstnames\":[\"П.\",\"Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головачева\"],\"firstnames\":[\"Е.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Турчин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]}],\"year\":\"2019\",\"keywords\":\"Дифракция, Наностержни, Оксид Цинка, Оптические Наноантенны, Оптические Свойства, Плазмон-Поляритон, Плазмонный Резонанс, Фотонная Запрещенная Зона, Фотонный Кристалл, ⛔ No DOI found\",\"pages\":\"209–213\",\"bibtex\":\"@article{__2019-2,\\n\\ttitle = {Оптические свойства фотонных кристаллов на основе наностержней оксида цинка, покрытых тонкой пленкой плазмонного материала},\\n\\tvolume = {1},\\n\\turl = {https://elibrary.ru/item.asp?id=39539483},\\n\\tabstract = {В данной работе исследовались зависимости оптических свойств фотонных кристаллов, представляющих двумерно-периодическую решетку наностержней оксида цинка от геометрических параметров и типов их тонкопленочного покрытия плазмонными материалами (Au, Ag, Cu, AZO, GZO, AGZO и т. п.). В расчетах учтены свойства металлов и диэлектриков в оптическом диапазоне. Характеристики двухмерно-периодических структур, образованных бесконечно длинными слоистыми цилиндрами на основе ZnO, рассчитаны методом разделения переменных в цилиндрической системе координат. Проведено сравнение полученных численных данных с результатами конечноэлементного моделирования.},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Электроника И Микроэлектроника Свч},\\n\\tauthor = {Лерер, А. М. and Тимошенко, П. Е. and Головачева, Е. В. and Кайдашев, Е. М. and Турчин, А. С.},\\n\\tyear = {2019},\\n\\tkeywords = {Дифракция, Наностержни, Оксид Цинка, Оптические Наноантенны, Оптические Свойства, Плазмон-Поляритон, Плазмонный Резонанс, Фотонная Запрещенная Зона, Фотонный Кристалл, ⛔ No DOI found},\\n\\tpages = {209--213},\\n}\\n\\n\",\"author_short\":[\"Лерер, А. М.\",\"Тимошенко, П. Е.\",\"Головачева, Е. В.\",\"Кайдашев, Е. М.\",\"Турчин, А. С.\"],\"key\":\"__2019-2\",\"id\":\"__2019-2\",\"bibbaseid\":\"------2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=39539483\"},\"keyword\":[\"Дифракция\",\"Наностержни\",\"Оксид Цинка\",\"Оптические Наноантенны\",\"Оптические Свойства\",\"Плазмон-Поляритон\",\"Плазмонный Резонанс\",\"Фотонная Запрещенная Зона\",\"Фотонный Кристалл\",\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{\"li, h\":\"https://lihuixidian.github.io/\"}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Уникальный атомный порядок гиперкагоме в геометрически фрустрированных иридиевых шпинелеподобных структурах\",\"issn\":\"1026-3500, 2658-784X\",\"url\":\"https://elibrary.ru/item.asp?id=30304556\",\"abstract\":\"Представлен краткий авторский обзор результатов теоретического исследования уникального атомного и орбитального порядка гиперкагоме в геометрически фрустрированных иридиевых шпинелеподобных структурах. Установлен структурный механизм образования атомного порядка гиперкагоме. Показано, что фундаментальной структурной особенностью иридиевых шпинелеподобных структур является существование замкнутых контуров химических связей Ir-Ir, каждый из которых состоит из десяти атомов - декагонов. Высказано предположение, что декагоны обусловливают аномальные химические и физические свойства кристаллов. Сделан прогноз структурных типов кристаллов, в которых может существовать атомный порядок гиперкагоме.\",\"language\":\"ru\",\"number\":\"10\",\"urldate\":\"2023-11-11\",\"journal\":\"Известия Академии Наук. Серия Химическая\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Таланов\"],\"firstnames\":[\"М.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Таланов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]}],\"year\":\"2017\",\"keywords\":\"Геометрическая Фрустрация, Декагоны, Порядок Гиперкагоме, Упорядоченные Шпинели, ⛔ No DOI found\",\"pages\":\"1719–1727\",\"bibtex\":\"@article{__2017-3,\\n\\ttitle = {Уникальный атомный порядок гиперкагоме в геометрически фрустрированных иридиевых шпинелеподобных структурах},\\n\\tissn = {1026-3500, 2658-784X},\\n\\turl = {https://elibrary.ru/item.asp?id=30304556},\\n\\tabstract = {Представлен краткий авторский обзор результатов теоретического исследования уникального атомного и орбитального порядка гиперкагоме в геометрически фрустрированных иридиевых шпинелеподобных структурах. Установлен структурный механизм образования атомного порядка гиперкагоме. Показано, что фундаментальной структурной особенностью иридиевых шпинелеподобных структур является существование замкнутых контуров химических связей Ir-Ir, каждый из которых состоит из десяти атомов - декагонов. Высказано предположение, что декагоны обусловливают аномальные химические и физические свойства кристаллов. Сделан прогноз структурных типов кристаллов, в которых может существовать атомный порядок гиперкагоме.},\\n\\tlanguage = {ru},\\n\\tnumber = {10},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Известия Академии Наук. Серия Химическая},\\n\\tauthor = {Таланов, М. В. and Таланов, В. М. and Широков, В. Б.},\\n\\tyear = {2017},\\n\\tkeywords = {Геометрическая Фрустрация, Декагоны, Порядок Гиперкагоме, Упорядоченные Шпинели, ⛔ No DOI found},\\n\\tpages = {1719--1727},\\n}\\n\\n\",\"author_short\":[\"Таланов, М. В.\",\"Таланов, В. М.\",\"Широков, В. Б.\"],\"key\":\"__2017-3\",\"id\":\"__2017-3\",\"bibbaseid\":\"----2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=30304556\"},\"keyword\":[\"Геометрическая Фрустрация\",\"Декагоны\",\"Порядок Гиперкагоме\",\"Упорядоченные Шпинели\",\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"downloads\":8,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Конечно-элементное моделирование в динамических задачах для упругих решеток микро- и нанокристаллов из оксида цинка\",\"volume\":\"2\",\"issn\":\"1813-4289\",\"url\":\"https://www.elibrary.ru/item.asp?id=12884469\",\"abstract\":\"Представлены результаты конечно-элементного моделирования процессов деформирования решетки нано- и микрокристаллов из оксида цинка. В рамках плоской теории электроупругости рассмотрены свободные и вынужденные колебания, а также нестационарные задачи для решетки микро- или нанокристаллов из оксида цинка, расположенных на подложке сапфира. Определены собственные частоты для системы решетка кристаллов - подложка, показано, что по найденному спектру большой системы (решетка - подложка) и спектру подложки можно определить первые собственные частоты одного нанокристалла. Это позволяет по экспериментальным данным для больших систем определить собственные частоты нанообъекта, которые непосредственно трудно определить другим способом. Знание собственных частот позволяет, в частности, судить о механических свойствах нанокристалла. Обсуждается возможность использования решеток нанокристаллов в качестве элементов наносенсоров.\",\"language\":\"ru\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Вестник Южного Научного Центра Ран\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Еремеев\"],\"firstnames\":[\"В.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Соловьев\"],\"firstnames\":[\"А.\",\"Н.\"],\"suffixes\":[]}],\"year\":\"2006\",\"keywords\":\"⛔ No DOI found\",\"pages\":\"10–15\",\"bibtex\":\"@article{_-_2006-1,\\n\\ttitle = {Конечно-элементное моделирование в динамических задачах для упругих решеток микро- и нанокристаллов из оксида цинка},\\n\\tvolume = {2},\\n\\tissn = {1813-4289},\\n\\turl = {https://www.elibrary.ru/item.asp?id=12884469},\\n\\tabstract = {Представлены результаты конечно-элементного моделирования процессов деформирования решетки нано- и микрокристаллов из оксида цинка. В рамках плоской теории электроупругости рассмотрены свободные и вынужденные колебания, а также нестационарные задачи для решетки микро- или нанокристаллов из оксида цинка, расположенных на подложке сапфира. Определены собственные частоты для системы решетка кристаллов - подложка, показано, что по найденному спектру большой системы (решетка - подложка) и спектру подложки можно определить первые собственные частоты одного нанокристалла. Это позволяет по экспериментальным данным для больших систем определить собственные частоты нанообъекта, которые непосредственно трудно определить другим способом. Знание собственных частот позволяет, в частности, судить о механических свойствах нанокристалла. Обсуждается возможность использования решеток нанокристаллов в качестве элементов наносенсоров.},\\n\\tlanguage = {ru},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Вестник Южного Научного Центра Ран},\\n\\tauthor = {Еремеев, В. А. and Кайдашев, Е. М. and Соловьев, А. Н.},\\n\\tyear = {2006},\\n\\tkeywords = {⛔ No DOI found},\\n\\tpages = {10--15},\\n}\\n\\n\",\"author_short\":[\"Еремеев, В. А.\",\"Кайдашев, Е. М.\",\"Соловьев, А. Н.\"],\"key\":\"_-_2006-1\",\"id\":\"_-_2006-1\",\"bibbaseid\":\"----2006\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.elibrary.ru/item.asp?id=12884469\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Влияние барьерных веществ на магниторезистивные свойства композитов на основе манганита лантана стронция\",\"issn\":\"2073-8633\",\"url\":\"https://elibrary.ru/item.asp?id=29911660\",\"abstract\":\"Based on our own, as well as literary experimental data, the analysis of the Influence of a barrier material used to create heterogeneous composites based on La0.7Sr0.3MnO3 on their magnetoresistive properties is carried out. Such composites differ in existence of an isotropic negative magnitorezistivnost (MR) connected from backs - dependent tunneling of carriers in magnetic field. The largest value MR up to 15% in the field of 15 kOe are shown when using glass-like GeO2 oxide at a percolation ratio of components.\",\"language\":\"ru\",\"number\":\"2 (45)\",\"urldate\":\"2023-11-11\",\"journal\":\"Инженерный Вестник Дона\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Кабиров\"],\"firstnames\":[\"Ю.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гавриляченко\"],\"firstnames\":[\"В.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Богатин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Чебанова\"],\"firstnames\":[\"Е.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Пруцакова\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Русакова\"],\"firstnames\":[\"Е.\",\"Б.\"],\"suffixes\":[]}],\"year\":\"2017\",\"keywords\":\"Барьерный Слой, Диэлектрическая Проницаемость, Керамика, Композитный Материал, Магниторезистивность, Манганит Лантана Стронция, Одношаговый Синтез, Порог Перколяции, Спиновая Поляризация, Туннелирование, ⛔ No DOI found\",\"pages\":\"4\",\"bibtex\":\"@article{__2017-4,\\n\\ttitle = {Влияние барьерных веществ на магниторезистивные свойства композитов на основе манганита лантана стронция},\\n\\tissn = {2073-8633},\\n\\turl = {https://elibrary.ru/item.asp?id=29911660},\\n\\tabstract = {Based on our own, as well as literary experimental data, the analysis of the Influence of a barrier material used to create heterogeneous composites based on La0.7Sr0.3MnO3 on their magnetoresistive properties is carried out. Such composites differ in existence of an isotropic negative magnitorezistivnost (MR) connected from backs - dependent tunneling of carriers in magnetic field. The largest value MR up to 15\\\\% in the field of 15 kOe are shown when using glass-like GeO2 oxide at a percolation ratio of components.},\\n\\tlanguage = {ru},\\n\\tnumber = {2 (45)},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Инженерный Вестник Дона},\\n\\tauthor = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Богатин, А. С. and Чебанова, Е. В. and Пруцакова, Н. В. and Русакова, Е. Б.},\\n\\tyear = {2017},\\n\\tkeywords = {Барьерный Слой, Диэлектрическая Проницаемость, Керамика, Композитный Материал, Магниторезистивность, Манганит Лантана Стронция, Одношаговый Синтез, Порог Перколяции, Спиновая Поляризация, Туннелирование, ⛔ No DOI found},\\n\\tpages = {4},\\n}\\n\\n\",\"author_short\":[\"Кабиров, Ю. В.\",\"Гавриляченко, В. Г.\",\"Богатин, А. С.\",\"Чебанова, Е. В.\",\"Пруцакова, Н. В.\",\"Русакова, Е. Б.\"],\"key\":\"__2017-4\",\"id\":\"__2017-4\",\"bibbaseid\":\"-------2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=29911660\"},\"keyword\":[\"Барьерный Слой\",\"Диэлектрическая Проницаемость\",\"Керамика\",\"Композитный Материал\",\"Магниторезистивность\",\"Манганит Лантана Стронция\",\"Одношаговый Синтез\",\"Порог Перколяции\",\"Спиновая Поляризация\",\"Туннелирование\",\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{\"li, h\":\"https://lihuixidian.github.io/\"}},\"downloads\":1,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Гетероэпитаксиальные плёнки мультиферроика феррита висмута, допированного неодимом\",\"volume\":\"179\",\"issn\":\"0042-1294\",\"url\":\"https://ufn.ru/ru/articles/2009/8/k/\",\"abstract\":\"Гетероэпитаксиальные плёнки мультиферроика феррита висмута, допированного неодимом, Мухортов В.М., Головко Ю.И., Юзюк Ю.И.\",\"language\":\"ru\",\"number\":\"8\",\"urldate\":\"2023-11-11\",\"journal\":\"Успехи физических наук\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2009\",\"keywords\":\"⛔ No DOI found\",\"pages\":\"909–913\",\"file\":\"Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\2X6KHVNX\\\\\\\\Мухортов и др. - 2009 - Гетероэпитаксиальные плёнки мультиферроика феррита.pdf:application/pdf\",\"bibtex\":\"@article{__2009-4,\\n\\ttitle = {Гетероэпитаксиальные плёнки мультиферроика феррита висмута, допированного неодимом},\\n\\tvolume = {179},\\n\\tissn = {0042-1294},\\n\\turl = {https://ufn.ru/ru/articles/2009/8/k/},\\n\\tabstract = {Гетероэпитаксиальные плёнки мультиферроика феррита висмута, допированного неодимом, Мухортов В.М., Головко Ю.И., Юзюк Ю.И.},\\n\\tlanguage = {ru},\\n\\tnumber = {8},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Успехи физических наук},\\n\\tauthor = {Мухортов, В. М. and Головко, Ю. И. and Юзюк, Ю. И.},\\n\\tmonth = aug,\\n\\tyear = {2009},\\n\\tkeywords = {⛔ No DOI found},\\n\\tpages = {909--913},\\n\\tfile = {Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\2X6KHVNX\\\\\\\\Мухортов и др. - 2009 - Гетероэпитаксиальные плёнки мультиферроика феррита.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Мухортов, В. М.\",\"Головко, Ю. И.\",\"Юзюк, Ю. И.\"],\"key\":\"__2009-4\",\"id\":\"__2009-4\",\"bibbaseid\":\"----2009\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://ufn.ru/ru/articles/2009/8/k/\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Оптические наноантенны на новых плазмонных материалах на основе оксида цинка\",\"volume\":\"1\",\"url\":\"https://elibrary.ru/item.asp?id=26607463\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"journal\":\"Электроника И Микроэлектроника Свч\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Лерер\"],\"firstnames\":[\"А.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Тимошенко\"],\"firstnames\":[\"П.\",\"Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головачева\"],\"firstnames\":[\"Е.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Пузанов\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]}],\"year\":\"2016\",\"keywords\":\"Дифракция, Оптические Наноантенны, Конечно-Элементное Моделирование, Фотонно-Кристаллические Структуры, Zno Наностержни, ⛔ No DOI found\",\"pages\":\"279–282\",\"bibtex\":\"@article{__2016-1,\\n\\ttitle = {Оптические наноантенны на новых плазмонных материалах на основе оксида цинка},\\n\\tvolume = {1},\\n\\turl = {https://elibrary.ru/item.asp?id=26607463},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Электроника И Микроэлектроника Свч},\\n\\tauthor = {Лерер, А. М. and Тимошенко, П. Е. and Головачева, Е. В. and Кайдашев, Е. М. and Пузанов, А. С.},\\n\\tyear = {2016},\\n\\tkeywords = {Дифракция, Оптические Наноантенны, Конечно-Элементное Моделирование, Фотонно-Кристаллические Структуры, Zno Наностержни, ⛔ No DOI found},\\n\\tpages = {279--282},\\n}\\n\\n\",\"author_short\":[\"Лерер, А. М.\",\"Тимошенко, П. Е.\",\"Головачева, Е. В.\",\"Кайдашев, Е. М.\",\"Пузанов, А. С.\"],\"key\":\"__2016-1\",\"id\":\"__2016-1\",\"bibbaseid\":\"------2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=26607463\"},\"keyword\":[\"Дифракция\",\"Оптические Наноантенны\",\"Конечно-Элементное Моделирование\",\"Фотонно-Кристаллические Структуры\",\"Zno Наностержни\",\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Особенности динамики переключения поляризации в тонких пленках цирконата–титаната–свинца\",\"volume\":\"75\",\"url\":\"https://journals.ioffe.ru/articles/viewPDF/8639\",\"number\":\"5\",\"journal\":\"Журнал технической физики\",\"author\":[{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Мухортов В.М.\"],\"suffixes\":[]},{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Колесников В.В.\"],\"suffixes\":[]},{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Головко Ю.И.\"],\"suffixes\":[]},{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Мащенко А.И.\"],\"suffixes\":[]},{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Бирюков С.В.\"],\"suffixes\":[]}],\"year\":\"2005\",\"keywords\":\"⛔ No DOI found\",\"pages\":\"126–131\",\"bibtex\":\"@article{___2005,\\n\\ttitle = {Особенности динамики переключения поляризации в тонких пленках цирконата–титаната–свинца},\\n\\tvolume = {75},\\n\\turl = {https://journals.ioffe.ru/articles/viewPDF/8639},\\n\\tnumber = {5},\\n\\tjournal = {Журнал технической физики},\\n\\tauthor = {{Мухортов В.М.} and {Колесников В.В.} and {Головко Ю.И.} and {Мащенко А.И.} and {Бирюков С.В.}},\\n\\tyear = {2005},\\n\\tkeywords = {⛔ No DOI found},\\n\\tpages = {126--131},\\n}\\n\\n\",\"author_short\":[\"Мухортов В.М.\",\"Колесников В.В.\",\"Головко Ю.И.\",\"Мащенко А.И.\",\"Бирюков С.В.\"],\"key\":\"___2005\",\"id\":\"___2005\",\"bibbaseid\":\"------2005\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/viewPDF/8639\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Магнитоэлектрические и нелинейно-оптические свойства пленок BiFeO$_{\\\\textrm{3}}$, допированных неодимом\",\"issn\":\"1813-8586\",\"url\":\"https://www.elibrary.ru/item.asp?id=11693334\",\"abstract\":\"Методом магнетронного распыления получены мо-нокристаллические и поликристаллические пленки фер-рита висмута. Показано, что монокристаллические пленки обладают высокими значениями остаточной по-ляризации и намагниченности насыщения. Наличие маг-нитоэлектрического взаимодействия подтверждено нели-нейно-оптическими измерениями.\",\"language\":\"ru\",\"number\":\"12\",\"urldate\":\"2023-11-11\",\"journal\":\"Нано- И Микросистемная Техника\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Кузнецов\"],\"firstnames\":[\"М.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мишина\"],\"firstnames\":[\"Е.\",\"Д.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Морозов\"],\"firstnames\":[\"А.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Сигов\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мошняга\"],\"firstnames\":[\"В.\",\"Т.\"],\"suffixes\":[]}],\"year\":\"2007\",\"keywords\":\"⛔ No DOI found\",\"pages\":\"20–22\",\"bibtex\":\"@article{__2007-3,\\n\\ttitle = {Магнитоэлектрические и нелинейно-оптические свойства пленок {BiFeO}$_{\\\\textrm{3}}$, допированных неодимом},\\n\\tissn = {1813-8586},\\n\\turl = {https://www.elibrary.ru/item.asp?id=11693334},\\n\\tabstract = {Методом магнетронного распыления получены мо-нокристаллические и поликристаллические пленки фер-рита висмута. Показано, что монокристаллические пленки обладают высокими значениями остаточной по-ляризации и намагниченности насыщения. Наличие маг-нитоэлектрического взаимодействия подтверждено нели-нейно-оптическими измерениями.},\\n\\tlanguage = {ru},\\n\\tnumber = {12},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Нано- И Микросистемная Техника},\\n\\tauthor = {Кузнецов, М. А. and Мишина, Е. Д. and Морозов, А. И. and Сигов, А. С. and Головко, Ю. И. and Мухортов, В. М. and Мошняга, В. Т.},\\n\\tyear = {2007},\\n\\tkeywords = {⛔ No DOI found},\\n\\tpages = {20--22},\\n}\\n\\n\",\"author_short\":[\"Кузнецов, М. А.\",\"Мишина, Е. Д.\",\"Морозов, А. И.\",\"Сигов, А. С.\",\"Головко, Ю. И.\",\"Мухортов, В. М.\",\"Мошняга, В. Т.\"],\"key\":\"__2007-3\",\"id\":\"__2007-3\",\"bibbaseid\":\"-------bifeotextrm3-2007\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.elibrary.ru/item.asp?id=11693334\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Спектры комбинационного рассеяния света титаната кадмия\",\"volume\":\"47\",\"url\":\"https://journals.ioffe.ru/articles/3735\",\"abstract\":\"Впервые получены поляризованные спектры комбинационного рассеяния света монокристаллических образцов CdTiO3 в области частот 5 \\\\textlessν\\\\textless 1000 cm$^{\\\\textrm{−1}}$ при температурах 10−1200 K. Основное внима ние уделено низкочастотной области, где обнаружено аномальное температурное поведение нескольких фононных мод. Высокотемпературными исследованиями выявлено существование четырех фононов с характерным для мягких мод поведением. Эти фононы отнесены к модам, восстанавливающим кубическую симметрию решетки. Экстраполяции их температурных зависимостей позволили выдвинуть гипотезу о существовании цепочки из трех гипотетических высокотемпературных фазовых переходов, аналогичных тем, что наблюдаются собственно в перовските CaTiO3. При температурах ниже 78 K спектр комбинационного рассеяния обогащается новыми линиями, появление которых связано с полярными искажениями ячейки. На низких частотах обнаружено три линии с аномальным поведением осцилляторных параметров, которое характерно для мягких мод в сегнетоэлектрических фазах. Предполагается возможность существования нескольких разных полярных состояний при низких температурах.\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Торгашев\"],\"firstnames\":[\"В.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Леманов\"],\"firstnames\":[\"В.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Спектор\"],\"firstnames\":[\"И.\",\"Е.\"],\"suffixes\":[]}],\"year\":\"2005\",\"keywords\":\"⛔ No DOI found\",\"pages\":\"324–333\",\"file\":\"Физика твердого тела:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\9NBHHWBQ\\\\\\\\3735.html:text/html;Физика твердого тела.pdf:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\3H3Z7B97\\\\\\\\Физика твердого тела.pdf:application/pdf\",\"bibtex\":\"@article{__2005,\\n\\ttitle = {Спектры комбинационного рассеяния света титаната кадмия},\\n\\tvolume = {47},\\n\\turl = {https://journals.ioffe.ru/articles/3735},\\n\\tabstract = {Впервые получены поляризованные спектры комбинационного рассеяния света монокристаллических\\nобразцов CdTiO3 в области частот 5 {\\\\textless}ν{\\\\textless} 1000 cm$^{\\\\textrm{−1}}$ при температурах 10−1200 K. Основное внима ние уделено низкочастотной области, где обнаружено аномальное температурное поведение нескольких\\nфононных мод. Высокотемпературными исследованиями выявлено существование четырех фононов с характерным для мягких мод поведением. Эти фононы отнесены к модам, восстанавливающим кубическую симметрию решетки. Экстраполяции их температурных зависимостей позволили выдвинуть гипотезу о существовании цепочки из трех гипотетических высокотемпературных фазовых переходов, аналогичных тем, что наблюдаются собственно в перовските CaTiO3. При температурах ниже 78 K спектр комбинационного рассеяния обогащается новыми линиями, появление которых связано с полярными искажениями ячейки. На низких частотах обнаружено три линии с аномальным поведением осцилляторных параметров, которое характерно для мягких мод в сегнетоэлектрических фазах. Предполагается возможность существования нескольких разных полярных состояний при низких температурах.},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Торгашев, В. И. and Юзюк, Ю. И. and Широков, В. Б. and Леманов, В. В. and Спектор, И. Е.},\\n\\tyear = {2005},\\n\\tkeywords = {⛔ No DOI found},\\n\\tpages = {324--333},\\n\\tfile = {Физика твердого тела:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\9NBHHWBQ\\\\\\\\3735.html:text/html;Физика твердого тела.pdf:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\3H3Z7B97\\\\\\\\Физика твердого тела.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Торгашев, В. И.\",\"Юзюк, Ю. И.\",\"Широков, В. Б.\",\"Леманов, В. В.\",\"Спектор, И. Е.\"],\"key\":\"__2005\",\"id\":\"__2005\",\"bibbaseid\":\"------2005\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/3735\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Формирование доменной структуры под действием деформационных полей в наноразмерных пленках титаната бария-стронция\",\"volume\":\"31\",\"url\":\"http://elibrary.lt/resursai/Uzsienio%20leidiniai/ioffe/pztf/2005/23/pztf_t31v23_12.pdf\",\"number\":\"23\",\"urldate\":\"2023-11-11\",\"journal\":\"Письма ЖТФ\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Колесников\"],\"firstnames\":[\"В.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бирюков\"],\"firstnames\":[\"С.\",\"В.\"],\"suffixes\":[]}],\"year\":\"2005\",\"keywords\":\"⛔ No DOI found\",\"pages\":\"75–81\",\"bibtex\":\"@article{__2005-1,\\n\\ttitle = {Формирование доменной структуры под действием деформационных полей в наноразмерных пленках титаната бария-стронция},\\n\\tvolume = {31},\\n\\turl = {http://elibrary.lt/resursai/Uzsienio%20leidiniai/ioffe/pztf/2005/23/pztf_t31v23_12.pdf},\\n\\tnumber = {23},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Письма ЖТФ},\\n\\tauthor = {Мухортов, В. М. and Головко, Ю. И. and Колесников, В. В. and Бирюков, С. В.},\\n\\tyear = {2005},\\n\\tkeywords = {⛔ No DOI found},\\n\\tpages = {75--81},\\n}\\n\\n\",\"author_short\":[\"Мухортов, В. М.\",\"Головко, Ю. И.\",\"Колесников, В. В.\",\"Бирюков, С. В.\"],\"key\":\"__2005-1\",\"id\":\"__2005-1\",\"bibbaseid\":\"-----2005\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://elibrary.lt/resursai/Uzsienio%20leidiniai/ioffe/pztf/2005/23/pztf_t31v23_12.pdf\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Переключение поляризации в наноразмерных пленках титаната бария стронция\",\"volume\":\"9\",\"issn\":\"1992-7223, 1993-4068\",\"url\":\"https://elibrary.ru/item.asp?id=21184158\",\"abstract\":\"Исследовано переключение поляризации сегнетоэлектрических тонких пленок Ba0.8Sr0.2TiO3 толщиной 2–150 нм, осажденных на Si(111) с Pt подслоем. Критическим параметром при переключении поляризации является площадь сегнетоэлектрического кристаллита. Пленки толщиной 2 нм обладают сегнетоэлектрическими свойствами.Polarization switching in Ba0.8Sr0.2TiO3 ferroelectric 2–150 nm-thick thin films deposited on Pt coated Si(111) substrates was studied. The area of the ferroelectric crystallite is shown to be a critical parameter for polarization switching. The 2 nm-thick films possess ferroelectric properties.\",\"language\":\"ru\",\"number\":\"1-2\",\"urldate\":\"2023-11-11\",\"journal\":\"Российские Нанотехнологии\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Сова\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]}],\"year\":\"2014\",\"keywords\":\"Кристаллит, Наноразмер, Наноразмерная Пленка, Поляризация, Сегнетоэлектрический, Титанат Бария Стронция, ⛔ No DOI found\",\"pages\":\"55–58\",\"bibtex\":\"@article{__2014-6,\\n\\ttitle = {Переключение поляризации в наноразмерных пленках титаната бария стронция},\\n\\tvolume = {9},\\n\\tissn = {1992-7223, 1993-4068},\\n\\turl = {https://elibrary.ru/item.asp?id=21184158},\\n\\tabstract = {Исследовано переключение поляризации сегнетоэлектрических тонких пленок Ba0.8Sr0.2TiO3 толщиной 2–150 нм, осажденных на Si(111) с Pt подслоем. Критическим параметром при переключении поляризации является площадь сегнетоэлектрического кристаллита. Пленки толщиной 2 нм обладают сегнетоэлектрическими свойствами.Polarization switching in Ba0.8Sr0.2TiO3 ferroelectric 2–150 nm-thick thin films deposited on Pt coated Si(111) substrates was studied. The area of the ferroelectric crystallite is shown to be a critical parameter for polarization switching. The 2 nm-thick films possess ferroelectric properties.},\\n\\tlanguage = {ru},\\n\\tnumber = {1-2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Российские Нанотехнологии},\\n\\tauthor = {Мухортов, В. М. and Сова, Е. М. and Широков, В. Б. and Головко, Ю. И. and Лянгузов, Н. В. and Юзюк, Ю. И.},\\n\\tyear = {2014},\\n\\tkeywords = {Кристаллит, Наноразмер, Наноразмерная Пленка, Поляризация, Сегнетоэлектрический, Титанат Бария Стронция, ⛔ No DOI found},\\n\\tpages = {55--58},\\n}\\n\\n\",\"author_short\":[\"Мухортов, В. М.\",\"Сова, Е. М.\",\"Широков, В. Б.\",\"Головко, Ю. И.\",\"Лянгузов, Н. В.\",\"Юзюк, Ю. И.\"],\"key\":\"__2014-6\",\"id\":\"__2014-6\",\"bibbaseid\":\"-------2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=21184158\"},\"keyword\":[\"Кристаллит\",\"Наноразмер\",\"Наноразмерная Пленка\",\"Поляризация\",\"Сегнетоэлектрический\",\"Титанат Бария Стронция\",\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"A comparative X-ray diffraction study of ferroelectric thin films and superlattices\",\"copyright\":\"© 2017 Taylor & Francis Group, LLC\",\"issn\":\"0015-0193\",\"url\":\"https://www.tandfonline.com/doi/abs/10.1080/00150193.2017.1289764\",\"abstract\":\"A number of ferroelectric thin films with various barium concentration and two sets of superlattices with different composition and number of constituent layers were investigated using X-ray diffra...\",\"language\":\"EN\",\"urldate\":\"2023-11-11\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Tikhonov\"],\"firstnames\":[\"Yu\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zakharchenko\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Y.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pavunny\"],\"firstnames\":[\"Sh\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ortega\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kumar\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"R.\",\"S.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2017\",\"note\":\"Publisher: Taylor & Francis\",\"keywords\":\"⛔ No DOI found\",\"file\":\"Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\VRJ96NXD\\\\\\\\full.html:text/html\",\"bibtex\":\"@article{tikhonov_comparative_2017,\\n\\ttitle = {A comparative {X}-ray diffraction study of ferroelectric thin films and superlattices},\\n\\tcopyright = {© 2017 Taylor \\\\& Francis Group, LLC},\\n\\tissn = {0015-0193},\\n\\turl = {https://www.tandfonline.com/doi/abs/10.1080/00150193.2017.1289764},\\n\\tabstract = {A number of ferroelectric thin films with various barium concentration and two sets of superlattices with different composition and number of constituent layers were investigated using X-ray diffra...},\\n\\tlanguage = {EN},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Tikhonov, Yu A. and Zakharchenko, I. N. and Razumnaya, A. G. and Yuzyuk, Y. I. and Pavunny, Sh and Ortega, N. and Kumar, A. and Katiyar, R. S.},\\n\\tmonth = feb,\\n\\tyear = {2017},\\n\\tnote = {Publisher: Taylor \\\\& Francis},\\n\\tkeywords = {⛔ No DOI found},\\n\\tfile = {Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\VRJ96NXD\\\\\\\\full.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Tikhonov, Y. A.\",\"Zakharchenko, I. N.\",\"Razumnaya, A. G.\",\"Yuzyuk, Y. I.\",\"Pavunny, S.\",\"Ortega, N.\",\"Kumar, A.\",\"Katiyar, R. S.\"],\"key\":\"tikhonov_comparative_2017\",\"id\":\"tikhonov_comparative_2017\",\"bibbaseid\":\"tikhonov-zakharchenko-razumnaya-yuzyuk-pavunny-ortega-kumar-katiyar-acomparativexraydiffractionstudyofferroelectricthinfilmsandsuperlattices-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.tandfonline.com/doi/abs/10.1080/00150193.2017.1289764\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Влияние механизма роста и термоупругих напряжений на динамику кристаллической решетки гетероэпитаксиальных пленок титаната бария–стронция\",\"url\":\"https://journals.ioffe.ru/articles/3167\",\"urldate\":\"2023-11-11\",\"bibtex\":\"@article{noauthor__nodate,\\n\\ttitle = {Влияние механизма роста и термоупругих напряжений на динамику кристаллической решетки гетероэпитаксиальных пленок титаната бария--стронция},\\n\\turl = {https://journals.ioffe.ru/articles/3167},\\n\\turldate = {2023-11-11},\\n}\\n\\n\",\"key\":\"noauthor__nodate\",\"id\":\"noauthor__nodate\",\"bibbaseid\":\"anonymous-\",\"role\":\"\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/3167\"},\"metadata\":{\"authorlinks\":{\"moore, a\":\"https://www.cl.cam.ac.uk/~awm22/talks.html\",\"powner, m\":\"https://bibbase.org/show?bib=benjaminthoma.github.io%2Fpubs.bib\",\"bergmann, r\":\"https://bibbase.org/show?bib=www.wi2.uni-trier.de/publications/WI2Publikationen.bib&group0=year&css=www.wi2.uni-trier.de/publications/WI2.css&filter=authors:Bergmann\",\"van harmelen, f\":\"https://www.cs.vu.nl/\",\"figueroa, n\":\"https://nbfigueroa.github.io/\",\"sammak, s\":\"https://shervinsammak.github.io/papers/\",\"patel, n\":\"https://niravatgit.github.io/INSPIRELab/publications.html#publications\",\"kouamé, d\":\"https://bibbase.org/show?bib=https%3A%2F%2Fwww.irit.fr%2F%7EDenis.Kouame%2Fwp-content%2Fuploads%2Fsites%2F16%2F2023%2F07%2Fpubli_dk_Juillet2023.bib&commas=true&msg=embed&noBootstrap=1\",\"grossi, g\":\"https://bibbase.org/show?bib=https://homes.di.unimi.it/grossi/Grossi_Giuliano.bib\",\"alexiev, v\":\"https://rawgit2.com/VladimirAlexiev/my/master/index.html\",\"bethard, s\":\"https://bethard.github.io/publications.html\",\"homburg, t\":\"https://situx.github.io/publications/\",\"banzhaf, w\":\"https://cse.msu.edu/~banzhafw/Publications_new.html\",\"gatica, j\":\"https://bibbase.org/show?bib=www2.uca.es%2Fdept%2Fcmat_qinor%2Fnanomat%2Fpeople%2FGatica.bib&groupby=year\",\"edwards, c\":\"https://people.ucsc.edu/\",\"miyagusuku, r\":\"https://www.real.utsunomiya-u.ac.jp/invmap/\",\"stephens-davidowitz, n\":\"http://www.noahsd.com/\",\"kouam�, d\":\"https://bibbase.org/show?bib=https%3A%2F%2Fwww.irit.fr%2F%7EDenis.Kouame%2Fwp-content%2Fuploads%2Fsites%2F16%2F2020%2F08%2Fpubli_dk_pc.bib&msg=embed\",\"lee, u\":\"https://bibbase.org/show?bib=https://dblp.org/pid/172/3208.bib\",\"sohrabi, s\":\"https://www.cs.toronto.edu/~shirin/\",\"mcintire, e\":\"https://predictiveecology.org/publications.html\",\"mirrazavi salehian, s\":\"https://nbfigueroa.github.io/\",\"monteiro, s\":\"https://sildomar.github.io/publications/\",\"picco, m\":\"https://www.lpthe.jussieu.fr/~picco/pub.html\",\"maranas, c\":\"https://bibbase.org/show?bib=www.maranasgroup.com/pub/maranasgroup.bib\",\"romoli, j\":\"https://jacoporomoli.github.io/Publications/\",\"maizel, a\":\"https://www.cos.uni-heidelberg.de/\",\"iovino, l\":\"https://www.ludovicoiovino.it/\",\"keller, a\":\"https://bibbase.org/show?bib=https://www.ccb.uni-saarland.de/wp-content/uploads/2024/01/references.bib_.txt&folding=1\",\"riviere, b\":\"http://compm.rice.edu/publications/\",\"beyer, a\":\"https://www.klassphil.hu-berlin.de/de/personen/andrea-beyer\",\"bluestein, d\":\"https://www.bme.stonybrook.edu/labs/dbluestein/aaapatient.html\",\"sabattini, l\":\"https://883789326-atari-embeds.googleusercontent.com/embeds/16cb204cf3a9d4d223a0a3fd8b0eec5d/inner-frame-minified.html\"}},\"downloads\":9,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Stress alteration in heteroepitaxial (Ba,Sr)TiO$_{\\\\textrm{3}}$/(001) MgO thin films via growth mechanism\",\"volume\":\"40\",\"issn\":\"0022-3727\",\"url\":\"https://dx.doi.org/10.1088/0022-3727/40/14/025\",\"doi\":\"10.1088/0022-3727/40/14/025\",\"abstract\":\"We have studied stress effects in heteroepitaxial (Ba0.7Sr0.3)TiO3 thin films deposited by rf sputtering on (0 0 1) MgO substrates. By varying the deposition conditions, three-dimensional (3D) nucleation growth and layer-by-layer growth mechanisms were realized. X-ray diffraction (XRD) measurements revealed that tetragonal distortion and Curie temperature (Tc) depend on the growth mechanism. The frequency of the E(TO) soft mode in the polarized Raman spectra correlated with the value of two-dimensional stress, determined from XRD experiments. Temperature-dependent lattice parameters and Raman spectra revealed an upward shift of the Curie temperature. Two-dimensional compressive stress was found to be larger in the film grown by the 3D nucleation mechanism.\",\"language\":\"en\",\"number\":\"14\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics D: Applied Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Simon\"],\"firstnames\":[\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zakharchenko\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Alyoshin\"],\"firstnames\":[\"V.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mukhortov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2007\",\"pages\":\"4271\",\"bibtex\":\"@article{yuzyuk_stress_2007,\\n\\ttitle = {Stress alteration in heteroepitaxial ({Ba},{Sr}){TiO}$_{\\\\textrm{3}}$/(001) {MgO} thin films via growth mechanism},\\n\\tvolume = {40},\\n\\tissn = {0022-3727},\\n\\turl = {https://dx.doi.org/10.1088/0022-3727/40/14/025},\\n\\tdoi = {10.1088/0022-3727/40/14/025},\\n\\tabstract = {We have studied stress effects in heteroepitaxial (Ba0.7Sr0.3)TiO3 thin films deposited by rf sputtering on (0 0 1) MgO substrates. By varying the deposition conditions, three-dimensional (3D) nucleation growth and layer-by-layer growth mechanisms were realized. X-ray diffraction (XRD) measurements revealed that tetragonal distortion and Curie temperature (Tc) depend on the growth mechanism. The frequency of the E(TO) soft mode in the polarized Raman spectra correlated with the value of two-dimensional stress, determined from XRD experiments. Temperature-dependent lattice parameters and Raman spectra revealed an upward shift of the Curie temperature. Two-dimensional compressive stress was found to be larger in the film grown by the 3D nucleation mechanism.},\\n\\tlanguage = {en},\\n\\tnumber = {14},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics D: Applied Physics},\\n\\tauthor = {Yuzyuk, Yu I. and Simon, P. and Zakharchenko, I. N. and Alyoshin, V. A. and Leontyev, I. N. and Mukhortov, V. M.},\\n\\tmonth = jun,\\n\\tyear = {2007},\\n\\tpages = {4271},\\n}\\n\\n\",\"author_short\":[\"Yuzyuk, Y. I.\",\"Simon, P.\",\"Zakharchenko, I. N.\",\"Alyoshin, V. A.\",\"Leontyev, I. N.\",\"Mukhortov, V. M.\"],\"key\":\"yuzyuk_stress_2007\",\"id\":\"yuzyuk_stress_2007\",\"bibbaseid\":\"yuzyuk-simon-zakharchenko-alyoshin-leontyev-mukhortov-stressalterationinheteroepitaxialbasrtiotextrm3001mgothinfilmsviagrowthmechanism-2007\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/0022-3727/40/14/025\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"book\",\"type\":\"book\",\"title\":\"Гетероструктуры на основе наноразмерных сегнетоэлектрических пленок: получение, свойства и применение\",\"isbn\":\"978-5-902982-42-5\",\"shorttitle\":\"Гетероструктуры на основе наноразмерных сегнетоэлектрических пленок\",\"url\":\"https://rusneb.ru/catalog/000199_000009_004241648/\",\"abstract\":\"«Гетероструктуры на основе наноразмерных сегнетоэлектрических пленок: получение, свойства и применение» (978-5-902982-42-5 (в пер.)) — Мухортов, Владимир Михайлович, 221, [1] с.. Издано: (2008). ✔Читать онлайн. ✔Адрес библиотеки с ближайшим печатным изданием ➤ RusNeb.ru.\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]}],\"year\":\"2008\",\"file\":\"Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\VMDT5IMU\\\\\\\\000199_000009_004241648.html:text/html\",\"bibtex\":\"@book{__2008-7,\\n\\ttitle = {Гетероструктуры на основе наноразмерных сегнетоэлектрических пленок: получение, свойства и применение},\\n\\tisbn = {978-5-902982-42-5},\\n\\tshorttitle = {Гетероструктуры на основе наноразмерных сегнетоэлектрических пленок},\\n\\turl = {https://rusneb.ru/catalog/000199_000009_004241648/},\\n\\tabstract = {«Гетероструктуры на основе наноразмерных сегнетоэлектрических пленок: получение, свойства и применение» (978-5-902982-42-5 (в пер.)) — Мухортов, Владимир Михайлович, 221, [1] с.. Издано: (2008). ✔Читать онлайн. ✔Адрес библиотеки с ближайшим печатным изданием ➤ RusNeb.ru.},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Мухортов, В. М. and Юзюк, Ю. И.},\\n\\tyear = {2008},\\n\\tfile = {Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\VMDT5IMU\\\\\\\\000199_000009_004241648.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Мухортов, В. М.\",\"Юзюк, Ю. И.\"],\"key\":\"__2008-7\",\"id\":\"__2008-7\",\"bibbaseid\":\"---2008\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://rusneb.ru/catalog/000199_000009_004241648/\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Mg$_{\\\\textrm{x}}$Zn$_{\\\\textrm{1−x}}$O(0⩽x\\\\textless0.2) nanowire arrays on sapphire grown by high-pressure pulsed-laser deposition\",\"volume\":\"86\",\"issn\":\"0003-6951\",\"url\":\"https://doi.org/10.1063/1.1898433\",\"doi\":\"10.1063/1.1898433\",\"abstract\":\"MgxZn1−xO nanowires with Mg-content x from 0 to 0.2 have been grown by high-pressure pulsed-laser deposition (PLD) on gold-covered sapphire single crystals. The PLD process allows for a unique wide-range control of morphology, diameter, and composition of the MgxZn1−xO nanowires. The diameter of single ZnO wires could be varied between about 50 and 3000 nm, and the Mg content x of MgxZn1−xO wire arrays was controlled via the PLD gas pressure. The microscopic homogeneity of Mg content is displayed by cathodoluminescence (CL) imaging of the excitonic peak energy. The fluctuation of CL peak energy between individual wires is about an order of magnitude smaller than the alloy broadening.\",\"number\":\"14\",\"urldate\":\"2023-11-11\",\"journal\":\"Applied Physics Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rahm\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nobis\"],\"firstnames\":[\"Th.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lenzner\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Wagner\"],\"firstnames\":[\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Spemann\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hochmuth\"],\"firstnames\":[\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2005\",\"pages\":\"143113\",\"bibtex\":\"@article{lorenz_mgxzn1xo0x02_2005,\\n\\ttitle = {Mg$_{\\\\textrm{x}}${Zn}$_{\\\\textrm{1−x}}${O}(0⩽x{\\\\textless}0.2) nanowire arrays on sapphire grown by high-pressure pulsed-laser deposition},\\n\\tvolume = {86},\\n\\tissn = {0003-6951},\\n\\turl = {https://doi.org/10.1063/1.1898433},\\n\\tdoi = {10.1063/1.1898433},\\n\\tabstract = {MgxZn1−xO nanowires with Mg-content x from 0 to 0.2 have been grown by high-pressure pulsed-laser deposition (PLD) on gold-covered sapphire single crystals. The PLD process allows for a unique wide-range control of morphology, diameter, and composition of the MgxZn1−xO nanowires. The diameter of single ZnO wires could be varied between about 50 and 3000 nm, and the Mg content x of MgxZn1−xO wire arrays was controlled via the PLD gas pressure. The microscopic homogeneity of Mg content is displayed by cathodoluminescence (CL) imaging of the excitonic peak energy. The fluctuation of CL peak energy between individual wires is about an order of magnitude smaller than the alloy broadening.},\\n\\tnumber = {14},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Applied Physics Letters},\\n\\tauthor = {Lorenz, M. and Kaidashev, E. M. and Rahm, A. and Nobis, Th. and Lenzner, J. and Wagner, G. and Spemann, D. and Hochmuth, H. and Grundmann, M.},\\n\\tmonth = mar,\\n\\tyear = {2005},\\n\\tpages = {143113},\\n}\\n\\n\",\"author_short\":[\"Lorenz, M.\",\"Kaidashev, E. M.\",\"Rahm, A.\",\"Nobis, T.\",\"Lenzner, J.\",\"Wagner, G.\",\"Spemann, D.\",\"Hochmuth, H.\",\"Grundmann, M.\"],\"key\":\"lorenz_mgxzn1xo0x02_2005\",\"id\":\"lorenz_mgxzn1xo0x02_2005\",\"bibbaseid\":\"lorenz-kaidashev-rahm-nobis-lenzner-wagner-spemann-hochmuth-etal-mgtextrmxzntextrm1xo0xtextless02nanowirearraysonsapphiregrownbyhighpressurepulsedlaserdeposition-2005\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.1898433\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Local symmetry breaking in Pb$_{\\\\textrm{x}}$Sr$_{\\\\textrm{1−x}}$TiO$_{\\\\textrm{3}}$ ceramics and composites studied by Raman spectroscopy\",\"volume\":\"98\",\"issn\":\"0021-8979\",\"url\":\"https://doi.org/10.1063/1.1989434\",\"doi\":\"10.1063/1.1989434\",\"abstract\":\"Local symmetry breaking in PbxSr1−xTiO3 (PST) solid solutions was revealed by Raman spectroscopy below and above the ferroelectric phase-transition temperature. In the paraelectric phase, local symmetry breaking associated with the polar clusters localized mostly at grain boundaries in ceramic samples leads to the activation of the polar modes far above the dielectric maximum. This effect was found remarkably enhanced in the PST:MgO composites due to the compositional inhomogeneity of the grain boundaries and the intergrain stresses in the composite. In the ferroelectric phase, the degeneracy of the E(TO1) soft mode was lifted due to translational symmetry breaking in the solid solutions with x=0.2 and 0.3, where the substitution of Sr by Pb replaces partially the ionic bonding between the A cations and the oxygens by a stronger covalent bonding.\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Applied Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Jain\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"R.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Somiya\"],\"firstnames\":[\"Y.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bhalla\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2005\",\"pages\":\"024116\",\"bibtex\":\"@article{jain_local_2005,\\n\\ttitle = {Local symmetry breaking in {Pb}$_{\\\\textrm{x}}${Sr}$_{\\\\textrm{1−x}}${TiO}$_{\\\\textrm{3}}$ ceramics and composites studied by {Raman} spectroscopy},\\n\\tvolume = {98},\\n\\tissn = {0021-8979},\\n\\turl = {https://doi.org/10.1063/1.1989434},\\n\\tdoi = {10.1063/1.1989434},\\n\\tabstract = {Local symmetry breaking in PbxSr1−xTiO3 (PST) solid solutions was revealed by Raman spectroscopy below and above the ferroelectric phase-transition temperature. In the paraelectric phase, local symmetry breaking associated with the polar clusters localized mostly at grain boundaries in ceramic samples leads to the activation of the polar modes far above the dielectric maximum. This effect was found remarkably enhanced in the PST:MgO composites due to the compositional inhomogeneity of the grain boundaries and the intergrain stresses in the composite. In the ferroelectric phase, the degeneracy of the E(TO1) soft mode was lifted due to translational symmetry breaking in the solid solutions with x=0.2 and 0.3, where the substitution of Sr by Pb replaces partially the ionic bonding between the A cations and the oxygens by a stronger covalent bonding.},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Applied Physics},\\n\\tauthor = {Jain, M. and Yuzyuk, Yu. I. and Katiyar, R. S. and Somiya, Y. and Bhalla, A. S.},\\n\\tmonth = jul,\\n\\tyear = {2005},\\n\\tpages = {024116},\\n}\\n\\n\",\"author_short\":[\"Jain, M.\",\"Yuzyuk, Y. I.\",\"Katiyar, R. S.\",\"Somiya, Y.\",\"Bhalla, A. S.\"],\"key\":\"jain_local_2005\",\"id\":\"jain_local_2005\",\"bibbaseid\":\"jain-yuzyuk-katiyar-somiya-bhalla-localsymmetrybreakinginpbtextrmxsrtextrm1xtiotextrm3ceramicsandcompositesstudiedbyramanspectroscopy-2005\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.1989434\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Polarized Raman Spectra of BaTiO$_{\\\\textrm{3}}$/SrTiO$_{\\\\textrm{3}}$ Superlattices\",\"volume\":\"329\",\"issn\":\"0015-0193\",\"url\":\"https://doi.org/10.1080/00150190500314833\",\"doi\":\"10.1080/00150190500314833\",\"abstract\":\"BaTiO 3 /SrTiO 3 superlattices were grown on (001)MgO substrates by pulsed-laser-deposition technique. The thickness of each layer varied from 6 to 25 unit cells. Polarization-dependent Raman spectra confirmed tetragonal symmetry of the superlattices with the polar axis being normal to the layers. The observed optic modes in the superlattices showed intermediate frequencies between corresponding bulk BaTiO 3 and SrTiO 3 values, while the E(TO 1 ) soft mode exhibited upward shift due to significant two-dimensional clamping caused by the lattice mismatch of the constituting layers. The observed downward shift of the soft mode revealed relaxation of two-dimensional stresses with increasing the stacking periodicity of the superlattices. The excitation of folded transverse acoustic phonons in the Raman spectra due to the new periodicity of the Brillouin zone was revealed. The observed data are quantitatively explained by a folding of the corresponding acoustic branch. It is shown that micro-Raman spectroscopy provides determination of a spatial variation of the layer thickness in graded superlattices. On leave from the Faculty of Physics, Rostov State University, Rostov-on-Don, Russia\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"Ram\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk†\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Das\"],\"firstnames\":[\"R.\",\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bhattacharya\"],\"firstnames\":[\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gupta\"],\"firstnames\":[\"V.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2005\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150190500314833\",\"pages\":\"3–12\",\"bibtex\":\"@article{katiyar_polarized_2005,\\n\\ttitle = {Polarized {Raman} {Spectra} of {BaTiO}$_{\\\\textrm{3}}$/{SrTiO}$_{\\\\textrm{3}}$ {Superlattices}},\\n\\tvolume = {329},\\n\\tissn = {0015-0193},\\n\\turl = {https://doi.org/10.1080/00150190500314833},\\n\\tdoi = {10.1080/00150190500314833},\\n\\tabstract = {BaTiO 3 /SrTiO 3 superlattices were grown on (001)MgO substrates by pulsed-laser-deposition technique. The thickness of each layer varied from 6 to 25 unit cells. Polarization-dependent Raman spectra confirmed tetragonal symmetry of the superlattices with the polar axis being normal to the layers. The observed optic modes in the superlattices showed intermediate frequencies between corresponding bulk BaTiO 3 and SrTiO 3 values, while the E(TO 1 ) soft mode exhibited upward shift due to significant two-dimensional clamping caused by the lattice mismatch of the constituting layers. The observed downward shift of the soft mode revealed relaxation of two-dimensional stresses with increasing the stacking periodicity of the superlattices. The excitation of folded transverse acoustic phonons in the Raman spectra due to the new periodicity of the Brillouin zone was revealed. The observed data are quantitatively explained by a folding of the corresponding acoustic branch. It is shown that micro-Raman spectroscopy provides determination of a spatial variation of the layer thickness in graded superlattices. On leave from the Faculty of Physics, Rostov State University, Rostov-on-Don, Russia},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Katiyar, Ram S. and Yuzyuk†, Yu. I. and Das, R. R. and Bhattacharya, P. and Gupta, V.},\\n\\tmonth = dec,\\n\\tyear = {2005},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/00150190500314833},\\n\\tpages = {3--12},\\n}\\n\\n\",\"author_short\":[\"Katiyar, R. S.\",\"Yuzyuk†, Y. I.\",\"Das, R. R.\",\"Bhattacharya, P.\",\"Gupta, V.\"],\"key\":\"katiyar_polarized_2005\",\"id\":\"katiyar_polarized_2005\",\"bibbaseid\":\"katiyar-yuzyuk-das-bhattacharya-gupta-polarizedramanspectraofbatiotextrm3srtiotextrm3superlattices-2005\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/00150190500314833\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Folded acoustic phonons and soft mode dynamics in BaTiO$_{\\\\textrm{3}}$/SrTiO$_{\\\\textrm{3}}$ superlattices\",\"volume\":\"69\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.69.132302\",\"doi\":\"10.1103/PhysRevB.69.132302\",\"abstract\":\"A series of BaTiO3/SrTiO3 superlattices with stacking periodicity of 6–10 unit cells were fabricated on (001)MgO substrates using pulsed-laser-deposition technique. Polarized Raman spectra revealed BaTiO3-like optical vibrations and confirmed tetragonal symmetry of the superlattices with the c axis being normal to the layers. Due to in-plane compressive stresses generated by the lattice mismatch of the constituting layers, the E(1TO) soft mode was underdamped and markedly shifted to higher frequencies with respect to its analogs in the bulk. The existence of perfect superlattice structure was evident from the observation of the folded acoustic phonons in Raman spectra. The frequencies of the folded phonons matched well with the calculated transverse-acoustic branches of the constituent materials. No phase transitions were revealed in the superlattices below room temperature, while phase transition to the paraelectric state is shifted up to 650–700 K and it is diffused.\",\"number\":\"13\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Das\"],\"firstnames\":[\"Rasmi\",\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bhattacharya\"],\"firstnames\":[\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gupta\"],\"firstnames\":[\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"R.\",\"S.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2004\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"132302\",\"bibtex\":\"@article{das_folded_2004,\\n\\ttitle = {Folded acoustic phonons and soft mode dynamics in {BaTiO}$_{\\\\textrm{3}}$/{SrTiO}$_{\\\\textrm{3}}$ superlattices},\\n\\tvolume = {69},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.69.132302},\\n\\tdoi = {10.1103/PhysRevB.69.132302},\\n\\tabstract = {A series of BaTiO3/SrTiO3 superlattices with stacking periodicity of 6–10 unit cells were fabricated on (001)MgO substrates using pulsed-laser-deposition technique. Polarized Raman spectra revealed BaTiO3-like optical vibrations and confirmed tetragonal symmetry of the superlattices with the c axis being normal to the layers. Due to in-plane compressive stresses generated by the lattice mismatch of the constituting layers, the E(1TO) soft mode was underdamped and markedly shifted to higher frequencies with respect to its analogs in the bulk. The existence of perfect superlattice structure was evident from the observation of the folded acoustic phonons in Raman spectra. The frequencies of the folded phonons matched well with the calculated transverse-acoustic branches of the constituent materials. No phase transitions were revealed in the superlattices below room temperature, while phase transition to the paraelectric state is shifted up to 650–700 K and it is diffused.},\\n\\tnumber = {13},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Das, Rasmi R. and Yuzyuk, Yu. I. and Bhattacharya, P. and Gupta, V. and Katiyar, R. S.},\\n\\tmonth = apr,\\n\\tyear = {2004},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {132302},\\n}\\n\\n\",\"author_short\":[\"Das, R. R.\",\"Yuzyuk, Y. I.\",\"Bhattacharya, P.\",\"Gupta, V.\",\"Katiyar, R. S.\"],\"key\":\"das_folded_2004\",\"id\":\"das_folded_2004\",\"bibbaseid\":\"das-yuzyuk-bhattacharya-gupta-katiyar-foldedacousticphononsandsoftmodedynamicsinbatiotextrm3srtiotextrm3superlattices-2004\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.69.132302\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Growth and characterization of c-axis oriented LiNbO$_{\\\\textrm{3}}$ film on a transparent conducting Al:ZnO inter-layer on Si\",\"volume\":\"19\",\"issn\":\"2044-5326\",\"shorttitle\":\"Growth and characterization of c-axis oriented LiNbO3 film on a transparent conducting Al\",\"url\":\"https://doi.org/10.1557/JMR.2004.0322\",\"doi\":\"10.1557/JMR.2004.0322\",\"abstract\":\"C-axis oriented lithium niobate (LiNbO3) films were deposited by pulsed-laser deposition on silicon using a transparent conducting interlayer of aluminum (Al)-doped zinc oxide (ZnO). Only two x-ray diffraction reflections corresponding to (006) and (0012) planes of LiNbO3 were observed in the films deposited at a 100-mTorr oxygen pressure and a 450–500 °C substrate temperature. Presence of sharp modes corresponding to E(TO) and A(LO), and absence of any superfluous peaks mainly around 900–905 cm−1 in the Raman spectra confirmed the formation of textured LiNbO3 film. Measured value of direct current and alternate current (AC) conductivities and dielectric constant are 8.6 × 10-12 Ω−1cm-1, 1.16 × 10-6 Ω−1cm-1, and 29.3, respectively, at room temperature. Behavior of dielectric constant and AC conductivity with frequency and temperature are close to the reported single-crystal data.\",\"language\":\"en\",\"number\":\"8\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Materials Research\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Gupta\"],\"firstnames\":[\"Vinay\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bhattacharya\"],\"firstnames\":[\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"R.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tomar\"],\"firstnames\":[\"Monika\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sreenivas\"],\"firstnames\":[\"K.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2004\",\"pages\":\"2235–2239\",\"bibtex\":\"@article{gupta_growth_2004,\\n\\ttitle = {Growth and characterization of c-axis oriented {LiNbO}$_{\\\\textrm{3}}$ film on a transparent conducting {Al}:{ZnO} inter-layer on {Si}},\\n\\tvolume = {19},\\n\\tissn = {2044-5326},\\n\\tshorttitle = {Growth and characterization of c-axis oriented {LiNbO3} film on a transparent conducting {Al}},\\n\\turl = {https://doi.org/10.1557/JMR.2004.0322},\\n\\tdoi = {10.1557/JMR.2004.0322},\\n\\tabstract = {C-axis oriented lithium niobate (LiNbO3) films were deposited by pulsed-laser deposition on silicon using a transparent conducting interlayer of aluminum (Al)-doped zinc oxide (ZnO). Only two x-ray diffraction reflections corresponding to (006) and (0012) planes of LiNbO3 were observed in the films deposited at a 100-mTorr oxygen pressure and a 450–500 °C substrate temperature. Presence of sharp modes corresponding to E(TO) and A(LO), and absence of any superfluous peaks mainly around 900–905 cm−1 in the Raman spectra confirmed the formation of textured LiNbO3 film. Measured value of direct current and alternate current (AC) conductivities and dielectric constant are 8.6 × 10-12 Ω−1cm-1, 1.16 × 10-6 Ω−1cm-1, and 29.3, respectively, at room temperature. Behavior of dielectric constant and AC conductivity with frequency and temperature are close to the reported single-crystal data.},\\n\\tlanguage = {en},\\n\\tnumber = {8},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Materials Research},\\n\\tauthor = {Gupta, Vinay and Bhattacharya, P. and Yuzyuk, Yu. I. and Katiyar, R. S. and Tomar, Monika and Sreenivas, K.},\\n\\tmonth = aug,\\n\\tyear = {2004},\\n\\tpages = {2235--2239},\\n}\\n\\n\",\"author_short\":[\"Gupta, V.\",\"Bhattacharya, P.\",\"Yuzyuk, Y. I.\",\"Katiyar, R. S.\",\"Tomar, M.\",\"Sreenivas, K.\"],\"key\":\"gupta_growth_2004\",\"id\":\"gupta_growth_2004\",\"bibbaseid\":\"gupta-bhattacharya-yuzyuk-katiyar-tomar-sreenivas-growthandcharacterizationofcaxisorientedlinbotextrm3filmonatransparentconductingalznointerlayeronsi-2004\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1557/JMR.2004.0322\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Raman scattering in sol–gel derived PbTiO$_{\\\\textrm{3}}$ films modified with Ca\",\"volume\":\"85\",\"issn\":\"0254-0584\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S025405840400029X\",\"doi\":\"10.1016/j.matchemphys.2004.01.001\",\"abstract\":\"X-ray diffraction (XRD) and Raman scattering in sol–gel derived Pb1−xCaxTiO3 (PCT) thin films are studied as a function of Ca content x. It is found that Ca2+ addition to PbTiO3 films results in a gradual decrease of tetragonality of the perovskite lattice accompanied with a considerable modification of the Raman spectra. A significant difference in Raman spectra of PCT films and available reference data for single crystals (x=0) is explained in terms of the large internal stress, small grain size, and structural disorder produced by Ca2+ substitution. It is found that the shift of the frequency of ferroelectric soft mode correlates well with the variation of tetragonality for x≤xc=0.4. The concentration dependence of the shift is strongly non-linear being qualitatively different from that observed earlier in other A-site doped lead titanate-based systems. According to XRD data, the averaged crystal structure for xc≈0.4 appears as pseudo-cubic, while Raman scattering revealed short-range order tetragonal distortion. The structural characteristics of PCT films are linked to their electromechanical properties measured earlier by interferometric technique.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Materials Chemistry and Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kholkin\"],\"firstnames\":[\"A.\",\"L\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bdikin\"],\"firstnames\":[\"I\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Almeida\"],\"firstnames\":[\"A\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chaves\"],\"firstnames\":[\"M.\",\"R\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Calzada\"],\"firstnames\":[\"M.\",\"L\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mendiola\"],\"firstnames\":[\"J\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2004\",\"keywords\":\"Ferroelectricity, Thin films, Raman spectroscopy and scattering, Sol–gel growth\",\"pages\":\"176–179\",\"bibtex\":\"@article{kholkin_raman_2004,\\n\\ttitle = {Raman scattering in sol–gel derived {PbTiO}$_{\\\\textrm{3}}$ films modified with {Ca}},\\n\\tvolume = {85},\\n\\tissn = {0254-0584},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S025405840400029X},\\n\\tdoi = {10.1016/j.matchemphys.2004.01.001},\\n\\tabstract = {X-ray diffraction (XRD) and Raman scattering in sol–gel derived Pb1−xCaxTiO3 (PCT) thin films are studied as a function of Ca content x. It is found that Ca2+ addition to PbTiO3 films results in a gradual decrease of tetragonality of the perovskite lattice accompanied with a considerable modification of the Raman spectra. A significant difference in Raman spectra of PCT films and available reference data for single crystals (x=0) is explained in terms of the large internal stress, small grain size, and structural disorder produced by Ca2+ substitution. It is found that the shift of the frequency of ferroelectric soft mode correlates well with the variation of tetragonality for x≤xc=0.4. The concentration dependence of the shift is strongly non-linear being qualitatively different from that observed earlier in other A-site doped lead titanate-based systems. According to XRD data, the averaged crystal structure for xc≈0.4 appears as pseudo-cubic, while Raman scattering revealed short-range order tetragonal distortion. The structural characteristics of PCT films are linked to their electromechanical properties measured earlier by interferometric technique.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Materials Chemistry and Physics},\\n\\tauthor = {Kholkin, A. L and Bdikin, I and Yuzyuk, Yu. I and Almeida, A and Chaves, M. R and Calzada, M. L and Mendiola, J},\\n\\tmonth = may,\\n\\tyear = {2004},\\n\\tkeywords = {Ferroelectricity, Thin films, Raman spectroscopy and scattering, Sol–gel growth},\\n\\tpages = {176--179},\\n}\\n\\n\",\"author_short\":[\"Kholkin, A. L\",\"Bdikin, I\",\"Yuzyuk, Y. I\",\"Almeida, A\",\"Chaves, M. R\",\"Calzada, M. L\",\"Mendiola, J\"],\"key\":\"kholkin_raman_2004\",\"id\":\"kholkin_raman_2004\",\"bibbaseid\":\"kholkin-bdikin-yuzyuk-almeida-chaves-calzada-mendiola-ramanscatteringinsolgelderivedpbtiotextrm3filmsmodifiedwithca-2004\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S025405840400029X\"},\"keyword\":[\"Ferroelectricity\",\"Thin films\",\"Raman spectroscopy and scattering\",\"Sol–gel growth\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Nanodimensional effects in the structure of epitaxial YBa$_{\\\\textrm{2}}$Cu$_{\\\\textrm{3}}$O$_{\\\\textrm{7-y}}$ films\",\"volume\":\"30\",\"issn\":\"1090-6533\",\"url\":\"https://doi.org/10.1134/1.1666963\",\"doi\":\"10.1134/1.1666963\",\"abstract\":\"We have studied the structure of YBa2Cu3O7−y(YBCO) high-Tcsuperconductor films obtained by deposition for various times under otherwise identical conditions. Thin YBCO films prepared by the nonaxial laser shadow deposition technique are epitaxial and have microstrains below 1×10−3. The main factor determining variations of the unit cell parameter c in the films is the difference of the crystal block size 〈D〉 in the direction normal to the film surface, which reflects the nanodimensional effects known in oxides.\",\"language\":\"en\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Technical Physics Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Korol’kov\"],\"firstnames\":[\"D.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Abdulvakhidov\"],\"firstnames\":[\"K.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kupriyanov\"],\"firstnames\":[\"M.\",\"F.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2004\",\"keywords\":\"Block Size, Cell Parameter, Film Surface, Identical Condition, Oxide\",\"pages\":\"135–137\",\"bibtex\":\"@article{korolkov_nanodimensional_2004,\\n\\ttitle = {Nanodimensional effects in the structure of epitaxial {YBa}$_{\\\\textrm{2}}${Cu}$_{\\\\textrm{3}}${O}$_{\\\\textrm{7-y}}$ films},\\n\\tvolume = {30},\\n\\tissn = {1090-6533},\\n\\turl = {https://doi.org/10.1134/1.1666963},\\n\\tdoi = {10.1134/1.1666963},\\n\\tabstract = {We have studied the structure of YBa2Cu3O7−y(YBCO) high-Tcsuperconductor films obtained by deposition for various times under otherwise identical conditions. Thin YBCO films prepared by the nonaxial laser shadow deposition technique are epitaxial and have microstrains below 1×10−3. The main factor determining variations of the unit cell parameter c in the films is the difference of the crystal block size 〈D〉 in the direction normal to the film surface, which reflects the nanodimensional effects known in oxides.},\\n\\tlanguage = {en},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Technical Physics Letters},\\n\\tauthor = {Korol’kov, D. S. and Kaidashev, E. M. and Abdulvakhidov, K. G. and Kupriyanov, M. F.},\\n\\tmonth = feb,\\n\\tyear = {2004},\\n\\tkeywords = {Block Size, Cell Parameter, Film Surface, Identical Condition, Oxide},\\n\\tpages = {135--137},\\n}\\n\\n\",\"author_short\":[\"Korol’kov, D. S.\",\"Kaidashev, E. M.\",\"Abdulvakhidov, K. G.\",\"Kupriyanov, M. F.\"],\"key\":\"korolkov_nanodimensional_2004\",\"id\":\"korolkov_nanodimensional_2004\",\"bibbaseid\":\"korolkov-kaidashev-abdulvakhidov-kupriyanov-nanodimensionaleffectsinthestructureofepitaxialybatextrm2cutextrm3otextrm7yfilms-2004\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/1.1666963\"},\"keyword\":[\"Block Size\",\"Cell Parameter\",\"Film Surface\",\"Identical Condition\",\"Oxide\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Lattice dynamics in PbMg$_{\\\\textrm{1/3}}$Nb$_{\\\\textrm{2/3}}$O$_{\\\\textrm{3}}$\",\"volume\":\"70\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.70.134110\",\"doi\":\"10.1103/PhysRevB.70.134110\",\"abstract\":\"Lattice dynamics for five ordered PbMg1∕3Nb2∕3O3 supercells were calculated from first principles by the frozen phonon method. Maximal symmetries of all supercells are reduced by structural instabilities. Lattice modes corresponding to these instabilities, equilibrium ionic positions, and infrared reflectivity spectra were computed for all supercells. Results are compared with our experimental data for a chemically disordered PMN single crystal.\",\"number\":\"13\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Prosandeev\"],\"firstnames\":[\"S.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Cockayne\"],\"firstnames\":[\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Burton\"],\"firstnames\":[\"B.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kamba\"],\"firstnames\":[\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Petzelt\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"R.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vakhrushev\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2004\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"134110\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\GZG82Z22\\\\¶rosandeev и др. - 2004 - Lattice dynamics in $ mathrm PbMg _ 1∕3 mathrm.pdf:application/pdf;APS Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\T9HNHJSG\\\\¶hysRevB.70.html:text/html\",\"bibtex\":\"@article{prosandeev_lattice_2004,\\n\\ttitle = {Lattice dynamics in {PbMg}$_{\\\\textrm{1/3}}${Nb}$_{\\\\textrm{2/3}}${O}$_{\\\\textrm{3}}$},\\n\\tvolume = {70},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.70.134110},\\n\\tdoi = {10.1103/PhysRevB.70.134110},\\n\\tabstract = {Lattice dynamics for five ordered PbMg1∕3Nb2∕3O3 supercells were calculated from first principles by the frozen phonon method. Maximal symmetries of all supercells are reduced by structural instabilities. Lattice modes corresponding to these instabilities, equilibrium ionic positions, and infrared reflectivity spectra were computed for all supercells. Results are compared with our experimental data for a chemically disordered PMN single crystal.},\\n\\tnumber = {13},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Prosandeev, S. A. and Cockayne, E. and Burton, B. P. and Kamba, S. and Petzelt, J. and Yuzyuk, Yu. and Katiyar, R. S. and Vakhrushev, S. B.},\\n\\tmonth = oct,\\n\\tyear = {2004},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {134110},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\GZG82Z22\\\\\\\\Prosandeev и др. - 2004 - Lattice dynamics in \\\\$ mathrm PbMg _ 1∕3 mathrm.pdf:application/pdf;APS Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\T9HNHJSG\\\\\\\\PhysRevB.70.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Prosandeev, S. A.\",\"Cockayne, E.\",\"Burton, B. P.\",\"Kamba, S.\",\"Petzelt, J.\",\"Yuzyuk, Y.\",\"Katiyar, R. S.\",\"Vakhrushev, S. B.\"],\"key\":\"prosandeev_lattice_2004\",\"id\":\"prosandeev_lattice_2004\",\"bibbaseid\":\"prosandeev-cockayne-burton-kamba-petzelt-yuzyuk-katiyar-vakhrushev-latticedynamicsinpbmgtextrm13nbtextrm23otextrm3-2004\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.70.134110\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"series\":\"The 3rd International Conference on Spectroscopic Ellipsometry\",\"title\":\"UV–VUV spectroscopic ellipsometry of ternary Mg$_{\\\\textrm{x}}$Zn$_{\\\\textrm{1−x}}$O (0≤x≤0.53) thin films\",\"volume\":\"455-456\",\"issn\":\"0040-6090\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S004060900301856X\",\"doi\":\"10.1016/j.tsf.2003.11.249\",\"abstract\":\"The ordinary optical dielectric functions of pulsed-laser-deposition grown wurtzite c-plane MgxZn1−xO (0≤x≤0.53) thin films have been determined by using spectroscopic ellipsometry in the photon energy range from 4.5 to 9.5 eV. The dielectric functions reveal features which resemble those previously detected in uniaxial AlGaN and identified as E1- and E2-type band-to-band transitions with no remarkable dependence of the transition energy on Mg content x. The E1- and E2-type transitions for ZnO are compared with pseudopotential band-structure calculations.\",\"urldate\":\"2023-11-11\",\"journal\":\"Thin Solid Films\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Schmidt-Grund\"],\"firstnames\":[\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Schubert\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rheinländer\"],\"firstnames\":[\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fritsch\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Schmidt\"],\"firstnames\":[\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Herzinger\"],\"firstnames\":[\"C.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2004\",\"keywords\":\"Optical properties, Dielectric function, Ellipsometry, MgZnO, Vacuum ultraviolet, Zinc oxide (ZnO), ZnMgO\",\"pages\":\"500–504\",\"file\":\"ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\E97NUBSQ\\\\§004060900301856X.html:text/html\",\"bibtex\":\"@article{schmidt-grund_uvvuv_2004,\\n\\tseries = {The 3rd {International} {Conference} on {Spectroscopic} {Ellipsometry}},\\n\\ttitle = {{UV}–{VUV} spectroscopic ellipsometry of ternary {Mg}$_{\\\\textrm{x}}${Zn}$_{\\\\textrm{1−x}}${O} (0≤x≤0.53) thin films},\\n\\tvolume = {455-456},\\n\\tissn = {0040-6090},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S004060900301856X},\\n\\tdoi = {10.1016/j.tsf.2003.11.249},\\n\\tabstract = {The ordinary optical dielectric functions of pulsed-laser-deposition grown wurtzite c-plane MgxZn1−xO (0≤x≤0.53) thin films have been determined by using spectroscopic ellipsometry in the photon energy range from 4.5 to 9.5 eV. The dielectric functions reveal features which resemble those previously detected in uniaxial AlGaN and identified as E1- and E2-type band-to-band transitions with no remarkable dependence of the transition energy on Mg content x. The E1- and E2-type transitions for ZnO are compared with pseudopotential band-structure calculations.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Thin Solid Films},\\n\\tauthor = {Schmidt-Grund, R. and Schubert, M. and Rheinländer, B. and Fritsch, D. and Schmidt, H. and Kaidashev, E. M. and Lorenz, M. and Herzinger, C. M. and Grundmann, M.},\\n\\tmonth = may,\\n\\tyear = {2004},\\n\\tkeywords = {Optical properties, Dielectric function, Ellipsometry, MgZnO, Vacuum ultraviolet, Zinc oxide (ZnO), ZnMgO},\\n\\tpages = {500--504},\\n\\tfile = {ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\E97NUBSQ\\\\\\\\S004060900301856X.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Schmidt-Grund, R.\",\"Schubert, M.\",\"Rheinländer, B.\",\"Fritsch, D.\",\"Schmidt, H.\",\"Kaidashev, E. M.\",\"Lorenz, M.\",\"Herzinger, C. M.\",\"Grundmann, M.\"],\"key\":\"schmidt-grund_uvvuv_2004\",\"id\":\"schmidt-grund_uvvuv_2004\",\"bibbaseid\":\"schmidtgrund-schubert-rheinlnder-fritsch-schmidt-kaidashev-lorenz-herzinger-etal-uvvuvspectroscopicellipsometryofternarymgtextrmxzntextrm1xo0x053thinfilms-2004\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S004060900301856X\"},\"keyword\":[\"Optical properties\",\"Dielectric function\",\"Ellipsometry\",\"MgZnO\",\"Vacuum ultraviolet\",\"Zinc oxide (ZnO)\",\"ZnMgO\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"series\":\"Proceedings of the Sixteenth International Conference on Ion Beam Analysis\",\"title\":\"Ion beam analysis of epitaxial (Mg, Cd)$_{\\\\textrm{x}}$Zn$_{\\\\textrm{1−x}}$O and ZnO:(Li, Al, Ga, Sb) thin films grown on c-plane sapphire\",\"volume\":\"219-220\",\"issn\":\"0168-583X\",\"shorttitle\":\"Ion beam analysis of epitaxial (Mg, Cd)xZn1−xO and ZnO\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0168583X0400223X\",\"doi\":\"10.1016/j.nimb.2004.01.183\",\"abstract\":\"In this study ZnO thin films, nominally undoped, doped with Li, Al, Ga and Sb and alloyed with Mg and Cd grown epitaxially on c-plane sapphire by pulsed laser deposition (PLD) were investigated. In order to correlate the optical and electrical properties, e.g. the band gap energy and carrier concentration, to the elemental composition, the films were analyzed by RBS, PIXE and PIGE using He+ and H+ ion beams. It was found that the element transfer from the PLD target to the film differs significantly for the individual doping and alloying elements, with concentration ratios between film and target ranging from ∼4% for Li and Cd to ∼400% for Ga. In general, the films exhibited a metal to oxygen ratio of 1:1, only the ZnO:Li films were slightly oxygen deficient. Furthermore, the crystalline quality of the films was investigated using ion channeling. The nominally undoped ZnO films which were deposited with low-temperature interlayers for lower lateral stress showed a normalized minimum RBS yield of χmin=3.3% under channeling conditions. Whereas the incorporation of isovalent alloying atoms into the ZnO films leads to a slight degradation of the crystalline quality only, doping degrades the crystalline quality remarkably, even at low dopant concentrations.\",\"urldate\":\"2023-11-11\",\"journal\":\"Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Spemann\"],\"firstnames\":[\"D\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"M\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vogt\"],\"firstnames\":[\"J\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Butz\"],\"firstnames\":[\"T\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2004\",\"keywords\":\"Elemental composition, Thin films, Zinc oxide, Crystalline quality\",\"pages\":\"891–896\",\"bibtex\":\"@article{spemann_ion_2004,\\n\\tseries = {Proceedings of the {Sixteenth} {International} {Conference} on {Ion} {Beam} {Analysis}},\\n\\ttitle = {Ion beam analysis of epitaxial ({Mg}, {Cd})$_{\\\\textrm{x}}${Zn}$_{\\\\textrm{1−x}}${O} and {ZnO}:({Li}, {Al}, {Ga}, {Sb}) thin films grown on c-plane sapphire},\\n\\tvolume = {219-220},\\n\\tissn = {0168-583X},\\n\\tshorttitle = {Ion beam analysis of epitaxial ({Mg}, {Cd}){xZn1}−{xO} and {ZnO}},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0168583X0400223X},\\n\\tdoi = {10.1016/j.nimb.2004.01.183},\\n\\tabstract = {In this study ZnO thin films, nominally undoped, doped with Li, Al, Ga and Sb and alloyed with Mg and Cd grown epitaxially on c-plane sapphire by pulsed laser deposition (PLD) were investigated. In order to correlate the optical and electrical properties, e.g. the band gap energy and carrier concentration, to the elemental composition, the films were analyzed by RBS, PIXE and PIGE using He+ and H+ ion beams. It was found that the element transfer from the PLD target to the film differs significantly for the individual doping and alloying elements, with concentration ratios between film and target ranging from ∼4\\\\% for Li and Cd to ∼400\\\\% for Ga. In general, the films exhibited a metal to oxygen ratio of 1:1, only the ZnO:Li films were slightly oxygen deficient. Furthermore, the crystalline quality of the films was investigated using ion channeling. The nominally undoped ZnO films which were deposited with low-temperature interlayers for lower lateral stress showed a normalized minimum RBS yield of χmin=3.3\\\\% under channeling conditions. Whereas the incorporation of isovalent alloying atoms into the ZnO films leads to a slight degradation of the crystalline quality only, doping degrades the crystalline quality remarkably, even at low dopant concentrations.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms},\\n\\tauthor = {Spemann, D and Kaidashev, E. M and Lorenz, M and Vogt, J and Butz, T},\\n\\tmonth = jun,\\n\\tyear = {2004},\\n\\tkeywords = {Elemental composition, Thin films, Zinc oxide, Crystalline quality},\\n\\tpages = {891--896},\\n}\\n\\n\",\"author_short\":[\"Spemann, D\",\"Kaidashev, E. M\",\"Lorenz, M\",\"Vogt, J\",\"Butz, T\"],\"key\":\"spemann_ion_2004\",\"id\":\"spemann_ion_2004\",\"bibbaseid\":\"spemann-kaidashev-lorenz-vogt-butz-ionbeamanalysisofepitaxialmgcdtextrmxzntextrm1xoandznolialgasbthinfilmsgrownoncplanesapphire-2004\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0168583X0400223X\"},\"keyword\":[\"Elemental composition\",\"Thin films\",\"Zinc oxide\",\"Crystalline quality\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Synchrotron x-ray diffraction and Raman scattering investigations of (Li$_{\\\\textrm{x}}$Na$_{\\\\textrm{1-x}}$)NbO$_{\\\\textrm{3}}$ solid solutions: Evidence of the rhombohedral phase\",\"volume\":\"69\",\"shorttitle\":\"Synchrotron x-ray diffraction and Raman scattering investigations of $(\\\\{{\\\\}mathrm\\\\{{Li}\\\\}\\\\}_\\\\{x\\\\}\\\\{{\\\\}mathrm\\\\{{Na}\\\\}\\\\}_\\\\{1{\\\\}ensuremath\\\\{-\\\\}x\\\\})\\\\{{\\\\}mathrm\\\\{{NbO}\\\\}\\\\}_\\\\{3\\\\}$ solid solutions\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.69.144105\",\"doi\":\"10.1103/PhysRevB.69.144105\",\"abstract\":\"The (LixNa1−x)NbO3 perovskite solid solutions are investigated using synchrotron x-ray diffraction and Raman spectroscopy in order to clarify the structural changes in the concentration range 0\\\\textless~x\\\\textless~0.145 at room temperature. The orthorhombic antiferroelectric P phase (space group Pbma, Z=8) exists up to x=0.02 and in the concentration interval 0.02\\\\textless~x\\\\textless~0.03 we have confirmed a previously reported transition to the orthorhombic ferroelectric Q phase (space group P21ma, Z=4). It is found that the Q phase is stable up to x=0.145 but in the narrow concentration interval at x=0.12 the dominating (86.2%) rhombohedral N phase (space group R3c, Z=2) coexists with the minor (13.8%) Q phase at room temperature. The crystal structure of this rhombohedral N phase has been refined using Rietveld method. Detailed comparison with similar low-temperature phase of pure NaNbO3 showed that the NbO6 octahedra are slightly distorted in the solid solution with x=0.12 while they are rather regular in NaNbO3. Raman spectra showed drastic changes associated with the P−Q transition and revealed coexistence of the P and Q phases in the interval 0.02\\\\textless~x\\\\textless~0.03. Abrupt transformation of the Raman response and remarkable narrowing of the Nb-O stretching vibrations related to the existence of the rhombohedral N phase at x=0.12 were observed.\",\"number\":\"14\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gagarina\"],\"firstnames\":[\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Simon\"],\"firstnames\":[\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Reznitchenko\"],\"firstnames\":[\"L.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hennet\"],\"firstnames\":[\"L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Thiaudière\"],\"firstnames\":[\"D.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2004\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"144105\",\"file\":\"APS Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\BS8JEKPQ\\\\¶hysRevB.69.html:text/html\",\"bibtex\":\"@article{yuzyuk_synchrotron_2004,\\n\\ttitle = {Synchrotron x-ray diffraction and {Raman} scattering investigations of ({Li}$_{\\\\textrm{x}}${Na}$_{\\\\textrm{1-x}}$){NbO}$_{\\\\textrm{3}}$ solid solutions: {Evidence} of the rhombohedral phase},\\n\\tvolume = {69},\\n\\tshorttitle = {Synchrotron x-ray diffraction and {Raman} scattering investigations of \\\\$(\\\\{{\\\\textbackslash}mathrm\\\\{{Li}\\\\}\\\\}\\\\_\\\\{x\\\\}\\\\{{\\\\textbackslash}mathrm\\\\{{Na}\\\\}\\\\}\\\\_\\\\{1{\\\\textbackslash}ensuremath\\\\{-\\\\}x\\\\})\\\\{{\\\\textbackslash}mathrm\\\\{{NbO}\\\\}\\\\}\\\\_\\\\{3\\\\}\\\\$ solid solutions},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.69.144105},\\n\\tdoi = {10.1103/PhysRevB.69.144105},\\n\\tabstract = {The (LixNa1−x)NbO3 perovskite solid solutions are investigated using synchrotron x-ray diffraction and Raman spectroscopy in order to clarify the structural changes in the concentration range 0{\\\\textless}{\\\\textasciitilde}x{\\\\textless}{\\\\textasciitilde}0.145 at room temperature. The orthorhombic antiferroelectric P phase (space group Pbma, Z=8) exists up to x=0.02 and in the concentration interval 0.02{\\\\textless}{\\\\textasciitilde}x{\\\\textless}{\\\\textasciitilde}0.03 we have confirmed a previously reported transition to the orthorhombic ferroelectric Q phase (space group P21ma, Z=4). It is found that the Q phase is stable up to x=0.145 but in the narrow concentration interval at x=0.12 the dominating (86.2\\\\%) rhombohedral N phase (space group R3c, Z=2) coexists with the minor (13.8\\\\%) Q phase at room temperature. The crystal structure of this rhombohedral N phase has been refined using Rietveld method. Detailed comparison with similar low-temperature phase of pure NaNbO3 showed that the NbO6 octahedra are slightly distorted in the solid solution with x=0.12 while they are rather regular in NaNbO3. Raman spectra showed drastic changes associated with the P−Q transition and revealed coexistence of the P and Q phases in the interval 0.02{\\\\textless}{\\\\textasciitilde}x{\\\\textless}{\\\\textasciitilde}0.03. Abrupt transformation of the Raman response and remarkable narrowing of the Nb-O stretching vibrations related to the existence of the rhombohedral N phase at x=0.12 were observed.},\\n\\tnumber = {14},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Yuzyuk, Yu. I. and Gagarina, E. and Simon, P. and Reznitchenko, L. A. and Hennet, L. and Thiaudière, D.},\\n\\tmonth = apr,\\n\\tyear = {2004},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {144105},\\n\\tfile = {APS Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\BS8JEKPQ\\\\\\\\PhysRevB.69.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Yuzyuk, Y. I.\",\"Gagarina, E.\",\"Simon, P.\",\"Reznitchenko, L. A.\",\"Hennet, L.\",\"Thiaudière, D.\"],\"key\":\"yuzyuk_synchrotron_2004\",\"id\":\"yuzyuk_synchrotron_2004\",\"bibbaseid\":\"yuzyuk-gagarina-simon-reznitchenko-hennet-thiaudire-synchrotronxraydiffractionandramanscatteringinvestigationsoflitextrmxnatextrm1xnbotextrm3solidsolutionsevidenceoftherhombohedralphase-2004\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.69.144105\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"series\":\"Proceedings of the 9th International Workshop on Oxide Electronics\",\"title\":\"Optical and electrical properties of epitaxial (Mg,Cd)$_{\\\\textrm{x}}$Zn$_{\\\\textrm{1−x}}$O, ZnO, and ZnO:(Ga,Al) thin films on c-plane sapphire grown by pulsed laser deposition\",\"volume\":\"47\",\"issn\":\"0038-1101\",\"shorttitle\":\"Optical and electrical properties of epitaxial (Mg,Cd)xZn1−xO, ZnO, and ZnO\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0038110103001989\",\"doi\":\"10.1016/S0038-1101(03)00198-9\",\"abstract\":\"A consistent set of epitaxial, n-type conducting ZnO thin films, nominally undoped, doped with Ga or Al, or alloyed with Mg or Cd, was grown by pulsed laser deposition (PLD) on single-crystalline c-plane sapphire (0001) substrates, and characterized by Hall measurement, and UV/VIS optical transmission spectroscopy. The optical band gap of undoped ZnO films at nearly 3.28 eV was shifted by alloying with Mg up to 4.5 eV and by alloying with Cd down to 3.18 eV, dependent on the alloy composition. In addition, highly doped ZnO:Al films show a blue-shifted optical absorption edge due to filling of electronic states in the conduction band. The Hall transport data of the PLD (Mg,Zn,Cd)O:(Ga,Al) thin films span a carrier concentration range of six orders of magnitude from 3×1014 to 3×1020 cm−3, which corresponds to a resistivity from 5×10−4 to 3×103 Ωcm. Structurally optimized, nominally undoped ZnO films grown with ZnO nucleation and top layer reached an electron mobility of 155 cm2/Vs (300 K), which is among the largest values reported for heteroepitaxial ZnO thin films so far. Finally, we succeeded in combining the low resistivity of ZnO:Ga and the band gap shift of MgZnO in MgZnO:Ga thin films. This results demonstrate the unique tunability of the optical and electrical properties of the ZnO-based wide-band gap material for future electronic devices.\",\"number\":\"12\",\"urldate\":\"2023-11-11\",\"journal\":\"Solid-State Electronics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[\"von\"],\"lastnames\":[\"Wenckstern\"],\"firstnames\":[\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Riede\"],\"firstnames\":[\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bundesmann\"],\"firstnames\":[\"C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Spemann\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Benndorf\"],\"firstnames\":[\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hochmuth\"],\"firstnames\":[\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rahm\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Semmelhack\"],\"firstnames\":[\"H.\",\"-C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2003\",\"keywords\":\"Electrical properties, Optical properties, Pulsed laser deposition, Thin films, Wide-band gap material, Zinc oxide\",\"pages\":\"2205–2209\",\"bibtex\":\"@article{lorenz_optical_2003,\\n\\tseries = {Proceedings of the 9th {International} {Workshop} on {Oxide} {Electronics}},\\n\\ttitle = {Optical and electrical properties of epitaxial ({Mg},{Cd})$_{\\\\textrm{x}}${Zn}$_{\\\\textrm{1−x}}${O}, {ZnO}, and {ZnO}:({Ga},{Al}) thin films on c-plane sapphire grown by pulsed laser deposition},\\n\\tvolume = {47},\\n\\tissn = {0038-1101},\\n\\tshorttitle = {Optical and electrical properties of epitaxial ({Mg},{Cd}){xZn1}−{xO}, {ZnO}, and {ZnO}},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0038110103001989},\\n\\tdoi = {10.1016/S0038-1101(03)00198-9},\\n\\tabstract = {A consistent set of epitaxial, n-type conducting ZnO thin films, nominally undoped, doped with Ga or Al, or alloyed with Mg or Cd, was grown by pulsed laser deposition (PLD) on single-crystalline c-plane sapphire (0001) substrates, and characterized by Hall measurement, and UV/VIS optical transmission spectroscopy. The optical band gap of undoped ZnO films at nearly 3.28 eV was shifted by alloying with Mg up to 4.5 eV and by alloying with Cd down to 3.18 eV, dependent on the alloy composition. In addition, highly doped ZnO:Al films show a blue-shifted optical absorption edge due to filling of electronic states in the conduction band. The Hall transport data of the PLD (Mg,Zn,Cd)O:(Ga,Al) thin films span a carrier concentration range of six orders of magnitude from 3×1014 to 3×1020 cm−3, which corresponds to a resistivity from 5×10−4 to 3×103 Ωcm. Structurally optimized, nominally undoped ZnO films grown with ZnO nucleation and top layer reached an electron mobility of 155 cm2/Vs (300 K), which is among the largest values reported for heteroepitaxial ZnO thin films so far. Finally, we succeeded in combining the low resistivity of ZnO:Ga and the band gap shift of MgZnO in MgZnO:Ga thin films. This results demonstrate the unique tunability of the optical and electrical properties of the ZnO-based wide-band gap material for future electronic devices.},\\n\\tnumber = {12},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Solid-State Electronics},\\n\\tauthor = {Lorenz, M. and Kaidashev, E. M. and von Wenckstern, H. and Riede, V. and Bundesmann, C. and Spemann, D. and Benndorf, G. and Hochmuth, H. and Rahm, A. and Semmelhack, H. -C. and Grundmann, M.},\\n\\tmonth = dec,\\n\\tyear = {2003},\\n\\tkeywords = {Electrical properties, Optical properties, Pulsed laser deposition, Thin films, Wide-band gap material, Zinc oxide},\\n\\tpages = {2205--2209},\\n}\\n\\n\",\"author_short\":[\"Lorenz, M.\",\"Kaidashev, E. M.\",\"von Wenckstern, H.\",\"Riede, V.\",\"Bundesmann, C.\",\"Spemann, D.\",\"Benndorf, G.\",\"Hochmuth, H.\",\"Rahm, A.\",\"Semmelhack, H. -.\",\"Grundmann, M.\"],\"key\":\"lorenz_optical_2003\",\"id\":\"lorenz_optical_2003\",\"bibbaseid\":\"lorenz-kaidashev-vonwenckstern-riede-bundesmann-spemann-benndorf-hochmuth-etal-opticalandelectricalpropertiesofepitaxialmgcdtextrmxzntextrm1xoznoandznogaalthinfilmsoncplanesapphiregrownbypulsedlaserdeposition-2003\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0038110103001989\"},\"keyword\":[\"Electrical properties\",\"Optical properties\",\"Pulsed laser deposition\",\"Thin films\",\"Wide-band gap material\",\"Zinc oxide\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"A time-resolved optical study of the paramagnetic dielectric-ferromagnetic metal transition in La$_{\\\\textrm{0.7}}$Ca$_{\\\\textrm{0.3}}$MnO$_{\\\\textrm{3}}$\",\"volume\":\"97\",\"issn\":\"1090-6509\",\"url\":\"https://doi.org/10.1134/1.1625069\",\"doi\":\"10.1134/1.1625069\",\"abstract\":\"The relaxation dynamics of charge carriers in an epitaxial La0.7Ca0.3MnO3 film was studied by the light reflection method with a femtosecond time resolution in a wide temperature range. The relaxation of time-resolved photoinduced reflections was shown to be two-component in the whole temperature range including the paramagnetic dielectric-ferromagnetic metal transition at T ≈ 150–160 K. The fast relaxation component had a maximum lifetime (τ ∼ 500 ps) in the transition region, and its contribution to relaxation increased as temperature decreased. The lifetime of the slow component was minimum (τ ∼ 15 fs) in the transition region. In addition, fast oscillations assigned to coherent phonons appeared in photoinduced responses at T \\\\textless 200 K. The dephasing time of these oscillations increased as temperature decreased, whereas their frequency changed insignificantly.\",\"language\":\"en\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Experimental and Theoretical Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Misochko\"],\"firstnames\":[\"1.\",\"O.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Georgiev\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dekorsy\"],\"firstnames\":[\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zakharchenko\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2003\",\"keywords\":\"Charge Carrier, Elementary Particle, Time Resolution, Transition Region, Wide Temperature Range\",\"pages\":\"788–793\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\JRJUDEGD\\\\\\\\Misochko и др. - 2003 - A time-resolved optical study of the paramagnetic .pdf:application/pdf\",\"bibtex\":\"@article{misochko_time-resolved_2003,\\n\\ttitle = {A time-resolved optical study of the paramagnetic dielectric-ferromagnetic metal transition in {La}$_{\\\\textrm{0.7}}${Ca}$_{\\\\textrm{0.3}}${MnO}$_{\\\\textrm{3}}$},\\n\\tvolume = {97},\\n\\tissn = {1090-6509},\\n\\turl = {https://doi.org/10.1134/1.1625069},\\n\\tdoi = {10.1134/1.1625069},\\n\\tabstract = {The relaxation dynamics of charge carriers in an epitaxial La0.7Ca0.3MnO3 film was studied by the light reflection method with a femtosecond time resolution in a wide temperature range. The relaxation of time-resolved photoinduced reflections was shown to be two-component in the whole temperature range including the paramagnetic dielectric-ferromagnetic metal transition at T ≈ 150–160 K. The fast relaxation component had a maximum lifetime (τ ∼ 500 ps) in the transition region, and its contribution to relaxation increased as temperature decreased. The lifetime of the slow component was minimum (τ ∼ 15 fs) in the transition region. In addition, fast oscillations assigned to coherent phonons appeared in photoinduced responses at T {\\\\textless} 200 K. The dephasing time of these oscillations increased as temperature decreased, whereas their frequency changed insignificantly.},\\n\\tlanguage = {en},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Experimental and Theoretical Physics},\\n\\tauthor = {Misochko, 1. O. V. and Kaidashev, E. M. and Georgiev, N. and Dekorsy, T. and Zakharchenko, I. N.},\\n\\tmonth = oct,\\n\\tyear = {2003},\\n\\tkeywords = {Charge Carrier, Elementary Particle, Time Resolution, Transition Region, Wide Temperature Range},\\n\\tpages = {788--793},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\JRJUDEGD\\\\\\\\Misochko и др. - 2003 - A time-resolved optical study of the paramagnetic .pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Misochko, 1. O. V.\",\"Kaidashev, E. M.\",\"Georgiev, N.\",\"Dekorsy, T.\",\"Zakharchenko, I. N.\"],\"key\":\"misochko_time-resolved_2003\",\"id\":\"misochko_time-resolved_2003\",\"bibbaseid\":\"misochko-kaidashev-georgiev-dekorsy-zakharchenko-atimeresolvedopticalstudyoftheparamagneticdielectricferromagneticmetaltransitioninlatextrm07catextrm03mnotextrm3-2003\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/1.1625069\"},\"keyword\":[\"Charge Carrier\",\"Elementary Particle\",\"Time Resolution\",\"Transition Region\",\"Wide Temperature Range\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Dielectric functions (1 to 5 eV) of wurtzite Mg$_{\\\\textrm{x}}$Zn$_{\\\\textrm{1−x}}$O (x⩽0.29) thin films\",\"volume\":\"82\",\"issn\":\"0003-6951\",\"url\":\"https://doi.org/10.1063/1.1565185\",\"doi\":\"10.1063/1.1565185\",\"abstract\":\"The optical dielectric functions for polarization perpendicular and parallel to the c-axis (optical axis) of pulsed-laser-deposition grown wurtzite MgxZn1−xO (0⩽x⩽0.29) thin films have been determined at room temperature using ellipsometry for photon energies from 1 to 5 eV. The dielectric functions reveal strong excitonic contributions for all Mg concentrations x. The band gap energies (E0A=3.369 eV for ZnO to 4.101 eV for x=0.29) show a remarkable blueshift. The exciton binding energy (61 meV for ZnO) decreases to approximately 50 meV for x≈0.17 and increases to approximately 58 meV for x=0.29. In contrast to ZnO, the MgxZn1−xO alloys are found uniaxial negative below the band gap energy, opposite to previously reported results.\",\"number\":\"14\",\"urldate\":\"2023-11-11\",\"journal\":\"Applied Physics Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Schmidt\"],\"firstnames\":[\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rheinländer\"],\"firstnames\":[\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Schubert\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Spemann\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Butz\"],\"firstnames\":[\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lenzner\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rahm\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Semmelhack\"],\"firstnames\":[\"H.\",\"C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2003\",\"pages\":\"2260–2262\",\"bibtex\":\"@article{schmidt_dielectric_2003,\\n\\ttitle = {Dielectric functions (1 to 5 {eV}) of wurtzite {Mg}$_{\\\\textrm{x}}${Zn}$_{\\\\textrm{1−x}}${O} (x⩽0.29) thin films},\\n\\tvolume = {82},\\n\\tissn = {0003-6951},\\n\\turl = {https://doi.org/10.1063/1.1565185},\\n\\tdoi = {10.1063/1.1565185},\\n\\tabstract = {The optical dielectric functions for polarization perpendicular and parallel to the c-axis (optical axis) of pulsed-laser-deposition grown wurtzite MgxZn1−xO (0⩽x⩽0.29) thin films have been determined at room temperature using ellipsometry for photon energies from 1 to 5 eV. The dielectric functions reveal strong excitonic contributions for all Mg concentrations x. The band gap energies (E0A=3.369 eV for ZnO to 4.101 eV for x=0.29) show a remarkable blueshift. The exciton binding energy (61 meV for ZnO) decreases to approximately 50 meV for x≈0.17 and increases to approximately 58 meV for x=0.29. In contrast to ZnO, the MgxZn1−xO alloys are found uniaxial negative below the band gap energy, opposite to previously reported results.},\\n\\tnumber = {14},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Applied Physics Letters},\\n\\tauthor = {Schmidt, R. and Rheinländer, B. and Schubert, M. and Spemann, D. and Butz, T. and Lenzner, J. and Kaidashev, E. M. and Lorenz, M. and Rahm, A. and Semmelhack, H. C. and Grundmann, M.},\\n\\tmonth = apr,\\n\\tyear = {2003},\\n\\tpages = {2260--2262},\\n}\\n\\n\",\"author_short\":[\"Schmidt, R.\",\"Rheinländer, B.\",\"Schubert, M.\",\"Spemann, D.\",\"Butz, T.\",\"Lenzner, J.\",\"Kaidashev, E. M.\",\"Lorenz, M.\",\"Rahm, A.\",\"Semmelhack, H. C.\",\"Grundmann, M.\"],\"key\":\"schmidt_dielectric_2003\",\"id\":\"schmidt_dielectric_2003\",\"bibbaseid\":\"schmidt-rheinlnder-schubert-spemann-butz-lenzner-kaidashev-lorenz-etal-dielectricfunctions1to5evofwurtzitemgtextrmxzntextrm1xox029thinfilms-2003\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.1565185\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Stress relaxation in heteroepitaxial (Ba, Sr)TiO$_{\\\\textrm{3}}$/(001) MgO thin film studied by micro-Raman spectroscopy\",\"volume\":\"68\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.68.104104\",\"doi\":\"10.1103/PhysRevB.68.104104\",\"abstract\":\"The evolution of stresses in a heteroepitaxial (Ba0.7Sr0.3)TiO3/(001)MgO thin film was studied by means of micro-Raman spectroscopy. A small part of the substrate was gradually dissolved, then partially unsupported and completely free-standing areas of the film were studied in a side-view backscattering geometry. The E(TO) soft mode was used to estimate local stresses in the thin film. Our experiments revealed stress relaxation and the gradient of the tetragonal distortion in the partially unsupported ferroelectric thin film. The length scale over which the stress relaxes in the heteroepitaxial film was estimated. The thermal strain arising mostly due to the difference between the thermal-expansion coefficients of the film and the substrate governs the domain structure and induces enhanced tetragonality in the film studied. We found that the partially unsupported thin film is polarization graded due to the stress gradient along the film-substrate interface.\",\"number\":\"10\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"R.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Alyoshin\"],\"firstnames\":[\"V.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zakharchenko\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Markov\"],\"firstnames\":[\"D.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sviridov\"],\"firstnames\":[\"E.\",\"V.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2003\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"104104\",\"bibtex\":\"@article{yuzyuk_stress_2003,\\n\\ttitle = {Stress relaxation in heteroepitaxial ({Ba}, {Sr}){TiO}$_{\\\\textrm{3}}$/(001) {MgO} thin film studied by micro-{Raman} spectroscopy},\\n\\tvolume = {68},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.68.104104},\\n\\tdoi = {10.1103/PhysRevB.68.104104},\\n\\tabstract = {The evolution of stresses in a heteroepitaxial (Ba0.7Sr0.3)TiO3/(001)MgO thin film was studied by means of micro-Raman spectroscopy. A small part of the substrate was gradually dissolved, then partially unsupported and completely free-standing areas of the film were studied in a side-view backscattering geometry. The E(TO) soft mode was used to estimate local stresses in the thin film. Our experiments revealed stress relaxation and the gradient of the tetragonal distortion in the partially unsupported ferroelectric thin film. The length scale over which the stress relaxes in the heteroepitaxial film was estimated. The thermal strain arising mostly due to the difference between the thermal-expansion coefficients of the film and the substrate governs the domain structure and induces enhanced tetragonality in the film studied. We found that the partially unsupported thin film is polarization graded due to the stress gradient along the film-substrate interface.},\\n\\tnumber = {10},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Yuzyuk, Yu. I. and Katiyar, R. S. and Alyoshin, V. A. and Zakharchenko, I. N. and Markov, D. A. and Sviridov, E. V.},\\n\\tmonth = sep,\\n\\tyear = {2003},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {104104},\\n}\\n\\n\",\"author_short\":[\"Yuzyuk, Y. I.\",\"Katiyar, R. S.\",\"Alyoshin, V. A.\",\"Zakharchenko, I. N.\",\"Markov, D. A.\",\"Sviridov, E. V.\"],\"key\":\"yuzyuk_stress_2003\",\"id\":\"yuzyuk_stress_2003\",\"bibbaseid\":\"yuzyuk-katiyar-alyoshin-zakharchenko-markov-sviridov-stressrelaxationinheteroepitaxialbasrtiotextrm3001mgothinfilmstudiedbymicroramanspectroscopy-2003\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.68.104104\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Phase transitions in (Ba$_{\\\\textrm{0.7}}$Sr$_{\\\\textrm{0.3}}$)TiO$_{\\\\textrm{3}}$/(001)MgO thin film studied by Raman scattering\",\"volume\":\"93\",\"issn\":\"0021-8979\",\"url\":\"https://doi.org/10.1063/1.1574173\",\"doi\":\"10.1063/1.1574173\",\"abstract\":\"Polarized Raman spectra of heteroepitaxial (Ba0.7Sr0.3)TiO3 thin film deposited on the (001)MgO substrate have been studied in the broad temperature range from 30 to 1300 K. Our results show that the ferroelectric–paraelectric phase transition is markedly shifted to higher temperatures with respect to the bulk ceramics of the same composition. Because of the two-dimensional compressive stresses imposed on the film by the substrate, the symmetry of the paraelectric phase is found to be tetragonal well above the Curie temperature. Near the deposition temperature (1173 K), the thermoelastic compressive stresses vanish and Raman response suggests nearly cubic symmetry. Raman measurements below room temperature show clearly that the phase transition to the rhombohedral phase is completely suppressed and only one phase transition from the tetragonal to the monoclinic phase is revealed at ∼150 K.\",\"number\":\"12\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Applied Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sauvajol\"],\"firstnames\":[\"J.\",\"L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Simon\"],\"firstnames\":[\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorman\"],\"firstnames\":[\"V.\",\"L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Alyoshin\"],\"firstnames\":[\"V.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zakharchenko\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sviridov\"],\"firstnames\":[\"E.\",\"V.\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2003\",\"pages\":\"9930–9937\",\"bibtex\":\"@article{yuzyuk_phase_2003,\\n\\ttitle = {Phase transitions in ({Ba}$_{\\\\textrm{0.7}}${Sr}$_{\\\\textrm{0.3}}$){TiO}$_{\\\\textrm{3}}$/(001){MgO} thin film studied by {Raman} scattering},\\n\\tvolume = {93},\\n\\tissn = {0021-8979},\\n\\turl = {https://doi.org/10.1063/1.1574173},\\n\\tdoi = {10.1063/1.1574173},\\n\\tabstract = {Polarized Raman spectra of heteroepitaxial (Ba0.7Sr0.3)TiO3 thin film deposited on the (001)MgO substrate have been studied in the broad temperature range from 30 to 1300 K. Our results show that the ferroelectric–paraelectric phase transition is markedly shifted to higher temperatures with respect to the bulk ceramics of the same composition. Because of the two-dimensional compressive stresses imposed on the film by the substrate, the symmetry of the paraelectric phase is found to be tetragonal well above the Curie temperature. Near the deposition temperature (1173 K), the thermoelastic compressive stresses vanish and Raman response suggests nearly cubic symmetry. Raman measurements below room temperature show clearly that the phase transition to the rhombohedral phase is completely suppressed and only one phase transition from the tetragonal to the monoclinic phase is revealed at ∼150 K.},\\n\\tnumber = {12},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Applied Physics},\\n\\tauthor = {Yuzyuk, Yu. I. and Sauvajol, J. L. and Simon, P. and Lorman, V. L. and Alyoshin, V. A. and Zakharchenko, I. N. and Sviridov, E. V.},\\n\\tmonth = may,\\n\\tyear = {2003},\\n\\tpages = {9930--9937},\\n}\\n\\n\",\"author_short\":[\"Yuzyuk, Y. I.\",\"Sauvajol, J. L.\",\"Simon, P.\",\"Lorman, V. L.\",\"Alyoshin, V. A.\",\"Zakharchenko, I. N.\",\"Sviridov, E. V.\"],\"key\":\"yuzyuk_phase_2003\",\"id\":\"yuzyuk_phase_2003\",\"bibbaseid\":\"yuzyuk-sauvajol-simon-lorman-alyoshin-zakharchenko-sviridov-phasetransitionsinbatextrm07srtextrm03tiotextrm3001mgothinfilmstudiedbyramanscattering-2003\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.1574173\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Comment on ``Structural ordering transition and repulsion of the giant LO-TO splitting in polycrystalline Ba$_{\\\\textrm{x}}$Sr$_{\\\\textrm{1-x}}$TiO$_{\\\\textrm{3}}$\",\"volume\":\"68\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.68.216101\",\"doi\":\"10.1103/PhysRevB.68.216101\",\"abstract\":\"Recently, Kuo et al. [S.-Y. Kuo, W.-Y. Liao, and W.-F. Hsieh, Phys. Rev. B 64, 224103 (2001)] reported a new structural ordering in sol-gel derived polycrystalline BaxSr1−xTiO3 around x≈0.4–0.5 at room temperature. We show that unpolarized Raman data obtained in this work were analyzed incorrectly. As a consequence, conclusions derived from Raman-scattering experiments in the above paper are questionable.\",\"number\":\"21\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Simon\"],\"firstnames\":[\"P.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2003\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"216101\",\"bibtex\":\"@article{yuzyuk_comment_2003,\\n\\ttitle = {Comment on ``{Structural} ordering transition and repulsion of the giant {LO}-{TO} splitting in polycrystalline {Ba}$_{\\\\textrm{x}}${Sr}$_{\\\\textrm{1-x}}${TiO}$_{\\\\textrm{3}}$},\\n\\tvolume = {68},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.68.216101},\\n\\tdoi = {10.1103/PhysRevB.68.216101},\\n\\tabstract = {Recently, Kuo et al. [S.-Y. Kuo, W.-Y. Liao, and W.-F. Hsieh, Phys. Rev. B 64, 224103 (2001)] reported a new structural ordering in sol-gel derived polycrystalline BaxSr1−xTiO3 around x≈0.4–0.5 at room temperature. We show that unpolarized Raman data obtained in this work were analyzed incorrectly. As a consequence, conclusions derived from Raman-scattering experiments in the above paper are questionable.},\\n\\tnumber = {21},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Yuzyuk, Yu. I. and Simon, P.},\\n\\tmonth = dec,\\n\\tyear = {2003},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {216101},\\n}\\n\\n\",\"author_short\":[\"Yuzyuk, Y. I.\",\"Simon, P.\"],\"key\":\"yuzyuk_comment_2003\",\"id\":\"yuzyuk_comment_2003\",\"bibbaseid\":\"yuzyuk-simon-commentonstructuralorderingtransitionandrepulsionofthegiantlotosplittinginpolycrystallinebatextrmxsrtextrm1xtiotextrm3-2003\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.68.216101\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Infrared dielectric functions and phonon modes of wurtzite Mg$_{\\\\textrm{x}}$Zn$_{\\\\textrm{1−x}}$O (x⩽0.2)\",\"volume\":\"81\",\"issn\":\"0003-6951\",\"url\":\"https://doi.org/10.1063/1.1509862\",\"doi\":\"10.1063/1.1509862\",\"abstract\":\"Infrared dielectric function spectra and phonon modes with polarization parallel and perpendicular to the c axis of high quality, highly relaxed, and single crystalline wurtzite MgxZn1−xO films with 0⩽x⩽0.2 prepared by pulsed-laser deposition on c-plane sapphire substrates were obtained from infrared spectroscopic ellipsometry (380–1200 cm−1) and Raman scattering studies. A two-mode behavior is found for the modes with E1 symmetry, a lattice mode and an impurity-type mode are obtained for the A1 symmetry phonons. Model dielectric function spectra will become useful for future infrared ellipsometry analysis of complex MgxZn1−xO-based heterostructures.\",\"number\":\"13\",\"urldate\":\"2023-11-11\",\"journal\":\"Applied Physics Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Bundesmann\"],\"firstnames\":[\"C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Schubert\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Spemann\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Butz\"],\"firstnames\":[\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ashkenov\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Neumann\"],\"firstnames\":[\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Wagner\"],\"firstnames\":[\"G.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2002\",\"pages\":\"2376–2378\",\"file\":\"Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\MGX7XX67\\\\\\\\Infrared-dielectric-functions-and-phonon-modes-of.html:text/html\",\"bibtex\":\"@article{bundesmann_infrared_2002,\\n\\ttitle = {Infrared dielectric functions and phonon modes of wurtzite {Mg}$_{\\\\textrm{x}}${Zn}$_{\\\\textrm{1−x}}${O} (x⩽0.2)},\\n\\tvolume = {81},\\n\\tissn = {0003-6951},\\n\\turl = {https://doi.org/10.1063/1.1509862},\\n\\tdoi = {10.1063/1.1509862},\\n\\tabstract = {Infrared dielectric function spectra and phonon modes with polarization parallel and perpendicular to the c axis of high quality, highly relaxed, and single crystalline wurtzite MgxZn1−xO films with 0⩽x⩽0.2 prepared by pulsed-laser deposition on c-plane sapphire substrates were obtained from infrared spectroscopic ellipsometry (380–1200 cm−1) and Raman scattering studies. A two-mode behavior is found for the modes with E1 symmetry, a lattice mode and an impurity-type mode are obtained for the A1 symmetry phonons. Model dielectric function spectra will become useful for future infrared ellipsometry analysis of complex MgxZn1−xO-based heterostructures.},\\n\\tnumber = {13},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Applied Physics Letters},\\n\\tauthor = {Bundesmann, C. and Schubert, M. and Spemann, D. and Butz, T. and Lorenz, M. and Kaidashev, E. M. and Grundmann, M. and Ashkenov, N. and Neumann, H. and Wagner, G.},\\n\\tmonth = sep,\\n\\tyear = {2002},\\n\\tpages = {2376--2378},\\n\\tfile = {Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\MGX7XX67\\\\\\\\Infrared-dielectric-functions-and-phonon-modes-of.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Bundesmann, C.\",\"Schubert, M.\",\"Spemann, D.\",\"Butz, T.\",\"Lorenz, M.\",\"Kaidashev, E. M.\",\"Grundmann, M.\",\"Ashkenov, N.\",\"Neumann, H.\",\"Wagner, G.\"],\"key\":\"bundesmann_infrared_2002\",\"id\":\"bundesmann_infrared_2002\",\"bibbaseid\":\"bundesmann-schubert-spemann-butz-lorenz-kaidashev-grundmann-ashkenov-etal-infrareddielectricfunctionsandphononmodesofwurtzitemgtextrmxzntextrm1xox02-2002\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.1509862\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Polarization-dependent Raman spectra of heteroepitaxial (Ba, Sr)TiO$_{\\\\textrm{3}}$/(001) MgO thin films\",\"volume\":\"65\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.65.134107\",\"doi\":\"10.1103/PhysRevB.65.134107\",\"abstract\":\"We have studied the concentration dependence of the Raman spectra of heteroepitaxial (Ba1−xSrx)TiO3 (BST) (x=0, 0.15, 0.30, and 0.45) thin films deposited by rf sputtering on (001) MgO substrates. It is found that substitution of Ba by Sr leads to the distortions of the Ti-O bonds and causes the appearance of new bands in the Raman spectra near the bands corresponding to the Ti-O vibrations. The Sr incorporation induces relatively large shifts of the low-frequency Raman peaks attributed to ETO and A1TO components of the soft mode. The ETO soft mode in BST films becomes underdamped for x\\\\textgreater~0.3 and is very sensitive to the two-dimensional compressive stresses.\",\"number\":\"13\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Alyoshin\"],\"firstnames\":[\"V.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zakharchenko\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sviridov\"],\"firstnames\":[\"E.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Almeida\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chaves\"],\"firstnames\":[\"M.\",\"R.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2002\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"134107\",\"file\":\"APS Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\DIUXSDGU\\\\¶hysRevB.65.html:text/html\",\"bibtex\":\"@article{yuzyuk_polarization-dependent_2002,\\n\\ttitle = {Polarization-dependent {Raman} spectra of heteroepitaxial ({Ba}, {Sr}){TiO}$_{\\\\textrm{3}}$/(001) {MgO} thin films},\\n\\tvolume = {65},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.65.134107},\\n\\tdoi = {10.1103/PhysRevB.65.134107},\\n\\tabstract = {We have studied the concentration dependence of the Raman spectra of heteroepitaxial (Ba1−xSrx)TiO3 (BST) (x=0, 0.15, 0.30, and 0.45) thin films deposited by rf sputtering on (001) MgO substrates. It is found that substitution of Ba by Sr leads to the distortions of the Ti-O bonds and causes the appearance of new bands in the Raman spectra near the bands corresponding to the Ti-O vibrations. The Sr incorporation induces relatively large shifts of the low-frequency Raman peaks attributed to ETO and A1TO components of the soft mode. The ETO soft mode in BST films becomes underdamped for x{\\\\textgreater}{\\\\textasciitilde}0.3 and is very sensitive to the two-dimensional compressive stresses.},\\n\\tnumber = {13},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Yuzyuk, Yu. I. and Alyoshin, V. A. and Zakharchenko, I. N. and Sviridov, E. V. and Almeida, A. and Chaves, M. R.},\\n\\tmonth = mar,\\n\\tyear = {2002},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {134107},\\n\\tfile = {APS Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\DIUXSDGU\\\\\\\\PhysRevB.65.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Yuzyuk, Y. I.\",\"Alyoshin, V. A.\",\"Zakharchenko, I. N.\",\"Sviridov, E. V.\",\"Almeida, A.\",\"Chaves, M. R.\"],\"key\":\"yuzyuk_polarization-dependent_2002\",\"id\":\"yuzyuk_polarization-dependent_2002\",\"bibbaseid\":\"yuzyuk-alyoshin-zakharchenko-sviridov-almeida-chaves-polarizationdependentramanspectraofheteroepitaxialbasrtiotextrm3001mgothinfilms-2002\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.65.134107\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Stress effect on the ferroelectric-to-paraelectric phase transition in heteroepitaxial (Ba, Sr)TiO$_{\\\\textrm{3}}$/(001) MgO thin film studied by Raman scattering and x-ray diffraction\",\"volume\":\"66\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.66.052103\",\"doi\":\"10.1103/PhysRevB.66.052103\",\"abstract\":\"We report experimental evidence for the stress-induced tetragonal symmetry of the paraelectric phase in heteroepitaxial (Ba0.7Sr0.3)TiO3 thin film deposited on the (001)MgO substrate. Our Raman and x-ray-diffraction data evidently show that symmetry of the paraelectric phase is tetragonal well above the Curie temperature due to the two-dimensional compressive stresses imposed on the film by the substrate. On approaching the deposition temperature the thermoelastic compressive stresses vanish and Raman measurements revealed cubic symmetry of the paraelectric phase.\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Simon\"],\"firstnames\":[\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zakharchenko\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Alyoshin\"],\"firstnames\":[\"V.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sviridov\"],\"firstnames\":[\"E.\",\"V.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2002\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"052103\",\"file\":\"APS Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\B9REP2NW\\\\¶hysRevB.66.html:text/html\",\"bibtex\":\"@article{yuzyuk_stress_2002,\\n\\ttitle = {Stress effect on the ferroelectric-to-paraelectric phase transition in heteroepitaxial ({Ba}, {Sr}){TiO}$_{\\\\textrm{3}}$/(001) {MgO} thin film studied by {Raman} scattering and x-ray diffraction},\\n\\tvolume = {66},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.66.052103},\\n\\tdoi = {10.1103/PhysRevB.66.052103},\\n\\tabstract = {We report experimental evidence for the stress-induced tetragonal symmetry of the paraelectric phase in heteroepitaxial (Ba0.7Sr0.3)TiO3 thin film deposited on the (001)MgO substrate. Our Raman and x-ray-diffraction data evidently show that symmetry of the paraelectric phase is tetragonal well above the Curie temperature due to the two-dimensional compressive stresses imposed on the film by the substrate. On approaching the deposition temperature the thermoelastic compressive stresses vanish and Raman measurements revealed cubic symmetry of the paraelectric phase.},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Yuzyuk, Yu. I. and Simon, P. and Zakharchenko, I. N. and Alyoshin, V. A. and Sviridov, E. V.},\\n\\tmonth = aug,\\n\\tyear = {2002},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {052103},\\n\\tfile = {APS Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\B9REP2NW\\\\\\\\PhysRevB.66.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Yuzyuk, Y. I.\",\"Simon, P.\",\"Zakharchenko, I. N.\",\"Alyoshin, V. A.\",\"Sviridov, E. V.\"],\"key\":\"yuzyuk_stress_2002\",\"id\":\"yuzyuk_stress_2002\",\"bibbaseid\":\"yuzyuk-simon-zakharchenko-alyoshin-sviridov-stresseffectontheferroelectrictoparaelectricphasetransitioninheteroepitaxialbasrtiotextrm3001mgothinfilmstudiedbyramanscatteringandxraydiffraction-2002\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.66.052103\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Crystal Structure and the Spectral Response of the Ba‐Doped SrTiO$_{\\\\textrm{3}}$ Incipient Ferroelectrics\",\"volume\":\"258\",\"issn\":\"0370-1972, 1521-3951\",\"url\":\"https://onlinelibrary.wiley.com/doi/10.1002/pssb.202100010\",\"doi\":\"10.1002/pssb.202100010\",\"abstract\":\"The crystal structure and lattice dynamics of quantum paraelectric Ba x Sr 1− x TiO 3 ( x  = 0, 0.01, 0.02) solid solutions are studied using X‐ray diffraction (XRD), Raman and terahertz‐infrared (THz‐IR) spectroscopies in a temperature range of 4–300 K. XRD and Raman spectroscopy reveal the cubic‐to‐tetragonal nonpolar structural phase transition at about 100 K. At the same time, Raman spectra manifest the presence of polar modes, TO 2 and TO 4 , normally prohibited in paraelectric phase. Emergence of these modes indicates the appearance of the polar nanoregions in a broad temperature range. The modes become more intensive at low temperatures, and temperature dependence of their intensities on cooling reveals the kink‐like change of the slope from flat to steep, indicating on activation of polar nanoregions. The transmission THz‐IR spectra show that squared frequency of the polar TO 1 soft mode, responsible for ferroelectric transition, follows Cochran's behavior at high temperatures. However, at low temperatures, it doesn't vanish at extrapolated Curie temperature but saturates, demonstrating the plateau feature below 20 K. This behavior, coherent with known saturation of the dielectric constant, indicates that transition to ferroelectric phase in Ba x Sr 1− x TiO 3 is suppressed by quantum fluctuations and the system stays in quantum paraelectric state at very low temperatures.\",\"language\":\"en\",\"number\":\"7\",\"urldate\":\"2023-11-10\",\"journal\":\"physica status solidi (b)\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Linnik\"],\"firstnames\":[\"Ekaterina\",\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lukyanchuk\"],\"firstnames\":[\"Igor\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"Alexey\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ragulya\"],\"firstnames\":[\"Andrey\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"Boris\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Alyabyeva\"],\"firstnames\":[\"Liudmila\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukov\"],\"firstnames\":[\"Sergey\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzane\"],\"firstnames\":[\"Daoud\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"Anna\",\"G.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2021\",\"pages\":\"2100010\",\"bibtex\":\"@article{linnik_crystal_2021,\\n\\ttitle = {Crystal {Structure} and the {Spectral} {Response} of the {Ba}‐{Doped} {SrTiO}$_{\\\\textrm{3}}$ {Incipient} {Ferroelectrics}},\\n\\tvolume = {258},\\n\\tissn = {0370-1972, 1521-3951},\\n\\turl = {https://onlinelibrary.wiley.com/doi/10.1002/pssb.202100010},\\n\\tdoi = {10.1002/pssb.202100010},\\n\\tabstract = {The crystal structure and lattice dynamics of quantum paraelectric Ba\\n                \\n                  x\\n                \\n                Sr\\n                \\n                  1−\\n                  x\\n                \\n                TiO\\n                3\\n                (\\n                x\\n                 = 0, 0.01, 0.02) solid solutions are studied using X‐ray diffraction (XRD), Raman and terahertz‐infrared (THz‐IR) spectroscopies in a temperature range of 4–300 K. XRD and Raman spectroscopy reveal the cubic‐to‐tetragonal nonpolar structural phase transition at about 100 K. At the same time, Raman spectra manifest the presence of polar modes, TO\\n                2\\n                and TO\\n                4\\n                , normally prohibited in paraelectric phase. Emergence of these modes indicates the appearance of the polar nanoregions in a broad temperature range. The modes become more intensive at low temperatures, and temperature dependence of their intensities on cooling reveals the kink‐like change of the slope from flat to steep, indicating on activation of polar nanoregions. The transmission THz‐IR spectra show that squared frequency of the polar TO\\n                1\\n                soft mode, responsible for ferroelectric transition, follows Cochran's behavior at high temperatures. However, at low temperatures, it doesn't vanish at extrapolated Curie temperature but saturates, demonstrating the plateau feature below 20 K. This behavior, coherent with known saturation of the dielectric constant, indicates that transition to ferroelectric phase in Ba\\n                \\n                  x\\n                \\n                Sr\\n                \\n                  1−\\n                  x\\n                \\n                TiO\\n                3\\n                is suppressed by quantum fluctuations and the system stays in quantum paraelectric state at very low temperatures.},\\n\\tlanguage = {en},\\n\\tnumber = {7},\\n\\turldate = {2023-11-10},\\n\\tjournal = {physica status solidi (b)},\\n\\tauthor = {Linnik, Ekaterina D. and Lukyanchuk, Igor A. and Mikheykin, Alexey S. and Ragulya, Andrey V. and Gorshunov, Boris P. and Alyabyeva, Liudmila N. and Zhukov, Sergey S. and Mezzane, Daoud and Razumnaya, Anna G.},\\n\\tmonth = jul,\\n\\tyear = {2021},\\n\\tpages = {2100010},\\n}\\n\\n\",\"author_short\":[\"Linnik, E. D.\",\"Lukyanchuk, I. A.\",\"Mikheykin, A. S.\",\"Ragulya, A. V.\",\"Gorshunov, B. P.\",\"Alyabyeva, L. N.\",\"Zhukov, S. S.\",\"Mezzane, D.\",\"Razumnaya, A. G.\"],\"key\":\"linnik_crystal_2021\",\"id\":\"linnik_crystal_2021\",\"bibbaseid\":\"linnik-lukyanchuk-mikheykin-ragulya-gorshunov-alyabyeva-zhukov-mezzane-etal-crystalstructureandthespectralresponseofthebadopedsrtiotextrm3incipientferroelectrics-2021\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://onlinelibrary.wiley.com/doi/10.1002/pssb.202100010\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"The ferroelectric field-effect transistor with negative capacitance\",\"volume\":\"8\",\"issn\":\"2057-3960\",\"url\":\"https://www.nature.com/articles/s41524-022-00738-2\",\"doi\":\"10.1038/s41524-022-00738-2\",\"abstract\":\"Abstract Integrating ferroelectric negative capacitance (NC) into the field-effect transistor (FET) promises to break fundamental limits of power dissipation known as Boltzmann tyranny. However, realizing the stable static negative capacitance in the non-transient non-hysteretic regime remains a daunting task. The problem stems from the lack of understanding of how the fundamental origin of the NC due to the emergence of the domain state can be put in use for implementing the NC FET. Here we put forth an ingenious design for the ferroelectric domain-based field-effect transistor with the stable reversible static negative capacitance. Using dielectric coating of the ferroelectric capacitor enables the tunability of the negative capacitance improving tremendously the performance of the field-effect transistors.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"npj Computational Materials\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Luk’yanchuk\"],\"firstnames\":[\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sené\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tikhonov\"],\"firstnames\":[\"Y.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vinokur\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2022\",\"pages\":\"52\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\RNZJZAMQ\\\\Łuk’yanchuk и др. - 2022 - The ferroelectric field-effect transistor with neg.pdf:application/pdf;Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\NWIGDCZ5\\\\Łuk’yanchuk и др. - 2022 - The ferroelectric field-effect transistor with neg.pdf:application/pdf\",\"bibtex\":\"@article{lukyanchuk_ferroelectric_2022,\\n\\ttitle = {The ferroelectric field-effect transistor with negative capacitance},\\n\\tvolume = {8},\\n\\tissn = {2057-3960},\\n\\turl = {https://www.nature.com/articles/s41524-022-00738-2},\\n\\tdoi = {10.1038/s41524-022-00738-2},\\n\\tabstract = {Abstract\\n            Integrating ferroelectric negative capacitance (NC) into the field-effect transistor (FET) promises to break fundamental limits of power dissipation known as Boltzmann tyranny. However, realizing the stable static negative capacitance in the non-transient non-hysteretic regime remains a daunting task. The problem stems from the lack of understanding of how the fundamental origin of the NC due to the emergence of the domain state can be put in use for implementing the NC FET. Here we put forth an ingenious design for the ferroelectric domain-based field-effect transistor with the stable reversible static negative capacitance. Using dielectric coating of the ferroelectric capacitor enables the tunability of the negative capacitance improving tremendously the performance of the field-effect transistors.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {npj Computational Materials},\\n\\tauthor = {Luk’yanchuk, I. and Razumnaya, A. and Sené, A. and Tikhonov, Y. and Vinokur, V. M.},\\n\\tmonth = mar,\\n\\tyear = {2022},\\n\\tpages = {52},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\RNZJZAMQ\\\\\\\\Luk’yanchuk и др. - 2022 - The ferroelectric field-effect transistor with neg.pdf:application/pdf;Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\NWIGDCZ5\\\\\\\\Luk’yanchuk и др. - 2022 - The ferroelectric field-effect transistor with neg.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Luk’yanchuk, I.\",\"Razumnaya, A.\",\"Sené, A.\",\"Tikhonov, Y.\",\"Vinokur, V. M.\"],\"key\":\"lukyanchuk_ferroelectric_2022\",\"id\":\"lukyanchuk_ferroelectric_2022\",\"bibbaseid\":\"lukyanchuk-razumnaya-sen-tikhonov-vinokur-theferroelectricfieldeffecttransistorwithnegativecapacitance-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.nature.com/articles/s41524-022-00738-2\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Synthesis of ZnO nanorods for piezoelectric resonators and sensors\",\"volume\":\"12\",\"issn\":\"2010-135X, 2010-1368\",\"url\":\"https://www.worldscientific.com/doi/abs/10.1142/S2010135X21600201\",\"doi\":\"10.1142/S2010135X21600201\",\"abstract\":\"Efficiency of the piezoelectric chemisensors may be considerably enhanced by use of zinc oxide nanorods as sensing elements. ZnO nanorod arrays being good piezoelectric materials possess large surface area, which provides extra benefits for chemisorption and photodetection. Highly oriented nanorod arrays are typically prepared onto highly crystalline substrates, whereas the nanorods growth onto metal contacts meets significant technological difficulties. In this paper, we report on carbothermal, electrochemical, and hydrothermal techniques of ZnO nanorod arrays synthesis on metal contacts. The optical and structural properties of the obtained nanorods were studied using scanning electron microscopy, X-ray diffraction (XRD), Raman spectroscopy, and luminescence spectroscopy. A reliable technique was developed for obtaining ohmic contact with the grown nanorods. I–U curves of prepared contact were studied. Carbothermal synthesis made it possible to obtain the most crystallinely perfect, homogeneous, and dense arrays of nanorods and control the concentration of point defects by changing the synthesis parameters over a wide range. The electrochemical synthesis demonstrated excellent results for synthesis of ZnO nanorods on the surface of resonator electrodes.\",\"language\":\"en\",\"number\":\"01\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Advanced Dielectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Nikolaev\"],\"firstnames\":[\"A.\",\"L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kazmina\"],\"firstnames\":[\"M.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lyanguzov\"],\"firstnames\":[\"N.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Abdulvakhidov\"],\"firstnames\":[\"K.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2022\",\"pages\":\"2160020\",\"bibtex\":\"@article{nikolaev_synthesis_2022,\\n\\ttitle = {Synthesis of {ZnO} nanorods for piezoelectric resonators and sensors},\\n\\tvolume = {12},\\n\\tissn = {2010-135X, 2010-1368},\\n\\turl = {https://www.worldscientific.com/doi/abs/10.1142/S2010135X21600201},\\n\\tdoi = {10.1142/S2010135X21600201},\\n\\tabstract = {Efficiency of the piezoelectric chemisensors may be considerably enhanced by use of zinc oxide nanorods as sensing elements. ZnO nanorod arrays being good piezoelectric materials possess large surface area, which provides extra benefits for chemisorption and photodetection. Highly oriented nanorod arrays are typically prepared onto highly crystalline substrates, whereas the nanorods growth onto metal contacts meets significant technological difficulties. In this paper, we report on carbothermal, electrochemical, and hydrothermal techniques of ZnO nanorod arrays synthesis on metal contacts. The optical and structural properties of the obtained nanorods were studied using scanning electron microscopy, X-ray diffraction (XRD), Raman spectroscopy, and luminescence spectroscopy. A reliable technique was developed for obtaining ohmic contact with the grown nanorods. I–U curves of prepared contact were studied. Carbothermal synthesis made it possible to obtain the most crystallinely perfect, homogeneous, and dense arrays of nanorods and control the concentration of point defects by changing the synthesis parameters over a wide range. The electrochemical synthesis demonstrated excellent results for synthesis of ZnO nanorods on the surface of resonator electrodes.},\\n\\tlanguage = {en},\\n\\tnumber = {01},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Advanced Dielectrics},\\n\\tauthor = {Nikolaev, A. L. and Kazmina, M. A. and Lyanguzov, N. V. and Abdulvakhidov, K. G. and Kaidashev, E. M.},\\n\\tmonth = feb,\\n\\tyear = {2022},\\n\\tpages = {2160020},\\n}\\n\\n\",\"author_short\":[\"Nikolaev, A. L.\",\"Kazmina, M. A.\",\"Lyanguzov, N. V.\",\"Abdulvakhidov, K. G.\",\"Kaidashev, E. M.\"],\"key\":\"nikolaev_synthesis_2022\",\"id\":\"nikolaev_synthesis_2022\",\"bibbaseid\":\"nikolaev-kazmina-lyanguzov-abdulvakhidov-kaidashev-synthesisofznonanorodsforpiezoelectricresonatorsandsensors-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.worldscientific.com/doi/abs/10.1142/S2010135X21600201\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Design of lead-free BCZT-based ceramics with enhanced piezoelectric energy harvesting performances\",\"volume\":\"24\",\"issn\":\"1463-9076, 1463-9084\",\"url\":\"http://xlink.rsc.org/?DOI=D1CP04723J\",\"doi\":\"10.1039/D1CP04723J\",\"abstract\":\"The benefits of the multiphase convergence strategy to design ferroelectric ceramics for piezoelectric energy harvesting applications over a broad temperature range. , The design of lead-free ceramics for piezoelectric energy harvesting applications has become a hot topic. Among these materials, Ba 0.85 Ca 0.15 Zr 0.10 Ti 0.90 O 3 (BCZT) and BaTi 0.89 Sn 0.11 O 3 (BTSn) are considered as potential candidates due to their enhanced piezoelectric properties. Here, the structural, electrical, piezoelectric and piezoelectric energy harvesting properties of the (1 − x )Ba 0.85 Ca 0.15 Zr 0.10 Ti 0.90 O 3 − x BaTi 0.89 Sn 0.11 O 3 ( x BTSn, x = 0.2, 0.4 and 0.6) system are investigated. A systematic study of the structural properties of the x BTSn samples was carried out using X-ray diffraction, Raman spectroscopy, and dielectric measurements. The addition of BTSn allows a successive phase transition, which broadens the application temperature range. The enhanced piezoelectric energy harvesting properties were found in the 0.2BTSn ceramic, where the large-signal and small-signal piezoelectric coefficients, piezoelectric voltage and the piezoelectric figure of merit reached 245 pm V −1 , 228 pC N −1 , 16.2 mV m N −1 and 3.7 pm 2 N −1 , respectively. Consequently, the combination of BCZT and BTSn could provide suitable lead-free materials with enhanced piezoelectric energy harvesting performances.\",\"language\":\"en\",\"number\":\"10\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Chemistry Chemical Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Merselmiz\"],\"firstnames\":[\"Soukaina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hanani\"],\"firstnames\":[\"Zouhair\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prah\"],\"firstnames\":[\"Uroš\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzane\"],\"firstnames\":[\"Daoud\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hajji\"],\"firstnames\":[\"Lahoucine\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Abkhar\"],\"firstnames\":[\"Zahra\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Spreitzer\"],\"firstnames\":[\"Matjaž\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vengust\"],\"firstnames\":[\"Damjan\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Uršič\"],\"firstnames\":[\"Hana\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fabijan\"],\"firstnames\":[\"David\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"Anna\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shapovalova\"],\"firstnames\":[\"Olesia\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Luk'yanchuk\"],\"firstnames\":[\"Igor\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kutnjak\"],\"firstnames\":[\"Zdravko\"],\"suffixes\":[]}],\"year\":\"2022\",\"pages\":\"6026–6036\",\"bibtex\":\"@article{merselmiz_design_2022,\\n\\ttitle = {Design of lead-free {BCZT}-based ceramics with enhanced piezoelectric energy harvesting performances},\\n\\tvolume = {24},\\n\\tissn = {1463-9076, 1463-9084},\\n\\turl = {http://xlink.rsc.org/?DOI=D1CP04723J},\\n\\tdoi = {10.1039/D1CP04723J},\\n\\tabstract = {The benefits of the multiphase convergence strategy to design ferroelectric ceramics for piezoelectric energy harvesting applications over a broad temperature range.\\n          , \\n            \\n              The design of lead-free ceramics for piezoelectric energy harvesting applications has become a hot topic. Among these materials, Ba\\n              0.85\\n              Ca\\n              0.15\\n              Zr\\n              0.10\\n              Ti\\n              0.90\\n              O\\n              3\\n              (BCZT) and BaTi\\n              0.89\\n              Sn\\n              0.11\\n              O\\n              3\\n              (BTSn) are considered as potential candidates due to their enhanced piezoelectric properties. Here, the structural, electrical, piezoelectric and piezoelectric energy harvesting properties of the (1 −\\n              x\\n              )Ba\\n              0.85\\n              Ca\\n              0.15\\n              Zr\\n              0.10\\n              Ti\\n              0.90\\n              O\\n              3\\n              −\\n              x\\n              BaTi\\n              0.89\\n              Sn\\n              0.11\\n              O\\n              3\\n              (\\n              x\\n              BTSn,\\n              x\\n              = 0.2, 0.4 and 0.6) system are investigated. A systematic study of the structural properties of the\\n              x\\n              BTSn samples was carried out using X-ray diffraction, Raman spectroscopy, and dielectric measurements. The addition of BTSn allows a successive phase transition, which broadens the application temperature range. The enhanced piezoelectric energy harvesting properties were found in the 0.2BTSn ceramic, where the large-signal and small-signal piezoelectric coefficients, piezoelectric voltage and the piezoelectric figure of merit reached 245 pm V\\n              −1\\n              , 228 pC N\\n              −1\\n              , 16.2 mV m N\\n              −1\\n              and 3.7 pm\\n              2\\n              N\\n              −1\\n              , respectively. Consequently, the combination of BCZT and BTSn could provide suitable lead-free materials with enhanced piezoelectric energy harvesting performances.},\\n\\tlanguage = {en},\\n\\tnumber = {10},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Chemistry Chemical Physics},\\n\\tauthor = {Merselmiz, Soukaina and Hanani, Zouhair and Prah, Uroš and Mezzane, Daoud and Hajji, Lahoucine and Abkhar, Zahra and Spreitzer, Matjaž and Vengust, Damjan and Uršič, Hana and Fabijan, David and Razumnaya, Anna G. and Shapovalova, Olesia and Luk'yanchuk, Igor A. and Kutnjak, Zdravko},\\n\\tyear = {2022},\\n\\tpages = {6026--6036},\\n}\\n\\n\",\"author_short\":[\"Merselmiz, S.\",\"Hanani, Z.\",\"Prah, U.\",\"Mezzane, D.\",\"Hajji, L.\",\"Abkhar, Z.\",\"Spreitzer, M.\",\"Vengust, D.\",\"Uršič, H.\",\"Fabijan, D.\",\"Razumnaya, A. G.\",\"Shapovalova, O.\",\"Luk'yanchuk, I. A.\",\"Kutnjak, Z.\"],\"key\":\"merselmiz_design_2022\",\"id\":\"merselmiz_design_2022\",\"bibbaseid\":\"merselmiz-hanani-prah-mezzane-hajji-abkhar-spreitzer-vengust-etal-designofleadfreebcztbasedceramicswithenhancedpiezoelectricenergyharvestingperformances-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://xlink.rsc.org/?DOI=D1CP04723J\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Graphene structures prepared via pulse alternating current technique\",\"volume\":\"32\",\"issn\":\"09599436\",\"url\":\"https://linkinghub.elsevier.com/retrieve/pii/S0959943622001249\",\"doi\":\"10.1016/j.mencom.2022.05.005\",\"language\":\"en\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Mendeleev Communications\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"Alexandra\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Avramenko\"],\"firstnames\":[\"Marina\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Faddeev\"],\"firstnames\":[\"Nikita\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\",\"V.\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2022\",\"pages\":\"308–310\",\"bibtex\":\"@article{kuriganova_graphene_2022,\\n\\ttitle = {Graphene structures prepared via pulse alternating current technique},\\n\\tvolume = {32},\\n\\tissn = {09599436},\\n\\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0959943622001249},\\n\\tdoi = {10.1016/j.mencom.2022.05.005},\\n\\tlanguage = {en},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Mendeleev Communications},\\n\\tauthor = {Kuriganova, Alexandra B. and Leontyev, Igor N. and Avramenko, Marina V. and Faddeev, Nikita A. and Smirnova, Nina V.},\\n\\tmonth = may,\\n\\tyear = {2022},\\n\\tpages = {308--310},\\n}\\n\\n\",\"author_short\":[\"Kuriganova, A. B.\",\"Leontyev, I. N.\",\"Avramenko, M. V.\",\"Faddeev, N. A.\",\"Smirnova, N. V.\"],\"key\":\"kuriganova_graphene_2022\",\"id\":\"kuriganova_graphene_2022\",\"bibbaseid\":\"kuriganova-leontyev-avramenko-faddeev-smirnova-graphenestructurespreparedviapulsealternatingcurrenttechnique-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://linkinghub.elsevier.com/retrieve/pii/S0959943622001249\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Ferromagnetoelectric phases of hexaferrites: a group-theoretical analysis\",\"volume\":\"77\",\"issn\":\"2052-5206\",\"shorttitle\":\"Ferromagnetoelectric phases of hexaferrites\",\"url\":\"https://scripts.iucr.org/cgi-bin/paper?S2052520621007125\",\"doi\":\"10.1107/S2052520621007125\",\"abstract\":\"A symmetry-guided approach for designing and tailoring magnetoelectric and multiferroic hexaferrites is proposed. A group-theoretical study of the magnetoferroelectric structures of a hexagonal ferrite was carried out. The results were applied to M-, W- and Z-type hexaferrites. It is shown that the magnetic structure cannot be collinear in the main magnetic phase, with the direction of the magnetic moment along the hexagonal axis. Magnetic sublattices are shown in which cation substitution should lead to the formation of a multiferroic state. A thermodynamic model of a hexagonal ferroelectric ferrimagnet was constructed, in which isostructural phase transitions were observed.\",\"number\":\"5\",\"urldate\":\"2023-11-10\",\"journal\":\"Acta Crystallographica Section B Structural Science, Crystal Engineering and Materials\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"Vladimir\",\"Borisovich\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"Anna\",\"Grigoryevna\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"Alexey\",\"Sergeevich\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2021\",\"pages\":\"740–748\",\"bibtex\":\"@article{shirokov_ferromagnetoelectric_2021,\\n\\ttitle = {Ferromagnetoelectric phases of hexaferrites: a group-theoretical analysis},\\n\\tvolume = {77},\\n\\tissn = {2052-5206},\\n\\tshorttitle = {Ferromagnetoelectric phases of hexaferrites},\\n\\turl = {https://scripts.iucr.org/cgi-bin/paper?S2052520621007125},\\n\\tdoi = {10.1107/S2052520621007125},\\n\\tabstract = {A symmetry-guided approach for designing and tailoring magnetoelectric and multiferroic hexaferrites is proposed. A group-theoretical study of the magnetoferroelectric structures of a hexagonal ferrite was carried out. The results were applied to M-, W- and Z-type hexaferrites. It is shown that the magnetic structure cannot be collinear in the main magnetic phase, with the direction of the magnetic moment along the hexagonal axis. Magnetic sublattices are shown in which cation substitution should lead to the formation of a multiferroic state. A thermodynamic model of a hexagonal ferroelectric ferrimagnet was constructed, in which isostructural phase transitions were observed.},\\n\\tnumber = {5},\\n\\turldate = {2023-11-10},\\n\\tjournal = {Acta Crystallographica Section B Structural Science, Crystal Engineering and Materials},\\n\\tauthor = {Shirokov, Vladimir Borisovich and Razumnaya, Anna Grigoryevna and Mikheykin, Alexey Sergeevich},\\n\\tmonth = oct,\\n\\tyear = {2021},\\n\\tpages = {740--748},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Razumnaya, A. G.\",\"Mikheykin, A. S.\"],\"key\":\"shirokov_ferromagnetoelectric_2021\",\"id\":\"shirokov_ferromagnetoelectric_2021\",\"bibbaseid\":\"shirokov-razumnaya-mikheykin-ferromagnetoelectricphasesofhexaferritesagrouptheoreticalanalysis-2021\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://scripts.iucr.org/cgi-bin/paper?S2052520621007125\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Modeling and live imaging of mechanical instabilities in the zebrafish aorta during hematopoiesis\",\"volume\":\"11\",\"issn\":\"2045-2322\",\"url\":\"https://www.nature.com/articles/s41598-021-88667-w\",\"doi\":\"10.1038/s41598-021-88667-w\",\"abstract\":\"Abstract All blood cells originate from hematopoietic stem/progenitor cells (HSPCs). HSPCs are formed from endothelial cells (ECs) of the dorsal aorta (DA), via endothelial-to-hematopoietic transition (EHT). The zebrafish is a primary model organism to study the process in vivo. While the role of mechanical stress in controlling gene expression promoting cell differentiation is actively investigated, mechanisms driving shape changes of the DA and individual ECs remain poorly understood. We address this problem by developing a new DA micromechanical model and applying it to experimental data on zebrafish morphogenesis. The model considers the DA as an isotropic tubular membrane subjected to hydrostatic blood pressure and axial stress. The DA evolution is described as a movement in the dimensionless controlling parameters space: normalized hydrostatic pressure and axial stress. We argue that HSPC production is accompanied by two mechanical instabilities arising in the system due to the plane stress in the DA walls and show how a complex interplay between mechanical forces in the system drives the emerging morphological changes.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-10\",\"journal\":\"Scientific Reports\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Chalin\"],\"firstnames\":[\"Dmitrii\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bureau\"],\"firstnames\":[\"Charlotte\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Parmeggiani\"],\"firstnames\":[\"Andrea\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergei\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kissa\"],\"firstnames\":[\"Karima\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golushko\"],\"firstnames\":[\"Ivan\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2021\",\"pages\":\"9316\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\¶XM8A3B8\\\\\\\\Chalin и др. - 2021 - Modeling and live imaging of mechanical instabilit.pdf:application/pdf\",\"bibtex\":\"@article{chalin_modeling_2021,\\n\\ttitle = {Modeling and live imaging of mechanical instabilities in the zebrafish aorta during hematopoiesis},\\n\\tvolume = {11},\\n\\tissn = {2045-2322},\\n\\turl = {https://www.nature.com/articles/s41598-021-88667-w},\\n\\tdoi = {10.1038/s41598-021-88667-w},\\n\\tabstract = {Abstract\\n            All blood cells originate from hematopoietic stem/progenitor cells (HSPCs). HSPCs are formed from endothelial cells (ECs) of the dorsal aorta (DA), via endothelial-to-hematopoietic transition (EHT). The zebrafish is a primary model organism to study the process in vivo. While the role of mechanical stress in controlling gene expression promoting cell differentiation is actively investigated, mechanisms driving shape changes of the DA and individual ECs remain poorly understood. We address this problem by developing a new DA micromechanical model and applying it to experimental data on zebrafish morphogenesis. The model considers the DA as an isotropic tubular membrane subjected to hydrostatic blood pressure and axial stress. The DA evolution is described as a movement in the dimensionless controlling parameters space: normalized hydrostatic pressure and axial stress. We argue that HSPC production is accompanied by two mechanical instabilities arising in the system due to the plane stress in the DA walls and show how a complex interplay between mechanical forces in the system drives the emerging morphological changes.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-10},\\n\\tjournal = {Scientific Reports},\\n\\tauthor = {Chalin, Dmitrii and Bureau, Charlotte and Parmeggiani, Andrea and Rochal, Sergei and Kissa, Karima and Golushko, Ivan},\\n\\tmonth = apr,\\n\\tyear = {2021},\\n\\tpages = {9316},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\PXM8A3B8\\\\\\\\Chalin и др. - 2021 - Modeling and live imaging of mechanical instabilit.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Chalin, D.\",\"Bureau, C.\",\"Parmeggiani, A.\",\"Rochal, S.\",\"Kissa, K.\",\"Golushko, I.\"],\"key\":\"chalin_modeling_2021\",\"id\":\"chalin_modeling_2021\",\"bibbaseid\":\"chalin-bureau-parmeggiani-rochal-kissa-golushko-modelingandliveimagingofmechanicalinstabilitiesinthezebrafishaortaduringhematopoiesis-2021\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.nature.com/articles/s41598-021-88667-w\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"The influence of the internal structure on the polarization properties of the solid solutions of the three-component system of the sodium – potassium – cadmium niobates\",\"volume\":\"575\",\"issn\":\"0015-0193, 1563-5112\",\"url\":\"https://www.tandfonline.com/doi/full/10.1080/00150193.2021.1888228\",\"doi\":\"10.1080/00150193.2021.1888228\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-10\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Moysa\"],\"firstnames\":[\"M.\",\"O.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nagaenko\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shilkina\"],\"firstnames\":[\"L.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Andryushin\"],\"firstnames\":[\"K.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Andryushina\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Reznichenko\"],\"firstnames\":[\"L.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudskiy\"],\"firstnames\":[\"D.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudskaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2021\",\"pages\":\"64–74\",\"bibtex\":\"@article{moysa_influence_2021,\\n\\ttitle = {The influence of the internal structure on the polarization properties of the solid solutions of the three-component system of the sodium – potassium – cadmium niobates},\\n\\tvolume = {575},\\n\\tissn = {0015-0193, 1563-5112},\\n\\turl = {https://www.tandfonline.com/doi/full/10.1080/00150193.2021.1888228},\\n\\tdoi = {10.1080/00150193.2021.1888228},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-10},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Moysa, M. O. and Nagaenko, A. V. and Shilkina, L. A. and Andryushin, K. P. and Andryushina, I. N. and Reznichenko, L. A. and Rudskiy, D. I. and Rudskaya, A. G.},\\n\\tmonth = apr,\\n\\tyear = {2021},\\n\\tpages = {64--74},\\n}\\n\\n\",\"author_short\":[\"Moysa, M. O.\",\"Nagaenko, A. V.\",\"Shilkina, L. A.\",\"Andryushin, K. P.\",\"Andryushina, I. N.\",\"Reznichenko, L. A.\",\"Rudskiy, D. I.\",\"Rudskaya, A. G.\"],\"key\":\"moysa_influence_2021\",\"id\":\"moysa_influence_2021\",\"bibbaseid\":\"moysa-nagaenko-shilkina-andryushin-andryushina-reznichenko-rudskiy-rudskaya-theinfluenceoftheinternalstructureonthepolarizationpropertiesofthesolidsolutionsofthethreecomponentsystemofthesodiumpotassiumcadmiumniobates-2021\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.tandfonline.com/doi/full/10.1080/00150193.2021.1888228\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Electric field control of antiferroelectric domain pattern\",\"volume\":\"103\",\"issn\":\"2469-9950, 2469-9969\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.103.214108\",\"doi\":\"10.1103/PhysRevB.103.214108\",\"language\":\"en\",\"number\":\"21\",\"urldate\":\"2023-11-10\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Vakhrushev\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Andronikova\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bronwald\"],\"firstnames\":[\"Iu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Koroleva\"],\"firstnames\":[\"E.\",\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chernyshov\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Filimonov\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Udovenko\"],\"firstnames\":[\"S.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudskoy\"],\"firstnames\":[\"A.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ishikawa\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Baron\"],\"firstnames\":[\"A.\",\"Q.\",\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bosak\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontiev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tagantsev\"],\"firstnames\":[\"Alexander\",\"K.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2021\",\"pages\":\"214108\",\"bibtex\":\"@article{vakhrushev_electric_2021,\\n\\ttitle = {Electric field control of antiferroelectric domain pattern},\\n\\tvolume = {103},\\n\\tissn = {2469-9950, 2469-9969},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.103.214108},\\n\\tdoi = {10.1103/PhysRevB.103.214108},\\n\\tlanguage = {en},\\n\\tnumber = {21},\\n\\turldate = {2023-11-10},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Vakhrushev, S. B. and Andronikova, D. and Bronwald, Iu. and Koroleva, E. Yu. and Chernyshov, D. and Filimonov, A. V. and Udovenko, S. A. and Rudskoy, A. I. and Ishikawa, D. and Baron, A. Q. R. and Bosak, A. and Leontiev, I. N. and Tagantsev, Alexander K.},\\n\\tmonth = jun,\\n\\tyear = {2021},\\n\\tpages = {214108},\\n}\\n\\n\",\"author_short\":[\"Vakhrushev, S. B.\",\"Andronikova, D.\",\"Bronwald, I.\",\"Koroleva, E. Y.\",\"Chernyshov, D.\",\"Filimonov, A. V.\",\"Udovenko, S. A.\",\"Rudskoy, A. I.\",\"Ishikawa, D.\",\"Baron, A. Q. R.\",\"Bosak, A.\",\"Leontiev, I. N.\",\"Tagantsev, A. K.\"],\"key\":\"vakhrushev_electric_2021\",\"id\":\"vakhrushev_electric_2021\",\"bibbaseid\":\"vakhrushev-andronikova-bronwald-koroleva-chernyshov-filimonov-udovenko-rudskoy-etal-electricfieldcontrolofantiferroelectricdomainpattern-2021\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.103.214108\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Dynamics of polarization vortices revealed in a ferroelectric material\",\"volume\":\"592\",\"issn\":\"0028-0836, 1476-4687\",\"url\":\"https://www.nature.com/articles/d41586-021-00887-2\",\"doi\":\"10.1038/d41586-021-00887-2\",\"language\":\"en\",\"number\":\"7854\",\"urldate\":\"2023-11-10\",\"journal\":\"Nature\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Luk’yanchuk\"],\"firstnames\":[\"Igor\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vinokur\"],\"firstnames\":[\"Valerii\",\"M.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2021\",\"pages\":\"359–360\",\"bibtex\":\"@article{lukyanchuk_dynamics_2021,\\n\\ttitle = {Dynamics of polarization vortices revealed in a ferroelectric material},\\n\\tvolume = {592},\\n\\tissn = {0028-0836, 1476-4687},\\n\\turl = {https://www.nature.com/articles/d41586-021-00887-2},\\n\\tdoi = {10.1038/d41586-021-00887-2},\\n\\tlanguage = {en},\\n\\tnumber = {7854},\\n\\turldate = {2023-11-10},\\n\\tjournal = {Nature},\\n\\tauthor = {Luk’yanchuk, Igor and Vinokur, Valerii M.},\\n\\tmonth = apr,\\n\\tyear = {2021},\\n\\tpages = {359--360},\\n}\\n\\n\",\"author_short\":[\"Luk’yanchuk, I.\",\"Vinokur, V. M.\"],\"key\":\"lukyanchuk_dynamics_2021\",\"id\":\"lukyanchuk_dynamics_2021\",\"bibbaseid\":\"lukyanchuk-vinokur-dynamicsofpolarizationvorticesrevealedinaferroelectricmaterial-2021\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.nature.com/articles/d41586-021-00887-2\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Tip-induced domain protrusion in ferroelectric films with in-plane polarization\",\"volume\":\"129\",\"issn\":\"0021-8979, 1089-7550\",\"url\":\"https://pubs.aip.org/jap/article/129/5/054103/1080347/Tip-induced-domain-protrusion-in-ferroelectric\",\"doi\":\"10.1063/5.0035950\",\"abstract\":\"Charge manipulation and fabrication of stable domain patterns in ferroelectric materials by scanning probe microscopy open up broad avenues for the development of tunable electronics. Harnessing the polarization energy and electrostatic forces with specific geometry of the system enables producing the nanoscale domains by-design. Along with that, domain engineering requires mastery of underlying physical mechanisms that govern the domain formation. Here, we present a theoretical description of the domain formation by a scanning probe microscopy tip in a ferroelectric film with strong in-plane anisotropy of polarization. We demonstrate that local charge injection produces wedge-shaped domains that propagate along the anisotropy axis, whereas the tip-written lines of charge generate a comb-like domain structure. The results of our calculations agree with earlier experimental observations and allow for the optimization of the targeted domain structures.\",\"language\":\"en\",\"number\":\"5\",\"urldate\":\"2023-11-10\",\"journal\":\"Journal of Applied Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kondovych\"],\"firstnames\":[\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gruverman\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Luk’yanchuk\"],\"firstnames\":[\"I.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2021\",\"pages\":\"054103\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\2AIGWX9B\\\\\\\\Kondovych и др. - 2021 - Tip-induced domain protrusion in ferroelectric fil.pdf:application/pdf\",\"bibtex\":\"@article{kondovych_tip-induced_2021,\\n\\ttitle = {Tip-induced domain protrusion in ferroelectric films with in-plane polarization},\\n\\tvolume = {129},\\n\\tissn = {0021-8979, 1089-7550},\\n\\turl = {https://pubs.aip.org/jap/article/129/5/054103/1080347/Tip-induced-domain-protrusion-in-ferroelectric},\\n\\tdoi = {10.1063/5.0035950},\\n\\tabstract = {Charge manipulation and fabrication of stable domain patterns in ferroelectric materials by scanning probe microscopy open up broad avenues for the development of tunable electronics. Harnessing the polarization energy and electrostatic forces with specific geometry of the system enables producing the nanoscale domains by-design. Along with that, domain engineering requires mastery of underlying physical mechanisms that govern the domain formation. Here, we present a theoretical description of the domain formation by a scanning probe microscopy tip in a ferroelectric film with strong in-plane anisotropy of polarization. We demonstrate that local charge injection produces wedge-shaped domains that propagate along the anisotropy axis, whereas the tip-written lines of charge generate a comb-like domain structure. The results of our calculations agree with earlier experimental observations and allow for the optimization of the targeted domain structures.},\\n\\tlanguage = {en},\\n\\tnumber = {5},\\n\\turldate = {2023-11-10},\\n\\tjournal = {Journal of Applied Physics},\\n\\tauthor = {Kondovych, S. and Gruverman, A. and Luk’yanchuk, I.},\\n\\tmonth = feb,\\n\\tyear = {2021},\\n\\tpages = {054103},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\2AIGWX9B\\\\\\\\Kondovych и др. - 2021 - Tip-induced domain protrusion in ferroelectric fil.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Kondovych, S.\",\"Gruverman, A.\",\"Luk’yanchuk, I.\"],\"key\":\"kondovych_tip-induced_2021\",\"id\":\"kondovych_tip-induced_2021\",\"bibbaseid\":\"kondovych-gruverman-lukyanchuk-tipinduceddomainprotrusioninferroelectricfilmswithinplanepolarization-2021\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://pubs.aip.org/jap/article/129/5/054103/1080347/Tip-induced-domain-protrusion-in-ferroelectric\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Reasons for the High Electrical Conductivity of Bismuth Ferrite and Ways to Minimize It\",\"volume\":\"11\",\"issn\":\"2076-3417\",\"url\":\"https://www.mdpi.com/2076-3417/11/3/1025\",\"doi\":\"10.3390/app11031025\",\"abstract\":\"The reasons for the high electrical conductivity of bismuth ferrite due to its natural composite structure, structural non-stoichiometry, redox processes, and the boundary position in the perovskite family have been considered. It has been shown that it is possible to significantly (2–3 orders of magnitude) reduce the conductivity of BiFeO3 by introducing large-sized ions of rare-earth elements (REE: La, Pr, Nd, Sm, Eu, Gd with 0.94 ≤ R¯ ≤ 1.04 Å) in amounts of up to 10 mol %. An interpretation of the observed effects has been given. A consideration about the appropriateness of taking into account the presented results when developing devices using materials of the BiFeO3/REE type has been expressed.\",\"language\":\"en\",\"number\":\"3\",\"urldate\":\"2023-11-10\",\"journal\":\"Applied Sciences\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Andryushin\"],\"firstnames\":[\"Konstantin\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sakhnenko\"],\"firstnames\":[\"Vladimir\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Turik\"],\"firstnames\":[\"Anatoliy\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shilkina\"],\"firstnames\":[\"Lidiya\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pavelko\"],\"firstnames\":[\"Alexey\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dudkina\"],\"firstnames\":[\"Svetlana\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudskaya\"],\"firstnames\":[\"Angela\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudskiy\"],\"firstnames\":[\"Daniil\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Verbenko\"],\"firstnames\":[\"Iliya\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hasbulatov\"],\"firstnames\":[\"Sidek\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Reznichenko\"],\"firstnames\":[\"Larisa\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Parinov\"],\"firstnames\":[\"Ivan\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chang\"],\"firstnames\":[\"Shun-Hsyung\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Wang\"],\"firstnames\":[\"Hung-Yu\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2021\",\"pages\":\"1025\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\6GVK6IPC\\\\\\\\Andryushin и др. - 2021 - Reasons for the High Electrical Conductivity of Bi.pdf:application/pdf\",\"bibtex\":\"@article{andryushin_reasons_2021,\\n\\ttitle = {Reasons for the {High} {Electrical} {Conductivity} of {Bismuth} {Ferrite} and {Ways} to {Minimize} {It}},\\n\\tvolume = {11},\\n\\tissn = {2076-3417},\\n\\turl = {https://www.mdpi.com/2076-3417/11/3/1025},\\n\\tdoi = {10.3390/app11031025},\\n\\tabstract = {The reasons for the high electrical conductivity of bismuth ferrite due to its natural composite structure, structural non-stoichiometry, redox processes, and the boundary position in the perovskite family have been considered. It has been shown that it is possible to significantly (2–3 orders of magnitude) reduce the conductivity of BiFeO3 by introducing large-sized ions of rare-earth elements (REE: La, Pr, Nd, Sm, Eu, Gd with 0.94 ≤ R¯ ≤ 1.04 Å) in amounts of up to 10 mol \\\\%. An interpretation of the observed effects has been given. A consideration about the appropriateness of taking into account the presented results when developing devices using materials of the BiFeO3/REE type has been expressed.},\\n\\tlanguage = {en},\\n\\tnumber = {3},\\n\\turldate = {2023-11-10},\\n\\tjournal = {Applied Sciences},\\n\\tauthor = {Andryushin, Konstantin and Sakhnenko, Vladimir and Turik, Anatoliy and Shilkina, Lidiya and Pavelko, Alexey and Dudkina, Svetlana and Rudskaya, Angela and Rudskiy, Daniil and Verbenko, Iliya and Hasbulatov, Sidek and Reznichenko, Larisa and Parinov, Ivan and Chang, Shun-Hsyung and Wang, Hung-Yu},\\n\\tmonth = jan,\\n\\tyear = {2021},\\n\\tpages = {1025},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\6GVK6IPC\\\\\\\\Andryushin и др. - 2021 - Reasons for the High Electrical Conductivity of Bi.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Andryushin, K.\",\"Sakhnenko, V.\",\"Turik, A.\",\"Shilkina, L.\",\"Pavelko, A.\",\"Dudkina, S.\",\"Rudskaya, A.\",\"Rudskiy, D.\",\"Verbenko, I.\",\"Hasbulatov, S.\",\"Reznichenko, L.\",\"Parinov, I.\",\"Chang, S.\",\"Wang, H.\"],\"key\":\"andryushin_reasons_2021\",\"id\":\"andryushin_reasons_2021\",\"bibbaseid\":\"andryushin-sakhnenko-turik-shilkina-pavelko-dudkina-rudskaya-rudskiy-etal-reasonsforthehighelectricalconductivityofbismuthferriteandwaystominimizeit-2021\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.mdpi.com/2076-3417/11/3/1025\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Non-Isothermal Decomposition as Efficient and Simple Synthesis Method of NiO/C Nanoparticles for Asymmetric Supercapacitors\",\"volume\":\"11\",\"issn\":\"2079-4991\",\"url\":\"https://www.mdpi.com/2079-4991/11/1/187\",\"doi\":\"10.3390/nano11010187\",\"abstract\":\"A series of NiO/C nanocomposites with NiO concentrations ranging from 10 to 90 wt% was synthesized using a simple and efficient two-step method based on non-isothermal decomposition of Nickel(II) bis(acetylacetonate). X-ray diffraction (XRD) measurements of these NiO/C nanocomposites demonstrate the presence of β-NiO. NiO/C nanocomposites are composed of spherical particles distributed over the carbon support surface. The average diameter of nickel oxide spheres increases with the NiO content and are estimated as 36, 50 and 205 nm for nanocomposites with 10, 50 and 80 wt% NiO concentrations, respectively. In turn, each NiO sphere contains several nickel oxide nanoparticles, whose average sizes are 7–8 nm. According to the tests performed using a three-electrode cell, specific capacitance (SC) of NiO/C nanocomposites increases from 200 to 400 F/g as the NiO content achieves a maximum of 60 wt% concentration, after which the SC decreases. The study of the NiO/C composite showing the highest SC in three- and two-electrode cells reveals that its SC remains almost unchanged while increasing the current density, and the sample demonstrates excellent cycling stability properties. Finally, NiO/C (60% NiO) composites are shown to be promising materials for charging quartz clocks with a power rating of 1.5 V (30 min).\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-10\",\"journal\":\"Nanomaterials\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Chernysheva\"],\"firstnames\":[\"Daria\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pudova\"],\"firstnames\":[\"Ludmila\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Popov\"],\"firstnames\":[\"Yuri\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"Olga\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Allix\"],\"firstnames\":[\"Mathieu\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rakhmatullin\"],\"firstnames\":[\"Aydar\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Nikolay\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nikolaev\"],\"firstnames\":[\"Andrey\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2021\",\"pages\":\"187\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\A9ZZXP6R\\\\\\\\Chernysheva и др. - 2021 - Non-Isothermal Decomposition as Efficient and Simp.pdf:application/pdf\",\"bibtex\":\"@article{chernysheva_non-isothermal_2021,\\n\\ttitle = {Non-{Isothermal} {Decomposition} as {Efficient} and {Simple} {Synthesis} {Method} of {NiO}/{C} {Nanoparticles} for {Asymmetric} {Supercapacitors}},\\n\\tvolume = {11},\\n\\tissn = {2079-4991},\\n\\turl = {https://www.mdpi.com/2079-4991/11/1/187},\\n\\tdoi = {10.3390/nano11010187},\\n\\tabstract = {A series of NiO/C nanocomposites with NiO concentrations ranging from 10 to 90 wt\\\\% was synthesized using a simple and efficient two-step method based on non-isothermal decomposition of Nickel(II) bis(acetylacetonate). X-ray diffraction (XRD) measurements of these NiO/C nanocomposites demonstrate the presence of β-NiO. NiO/C nanocomposites are composed of spherical particles distributed over the carbon support surface. The average diameter of nickel oxide spheres increases with the NiO content and are estimated as 36, 50 and 205 nm for nanocomposites with 10, 50 and 80 wt\\\\% NiO concentrations, respectively. In turn, each NiO sphere contains several nickel oxide nanoparticles, whose average sizes are 7–8 nm. According to the tests performed using a three-electrode cell, specific capacitance (SC) of NiO/C nanocomposites increases from 200 to 400 F/g as the NiO content achieves a maximum of 60 wt\\\\% concentration, after which the SC decreases. The study of the NiO/C composite showing the highest SC in three- and two-electrode cells reveals that its SC remains almost unchanged while increasing the current density, and the sample demonstrates excellent cycling stability properties. Finally, NiO/C (60\\\\% NiO) composites are shown to be promising materials for charging quartz clocks with a power rating of 1.5 V (30 min).},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-10},\\n\\tjournal = {Nanomaterials},\\n\\tauthor = {Chernysheva, Daria and Pudova, Ludmila and Popov, Yuri and Smirnova, Nina and Maslova, Olga and Allix, Mathieu and Rakhmatullin, Aydar and Leontyev, Nikolay and Nikolaev, Andrey and Leontyev, Igor},\\n\\tmonth = jan,\\n\\tyear = {2021},\\n\\tpages = {187},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\A9ZZXP6R\\\\\\\\Chernysheva и др. - 2021 - Non-Isothermal Decomposition as Efficient and Simp.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Chernysheva, D.\",\"Pudova, L.\",\"Popov, Y.\",\"Smirnova, N.\",\"Maslova, O.\",\"Allix, M.\",\"Rakhmatullin, A.\",\"Leontyev, N.\",\"Nikolaev, A.\",\"Leontyev, I.\"],\"key\":\"chernysheva_non-isothermal_2021\",\"id\":\"chernysheva_non-isothermal_2021\",\"bibbaseid\":\"chernysheva-pudova-popov-smirnova-maslova-allix-rakhmatullin-leontyev-etal-nonisothermaldecompositionasefficientandsimplesynthesismethodofniocnanoparticlesforasymmetricsupercapacitors-2021\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.mdpi.com/2079-4991/11/1/187\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Pulsed laser deposition of Au nanoparticles on ZnO nanostructures\",\"volume\":\"1029\",\"issn\":\"1757-8981, 1757-899X\",\"url\":\"https://iopscience.iop.org/article/10.1088/1757-899X/1029/1/012064\",\"doi\":\"10.1088/1757-899X/1029/1/012064\",\"abstract\":\"Abstract Au nanoparticles and ultrathin gold films were obtained on the surface of thin (100 nm) ZnO films on Si (001) by pulsed laser deposition (PLD) at high argon pressure by sputtering a pure gold target with a CL3100 pulsed excimer laser (λ = 248 nm) at room temperature. The dependence of the size and distribution of nanoparticles on the argon pressure in the vacuum chamber (PAr), the power density of laser radiation (j), and the number of laser pulses (N) was investigated. Also, to obtain nanostructures, axial and non-axial deposition was used, where the substrate was located perpendicular and parallel to the plasma torch, respectively. Stable modes of obtaining gold nanoparticles with high uniformity and average size from 4 to 10 nm were demonstrated. The modes of stable and reproducible deposition of ultrathin Au films (23-42 nm) and percolation structures (18-20 nm) were also demonstrated. Thus, PLD is a reliable and flexible tool for obtaining nanoparticles and ultrathin Au films the average size and thickness of which can be predictably controlled by varying the deposition parameters. This technique is well suited for coating with gold nanoparticles the surface of nanostructured materials based on chemically active substances that are particularly sensitive to surface cleanliness, which cannot be coated by standard methods.\",\"number\":\"1\",\"urldate\":\"2023-11-10\",\"journal\":\"IOP Conference Series: Materials Science and Engineering\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Nikolaev\"],\"firstnames\":[\"A\",\"L\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kamencev\"],\"firstnames\":[\"A\",\"S\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lyanguzov\"],\"firstnames\":[\"N\",\"V\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Aizikovich\"],\"firstnames\":[\"S\",\"M\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2021\",\"pages\":\"012064\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\N97WGD4I\\\\\\\\Nikolaev и др. - 2021 - Pulsed laser deposition of Au nanoparticles on ZnO.pdf:application/pdf\",\"bibtex\":\"@article{nikolaev_pulsed_2021,\\n\\ttitle = {Pulsed laser deposition of {Au} nanoparticles on {ZnO} nanostructures},\\n\\tvolume = {1029},\\n\\tissn = {1757-8981, 1757-899X},\\n\\turl = {https://iopscience.iop.org/article/10.1088/1757-899X/1029/1/012064},\\n\\tdoi = {10.1088/1757-899X/1029/1/012064},\\n\\tabstract = {Abstract\\n            Au nanoparticles and ultrathin gold films were obtained on the surface of thin (100 nm) ZnO films on Si (001) by pulsed laser deposition (PLD) at high argon pressure by sputtering a pure gold target with a CL3100 pulsed excimer laser (λ = 248 nm) at room temperature. The dependence of the size and distribution of nanoparticles on the argon pressure in the vacuum chamber (PAr), the power density of laser radiation (j), and the number of laser pulses (N) was investigated. Also, to obtain nanostructures, axial and non-axial deposition was used, where the substrate was located perpendicular and parallel to the plasma torch, respectively. Stable modes of obtaining gold nanoparticles with high uniformity and average size from 4 to 10 nm were demonstrated. The modes of stable and reproducible deposition of ultrathin Au films (23-42 nm) and percolation structures (18-20 nm) were also demonstrated. Thus, PLD is a reliable and flexible tool for obtaining nanoparticles and ultrathin Au films the average size and thickness of which can be predictably controlled by varying the deposition parameters. This technique is well suited for coating with gold nanoparticles the surface of nanostructured materials based on chemically active substances that are particularly sensitive to surface cleanliness, which cannot be coated by standard methods.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-10},\\n\\tjournal = {IOP Conference Series: Materials Science and Engineering},\\n\\tauthor = {Nikolaev, A L and Kamencev, A S and Lyanguzov, N V and Aizikovich, S M},\\n\\tmonth = jan,\\n\\tyear = {2021},\\n\\tpages = {012064},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\N97WGD4I\\\\\\\\Nikolaev и др. - 2021 - Pulsed laser deposition of Au nanoparticles on ZnO.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Nikolaev, A L\",\"Kamencev, A S\",\"Lyanguzov, N V\",\"Aizikovich, S M\"],\"key\":\"nikolaev_pulsed_2021\",\"id\":\"nikolaev_pulsed_2021\",\"bibbaseid\":\"nikolaev-kamencev-lyanguzov-aizikovich-pulsedlaserdepositionofaunanoparticlesonznonanostructures-2021\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://iopscience.iop.org/article/10.1088/1757-899X/1029/1/012064\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Lead-substituted barium hexaferrite for tunable terahertz optoelectronics\",\"volume\":\"13\",\"issn\":\"1884-4049, 1884-4057\",\"url\":\"https://www.nature.com/articles/s41427-021-00331-x\",\"doi\":\"10.1038/s41427-021-00331-x\",\"abstract\":\"Abstract Due to their outstanding dielectric and magnetic properties, hexaferrites are attracting ever-increasing attention for developing electronic components of next-generation communication systems. The complex crystal structure of hexaferrites and the critical dependences of their electric and magnetic properties on external factors, such as magnetic/electric fields, pressure, and doping, open ample opportunities for targeted tuning of these properties when designing specific devices. Here we explored the electromagnetic properties of lead-substituted barium hexaferrite, Ba 1− x Pb x Fe 12 O 19 , a compound featuring an extremely rich set of physical phenomena that are inherent in the dielectric and magnetic subsystems and can have a significant effect on its electromagnetic response at terahertz frequencies. We performed the first detailed measurements of the temperature-dependent (5–300 K) dielectric response of single-crystalline Ba 1− x Pb x Fe 12 O 19 in an extremely broad spectral range of 1 Hz–240 THz. We fully analyzed numerous phenomena with a corresponding wide distribution of specific energies that can affect the terahertz properties of the material. The most important fundamental finding is the observation of a ferroelectric-like terahertz excitation with an unusual temperature behavior of its frequency and strength. We suggest microscopic models that explain the origin of the excitation and its nonstandard temperature evolution. Several narrower terahertz excitations are associated with electronic transitions between the fine-structure components of the Fe 2+ ground state. The discovered radio-frequency relaxations are attributed to the response of magnetic domains. Gigahertz resonances are presumably of magnetoelectric origin. The obtained data on diverse electromagnetic properties of Ba 1− x Pb x Fe 12 O 19 compounds provide information that makes the entire class of hexaferrites attractive for manufacturing electronic devices for the terahertz range.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-10\",\"journal\":\"NPG Asia Materials\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Alyabyeva\"],\"firstnames\":[\"L.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vinnik\"],\"firstnames\":[\"D.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Anzin\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ahmed\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bednyakov\"],\"firstnames\":[\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kadlec\"],\"firstnames\":[\"C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kadlec\"],\"firstnames\":[\"F.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"De\",\"Prado\"],\"firstnames\":[\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokleška\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Proschek\"],\"firstnames\":[\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kamba\"],\"firstnames\":[\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pronin\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Abalmasov\"],\"firstnames\":[\"V.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dremov\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Schmid\"],\"firstnames\":[\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Savinov\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lunkenheimer\"],\"firstnames\":[\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"B.\",\"P.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2021\",\"pages\":\"63\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\3G3UAQ2R\\\\\\\\Alyabyeva и др. - 2021 - Lead-substituted barium hexaferrite for tunable te.pdf:application/pdf\",\"bibtex\":\"@article{alyabyeva_lead-substituted_2021,\\n\\ttitle = {Lead-substituted barium hexaferrite for tunable terahertz optoelectronics},\\n\\tvolume = {13},\\n\\tissn = {1884-4049, 1884-4057},\\n\\turl = {https://www.nature.com/articles/s41427-021-00331-x},\\n\\tdoi = {10.1038/s41427-021-00331-x},\\n\\tabstract = {Abstract\\n            \\n              Due to their outstanding dielectric and magnetic properties, hexaferrites are attracting ever-increasing attention for developing electronic components of next-generation communication systems. The complex crystal structure of hexaferrites and the critical dependences of their electric and magnetic properties on external factors, such as magnetic/electric fields, pressure, and doping, open ample opportunities for targeted tuning of these properties when designing specific devices. Here we explored the electromagnetic properties of lead-substituted barium hexaferrite, Ba\\n              \\n                1−\\n                x\\n              \\n              Pb\\n              \\n                x\\n              \\n              Fe\\n              12\\n              O\\n              19\\n              , a compound featuring an extremely rich set of physical phenomena that are inherent in the dielectric and magnetic subsystems and can have a significant effect on its electromagnetic response at terahertz frequencies. We performed the first detailed measurements of the temperature-dependent (5–300 K) dielectric response of single-crystalline Ba\\n              \\n                1−\\n                x\\n              \\n              Pb\\n              \\n                x\\n              \\n              Fe\\n              12\\n              O\\n              19\\n              in an extremely broad spectral range of 1 Hz–240 THz. We fully analyzed numerous phenomena with a corresponding wide distribution of specific energies that can affect the terahertz properties of the material. The most important fundamental finding is the observation of a ferroelectric-like terahertz excitation with an unusual temperature behavior of its frequency and strength. We suggest microscopic models that explain the origin of the excitation and its nonstandard temperature evolution. Several narrower terahertz excitations are associated with electronic transitions between the fine-structure components of the Fe\\n              2+\\n              ground state. The discovered radio-frequency relaxations are attributed to the response of magnetic domains. Gigahertz resonances are presumably of magnetoelectric origin. The obtained data on diverse electromagnetic properties of Ba\\n              \\n                1−\\n                x\\n              \\n              Pb\\n              \\n                x\\n              \\n              Fe\\n              12\\n              O\\n              19\\n              compounds provide information that makes the entire class of hexaferrites attractive for manufacturing electronic devices for the terahertz range.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-10},\\n\\tjournal = {NPG Asia Materials},\\n\\tauthor = {Alyabyeva, L. N. and Prokhorov, A. S. and Vinnik, D. A. and Anzin, V. B. and Ahmed, A. G. and Mikheykin, A. and Bednyakov, P. and Kadlec, C. and Kadlec, F. and De Prado, E. and Prokleška, J. and Proschek, P. and Kamba, S. and Pronin, A. V. and Dressel, M. and Abalmasov, V. A. and Dremov, V. V. and Schmid, S. and Savinov, M. and Lunkenheimer, P. and Gorshunov, B. P.},\\n\\tmonth = dec,\\n\\tyear = {2021},\\n\\tpages = {63},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\3G3UAQ2R\\\\\\\\Alyabyeva и др. - 2021 - Lead-substituted barium hexaferrite for tunable te.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Alyabyeva, L. N.\",\"Prokhorov, A. S.\",\"Vinnik, D. A.\",\"Anzin, V. B.\",\"Ahmed, A. G.\",\"Mikheykin, A.\",\"Bednyakov, P.\",\"Kadlec, C.\",\"Kadlec, F.\",\"De Prado, E.\",\"Prokleška, J.\",\"Proschek, P.\",\"Kamba, S.\",\"Pronin, A. V.\",\"Dressel, M.\",\"Abalmasov, V. A.\",\"Dremov, V. V.\",\"Schmid, S.\",\"Savinov, M.\",\"Lunkenheimer, P.\",\"Gorshunov, B. P.\"],\"key\":\"alyabyeva_lead-substituted_2021\",\"id\":\"alyabyeva_lead-substituted_2021\",\"bibbaseid\":\"alyabyeva-prokhorov-vinnik-anzin-ahmed-mikheykin-bednyakov-kadlec-etal-leadsubstitutedbariumhexaferritefortunableterahertzoptoelectronics-2021\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.nature.com/articles/s41427-021-00331-x\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"One step simultaneous electrochemical synthesis of NiO/multilayer graphene nanocomposite as an electrode material for high performance supercapacitors\",\"volume\":\"31\",\"issn\":\"09599436\",\"url\":\"https://linkinghub.elsevier.com/retrieve/pii/S0959943621000596\",\"doi\":\"10.1016/j.mencom.2021.03.005\",\"language\":\"en\",\"number\":\"2\",\"urldate\":\"2023-11-10\",\"journal\":\"Mendeleev Communications\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Chernysheva\"],\"firstnames\":[\"Daria\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Avramenko\"],\"firstnames\":[\"Marina\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lyanguzov\"],\"firstnames\":[\"Nikolay\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grebenyuk\"],\"firstnames\":[\"Tatyana\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\",\"V.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2021\",\"pages\":\"160–162\",\"bibtex\":\"@article{chernysheva_one_2021,\\n\\ttitle = {One step simultaneous electrochemical synthesis of {NiO}/multilayer graphene nanocomposite as an electrode material for high performance supercapacitors},\\n\\tvolume = {31},\\n\\tissn = {09599436},\\n\\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0959943621000596},\\n\\tdoi = {10.1016/j.mencom.2021.03.005},\\n\\tlanguage = {en},\\n\\tnumber = {2},\\n\\turldate = {2023-11-10},\\n\\tjournal = {Mendeleev Communications},\\n\\tauthor = {Chernysheva, Daria V. and Leontyev, Igor N. and Avramenko, Marina V. and Lyanguzov, Nikolay V. and Grebenyuk, Tatyana I. and Smirnova, Nina V.},\\n\\tmonth = mar,\\n\\tyear = {2021},\\n\\tpages = {160--162},\\n}\\n\\n\",\"author_short\":[\"Chernysheva, D. V.\",\"Leontyev, I. N.\",\"Avramenko, M. V.\",\"Lyanguzov, N. V.\",\"Grebenyuk, T. I.\",\"Smirnova, N. V.\"],\"key\":\"chernysheva_one_2021\",\"id\":\"chernysheva_one_2021\",\"bibbaseid\":\"chernysheva-leontyev-avramenko-lyanguzov-grebenyuk-smirnova-onestepsimultaneouselectrochemicalsynthesisofniomultilayergraphenenanocompositeasanelectrodematerialforhighperformancesupercapacitors-2021\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://linkinghub.elsevier.com/retrieve/pii/S0959943621000596\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"The influence of thermodynamic background on the phase picture, macroresponses and the effects of the temporary aging of lead titanium doped with alkaline earth metal oxides\",\"volume\":\"47\",\"issn\":\"02728842\",\"url\":\"https://linkinghub.elsevier.com/retrieve/pii/S0272884220331928\",\"doi\":\"10.1016/j.ceramint.2020.10.149\",\"language\":\"en\",\"number\":\"4\",\"urldate\":\"2023-11-10\",\"journal\":\"Ceramics International\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Nagaenko\"],\"firstnames\":[\"A.V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Andryushina\"],\"firstnames\":[\"I.N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Andryushin\"],\"firstnames\":[\"K.P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shilkina\"],\"firstnames\":[\"L.A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudskaya\"],\"firstnames\":[\"A.G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Reznichenko\"],\"firstnames\":[\"L.A.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2021\",\"pages\":\"5639–5647\",\"bibtex\":\"@article{nagaenko_influence_2021,\\n\\ttitle = {The influence of thermodynamic background on the phase picture, macroresponses and the effects of the temporary aging of lead titanium doped with alkaline earth metal oxides},\\n\\tvolume = {47},\\n\\tissn = {02728842},\\n\\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0272884220331928},\\n\\tdoi = {10.1016/j.ceramint.2020.10.149},\\n\\tlanguage = {en},\\n\\tnumber = {4},\\n\\turldate = {2023-11-10},\\n\\tjournal = {Ceramics International},\\n\\tauthor = {Nagaenko, A.V. and Andryushina, I.N. and Andryushin, K.P. and Shilkina, L.A. and Rudskaya, A.G. and Reznichenko, L.A.},\\n\\tmonth = feb,\\n\\tyear = {2021},\\n\\tpages = {5639--5647},\\n}\\n\\n\",\"author_short\":[\"Nagaenko, A.\",\"Andryushina, I.\",\"Andryushin, K.\",\"Shilkina, L.\",\"Rudskaya, A.\",\"Reznichenko, L.\"],\"key\":\"nagaenko_influence_2021\",\"id\":\"nagaenko_influence_2021\",\"bibbaseid\":\"nagaenko-andryushina-andryushin-shilkina-rudskaya-reznichenko-theinfluenceofthermodynamicbackgroundonthephasepicturemacroresponsesandtheeffectsofthetemporaryagingofleadtitaniumdopedwithalkalineearthmetaloxides-2021\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://linkinghub.elsevier.com/retrieve/pii/S0272884220331928\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Thermal-stability of the enhanced piezoelectric, energy storage and electrocaloric properties of a lead-free BCZT ceramic\",\"volume\":\"11\",\"issn\":\"2046-2069\",\"url\":\"http://xlink.rsc.org/?DOI=D0RA09707A\",\"doi\":\"10.1039/D0RA09707A\",\"abstract\":\"High-thermal stability of the recovered energy density and significant electrocaloric temperature change over a broad temperature span in a lead-free BCZT ceramic. , The lead-free Ba 0.85 Ca 0.15 Zr 0.10 Ti 0.90 O 3 (BCZT) relaxor ferroelectric ceramic has aroused much attention due to its enhanced piezoelectric, energy storage and electrocaloric properties. In this study, the BCZT ceramic was elaborated by the solid-state reaction route, and the temperature-dependence of the structural, electrical, piezoelectric, energy storage and electrocaloric properties was investigated. X-ray diffraction analysis revealed a pure perovskite phase, and the temperature-dependence of Raman spectroscopy, dielectric and ferroelectric measurements revealed the phase transitions in the BCZT ceramic. At room temperature, the strain and the large-signal piezoelectric coefficient reached a maximum of 0.062% and 234 pm V −1 , respectively. Furthermore, enhanced recovered energy density ( W rec = 62 mJ cm −3 ) and high-energy storage efficiency ( η ) of 72.9% at 130 °C were found. The BCZT ceramic demonstrated excellent thermal stability of the energy storage variation (ESV), less than ±5.5% in the temperature range of 30–100 °C compared to other lead-free ceramics. The electrocaloric response in the BCZT ceramic was explored via the indirect approach by using the Maxwell relation. Significant electrocaloric temperature change (Δ T ) of 0.57 K over a broad temperature span ( T span = 70 °C) and enhanced coefficient of performance (COP = 11) were obtained under 25 kV cm −1 . The obtained results make the BCZT ceramic a suitable eco-friendly material for energy storage and solid-state electrocaloric cooling devices.\",\"language\":\"en\",\"number\":\"16\",\"urldate\":\"2023-11-10\",\"journal\":\"RSC Advances\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Merselmiz\"],\"firstnames\":[\"Soukaina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hanani\"],\"firstnames\":[\"Zouhair\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzane\"],\"firstnames\":[\"Daoud\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"Anna\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Amjoud\"],\"firstnames\":[\"M'barek\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hajji\"],\"firstnames\":[\"Lahoucine\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Terenchuk\"],\"firstnames\":[\"Svitlana\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rožič\"],\"firstnames\":[\"Brigita\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Luk'yanchuk\"],\"firstnames\":[\"Igor\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kutnjak\"],\"firstnames\":[\"Zdravko\"],\"suffixes\":[]}],\"year\":\"2021\",\"pages\":\"9459–9468\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\AUJR9SKH\\\\\\\\Merselmiz и др. - 2021 - Thermal-stability of the enhanced piezoelectric, e.pdf:application/pdf\",\"bibtex\":\"@article{merselmiz_thermal-stability_2021,\\n\\ttitle = {Thermal-stability of the enhanced piezoelectric, energy storage and electrocaloric properties of a lead-free {BCZT} ceramic},\\n\\tvolume = {11},\\n\\tissn = {2046-2069},\\n\\turl = {http://xlink.rsc.org/?DOI=D0RA09707A},\\n\\tdoi = {10.1039/D0RA09707A},\\n\\tabstract = {High-thermal stability of the recovered energy density and significant electrocaloric temperature change over a broad temperature span in a lead-free BCZT ceramic.\\n          , \\n            \\n              The lead-free Ba\\n              0.85\\n              Ca\\n              0.15\\n              Zr\\n              0.10\\n              Ti\\n              0.90\\n              O\\n              3\\n              (BCZT) relaxor ferroelectric ceramic has aroused much attention due to its enhanced piezoelectric, energy storage and electrocaloric properties. In this study, the BCZT ceramic was elaborated by the solid-state reaction route, and the temperature-dependence of the structural, electrical, piezoelectric, energy storage and electrocaloric properties was investigated. X-ray diffraction analysis revealed a pure perovskite phase, and the temperature-dependence of Raman spectroscopy, dielectric and ferroelectric measurements revealed the phase transitions in the BCZT ceramic. At room temperature, the strain and the large-signal piezoelectric coefficient\\n              \\n              reached a maximum of 0.062\\\\% and 234 pm V\\n              −1\\n              , respectively. Furthermore, enhanced recovered energy density (\\n              W\\n              rec\\n              = 62 mJ cm\\n              −3\\n              ) and high-energy storage efficiency (\\n              η\\n              ) of 72.9\\\\% at 130 °C were found. The BCZT ceramic demonstrated excellent thermal stability of the energy storage variation (ESV), less than ±5.5\\\\% in the temperature range of 30–100 °C compared to other lead-free ceramics. The electrocaloric response in the BCZT ceramic was explored\\n              via\\n              the indirect approach by using the Maxwell relation. Significant electrocaloric temperature change (Δ\\n              T\\n              ) of 0.57 K over a broad temperature span (\\n              T\\n              span\\n              = 70 °C) and enhanced coefficient of performance (COP = 11) were obtained under 25 kV cm\\n              −1\\n              . The obtained results make the BCZT ceramic a suitable eco-friendly material for energy storage and solid-state electrocaloric cooling devices.},\\n\\tlanguage = {en},\\n\\tnumber = {16},\\n\\turldate = {2023-11-10},\\n\\tjournal = {RSC Advances},\\n\\tauthor = {Merselmiz, Soukaina and Hanani, Zouhair and Mezzane, Daoud and Razumnaya, Anna G. and Amjoud, M'barek and Hajji, Lahoucine and Terenchuk, Svitlana and Rožič, Brigita and Luk'yanchuk, Igor A. and Kutnjak, Zdravko},\\n\\tyear = {2021},\\n\\tpages = {9459--9468},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\AUJR9SKH\\\\\\\\Merselmiz и др. - 2021 - Thermal-stability of the enhanced piezoelectric, e.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Merselmiz, S.\",\"Hanani, Z.\",\"Mezzane, D.\",\"Razumnaya, A. G.\",\"Amjoud, M.\",\"Hajji, L.\",\"Terenchuk, S.\",\"Rožič, B.\",\"Luk'yanchuk, I. A.\",\"Kutnjak, Z.\"],\"key\":\"merselmiz_thermal-stability_2021\",\"id\":\"merselmiz_thermal-stability_2021\",\"bibbaseid\":\"merselmiz-hanani-mezzane-razumnaya-amjoud-hajji-terenchuk-roi-etal-thermalstabilityoftheenhancedpiezoelectricenergystorageandelectrocaloricpropertiesofaleadfreebcztceramic-2021\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://xlink.rsc.org/?DOI=D0RA09707A\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Twin-boundary engineering and thickness effect on strontium-barium niobate thin films on MgO substrate\",\"volume\":\"888\",\"issn\":\"09258388\",\"url\":\"https://linkinghub.elsevier.com/retrieve/pii/S0925838821029984\",\"doi\":\"10.1016/j.jallcom.2021.161589\",\"language\":\"en\",\"urldate\":\"2023-11-10\",\"journal\":\"Journal of Alloys and Compounds\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"A.S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Marssi\"],\"firstnames\":[\"M.\",\"El\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzane\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lyanguzov\"],\"firstnames\":[\"N.V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pavlenko\"],\"firstnames\":[\"A.V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Stryukov\"],\"firstnames\":[\"D.V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.G.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2021\",\"pages\":\"161589\",\"bibtex\":\"@article{mikheykin_twin-boundary_2021,\\n\\ttitle = {Twin-boundary engineering and thickness effect on strontium-barium niobate thin films on {MgO} substrate},\\n\\tvolume = {888},\\n\\tissn = {09258388},\\n\\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0925838821029984},\\n\\tdoi = {10.1016/j.jallcom.2021.161589},\\n\\tlanguage = {en},\\n\\turldate = {2023-11-10},\\n\\tjournal = {Journal of Alloys and Compounds},\\n\\tauthor = {Mikheykin, A.S. and Shirokov, V.B. and Marssi, M. El and Mezzane, D. and Lyanguzov, N.V. and Pavlenko, A.V. and Stryukov, D.V. and Razumnaya, A.G.},\\n\\tmonth = dec,\\n\\tyear = {2021},\\n\\tpages = {161589},\\n}\\n\\n\",\"author_short\":[\"Mikheykin, A.\",\"Shirokov, V.\",\"Marssi, M. E.\",\"Mezzane, D.\",\"Lyanguzov, N.\",\"Pavlenko, A.\",\"Stryukov, D.\",\"Razumnaya, A.\"],\"key\":\"mikheykin_twin-boundary_2021\",\"id\":\"mikheykin_twin-boundary_2021\",\"bibbaseid\":\"mikheykin-shirokov-marssi-mezzane-lyanguzov-pavlenko-stryukov-razumnaya-twinboundaryengineeringandthicknesseffectonstrontiumbariumniobatethinfilmsonmgosubstrate-2021\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://linkinghub.elsevier.com/retrieve/pii/S0925838821029984\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Photocatalytic degradation of ciprofloxacin in water at nano-ZnO prepared by pulse alternating current electrochemical synthesis\",\"volume\":\"40\",\"issn\":\"22147144\",\"url\":\"https://linkinghub.elsevier.com/retrieve/pii/S2214714420306863\",\"doi\":\"10.1016/j.jwpe.2020.101809\",\"language\":\"en\",\"urldate\":\"2023-11-10\",\"journal\":\"Journal of Water Process Engineering\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Ulyankina\"],\"firstnames\":[\"Anna\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Molodtsova\"],\"firstnames\":[\"Tatiana\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshenkov\"],\"firstnames\":[\"Mikhail\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhigunov\"],\"firstnames\":[\"Denis\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Konstantinova\"],\"firstnames\":[\"Elizaveta\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lastovina\"],\"firstnames\":[\"Tatiana\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tolasz\"],\"firstnames\":[\"Jakub\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Henych\"],\"firstnames\":[\"Jiří\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Licciardello\"],\"firstnames\":[\"Nadia\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Cuniberti\"],\"firstnames\":[\"Gianaurelio\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2021\",\"pages\":\"101809\",\"bibtex\":\"@article{ulyankina_photocatalytic_2021,\\n\\ttitle = {Photocatalytic degradation of ciprofloxacin in water at nano-{ZnO} prepared by pulse alternating current electrochemical synthesis},\\n\\tvolume = {40},\\n\\tissn = {22147144},\\n\\turl = {https://linkinghub.elsevier.com/retrieve/pii/S2214714420306863},\\n\\tdoi = {10.1016/j.jwpe.2020.101809},\\n\\tlanguage = {en},\\n\\turldate = {2023-11-10},\\n\\tjournal = {Journal of Water Process Engineering},\\n\\tauthor = {Ulyankina, Anna and Molodtsova, Tatiana and Gorshenkov, Mikhail and Leontyev, Igor and Zhigunov, Denis and Konstantinova, Elizaveta and Lastovina, Tatiana and Tolasz, Jakub and Henych, Jiří and Licciardello, Nadia and Cuniberti, Gianaurelio and Smirnova, Nina},\\n\\tmonth = apr,\\n\\tyear = {2021},\\n\\tpages = {101809},\\n}\\n\\n\",\"author_short\":[\"Ulyankina, A.\",\"Molodtsova, T.\",\"Gorshenkov, M.\",\"Leontyev, I.\",\"Zhigunov, D.\",\"Konstantinova, E.\",\"Lastovina, T.\",\"Tolasz, J.\",\"Henych, J.\",\"Licciardello, N.\",\"Cuniberti, G.\",\"Smirnova, N.\"],\"key\":\"ulyankina_photocatalytic_2021\",\"id\":\"ulyankina_photocatalytic_2021\",\"bibbaseid\":\"ulyankina-molodtsova-gorshenkov-leontyev-zhigunov-konstantinova-lastovina-tolasz-etal-photocatalyticdegradationofciprofloxacininwateratnanoznopreparedbypulsealternatingcurrentelectrochemicalsynthesis-2021\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://linkinghub.elsevier.com/retrieve/pii/S2214714420306863\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Individual arc-discharge synthesized multiwalled carbon nanotubes probed with multiple measurement techniques\",\"volume\":\"38\",\"issn\":\"2166-2746, 2166-2754\",\"url\":\"https://pubs.aip.org/jvb/article/38/4/042804/592550/Individual-arc-discharge-synthesized-multiwalled\",\"doi\":\"10.1116/6.0000187\",\"abstract\":\"Arc-discharge synthesized multiwalled carbon nanotubes (AD-MWNT), or related MWNTs, exhibit a good quality compared to the more common type of MWNT synthesized by catalytic chemical vapor deposition methods. Yet experimental measurements on these are rather few and typically have not correlated data from different measurement techniques. Here, the authors report Raman spectroscopy, scanning probe microscopy, conductivity measurements, and force microscopy on single AD-MWNTs. The results demonstrate the high quality of AD-MWNTs and are compatible with the view of them as the best approximation of MWNTs as an assembly of defect-free concentric individual single-walled carbon nanotubes. The authors also demonstrate conductance measurements over a step on the surface of an AD-MWNT, which is due to an abruptly broken outer layer(s), whereby the interlayer resistance is measured.\",\"language\":\"en\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Vacuum Science & Technology B, Nanotechnology and Microelectronics: Materials, Processing, Measurement, and Phenomena\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Ahlskog\"],\"firstnames\":[\"Markus\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hokkanen\"],\"firstnames\":[\"Matti\",\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Levshov\"],\"firstnames\":[\"Dmitry\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Svensson\"],\"firstnames\":[\"Krister\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Volodin\"],\"firstnames\":[\"Alexander\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Van\",\"Haesendonck\"],\"firstnames\":[\"Chris\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2020\",\"pages\":\"042804\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\76DFFX6C\\\\\\\\Ahlskog и др. - 2020 - Individual arc-discharge synthesized multiwalled c.pdf:application/pdf\",\"bibtex\":\"@article{ahlskog_individual_2020,\\n\\ttitle = {Individual arc-discharge synthesized multiwalled carbon nanotubes probed with multiple measurement techniques},\\n\\tvolume = {38},\\n\\tissn = {2166-2746, 2166-2754},\\n\\turl = {https://pubs.aip.org/jvb/article/38/4/042804/592550/Individual-arc-discharge-synthesized-multiwalled},\\n\\tdoi = {10.1116/6.0000187},\\n\\tabstract = {Arc-discharge synthesized multiwalled carbon nanotubes (AD-MWNT), or related MWNTs, exhibit a good quality compared to the more common type of MWNT synthesized by catalytic chemical vapor deposition methods. Yet experimental measurements on these are rather few and typically have not correlated data from different measurement techniques. Here, the authors report Raman spectroscopy, scanning probe microscopy, conductivity measurements, and force microscopy on single AD-MWNTs. The results demonstrate the high quality of AD-MWNTs and are compatible with the view of them as the best approximation of MWNTs as an assembly of defect-free concentric individual single-walled carbon nanotubes. The authors also demonstrate conductance measurements over a step on the surface of an AD-MWNT, which is due to an abruptly broken outer layer(s), whereby the interlayer resistance is measured.},\\n\\tlanguage = {en},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Vacuum Science \\\\& Technology B, Nanotechnology and Microelectronics: Materials, Processing, Measurement, and Phenomena},\\n\\tauthor = {Ahlskog, Markus and Hokkanen, Matti J. and Levshov, Dmitry and Svensson, Krister and Volodin, Alexander and Van Haesendonck, Chris},\\n\\tmonth = jul,\\n\\tyear = {2020},\\n\\tpages = {042804},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\76DFFX6C\\\\\\\\Ahlskog и др. - 2020 - Individual arc-discharge synthesized multiwalled c.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Ahlskog, M.\",\"Hokkanen, M. J.\",\"Levshov, D.\",\"Svensson, K.\",\"Volodin, A.\",\"Van Haesendonck, C.\"],\"key\":\"ahlskog_individual_2020\",\"id\":\"ahlskog_individual_2020\",\"bibbaseid\":\"ahlskog-hokkanen-levshov-svensson-volodin-vanhaesendonck-individualarcdischargesynthesizedmultiwalledcarbonnanotubesprobedwithmultiplemeasurementtechniques-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://pubs.aip.org/jvb/article/38/4/042804/592550/Individual-arc-discharge-synthesized-multiwalled\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Band structure and inter-tube optical transitions in double-walled carbon nanotubes\",\"volume\":\"102\",\"issn\":\"2469-9950, 2469-9969\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.102.115426\",\"doi\":\"10.1103/PhysRevB.102.115426\",\"language\":\"en\",\"number\":\"11\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Chalin\"],\"firstnames\":[\"D.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2020\",\"pages\":\"115426\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\2XJKU38W\\\\\\\\Chalin и Rochal - 2020 - Band structure and inter-tube optical transitions .pdf:application/pdf\",\"bibtex\":\"@article{chalin_band_2020,\\n\\ttitle = {Band structure and inter-tube optical transitions in double-walled carbon nanotubes},\\n\\tvolume = {102},\\n\\tissn = {2469-9950, 2469-9969},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.102.115426},\\n\\tdoi = {10.1103/PhysRevB.102.115426},\\n\\tlanguage = {en},\\n\\tnumber = {11},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Chalin, D. V. and Rochal, S. B.},\\n\\tmonth = sep,\\n\\tyear = {2020},\\n\\tpages = {115426},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\2XJKU38W\\\\\\\\Chalin и Rochal - 2020 - Band structure and inter-tube optical transitions .pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Chalin, D. V.\",\"Rochal, S. B.\"],\"key\":\"chalin_band_2020\",\"id\":\"chalin_band_2020\",\"bibbaseid\":\"chalin-rochal-bandstructureandintertubeopticaltransitionsindoublewalledcarbonnanotubes-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.102.115426\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Characterization of Enamel and Dentine about a White Spot Lesion: Mechanical Properties, Mineral Density, Microstructure and Molecular Composition\",\"volume\":\"10\",\"issn\":\"2079-4991\",\"shorttitle\":\"Characterization of Enamel and Dentine about a White Spot Lesion\",\"url\":\"https://www.mdpi.com/2079-4991/10/9/1889\",\"doi\":\"10.3390/nano10091889\",\"abstract\":\"The study focuses on in vitro tracing of some fundamental changes that emerge in teeth at the initial stage of caries development using multiple approaches. The research was conducted on a mostly sound maxillary molar tooth but with a clearly visible natural proximal white spot lesion (WSL). Values of mineral density, reduced Young’s modulus, indentation hardness and creep as well as the molecular composition and surface microstructure of the WSL and bordering dentine area were studied. The results obtained were compared to those of sound enamel and dentine on the same tooth. A decrease of mechanical properties and mineral density both for the WSL and bordering dentine was detected in comparison to the sound counterparts, as well as increase of creep for the enamel WSL. Differences in molecular composition and surface microstructure (including the indenter impressions) were found and described. WSL induces a serious change in the state of not only the visually affected enamel but also surrounding visually intact enamel and dentine in its vicinity. The results provide the basis for future studies of efficacy of minimal invasive treatments of caries.\",\"language\":\"en\",\"number\":\"9\",\"urldate\":\"2023-11-11\",\"journal\":\"Nanomaterials\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Sadyrin\"],\"firstnames\":[\"Evgeniy\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Swain\"],\"firstnames\":[\"Michael\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mitrin\"],\"firstnames\":[\"Boris\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rzhepakovsky\"],\"firstnames\":[\"Igor\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nikolaev\"],\"firstnames\":[\"Andrey\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Irkha\"],\"firstnames\":[\"Vladimir\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yogina\"],\"firstnames\":[\"Diana\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lyanguzov\"],\"firstnames\":[\"Nikolay\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maksyukov\"],\"firstnames\":[\"Stanislav\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Aizikovich\"],\"firstnames\":[\"Sergei\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2020\",\"pages\":\"1889\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\95JZJ5NP\\\\§adyrin и др. - 2020 - Characterization of Enamel and Dentine about a Whi.pdf:application/pdf\",\"bibtex\":\"@article{sadyrin_characterization_2020,\\n\\ttitle = {Characterization of {Enamel} and {Dentine} about a {White} {Spot} {Lesion}: {Mechanical} {Properties}, {Mineral} {Density}, {Microstructure} and {Molecular} {Composition}},\\n\\tvolume = {10},\\n\\tissn = {2079-4991},\\n\\tshorttitle = {Characterization of {Enamel} and {Dentine} about a {White} {Spot} {Lesion}},\\n\\turl = {https://www.mdpi.com/2079-4991/10/9/1889},\\n\\tdoi = {10.3390/nano10091889},\\n\\tabstract = {The study focuses on in vitro tracing of some fundamental changes that emerge in teeth at the initial stage of caries development using multiple approaches. The research was conducted on a mostly sound maxillary molar tooth but with a clearly visible natural proximal white spot lesion (WSL). Values of mineral density, reduced Young’s modulus, indentation hardness and creep as well as the molecular composition and surface microstructure of the WSL and bordering dentine area were studied. The results obtained were compared to those of sound enamel and dentine on the same tooth. A decrease of mechanical properties and mineral density both for the WSL and bordering dentine was detected in comparison to the sound counterparts, as well as increase of creep for the enamel WSL. Differences in molecular composition and surface microstructure (including the indenter impressions) were found and described. WSL induces a serious change in the state of not only the visually affected enamel but also surrounding visually intact enamel and dentine in its vicinity. The results provide the basis for future studies of efficacy of minimal invasive treatments of caries.},\\n\\tlanguage = {en},\\n\\tnumber = {9},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Nanomaterials},\\n\\tauthor = {Sadyrin, Evgeniy and Swain, Michael and Mitrin, Boris and Rzhepakovsky, Igor and Nikolaev, Andrey and Irkha, Vladimir and Yogina, Diana and Lyanguzov, Nikolay and Maksyukov, Stanislav and Aizikovich, Sergei},\\n\\tmonth = sep,\\n\\tyear = {2020},\\n\\tpages = {1889},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\95JZJ5NP\\\\\\\\Sadyrin и др. - 2020 - Characterization of Enamel and Dentine about a Whi.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Sadyrin, E.\",\"Swain, M.\",\"Mitrin, B.\",\"Rzhepakovsky, I.\",\"Nikolaev, A.\",\"Irkha, V.\",\"Yogina, D.\",\"Lyanguzov, N.\",\"Maksyukov, S.\",\"Aizikovich, S.\"],\"key\":\"sadyrin_characterization_2020\",\"id\":\"sadyrin_characterization_2020\",\"bibbaseid\":\"sadyrin-swain-mitrin-rzhepakovsky-nikolaev-irkha-yogina-lyanguzov-etal-characterizationofenamelanddentineaboutawhitespotlesionmechanicalpropertiesmineraldensitymicrostructureandmolecularcomposition-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.mdpi.com/2079-4991/10/9/1889\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"A Comparison of “Bottom-Up” and “Top-Down” Approaches to the Synthesis of Pt/C Electrocatalysts\",\"volume\":\"8\",\"issn\":\"2227-9717\",\"url\":\"https://www.mdpi.com/2227-9717/8/8/947\",\"doi\":\"10.3390/pr8080947\",\"abstract\":\"Three 40 wt % Pt/C electrocatalysts prepared using two different approaches—the polyol process and electrochemical dispersion of platinum under pulse alternating current—and a commercial Pt/C catalyst (Johnson Matthey prod.) were examined via X-ray diffraction (XRD) and transmission electron microscopy (TEM). The stability characteristics of the Pt/C catalysts were studied via long-term cycling, revealing that, for all cycling modes, the best stability was achieved for the Pt/C catalyst with the largest platinum nanoparticle sizes, which was synthesized via electrochemical dispersion of platinum under pulse alternating current. Our results show that the mass and specific electrocatalytic activities of Pt/C catalysts toward ethanol electrooxidation are determined by the value of the electrochemically active Pt surface area in the catalysts.\",\"language\":\"en\",\"number\":\"8\",\"urldate\":\"2023-11-11\",\"journal\":\"Processes\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"Alexandra\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Faddeev\"],\"firstnames\":[\"Nikita\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshenkov\"],\"firstnames\":[\"Mikhail\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kuznetsov\"],\"firstnames\":[\"Dmitri\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2020\",\"pages\":\"947\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\86DZKUPG\\\\\\\\Kuriganova и др. - 2020 - A Comparison of “Bottom-Up” and “Top-Down” Approac.pdf:application/pdf\",\"bibtex\":\"@article{kuriganova_comparison_2020,\\n\\ttitle = {A {Comparison} of “{Bottom}-{Up}” and “{Top}-{Down}” {Approaches} to the {Synthesis} of {Pt}/{C} {Electrocatalysts}},\\n\\tvolume = {8},\\n\\tissn = {2227-9717},\\n\\turl = {https://www.mdpi.com/2227-9717/8/8/947},\\n\\tdoi = {10.3390/pr8080947},\\n\\tabstract = {Three 40 wt \\\\% Pt/C electrocatalysts prepared using two different approaches—the polyol process and electrochemical dispersion of platinum under pulse alternating current—and a commercial Pt/C catalyst (Johnson Matthey prod.) were examined via X-ray diffraction (XRD) and transmission electron microscopy (TEM). The stability characteristics of the Pt/C catalysts were studied via long-term cycling, revealing that, for all cycling modes, the best stability was achieved for the Pt/C catalyst with the largest platinum nanoparticle sizes, which was synthesized via electrochemical dispersion of platinum under pulse alternating current. Our results show that the mass and specific electrocatalytic activities of Pt/C catalysts toward ethanol electrooxidation are determined by the value of the electrochemically active Pt surface area in the catalysts.},\\n\\tlanguage = {en},\\n\\tnumber = {8},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Processes},\\n\\tauthor = {Kuriganova, Alexandra and Faddeev, Nikita and Gorshenkov, Mikhail and Kuznetsov, Dmitri and Leontyev, Igor and Smirnova, Nina},\\n\\tmonth = aug,\\n\\tyear = {2020},\\n\\tpages = {947},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\86DZKUPG\\\\\\\\Kuriganova и др. - 2020 - A Comparison of “Bottom-Up” and “Top-Down” Approac.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Kuriganova, A.\",\"Faddeev, N.\",\"Gorshenkov, M.\",\"Kuznetsov, D.\",\"Leontyev, I.\",\"Smirnova, N.\"],\"key\":\"kuriganova_comparison_2020\",\"id\":\"kuriganova_comparison_2020\",\"bibbaseid\":\"kuriganova-faddeev-gorshenkov-kuznetsov-leontyev-smirnova-acomparisonofbottomupandtopdownapproachestothesynthesisofptcelectrocatalysts-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.mdpi.com/2227-9717/8/8/947\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"PAC Synthesis and Comparison of Catalysts for Direct Ethanol Fuel Cells\",\"volume\":\"8\",\"issn\":\"2227-9717\",\"url\":\"https://www.mdpi.com/2227-9717/8/6/712\",\"doi\":\"10.3390/pr8060712\",\"abstract\":\"Pt/C, PtMOn/C (M = Ni, Sn, Ti, and PtX/C (X = Rh, Ir) catalyst systems were prepared by using the pulse alternating current (PAC) technique. Physical and electrochemical parameters of samples were carried out by x-ray powder diffraction (XRD), transmission electron microscopy (TEM), and CO stripping. The catalytic activity of the synthesized samples for the ethanol electrooxidation reaction (EOR) was investigated. The XRD patterns of the samples showed the presence of diffraction peaks characteristic for Pt, NiO, SnO2, TiO2, Rh, and Ir. The TEM images indicate that the Pt, Rh, and PtIr (alloys) particles had a uniform distribution over the carbon surface in the Pt/C, PtRh/C, PtIr/C, and PtMOn/C (M = Ni, Sn, Ti) catalysts. The electrochemically active surface area of catalysts was determined by the CO-stripping method. The addition of a second element to Pt or the use of hybrid supported catalysts can evidently improve the EOR activity. A remarkable positive affecting shift of the onset potential for the EOR was observed as follows: PtSnO2/C \\\\textgreater PtTiO2/C ≈ PtIr/C ≈ PtNiO/C \\\\textgreater PtRh/C ≈ Pt/C. The addition of SnO2 to Pt/C catalyst led to the decrease of the onset potential and to significantly facilitate the EOR. The long-term cyclic stability of the synthesized catalysts was investigated. Thereby, the PtSnO2/C catalyst prepared by the PAC technique can be considered as a promising anode catalyst for direct ethanol fuel cells.\",\"language\":\"en\",\"number\":\"6\",\"urldate\":\"2023-11-11\",\"journal\":\"Processes\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"Alexandra\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chernysheva\"],\"firstnames\":[\"Daria\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Faddeev\"],\"firstnames\":[\"Nikita\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dobrovolskii\"],\"firstnames\":[\"Yury\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2020\",\"pages\":\"712\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\JUTMKRJV\\\\\\\\Kuriganova и др. - 2020 - PAC Synthesis and Comparison of Catalysts for Dire.pdf:application/pdf\",\"bibtex\":\"@article{kuriganova_pac_2020,\\n\\ttitle = {{PAC} {Synthesis} and {Comparison} of {Catalysts} for {Direct} {Ethanol} {Fuel} {Cells}},\\n\\tvolume = {8},\\n\\tissn = {2227-9717},\\n\\turl = {https://www.mdpi.com/2227-9717/8/6/712},\\n\\tdoi = {10.3390/pr8060712},\\n\\tabstract = {Pt/C, PtMOn/C (M = Ni, Sn, Ti, and PtX/C (X = Rh, Ir) catalyst systems were prepared by using the pulse alternating current (PAC) technique. Physical and electrochemical parameters of samples were carried out by x-ray powder diffraction (XRD), transmission electron microscopy (TEM), and CO stripping. The catalytic activity of the synthesized samples for the ethanol electrooxidation reaction (EOR) was investigated. The XRD patterns of the samples showed the presence of diffraction peaks characteristic for Pt, NiO, SnO2, TiO2, Rh, and Ir. The TEM images indicate that the Pt, Rh, and PtIr (alloys) particles had a uniform distribution over the carbon surface in the Pt/C, PtRh/C, PtIr/C, and PtMOn/C (M = Ni, Sn, Ti) catalysts. The electrochemically active surface area of catalysts was determined by the CO-stripping method. The addition of a second element to Pt or the use of hybrid supported catalysts can evidently improve the EOR activity. A remarkable positive affecting shift of the onset potential for the EOR was observed as follows: PtSnO2/C {\\\\textgreater} PtTiO2/C ≈ PtIr/C ≈ PtNiO/C {\\\\textgreater} PtRh/C ≈ Pt/C. The addition of SnO2 to Pt/C catalyst led to the decrease of the onset potential and to significantly facilitate the EOR. The long-term cyclic stability of the synthesized catalysts was investigated. Thereby, the PtSnO2/C catalyst prepared by the PAC technique can be considered as a promising anode catalyst for direct ethanol fuel cells.},\\n\\tlanguage = {en},\\n\\tnumber = {6},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Processes},\\n\\tauthor = {Kuriganova, Alexandra and Chernysheva, Daria and Faddeev, Nikita and Leontyev, Igor and Smirnova, Nina and Dobrovolskii, Yury},\\n\\tmonth = jun,\\n\\tyear = {2020},\\n\\tpages = {712},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\JUTMKRJV\\\\\\\\Kuriganova и др. - 2020 - PAC Synthesis and Comparison of Catalysts for Dire.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Kuriganova, A.\",\"Chernysheva, D.\",\"Faddeev, N.\",\"Leontyev, I.\",\"Smirnova, N.\",\"Dobrovolskii, Y.\"],\"key\":\"kuriganova_pac_2020\",\"id\":\"kuriganova_pac_2020\",\"bibbaseid\":\"kuriganova-chernysheva-faddeev-leontyev-smirnova-dobrovolskii-pacsynthesisandcomparisonofcatalystsfordirectethanolfuelcells-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.mdpi.com/2227-9717/8/6/712\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Crystal-like order and defects in metazoan epithelia with spherical geometry\",\"volume\":\"10\",\"issn\":\"2045-2322\",\"url\":\"https://www.nature.com/articles/s41598-020-64598-w\",\"doi\":\"10.1038/s41598-020-64598-w\",\"abstract\":\"Abstract Since Robert Hooke studied cork cell patterns in 1665, scientists have been puzzled by why cells form such ordered structures. The laws underlying this type of organization are universal, and we study them comparing the living and non-living two-dimensional systems self-organizing at the spherical surface. Such-type physical systems often possess trigonal order with specific elongated defects, scars and pleats, where the 5-valence and 7-valence vertices alternate. In spite of the fact that the same physical and topological rules are involved in the structural organization of biological systems, such topological defects were never reported in epithelia. We have discovered them in the follicular spherical epithelium of ascidians that are emerging models in developmental biology. Surprisingly, the considered defects appear in the epithelium even when the number of cells in it is significantly less than the previously known threshold value. We explain this result by differences in the cell sizes and check our hypothesis considering the self-assembly of different random size particles on the spherical surface. Scars, pleats and other complex defects found in ascidian samples can play an unexpected and decisive role in the permanent renewal and reorganization of epithelia, which forms or lines many tissues and organs in metazoans.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Scientific Reports\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Roshal\"],\"firstnames\":[\"Daria\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Azzag\"],\"firstnames\":[\"Karim\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Le\",\"Goff\"],\"firstnames\":[\"Emilie\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergei\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Baghdiguian\"],\"firstnames\":[\"Stephen\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2020\",\"pages\":\"7652\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\JI45G85W\\\\\\\\Roshal и др. - 2020 - Crystal-like order and defects in metazoan epithel.pdf:application/pdf;Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\J7BDDRP3\\\\\\\\Roshal и др. - 2020 - Crystal-like order and defects in metazoan epithel.pdf:application/pdf\",\"bibtex\":\"@article{roshal_crystal-like_2020,\\n\\ttitle = {Crystal-like order and defects in metazoan epithelia with spherical geometry},\\n\\tvolume = {10},\\n\\tissn = {2045-2322},\\n\\turl = {https://www.nature.com/articles/s41598-020-64598-w},\\n\\tdoi = {10.1038/s41598-020-64598-w},\\n\\tabstract = {Abstract\\n            Since Robert Hooke studied cork cell patterns in 1665, scientists have been puzzled by why cells form such ordered structures. The laws underlying this type of organization are universal, and we study them comparing the living and non-living two-dimensional systems self-organizing at the spherical surface. Such-type physical systems often possess trigonal order with specific elongated defects, scars and pleats, where the 5-valence and 7-valence vertices alternate. In spite of the fact that the same physical and topological rules are involved in the structural organization of biological systems, such topological defects were never reported in epithelia. We have discovered them in the follicular spherical epithelium of ascidians that are emerging models in developmental biology. Surprisingly, the considered defects appear in the epithelium even when the number of cells in it is significantly less than the previously known threshold value. We explain this result by differences in the cell sizes and check our hypothesis considering the self-assembly of different random size particles on the spherical surface. Scars, pleats and other complex defects found in ascidian samples can play an unexpected and decisive role in the permanent renewal and reorganization of epithelia, which forms or lines many tissues and organs in metazoans.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Scientific Reports},\\n\\tauthor = {Roshal, Daria S. and Azzag, Karim and Le Goff, Emilie and Rochal, Sergei B. and Baghdiguian, Stephen},\\n\\tmonth = may,\\n\\tyear = {2020},\\n\\tpages = {7652},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\JI45G85W\\\\\\\\Roshal и др. - 2020 - Crystal-like order and defects in metazoan epithel.pdf:application/pdf;Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\J7BDDRP3\\\\\\\\Roshal и др. - 2020 - Crystal-like order and defects in metazoan epithel.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Roshal, D. S.\",\"Azzag, K.\",\"Le Goff, E.\",\"Rochal, S. B.\",\"Baghdiguian, S.\"],\"key\":\"roshal_crystal-like_2020\",\"id\":\"roshal_crystal-like_2020\",\"bibbaseid\":\"roshal-azzag-legoff-rochal-baghdiguian-crystallikeorderanddefectsinmetazoanepitheliawithsphericalgeometry-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.nature.com/articles/s41598-020-64598-w\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"address\":\"Saratov, Russian Federation\",\"title\":\"Surface acoustic waves based method to study photothermal response of plasmonic nano-objects and metasurfaces\",\"isbn\":\"978-1-5106-3718-4 978-1-5106-3719-1\",\"url\":\"https://www.spiedigitallibrary.org/conference-proceedings-of-spie/11457/2559972/Surface-acoustic-waves-based-method-to-study-photothermal-response-of/10.1117/12.2559972.full\",\"doi\":\"10.1117/12.2559972\",\"urldate\":\"2023-11-11\",\"booktitle\":\"Saratov Fall Meeting 2019: Optical and Nano-Technologies for Biology and Medicine\",\"publisher\":\"SPIE\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kaydashev\"],\"firstnames\":[\"Vladimir\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"Pavel\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kutepov\"],\"firstnames\":[\"Maxim\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Karapetyan\"],\"firstnames\":[\"Gevork\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kirtaev\"],\"firstnames\":[\"Roman\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"Evgeni\"],\"suffixes\":[]}],\"editor\":[{\"propositions\":[],\"lastnames\":[\"Tuchin\"],\"firstnames\":[\"Valery\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Genina\"],\"firstnames\":[\"Elina\",\"A.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2020\",\"pages\":\"13\",\"bibtex\":\"@inproceedings{kaydashev_surface_2020,\\n\\taddress = {Saratov, Russian Federation},\\n\\ttitle = {Surface acoustic waves based method to study photothermal response of plasmonic nano-objects and metasurfaces},\\n\\tisbn = {978-1-5106-3718-4 978-1-5106-3719-1},\\n\\turl = {https://www.spiedigitallibrary.org/conference-proceedings-of-spie/11457/2559972/Surface-acoustic-waves-based-method-to-study-photothermal-response-of/10.1117/12.2559972.full},\\n\\tdoi = {10.1117/12.2559972},\\n\\turldate = {2023-11-11},\\n\\tbooktitle = {Saratov {Fall} {Meeting} 2019: {Optical} and {Nano}-{Technologies} for {Biology} and {Medicine}},\\n\\tpublisher = {SPIE},\\n\\tauthor = {Kaydashev, Vladimir E. and Timoshenko, Pavel and Kutepov, Maxim and Karapetyan, Gevork and Kirtaev, Roman and Kaidashev, Evgeni},\\n\\teditor = {Tuchin, Valery V. and Genina, Elina A.},\\n\\tmonth = apr,\\n\\tyear = {2020},\\n\\tpages = {13},\\n}\\n\\n\",\"author_short\":[\"Kaydashev, V. E.\",\"Timoshenko, P.\",\"Kutepov, M.\",\"Karapetyan, G.\",\"Kirtaev, R.\",\"Kaidashev, E.\"],\"editor_short\":[\"Tuchin, V. V.\",\"Genina, E. A.\"],\"key\":\"kaydashev_surface_2020\",\"id\":\"kaydashev_surface_2020\",\"bibbaseid\":\"kaydashev-timoshenko-kutepov-karapetyan-kirtaev-kaidashev-surfaceacousticwavesbasedmethodtostudyphotothermalresponseofplasmonicnanoobjectsandmetasurfaces-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.spiedigitallibrary.org/conference-proceedings-of-spie/11457/2559972/Surface-acoustic-waves-based-method-to-study-photothermal-response-of/10.1117/12.2559972.full\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Controllable skyrmion chirality in ferroelectrics\",\"volume\":\"10\",\"issn\":\"2045-2322\",\"url\":\"https://www.nature.com/articles/s41598-020-65291-8\",\"doi\":\"10.1038/s41598-020-65291-8\",\"abstract\":\"Abstract Chirality, an intrinsic handedness, is one of the most intriguing fundamental phenomena in nature. Materials composed of chiral molecules find broad applications in areas ranging from nonlinear optics and spintronics to biology and pharmaceuticals. However, chirality is usually an invariable inherent property of a given material that cannot be easily changed at will. Here, we demonstrate that ferroelectric nanodots support skyrmions the chirality of which can be controlled and switched. We devise protocols for realizing control and efficient manipulations of the different types of skyrmions. Our findings open the route for controlled chirality with potential applications in ferroelectric-based information technologies.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Scientific Reports\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Tikhonov\"],\"firstnames\":[\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kondovych\"],\"firstnames\":[\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mangeri\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pavlenko\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Baudry\"],\"firstnames\":[\"L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sené\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Galda\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nakhmanson\"],\"firstnames\":[\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Heinonen\"],\"firstnames\":[\"O.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Luk’yanchuk\"],\"firstnames\":[\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vinokur\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2020\",\"pages\":\"8657\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\AXZJJ5II\\\\\\\\Tikhonov и др. - 2020 - Controllable skyrmion chirality in ferroelectrics.pdf:application/pdf\",\"bibtex\":\"@article{tikhonov_controllable_2020,\\n\\ttitle = {Controllable skyrmion chirality in ferroelectrics},\\n\\tvolume = {10},\\n\\tissn = {2045-2322},\\n\\turl = {https://www.nature.com/articles/s41598-020-65291-8},\\n\\tdoi = {10.1038/s41598-020-65291-8},\\n\\tabstract = {Abstract\\n            Chirality, an intrinsic handedness, is one of the most intriguing fundamental phenomena in nature. Materials composed of chiral molecules find broad applications in areas ranging from nonlinear optics and spintronics to biology and pharmaceuticals. However, chirality is usually an invariable inherent property of a given material that cannot be easily changed at will. Here, we demonstrate that ferroelectric nanodots support skyrmions the chirality of which can be controlled and switched. We devise protocols for realizing control and efficient manipulations of the different types of skyrmions. Our findings open the route for controlled chirality with potential applications in ferroelectric-based information technologies.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Scientific Reports},\\n\\tauthor = {Tikhonov, Yu. and Kondovych, S. and Mangeri, J. and Pavlenko, M. and Baudry, L. and Sené, A. and Galda, A. and Nakhmanson, S. and Heinonen, O. and Razumnaya, A. and Luk’yanchuk, I. and Vinokur, V. M.},\\n\\tmonth = may,\\n\\tyear = {2020},\\n\\tpages = {8657},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\AXZJJ5II\\\\\\\\Tikhonov и др. - 2020 - Controllable skyrmion chirality in ferroelectrics.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Tikhonov, Y.\",\"Kondovych, S.\",\"Mangeri, J.\",\"Pavlenko, M.\",\"Baudry, L.\",\"Sené, A.\",\"Galda, A.\",\"Nakhmanson, S.\",\"Heinonen, O.\",\"Razumnaya, A.\",\"Luk’yanchuk, I.\",\"Vinokur, V. M.\"],\"key\":\"tikhonov_controllable_2020\",\"id\":\"tikhonov_controllable_2020\",\"bibbaseid\":\"tikhonov-kondovych-mangeri-pavlenko-baudry-sen-galda-nakhmanson-etal-controllableskyrmionchiralityinferroelectrics-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.nature.com/articles/s41598-020-65291-8\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Hopfions emerge in ferroelectrics\",\"volume\":\"11\",\"issn\":\"2041-1723\",\"url\":\"https://www.nature.com/articles/s41467-020-16258-w\",\"doi\":\"10.1038/s41467-020-16258-w\",\"abstract\":\"Abstract Paradigmatic knotted solitons, Hopfions, that are characterized by topological Hopf invariant, attract an intense attention in the diverse areas of physics ranging from high-energy physics, cosmology and astrophysics to biology, magneto- and hydrodynamics and condensed matter physics. Yet, while being of broad interest, they remain elusive and under-explored. Here we demonstrate that Hopfions emerge as a basic configuration of polarization field in confined ferroelectric nanoparticles. Our findings establish that Hopfions are of fundamental importance for the electromagnetic behavior of the nanocomposits and can result in advanced functionalities of these materials.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Nature Communications\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Luk’yanchuk\"],\"firstnames\":[\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tikhonov\"],\"firstnames\":[\"Y.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vinokur\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2020\",\"pages\":\"2433\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\B5GV9UWB\\\\Łuk’yanchuk и др. - 2020 - Hopfions emerge in ferroelectrics.pdf:application/pdf\",\"bibtex\":\"@article{lukyanchuk_hopfions_2020,\\n\\ttitle = {Hopfions emerge in ferroelectrics},\\n\\tvolume = {11},\\n\\tissn = {2041-1723},\\n\\turl = {https://www.nature.com/articles/s41467-020-16258-w},\\n\\tdoi = {10.1038/s41467-020-16258-w},\\n\\tabstract = {Abstract\\n            Paradigmatic knotted solitons, Hopfions, that are characterized by topological Hopf invariant, attract an intense attention in the diverse areas of physics ranging from high-energy physics, cosmology and astrophysics to biology, magneto- and hydrodynamics and condensed matter physics. Yet, while being of broad interest, they remain elusive and under-explored. Here we demonstrate that Hopfions emerge as a basic configuration of polarization field in confined ferroelectric nanoparticles. Our findings establish that Hopfions are of fundamental importance for the electromagnetic behavior of the nanocomposits and can result in advanced functionalities of these materials.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Nature Communications},\\n\\tauthor = {Luk’yanchuk, I. and Tikhonov, Y. and Razumnaya, A. and Vinokur, V. M.},\\n\\tmonth = may,\\n\\tyear = {2020},\\n\\tpages = {2433},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\B5GV9UWB\\\\\\\\Luk’yanchuk и др. - 2020 - Hopfions emerge in ferroelectrics.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Luk’yanchuk, I.\",\"Tikhonov, Y.\",\"Razumnaya, A.\",\"Vinokur, V. M.\"],\"key\":\"lukyanchuk_hopfions_2020\",\"id\":\"lukyanchuk_hopfions_2020\",\"bibbaseid\":\"lukyanchuk-tikhonov-razumnaya-vinokur-hopfionsemergeinferroelectrics-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.nature.com/articles/s41467-020-16258-w\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Lattice Dynamics of the Strontium Ferrotungstate in the Temperature Range 300–700 K\",\"volume\":\"62\",\"issn\":\"1063-7834, 1090-6460\",\"url\":\"http://link.springer.com/10.1134/S1063783420120033\",\"doi\":\"10.1134/S1063783420120033\",\"language\":\"en\",\"number\":\"12\",\"urldate\":\"2023-11-11\",\"journal\":\"Physics of the Solid State\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Anokhin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pavlenko\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2020\",\"pages\":\"2434–2438\",\"bibtex\":\"@article{anokhin_lattice_2020,\\n\\ttitle = {Lattice {Dynamics} of the {Strontium} {Ferrotungstate} in the {Temperature} {Range} 300–700 {K}},\\n\\tvolume = {62},\\n\\tissn = {1063-7834, 1090-6460},\\n\\turl = {http://link.springer.com/10.1134/S1063783420120033},\\n\\tdoi = {10.1134/S1063783420120033},\\n\\tlanguage = {en},\\n\\tnumber = {12},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physics of the Solid State},\\n\\tauthor = {Anokhin, A. S. and Razumnaya, A. G. and Pavlenko, A. V.},\\n\\tmonth = dec,\\n\\tyear = {2020},\\n\\tpages = {2434--2438},\\n}\\n\\n\",\"author_short\":[\"Anokhin, A. S.\",\"Razumnaya, A. G.\",\"Pavlenko, A. V.\"],\"key\":\"anokhin_lattice_2020\",\"id\":\"anokhin_lattice_2020\",\"bibbaseid\":\"anokhin-razumnaya-pavlenko-latticedynamicsofthestrontiumferrotungstateinthetemperaturerange300700k-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://link.springer.com/10.1134/S1063783420120033\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Electrochemical dispersion technique for the preparation of Sn-doped Pt particles and their use as electrocatalysts\",\"volume\":\"30\",\"issn\":\"09599436\",\"url\":\"https://linkinghub.elsevier.com/retrieve/pii/S0959943620302625\",\"doi\":\"10.1016/j.mencom.2020.09.037\",\"language\":\"en\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Mendeleev Communications\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"Alexandra\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ulyankina\"],\"firstnames\":[\"Anna\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\",\"V.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2020\",\"pages\":\"663–665\",\"bibtex\":\"@article{kuriganova_electrochemical_2020,\\n\\ttitle = {Electrochemical dispersion technique for the preparation of {Sn}-doped {Pt} particles and their use as electrocatalysts},\\n\\tvolume = {30},\\n\\tissn = {09599436},\\n\\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0959943620302625},\\n\\tdoi = {10.1016/j.mencom.2020.09.037},\\n\\tlanguage = {en},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Mendeleev Communications},\\n\\tauthor = {Kuriganova, Alexandra B. and Leontyev, Igor N. and Ulyankina, Anna A. and Smirnova, Nina V.},\\n\\tmonth = sep,\\n\\tyear = {2020},\\n\\tpages = {663--665},\\n}\\n\\n\",\"author_short\":[\"Kuriganova, A. B.\",\"Leontyev, I. N.\",\"Ulyankina, A. A.\",\"Smirnova, N. V.\"],\"key\":\"kuriganova_electrochemical_2020\",\"id\":\"kuriganova_electrochemical_2020\",\"bibbaseid\":\"kuriganova-leontyev-ulyankina-smirnova-electrochemicaldispersiontechniqueforthepreparationofsndopedptparticlesandtheiruseaselectrocatalysts-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://linkinghub.elsevier.com/retrieve/pii/S0959943620302625\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"2N+4-rule and an atlas of bulk optical resonances of zigzag graphene nanoribbons\",\"volume\":\"11\",\"issn\":\"2041-1723\",\"url\":\"https://www.nature.com/articles/s41467-019-13728-8\",\"doi\":\"10.1038/s41467-019-13728-8\",\"abstract\":\"Abstract Development of on-chip integrated carbon-based optoelectronic nanocircuits requires fast and non-invasive structural characterization of their building blocks. Recent advances in synthesis of single wall carbon nanotubes and graphene nanoribbons allow for their use as atomically precise building blocks. However, while cataloged experimental data are available for the structural characterization of carbon nanotubes, such an atlas is absent for graphene nanoribbons. Here we theoretically investigate the optical absorption resonances of armchair carbon nanotubes and zigzag graphene nanoribbons continuously spanning the tube (ribbon) transverse sizes from 0.5(0.4) nm to 8.1(12.8) nm. We show that the linear mapping is guaranteed between the tube and ribbon bulk resonance when the number of atoms in the tube unit cell is $$2N+4$$ 2 N + 4 , where $$N$$ N is the number of atoms in the ribbon unit cell. Thus, an atlas of carbon nanotubes optical transitions can be mapped to an atlas of zigzag graphene nanoribbons.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-10\",\"journal\":\"Nature Communications\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Payod\"],\"firstnames\":[\"Renebeth\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grassano\"],\"firstnames\":[\"Davide\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Santos\"],\"firstnames\":[\"Gil\",\"Nonato\",\"C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Levshov\"],\"firstnames\":[\"Dmitry\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pulci\"],\"firstnames\":[\"Olivia\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Saroka\"],\"firstnames\":[\"Vasil\",\"A.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2020\",\"pages\":\"82\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\GVJGZB4S\\\\¶ayod и др. - 2020 - 2N+4-rule and an atlas of bulk optical resonances .pdf:application/pdf\",\"bibtex\":\"@article{payod_2n4-rule_2020,\\n\\ttitle = {{2N}+4-rule and an atlas of bulk optical resonances of zigzag graphene nanoribbons},\\n\\tvolume = {11},\\n\\tissn = {2041-1723},\\n\\turl = {https://www.nature.com/articles/s41467-019-13728-8},\\n\\tdoi = {10.1038/s41467-019-13728-8},\\n\\tabstract = {Abstract\\n            \\n              Development of on-chip integrated carbon-based optoelectronic nanocircuits requires fast and non-invasive structural characterization of their building blocks. Recent advances in synthesis of single wall carbon nanotubes and graphene nanoribbons allow for their use as atomically precise building blocks. However, while cataloged experimental data are available for the structural characterization of carbon nanotubes, such an atlas is absent for graphene nanoribbons. Here we theoretically investigate the optical absorption resonances of armchair carbon nanotubes and zigzag graphene nanoribbons continuously spanning the tube (ribbon) transverse sizes from 0.5(0.4) nm to 8.1(12.8) nm. We show that the linear mapping is guaranteed between the tube and ribbon bulk resonance when the number of atoms in the tube unit cell is\\n              \\n                \\n                  \\\\$\\\\$2N+4\\\\$\\\\$\\n                  \\n                    2\\n                    N\\n                    +\\n                    4\\n                  \\n                \\n              \\n              , where\\n              \\n                \\n                  \\\\$\\\\$N\\\\$\\\\$\\n                  \\n                    N\\n                  \\n                \\n              \\n              is the number of atoms in the ribbon unit cell. Thus, an atlas of carbon nanotubes optical transitions can be mapped to an atlas of zigzag graphene nanoribbons.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-10},\\n\\tjournal = {Nature Communications},\\n\\tauthor = {Payod, Renebeth B. and Grassano, Davide and Santos, Gil Nonato C. and Levshov, Dmitry I. and Pulci, Olivia and Saroka, Vasil A.},\\n\\tmonth = jan,\\n\\tyear = {2020},\\n\\tpages = {82},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\GVJGZB4S\\\\\\\\Payod и др. - 2020 - 2N+4-rule and an atlas of bulk optical resonances .pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Payod, R. B.\",\"Grassano, D.\",\"Santos, G. N. C.\",\"Levshov, D. I.\",\"Pulci, O.\",\"Saroka, V. A.\"],\"key\":\"payod_2n4-rule_2020\",\"id\":\"payod_2n4-rule_2020\",\"bibbaseid\":\"payod-grassano-santos-levshov-pulci-saroka-2n4ruleandanatlasofbulkopticalresonancesofzigzaggraphenenanoribbons-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.nature.com/articles/s41467-019-13728-8\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Tunable Electromechanical Properties of a Barium Strontium Titanate Ferroelectric Film Under a Uniaxial Stress\",\"volume\":\"67\",\"issn\":\"0885-3010, 1525-8955\",\"url\":\"https://ieeexplore.ieee.org/document/9146729/\",\"doi\":\"10.1109/TUFFC.2020.3011591\",\"number\":\"12\",\"urldate\":\"2023-11-11\",\"journal\":\"IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"Vladimir\",\"Borisovich\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"Pavel\",\"Evgenjevich\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pan'kin\"],\"firstnames\":[\"Artyom\",\"Vital'yevich\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"Anna\",\"Grigoryevna\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2020\",\"pages\":\"2704–2709\",\"bibtex\":\"@article{shirokov_tunable_2020,\\n\\ttitle = {Tunable {Electromechanical} {Properties} of a {Barium} {Strontium} {Titanate} {Ferroelectric} {Film} {Under} a {Uniaxial} {Stress}},\\n\\tvolume = {67},\\n\\tissn = {0885-3010, 1525-8955},\\n\\turl = {https://ieeexplore.ieee.org/document/9146729/},\\n\\tdoi = {10.1109/TUFFC.2020.3011591},\\n\\tnumber = {12},\\n\\turldate = {2023-11-11},\\n\\tjournal = {IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control},\\n\\tauthor = {Shirokov, Vladimir Borisovich and Timoshenko, Pavel Evgenjevich and Pan'kin, Artyom Vital'yevich and Razumnaya, Anna Grigoryevna},\\n\\tmonth = dec,\\n\\tyear = {2020},\\n\\tpages = {2704--2709},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Timoshenko, P. E.\",\"Pan'kin, A. V.\",\"Razumnaya, A. G.\"],\"key\":\"shirokov_tunable_2020\",\"id\":\"shirokov_tunable_2020\",\"bibbaseid\":\"shirokov-timoshenko-pankin-razumnaya-tunableelectromechanicalpropertiesofabariumstrontiumtitanateferroelectricfilmunderauniaxialstress-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://ieeexplore.ieee.org/document/9146729/\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Structural, dielectric, and ferroelectric properties of lead-free BCZT ceramics elaborated by low-temperature hydrothermal processing\",\"volume\":\"31\",\"issn\":\"0957-4522, 1573-482X\",\"url\":\"https://link.springer.com/10.1007/s10854-020-03555-9\",\"doi\":\"10.1007/s10854-020-03555-9\",\"language\":\"en\",\"number\":\"13\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Materials Science: Materials in Electronics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Hanani\"],\"firstnames\":[\"Zouhair\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzane\"],\"firstnames\":[\"Daoud\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Amjoud\"],\"firstnames\":[\"M’barek\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gagou\"],\"firstnames\":[\"Yaovi\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hoummada\"],\"firstnames\":[\"Khalid\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Perrin\"],\"firstnames\":[\"Carine\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"Anna\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kutnjak\"],\"firstnames\":[\"Zdravko\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bouzina\"],\"firstnames\":[\"Adnane\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Marssi\"],\"firstnames\":[\"Mimoun\",\"El\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gouné\"],\"firstnames\":[\"Mohamed\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rožič\"],\"firstnames\":[\"Brigita\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2020\",\"pages\":\"10096–10104\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\ZEME2MZQ\\\\a̋nani и др. - 2020 - Structural, dielectric, and ferroelectric properti.pdf:application/pdf\",\"bibtex\":\"@article{hanani_structural_2020,\\n\\ttitle = {Structural, dielectric, and ferroelectric properties of lead-free {BCZT} ceramics elaborated by low-temperature hydrothermal processing},\\n\\tvolume = {31},\\n\\tissn = {0957-4522, 1573-482X},\\n\\turl = {https://link.springer.com/10.1007/s10854-020-03555-9},\\n\\tdoi = {10.1007/s10854-020-03555-9},\\n\\tlanguage = {en},\\n\\tnumber = {13},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Materials Science: Materials in Electronics},\\n\\tauthor = {Hanani, Zouhair and Mezzane, Daoud and Amjoud, M’barek and Gagou, Yaovi and Hoummada, Khalid and Perrin, Carine and Razumnaya, Anna G. and Kutnjak, Zdravko and Bouzina, Adnane and Marssi, Mimoun El and Gouné, Mohamed and Rožič, Brigita},\\n\\tmonth = jul,\\n\\tyear = {2020},\\n\\tpages = {10096--10104},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\ZEME2MZQ\\\\\\\\Hanani и др. - 2020 - Structural, dielectric, and ferroelectric properti.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Hanani, Z.\",\"Mezzane, D.\",\"Amjoud, M.\",\"Gagou, Y.\",\"Hoummada, K.\",\"Perrin, C.\",\"Razumnaya, A. G.\",\"Kutnjak, Z.\",\"Bouzina, A.\",\"Marssi, M. E.\",\"Gouné, M.\",\"Rožič, B.\"],\"key\":\"hanani_structural_2020\",\"id\":\"hanani_structural_2020\",\"bibbaseid\":\"hanani-mezzane-amjoud-gagou-hoummada-perrin-razumnaya-kutnjak-etal-structuraldielectricandferroelectricpropertiesofleadfreebcztceramicselaboratedbylowtemperaturehydrothermalprocessing-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.springer.com/10.1007/s10854-020-03555-9\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Enhanced dielectric and electrocaloric properties in lead-free rod-like BCZT ceramics\",\"volume\":\"9\",\"issn\":\"2226-4108, 2227-8508\",\"url\":\"http://link.springer.com/10.1007/s40145-020-0361-1\",\"doi\":\"10.1007/s40145-020-0361-1\",\"abstract\":\"Abstract Ba 0.85 Ca 0.15 Zr 0.10 Ti 0.90 O 3 (BCZT) lead-free ceramics demonstrated excellent dielectric, ferroelectric, and piezoelectric properties at the morphotropic phase boundary (MPB). So far, to study the effect of morphological changes on dielectric and ferroelectric properties in lead-free BCZT ceramics, researchers have mostly focused on the influence of spherical grain shape change. In this study, BCZT ceramics with rod-like grains and aspect ratio of about 10 were synthesized by surfactant-assisted solvothermal route. X-ray diffraction (XRD) and selected area electron diffraction (SAED) performed at room temperature confirm the crystallization of pure perovskite with tetragonal symmetry. Scanning electron microscopy (SEM) image showed that BCZT ceramics have kept the 1D rod-like grains with an average aspect ratio of about 4. Rod-like BCZT ceramics exhibit enhanced dielectric ferroelectric (ɛ r = 11,906, tanδ = 0.014, P r = 6.01 μgC/cm 2 , and E c = 2.46 kV/cm), and electrocaloric properties (Δ T = 0.492 K and gZ = 0.289 (K·mm)/kV at 17 kV/cm) with respect to spherical BCZT ceramics. Therefore, rod-like BCZT lead-free ceramics have good potential to be used in solid-state refrigeration technology.\",\"language\":\"en\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Advanced Ceramics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Hanani\"],\"firstnames\":[\"Zouhair\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Merselmiz\"],\"firstnames\":[\"Soukaina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Danine\"],\"firstnames\":[\"Abdelaadim\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Stein\"],\"firstnames\":[\"Nicolas\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzane\"],\"firstnames\":[\"Daoud\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Amjoud\"],\"firstnames\":[\"M’barek\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lahcini\"],\"firstnames\":[\"Mohammed\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gagou\"],\"firstnames\":[\"Yaovi\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Spreitzer\"],\"firstnames\":[\"Matjaz\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vengust\"],\"firstnames\":[\"Damjan\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kutnjak\"],\"firstnames\":[\"Zdravko\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"Mimoun\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Luk’yanchuk\"],\"firstnames\":[\"Igor\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gouné\"],\"firstnames\":[\"Mohamed\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2020\",\"pages\":\"210–219\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\¶IFXGEQ5\\\\a̋nani и др. - 2020 - Enhanced dielectric and electrocaloric properties .pdf:application/pdf\",\"bibtex\":\"@article{hanani_enhanced_2020,\\n\\ttitle = {Enhanced dielectric and electrocaloric properties in lead-free rod-like {BCZT} ceramics},\\n\\tvolume = {9},\\n\\tissn = {2226-4108, 2227-8508},\\n\\turl = {http://link.springer.com/10.1007/s40145-020-0361-1},\\n\\tdoi = {10.1007/s40145-020-0361-1},\\n\\tabstract = {Abstract\\n            \\n              Ba\\n              0.85\\n              Ca\\n              0.15\\n              Zr\\n              0.10\\n              Ti\\n              0.90\\n              O\\n              3\\n              (BCZT) lead-free ceramics demonstrated excellent dielectric, ferroelectric, and piezoelectric properties at the morphotropic phase boundary (MPB). So far, to study the effect of morphological changes on dielectric and ferroelectric properties in lead-free BCZT ceramics, researchers have mostly focused on the influence of spherical grain shape change. In this study, BCZT ceramics with rod-like grains and aspect ratio of about 10 were synthesized by surfactant-assisted solvothermal route. X-ray diffraction (XRD) and selected area electron diffraction (SAED) performed at room temperature confirm the crystallization of pure perovskite with tetragonal symmetry. Scanning electron microscopy (SEM) image showed that BCZT ceramics have kept the 1D rod-like grains with an average aspect ratio of about 4. Rod-like BCZT ceramics exhibit enhanced dielectric ferroelectric (ɛ\\n              r\\n              = 11,906, tanδ = 0.014,\\n              P\\n              r\\n              = 6.01 μgC/cm\\n              2\\n              , and\\n              E\\n              c\\n              = 2.46 kV/cm), and electrocaloric properties (Δ\\n              T\\n              = 0.492 K and gZ = 0.289 (K·mm)/kV at 17 kV/cm) with respect to spherical BCZT ceramics. Therefore, rod-like BCZT lead-free ceramics have good potential to be used in solid-state refrigeration technology.},\\n\\tlanguage = {en},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Advanced Ceramics},\\n\\tauthor = {Hanani, Zouhair and Merselmiz, Soukaina and Danine, Abdelaadim and Stein, Nicolas and Mezzane, Daoud and Amjoud, M’barek and Lahcini, Mohammed and Gagou, Yaovi and Spreitzer, Matjaz and Vengust, Damjan and Kutnjak, Zdravko and El Marssi, Mimoun and Luk’yanchuk, Igor A. and Gouné, Mohamed},\\n\\tmonth = apr,\\n\\tyear = {2020},\\n\\tpages = {210--219},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\PIFXGEQ5\\\\\\\\Hanani и др. - 2020 - Enhanced dielectric and electrocaloric properties .pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Hanani, Z.\",\"Merselmiz, S.\",\"Danine, A.\",\"Stein, N.\",\"Mezzane, D.\",\"Amjoud, M.\",\"Lahcini, M.\",\"Gagou, Y.\",\"Spreitzer, M.\",\"Vengust, D.\",\"Kutnjak, Z.\",\"El Marssi, M.\",\"Luk’yanchuk, I. A.\",\"Gouné, M.\"],\"key\":\"hanani_enhanced_2020\",\"id\":\"hanani_enhanced_2020\",\"bibbaseid\":\"hanani-merselmiz-danine-stein-mezzane-amjoud-lahcini-gagou-etal-enhanceddielectricandelectrocaloricpropertiesinleadfreerodlikebcztceramics-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://link.springer.com/10.1007/s40145-020-0361-1\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Terahertz-infrared spectroscopy of Ti4+-doped M-type barium hexaferrite\",\"volume\":\"820\",\"issn\":\"09258388\",\"url\":\"https://linkinghub.elsevier.com/retrieve/pii/S0925838819346444\",\"doi\":\"10.1016/j.jallcom.2019.153398\",\"language\":\"en\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Alloys and Compounds\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Alyabyeva\"],\"firstnames\":[\"Liudmila\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yegiyan\"],\"firstnames\":[\"Samvel\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"Victor\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"Anatoly\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vinnik\"],\"firstnames\":[\"Denis\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gudkova\"],\"firstnames\":[\"Svetlana\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zherebtsov\"],\"firstnames\":[\"Dmitry\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"Martin\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"Boris\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2020\",\"pages\":\"153398\",\"bibtex\":\"@article{alyabyeva_terahertz-infrared_2020,\\n\\ttitle = {Terahertz-infrared spectroscopy of {Ti4}+-doped {M}-type barium hexaferrite},\\n\\tvolume = {820},\\n\\tissn = {09258388},\\n\\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0925838819346444},\\n\\tdoi = {10.1016/j.jallcom.2019.153398},\\n\\tlanguage = {en},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Alloys and Compounds},\\n\\tauthor = {Alyabyeva, Liudmila and Yegiyan, Samvel and Torgashev, Victor and Prokhorov, Anatoly S. and Vinnik, Denis and Gudkova, Svetlana and Zherebtsov, Dmitry and Dressel, Martin and Gorshunov, Boris},\\n\\tmonth = apr,\\n\\tyear = {2020},\\n\\tpages = {153398},\\n}\\n\\n\",\"author_short\":[\"Alyabyeva, L.\",\"Yegiyan, S.\",\"Torgashev, V.\",\"Prokhorov, A. S.\",\"Vinnik, D.\",\"Gudkova, S.\",\"Zherebtsov, D.\",\"Dressel, M.\",\"Gorshunov, B.\"],\"key\":\"alyabyeva_terahertz-infrared_2020\",\"id\":\"alyabyeva_terahertz-infrared_2020\",\"bibbaseid\":\"alyabyeva-yegiyan-torgashev-prokhorov-vinnik-gudkova-zherebtsov-dressel-etal-terahertzinfraredspectroscopyofti4dopedmtypebariumhexaferrite-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://linkinghub.elsevier.com/retrieve/pii/S0925838819346444\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Thermally-stable high energy storage performances and large electrocaloric effect over a broad temperature span in lead-free BCZT ceramic\",\"volume\":\"10\",\"issn\":\"2046-2069\",\"url\":\"http://xlink.rsc.org/?DOI=D0RA06116F\",\"doi\":\"10.1039/D0RA06116F\",\"abstract\":\"Thermally-stable recovered energy density and significant electrocaloric temperature change over a broad temperature span in BCZT ceramic elaborated by low-temperature hydrothermal processing. , Ba 0.85 Ca 0.15 Zr 0.10 Ti 0.90 O 3 (BCZT) relaxor ferroelectric ceramics exhibit enhanced energy storage and electrocaloric performances due to their excellent dielectric and ferroelectric properties. In this study, the temperature-dependence of the structural and dielectric properties, as well as the field and temperature-dependence of the energy storage and the electrocaloric properties in BCZT ceramics elaborated at low-temperature hydrothermal processing are investigated. X-ray diffraction and Raman spectroscopy results confirmed the ferroelectric–paraelectric phase transition in the BCZT ceramic. At room temperature and 1 kHz, the dielectric constant and dielectric loss reached 5000 and 0.029, respectively. The BCZT ceramic showed a large recovered energy density ( W rec ) of 414.1 mJ cm −3 at 380 K, with an energy efficiency of 78.6%, and high thermal-stability of W rec of 3.9% in the temperature range of 340–400 K. The electrocaloric effect in BCZT was explored via an indirect approach following the Maxwell relation at 60 kV cm −1 . The significant electrocaloric temperature change of 1.479 K at 367 K, a broad temperature span of 87 K, an enhanced refrigerant capacity of 140.33 J kg −1 , and a high coefficient of performance of 6.12 obtained at 60 kV cm −1 make BCZT ceramics potentially useful coolant materials in the development of future eco-friendly solid-state refrigeration technology.\",\"language\":\"en\",\"number\":\"51\",\"urldate\":\"2023-11-11\",\"journal\":\"RSC Advances\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Hanani\"],\"firstnames\":[\"Zouhair\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Merselmiz\"],\"firstnames\":[\"Soukaina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzane\"],\"firstnames\":[\"Daoud\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Amjoud\"],\"firstnames\":[\"M'barek\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bradeško\"],\"firstnames\":[\"Andraž\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rožič\"],\"firstnames\":[\"Brigita\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lahcini\"],\"firstnames\":[\"Mohammed\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"Mimoun\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ragulya\"],\"firstnames\":[\"Andrey\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Luk'yanchuk\"],\"firstnames\":[\"Igor\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kutnjak\"],\"firstnames\":[\"Zdravko\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gouné\"],\"firstnames\":[\"Mohamed\"],\"suffixes\":[]}],\"year\":\"2020\",\"pages\":\"30746–30755\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\3987HKNB\\\\a̋nani и др. - 2020 - Thermally-stable high energy storage performances .pdf:application/pdf\",\"bibtex\":\"@article{hanani_thermally-stable_2020,\\n\\ttitle = {Thermally-stable high energy storage performances and large electrocaloric effect over a broad temperature span in lead-free {BCZT} ceramic},\\n\\tvolume = {10},\\n\\tissn = {2046-2069},\\n\\turl = {http://xlink.rsc.org/?DOI=D0RA06116F},\\n\\tdoi = {10.1039/D0RA06116F},\\n\\tabstract = {Thermally-stable recovered energy density and significant electrocaloric temperature change over a broad temperature span in BCZT ceramic elaborated by low-temperature hydrothermal processing.\\n          , \\n            \\n              Ba\\n              0.85\\n              Ca\\n              0.15\\n              Zr\\n              0.10\\n              Ti\\n              0.90\\n              O\\n              3\\n              (BCZT) relaxor ferroelectric ceramics exhibit enhanced energy storage and electrocaloric performances due to their excellent dielectric and ferroelectric properties. In this study, the temperature-dependence of the structural and dielectric properties, as well as the field and temperature-dependence of the energy storage and the electrocaloric properties in BCZT ceramics elaborated at low-temperature hydrothermal processing are investigated. X-ray diffraction and Raman spectroscopy results confirmed the ferroelectric–paraelectric phase transition in the BCZT ceramic. At room temperature and 1 kHz, the dielectric constant and dielectric loss reached 5000 and 0.029, respectively. The BCZT ceramic showed a large recovered energy density (\\n              W\\n              rec\\n              ) of 414.1 mJ cm\\n              −3\\n              at 380 K, with an energy efficiency of 78.6\\\\%, and high thermal-stability of\\n              W\\n              rec\\n              of 3.9\\\\% in the temperature range of 340–400 K. The electrocaloric effect in BCZT was explored\\n              via\\n              an indirect approach following the Maxwell relation at 60 kV cm\\n              −1\\n              . The significant electrocaloric temperature change of 1.479 K at 367 K, a broad temperature span of 87 K, an enhanced refrigerant capacity of 140.33 J kg\\n              −1\\n              , and a high coefficient of performance of 6.12 obtained at 60 kV cm\\n              −1\\n              make BCZT ceramics potentially useful coolant materials in the development of future eco-friendly solid-state refrigeration technology.},\\n\\tlanguage = {en},\\n\\tnumber = {51},\\n\\turldate = {2023-11-11},\\n\\tjournal = {RSC Advances},\\n\\tauthor = {Hanani, Zouhair and Merselmiz, Soukaina and Mezzane, Daoud and Amjoud, M'barek and Bradeško, Andraž and Rožič, Brigita and Lahcini, Mohammed and El Marssi, Mimoun and Ragulya, Andrey V. and Luk'yanchuk, Igor A. and Kutnjak, Zdravko and Gouné, Mohamed},\\n\\tyear = {2020},\\n\\tpages = {30746--30755},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\3987HKNB\\\\\\\\Hanani и др. - 2020 - Thermally-stable high energy storage performances .pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Hanani, Z.\",\"Merselmiz, S.\",\"Mezzane, D.\",\"Amjoud, M.\",\"Bradeško, A.\",\"Rožič, B.\",\"Lahcini, M.\",\"El Marssi, M.\",\"Ragulya, A. V.\",\"Luk'yanchuk, I. A.\",\"Kutnjak, Z.\",\"Gouné, M.\"],\"key\":\"hanani_thermally-stable_2020\",\"id\":\"hanani_thermally-stable_2020\",\"bibbaseid\":\"hanani-merselmiz-mezzane-amjoud-bradeko-roi-lahcini-elmarssi-etal-thermallystablehighenergystorageperformancesandlargeelectrocaloriceffectoverabroadtemperaturespaninleadfreebcztceramic-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://xlink.rsc.org/?DOI=D0RA06116F\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Finite-element Modeling of SAW-filters Based on Thin Films of Barium Strontium Titanate\",\"volume\":\"17\",\"issn\":\"1729-5459\",\"url\":\"https://elibrary.ru/doi_resolution.asp?doi=10%2E31429%2Fvestnik%2D17%2D4%2D48%2D56\",\"doi\":\"10.31429/vestnik-17-4-48-56\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Ecological Bulletin of Research Centers of the Black Sea Economic Cooperation\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kalinchuk\"],\"firstnames\":[\"V.V.\"],\"suffixes\":[]}],\"year\":\"2020\",\"pages\":\"48–56\",\"bibtex\":\"@article{timoshenko_finite-element_2020,\\n\\ttitle = {Finite-element {Modeling} of {SAW}-filters {Based} on {Thin} {Films} of {Barium} {Strontium} {Titanate}},\\n\\tvolume = {17},\\n\\tissn = {1729-5459},\\n\\turl = {https://elibrary.ru/doi_resolution.asp?doi=10%2E31429%2Fvestnik%2D17%2D4%2D48%2D56},\\n\\tdoi = {10.31429/vestnik-17-4-48-56},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ecological Bulletin of Research Centers of the Black Sea Economic Cooperation},\\n\\tauthor = {Timoshenko, P.E. and Shirokov, V.B. and Kalinchuk, V.V.},\\n\\tyear = {2020},\\n\\tpages = {48--56},\\n}\\n\\n\",\"author_short\":[\"Timoshenko, P.\",\"Shirokov, V.\",\"Kalinchuk, V.\"],\"key\":\"timoshenko_finite-element_2020\",\"id\":\"timoshenko_finite-element_2020\",\"bibbaseid\":\"timoshenko-shirokov-kalinchuk-finiteelementmodelingofsawfiltersbasedonthinfilmsofbariumstrontiumtitanate-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/doi_resolution.asp?doi=10%2E31429%2Fvestnik%2D17%2D4%2D48%2D56\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Irreversible and reversible morphological changes in the <i>ϕ</i> 6 capsid and similar viral shells: symmetry and micromechanics\",\"volume\":\"16\",\"issn\":\"1744-683X, 1744-6848\",\"shorttitle\":\"Irreversible and reversible morphological changes in the <i>ϕ</i> 6 capsid and similar viral shells\",\"url\":\"http://xlink.rsc.org/?DOI=D0SM01338B\",\"doi\":\"10.1039/D0SM01338B\",\"abstract\":\"We propose a new micromechanical model perfectly describing the capsid shapes and morphological transformations that occur between the states of the dodecahedral ϕ 6 capsid and similar viral shells due to the sequential packaging of RNA segments. , Understanding the physicochemical processes occurring in viruses during their maturation is of fundamental importance since only mature viruses can infect host cells. Here we consider the irreversible and reversible morphological changes that occur with the dodecahedral ϕ 6 procapsid during the sequential packaging of 3 RNA segments forming the viral genome. It is shown that the dodecahedral shape of all the four observed capsid states is perfectly reproduced by a sphere radially deformed by only two irreducible spherical harmonics with icosahedral symmetry and wave numbers l = 6 and l = 10. The rotation of proteins around the 3-fold axes at the Procapsid → Intermediate 1 irreversible transformation is in fact also well described with the shear field containing only two irreducible harmonics with the same two wave numbers. The high stability of the Intermediate 1 state is discussed and the shapes of the Intermediate 2 state and Capsid (reversibly transforming back to the Intermediate 1 state) are shown to be mainly due to the isotropic pressure that the encapsidated RNA segments exert on the shell walls. The hidden symmetry of the capsid and the physicochemical features of the in vitro genome extraction from the viral shell are also elucidated.\",\"language\":\"en\",\"number\":\"40\",\"urldate\":\"2023-11-11\",\"journal\":\"Soft Matter\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Konevtsova\"],\"firstnames\":[\"Olga\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Roshal\"],\"firstnames\":[\"Daria\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Podgornik\"],\"firstnames\":[\"Rudolf\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergei\",\"B.\"],\"suffixes\":[]}],\"year\":\"2020\",\"pages\":\"9383–9392\",\"bibtex\":\"@article{konevtsova_irreversible_2020,\\n\\ttitle = {Irreversible and reversible morphological changes in the \\\\textit{ϕ} 6 capsid and similar viral shells: symmetry and micromechanics},\\n\\tvolume = {16},\\n\\tissn = {1744-683X, 1744-6848},\\n\\tshorttitle = {Irreversible and reversible morphological changes in the \\\\textit{ϕ} 6 capsid and similar viral shells},\\n\\turl = {http://xlink.rsc.org/?DOI=D0SM01338B},\\n\\tdoi = {10.1039/D0SM01338B},\\n\\tabstract = {We propose a new micromechanical model perfectly describing the capsid shapes and morphological transformations that occur between the states of the dodecahedral\\n              ϕ\\n              6 capsid and similar viral shells due to the sequential packaging of RNA segments.\\n            \\n          , \\n            \\n              Understanding the physicochemical processes occurring in viruses during their maturation is of fundamental importance since only mature viruses can infect host cells. Here we consider the irreversible and reversible morphological changes that occur with the dodecahedral\\n              ϕ\\n              6 procapsid during the sequential packaging of 3 RNA segments forming the viral genome. It is shown that the dodecahedral shape of all the four observed capsid states is perfectly reproduced by a sphere radially deformed by only two irreducible spherical harmonics with icosahedral symmetry and wave numbers\\n              l\\n              = 6 and\\n              l\\n              = 10. The rotation of proteins around the 3-fold axes at the Procapsid → Intermediate 1 irreversible transformation is in fact also well described with the shear field containing only two irreducible harmonics with the same two wave numbers. The high stability of the Intermediate 1 state is discussed and the shapes of the Intermediate 2 state and Capsid (reversibly transforming back to the Intermediate 1 state) are shown to be mainly due to the isotropic pressure that the encapsidated RNA segments exert on the shell walls. The hidden symmetry of the capsid and the physicochemical features of the\\n              in vitro\\n              genome extraction from the viral shell are also elucidated.},\\n\\tlanguage = {en},\\n\\tnumber = {40},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Soft Matter},\\n\\tauthor = {Konevtsova, Olga V. and Roshal, Daria S. and Podgornik, Rudolf and Rochal, Sergei B.},\\n\\tyear = {2020},\\n\\tpages = {9383--9392},\\n}\\n\\n\",\"author_short\":[\"Konevtsova, O. V.\",\"Roshal, D. S.\",\"Podgornik, R.\",\"Rochal, S. B.\"],\"key\":\"konevtsova_irreversible_2020\",\"id\":\"konevtsova_irreversible_2020\",\"bibbaseid\":\"konevtsova-roshal-podgornik-rochal-irreversibleandreversiblemorphologicalchangesintheii6capsidandsimilarviralshellssymmetryandmicromechanics-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://xlink.rsc.org/?DOI=D0SM01338B\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Carbon nanotube sorting due to commensurate molecular wrapping\",\"volume\":\"12\",\"issn\":\"2040-3364, 2040-3372\",\"url\":\"http://xlink.rsc.org/?DOI=D0NR03236K\",\"doi\":\"10.1039/D0NR03236K\",\"abstract\":\"Commensurate wrapping of carbon nanotubes ensures their selection by flavin group molecules. , Single-walled carbon nanotubes (SWCNTs) can be sorted by their structural parameters using organic molecules and polymers: some of which, demonstrating a profound affinity only for specific nanotubes, form dense coatings on them. Here, analyzing well-known examples of flavin group molecules and those of 2,4-dichlorophenoxyacetic acid, we show for the first time that successful formation of the considered coatings depends on the ability of molecules to wrap around the SWCNT in a commensurate way. Commensurability provides a decrease in the free energy of the resulting bilayer system and makes the coating much more stable. Concurrently, it strongly relates the nanotube chiral vector with the geometric characteristics of the adhering molecules, which leads to revealed selection rules. If they are not satisfied, the deposition of molecules does not occur or is insignificant. The proposed theory unambiguously explains known experimental results on the formation of spiral wrappings of SWCNTs by flavin group molecules and points out other organic molecules and polymers suitable for effective CNT sorting.\",\"language\":\"en\",\"number\":\"29\",\"urldate\":\"2023-11-11\",\"journal\":\"Nanoscale\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Konevtsova\"],\"firstnames\":[\"Olga\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Roshal\"],\"firstnames\":[\"Daria\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dmitriev\"],\"firstnames\":[\"Vladimir\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergei\",\"B.\"],\"suffixes\":[]}],\"year\":\"2020\",\"pages\":\"15725–15735\",\"bibtex\":\"@article{konevtsova_carbon_2020,\\n\\ttitle = {Carbon nanotube sorting due to commensurate molecular wrapping},\\n\\tvolume = {12},\\n\\tissn = {2040-3364, 2040-3372},\\n\\turl = {http://xlink.rsc.org/?DOI=D0NR03236K},\\n\\tdoi = {10.1039/D0NR03236K},\\n\\tabstract = {Commensurate wrapping of carbon nanotubes ensures their selection by flavin group molecules.\\n          , \\n            Single-walled carbon nanotubes (SWCNTs) can be sorted by their structural parameters using organic molecules and polymers: some of which, demonstrating a profound affinity only for specific nanotubes, form dense coatings on them. Here, analyzing well-known examples of flavin group molecules and those of 2,4-dichlorophenoxyacetic acid, we show for the first time that successful formation of the considered coatings depends on the ability of molecules to wrap around the SWCNT in a commensurate way. Commensurability provides a decrease in the free energy of the resulting bilayer system and makes the coating much more stable. Concurrently, it strongly relates the nanotube chiral vector with the geometric characteristics of the adhering molecules, which leads to revealed selection rules. If they are not satisfied, the deposition of molecules does not occur or is insignificant. The proposed theory unambiguously explains known experimental results on the formation of spiral wrappings of SWCNTs by flavin group molecules and points out other organic molecules and polymers suitable for effective CNT sorting.},\\n\\tlanguage = {en},\\n\\tnumber = {29},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Nanoscale},\\n\\tauthor = {Konevtsova, Olga V. and Roshal, Daria S. and Dmitriev, Vladimir P. and Rochal, Sergei B.},\\n\\tyear = {2020},\\n\\tpages = {15725--15735},\\n}\\n\\n\",\"author_short\":[\"Konevtsova, O. V.\",\"Roshal, D. S.\",\"Dmitriev, V. P.\",\"Rochal, S. B.\"],\"key\":\"konevtsova_carbon_2020\",\"id\":\"konevtsova_carbon_2020\",\"bibbaseid\":\"konevtsova-roshal-dmitriev-rochal-carbonnanotubesortingduetocommensuratemolecularwrapping-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://xlink.rsc.org/?DOI=D0NR03236K\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Mechanical instabilities of aorta drive blood stem cell production: a live study\",\"volume\":\"77\",\"issn\":\"1420-9071\",\"shorttitle\":\"Mechanical instabilities of aorta drive blood stem cell production\",\"url\":\"https://doi.org/10.1007/s00018-019-03372-2\",\"doi\":\"10.1007/s00018-019-03372-2\",\"abstract\":\"During embryogenesis of all vertebrates, haematopoietic stem/progenitor cells (HSPCs) extrude from the aorta by a complex process named endothelial-to-haematopoietic transition (EHT). HSPCs will then colonize haematopoietic organs allowing haematopoiesis throughout adult life. The mechanism underlying EHT including the role of each aortic endothelial cell (EC) within the global aorta dynamics remains unknown. In the present study, we show for the first time that EHT involves the remodelling of individual cells within a collective migration of ECs which is tightly orchestrated, resulting in HSPCs extrusion in the sub-aortic space without compromising aorta integrity. By performing a cross-disciplinary study which combines high-resolution 4D imaging and theoretical analysis based on the concepts of classical mechanics, we propose that this complex developmental process is dependent on mechanical instabilities of the aorta preparing and facilitating the extrusion of HSPCs.\",\"language\":\"en\",\"number\":\"17\",\"urldate\":\"2023-11-11\",\"journal\":\"Cellular and Molecular Life Sciences\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Poullet\"],\"firstnames\":[\"Nausicaa\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golushko\"],\"firstnames\":[\"Ivan\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorman\"],\"firstnames\":[\"Vladimir\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Travnickova\"],\"firstnames\":[\"Jana\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bureau\"],\"firstnames\":[\"Charlotte\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chalin\"],\"firstnames\":[\"Dmitrii\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergei\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Parmeggiani\"],\"firstnames\":[\"Andrea\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kissa\"],\"firstnames\":[\"Karima\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2020\",\"keywords\":\"4D microscopy, Endothelial-to-haematopoietic transition, Haematopoiesis, Modeling, Zebrafish\",\"pages\":\"3453–3464\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\8C4TEQZS\\\\¶oullet и др. - 2020 - Mechanical instabilities of aorta drive blood stem.pdf:application/pdf;Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\6C7BISAS\\\\¶oullet и др. - 2020 - Mechanical instabilities of aorta drive blood stem.pdf:application/pdf\",\"bibtex\":\"@article{poullet_mechanical_2020,\\n\\ttitle = {Mechanical instabilities of aorta drive blood stem cell production: a live study},\\n\\tvolume = {77},\\n\\tissn = {1420-9071},\\n\\tshorttitle = {Mechanical instabilities of aorta drive blood stem cell production},\\n\\turl = {https://doi.org/10.1007/s00018-019-03372-2},\\n\\tdoi = {10.1007/s00018-019-03372-2},\\n\\tabstract = {During embryogenesis of all vertebrates, haematopoietic stem/progenitor cells (HSPCs) extrude from the aorta by a complex process named endothelial-to-haematopoietic transition (EHT). HSPCs will then colonize haematopoietic organs allowing haematopoiesis throughout adult life. The mechanism underlying EHT including the role of each aortic endothelial cell (EC) within the global aorta dynamics remains unknown. In the present study, we show for the first time that EHT involves the remodelling of individual cells within a collective migration of ECs which is tightly orchestrated, resulting in HSPCs extrusion in the sub-aortic space without compromising aorta integrity. By performing a cross-disciplinary study which combines high-resolution 4D imaging and theoretical analysis based on the concepts of classical mechanics, we propose that this complex developmental process is dependent on mechanical instabilities of the aorta preparing and facilitating the extrusion of HSPCs.},\\n\\tlanguage = {en},\\n\\tnumber = {17},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Cellular and Molecular Life Sciences},\\n\\tauthor = {Poullet, Nausicaa and Golushko, Ivan and Lorman, Vladimir and Travnickova, Jana and Bureau, Charlotte and Chalin, Dmitrii and Rochal, Sergei and Parmeggiani, Andrea and Kissa, Karima},\\n\\tmonth = sep,\\n\\tyear = {2020},\\n\\tkeywords = {4D microscopy, Endothelial-to-haematopoietic transition, Haematopoiesis, Modeling, Zebrafish},\\n\\tpages = {3453--3464},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\8C4TEQZS\\\\\\\\Poullet и др. - 2020 - Mechanical instabilities of aorta drive blood stem.pdf:application/pdf;Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\6C7BISAS\\\\\\\\Poullet и др. - 2020 - Mechanical instabilities of aorta drive blood stem.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Poullet, N.\",\"Golushko, I.\",\"Lorman, V.\",\"Travnickova, J.\",\"Bureau, C.\",\"Chalin, D.\",\"Rochal, S.\",\"Parmeggiani, A.\",\"Kissa, K.\"],\"key\":\"poullet_mechanical_2020\",\"id\":\"poullet_mechanical_2020\",\"bibbaseid\":\"poullet-golushko-lorman-travnickova-bureau-chalin-rochal-parmeggiani-etal-mechanicalinstabilitiesofaortadrivebloodstemcellproductionalivestudy-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1007/s00018-019-03372-2\"},\"keyword\":[\"4D microscopy\",\"Endothelial-to-haematopoietic transition\",\"Haematopoiesis\",\"Modeling\",\"Zebrafish\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Effect of aluminium substitution on low energy electrodynamics of barium-lead M-type hexagonal ferrites\",\"volume\":\"1389\",\"issn\":\"1742-6596\",\"url\":\"https://dx.doi.org/10.1088/1742-6596/1389/1/012044\",\"doi\":\"10.1088/1742-6596/1389/1/012044\",\"abstract\":\"We present the first detailed study of the terahertz-infrared dielectric response of single crystalline lead-substituted M-type barium hexaferrites doped with Al3+. The broadband spectra of complex dielectric permittivity ε*(v)=ε’(v)+iε\\\"(v) of Ba0.8Pb0.2AlxFe12-xO19 with concentrations of the dopant x(Al)=1.2, 3, 3.3 are obtained for two principle polarizations using Fourier-transform infrared spectroscopy and terahertz time-domain spectroscopy in the temperature range from 4 to 300 K and at frequencies from 10 cm−1 up to 8000 cm−1. We observe a rich set of excitations and assign them to the electronic transitions within the ground state 5E of the 4-fold coordinated divalent iron and to phonon resonances. Effect of Al3+ cation substitution on low energy (terahertz) dielectric response and infrared phonon spectra of barium-lead M-type hexaferrites is analysed and discussed.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics: Conference Series\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Ahmed\"],\"firstnames\":[\"Asmaa\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Alyabyeva\"],\"firstnames\":[\"Liudmila\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"Victor\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"Anatoly\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vinnik\"],\"firstnames\":[\"Denis\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"Martin\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"Boris\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2019\",\"note\":\"Publisher: IOP Publishing\",\"pages\":\"012044\",\"file\":\"IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\F2HHUAX3\\\\\\\\Ahmed и др. - 2019 - Effect of aluminium substitution on low energy ele.pdf:application/pdf\",\"bibtex\":\"@article{ahmed_effect_2019,\\n\\ttitle = {Effect of aluminium substitution on low energy electrodynamics of barium-lead {M}-type hexagonal ferrites},\\n\\tvolume = {1389},\\n\\tissn = {1742-6596},\\n\\turl = {https://dx.doi.org/10.1088/1742-6596/1389/1/012044},\\n\\tdoi = {10.1088/1742-6596/1389/1/012044},\\n\\tabstract = {We present the first detailed study of the terahertz-infrared dielectric response of single crystalline lead-substituted M-type barium hexaferrites doped with Al3+. The broadband spectra of complex dielectric permittivity ε*(v)=ε’(v)+iε\\\"(v) of Ba0.8Pb0.2AlxFe12-xO19 with concentrations of the dopant x(Al)=1.2, 3, 3.3 are obtained for two principle polarizations using Fourier-transform infrared spectroscopy and terahertz time-domain spectroscopy in the temperature range from 4 to 300 K and at frequencies from 10 cm−1 up to 8000 cm−1. We observe a rich set of excitations and assign them to the electronic transitions within the ground state 5E of the 4-fold coordinated divalent iron and to phonon resonances. Effect of Al3+ cation substitution on low energy (terahertz) dielectric response and infrared phonon spectra of barium-lead M-type hexaferrites is analysed and discussed.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics: Conference Series},\\n\\tauthor = {Ahmed, Asmaa and Alyabyeva, Liudmila and Torgashev, Victor and Prokhorov, Anatoly S. and Vinnik, Denis and Dressel, Martin and Gorshunov, Boris},\\n\\tmonth = nov,\\n\\tyear = {2019},\\n\\tnote = {Publisher: IOP Publishing},\\n\\tpages = {012044},\\n\\tfile = {IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\F2HHUAX3\\\\\\\\Ahmed и др. - 2019 - Effect of aluminium substitution on low energy ele.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Ahmed, A.\",\"Alyabyeva, L.\",\"Torgashev, V.\",\"Prokhorov, A. S.\",\"Vinnik, D.\",\"Dressel, M.\",\"Gorshunov, B.\"],\"key\":\"ahmed_effect_2019\",\"id\":\"ahmed_effect_2019\",\"bibbaseid\":\"ahmed-alyabyeva-torgashev-prokhorov-vinnik-dressel-gorshunov-effectofaluminiumsubstitutiononlowenergyelectrodynamicsofbariumleadmtypehexagonalferrites-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/1742-6596/1389/1/012044\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Structure, lattice dynamics, properties of bismuth titanate heterostructures\",\"volume\":\"53\",\"issn\":\"0022-3727\",\"url\":\"https://dx.doi.org/10.1088/1361-6463/ab4bf6\",\"doi\":\"10.1088/1361-6463/ab4bf6\",\"abstract\":\"We investigated the epitaxial Bi4Ti3O12 (BTO) thin films with different thicknesses on a (0 0 1) MgO substrate with a Ba0.4Sr0.6TiO3 buffer layer (4 nm). The crystallographic axis [1 0 0] of Bi4Ti3O12 film is rotated on degrees relative to [1 0 0] MgO axis. When the thickness of Bi4Ti3O12 film is less than 40 nm, the unit cell of the film is compressed in the normal to the interface plane direction. In cases of large film thicknesses, the sign of strain changes and correspondingly the unit cell is stretched. Switched spontaneous polarization in the interface plane with 180° domain structure occurs at 10 nm film thickness and increases with a thickness up to 55 C cm−2. Changes in the Raman spectra of the Bi4Ti3O12 films indicates to increase of monoclinic distortion of the film unit cell in comparison with the bulk unit cell. The anisotropy of in-plane dielectric properties and the effect of internal strain on dielectric properties for the Bi4Ti3O12 films are confirmed by the study of the dielectric characteristics of the films.\",\"language\":\"en\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics D: Applied Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Mukhortov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golovko\"],\"firstnames\":[\"Yu\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Anokhin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Stryukov\"],\"firstnames\":[\"D.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Biryukov\"],\"firstnames\":[\"S.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2019\",\"note\":\"Publisher: IOP Publishing\",\"pages\":\"035304\",\"bibtex\":\"@article{mukhortov_structure_2019,\\n\\ttitle = {Structure, lattice dynamics, properties of bismuth titanate heterostructures},\\n\\tvolume = {53},\\n\\tissn = {0022-3727},\\n\\turl = {https://dx.doi.org/10.1088/1361-6463/ab4bf6},\\n\\tdoi = {10.1088/1361-6463/ab4bf6},\\n\\tabstract = {We investigated the epitaxial Bi4Ti3O12 (BTO) thin films with different thicknesses on a (0 0 1) MgO substrate with a Ba0.4Sr0.6TiO3 buffer layer (4 nm). The crystallographic axis [1 0 0] of Bi4Ti3O12 film is rotated on degrees relative to [1 0 0] MgO axis. When the thickness of Bi4Ti3O12 film is less than 40 nm, the unit cell of the film is compressed in the normal to the interface plane direction. In cases of large film thicknesses, the sign of strain changes and correspondingly the unit cell is stretched. Switched spontaneous polarization in the interface plane with 180° domain structure occurs at 10 nm film thickness and increases with a thickness up to 55 C cm−2. Changes in the Raman spectra of the Bi4Ti3O12 films indicates to increase of monoclinic distortion of the film unit cell in comparison with the bulk unit cell. The anisotropy of in-plane dielectric properties and the effect of internal strain on dielectric properties for the Bi4Ti3O12 films are confirmed by the study of the dielectric characteristics of the films.},\\n\\tlanguage = {en},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics D: Applied Physics},\\n\\tauthor = {Mukhortov, V. M. and Golovko, Yu I. and Anokhin, A. S. and Stryukov, D. V. and Biryukov, S. V. and Timoshenko, P. E.},\\n\\tmonth = nov,\\n\\tyear = {2019},\\n\\tnote = {Publisher: IOP Publishing},\\n\\tpages = {035304},\\n}\\n\\n\",\"author_short\":[\"Mukhortov, V. M.\",\"Golovko, Y. I.\",\"Anokhin, A. S.\",\"Stryukov, D. V.\",\"Biryukov, S. V.\",\"Timoshenko, P. E.\"],\"key\":\"mukhortov_structure_2019\",\"id\":\"mukhortov_structure_2019\",\"bibbaseid\":\"mukhortov-golovko-anokhin-stryukov-biryukov-timoshenko-structurelatticedynamicspropertiesofbismuthtitanateheterostructures-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/1361-6463/ab4bf6\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"key\":\"noauthor_notitle_nodate-4\",\"id\":\"noauthor_notitle_nodate-4\",\"bibbaseid\":\"anonymous-\",\"role\":\"\",\"urls\":{},\"metadata\":{\"authorlinks\":{\"moore, a\":\"https://www.cl.cam.ac.uk/~awm22/talks.html\",\"powner, m\":\"https://bibbase.org/show?bib=benjaminthoma.github.io%2Fpubs.bib\",\"bergmann, r\":\"https://bibbase.org/show?bib=www.wi2.uni-trier.de/publications/WI2Publikationen.bib&group0=year&css=www.wi2.uni-trier.de/publications/WI2.css&filter=authors:Bergmann\",\"van harmelen, f\":\"https://www.cs.vu.nl/\",\"figueroa, n\":\"https://nbfigueroa.github.io/\",\"sammak, s\":\"https://shervinsammak.github.io/papers/\",\"patel, n\":\"https://niravatgit.github.io/INSPIRELab/publications.html#publications\",\"kouamé, d\":\"https://bibbase.org/show?bib=https%3A%2F%2Fwww.irit.fr%2F%7EDenis.Kouame%2Fwp-content%2Fuploads%2Fsites%2F16%2F2023%2F07%2Fpubli_dk_Juillet2023.bib&commas=true&msg=embed&noBootstrap=1\",\"grossi, g\":\"https://bibbase.org/show?bib=https://homes.di.unimi.it/grossi/Grossi_Giuliano.bib\",\"alexiev, v\":\"https://rawgit2.com/VladimirAlexiev/my/master/index.html\",\"bethard, s\":\"https://bethard.github.io/publications.html\",\"homburg, t\":\"https://situx.github.io/publications/\",\"banzhaf, w\":\"https://cse.msu.edu/~banzhafw/Publications_new.html\",\"gatica, j\":\"https://bibbase.org/show?bib=www2.uca.es%2Fdept%2Fcmat_qinor%2Fnanomat%2Fpeople%2FGatica.bib&groupby=year\",\"edwards, c\":\"https://people.ucsc.edu/\",\"miyagusuku, r\":\"https://www.real.utsunomiya-u.ac.jp/invmap/\",\"stephens-davidowitz, n\":\"http://www.noahsd.com/\",\"kouam�, d\":\"https://bibbase.org/show?bib=https%3A%2F%2Fwww.irit.fr%2F%7EDenis.Kouame%2Fwp-content%2Fuploads%2Fsites%2F16%2F2020%2F08%2Fpubli_dk_pc.bib&msg=embed\",\"lee, u\":\"https://bibbase.org/show?bib=https://dblp.org/pid/172/3208.bib\",\"sohrabi, s\":\"https://www.cs.toronto.edu/~shirin/\",\"mcintire, e\":\"https://predictiveecology.org/publications.html\",\"mirrazavi salehian, s\":\"https://nbfigueroa.github.io/\",\"monteiro, s\":\"https://sildomar.github.io/publications/\",\"picco, m\":\"https://www.lpthe.jussieu.fr/~picco/pub.html\",\"maranas, c\":\"https://bibbase.org/show?bib=www.maranasgroup.com/pub/maranasgroup.bib\",\"romoli, j\":\"https://jacoporomoli.github.io/Publications/\",\"maizel, a\":\"https://www.cos.uni-heidelberg.de/\",\"iovino, l\":\"https://www.ludovicoiovino.it/\",\"keller, a\":\"https://bibbase.org/show?bib=https://www.ccb.uni-saarland.de/wp-content/uploads/2024/01/references.bib_.txt&folding=1\",\"riviere, b\":\"http://compm.rice.edu/publications/\",\"beyer, a\":\"https://www.klassphil.hu-berlin.de/de/personen/andrea-beyer\",\"bluestein, d\":\"https://www.bme.stonybrook.edu/labs/dbluestein/aaapatient.html\",\"sabattini, l\":\"https://883789326-atari-embeds.googleusercontent.com/embeds/16cb204cf3a9d4d223a0a3fd8b0eec5d/inner-frame-minified.html\"}},\"downloads\":9,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Terahertz frequency selective surfaces using heterostructures based on two-dimensional diffraction grating of single-walled carbon nanotubes\",\"volume\":\"14\",\"issn\":\"1947-5411, 1947-542X\",\"url\":\"https://www.tandfonline.com/doi/full/10.1080/19475411.2022.2148307\",\"doi\":\"10.1080/19475411.2022.2148307\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"International Journal of Smart and Nano Materials\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"Pavel\",\"Evgenjevich\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lerer\"],\"firstnames\":[\"Alexander\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergei\",\"Bernardovich\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2022\",\"keywords\":\"Q1\",\"pages\":\"21–35\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\4F954CZU\\\\\\\\Timoshenko и др. - 2023 - Terahertz frequency selective surfaces using heter.pdf:application/pdf\",\"bibtex\":\"@article{timoshenko_terahertz_2022,\\n\\ttitle = {Terahertz frequency selective surfaces using heterostructures based on two-dimensional diffraction grating of single-walled carbon nanotubes},\\n\\tvolume = {14},\\n\\tissn = {1947-5411, 1947-542X},\\n\\turl = {https://www.tandfonline.com/doi/full/10.1080/19475411.2022.2148307},\\n\\tdoi = {10.1080/19475411.2022.2148307},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {International Journal of Smart and Nano Materials},\\n\\tauthor = {Timoshenko, Pavel Evgenjevich and Lerer, Alexander and Rochal, Sergei Bernardovich},\\n\\tmonth = dec,\\n\\tyear = {2022},\\n\\tkeywords = {Q1},\\n\\tpages = {21--35},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\4F954CZU\\\\\\\\Timoshenko и др. - 2023 - Terahertz frequency selective surfaces using heter.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Timoshenko, P. E.\",\"Lerer, A.\",\"Rochal, S. B.\"],\"key\":\"timoshenko_terahertz_2022\",\"id\":\"timoshenko_terahertz_2022\",\"bibbaseid\":\"timoshenko-lerer-rochal-terahertzfrequencyselectivesurfacesusingheterostructuresbasedontwodimensionaldiffractiongratingofsinglewalledcarbonnanotubes-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.tandfonline.com/doi/full/10.1080/19475411.2022.2148307\"},\"keyword\":[\"Q1\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Vanadium clusters formation in geometrically frustrated spinel oxide AlV$_{\\\\textrm{2}}$O$_{\\\\textrm{4}}$\",\"volume\":\"74\",\"copyright\":\"Copyright (c) 2018 International Union of Crystallography\",\"issn\":\"2052-5206\",\"url\":\"http://scripts.iucr.org/cgi-bin/paper?dq5028\",\"doi\":\"10.1107/S2052520618007242\",\"abstract\":\"The spinel oxide AlV2O4 is a unique material, in which the formation of clusters is accompanied by atomic, charge and orbital ordering and a rhombohedral lattice distortion. In this work a theory of the structural phase transition in AlV2O4 is proposed. This theory is based on the study of the order-parameter symmetry, thermodynamics, electron density distribution, crystal chemistry and mechanisms of formation of the atomic and orbital structures of the rhombohedral phase. It is established that the critical order parameter is transformed according to irreducible representation k9(τ4) (in Kovalev notation) of the Fd \\\\bar\\\\3\\\\m space group. Knowledge of the order-parameter symmetry allows us to show that the derived AlV2O4 rhombohedral structure is a result of displacements of all atom types and the ordering of Al atoms (1:1 order type in tetrahedral spinel sites), V atoms (1:1:6 order type in octahedral sites) and O atoms (1:1:3:3 order type), and the ordering of dxy, dxz and dyz orbitals. Application of the density functional theory showed that V atoms in the Kagomé sublattice formed separate trimers. Also, no sign of metallic bonding between separate vanadium trimers in the heptamer structure was found. The density functional theory study and the crystal chemical analysis of V—O bond lengths allowed us to assume the existence of dimers and trimers as main clusters in the structure of the AlV2O4 rhombohedral modification. The trimer model of the low-symmetry AlV2O4 structure is proposed. Within the Landau theory of phase transitions, typical diagrams of possible phase states are built. It is shown that phase states can be changed as a first-order phase transition close to the second order in the vicinity of tricritical points of the phase diagrams.\",\"language\":\"en\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Acta Crystallographica Section B: Structural Science, Crystal Engineering and Materials\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"M.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Avakyan\"],\"firstnames\":[\"L.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Borlakov\"],\"firstnames\":[\"K.\",\"S.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2018\",\"note\":\"Number: 4 Publisher: International Union of Crystallography\",\"pages\":\"337–353\",\"bibtex\":\"@article{talanov_vanadium_2018,\\n\\ttitle = {Vanadium clusters formation in geometrically frustrated spinel oxide {AlV}$_{\\\\textrm{2}}${O}$_{\\\\textrm{4}}$},\\n\\tvolume = {74},\\n\\tcopyright = {Copyright (c) 2018 International Union of Crystallography},\\n\\tissn = {2052-5206},\\n\\turl = {http://scripts.iucr.org/cgi-bin/paper?dq5028},\\n\\tdoi = {10.1107/S2052520618007242},\\n\\tabstract = {The spinel oxide AlV2O4 is a unique material, in which the formation of clusters is accompanied by atomic, charge and orbital ordering and a rhombohedral lattice distortion. In this work a theory of the structural phase transition in AlV2O4 is proposed. This theory is based on the study of the order-parameter symmetry, thermodynamics, electron density distribution, crystal chemistry and mechanisms of formation of the atomic and orbital structures of the rhombohedral phase. It is established that the critical order parameter is transformed according to irreducible representation k9(τ4) (in Kovalev notation) of the Fd {\\\\textbackslash}bar\\\\{3\\\\}m space group. Knowledge of the order-parameter symmetry allows us to show that the derived AlV2O4 rhombohedral structure is a result of displacements of all atom types and the ordering of Al atoms (1:1 order type in tetrahedral spinel sites), V atoms (1:1:6 order type in octahedral sites) and O atoms (1:1:3:3 order type), and the ordering of dxy, dxz and dyz orbitals. Application of the density functional theory showed that V atoms in the Kagomé sublattice formed separate trimers. Also, no sign of metallic bonding between separate vanadium trimers in the heptamer structure was found. The density functional theory study and the crystal chemical analysis of V—O bond lengths allowed us to assume the existence of dimers and trimers as main clusters in the structure of the AlV2O4 rhombohedral modification. The trimer model of the low-symmetry AlV2O4 structure is proposed. Within the Landau theory of phase transitions, typical diagrams of possible phase states are built. It is shown that phase states can be changed as a first-order phase transition close to the second order in the vicinity of tricritical points of the phase diagrams.},\\n\\tlanguage = {en},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Acta Crystallographica Section B: Structural Science, Crystal Engineering and Materials},\\n\\tauthor = {Talanov, M. V. and Shirokov, V. B. and Avakyan, L. A. and Talanov, V. M. and Borlakov, K. S.},\\n\\tmonth = aug,\\n\\tyear = {2018},\\n\\tnote = {Number: 4\\nPublisher: International Union of Crystallography},\\n\\tpages = {337--353},\\n}\\n\\n\",\"author_short\":[\"Talanov, M. V.\",\"Shirokov, V. B.\",\"Avakyan, L. A.\",\"Talanov, V. M.\",\"Borlakov, K. S.\"],\"key\":\"talanov_vanadium_2018\",\"id\":\"talanov_vanadium_2018\",\"bibbaseid\":\"talanov-shirokov-avakyan-talanov-borlakov-vanadiumclustersformationingeometricallyfrustratedspineloxidealvtextrm2otextrm4-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://scripts.iucr.org/cgi-bin/paper?dq5028\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Valence state of cations in manganites Pr$_{\\\\textrm{1-x}}$Ca$_{\\\\textrm{x}}$MnO$_{\\\\textrm{3}}$ (0.3 ≤ x ≤ 0.5) from X-ray diffraction and X-ray photoelectron spectroscopy\",\"volume\":\"740\",\"issn\":\"0925-8388\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0925838818300021\",\"doi\":\"10.1016/j.jallcom.2018.01.002\",\"abstract\":\"Polycrystalline Pr1-xCaxMnO3 (х = 0.3, 0.35, 04, 0.45, and 0.5) samples are synthesized by solid-state reaction method. Crystal structure of the samples is studied by X-ray diffraction method with Rietveld refinement. Diffraction patterns from all the samples are well indexed within the Pnma space group. It is shown that lattice parameters and unit cell volume decrease monotonically and O−Mn−O angles become closer to the ideal 180⁰ value upon the growth of x. Mn2p, Mn3s, Ca2p, Pr3d, Pr4d, and O1s X-ray photoelectron spectra are measured. Pr3d and Pr4d spectra are calculated in isolated ion approximation with approximate accounting for the charge transfer effect. Elemental compositions of samples are measured by the XPS method; they differ noticeably from the nominal ones. Charge compensation upon heterovalent Pr3+ → Ca2+ substitution is shown to realize via two mechanisms: creation of oxygen vacancies and formation of Mn4+ ions coexisting with Mn3+. Relative Mn4+/Mn3+ abundances are determined via decomposition of Mn2p and Mn3s XPS into contributions from the spectra of tri- and quadrivalent Mn ions. The amount of Mn4+ ions is shown to increase with Ca content x.\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Alloys and Compounds\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kozakov\"],\"firstnames\":[\"A.\",\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kochur\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Trotsenko\"],\"firstnames\":[\"V.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nikolskii\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"B.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2018\",\"keywords\":\"XPS, Manganites, Cations valence state, Elemental composition, Mn/Mn content, PCaMnO (PCMO) ceramics, Vacancies, XRD\",\"pages\":\"132–142\",\"bibtex\":\"@article{kozakov_valence_2018,\\n\\ttitle = {Valence state of cations in manganites {Pr}$_{\\\\textrm{1-x}}${Ca}$_{\\\\textrm{x}}${MnO}$_{\\\\textrm{3}}$ (0.3 ≤ x ≤ 0.5) from {X}-ray diffraction and {X}-ray photoelectron spectroscopy},\\n\\tvolume = {740},\\n\\tissn = {0925-8388},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0925838818300021},\\n\\tdoi = {10.1016/j.jallcom.2018.01.002},\\n\\tabstract = {Polycrystalline Pr1-xCaxMnO3 (х = 0.3, 0.35, 04, 0.45, and 0.5) samples are synthesized by solid-state reaction method. Crystal structure of the samples is studied by X-ray diffraction method with Rietveld refinement. Diffraction patterns from all the samples are well indexed within the Pnma space group. It is shown that lattice parameters and unit cell volume decrease monotonically and O−Mn−O angles become closer to the ideal 180⁰ value upon the growth of x. Mn2p, Mn3s, Ca2p, Pr3d, Pr4d, and O1s X-ray photoelectron spectra are measured. Pr3d and Pr4d spectra are calculated in isolated ion approximation with approximate accounting for the charge transfer effect. Elemental compositions of samples are measured by the XPS method; they differ noticeably from the nominal ones. Charge compensation upon heterovalent Pr3+ → Ca2+ substitution is shown to realize via two mechanisms: creation of oxygen vacancies and formation of Mn4+ ions coexisting with Mn3+. Relative Mn4+/Mn3+ abundances are determined via decomposition of Mn2p and Mn3s XPS into contributions from the spectra of tri- and quadrivalent Mn ions. The amount of Mn4+ ions is shown to increase with Ca content x.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Alloys and Compounds},\\n\\tauthor = {Kozakov, A. T. and Kochur, A. G. and Trotsenko, V. G. and Nikolskii, A. V. and El Marssi, M. and Gorshunov, B. P. and Torgashev, V. I.},\\n\\tmonth = apr,\\n\\tyear = {2018},\\n\\tkeywords = {XPS, Manganites, Cations valence state, Elemental composition, Mn/Mn content, PCaMnO (PCMO) ceramics, Vacancies, XRD},\\n\\tpages = {132--142},\\n}\\n\\n\",\"author_short\":[\"Kozakov, A. T.\",\"Kochur, A. G.\",\"Trotsenko, V. G.\",\"Nikolskii, A. V.\",\"El Marssi, M.\",\"Gorshunov, B. P.\",\"Torgashev, V. I.\"],\"key\":\"kozakov_valence_2018\",\"id\":\"kozakov_valence_2018\",\"bibbaseid\":\"kozakov-kochur-trotsenko-nikolskii-elmarssi-gorshunov-torgashev-valencestateofcationsinmanganitesprtextrm1xcatextrmxmnotextrm303x05fromxraydiffractionandxrayphotoelectronspectroscopy-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0925838818300021\"},\"keyword\":[\"XPS\",\"Manganites\",\"Cations valence state\",\"Elemental composition\",\"Mn/Mn content\",\"PCaMnO (PCMO) ceramics\",\"Vacancies\",\"XRD\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Temperature Behavior of the Rotational Order Parameters in a La$_{\\\\textrm{0.25}}$Ca$_{\\\\textrm{0.75}}$MnO$_{\\\\textrm{3}}$ Solid Solution\",\"volume\":\"82\",\"issn\":\"1934-9432\",\"url\":\"https://doi.org/10.3103/S1062873818030310\",\"doi\":\"10.3103/S1062873818030310\",\"abstract\":\"The behavior of the crystal structure of a La0.25Ca0.75MnO3 solid solution in the temperature range of 80–725 K is studied. It is established that rotational structural distortions predominate during the transition to a charge-ordered state\",\"language\":\"en\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Bulletin of the Russian Academy of Sciences: Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Trotsenko\"],\"firstnames\":[\"V.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bush\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kadyrov\"],\"firstnames\":[\"L.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"B.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2018\",\"pages\":\"335–337\",\"bibtex\":\"@article{trotsenko_temperature_2018,\\n\\ttitle = {Temperature {Behavior} of the {Rotational} {Order} {Parameters} in a {La}$_{\\\\textrm{0.25}}${Ca}$_{\\\\textrm{0.75}}${MnO}$_{\\\\textrm{3}}$ {Solid} {Solution}},\\n\\tvolume = {82},\\n\\tissn = {1934-9432},\\n\\turl = {https://doi.org/10.3103/S1062873818030310},\\n\\tdoi = {10.3103/S1062873818030310},\\n\\tabstract = {The behavior of the crystal structure of a La0.25Ca0.75MnO3 solid solution in the temperature range of 80–725 K is studied. It is established that rotational structural distortions predominate during the transition to a charge-ordered state},\\n\\tlanguage = {en},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Bulletin of the Russian Academy of Sciences: Physics},\\n\\tauthor = {Trotsenko, V. G. and Mikheykin, A. S. and Shirokov, V. B. and Razumnaya, A. G. and Bush, A. A. and Kadyrov, L. S. and El Marssi, M. and Gorshunov, B. P. and Torgashev, V. I.},\\n\\tmonth = mar,\\n\\tyear = {2018},\\n\\tpages = {335--337},\\n}\\n\\n\",\"author_short\":[\"Trotsenko, V. G.\",\"Mikheykin, A. S.\",\"Shirokov, V. B.\",\"Razumnaya, A. G.\",\"Bush, A. A.\",\"Kadyrov, L. S.\",\"El Marssi, M.\",\"Gorshunov, B. P.\",\"Torgashev, V. I.\"],\"key\":\"trotsenko_temperature_2018\",\"id\":\"trotsenko_temperature_2018\",\"bibbaseid\":\"trotsenko-mikheykin-shirokov-razumnaya-bush-kadyrov-elmarssi-gorshunov-etal-temperaturebehavioroftherotationalorderparametersinalatextrm025catextrm075mnotextrm3solidsolution-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.3103/S1062873818030310\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Effect of a magnetic field on the permittivity of 80%La$_{\\\\textrm{0.7}}$Sr$_{\\\\textrm{0.3}}$MnO$_{\\\\textrm{3}}$/20%GeO$_{\\\\textrm{2}}$ composite\",\"volume\":\"60\",\"issn\":\"1090-6460\",\"url\":\"https://doi.org/10.1134/S1063783418010110\",\"doi\":\"10.1134/S1063783418010110\",\"abstract\":\"The dielectric properties of a magnetoresistive conducting two-phase 80%La0.7Sr0.3MnO3/20%GeO2 (wt %) composite have been studied near the percolation threshold in magnetic fields from 0 to 15 kOe at frequencies of the measurement field from 5 kHz to 1 MHz. The samples have inductive impedances; i.e., their permittivities can be considered negative due to a high conductivity in this frequency range. The permittivity increases in magnitude in magnetic field, and the values of the magnetodielectric coefficient reach 23% at room temperature. The reasons for the effect of magnetic field on the dielectric permittivity of samples are discussed.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Physics of the Solid State\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kabirov\"],\"firstnames\":[\"Yu.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gavrilyachenko\"],\"firstnames\":[\"V.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bogatin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sitalo\"],\"firstnames\":[\"E.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yatsenko\"],\"firstnames\":[\"V.\",\"K.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2018\",\"pages\":\"60–63\",\"bibtex\":\"@article{kabirov_effect_2018,\\n\\ttitle = {Effect of a magnetic field on the permittivity of 80\\\\%{La}$_{\\\\textrm{0.7}}${Sr}$_{\\\\textrm{0.3}}${MnO}$_{\\\\textrm{3}}$/20\\\\%{GeO}$_{\\\\textrm{2}}$ composite},\\n\\tvolume = {60},\\n\\tissn = {1090-6460},\\n\\turl = {https://doi.org/10.1134/S1063783418010110},\\n\\tdoi = {10.1134/S1063783418010110},\\n\\tabstract = {The dielectric properties of a magnetoresistive conducting two-phase 80\\\\%La0.7Sr0.3MnO3/20\\\\%GeO2 (wt \\\\%) composite have been studied near the percolation threshold in magnetic fields from 0 to 15 kOe at frequencies of the measurement field from 5 kHz to 1 MHz. The samples have inductive impedances; i.e., their permittivities can be considered negative due to a high conductivity in this frequency range. The permittivity increases in magnitude in magnetic field, and the values of the magnetodielectric coefficient reach 23\\\\% at room temperature. The reasons for the effect of magnetic field on the dielectric permittivity of samples are discussed.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physics of the Solid State},\\n\\tauthor = {Kabirov, Yu. V. and Gavrilyachenko, V. G. and Bogatin, A. S. and Sitalo, E. I. and Yatsenko, V. K.},\\n\\tmonth = jan,\\n\\tyear = {2018},\\n\\tpages = {60--63},\\n}\\n\\n\",\"author_short\":[\"Kabirov, Y. V.\",\"Gavrilyachenko, V. G.\",\"Bogatin, A. S.\",\"Sitalo, E. I.\",\"Yatsenko, V. K.\"],\"key\":\"kabirov_effect_2018\",\"id\":\"kabirov_effect_2018\",\"bibbaseid\":\"kabirov-gavrilyachenko-bogatin-sitalo-yatsenko-effectofamagneticfieldonthepermittivityof80latextrm07srtextrm03mnotextrm320geotextrm2composite-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1063783418010110\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Collective Infrared Excitation in LuB$_{\\\\textrm{12}}$ Cage-Glass\",\"volume\":\"107\",\"issn\":\"1090-6487\",\"url\":\"https://doi.org/10.1134/S0021364018020029\",\"doi\":\"10.1134/S0021364018020029\",\"abstract\":\"By measuring room temperature infrared (40–35000 cm–1) reflectivity of metallic LuB12 single crystals with different isotopic compositions (natB, 10B, 11B), we find that to model the spectrum we had to introduce, additionally to Drude free-carrier component, a broad excitation with unusually large dielectric contribution (Δε = 8000 ± 4000), which is characterized by a non-Lorentzian lineshape. It is suggested that the origin of the excitation is connected with cooperative dynamics of Jahn–Teller active B12 molecules producing quasilocal vibrations (rattling modes) of caged lutetium ions. The coupling of the Lu3+ rattling motions with the charge carriers of conduction band is proposed to be the reason of strongly damped character of the excitation.\",\"language\":\"en\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"JETP Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"B.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"E.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Komandin\"],\"firstnames\":[\"G.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Muratov\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Aleshchenko\"],\"firstnames\":[\"Yu.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Demishev\"],\"firstnames\":[\"S.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shitsevalova\"],\"firstnames\":[\"N.\",\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Filipov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sluchanko\"],\"firstnames\":[\"N.\",\"E.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2018\",\"pages\":\"100–105\",\"bibtex\":\"@article{gorshunov_collective_2018,\\n\\ttitle = {Collective {Infrared} {Excitation} in {LuB}$_{\\\\textrm{12}}$ {Cage}-{Glass}},\\n\\tvolume = {107},\\n\\tissn = {1090-6487},\\n\\turl = {https://doi.org/10.1134/S0021364018020029},\\n\\tdoi = {10.1134/S0021364018020029},\\n\\tabstract = {By measuring room temperature infrared (40–35000 cm–1) reflectivity of metallic LuB12 single crystals with different isotopic compositions (natB, 10B, 11B), we find that to model the spectrum we had to introduce, additionally to Drude free-carrier component, a broad excitation with unusually large dielectric contribution (Δε = 8000 ± 4000), which is characterized by a non-Lorentzian lineshape. It is suggested that the origin of the excitation is connected with cooperative dynamics of Jahn–Teller active B12 molecules producing quasilocal vibrations (rattling modes) of caged lutetium ions. The coupling of the Lu3+ rattling motions with the charge carriers of conduction band is proposed to be the reason of strongly damped character of the excitation.},\\n\\tlanguage = {en},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {JETP Letters},\\n\\tauthor = {Gorshunov, B. P. and Zhukova, E. S. and Komandin, G. A. and Torgashev, V. I. and Muratov, A. V. and Aleshchenko, Yu. A. and Demishev, S. V. and Shitsevalova, N. Yu. and Filipov, V. B. and Sluchanko, N. E.},\\n\\tmonth = jan,\\n\\tyear = {2018},\\n\\tpages = {100--105},\\n}\\n\\n\",\"author_short\":[\"Gorshunov, B. P.\",\"Zhukova, E. S.\",\"Komandin, G. A.\",\"Torgashev, V. I.\",\"Muratov, A. V.\",\"Aleshchenko, Y. A.\",\"Demishev, S. V.\",\"Shitsevalova, N. Y.\",\"Filipov, V. B.\",\"Sluchanko, N. E.\"],\"key\":\"gorshunov_collective_2018\",\"id\":\"gorshunov_collective_2018\",\"bibbaseid\":\"gorshunov-zhukova-komandin-torgashev-muratov-aleshchenko-demishev-shitsevalova-etal-collectiveinfraredexcitationinlubtextrm12cageglass-2018\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S0021364018020029\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"patent\",\"type\":\"patent\",\"title\":\"Пассивный беспроводный датчик ультрафиолетового излучения на поверхностных акустических волнах\",\"url\":\"https://findpatent.ru/patent/261/2613590.html\",\"number\":\"RU 2613590\",\"author\":[{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Кайдашев Евгений Михайлович (RU)\"],\"suffixes\":[]},{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Кайдашев Владимир Евгеньевич (RU)\"],\"suffixes\":[]},{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Карапетьян Геворк Яковлевич (RU)\"],\"suffixes\":[]},{\"firstnames\":[],\"propositions\":[],\"lastnames\":[\"Жилин Денис Анатольевич (RU)\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2017\",\"bibtex\":\"@patent{___ru__2017,\\n\\ttitle = {Пассивный беспроводный датчик ультрафиолетового излучения на поверхностных акустических волнах},\\n\\turl = {https://findpatent.ru/patent/261/2613590.html},\\n\\tnumber = {RU 2613590},\\n\\tauthor = {{Кайдашев Евгений Михайлович (RU)} and {Кайдашев Владимир Евгеньевич (RU)} and {Карапетьян Геворк Яковлевич (RU)} and {Жилин Денис Анатольевич (RU)}},\\n\\tmonth = mar,\\n\\tyear = {2017},\\n}\\n\\n\",\"author_short\":[\"Кайдашев Евгений Михайлович (RU)\",\"Кайдашев Владимир Евгеньевич (RU)\",\"Карапетьян Геворк Яковлевич (RU)\",\"Жилин Денис Анатольевич (RU)\"],\"key\":\"___ru__2017\",\"id\":\"___ru__2017\",\"bibbaseid\":\"ru-ru-ru-ru--2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://findpatent.ru/patent/261/2613590.html\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Polarization Topology at the Nominally Charged Domain Walls in Uniaxial Ferroelectrics\",\"volume\":\"34\",\"issn\":\"0935-9648, 1521-4095\",\"url\":\"https://onlinelibrary.wiley.com/doi/10.1002/adma.202203028\",\"doi\":\"10.1002/adma.202203028\",\"abstract\":\"Abstract Ferroelectric domain walls provide a fertile environment for novel materials physics. If a polarization discontinuity arises, it can drive a redistribution of electronic carriers and changes in band structure, which often result in emergent 2D conductivity. If such a discontinuity is not tolerated, then its amelioration usually involves the formation of complex topological patterns, such as flux‐closure domains, dipolar vortices, skyrmions, merons, or Hopfions. The degrees of freedom required for the development of such patterns, in which dipolar rotation is a hallmark, are readily found in multiaxial ferroelectrics. In uniaxial ferroelectrics, where only two opposite polar orientations are possible, it has been assumed that discontinuities are unavoidable when antiparallel components of polarization meet. This perception has been borne out by the appearance of charged conducting domain walls in systems such as hexagonal manganites and lithium niobate. Here, experimental and theoretical investigations on lead germanate (Pb 5 Ge 3 O 11 ) reveal that polar discontinuities can be obviated at head‐to‐head and tail‐to‐tail domain walls by mutual domain bifurcation along two different axes, creating a characteristic saddle‐point domain wall morphology and associated novel dipolar topology, removing the need for screening charge accumulation and associated conductivity enhancement.\",\"language\":\"en\",\"number\":\"45\",\"urldate\":\"2023-11-11\",\"journal\":\"Advanced Materials\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Tikhonov\"],\"firstnames\":[\"Yurii\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maguire\"],\"firstnames\":[\"Jesi\",\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"McCluskey\"],\"firstnames\":[\"Conor\",\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"McConville\"],\"firstnames\":[\"James\",\"P.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kumar\"],\"firstnames\":[\"Amit\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lu\"],\"firstnames\":[\"Haidong\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Meier\"],\"firstnames\":[\"Dennis\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"Anna\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gregg\"],\"firstnames\":[\"John\",\"Martin\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gruverman\"],\"firstnames\":[\"Alexei\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vinokur\"],\"firstnames\":[\"Valerii\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Luk'yanchuk\"],\"firstnames\":[\"Igor\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2022\",\"pages\":\"2203028\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\2JEF82TV\\\\\\\\Tikhonov и др. - 2022 - Polarization Topology at the Nominally Charged Dom.pdf:application/pdf\",\"bibtex\":\"@article{tikhonov_polarization_2022,\\n\\ttitle = {Polarization {Topology} at the {Nominally} {Charged} {Domain} {Walls} in {Uniaxial} {Ferroelectrics}},\\n\\tvolume = {34},\\n\\tissn = {0935-9648, 1521-4095},\\n\\turl = {https://onlinelibrary.wiley.com/doi/10.1002/adma.202203028},\\n\\tdoi = {10.1002/adma.202203028},\\n\\tabstract = {Abstract\\n            \\n              Ferroelectric domain walls provide a fertile environment for novel materials physics. If a polarization discontinuity arises, it can drive a redistribution of electronic carriers and changes in band structure, which often result in emergent 2D conductivity. If such a discontinuity is not tolerated, then its amelioration usually involves the formation of complex topological patterns, such as flux‐closure domains, dipolar vortices, skyrmions, merons, or Hopfions. The degrees of freedom required for the development of such patterns, in which dipolar rotation is a hallmark, are readily found in multiaxial ferroelectrics. In uniaxial ferroelectrics, where only two opposite polar orientations are possible, it has been assumed that discontinuities are unavoidable when antiparallel components of polarization meet. This perception has been borne out by the appearance of charged conducting domain walls in systems such as hexagonal manganites and lithium niobate. Here, experimental and theoretical investigations on lead germanate (Pb\\n              5\\n              Ge\\n              3\\n              O\\n              11\\n              ) reveal that polar discontinuities can be obviated at head‐to‐head and tail‐to‐tail domain walls by mutual domain bifurcation along two different axes, creating a characteristic saddle‐point domain wall morphology and associated novel dipolar topology, removing the need for screening charge accumulation and associated conductivity enhancement.},\\n\\tlanguage = {en},\\n\\tnumber = {45},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Advanced Materials},\\n\\tauthor = {Tikhonov, Yurii and Maguire, Jesi R. and McCluskey, Conor J. and McConville, James P. V. and Kumar, Amit and Lu, Haidong and Meier, Dennis and Razumnaya, Anna and Gregg, John Martin and Gruverman, Alexei and Vinokur, Valerii M. and Luk'yanchuk, Igor},\\n\\tmonth = nov,\\n\\tyear = {2022},\\n\\tpages = {2203028},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\2JEF82TV\\\\\\\\Tikhonov и др. - 2022 - Polarization Topology at the Nominally Charged Dom.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Tikhonov, Y.\",\"Maguire, J. R.\",\"McCluskey, C. J.\",\"McConville, J. P. V.\",\"Kumar, A.\",\"Lu, H.\",\"Meier, D.\",\"Razumnaya, A.\",\"Gregg, J. M.\",\"Gruverman, A.\",\"Vinokur, V. M.\",\"Luk'yanchuk, I.\"],\"key\":\"tikhonov_polarization_2022\",\"id\":\"tikhonov_polarization_2022\",\"bibbaseid\":\"tikhonov-maguire-mccluskey-mcconville-kumar-lu-meier-razumnaya-etal-polarizationtopologyatthenominallychargeddomainwallsinuniaxialferroelectrics-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://onlinelibrary.wiley.com/doi/10.1002/adma.202203028\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Phase Diagram of a Strained Ferroelectric Nanowire\",\"volume\":\"12\",\"issn\":\"2073-4352\",\"url\":\"https://www.mdpi.com/2073-4352/12/4/453\",\"doi\":\"10.3390/cryst12040453\",\"abstract\":\"Ferroelectric materials manifest unique dielectric, ferroelastic, and piezoelectric properties. A targeted design of ferroelectrics at the nanoscale is not only of fundamental appeal but holds the highest potential for applications. Compared to two-dimensional nanostructures such as thin films and superlattices, one-dimensional ferroelectric nanowires are investigated to a much lesser extent. Here, we reveal a variety of the topological polarization states, particularly the vortex and helical chiral phases, in loaded ferroelectric nanowires, which enable us to complete the strain–temperature phase diagram of the one-dimensional ferroelectrics. These phases are of prime importance for optoelectronics and quantum communication technologies.\",\"language\":\"en\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Crystals\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Pavlenko\"],\"firstnames\":[\"Maksim\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Di\",\"Rino\"],\"firstnames\":[\"Franco\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Boron\"],\"firstnames\":[\"Leo\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kondovych\"],\"firstnames\":[\"Svitlana\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sené\"],\"firstnames\":[\"Anaïs\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tikhonov\"],\"firstnames\":[\"Yuri\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"Anna\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vinokur\"],\"firstnames\":[\"Valerii\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sepliarsky\"],\"firstnames\":[\"Marcelo\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lukyanchuk\"],\"firstnames\":[\"Igor\",\"A.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2022\",\"pages\":\"453\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\9V22JHFK\\\\¶avlenko и др. - 2022 - Phase Diagram of a Strained Ferroelectric Nanowire.pdf:application/pdf;Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\NDRVUCFW\\\\¶avlenko и др. - 2022 - Phase Diagram of a Strained Ferroelectric Nanowire.pdf:application/pdf\",\"bibtex\":\"@article{pavlenko_phase_2022,\\n\\ttitle = {Phase {Diagram} of a {Strained} {Ferroelectric} {Nanowire}},\\n\\tvolume = {12},\\n\\tissn = {2073-4352},\\n\\turl = {https://www.mdpi.com/2073-4352/12/4/453},\\n\\tdoi = {10.3390/cryst12040453},\\n\\tabstract = {Ferroelectric materials manifest unique dielectric, ferroelastic, and piezoelectric properties. A targeted design of ferroelectrics at the nanoscale is not only of fundamental appeal but holds the highest potential for applications. Compared to two-dimensional nanostructures such as thin films and superlattices, one-dimensional ferroelectric nanowires are investigated to a much lesser extent. Here, we reveal a variety of the topological polarization states, particularly the vortex and helical chiral phases, in loaded ferroelectric nanowires, which enable us to complete the strain–temperature phase diagram of the one-dimensional ferroelectrics. These phases are of prime importance for optoelectronics and quantum communication technologies.},\\n\\tlanguage = {en},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Crystals},\\n\\tauthor = {Pavlenko, Maksim A. and Di Rino, Franco and Boron, Leo and Kondovych, Svitlana and Sené, Anaïs and Tikhonov, Yuri A. and Razumnaya, Anna G. and Vinokur, Valerii M. and Sepliarsky, Marcelo and Lukyanchuk, Igor A.},\\n\\tmonth = mar,\\n\\tyear = {2022},\\n\\tpages = {453},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\9V22JHFK\\\\\\\\Pavlenko и др. - 2022 - Phase Diagram of a Strained Ferroelectric Nanowire.pdf:application/pdf;Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\NDRVUCFW\\\\\\\\Pavlenko и др. - 2022 - Phase Diagram of a Strained Ferroelectric Nanowire.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Pavlenko, M. A.\",\"Di Rino, F.\",\"Boron, L.\",\"Kondovych, S.\",\"Sené, A.\",\"Tikhonov, Y. A.\",\"Razumnaya, A. G.\",\"Vinokur, V. M.\",\"Sepliarsky, M.\",\"Lukyanchuk, I. A.\"],\"key\":\"pavlenko_phase_2022\",\"id\":\"pavlenko_phase_2022\",\"bibbaseid\":\"pavlenko-dirino-boron-kondovych-sen-tikhonov-razumnaya-vinokur-etal-phasediagramofastrainedferroelectricnanowire-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.mdpi.com/2073-4352/12/4/453\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Packing and trimer-to-dimer protein reconstruction in icosahedral viral shells with a single type of symmetrical structural unit\",\"volume\":\"4\",\"issn\":\"2516-0230\",\"url\":\"http://xlink.rsc.org/?DOI=D2NA00461E\",\"doi\":\"10.1039/D2NA00461E\",\"abstract\":\"Modelling morphological transformation in Flavivirus proteinaceous shells at maturation. Locally periodic arrangement of pr peptides makes the dimeric state energetically more favorable at a low pH level. , Understanding the principles of protein packing and the mechanisms driving morphological transformations in virus shells (capsids) during their maturation can be pivotal for the development of new antiviral strategies. Here, we study how these principles and mechanisms manifest themselves in icosahedral viral capsids assembled from identical symmetric structural units (capsomeres). To rationalize such shells, we model capsomers as symmetrical groups of identical particles interacting with a short-range potential typical of the classic Tammes problem. The capsomere particles are assumed to retain their relative positions on the vertices of planar polygons placed on the spherical shell and to interact only with the particles from other capsomeres. Minimization of the interaction energy enforces equal distances between the nearest particles belonging to neighboring capsomeres and minimizes the number of different local environments. Thus, our model implements the Caspar and Klug quasi-equivalence principle and leads to packings strikingly similar to real capsids. We then study a reconstruction of protein trimers into dimers in a Flavivirus shell during its maturation, connecting the relevant structural changes with the modifications of the electrostatic charges of proteins, wrought by the oxidative switch in the bathing solution that is essential for the process. We highlight the key role of pr peptides in the shell reconstruction and show that the highly ordered arrangement of these subunits in the dimeric state is energetically favored at a low pH level. We also discuss the electrostatic mechanisms controlling the release of pr peptides in the last irreversible step of the maturation process.\",\"language\":\"en\",\"number\":\"21\",\"urldate\":\"2023-11-11\",\"journal\":\"Nanoscale Advances\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergei\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Konevtsova\"],\"firstnames\":[\"Olga\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Roshal\"],\"firstnames\":[\"Daria\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Božič\"],\"firstnames\":[\"Anže\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golushko\"],\"firstnames\":[\"Ivan\",\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Podgornik\"],\"firstnames\":[\"Rudolf\"],\"suffixes\":[]}],\"year\":\"2022\",\"pages\":\"4677–4688\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\DB8I4DZC\\\\\\\\Rochal и др. - 2022 - Packing and trimer-to-dimer protein reconstruction.pdf:application/pdf;Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\7PKD38HX\\\\\\\\Rochal и др. - 2022 - Packing and trimer-to-dimer protein reconstruction.pdf:application/pdf\",\"bibtex\":\"@article{rochal_packing_2022,\\n\\ttitle = {Packing and trimer-to-dimer protein reconstruction in icosahedral viral shells with a single type of symmetrical structural unit},\\n\\tvolume = {4},\\n\\tissn = {2516-0230},\\n\\turl = {http://xlink.rsc.org/?DOI=D2NA00461E},\\n\\tdoi = {10.1039/D2NA00461E},\\n\\tabstract = {Modelling morphological transformation in\\n              Flavivirus\\n              proteinaceous shells at maturation. Locally periodic arrangement of pr peptides makes the dimeric state energetically more favorable at a low pH level.\\n            \\n          , \\n            \\n              Understanding the principles of protein packing and the mechanisms driving morphological transformations in virus shells (capsids) during their maturation can be pivotal for the development of new antiviral strategies. Here, we study how these principles and mechanisms manifest themselves in icosahedral viral capsids assembled from identical symmetric structural units (capsomeres). To rationalize such shells, we model capsomers as symmetrical groups of identical particles interacting with a short-range potential typical of the classic Tammes problem. The capsomere particles are assumed to retain their relative positions on the vertices of planar polygons placed on the spherical shell and to interact only with the particles from other capsomeres. Minimization of the interaction energy enforces equal distances between the nearest particles belonging to neighboring capsomeres and minimizes the number of different local environments. Thus, our model implements the Caspar and Klug quasi-equivalence principle and leads to packings strikingly similar to real capsids. We then study a reconstruction of protein trimers into dimers in a\\n              Flavivirus\\n              shell during its maturation, connecting the relevant structural changes with the modifications of the electrostatic charges of proteins, wrought by the oxidative switch in the bathing solution that is essential for the process. We highlight the key role of pr peptides in the shell reconstruction and show that the highly ordered arrangement of these subunits in the dimeric state is energetically favored at a low pH level. We also discuss the electrostatic mechanisms controlling the release of pr peptides in the last irreversible step of the maturation process.},\\n\\tlanguage = {en},\\n\\tnumber = {21},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Nanoscale Advances},\\n\\tauthor = {Rochal, Sergei B. and Konevtsova, Olga V. and Roshal, Daria S. and Božič, Anže and Golushko, Ivan Yu. and Podgornik, Rudolf},\\n\\tyear = {2022},\\n\\tpages = {4677--4688},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\DB8I4DZC\\\\\\\\Rochal и др. - 2022 - Packing and trimer-to-dimer protein reconstruction.pdf:application/pdf;Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\7PKD38HX\\\\\\\\Rochal и др. - 2022 - Packing and trimer-to-dimer protein reconstruction.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Rochal, S. B.\",\"Konevtsova, O. V.\",\"Roshal, D. S.\",\"Božič, A.\",\"Golushko, I. Y.\",\"Podgornik, R.\"],\"key\":\"rochal_packing_2022\",\"id\":\"rochal_packing_2022\",\"bibbaseid\":\"rochal-konevtsova-roshal-boi-golushko-podgornik-packingandtrimertodimerproteinreconstructioninicosahedralviralshellswithasingletypeofsymmetricalstructuralunit-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://xlink.rsc.org/?DOI=D2NA00461E\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Thermodynamic theory of Pb$_{\\\\textrm{x}}$Sr$_{\\\\textrm{1-x}}$TiO$_{\\\\textrm{3}}$ solid solutions\",\"volume\":\"161\",\"issn\":\"00223697\",\"url\":\"https://linkinghub.elsevier.com/retrieve/pii/S0022369721004613\",\"doi\":\"10.1016/j.jpcs.2021.110395\",\"language\":\"en\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics and Chemistry of Solids\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"A.S.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2022\",\"pages\":\"110395\",\"bibtex\":\"@article{shirokov_thermodynamic_2022,\\n\\ttitle = {Thermodynamic theory of {Pb}$_{\\\\textrm{x}}${Sr}$_{\\\\textrm{1-x}}${TiO}$_{\\\\textrm{3}}$ solid solutions},\\n\\tvolume = {161},\\n\\tissn = {00223697},\\n\\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0022369721004613},\\n\\tdoi = {10.1016/j.jpcs.2021.110395},\\n\\tlanguage = {en},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics and Chemistry of Solids},\\n\\tauthor = {Shirokov, V.B. and Razumnaya, A.G. and Mikheykin, A.S.},\\n\\tmonth = feb,\\n\\tyear = {2022},\\n\\tpages = {110395},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V.\",\"Razumnaya, A.\",\"Mikheykin, A.\"],\"key\":\"shirokov_thermodynamic_2022\",\"id\":\"shirokov_thermodynamic_2022\",\"bibbaseid\":\"shirokov-razumnaya-mikheykin-thermodynamictheoryofpbtextrmxsrtextrm1xtiotextrm3solidsolutions-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://linkinghub.elsevier.com/retrieve/pii/S0022369721004613\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Study of the structural-phase state and physical properties of (1 − x)(CoFe$_{\\\\textrm{2}}$O$_{\\\\textrm{4}}$) − x(PbTiO$_{\\\\textrm{3}}$) compositions\",\"volume\":\"128\",\"issn\":\"0947-8396, 1432-0630\",\"url\":\"https://link.springer.com/10.1007/s00339-022-05442-y\",\"doi\":\"10.1007/s00339-022-05442-y\",\"language\":\"en\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Applied Physics A\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Abdulvakhidov\"],\"firstnames\":[\"Bashir\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Li\"],\"firstnames\":[\"Zhengyou\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Abdulvakhidov\"],\"firstnames\":[\"Kamaludin\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Soldatov\"],\"firstnames\":[\"Alexander\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nazarenko\"],\"firstnames\":[\"Alexander\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kulbuzhev\"],\"firstnames\":[\"Bashir\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mardasova\"],\"firstnames\":[\"Irina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lyanguzov\"],\"firstnames\":[\"Nikolay\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sitalo\"],\"firstnames\":[\"Evgeniy\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sadykov\"],\"firstnames\":[\"Sadyk\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sirota\"],\"firstnames\":[\"Marina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dmitrenko\"],\"firstnames\":[\"Ivan\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Manukyan\"],\"firstnames\":[\"Aram\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2022\",\"pages\":\"293\",\"bibtex\":\"@article{abdulvakhidov_study_2022,\\n\\ttitle = {Study of the structural-phase state and physical properties of (1 − x)({CoFe}$_{\\\\textrm{2}}${O}$_{\\\\textrm{4}}$) − x({PbTiO}$_{\\\\textrm{3}}$) compositions},\\n\\tvolume = {128},\\n\\tissn = {0947-8396, 1432-0630},\\n\\turl = {https://link.springer.com/10.1007/s00339-022-05442-y},\\n\\tdoi = {10.1007/s00339-022-05442-y},\\n\\tlanguage = {en},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Applied Physics A},\\n\\tauthor = {Abdulvakhidov, Bashir and Li, Zhengyou and Abdulvakhidov, Kamaludin and Soldatov, Alexander and Nazarenko, Alexander and Kulbuzhev, Bashir and Mardasova, Irina and Lyanguzov, Nikolay and Sitalo, Evgeniy and Sadykov, Sadyk and Sirota, Marina and Dmitrenko, Ivan and Manukyan, Aram},\\n\\tmonth = apr,\\n\\tyear = {2022},\\n\\tpages = {293},\\n}\\n\\n\",\"author_short\":[\"Abdulvakhidov, B.\",\"Li, Z.\",\"Abdulvakhidov, K.\",\"Soldatov, A.\",\"Nazarenko, A.\",\"Kulbuzhev, B.\",\"Mardasova, I.\",\"Lyanguzov, N.\",\"Sitalo, E.\",\"Sadykov, S.\",\"Sirota, M.\",\"Dmitrenko, I.\",\"Manukyan, A.\"],\"key\":\"abdulvakhidov_study_2022\",\"id\":\"abdulvakhidov_study_2022\",\"bibbaseid\":\"abdulvakhidov-li-abdulvakhidov-soldatov-nazarenko-kulbuzhev-mardasova-lyanguzov-etal-studyofthestructuralphasestateandphysicalpropertiesof1xcofetextrm2otextrm4xpbtiotextrm3compositions-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.springer.com/10.1007/s00339-022-05442-y\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Enhanced near-ambient temperature energy storage and electrocaloric effect in the lead-free BaTi$_{\\\\textrm{0.89}}$Sn$_{\\\\textrm{0.11}}$O$_{\\\\textrm{3}}$ ceramic synthesized by sol–gel method\",\"volume\":\"33\",\"issn\":\"0957-4522, 1573-482X\",\"url\":\"https://link.springer.com/10.1007/s10854-022-08233-6\",\"doi\":\"10.1007/s10854-022-08233-6\",\"language\":\"en\",\"number\":\"16\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Materials Science: Materials in Electronics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Zahid\"],\"firstnames\":[\"Marwa\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hadouch\"],\"firstnames\":[\"Youness\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Amjoud\"],\"firstnames\":[\"M’barek\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzane\"],\"firstnames\":[\"Daoud\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gouné\"],\"firstnames\":[\"Mohamed\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hoummada\"],\"firstnames\":[\"Khalid\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Alimoussa\"],\"firstnames\":[\"Abdelhadi\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"Anna\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rožič\"],\"firstnames\":[\"Brigita\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kutnjak\"],\"firstnames\":[\"Zdravko\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2022\",\"pages\":\"12900–12911\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\JXG9ZCDZ\\\\\\\\Zahid и др. - 2022 - Enhanced near-ambient temperature energy storage a.pdf:application/pdf;Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\GCABVF4P\\\\\\\\Zahid и др. - 2022 - Enhanced near-ambient temperature energy storage a.pdf:application/pdf\",\"bibtex\":\"@article{zahid_enhanced_2022,\\n\\ttitle = {Enhanced near-ambient temperature energy storage and electrocaloric effect in the lead-free {BaTi}$_{\\\\textrm{0.89}}${Sn}$_{\\\\textrm{0.11}}${O}$_{\\\\textrm{3}}$ ceramic synthesized by sol–gel method},\\n\\tvolume = {33},\\n\\tissn = {0957-4522, 1573-482X},\\n\\turl = {https://link.springer.com/10.1007/s10854-022-08233-6},\\n\\tdoi = {10.1007/s10854-022-08233-6},\\n\\tlanguage = {en},\\n\\tnumber = {16},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Materials Science: Materials in Electronics},\\n\\tauthor = {Zahid, Marwa and Hadouch, Youness and Amjoud, M’barek and Mezzane, Daoud and Gouné, Mohamed and Hoummada, Khalid and Alimoussa, Abdelhadi and Razumnaya, Anna G. and Rožič, Brigita and Kutnjak, Zdravko},\\n\\tmonth = jun,\\n\\tyear = {2022},\\n\\tpages = {12900--12911},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\JXG9ZCDZ\\\\\\\\Zahid и др. - 2022 - Enhanced near-ambient temperature energy storage a.pdf:application/pdf;Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\GCABVF4P\\\\\\\\Zahid и др. - 2022 - Enhanced near-ambient temperature energy storage a.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Zahid, M.\",\"Hadouch, Y.\",\"Amjoud, M.\",\"Mezzane, D.\",\"Gouné, M.\",\"Hoummada, K.\",\"Alimoussa, A.\",\"Razumnaya, A. G.\",\"Rožič, B.\",\"Kutnjak, Z.\"],\"key\":\"zahid_enhanced_2022\",\"id\":\"zahid_enhanced_2022\",\"bibbaseid\":\"zahid-hadouch-amjoud-mezzane-goun-hoummada-alimoussa-razumnaya-etal-enhancednearambienttemperatureenergystorageandelectrocaloriceffectintheleadfreebatitextrm089sntextrm011otextrm3ceramicsynthesizedbysolgelmethod-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.springer.com/10.1007/s10854-022-08233-6\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Enhanced electrocaloric and energy-storage properties of environment-friendly ferroelectric Ba$_{\\\\textrm{0.9}}$Sr$_{\\\\textrm{0.1}}$Ti$_{\\\\textrm{1−x}}$Sn$_{\\\\textrm{x}}$O$_{\\\\textrm{3}}$ ceramics\",\"volume\":\"31\",\"issn\":\"23524928\",\"url\":\"https://linkinghub.elsevier.com/retrieve/pii/S2352492822002227\",\"doi\":\"10.1016/j.mtcomm.2022.103351\",\"language\":\"en\",\"urldate\":\"2023-11-11\",\"journal\":\"Materials Today Communications\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Zaitouni\"],\"firstnames\":[\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hajji\"],\"firstnames\":[\"L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzane\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Choukri\"],\"firstnames\":[\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gagou\"],\"firstnames\":[\"Y.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hoummada\"],\"firstnames\":[\"K.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Alimoussa\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rožič\"],\"firstnames\":[\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Črešnar\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kutnjak\"],\"firstnames\":[\"Z.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2022\",\"pages\":\"103351\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\24PCRTWA\\\\\\\\Zaitouni и др. - 2022 - Enhanced electrocaloric and energy-storage propert.pdf:application/pdf;Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\C3NG5P6W\\\\\\\\Zaitouni и др. - 2022 - Enhanced electrocaloric and energy-storage propert.pdf:application/pdf\",\"bibtex\":\"@article{zaitouni_enhanced_2022,\\n\\ttitle = {Enhanced electrocaloric and energy-storage properties of environment-friendly ferroelectric {Ba}$_{\\\\textrm{0.9}}${Sr}$_{\\\\textrm{0.1}}${Ti}$_{\\\\textrm{1−x}}${Sn}$_{\\\\textrm{x}}${O}$_{\\\\textrm{3}}$ ceramics},\\n\\tvolume = {31},\\n\\tissn = {23524928},\\n\\turl = {https://linkinghub.elsevier.com/retrieve/pii/S2352492822002227},\\n\\tdoi = {10.1016/j.mtcomm.2022.103351},\\n\\tlanguage = {en},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Materials Today Communications},\\n\\tauthor = {Zaitouni, H. and Hajji, L. and Mezzane, D. and Choukri, E. and Razumnaya, A.G. and Gagou, Y. and Hoummada, K. and Alimoussa, A. and Rožič, B. and Črešnar, D. and El Marssi, M. and Kutnjak, Z.},\\n\\tmonth = jun,\\n\\tyear = {2022},\\n\\tpages = {103351},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\24PCRTWA\\\\\\\\Zaitouni и др. - 2022 - Enhanced electrocaloric and energy-storage propert.pdf:application/pdf;Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\C3NG5P6W\\\\\\\\Zaitouni и др. - 2022 - Enhanced electrocaloric and energy-storage propert.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Zaitouni, H.\",\"Hajji, L.\",\"Mezzane, D.\",\"Choukri, E.\",\"Razumnaya, A.\",\"Gagou, Y.\",\"Hoummada, K.\",\"Alimoussa, A.\",\"Rožič, B.\",\"Črešnar, D.\",\"El Marssi, M.\",\"Kutnjak, Z.\"],\"key\":\"zaitouni_enhanced_2022\",\"id\":\"zaitouni_enhanced_2022\",\"bibbaseid\":\"zaitouni-hajji-mezzane-choukri-razumnaya-gagou-hoummada-alimoussa-etal-enhancedelectrocaloricandenergystoragepropertiesofenvironmentfriendlyferroelectricbatextrm09srtextrm01titextrm1xsntextrmxotextrm3ceramics-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://linkinghub.elsevier.com/retrieve/pii/S2352492822002227\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Electrocaloric effect and high energy storage efficiency in lead-free Ba$_{\\\\textrm{0.95}}$Ca$_{\\\\textrm{0.05}}$Ti$_{\\\\textrm{0.89}}$Sn$_{\\\\textrm{0.11}}$O$_{\\\\textrm{3}}$ ceramic elaborated by sol–gel method\",\"volume\":\"33\",\"issn\":\"0957-4522, 1573-482X\",\"url\":\"https://link.springer.com/10.1007/s10854-021-07411-2\",\"doi\":\"10.1007/s10854-021-07411-2\",\"language\":\"en\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Materials Science: Materials in Electronics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Hadouch\"],\"firstnames\":[\"Youness\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ben\",\"Moumen\"],\"firstnames\":[\"Said\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzourh\"],\"firstnames\":[\"Hanane\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzane\"],\"firstnames\":[\"Daoud\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Amjoud\"],\"firstnames\":[\"M’barek\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Asbani\"],\"firstnames\":[\"Bouchra\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"Anna\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gagou\"],\"firstnames\":[\"Yaovi\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rožič\"],\"firstnames\":[\"Brigita\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kutnjak\"],\"firstnames\":[\"Zdravko\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"Mimoun\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2022\",\"pages\":\"2067–2079\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\3DEEINNF\\\\a̋douch и др. - 2022 - Electrocaloric effect and high energy storage effi.pdf:application/pdf;Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\ECS5QNNK\\\\a̋douch и др. - 2022 - Electrocaloric effect and high energy storage effi.pdf:application/pdf\",\"bibtex\":\"@article{hadouch_electrocaloric_2022,\\n\\ttitle = {Electrocaloric effect and high energy storage efficiency in lead-free {Ba}$_{\\\\textrm{0.95}}${Ca}$_{\\\\textrm{0.05}}${Ti}$_{\\\\textrm{0.89}}${Sn}$_{\\\\textrm{0.11}}${O}$_{\\\\textrm{3}}$ ceramic elaborated by sol–gel method},\\n\\tvolume = {33},\\n\\tissn = {0957-4522, 1573-482X},\\n\\turl = {https://link.springer.com/10.1007/s10854-021-07411-2},\\n\\tdoi = {10.1007/s10854-021-07411-2},\\n\\tlanguage = {en},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Materials Science: Materials in Electronics},\\n\\tauthor = {Hadouch, Youness and Ben Moumen, Said and Mezzourh, Hanane and Mezzane, Daoud and Amjoud, M’barek and Asbani, Bouchra and Razumnaya, Anna G. and Gagou, Yaovi and Rožič, Brigita and Kutnjak, Zdravko and El Marssi, Mimoun},\\n\\tmonth = feb,\\n\\tyear = {2022},\\n\\tpages = {2067--2079},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\3DEEINNF\\\\\\\\Hadouch и др. - 2022 - Electrocaloric effect and high energy storage effi.pdf:application/pdf;Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\ECS5QNNK\\\\\\\\Hadouch и др. - 2022 - Electrocaloric effect and high energy storage effi.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Hadouch, Y.\",\"Ben Moumen, S.\",\"Mezzourh, H.\",\"Mezzane, D.\",\"Amjoud, M.\",\"Asbani, B.\",\"Razumnaya, A. G.\",\"Gagou, Y.\",\"Rožič, B.\",\"Kutnjak, Z.\",\"El Marssi, M.\"],\"key\":\"hadouch_electrocaloric_2022\",\"id\":\"hadouch_electrocaloric_2022\",\"bibbaseid\":\"hadouch-benmoumen-mezzourh-mezzane-amjoud-asbani-razumnaya-gagou-etal-electrocaloriceffectandhighenergystorageefficiencyinleadfreebatextrm095catextrm005titextrm089sntextrm011otextrm3ceramicelaboratedbysolgelmethod-2022\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.springer.com/10.1007/s10854-021-07411-2\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Raman Response of Quantum Critical Ferroelectric Pb-Doped SrTiO$_{\\\\textrm{3}}$\",\"volume\":\"11\",\"issn\":\"2073-4352\",\"url\":\"https://www.mdpi.com/2073-4352/11/12/1469\",\"doi\":\"10.3390/cryst11121469\",\"abstract\":\"A quantum paraelectric SrTiO3 is a material situated in close proximity to a quantum critical point (QCP) of ferroelectric transition in which the critical temperature to the ferroelectric state is suppressed down to 0 K. However, the understanding of the behavior of the phase transition in the vicinity of this point remains challenging. Using the concentration x of Pb in solid solution Sr1−xPbxTiO3 (PSTx) as a tuning parameter and applying the combination of Raman and dielectric spectroscopy methods, we approach the QCP in PSTx and study the interplay of classical and quantum phenomena in the region of criticality. We obtain the critical temperature of PSTx and the evolution of the temperature-dependent dynamical properties of the system as a function of x to reveal the mechanism of the transition. We show that the ferroelectric transition occurs gradually through the emergence of the polar nanoregions inside the non-polar tetragonal phase with their further expansion on cooling. We also study the ferroelastic cubic-to-tetragonal structural transition, occurring at higher temperatures, and show that its properties are almost concentration-independent and not affected by the quantum criticality.\",\"language\":\"en\",\"number\":\"12\",\"urldate\":\"2023-11-10\",\"journal\":\"Crystals\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Linnik\"],\"firstnames\":[\"Ekaterina\",\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"Alexey\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rubi\"],\"firstnames\":[\"Diego\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"Vladimir\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzane\"],\"firstnames\":[\"Daoud\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kondovych\"],\"firstnames\":[\"Svitlana\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lukyanchuk\"],\"firstnames\":[\"Igor\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"Anna\",\"G.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2021\",\"pages\":\"1469\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\DT8BPF4T\\\\Łinnik и др. - 2021 - Raman Response of Quantum Critical Ferroelectric P.pdf:application/pdf\",\"bibtex\":\"@article{linnik_raman_2021,\\n\\ttitle = {Raman {Response} of {Quantum} {Critical} {Ferroelectric} {Pb}-{Doped} {SrTiO}$_{\\\\textrm{3}}$},\\n\\tvolume = {11},\\n\\tissn = {2073-4352},\\n\\turl = {https://www.mdpi.com/2073-4352/11/12/1469},\\n\\tdoi = {10.3390/cryst11121469},\\n\\tabstract = {A quantum paraelectric SrTiO3 is a material situated in close proximity to a quantum critical point (QCP) of ferroelectric transition in which the critical temperature to the ferroelectric state is suppressed down to 0 K. However, the understanding of the behavior of the phase transition in the vicinity of this point remains challenging. Using the concentration x of Pb in solid solution Sr1−xPbxTiO3 (PSTx) as a tuning parameter and applying the combination of Raman and dielectric spectroscopy methods, we approach the QCP in PSTx and study the interplay of classical and quantum phenomena in the region of criticality. We obtain the critical temperature of PSTx and the evolution of the temperature-dependent dynamical properties of the system as a function of x to reveal the mechanism of the transition. We show that the ferroelectric transition occurs gradually through the emergence of the polar nanoregions inside the non-polar tetragonal phase with their further expansion on cooling. We also study the ferroelastic cubic-to-tetragonal structural transition, occurring at higher temperatures, and show that its properties are almost concentration-independent and not affected by the quantum criticality.},\\n\\tlanguage = {en},\\n\\tnumber = {12},\\n\\turldate = {2023-11-10},\\n\\tjournal = {Crystals},\\n\\tauthor = {Linnik, Ekaterina D. and Mikheykin, Alexey S. and Rubi, Diego and Shirokov, Vladimir B. and Mezzane, Daoud and Kondovych, Svitlana V. and Lukyanchuk, Igor A. and Razumnaya, Anna G.},\\n\\tmonth = nov,\\n\\tyear = {2021},\\n\\tpages = {1469},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\DT8BPF4T\\\\\\\\Linnik и др. - 2021 - Raman Response of Quantum Critical Ferroelectric P.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Linnik, E. D.\",\"Mikheykin, A. S.\",\"Rubi, D.\",\"Shirokov, V. B.\",\"Mezzane, D.\",\"Kondovych, S. V.\",\"Lukyanchuk, I. A.\",\"Razumnaya, A. G.\"],\"key\":\"linnik_raman_2021\",\"id\":\"linnik_raman_2021\",\"bibbaseid\":\"linnik-mikheykin-rubi-shirokov-mezzane-kondovych-lukyanchuk-razumnaya-ramanresponseofquantumcriticalferroelectricpbdopedsrtiotextrm3-2021\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.mdpi.com/2073-4352/11/12/1469\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Structural features of the A$_{\\\\textrm{2}}$TiSi$_{\\\\textrm{2}}$O$_{\\\\textrm{8}}$ ( <i>A</i> -Ba and Pb) compounds\",\"volume\":\"10\",\"issn\":\"2010-135X, 2010-1368\",\"url\":\"https://www.worldscientific.com/doi/abs/10.1142/S2010135X20500228\",\"doi\":\"10.1142/S2010135X20500228\",\"abstract\":\"X-ray diffraction studies of synthesized Ba 2 TiSi 2 O 8 have shown that this compound has a fresnoite structure and is characterized by a polar phase [Formula: see text]4bm at room temperature. The synthesis of Pb 2 TiSi 2 O 8 in the fresnoite phase under the selected synthesis conditions has led to the formation of a perovskite tetragonal phase [Formula: see text]4mm corresponding to PbTiO 3 .\",\"language\":\"en\",\"number\":\"05\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Advanced Dielectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Weber\"],\"firstnames\":[\"Svetlana\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lebedinskaya\"],\"firstnames\":[\"Alla\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudsky\"],\"firstnames\":[\"Daniil\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kabirov\"],\"firstnames\":[\"Yuri\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudskaya\"],\"firstnames\":[\"Anzhela\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kupriyanov\"],\"firstnames\":[\"Michael\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2020\",\"pages\":\"2050022\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\CQ956RAJ\\\\\\\\Weber и др. - 2020 - Structural features of the A2TiSi2O8 ( A -B.pdf:application/pdf\",\"bibtex\":\"@article{weber_structural_2020,\\n\\ttitle = {Structural features of the {A}$_{\\\\textrm{2}}${TiSi}$_{\\\\textrm{2}}${O}$_{\\\\textrm{8}}$ ( \\\\textit{{A}} -{Ba} and {Pb}) compounds},\\n\\tvolume = {10},\\n\\tissn = {2010-135X, 2010-1368},\\n\\turl = {https://www.worldscientific.com/doi/abs/10.1142/S2010135X20500228},\\n\\tdoi = {10.1142/S2010135X20500228},\\n\\tabstract = {X-ray diffraction studies of synthesized Ba\\n              2\\n              TiSi\\n              2\\n              O\\n              8\\n              have shown that this compound has a fresnoite structure and is characterized by a polar phase [Formula: see text]4bm at room temperature. The synthesis of Pb\\n              2\\n              TiSi\\n              2\\n              O\\n              8\\n              in the fresnoite phase under the selected synthesis conditions has led to the formation of a perovskite tetragonal phase [Formula: see text]4mm corresponding to PbTiO\\n              3\\n              .},\\n\\tlanguage = {en},\\n\\tnumber = {05},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Advanced Dielectrics},\\n\\tauthor = {Weber, Svetlana and Lebedinskaya, Alla and Rudsky, Daniil and Kabirov, Yuri and Rudskaya, Anzhela and Kupriyanov, Michael},\\n\\tmonth = oct,\\n\\tyear = {2020},\\n\\tpages = {2050022},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\CQ956RAJ\\\\\\\\Weber и др. - 2020 - Structural features of the A2TiSi2O8 ( A -B.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Weber, S.\",\"Lebedinskaya, A.\",\"Rudsky, D.\",\"Kabirov, Y.\",\"Rudskaya, A.\",\"Kupriyanov, M.\"],\"key\":\"weber_structural_2020\",\"id\":\"weber_structural_2020\",\"bibbaseid\":\"weber-lebedinskaya-rudsky-kabirov-rudskaya-kupriyanov-structuralfeaturesoftheatextrm2tisitextrm2otextrm8iaibaandpbcompounds-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.worldscientific.com/doi/abs/10.1142/S2010135X20500228\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Soft modes behavior in bilayer (Ba,Sr)TiO$_{\\\\textrm{3}}$ /(Ba,Sr)TiO$_{\\\\textrm{3}}$ heterostructures\",\"volume\":\"567\",\"issn\":\"0015-0193, 1563-5112\",\"url\":\"https://www.tandfonline.com/doi/full/10.1080/00150193.2020.1791593\",\"doi\":\"10.1080/00150193.2020.1791593\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2020\",\"pages\":\"102–112\",\"bibtex\":\"@article{shirokov_soft_2020,\\n\\ttitle = {Soft modes behavior in bilayer ({Ba},{Sr}){TiO}$_{\\\\textrm{3}}$ /({Ba},{Sr}){TiO}$_{\\\\textrm{3}}$ heterostructures},\\n\\tvolume = {567},\\n\\tissn = {0015-0193, 1563-5112},\\n\\turl = {https://www.tandfonline.com/doi/full/10.1080/00150193.2020.1791593},\\n\\tdoi = {10.1080/00150193.2020.1791593},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Shirokov, V. B. and Razumnaya, A. G.},\\n\\tmonth = oct,\\n\\tyear = {2020},\\n\\tpages = {102--112},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Razumnaya, A. G.\"],\"key\":\"shirokov_soft_2020\",\"id\":\"shirokov_soft_2020\",\"bibbaseid\":\"shirokov-razumnaya-softmodesbehaviorinbilayerbasrtiotextrm3basrtiotextrm3heterostructures-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.tandfonline.com/doi/full/10.1080/00150193.2020.1791593\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"High energy storage efficiency and large electrocaloric effect in lead-free BaTi$_{\\\\textrm{0.89}}$Sn$_{\\\\textrm{0.11}}$O$_{\\\\textrm{3}}$ ceramic\",\"volume\":\"46\",\"issn\":\"02728842\",\"url\":\"https://linkinghub.elsevier.com/retrieve/pii/S027288422031823X\",\"doi\":\"10.1016/j.ceramint.2020.06.163\",\"language\":\"en\",\"number\":\"15\",\"urldate\":\"2023-11-11\",\"journal\":\"Ceramics International\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Merselmiz\"],\"firstnames\":[\"Soukaina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hanani\"],\"firstnames\":[\"Zouhair\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzane\"],\"firstnames\":[\"Daoud\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Spreitzer\"],\"firstnames\":[\"Matjaž\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bradeško\"],\"firstnames\":[\"Andraž\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fabijan\"],\"firstnames\":[\"David\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vengust\"],\"firstnames\":[\"Damjan\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Amjoud\"],\"firstnames\":[\"M’Barek\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hajji\"],\"firstnames\":[\"Lahoucine\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Abkhar\"],\"firstnames\":[\"Zahra\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"Anna\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rožič\"],\"firstnames\":[\"Brigita\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Luk'yanchuk\"],\"firstnames\":[\"Igor\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kutnjak\"],\"firstnames\":[\"Zdravko\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2020\",\"pages\":\"23867–23876\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\K8VED7CU\\\\\\\\Merselmiz и др. - 2020 - High energy storage efficiency and large electroca.pdf:application/pdf\",\"bibtex\":\"@article{merselmiz_high_2020,\\n\\ttitle = {High energy storage efficiency and large electrocaloric effect in lead-free {BaTi}$_{\\\\textrm{0.89}}${Sn}$_{\\\\textrm{0.11}}${O}$_{\\\\textrm{3}}$ ceramic},\\n\\tvolume = {46},\\n\\tissn = {02728842},\\n\\turl = {https://linkinghub.elsevier.com/retrieve/pii/S027288422031823X},\\n\\tdoi = {10.1016/j.ceramint.2020.06.163},\\n\\tlanguage = {en},\\n\\tnumber = {15},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ceramics International},\\n\\tauthor = {Merselmiz, Soukaina and Hanani, Zouhair and Mezzane, Daoud and Spreitzer, Matjaž and Bradeško, Andraž and Fabijan, David and Vengust, Damjan and Amjoud, M’Barek and Hajji, Lahoucine and Abkhar, Zahra and Razumnaya, Anna G. and Rožič, Brigita and Luk'yanchuk, Igor A. and Kutnjak, Zdravko},\\n\\tmonth = oct,\\n\\tyear = {2020},\\n\\tpages = {23867--23876},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\K8VED7CU\\\\\\\\Merselmiz и др. - 2020 - High energy storage efficiency and large electroca.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Merselmiz, S.\",\"Hanani, Z.\",\"Mezzane, D.\",\"Spreitzer, M.\",\"Bradeško, A.\",\"Fabijan, D.\",\"Vengust, D.\",\"Amjoud, M.\",\"Hajji, L.\",\"Abkhar, Z.\",\"Razumnaya, A. G.\",\"Rožič, B.\",\"Luk'yanchuk, I. A.\",\"Kutnjak, Z.\"],\"key\":\"merselmiz_high_2020\",\"id\":\"merselmiz_high_2020\",\"bibbaseid\":\"merselmiz-hanani-mezzane-spreitzer-bradeko-fabijan-vengust-amjoud-etal-highenergystorageefficiencyandlargeelectrocaloriceffectinleadfreebatitextrm089sntextrm011otextrm3ceramic-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://linkinghub.elsevier.com/retrieve/pii/S027288422031823X\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Built-in electric field induces polarization rotation in bilayer BiFeO$_{\\\\textrm{3}}$/(Ba,Sr)TiO$_{\\\\textrm{3}}$ thin films\",\"volume\":\"812\",\"issn\":\"09258388\",\"url\":\"https://linkinghub.elsevier.com/retrieve/pii/S0925838819334103\",\"doi\":\"10.1016/j.jallcom.2019.152164\",\"language\":\"en\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Alloys and Compounds\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"A.S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Stryukov\"],\"firstnames\":[\"D.V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Anokhin\"],\"firstnames\":[\"A.S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pavlenko\"],\"firstnames\":[\"A.V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaliteevski\"],\"firstnames\":[\"M.A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzane\"],\"firstnames\":[\"D.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lukyanchuk\"],\"firstnames\":[\"I.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2020\",\"pages\":\"152164\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\5XSCX5X3\\\\\\\\Razumnaya и др. - 2020 - Built-in electric field induces polarization rotat.pdf:application/pdf\",\"bibtex\":\"@article{razumnaya_built-electric_2020,\\n\\ttitle = {Built-in electric field induces polarization rotation in bilayer {BiFeO}$_{\\\\textrm{3}}$/({Ba},{Sr}){TiO}$_{\\\\textrm{3}}$ thin films},\\n\\tvolume = {812},\\n\\tissn = {09258388},\\n\\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0925838819334103},\\n\\tdoi = {10.1016/j.jallcom.2019.152164},\\n\\tlanguage = {en},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Alloys and Compounds},\\n\\tauthor = {Razumnaya, A.G. and Mikheykin, A.S. and Stryukov, D.V. and Anokhin, A.S. and Pavlenko, A.V. and Shirokov, V.B. and Kaliteevski, M.A. and Mezzane, D. and Lukyanchuk, I.},\\n\\tmonth = jan,\\n\\tyear = {2020},\\n\\tpages = {152164},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\5XSCX5X3\\\\\\\\Razumnaya и др. - 2020 - Built-in electric field induces polarization rotat.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Razumnaya, A.\",\"Mikheykin, A.\",\"Stryukov, D.\",\"Anokhin, A.\",\"Pavlenko, A.\",\"Shirokov, V.\",\"Kaliteevski, M.\",\"Mezzane, D.\",\"Lukyanchuk, I.\"],\"key\":\"razumnaya_built-electric_2020\",\"id\":\"razumnaya_built-electric_2020\",\"bibbaseid\":\"razumnaya-mikheykin-stryukov-anokhin-pavlenko-shirokov-kaliteevski-mezzane-etal-builtinelectricfieldinducespolarizationrotationinbilayerbifeotextrm3basrtiotextrm3thinfilms-2020\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://linkinghub.elsevier.com/retrieve/pii/S0925838819334103\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Terahertz-infrared spectroscopy of single crystalline m-type hexaferrite BaTi$_{\\\\textrm{x}}$Fe$_{\\\\textrm{12-x}}$O$_{\\\\textrm{19}}$\",\"volume\":\"1389\",\"issn\":\"1742-6596\",\"url\":\"https://dx.doi.org/10.1088/1742-6596/1389/1/012038\",\"doi\":\"10.1088/1742-6596/1389/1/012038\",\"abstract\":\"We have studied polarization-dependent broad-band dielectric response of single-crystalline Ti-substituted barium hexaferrites BaTixFe12-xO19, x=0.64., 0.75, 1.1, in the frequency range from 10 to 8000 cm−1 and at temperatures from 5 to 300 K. In addition to a rich set of phonon resonances located at frequencies from 90 to 800 cm−1 we observed an unusual low-energy response (terahertz region, 10-100 cm−1) stemming from two different effects: relaxational process and second order spin-orbit coupling in Fe2+ ground state, that may set up new prospects for doped hexaferrites in terahertz technologies.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics: Conference Series\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Yegiyan\"],\"firstnames\":[\"S.\",\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Alyabyeva\"],\"firstnames\":[\"L.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vinnik\"],\"firstnames\":[\"D.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gudkova\"],\"firstnames\":[\"S.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"B.\",\"P.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2019\",\"note\":\"Publisher: IOP Publishing\",\"pages\":\"012038\",\"file\":\"IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\UWP6ZQD3\\\\\\\\Yegiyan и др. - 2019 - Terahertz-infrared spectroscopy of single crystall.pdf:application/pdf\",\"bibtex\":\"@article{yegiyan_terahertz-infrared_2019,\\n\\ttitle = {Terahertz-infrared spectroscopy of single crystalline m-type hexaferrite {BaTi}$_{\\\\textrm{x}}${Fe}$_{\\\\textrm{12-x}}${O}$_{\\\\textrm{19}}$},\\n\\tvolume = {1389},\\n\\tissn = {1742-6596},\\n\\turl = {https://dx.doi.org/10.1088/1742-6596/1389/1/012038},\\n\\tdoi = {10.1088/1742-6596/1389/1/012038},\\n\\tabstract = {We have studied polarization-dependent broad-band dielectric response of single-crystalline Ti-substituted barium hexaferrites BaTixFe12-xO19, x=0.64., 0.75, 1.1, in the frequency range from 10 to 8000 cm−1 and at temperatures from 5 to 300 K. In addition to a rich set of phonon resonances located at frequencies from 90 to 800 cm−1 we observed an unusual low-energy response (terahertz region, 10-100 cm−1) stemming from two different effects: relaxational process and second order spin-orbit coupling in Fe2+ ground state, that may set up new prospects for doped hexaferrites in terahertz technologies.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics: Conference Series},\\n\\tauthor = {Yegiyan, S. R. and Alyabyeva, L. N. and Torgashev, V. I. and Vinnik, D. A. and Gudkova, S. A. and Prokhorov, A. S. and Dressel, M. and Gorshunov, B. P.},\\n\\tmonth = nov,\\n\\tyear = {2019},\\n\\tnote = {Publisher: IOP Publishing},\\n\\tpages = {012038},\\n\\tfile = {IOP Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\UWP6ZQD3\\\\\\\\Yegiyan и др. - 2019 - Terahertz-infrared spectroscopy of single crystall.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Yegiyan, S. R.\",\"Alyabyeva, L. N.\",\"Torgashev, V. I.\",\"Vinnik, D. A.\",\"Gudkova, S. A.\",\"Prokhorov, A. S.\",\"Dressel, M.\",\"Gorshunov, B. P.\"],\"key\":\"yegiyan_terahertz-infrared_2019\",\"id\":\"yegiyan_terahertz-infrared_2019\",\"bibbaseid\":\"yegiyan-alyabyeva-torgashev-vinnik-gudkova-prokhorov-dressel-gorshunov-terahertzinfraredspectroscopyofsinglecrystallinemtypehexaferritebatitextrmxfetextrm12xotextrm19-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1088/1742-6596/1389/1/012038\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Structure, microstructure, dielectric and piezoelectric properties of (1-x-y)BiFeO$_{\\\\textrm{3}}$-xPbFe$_{\\\\textrm{0.5}}$Nb$_{\\\\textrm{0.5}}$O$_{\\\\textrm{3}}$-yPbTiO$_{\\\\textrm{3}}$ ceramics\",\"volume\":\"45\",\"issn\":\"0272-8842\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0272884219310296\",\"doi\":\"10.1016/j.ceramint.2019.04.204\",\"abstract\":\"Ceramics of seven quasi-binary concentration sections of the ternary solid solution system (1-x-y)BiFeO3-xPbFe0.5Nb0.5O3-yPbTiO3 were prepared by the conventional solid-phase reaction method in the range of 0.05 ≤ x ≤ 0.325; 0.05 ≤ y ≤ 0.325. By using x-ray diffraction technique, the phase diagram of the system was constructed which was shown to contain the regions of tetragonal and rhombohedral symmetry and the morphotropic phase boundary between them. Grain morphology, dielectric and piezoelectric properties of selected solid solutions were investigated. The highest piezoelectric coefficient d33 = 50 pC/N was obtained. Dielectric characteristics of ceramics revealed ferroelectric relaxor behavior and region of diffuse phase transition from the paraelectric to ferroelectric phase in the temperature range of 600–800 K.\",\"number\":\"12\",\"urldate\":\"2023-11-11\",\"journal\":\"Ceramics International\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Boldyrev\"],\"firstnames\":[\"N.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pavlenko\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shilkina\"],\"firstnames\":[\"L.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nazarenko\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bokov\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Reznichenko\"],\"firstnames\":[\"L.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudskaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Panchenko\"],\"firstnames\":[\"E.\",\"I.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2019\",\"keywords\":\"Dielectric properties, Perovskites multiferroics, Piezoelectric properties, Solid solutions\",\"pages\":\"14768–14774\",\"file\":\"ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\FR6CF252\\\\§0272884219310296.html:text/html\",\"bibtex\":\"@article{boldyrev_structure_2019,\\n\\ttitle = {Structure, microstructure, dielectric and piezoelectric properties of (1-x-y){BiFeO}$_{\\\\textrm{3}}$-{xPbFe}$_{\\\\textrm{0.5}}${Nb}$_{\\\\textrm{0.5}}${O}$_{\\\\textrm{3}}$-{yPbTiO}$_{\\\\textrm{3}}$ ceramics},\\n\\tvolume = {45},\\n\\tissn = {0272-8842},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0272884219310296},\\n\\tdoi = {10.1016/j.ceramint.2019.04.204},\\n\\tabstract = {Ceramics of seven quasi-binary concentration sections of the ternary solid solution system (1-x-y)BiFeO3-xPbFe0.5Nb0.5O3-yPbTiO3 were prepared by the conventional solid-phase reaction method in the range of 0.05 ≤ x ≤ 0.325; 0.05 ≤ y ≤ 0.325. By using x-ray diffraction technique, the phase diagram of the system was constructed which was shown to contain the regions of tetragonal and rhombohedral symmetry and the morphotropic phase boundary between them. Grain morphology, dielectric and piezoelectric properties of selected solid solutions were investigated. The highest piezoelectric coefficient d33 = 50 pC/N was obtained. Dielectric characteristics of ceramics revealed ferroelectric relaxor behavior and region of diffuse phase transition from the paraelectric to ferroelectric phase in the temperature range of 600–800 K.},\\n\\tnumber = {12},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ceramics International},\\n\\tauthor = {Boldyrev, N. A. and Pavlenko, A. V. and Shilkina, L. A. and Nazarenko, A. V. and Bokov, A. A. and Reznichenko, L. A. and Rudskaya, A. G. and Panchenko, E. I.},\\n\\tmonth = aug,\\n\\tyear = {2019},\\n\\tkeywords = {Dielectric properties, Perovskites multiferroics, Piezoelectric properties, Solid solutions},\\n\\tpages = {14768--14774},\\n\\tfile = {ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\FR6CF252\\\\\\\\S0272884219310296.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Boldyrev, N. A.\",\"Pavlenko, A. V.\",\"Shilkina, L. A.\",\"Nazarenko, A. V.\",\"Bokov, A. A.\",\"Reznichenko, L. A.\",\"Rudskaya, A. G.\",\"Panchenko, E. I.\"],\"key\":\"boldyrev_structure_2019\",\"id\":\"boldyrev_structure_2019\",\"bibbaseid\":\"boldyrev-pavlenko-shilkina-nazarenko-bokov-reznichenko-rudskaya-panchenko-structuremicrostructuredielectricandpiezoelectricpropertiesof1xybifeotextrm3xpbfetextrm05nbtextrm05otextrm3ypbtiotextrm3ceramics-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0272884219310296\"},\"keyword\":[\"Dielectric properties\",\"Perovskites multiferroics\",\"Piezoelectric properties\",\"Solid solutions\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Piezoresistance and magnetoresistance of composites based on manganite La$_{\\\\textrm{0.7}}$Sr$_{\\\\textrm{0.3}}$MnO$_{\\\\textrm{3}}$\",\"volume\":\"9\",\"issn\":\"2218-5046\",\"url\":\"https://lettersonmaterials.com/en/Readers/Article.aspx?aid=15201\",\"doi\":\"10.22226/2410-3535-2019-2-223-227\",\"abstract\":\"The development of new sensitive multifunctional materials, which simultaneously react both to mechanical pressure and a constant magnetic field, is one of challenges of the modern materials science. In order to create materials that can simultaneously possess extrinsic piezoresistance and magnetoresistance, polymer composites based on La0.7Sr0.3MnO3 (LSMO) and low density polyethylene (LDPE) of composition (100‑x)LSMO / xLDPE at x = 7, 8, 9, 12, 15, 17, 18, 22 mass percent have been synthesized in this work. The composites have been synthesized at 170°C and a pressure of 50 MPa in the presence of hydrocarbons. The phase composition of the obtained samples has been studied by X-ray diffraction and infrared spectroscopy. Electric, piezoresistance and magnetoresistance properties of the samples have been studied. It has been found out that with increasing concentration of polyethylene, the electrical resistance of the samples also increases. It has been established that the percolation threshold of the composites is about 13 wt.% of polyethylene. A maximum is observed in the dependence of the electrical resistance of the samples on the uniaxial pressure at a concentration of polyethylene near the percolation threshold at x =15 wt.%. Samples with concentration of x =15 wt.% of low density polyethylene show extrinsic piezoresistance of about 17 % in the pressure range 0 – 270 kPa. Significant hysteresis is observed when considering the dependence of piezoresistance on pressure for all samples. The pressure sensitivity for a sample of 85 %LSMO / 15 %LDPE reaches 8.40 mΩ / Pa. The maximum values of the negative isotropic tunnel magnetoresistance of the composites 88 %LSMO / 12 %LDPE have values of about 2 % in a 15 kOe magnetic field. We believe that the materials studied in the paper could be useful for designing multifunctional biosensors of mechanical pressure and constant magnetic field.\",\"language\":\"en\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Letters on Materials\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kabirov\"],\"firstnames\":[\"Y.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bogatin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sidorenko\"],\"firstnames\":[\"E.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Belokobylsky\"],\"firstnames\":[\"M.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheikin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Letovaltsev\"],\"firstnames\":[\"A.\",\"O.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bulanova\"],\"firstnames\":[\"A.\",\"L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prutsakova\"],\"firstnames\":[\"N.\",\"V.\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2019\",\"note\":\"Publisher: Letters on Materials\",\"pages\":\"223–227\",\"file\":\"Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\KQGQ4KDV\\\\\\\\Kabirov и др. - 2019 - Piezoresistance and magnetoresistance of composite.pdf:application/pdf\",\"bibtex\":\"@article{kabirov_piezoresistance_2019,\\n\\ttitle = {Piezoresistance and magnetoresistance of composites based on manganite {La}$_{\\\\textrm{0.7}}${Sr}$_{\\\\textrm{0.3}}${MnO}$_{\\\\textrm{3}}$},\\n\\tvolume = {9},\\n\\tissn = {2218-5046},\\n\\turl = {https://lettersonmaterials.com/en/Readers/Article.aspx?aid=15201},\\n\\tdoi = {10.22226/2410-3535-2019-2-223-227},\\n\\tabstract = {The development of new sensitive multifunctional materials, which simultaneously react both to mechanical pressure and a constant magnetic field, is one of challenges of the modern materials science. In order to create materials that can simultaneously possess extrinsic piezoresistance and magnetoresistance, polymer composites based on La0.7Sr0.3MnO3 (LSMO) and low density polyethylene (LDPE) of composition (100‑x)LSMO / xLDPE at x = 7, 8, 9, 12, 15, 17, 18, 22 mass percent have been synthesized in this work. The composites have been synthesized at 170°C and a pressure of 50 MPa in the presence of hydrocarbons. The phase composition of the obtained samples has been studied by X-ray diffraction and infrared spectroscopy. Electric, piezoresistance and magnetoresistance properties of the samples have been studied. It has been found out that with increasing concentration of polyethylene, the electrical resistance of the samples also increases. It has been established that the percolation threshold of the composites is about 13 wt.\\\\% of polyethylene. A maximum is observed in the dependence of the electrical resistance of the samples on the uniaxial pressure at a concentration of polyethylene near the percolation threshold at x =15 wt.\\\\%. Samples with concentration of x =15 wt.\\\\% of low density polyethylene show extrinsic piezoresistance of about 17 \\\\% in the pressure range 0 – 270 kPa. Significant hysteresis is observed when considering the dependence of piezoresistance on pressure for all samples. The pressure sensitivity for a sample of 85 \\\\%LSMO / 15 \\\\%LDPE reaches 8.40 mΩ / Pa. The maximum values of the negative isotropic tunnel magnetoresistance of the composites 88 \\\\%LSMO / 12 \\\\%LDPE have values of about 2 \\\\% in a 15 kOe magnetic field. We believe that the materials studied in the paper could be useful for designing multifunctional biosensors of mechanical pressure and constant magnetic field.},\\n\\tlanguage = {en},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Letters on Materials},\\n\\tauthor = {Kabirov, Y. V. and Bogatin, A. S. and Sidorenko, E. N. and Belokobylsky, M. V. and Mikheikin, A. S. and Letovaltsev, A. O. and Bulanova, A. L. and Prutsakova, N. V.},\\n\\tmonth = may,\\n\\tyear = {2019},\\n\\tnote = {Publisher: Letters on Materials},\\n\\tpages = {223--227},\\n\\tfile = {Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\KQGQ4KDV\\\\\\\\Kabirov и др. - 2019 - Piezoresistance and magnetoresistance of composite.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Kabirov, Y. V.\",\"Bogatin, A. S.\",\"Sidorenko, E. N.\",\"Belokobylsky, M. V.\",\"Mikheikin, A. S.\",\"Letovaltsev, A. O.\",\"Bulanova, A. L.\",\"Prutsakova, N. V.\"],\"key\":\"kabirov_piezoresistance_2019\",\"id\":\"kabirov_piezoresistance_2019\",\"bibbaseid\":\"kabirov-bogatin-sidorenko-belokobylsky-mikheikin-letovaltsev-bulanova-prutsakova-piezoresistanceandmagnetoresistanceofcompositesbasedonmanganitelatextrm07srtextrm03mnotextrm3-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://lettersonmaterials.com/en/Readers/Article.aspx?aid=15201\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Phase transitions, energy storage performances and electrocaloric effect of the lead-free Ba$_{\\\\textrm{0.85}}$Ca$_{\\\\textrm{0.15}}$Zr$_{\\\\textrm{0.10}}$Ti$_{\\\\textrm{0.90}}$O$_{\\\\textrm{3}}$ ceramic relaxor\",\"volume\":\"30\",\"issn\":\"1573-482X\",\"url\":\"https://doi.org/10.1007/s10854-019-00946-5\",\"doi\":\"10.1007/s10854-019-00946-5\",\"abstract\":\"Lead-free Ba0.85Ca0.15Zr0.10Ti0.90O3 (BCZT) ceramic exhibits excellent dielectric, ferroelectric and piezoelectric properties at the morphotropic phase boundary (MPB). Previously, we demonstrated that the use of the anionic surfactant sodium dodecyl sulfate (SDS, NaC12H25SO4) could enhance the dielectric properties of BCZT ceramic using surfactant-assisted solvothermal processing [1]. In the present study, structural, dielectric, ferroelectric properties, as well as electrocaloric effect and energy storage performances of this BCZT ceramic were thoroughly investigated. X-ray diffraction (XRD) measurements revealed the presence of single perovskite phase at room temperature with the coexistence of orthorhombic and tetragonal symmetries. In-situ Raman spectroscopy results confirmed the existence of all phase transitions from rhombohedral through orthorhombic and tetragonal to cubic symmetries when the temperature varies as reported in undoped-BaTiO3. Evolution of energy storage performances with temperature have been investigated. BCZT ceramic exhibits a high energy storage efficiency of ~ 80% at 120 °C. In addition, the electrocaloric responsivity was found to be 0.164 × 10−6 K·m/V at 363 K.\",\"language\":\"en\",\"number\":\"7\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Materials Science: Materials in Electronics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Hanani\"],\"firstnames\":[\"Zouhair\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mezzane\"],\"firstnames\":[\"Daoud\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Amjoud\"],\"firstnames\":[\"M’barek\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"Anna\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fourcade\"],\"firstnames\":[\"Sébastien\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gagou\"],\"firstnames\":[\"Yaovi\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Hoummada\"],\"firstnames\":[\"Khalid\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"Mimoun\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gouné\"],\"firstnames\":[\"Mohamed\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2019\",\"pages\":\"6430–6438\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\8NW2JEKW\\\\a̋nani и др. - 2019 - Phase transitions, energy storage performances and.pdf:application/pdf\",\"bibtex\":\"@article{hanani_phase_2019,\\n\\ttitle = {Phase transitions, energy storage performances and electrocaloric effect of the lead-free {Ba}$_{\\\\textrm{0.85}}${Ca}$_{\\\\textrm{0.15}}${Zr}$_{\\\\textrm{0.10}}${Ti}$_{\\\\textrm{0.90}}${O}$_{\\\\textrm{3}}$ ceramic relaxor},\\n\\tvolume = {30},\\n\\tissn = {1573-482X},\\n\\turl = {https://doi.org/10.1007/s10854-019-00946-5},\\n\\tdoi = {10.1007/s10854-019-00946-5},\\n\\tabstract = {Lead-free Ba0.85Ca0.15Zr0.10Ti0.90O3 (BCZT) ceramic exhibits excellent dielectric, ferroelectric and piezoelectric properties at the morphotropic phase boundary (MPB). Previously, we demonstrated that the use of the anionic surfactant sodium dodecyl sulfate (SDS, NaC12H25SO4) could enhance the dielectric properties of BCZT ceramic using surfactant-assisted solvothermal processing [1]. In the present study, structural, dielectric, ferroelectric properties, as well as electrocaloric effect and energy storage performances of this BCZT ceramic were thoroughly investigated. X-ray diffraction (XRD) measurements revealed the presence of single perovskite phase at room temperature with the coexistence of orthorhombic and tetragonal symmetries. In-situ Raman spectroscopy results confirmed the existence of all phase transitions from rhombohedral through orthorhombic and tetragonal to cubic symmetries when the temperature varies as reported in undoped-BaTiO3. Evolution of energy storage performances with temperature have been investigated. BCZT ceramic exhibits a high energy storage efficiency of {\\\\textasciitilde} 80\\\\% at 120 °C. In addition, the electrocaloric responsivity was found to be 0.164 × 10−6 K·m/V at 363 K.},\\n\\tlanguage = {en},\\n\\tnumber = {7},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Materials Science: Materials in Electronics},\\n\\tauthor = {Hanani, Zouhair and Mezzane, Daoud and Amjoud, M’barek and Razumnaya, Anna G. and Fourcade, Sébastien and Gagou, Yaovi and Hoummada, Khalid and El Marssi, Mimoun and Gouné, Mohamed},\\n\\tmonth = apr,\\n\\tyear = {2019},\\n\\tpages = {6430--6438},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\8NW2JEKW\\\\\\\\Hanani и др. - 2019 - Phase transitions, energy storage performances and.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Hanani, Z.\",\"Mezzane, D.\",\"Amjoud, M.\",\"Razumnaya, A. G.\",\"Fourcade, S.\",\"Gagou, Y.\",\"Hoummada, K.\",\"El Marssi, M.\",\"Gouné, M.\"],\"key\":\"hanani_phase_2019\",\"id\":\"hanani_phase_2019\",\"bibbaseid\":\"hanani-mezzane-amjoud-razumnaya-fourcade-gagou-hoummada-elmarssi-etal-phasetransitionsenergystorageperformancesandelectrocaloriceffectoftheleadfreebatextrm085catextrm015zrtextrm010titextrm090otextrm3ceramicrelaxor-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1007/s10854-019-00946-5\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Phase transitions in Bi$_{\\\\textrm{4}}$Ti$_{\\\\textrm{3}}$O$_{\\\\textrm{12}}$\",\"volume\":\"75\",\"copyright\":\"Copyright (c) 2019 International Union of Crystallography\",\"issn\":\"2052-5206\",\"url\":\"https://journals.iucr.org/b/issues/2019/06/00/dq5041/\",\"doi\":\"10.1107/S2052520619011843\",\"abstract\":\"A Landau-type phase diagram describing the temperature phase transitions in the layered perovskite ferroelectric Bi4Ti3O12 is constructed.\",\"language\":\"en\",\"number\":\"6\",\"urldate\":\"2023-11-11\",\"journal\":\"Acta Crystallographica Section B: Structural Science, Crystal Engineering and Materials\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"M.\",\"V.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2019\",\"note\":\"Number: 6 Publisher: International Union of Crystallography\",\"pages\":\"978–986\",\"bibtex\":\"@article{shirokov_phase_2019,\\n\\ttitle = {Phase transitions in {Bi}$_{\\\\textrm{4}}${Ti}$_{\\\\textrm{3}}${O}$_{\\\\textrm{12}}$},\\n\\tvolume = {75},\\n\\tcopyright = {Copyright (c) 2019 International Union of Crystallography},\\n\\tissn = {2052-5206},\\n\\turl = {https://journals.iucr.org/b/issues/2019/06/00/dq5041/},\\n\\tdoi = {10.1107/S2052520619011843},\\n\\tabstract = {A Landau-type phase diagram describing the temperature phase transitions in the layered perovskite ferroelectric Bi4Ti3O12 is constructed.},\\n\\tlanguage = {en},\\n\\tnumber = {6},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Acta Crystallographica Section B: Structural Science, Crystal Engineering and Materials},\\n\\tauthor = {Shirokov, V. B. and Talanov, M. V.},\\n\\tmonth = dec,\\n\\tyear = {2019},\\n\\tnote = {Number: 6\\nPublisher: International Union of Crystallography},\\n\\tpages = {978--986},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Talanov, M. V.\"],\"key\":\"shirokov_phase_2019\",\"id\":\"shirokov_phase_2019\",\"bibbaseid\":\"shirokov-talanov-phasetransitionsinbitextrm4titextrm3otextrm12-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.iucr.org/b/issues/2019/06/00/dq5041/\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"INVESTIGATION OF STRUCTURAL, MICROSTRUCTURAL AND ELECTROCHEMICAL CHARACTERISTICS OF Pt/SnO$_{\\\\textrm{x}}$-C ELECTROCATALYSTS PREPARED VIA ELECTROCHEMICAL DISPERSION OF TIN AND PLATINUM\",\"volume\":\"62\",\"issn\":\"2500-3070\",\"url\":\"http://ctj-isuct.ru/article/view/1551\",\"doi\":\"10.6060/ivkkt.20196209.5945\",\"abstract\":\"Аннотация Порошки оксидов олова (SnOx) с различной структурой и составом и Pt/SnOx-C электрокатализаторы для топливных элементов с прямым окислением этанола были получены путем электрохимического диспергирования оловянных и платиновых электродов под действием импульсного переменного тока с использованием электролитов с различными типами анионов (Cl- и F-). Полученные порошки оксидов олова, композиционные носители SnOx-C и катализаторы Pt/SnOx-C были исследованы различными методами: рентгеновская дифракция, рамановская спектроскопия, сканирующая и просвечивающая электронная микроскопия. Наночастицы SnO2 со средним размером 5 - 8 нм были синтезированы в Cl- -содержащем растворе. В свою очередь, было обнаружено, что во F- - содержащем электролите были получены наночастицы SnO с выраженной анизотропией формы и размером частиц. Полученные оксиды олова использовались в качестве предшественников в синтезе Pt/SnOx-C катализаторов (загрузка Pt 20%, D111 = 10,5-13,5 нм) также с применением технологии электрохимического диспергирования под действием импульсного переменного тока. Электрохимически активная площадь поверхности Pt/SnOx-C электрокатализаторов, определенная методом окислительной десорбции CO, составляла 13-15 м2г-1. Электрокаталитическую активность электрокатализаторов изучали для реакции электрохимического окисления этанола методами циклической вольтамперометрии с использованием вращающегося дискового электрода. Было обнаружено, что присутствие оксидов олова оказывает одинаковое влияние на реакции электрохимического окисления СО и этанола независимо от структурных особенностей их частиц. \\\\textlessspan style=\\\"opacity: 0;\\\"\\\\textgreater . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . \\\\textless/span\\\\textgreater\",\"language\":\"ru-RU\",\"number\":\"9\",\"urldate\":\"2023-11-11\",\"journal\":\"ИЗВЕСТИЯ ВЫСШИХ УЧЕБНЫХ ЗАВЕДЕНИЙ. СЕРИЯ «ХИМИЯ И ХИМИЧЕСКАЯ ТЕХНОЛОГИЯ»\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"Alexandra\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Avramenko\"],\"firstnames\":[\"Marina\",\"V.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2019\",\"keywords\":\"Pt/C, оксиды олова, топливный элемент, электроокисление этанола, электрохимическое диспергирование\",\"pages\":\"53–59\",\"file\":\"Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\VKA94EMJ\\\\\\\\Kuriganova и др. - 2019 - INVESTIGATION OF STRUCTURAL, MICROSTRUCTURAL AND E.pdf:application/pdf\",\"bibtex\":\"@article{kuriganova_investigation_2019,\\n\\ttitle = {{INVESTIGATION} {OF} {STRUCTURAL}, {MICROSTRUCTURAL} {AND} {ELECTROCHEMICAL} {CHARACTERISTICS} {OF} {Pt}/{SnO}$_{\\\\textrm{x}}$-{C} {ELECTROCATALYSTS} {PREPARED} {VIA} {ELECTROCHEMICAL} {DISPERSION} {OF} {TIN} {AND} {PLATINUM}},\\n\\tvolume = {62},\\n\\tissn = {2500-3070},\\n\\turl = {http://ctj-isuct.ru/article/view/1551},\\n\\tdoi = {10.6060/ivkkt.20196209.5945},\\n\\tabstract = {Аннотация\\n\\t\\t\\t\\t\\tПорошки оксидов олова (SnOx) с различной структурой и составом и Pt/SnOx-C электрокатализаторы для топливных элементов с прямым окислением этанола были получены путем электрохимического диспергирования оловянных и платиновых электродов под действием импульсного переменного тока с использованием электролитов с различными типами анионов (Cl- и F-). Полученные порошки оксидов олова, композиционные носители SnOx-C и катализаторы Pt/SnOx-C были исследованы различными методами: рентгеновская дифракция, рамановская спектроскопия, сканирующая и просвечивающая электронная микроскопия. Наночастицы SnO2 со средним размером 5 - 8 нм были синтезированы в Cl- -содержащем растворе. В свою очередь, было обнаружено, что во F- - содержащем электролите были получены наночастицы SnO с выраженной анизотропией формы и размером частиц. Полученные оксиды олова использовались в качестве предшественников в синтезе Pt/SnOx-C катализаторов (загрузка Pt 20\\\\%, D111 = 10,5-13,5 нм) также с применением технологии электрохимического диспергирования под действием импульсного переменного тока. Электрохимически активная площадь поверхности Pt/SnOx-C электрокатализаторов, определенная методом окислительной десорбции CO, составляла 13-15 м2г-1. Электрокаталитическую активность электрокатализаторов изучали для реакции электрохимического окисления этанола методами циклической вольтамперометрии с использованием вращающегося дискового электрода. Было обнаружено, что присутствие оксидов олова оказывает одинаковое влияние на реакции электрохимического окисления СО и этанола независимо от структурных особенностей их частиц.\\n{\\\\textless}span style=\\\"opacity: 0;\\\"{\\\\textgreater} . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . {\\\\textless}/span{\\\\textgreater}},\\n\\tlanguage = {ru-RU},\\n\\tnumber = {9},\\n\\turldate = {2023-11-11},\\n\\tjournal = {ИЗВЕСТИЯ ВЫСШИХ УЧЕБНЫХ ЗАВЕДЕНИЙ. СЕРИЯ «ХИМИЯ И ХИМИЧЕСКАЯ ТЕХНОЛОГИЯ»},\\n\\tauthor = {Kuriganova, Alexandra B. and Smirnova, Nina V. and Leontyev, Igor N. and Avramenko, Marina V.},\\n\\tmonth = aug,\\n\\tyear = {2019},\\n\\tkeywords = {Pt/C, оксиды олова, топливный элемент, электроокисление этанола, электрохимическое диспергирование},\\n\\tpages = {53--59},\\n\\tfile = {Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\VKA94EMJ\\\\\\\\Kuriganova и др. - 2019 - INVESTIGATION OF STRUCTURAL, MICROSTRUCTURAL AND E.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Kuriganova, A. B.\",\"Smirnova, N. V.\",\"Leontyev, I. N.\",\"Avramenko, M. V.\"],\"key\":\"kuriganova_investigation_2019\",\"id\":\"kuriganova_investigation_2019\",\"bibbaseid\":\"kuriganova-smirnova-leontyev-avramenko-investigationofstructuralmicrostructuralandelectrochemicalcharacteristicsofptsnotextrmxcelectrocatalystspreparedviaelectrochemicaldispersionoftinandplatinum-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://ctj-isuct.ru/article/view/1551\"},\"keyword\":[\"Pt/C\",\"оксиды олова\",\"топливный элемент\",\"электроокисление этанола\",\"электрохимическое диспергирование\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Electrochemical Synthesis of TiO$_{\\\\textrm{2}}$ under Pulse Alternating Current: Effect of Thermal Treatment on the Photocatalytic Activity\",\"volume\":\"4\",\"copyright\":\"© 2019 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim\",\"issn\":\"2365-6549\",\"shorttitle\":\"Electrochemical Synthesis of TiO2 under Pulse Alternating Current\",\"url\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201803367\",\"doi\":\"10.1002/slct.201803367\",\"abstract\":\"The current work aimed to study the effect of thermal treatment on the structural, optical, and photocatalytic properties of TiO2 nanoparticles synthesized by a novel large-scale electrochemical method using pulse alternating current (PAC). The obtained titania was characterized via XRD, TEM, XPS, UV-Vis DRS, PL, Raman and FTIR spectroscopy. The as-prepared TiO2 was found to be poorly crystallized and partly amorphous. Following thermal annealing, the anatase structure is developed at temperatures of 400–600 °C. The photoreactivity of the TiO2 nanoparticles was evaluated for the degradation of methylene blue (MB) and rhodamin B (RhB) dyes under UVA irradiation. As shown, the adsorption properties and photocatalytic activity of the as-prepared TiO2 strongly depend on the chemical nature of the dye. The enhanced photocatalytic performance for the MB and RhB degradation was observed for the sample annealed at 400 °C, which coincides with a balance between the degree of crystallinity, specific surface area, optical properties and efficiency of electron-hole pair separation.\",\"language\":\"en\",\"number\":\"6\",\"urldate\":\"2023-11-11\",\"journal\":\"ChemistrySelect\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Ulyankina\"],\"firstnames\":[\"Anna\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Avramenko\"],\"firstnames\":[\"Marina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kusnetsov\"],\"firstnames\":[\"Denis\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Firestein\"],\"firstnames\":[\"Konstantin\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhigunov\"],\"firstnames\":[\"Denis\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\"],\"suffixes\":[]}],\"year\":\"2019\",\"note\":\"_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/slct.201803367\",\"keywords\":\"crystallinity, dye, electrochemical synthesis, photocatalysis, titanium dioxide\",\"pages\":\"2001–2007\",\"file\":\"Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\NQTKT7VJ\\\\\\\\slct.html:text/html\",\"bibtex\":\"@article{ulyankina_electrochemical_2019,\\n\\ttitle = {Electrochemical {Synthesis} of {TiO}$_{\\\\textrm{2}}$ under {Pulse} {Alternating} {Current}: {Effect} of {Thermal} {Treatment} on the {Photocatalytic} {Activity}},\\n\\tvolume = {4},\\n\\tcopyright = {© 2019 Wiley-VCH Verlag GmbH \\\\& Co. KGaA, Weinheim},\\n\\tissn = {2365-6549},\\n\\tshorttitle = {Electrochemical {Synthesis} of {TiO2} under {Pulse} {Alternating} {Current}},\\n\\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201803367},\\n\\tdoi = {10.1002/slct.201803367},\\n\\tabstract = {The current work aimed to study the effect of thermal treatment on the structural, optical, and photocatalytic properties of TiO2 nanoparticles synthesized by a novel large-scale electrochemical method using pulse alternating current (PAC). The obtained titania was characterized via XRD, TEM, XPS, UV-Vis DRS, PL, Raman and FTIR spectroscopy. The as-prepared TiO2 was found to be poorly crystallized and partly amorphous. Following thermal annealing, the anatase structure is developed at temperatures of 400–600 °C. The photoreactivity of the TiO2 nanoparticles was evaluated for the degradation of methylene blue (MB) and rhodamin B (RhB) dyes under UVA irradiation. As shown, the adsorption properties and photocatalytic activity of the as-prepared TiO2 strongly depend on the chemical nature of the dye. The enhanced photocatalytic performance for the MB and RhB degradation was observed for the sample annealed at 400 °C, which coincides with a balance between the degree of crystallinity, specific surface area, optical properties and efficiency of electron-hole pair separation.},\\n\\tlanguage = {en},\\n\\tnumber = {6},\\n\\turldate = {2023-11-11},\\n\\tjournal = {ChemistrySelect},\\n\\tauthor = {Ulyankina, Anna and Avramenko, Marina and Kusnetsov, Denis and Firestein, Konstantin and Zhigunov, Denis and Smirnova, Nina},\\n\\tyear = {2019},\\n\\tnote = {\\\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/slct.201803367},\\n\\tkeywords = {crystallinity, dye, electrochemical synthesis, photocatalysis, titanium dioxide},\\n\\tpages = {2001--2007},\\n\\tfile = {Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\NQTKT7VJ\\\\\\\\slct.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Ulyankina, A.\",\"Avramenko, M.\",\"Kusnetsov, D.\",\"Firestein, K.\",\"Zhigunov, D.\",\"Smirnova, N.\"],\"key\":\"ulyankina_electrochemical_2019\",\"id\":\"ulyankina_electrochemical_2019\",\"bibbaseid\":\"ulyankina-avramenko-kusnetsov-firestein-zhigunov-smirnova-electrochemicalsynthesisoftiotextrm2underpulsealternatingcurrenteffectofthermaltreatmentonthephotocatalyticactivity-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201803367\"},\"keyword\":[\"crystallinity\",\"dye\",\"electrochemical synthesis\",\"photocatalysis\",\"titanium dioxide\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Температурная зависимость фононных и магнонных мод в гетероструктурах мультиферроик - сегнетоэлектрик\",\"issn\":\"2500-0640\",\"url\":\"https://www.libnauka.ru/item.php?doi=10.7868/S25000640190103\",\"doi\":\"10.7868/S25000640190103\",\"abstract\":\"Пленки феррита висмута BiFeO выращены на монокристаллической подложке (001) MgO по блочному механизму роста методом высокочастотного катодного распыления с использованием в качестве буферного слоя сегнетоэлектрика BaSr _ TiO при варьировании состава x. Изучение гетероструктур методом рентгеновской дифракции показало, что пленки характеризуются псевдотетрагональной симметрией при комнатной температуре. Определено, что степень тетрагонального искажения слоев BaSr _ TiO возрастает с увеличением концентрации Ba, в то время как в слоях BiFeO она остается практически неизменной. Методом атомно-силовой микроскопии установлено, что пленки BiFeOвыросли по блочному механизму роста, причем блоки строго ориентированы относительно друг друга и кристаллографических осей подложки MgO. Высокотемпературные исследования спектров комбинационного рассеяния света в широком диапазоне температур 295-900 K и частот от 50 до 1600 смпоказали, что интенсивность полосы 1250 см, соответствующей плотности состояний двухмагнонных возбуждений, линейно понижается при повышении температуры. Анализ температурного поведения полосы 1250 см позволяет предполагать, что в изученных пленках BiFeO антиферромагнитный фазовый переход происходит в диапазоне температур 600-700 K. Использование сегнетоэлектрических буферных слоев BaSr _ TiO с разной степенью тетрагонального искажения позволяет управлять деформацией пленок BiFeO, возникающей в результате несоответствия параметров решеток в смежных слоях, и тем самым искусственно варьировать свойства данных структур.\",\"language\":\"ru\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Science in the South of Russia\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Бабарикин\"],\"firstnames\":[\"Д.С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Разумная\"],\"firstnames\":[\"А.Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Стрюков\"],\"firstnames\":[\"Д.В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Анохин\"],\"firstnames\":[\"А.С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Михейкин\"],\"firstnames\":[\"А.С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Павленко\"],\"firstnames\":[\"А.В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Зинченко\"],\"firstnames\":[\"С.П.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.М.\"],\"suffixes\":[]}],\"year\":\"2019\",\"pages\":\"21–30\",\"file\":\"Бабарикин и др. - 2019 - Температурная зависимость фононных и магнонных мод.pdf:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\2GW49MUE\\\\\\\\Бабарикин и др. - 2019 - Температурная зависимость фононных и магнонных мод.pdf:application/pdf\",\"bibtex\":\"@article{__2019-3,\\n\\ttitle = {Температурная зависимость фононных и магнонных мод в гетероструктурах мультиферроик - сегнетоэлектрик},\\n\\tissn = {2500-0640},\\n\\turl = {https://www.libnauka.ru/item.php?doi=10.7868/S25000640190103},\\n\\tdoi = {10.7868/S25000640190103},\\n\\tabstract = {Пленки феррита висмута BiFeO выращены на монокристаллической подложке (001) MgO по блочному механизму роста методом высокочастотного катодного распыления с использованием в качестве буферного слоя сегнетоэлектрика BaSr \\\\_ TiO при варьировании состава x. Изучение гетероструктур методом рентгеновской дифракции показало, что пленки характеризуются псевдотетрагональной симметрией при комнатной температуре. Определено, что степень тетрагонального искажения слоев BaSr \\\\_ TiO возрастает с увеличением концентрации Ba, в то время как в слоях BiFeO она остается практически неизменной. Методом атомно-силовой микроскопии установлено, что пленки BiFeOвыросли по блочному механизму роста, причем блоки строго ориентированы относительно друг друга и кристаллографических осей подложки MgO. Высокотемпературные исследования спектров комбинационного рассеяния света в широком диапазоне температур 295-900 K и частот от 50 до 1600 смпоказали, что интенсивность полосы 1250 см, соответствующей плотности состояний двухмагнонных возбуждений, линейно понижается при повышении температуры. Анализ температурного поведения полосы 1250 см позволяет предполагать, что в изученных пленках BiFeO антиферромагнитный фазовый переход происходит в диапазоне температур 600-700 K. Использование сегнетоэлектрических буферных слоев BaSr \\\\_ TiO с разной степенью тетрагонального искажения позволяет управлять деформацией пленок BiFeO, возникающей в результате несоответствия параметров решеток в смежных слоях, и тем самым искусственно варьировать свойства данных структур.},\\n\\tlanguage = {ru},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Science in the South of Russia},\\n\\tauthor = {Бабарикин, Д.С. and Разумная, А.Г. and Стрюков, Д.В. and Анохин, А.С. and Михейкин, А.С. and Павленко, А.В. and Широков, В.Б. and Зинченко, С.П. and Мухортов, В.М.},\\n\\tyear = {2019},\\n\\tpages = {21--30},\\n\\tfile = {Бабарикин и др. - 2019 - Температурная зависимость фононных и магнонных мод.pdf:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\2GW49MUE\\\\\\\\Бабарикин и др. - 2019 - Температурная зависимость фононных и магнонных мод.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Бабарикин, Д.\",\"Разумная, А.\",\"Стрюков, Д.\",\"Анохин, А.\",\"Михейкин, А.\",\"Павленко, А.\",\"Широков, В.\",\"Зинченко, С.\",\"Мухортов, В.\"],\"key\":\"__2019-3\",\"id\":\"__2019-3\",\"bibbaseid\":\"--------etal--2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.libnauka.ru/item.php?doi=10.7868/S25000640190103\"},\"metadata\":{\"authorlinks\":{\"miyagusuku, r\":\"https://www.real.utsunomiya-u.ac.jp/invmap/\"}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Characterization of an UO$_{\\\\textrm{2}}$ ceramic via Raman imaging and electron back-scattering diffraction\",\"volume\":\"147\",\"issn\":\"1044-5803\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S1044580318315651\",\"doi\":\"10.1016/j.matchar.2018.11.006\",\"abstract\":\"A surface state analysis of an UO2 ceramic is performed by combining Raman imaging and electron back-scattering diffraction. Special attention is paid to the behavior of the T2g band intensity versus the crystalline orientation. In order to clarify the origin of the T2g intensity variation in the appropriate Raman image, electron back-scattering diffraction (EBSD) measurements are carried out. EBSD data allow a theoretical estimation of the Raman T2g band intensities. Both maps have been compared in order to correlate them, and to distinguish regions where they are analogous, from those where some physical or chemical effects (stoichiometry, or strains) induce different behavior. More generally, this highlights the interest and the complementarity of combining Raman spectroscopy and EBSD for a better microstructure knowledge.\",\"urldate\":\"2023-11-11\",\"journal\":\"Materials Characterization\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"O.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Iltis\"],\"firstnames\":[\"X.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Desgranges\"],\"firstnames\":[\"L.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ammar\"],\"firstnames\":[\"M.\",\"R.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Genevois\"],\"firstnames\":[\"C.\"],\"suffixes\":[]},{\"propositions\":[\"de\"],\"lastnames\":[\"Bilbao\"],\"firstnames\":[\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Canizarès\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Barannikova\"],\"firstnames\":[\"S.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Simon\"],\"firstnames\":[\"P.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2019\",\"keywords\":\"Crystalline orientation, Crystallographic indices, EBSD, Euler angles, Pole figures, Raman imaging, T band, UO\",\"pages\":\"280–285\",\"file\":\"ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\IZ29TZSV\\\\§1044580318315651.html:text/html\",\"bibtex\":\"@article{maslova_characterization_2019,\\n\\ttitle = {Characterization of an {UO}$_{\\\\textrm{2}}$ ceramic via {Raman} imaging and electron back-scattering diffraction},\\n\\tvolume = {147},\\n\\tissn = {1044-5803},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S1044580318315651},\\n\\tdoi = {10.1016/j.matchar.2018.11.006},\\n\\tabstract = {A surface state analysis of an UO2 ceramic is performed by combining Raman imaging and electron back-scattering diffraction. Special attention is paid to the behavior of the T2g band intensity versus the crystalline orientation. In order to clarify the origin of the T2g intensity variation in the appropriate Raman image, electron back-scattering diffraction (EBSD) measurements are carried out. EBSD data allow a theoretical estimation of the Raman T2g band intensities. Both maps have been compared in order to correlate them, and to distinguish regions where they are analogous, from those where some physical or chemical effects (stoichiometry, or strains) induce different behavior. More generally, this highlights the interest and the complementarity of combining Raman spectroscopy and EBSD for a better microstructure knowledge.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Materials Characterization},\\n\\tauthor = {Maslova, O. A. and Iltis, X. and Desgranges, L. and Ammar, M. R. and Genevois, C. and de Bilbao, E. and Canizarès, A. and Barannikova, S. A. and Leontyev, I. N. and Simon, P.},\\n\\tmonth = jan,\\n\\tyear = {2019},\\n\\tkeywords = {Crystalline orientation, Crystallographic indices, EBSD, Euler angles, Pole figures, Raman imaging, T band, UO},\\n\\tpages = {280--285},\\n\\tfile = {ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\IZ29TZSV\\\\\\\\S1044580318315651.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Maslova, O. A.\",\"Iltis, X.\",\"Desgranges, L.\",\"Ammar, M. R.\",\"Genevois, C.\",\"de Bilbao, E.\",\"Canizarès, A.\",\"Barannikova, S. A.\",\"Leontyev, I. N.\",\"Simon, P.\"],\"key\":\"maslova_characterization_2019\",\"id\":\"maslova_characterization_2019\",\"bibbaseid\":\"maslova-iltis-desgranges-ammar-genevois-debilbao-canizars-barannikova-etal-characterizationofanuotextrm2ceramicviaramanimagingandelectronbackscatteringdiffraction-2019\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S1044580318315651\"},\"keyword\":[\"Crystalline orientation\",\"Crystallographic indices\",\"EBSD\",\"Euler angles\",\"Pole figures\",\"Raman imaging\",\"T band\",\"UO\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"СТРУКТУРА И ОПТИЧЕСКИЕ СВОЙСТВА ZnO-НАНОКРИСТАЛЛОВ, ПОЛУЧЕННЫХ МЕТОДОМ ИМПУЛЬСНОГО ЛАЗЕРНОГО НАПЫЛЕНИЯ НА ПЛЕНКАХ GaN/Si(111) С ИСПОЛЬЗОВАНИЕМ Au- И NiO-КАТАЛИЗАТОРОВ\",\"volume\":\"72\",\"issn\":\"0367-6765\",\"url\":\"https://www.elibrary.ru/item.asp?id=11036052\",\"abstract\":\"Исследован рост ZnO-нанокристаллов на пленочном подслое GaN/Si(111) методом импульсного лазерного напыления при высоком давлении аргона с использованием Au- и NiO-катализаторов. Использование низкотемпературного NiO-катализатора позволяет снизить оптимальную температуру роста с 900°C (в случае Au-катализатора) до T = 570°C и вырастить высокоориентированные в направлении оси c решетки ZnO-нанокристаллов диаметром 20 нм полностью свободных от дислокаций.\",\"language\":\"ru\",\"number\":\"8\",\"urldate\":\"2023-11-11\",\"journal\":\"Известия Российской Академии Наук. Серия Физическая\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kайдашев\"],\"firstnames\":[\"E.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lorenz\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lenzner\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ramm\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nobis\"],\"firstnames\":[\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grundmann\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zakharov\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Козаков\"],\"firstnames\":[\"А.\",\"Т.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Шевцова\"],\"firstnames\":[\"С.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Абдулвахидов\"],\"firstnames\":[\"К.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"В.\",\"Е.\"],\"suffixes\":[]}],\"year\":\"2008\",\"keywords\":\"⛔ No DOI found\",\"pages\":\"1195–1197\",\"bibtex\":\"@article{k__2008,\\n\\ttitle = {{СТРУКТУРА} И ОПТИЧЕСКИЕ СВОЙСТВА {ZnO}-НАНОКРИСТАЛЛОВ, ПОЛУЧЕННЫХ МЕТОДОМ ИМПУЛЬСНОГО ЛАЗЕРНОГО НАПЫЛЕНИЯ НА ПЛЕНКАХ {GaN}/{Si}(111) С ИСПОЛЬЗОВАНИЕМ {Au}- И {NiO}-КАТАЛИЗАТОРОВ},\\n\\tvolume = {72},\\n\\tissn = {0367-6765},\\n\\turl = {https://www.elibrary.ru/item.asp?id=11036052},\\n\\tabstract = {Исследован рост ZnO-нанокристаллов на пленочном подслое GaN/Si(111) методом импульсного лазерного напыления при высоком давлении аргона с использованием Au- и NiO-катализаторов. Использование низкотемпературного NiO-катализатора позволяет снизить оптимальную температуру роста с 900°C (в случае Au-катализатора) до T = 570°C и вырастить высокоориентированные в направлении оси c решетки ZnO-нанокристаллов диаметром 20 нм полностью свободных от дислокаций.},\\n\\tlanguage = {ru},\\n\\tnumber = {8},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Известия Российской Академии Наук. Серия Физическая},\\n\\tauthor = {Kайдашев, E. M. and Lorenz, M. and Lenzner, J. and Ramm, A. and Nobis, T. and Grundmann, M. and Zakharov, N. and Козаков, А. Т. and Шевцова, С. И. and Абдулвахидов, К. Г. and Кайдашев, В. Е.},\\n\\tyear = {2008},\\n\\tkeywords = {⛔ No DOI found},\\n\\tpages = {1195--1197},\\n}\\n\\n\",\"author_short\":[\"Kайдашев, E. M.\",\"Lorenz, M.\",\"Lenzner, J.\",\"Ramm, A.\",\"Nobis, T.\",\"Grundmann, M.\",\"Zakharov, N.\",\"Козаков, А. Т.\",\"Шевцова, С. И.\",\"Абдулвахидов, К. Г.\",\"Кайдашев, В. Е.\"],\"key\":\"k__2008\",\"id\":\"k__2008\",\"bibbaseid\":\"k-lorenz-lenzner-ramm-nobis-grundmann-zakharov--etal-znogansi111aunio-2008\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.elibrary.ru/item.asp?id=11036052\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"THE STRUCTURE AND PARAMAGNETISM OF (1-x)BiFeO$_{\\\\textrm{3}}$ – xYMnO$_{\\\\textrm{3}}$ SOLID SOLUTIONS\",\"url\":\"https://elibrary.ru/item.asp?id=30471203\",\"abstract\":\"In solid solutions of (1–x)BiFeO 3 –xYMnO 3 around x = 0.5 the monoclinic phase with C2 symmetry is detected. It was found that the Lande parameter values of the electronic paramagnetic resonance signals (g-factors) of compositions with 0 \\\\textless x \\\\textless 0.8 differ from g-factor of the free electron (g e = 2.0023) and depend on concentration of x with the maximum value for x = 0.5. Also paramagnetic parameters correlate with bond lengths and angles between Fe/Mn-centred octahedron in the perovskite structures.\",\"language\":\"en\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Nazarenko\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zaletov\"],\"firstnames\":[\"V.\",\"G.\"],\"suffixes\":[]},{\"firstnames\":[\"Kabirov\"],\"propositions\":[],\"lastnames\":[\"Yu.v.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chagovets\"],\"firstnames\":[\"S.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ananyeva\"],\"firstnames\":[\"E.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudskaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kupriyanov\"],\"firstnames\":[\"M.\",\"F.\"],\"suffixes\":[]}],\"year\":\"2017\",\"keywords\":\"Perovskite, (1-X)bifeo3 -Xymno3, Bifeo3, Epr, Multiferroics, Xrd, Ymno3, ⛔ No DOI found\",\"bibtex\":\"@inproceedings{nazarenko_structure_2017,\\n\\ttitle = {{THE} {STRUCTURE} {AND} {PARAMAGNETISM} {OF} (1-x){BiFeO}$_{\\\\textrm{3}}$ – {xYMnO}$_{\\\\textrm{3}}$ {SOLID} {SOLUTIONS}},\\n\\turl = {https://elibrary.ru/item.asp?id=30471203},\\n\\tabstract = {In solid solutions of (1–x)BiFeO 3 –xYMnO 3 around x = 0.5 the monoclinic phase with C2 symmetry is detected. It was found that the Lande parameter values of the electronic paramagnetic resonance signals (g-factors) of compositions with 0 {\\\\textless} x {\\\\textless} 0.8 differ from g-factor of the free electron (g e = 2.0023) and depend on concentration of x with the maximum value for x = 0.5. Also paramagnetic parameters correlate with bond lengths and angles between Fe/Mn-centred octahedron in the perovskite structures.},\\n\\tlanguage = {en},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Nazarenko, A. V. and Zaletov, V. G. and Kabirov Yu.v. and Chagovets, S. V. and Ananyeva, E. V. and Rudskaya, A. G. and Kupriyanov, M. F.},\\n\\tyear = {2017},\\n\\tkeywords = {Perovskite, (1-X)bifeo3 -Xymno3, Bifeo3, Epr, Multiferroics, Xrd, Ymno3, ⛔ No DOI found},\\n}\\n\\n\",\"author_short\":[\"Nazarenko, A. V.\",\"Zaletov, V. G.\",\"Yu.v., K.\",\"Chagovets, S. V.\",\"Ananyeva, E. V.\",\"Rudskaya, A. G.\",\"Kupriyanov, M. F.\"],\"key\":\"nazarenko_structure_2017\",\"id\":\"nazarenko_structure_2017\",\"bibbaseid\":\"nazarenko-zaletov-yuv-chagovets-ananyeva-rudskaya-kupriyanov-thestructureandparamagnetismof1xbifeotextrm3xymnotextrm3solidsolutions-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=30471203\"},\"keyword\":[\"Perovskite\",\"(1-X)bifeo3 -Xymno3\",\"Bifeo3\",\"Epr\",\"Multiferroics\",\"Xrd\",\"Ymno3\",\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Terahertz spectroscopy of low-energy excitations in Eu$_{\\\\textrm{0.42}}$Sr$_{\\\\textrm{0.58}}$MnO$_{\\\\textrm{3}}$\",\"volume\":\"96\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.96.245120\",\"doi\":\"10.1103/PhysRevB.96.245120\",\"abstract\":\"The origin of low-energy excitations in the polycrystalline Eu0.42Sr0.58MnO3 manganite is explored by terahertz and infrared spectroscopies. The transition from the charge and/or orbital to antiferromagnetic order (TN=130−140K) is seen as smooth (spread over a temperature range from 50 to 100 K) decrease of free-carrier conductivity with the activation energy change from 86 meV (high temperatures) to 0.52 meV (low temperatures). A broad relaxation is observed at around 10cm−1 which we associate with the dynamics of free charge carriers in the presence of random localizing potential. We discover an absorption resonance at ≈50cm−1 below TN that is assigned to the formation of hybridized “acoustic phonon-magnon” quasiparticles.\",\"number\":\"24\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kadyrov\"],\"firstnames\":[\"L.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"E.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhang\"],\"firstnames\":[\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gagkaeva\"],\"firstnames\":[\"Z.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"B.\",\"P.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2017\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"245120\",\"file\":\"APS Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\GFXPT7MJ\\\\¶hysRevB.96.html:text/html\",\"bibtex\":\"@article{kadyrov_terahertz_2017,\\n\\ttitle = {Terahertz spectroscopy of low-energy excitations in {Eu}$_{\\\\textrm{0.42}}${Sr}$_{\\\\textrm{0.58}}${MnO}$_{\\\\textrm{3}}$},\\n\\tvolume = {96},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.96.245120},\\n\\tdoi = {10.1103/PhysRevB.96.245120},\\n\\tabstract = {The origin of low-energy excitations in the polycrystalline Eu0.42Sr0.58MnO3 manganite is explored by terahertz and infrared spectroscopies. The transition from the charge and/or orbital to antiferromagnetic order (TN=130−140K) is seen as smooth (spread over a temperature range from 50 to 100 K) decrease of free-carrier conductivity with the activation energy change from 86 meV (high temperatures) to 0.52 meV (low temperatures). A broad relaxation is observed at around 10cm−1 which we associate with the dynamics of free charge carriers in the presence of random localizing potential. We discover an absorption resonance at ≈50cm−1 below TN that is assigned to the formation of hybridized “acoustic phonon-magnon” quasiparticles.},\\n\\tnumber = {24},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Kadyrov, L. S. and Zhukova, E. S. and Torgashev, V. I. and Zhang, T. and Gagkaeva, Z. V. and Dressel, M. and Gorshunov, B. P.},\\n\\tmonth = dec,\\n\\tyear = {2017},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {245120},\\n\\tfile = {APS Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\GFXPT7MJ\\\\\\\\PhysRevB.96.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Kadyrov, L. S.\",\"Zhukova, E. S.\",\"Torgashev, V. I.\",\"Zhang, T.\",\"Gagkaeva, Z. V.\",\"Dressel, M.\",\"Gorshunov, B. P.\"],\"key\":\"kadyrov_terahertz_2017\",\"id\":\"kadyrov_terahertz_2017\",\"bibbaseid\":\"kadyrov-zhukova-torgashev-zhang-gagkaeva-dressel-gorshunov-terahertzspectroscopyoflowenergyexcitationsineutextrm042srtextrm058mnotextrm3-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.96.245120\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"Reconstructive Phase Transition in YMnO$_{\\\\textrm{3}}$ –BiFeO$_{\\\\textrm{3}}$ Solid Solutions\",\"url\":\"https://elibrary.ru/item.asp?id=30471067\",\"abstract\":\"The structures of the (1–x)YMnO 3 –xBiFeO 3 (0.05 ≤ x ≤ 0.25) solid solutions have been studied by means of the X-ray diffraction method. It was established that in the compounds of the (1–x)YMnO 3 –xBiFeO 3 system the P6 3 cm, the Pbam and Pnma phases are observed at room temperature after annealing at T 1 = 950 °C. The results revealed that in the compounds of the (1–x)YMnO 3 –xBiFeO 3 system the P6 3 cm and Pnma phases take place at room temperature after annealing at T 2 = 1100 °C. The symmetry of the phases, the unit cell parameters, the positional atomic parameters have been determined.\",\"language\":\"en\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Chagovets\"],\"firstnames\":[\"S.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nazarenko\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kozarenko\"],\"firstnames\":[\"S.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudskaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kupriyanov\"],\"firstnames\":[\"M.\",\"F.\"],\"suffixes\":[]}],\"year\":\"2017\",\"keywords\":\"(1-X)bifeo 3 -Xymno 3, Multiferroic, Phase Transition, X-Ray Diffraction, ⛔ No DOI found\",\"bibtex\":\"@inproceedings{chagovets_reconstructive_2017,\\n\\ttitle = {Reconstructive {Phase} {Transition} in {YMnO}$_{\\\\textrm{3}}$ –{BiFeO}$_{\\\\textrm{3}}$ {Solid} {Solutions}},\\n\\turl = {https://elibrary.ru/item.asp?id=30471067},\\n\\tabstract = {The structures of the (1–x)YMnO 3 –xBiFeO 3 (0.05 ≤ x ≤ 0.25) solid solutions have been studied by means of the X-ray diffraction method. It was established that in the compounds of the (1–x)YMnO 3 –xBiFeO 3 system the P6 3 cm, the Pbam and Pnma phases are observed at room temperature after annealing at T 1 = 950 °C. The results revealed that in the compounds of the (1–x)YMnO 3 –xBiFeO 3 system the P6 3 cm and Pnma phases take place at room temperature after annealing at T 2 = 1100 °C. The symmetry of the phases, the unit cell parameters, the positional atomic parameters have been determined.},\\n\\tlanguage = {en},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Chagovets, S. V. and Nazarenko, A. V. and Kozarenko, S. S. and Rudskaya, A. G. and Kupriyanov, M. F.},\\n\\tyear = {2017},\\n\\tkeywords = {(1-X)bifeo 3 -Xymno 3, Multiferroic, Phase Transition, X-Ray Diffraction, ⛔ No DOI found},\\n}\\n\\n\",\"author_short\":[\"Chagovets, S. V.\",\"Nazarenko, A. V.\",\"Kozarenko, S. S.\",\"Rudskaya, A. G.\",\"Kupriyanov, M. F.\"],\"key\":\"chagovets_reconstructive_2017\",\"id\":\"chagovets_reconstructive_2017\",\"bibbaseid\":\"chagovets-nazarenko-kozarenko-rudskaya-kupriyanov-reconstructivephasetransitioninymnotextrm3bifeotextrm3solidsolutions-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=30471067\"},\"keyword\":[\"(1-X)bifeo 3 -Xymno 3\",\"Multiferroic\",\"Phase Transition\",\"X-Ray Diffraction\",\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Lattice dynamics and structural distortions in the multiferroic (Ba,Sr)TiO$_{\\\\textrm{3}}$/(Bi,Nd)FeO$_{\\\\textrm{3}}$ heterostructures\",\"volume\":\"636\",\"issn\":\"0040-6090\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0040609017304443\",\"doi\":\"10.1016/j.tsf.2017.06.009\",\"abstract\":\"We report the synthesis, the structure and phonon spectra studies of epitaxial double-layer heterostructures consisting of Bi0.98Nd0.02FeO3 and Ba0.8Sr0.2TiO3 layers deposited on (100) MgO substrates. The results of x-ray diffraction and the polarization characteristics of Raman spectra suggest a monoclinic symmetry of the systems at room temperature. The observed spectra demonstrate the non-monotonous dependence on the layer thickness that apparently can be related with specificity of the light propagation in the layered thin-film systems.\",\"urldate\":\"2023-11-11\",\"journal\":\"Thin Solid Films\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Stryukov\"],\"firstnames\":[\"D.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golovko\"],\"firstnames\":[\"Yu\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Anokhin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lukyanchuk\"],\"firstnames\":[\"I.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mukhortov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2017\",\"keywords\":\"X-ray diffraction, Raman spectroscopy, Bismuth ferrite, Heterostructures, Lattice distortions, Lattice dynamics, Sputtering\",\"pages\":\"220–224\",\"file\":\"ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\TD9K6CTD\\\\§0040609017304443.html:text/html\",\"bibtex\":\"@article{stryukov_lattice_2017,\\n\\ttitle = {Lattice dynamics and structural distortions in the multiferroic ({Ba},{Sr}){TiO}$_{\\\\textrm{3}}$/({Bi},{Nd}){FeO}$_{\\\\textrm{3}}$ heterostructures},\\n\\tvolume = {636},\\n\\tissn = {0040-6090},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0040609017304443},\\n\\tdoi = {10.1016/j.tsf.2017.06.009},\\n\\tabstract = {We report the synthesis, the structure and phonon spectra studies of epitaxial double-layer heterostructures consisting of Bi0.98Nd0.02FeO3 and Ba0.8Sr0.2TiO3 layers deposited on (100) MgO substrates. The results of x-ray diffraction and the polarization characteristics of Raman spectra suggest a monoclinic symmetry of the systems at room temperature. The observed spectra demonstrate the non-monotonous dependence on the layer thickness that apparently can be related with specificity of the light propagation in the layered thin-film systems.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Thin Solid Films},\\n\\tauthor = {Stryukov, D. V. and Razumnaya, A. G. and Golovko, Yu I. and Anokhin, A. S. and Lukyanchuk, I. A. and Shirokov, V. B. and Mukhortov, V. M.},\\n\\tmonth = aug,\\n\\tyear = {2017},\\n\\tkeywords = {X-ray diffraction, Raman spectroscopy, Bismuth ferrite, Heterostructures, Lattice distortions, Lattice dynamics, Sputtering},\\n\\tpages = {220--224},\\n\\tfile = {ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\TD9K6CTD\\\\\\\\S0040609017304443.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Stryukov, D. V.\",\"Razumnaya, A. G.\",\"Golovko, Y. I.\",\"Anokhin, A. S.\",\"Lukyanchuk, I. A.\",\"Shirokov, V. B.\",\"Mukhortov, V. M.\"],\"key\":\"stryukov_lattice_2017\",\"id\":\"stryukov_lattice_2017\",\"bibbaseid\":\"stryukov-razumnaya-golovko-anokhin-lukyanchuk-shirokov-mukhortov-latticedynamicsandstructuraldistortionsinthemultiferroicbasrtiotextrm3bindfeotextrm3heterostructures-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0040609017304443\"},\"keyword\":[\"X-ray diffraction\",\"Raman spectroscopy\",\"Bismuth ferrite\",\"Heterostructures\",\"Lattice distortions\",\"Lattice dynamics\",\"Sputtering\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Invar effect accompanying charge order in La$_{\\\\textrm{0.25}}$Ca$_{\\\\textrm{0.75}}$MnO$_{\\\\textrm{3}}$\",\"volume\":\"72\",\"issn\":\"1293-2558\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S1293255817305381\",\"doi\":\"10.1016/j.solidstatesciences.2017.08.020\",\"abstract\":\"To determine the role of the Jahn-Teller effect in the orbital and charge ordering of mixed crystals of the strongly correlated La1-xCaxMnO3 system, we have used the diffraction of synchrotron radiation and the subsequent Rietveld analysis of diffraction patterns in order to obtain structural data for La0.25Ca0.75MnO3 compound in the temperature range from 90 to 325 K with a step of ∼2 K. For the first time for this compound, an Invar effect was observed below the charge-order temperature. In the entire temperature range, atomic displacements were analyzed and correlations between charge ordering and deformational modes were made, on the basis of which the secondary role of the Jahn-Teller effect in observed structure distortions was established. A hypothesis of a spin crossover in the vicinity of the charge-ordering temperature is proposed that describes adequately both the obtained structural data and the results of measurements of the macroscopic magnetic and elastic properties of the studied compound as well as related materials with charge ordering.\",\"urldate\":\"2023-11-11\",\"journal\":\"Solid State Sciences\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Trotsenko\"],\"firstnames\":[\"V.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"B.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bush\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2017\",\"keywords\":\"Charge ordering, Correlated electron systems, Invar effect, Spin crossover\",\"pages\":\"144–149\",\"bibtex\":\"@article{trotsenko_invar_2017,\\n\\ttitle = {Invar effect accompanying charge order in {La}$_{\\\\textrm{0.25}}${Ca}$_{\\\\textrm{0.75}}${MnO}$_{\\\\textrm{3}}$},\\n\\tvolume = {72},\\n\\tissn = {1293-2558},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S1293255817305381},\\n\\tdoi = {10.1016/j.solidstatesciences.2017.08.020},\\n\\tabstract = {To determine the role of the Jahn-Teller effect in the orbital and charge ordering of mixed crystals of the strongly correlated La1-xCaxMnO3 system, we have used the diffraction of synchrotron radiation and the subsequent Rietveld analysis of diffraction patterns in order to obtain structural data for La0.25Ca0.75MnO3 compound in the temperature range from 90 to 325 K with a step of ∼2 K. For the first time for this compound, an Invar effect was observed below the charge-order temperature. In the entire temperature range, atomic displacements were analyzed and correlations between charge ordering and deformational modes were made, on the basis of which the secondary role of the Jahn-Teller effect in observed structure distortions was established. A hypothesis of a spin crossover in the vicinity of the charge-ordering temperature is proposed that describes adequately both the obtained structural data and the results of measurements of the macroscopic magnetic and elastic properties of the studied compound as well as related materials with charge ordering.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Solid State Sciences},\\n\\tauthor = {Trotsenko, V. G. and Mikheykin, A. S. and Shirokov, V. B. and Razumnaya, A. G. and El Marssi, M. and Gorshunov, B. P. and Bush, A. A. and Torgashev, V. I.},\\n\\tmonth = oct,\\n\\tyear = {2017},\\n\\tkeywords = {Charge ordering, Correlated electron systems, Invar effect, Spin crossover},\\n\\tpages = {144--149},\\n}\\n\\n\",\"author_short\":[\"Trotsenko, V. G.\",\"Mikheykin, A. S.\",\"Shirokov, V. B.\",\"Razumnaya, A. G.\",\"El Marssi, M.\",\"Gorshunov, B. P.\",\"Bush, A. A.\",\"Torgashev, V. I.\"],\"key\":\"trotsenko_invar_2017\",\"id\":\"trotsenko_invar_2017\",\"bibbaseid\":\"trotsenko-mikheykin-shirokov-razumnaya-elmarssi-gorshunov-bush-torgashev-invareffectaccompanyingchargeorderinlatextrm025catextrm075mnotextrm3-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S1293255817305381\"},\"keyword\":[\"Charge ordering\",\"Correlated electron systems\",\"Invar effect\",\"Spin crossover\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Fast proton conduction in Cs$_{\\\\textrm{3}}$(HSO$_{\\\\textrm{4}}$)$_{\\\\textrm{2}}$(H$_{\\\\textrm{2}}$PO$_{\\\\textrm{4}}$) and Cs$_{\\\\textrm{4}}$(HSO$_{\\\\textrm{4}}$)$_{\\\\textrm{3}}$(H$_{\\\\textrm{2}}$PO$_{\\\\textrm{4}}$)\",\"volume\":\"305\",\"issn\":\"0167-2738\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0167273816307147\",\"doi\":\"10.1016/j.ssi.2017.04.017\",\"abstract\":\"X-ray powder diffraction studies were performed on Cs3(HSO4)2(H2PO4) and Cs4(HSO4)3(H2PO4) in the range 340–440K. For the both compounds a first order phase transition from the monoclinic C2/c phase to the mixture of cubic Pm-3m and tetragonal I41/amd superprotonic phases takes place at 408–414 and 412–414K respectively; the ratio between cubic and tetragonal depends on material and temperature. The tetragonal phase transforms to the cubic modification on heating and this transition is reversible.\",\"urldate\":\"2023-11-11\",\"journal\":\"Solid State Ionics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chernyshov\"],\"firstnames\":[\"D.\",\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Makarova\"],\"firstnames\":[\"I.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grebenev\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Komornikov\"],\"firstnames\":[\"V.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Selezneva\"],\"firstnames\":[\"E.\",\"V.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2017\",\"keywords\":\"Solid solutions, Phase transition, Superprotonics, XRPD\",\"pages\":\"30–35\",\"file\":\"ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\ZKIPJH5U\\\\§0167273816307147.html:text/html\",\"bibtex\":\"@article{mikheykin_fast_2017,\\n\\ttitle = {Fast proton conduction in {Cs}$_{\\\\textrm{3}}$({HSO}$_{\\\\textrm{4}}$)$_{\\\\textrm{2}}$({H}$_{\\\\textrm{2}}${PO}$_{\\\\textrm{4}}$) and {Cs}$_{\\\\textrm{4}}$({HSO}$_{\\\\textrm{4}}$)$_{\\\\textrm{3}}$({H}$_{\\\\textrm{2}}${PO}$_{\\\\textrm{4}}$)},\\n\\tvolume = {305},\\n\\tissn = {0167-2738},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0167273816307147},\\n\\tdoi = {10.1016/j.ssi.2017.04.017},\\n\\tabstract = {X-ray powder diffraction studies were performed on Cs3(HSO4)2(H2PO4) and Cs4(HSO4)3(H2PO4) in the range 340–440K. For the both compounds a first order phase transition from the monoclinic C2/c phase to the mixture of cubic Pm-3m and tetragonal I41/amd superprotonic phases takes place at 408–414 and 412–414K respectively; the ratio between cubic and tetragonal depends on material and temperature. The tetragonal phase transforms to the cubic modification on heating and this transition is reversible.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Solid State Ionics},\\n\\tauthor = {Mikheykin, A. S. and Chernyshov, D. Yu. and Makarova, I. P. and Grebenev, V. V. and Komornikov, V. A. and Selezneva, E. V.},\\n\\tmonth = jul,\\n\\tyear = {2017},\\n\\tkeywords = {Solid solutions, Phase transition, Superprotonics, XRPD},\\n\\tpages = {30--35},\\n\\tfile = {ScienceDirect Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\ZKIPJH5U\\\\\\\\S0167273816307147.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Mikheykin, A. S.\",\"Chernyshov, D. Y.\",\"Makarova, I. P.\",\"Grebenev, V. V.\",\"Komornikov, V. A.\",\"Selezneva, E. V.\"],\"key\":\"mikheykin_fast_2017\",\"id\":\"mikheykin_fast_2017\",\"bibbaseid\":\"mikheykin-chernyshov-makarova-grebenev-komornikov-selezneva-fastprotonconductionincstextrm3hsotextrm4textrm2htextrm2potextrm4andcstextrm4hsotextrm4textrm3htextrm2potextrm4-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0167273816307147\"},\"keyword\":[\"Solid solutions\",\"Phase transition\",\"Superprotonics\",\"XRPD\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Electrochemically synthesized Pt/TiO$_{\\\\textrm{2}}$-C catalysts for direct methanol fuel cell applications\",\"volume\":\"27\",\"issn\":\"0959-9436\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0959943617300214\",\"doi\":\"10.1016/j.mencom.2017.01.021\",\"abstract\":\"The Pt/TiO2-C catalysts with different TiO2 loadings have been prepared by electrochemical oxidation/dispersion, and their good catalytic activity in CO stripping and methanol electrooxidation reactions has been shown.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Mendeleev Communications\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"Alexandra\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Alexandrin\"],\"firstnames\":[\"Alexander\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Maslova\"],\"firstnames\":[\"Olga\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rakhmatullin\"],\"firstnames\":[\"Aydar\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\",\"V.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2017\",\"pages\":\"67–69\",\"bibtex\":\"@article{kuriganova_electrochemically_2017,\\n\\ttitle = {Electrochemically synthesized {Pt}/{TiO}$_{\\\\textrm{2}}$-{C} catalysts for direct methanol fuel cell applications},\\n\\tvolume = {27},\\n\\tissn = {0959-9436},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0959943617300214},\\n\\tdoi = {10.1016/j.mencom.2017.01.021},\\n\\tabstract = {The Pt/TiO2-C catalysts with different TiO2 loadings have been prepared by electrochemical oxidation/dispersion, and their good catalytic activity in CO stripping and methanol electrooxidation reactions has been shown.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Mendeleev Communications},\\n\\tauthor = {Kuriganova, Alexandra B. and Leontyev, Igor N. and Alexandrin, Alexander S. and Maslova, Olga A. and Rakhmatullin, Aydar I. and Smirnova, Nina V.},\\n\\tmonth = jan,\\n\\tyear = {2017},\\n\\tpages = {67--69},\\n}\\n\\n\",\"author_short\":[\"Kuriganova, A. B.\",\"Leontyev, I. N.\",\"Alexandrin, A. S.\",\"Maslova, O. A.\",\"Rakhmatullin, A. I.\",\"Smirnova, N. V.\"],\"key\":\"kuriganova_electrochemically_2017\",\"id\":\"kuriganova_electrochemically_2017\",\"bibbaseid\":\"kuriganova-leontyev-alexandrin-maslova-rakhmatullin-smirnova-electrochemicallysynthesizedpttiotextrm2ccatalystsfordirectmethanolfuelcellapplications-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0959943617300214\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"address\":\"Cham\",\"series\":\"Springer Proceedings in Physics\",\"title\":\"Crystal Structure, Phase and Elemental Composition and Chemical Bonding in Bi$_{\\\\textrm{1−{X}}}$A$_{\\\\textrm{{X}}}$FeO$_{\\\\textrm{3±{Y}}}$ Systems (A = Sr, Ca; 0 ≤X ≤ 1) from X-ray Diffraction, Mössbauer, and X-ray Photoelectron Spectra\",\"isbn\":\"978-3-319-56062-5\",\"doi\":\"10.1007/978-3-319-56062-5_13\",\"abstract\":\"An integrated study of samples of Bi1−xAxFeO3±y(A = Sr, Ca) systems for 0 ≤ x ≤ 1 (step 0.1) is performed using X-ray diffractionX-ray diffraction (XRD)(XRD), Mössbauer spectroscopy (MS), and X-ray photoelectron spectroscopyX-ray photoelectron spectroscopy (XPS)(XPS). Considerable deviations of actual elemental compositions from nominal ones in the samples of both systems are discovered. Both Fe3+ and Fe4+ ions are found to be present in the samples of the Bi1−xSrxFeO3±ysystem with x \\\\textgreater 0. No Fe4+ ions are discovered upon substitution of Bi3+ by Ca2+ in Bi1−xCaxFeO3±y, neither by Mössbauer spectroscopy, nor by XPS. Charge compensation in Bi1−xCaxFeO3±ytakes place mostly via creation of oxygen vacancies.\",\"language\":\"en\",\"booktitle\":\"Advanced Materials\",\"publisher\":\"Springer International Publishing\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kozakov\"],\"firstnames\":[\"A.\",\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kochur\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kubrin\"],\"firstnames\":[\"S.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Trotsenko\"],\"firstnames\":[\"V.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bush\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nikolskii\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]}],\"editor\":[{\"propositions\":[],\"lastnames\":[\"Parinov\"],\"firstnames\":[\"Ivan\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chang\"],\"firstnames\":[\"Shun-Hsyung\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Jani\"],\"firstnames\":[\"Muaffaq\",\"A.\"],\"suffixes\":[]}],\"year\":\"2017\",\"keywords\":\"Actual Elemental Composition, concentrationsConcentration, Mössbauer Spectroscopy, Octahedral Oxygen Environment, xCa xFeO\",\"pages\":\"145–153\",\"bibtex\":\"@inproceedings{kozakov_crystal_2017,\\n\\taddress = {Cham},\\n\\tseries = {Springer {Proceedings} in {Physics}},\\n\\ttitle = {Crystal {Structure}, {Phase} and {Elemental} {Composition} and {Chemical} {Bonding} in {Bi}$_{\\\\textrm{1−{X}}}${A}$_{\\\\textrm{{X}}}${FeO}$_{\\\\textrm{3±{Y}}}$ {Systems} ({A} = {Sr}, {Ca}; 0 ≤{X} ≤ 1) from {X}-ray {Diffraction}, {Mössbauer}, and {X}-ray {Photoelectron} {Spectra}},\\n\\tisbn = {978-3-319-56062-5},\\n\\tdoi = {10.1007/978-3-319-56062-5_13},\\n\\tabstract = {An integrated study of samples of Bi1−xAxFeO3±y(A = Sr, Ca) systems for 0 ≤ x ≤ 1 (step 0.1) is performed using X-ray diffractionX-ray diffraction (XRD)(XRD), Mössbauer spectroscopy (MS), and X-ray photoelectron spectroscopyX-ray photoelectron spectroscopy (XPS)(XPS). Considerable deviations of actual elemental compositions from nominal ones in the samples of both systems are discovered. Both Fe3+ and Fe4+ ions are found to be present in the samples of the Bi1−xSrxFeO3±ysystem with x {\\\\textgreater} 0. No Fe4+ ions are discovered upon substitution of Bi3+ by Ca2+ in Bi1−xCaxFeO3±y, neither by Mössbauer spectroscopy, nor by XPS. Charge compensation in Bi1−xCaxFeO3±ytakes place mostly via creation of oxygen vacancies.},\\n\\tlanguage = {en},\\n\\tbooktitle = {Advanced {Materials}},\\n\\tpublisher = {Springer International Publishing},\\n\\tauthor = {Kozakov, A. T. and Kochur, A. G. and Torgashev, V. I. and Kubrin, S. P. and Trotsenko, V. G. and Bush, A. A. and Nikolskii, A. V.},\\n\\teditor = {Parinov, Ivan A. and Chang, Shun-Hsyung and Jani, Muaffaq A.},\\n\\tyear = {2017},\\n\\tkeywords = {Actual Elemental Composition, concentrationsConcentration, Mössbauer Spectroscopy, Octahedral Oxygen Environment, xCa xFeO},\\n\\tpages = {145--153},\\n}\\n\\n\",\"author_short\":[\"Kozakov, A. T.\",\"Kochur, A. G.\",\"Torgashev, V. I.\",\"Kubrin, S. P.\",\"Trotsenko, V. G.\",\"Bush, A. A.\",\"Nikolskii, A. V.\"],\"editor_short\":[\"Parinov, I. A.\",\"Chang, S.\",\"Jani, M. A.\"],\"key\":\"kozakov_crystal_2017\",\"id\":\"kozakov_crystal_2017\",\"bibbaseid\":\"kozakov-kochur-torgashev-kubrin-trotsenko-bush-nikolskii-crystalstructurephaseandelementalcompositionandchemicalbondinginbitextrm1xatextrmxfeotextrm3ysystemsasrca0x1fromxraydiffractionmssbauerandxrayphotoelectronspectra-2017\",\"role\":\"author\",\"urls\":{},\"keyword\":[\"Actual Elemental Composition\",\"concentrationsConcentration\",\"Mössbauer Spectroscopy\",\"Octahedral Oxygen Environment\",\"xCa xFeO\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"Acoustic properties of BST0$_{\\\\textrm{8}}$ films tunable by bias electric field\",\"url\":\"https://ieeexplore.ieee.org/document/7819084?reload=true\",\"doi\":\"10.1109/Dynamics.2016.7819084\",\"abstract\":\"The effect of a bias electric field on the material coefficients of Ba0.8Sr0.2O3 (BST08) thin films was studied. The material constants are derived from piezoelectric effect equations by the linearization of nonlinear phenomenological state equations. The numerical results are obtained for the case of BST08 film with a misfit strain value equal to −4×10−3 located on a cubic substrate for the (001) cut plane in the electric field up to 5×107V/m applied along [100] direction in the film plane. The electromechanical coupling coefficient k11 reaches a maximum under applied electric field.\",\"urldate\":\"2023-11-11\",\"booktitle\":\"2016 Dynamics of Systems, Mechanisms and Machines (Dynamics)\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kalinchuck\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2016\",\"pages\":\"1–4\",\"bibtex\":\"@inproceedings{shirokov_acoustic_2016,\\n\\ttitle = {Acoustic properties of {BST0}$_{\\\\textrm{8}}$ films tunable by bias electric field},\\n\\turl = {https://ieeexplore.ieee.org/document/7819084?reload=true},\\n\\tdoi = {10.1109/Dynamics.2016.7819084},\\n\\tabstract = {The effect of a bias electric field on the material coefficients of Ba0.8Sr0.2O3 (BST08) thin films was studied. The material constants are derived from piezoelectric effect equations by the linearization of nonlinear phenomenological state equations. The numerical results are obtained for the case of BST08 film with a misfit strain value equal to −4×10−3 located on a cubic substrate for the (001) cut plane in the electric field up to 5×107V/m applied along [100] direction in the film plane. The electromechanical coupling coefficient k11 reaches a maximum under applied electric field.},\\n\\turldate = {2023-11-11},\\n\\tbooktitle = {2016 {Dynamics} of {Systems}, {Mechanisms} and {Machines} ({Dynamics})},\\n\\tauthor = {Shirokov, V. B and Kalinchuck, V. V. and Timoshenko, P. E. and Shirokov, V. B. and Timoshenko, P. E. and Yuzyuk, Yu. I.},\\n\\tmonth = nov,\\n\\tyear = {2016},\\n\\tpages = {1--4},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B\",\"Kalinchuck, V. V.\",\"Timoshenko, P. E.\",\"Shirokov, V. B.\",\"Timoshenko, P. E.\",\"Yuzyuk, Y. I.\"],\"key\":\"shirokov_acoustic_2016\",\"id\":\"shirokov_acoustic_2016\",\"bibbaseid\":\"shirokov-kalinchuck-timoshenko-shirokov-timoshenko-yuzyuk-acousticpropertiesofbst0textrm8filmstunablebybiaselectricfield-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://ieeexplore.ieee.org/document/7819084?reload=true\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Эффект поля в структуре металл - сегнетоэлектрик - полупроводник с использованием многослойного сегнетоэлектрика\",\"volume\":\"13\",\"issn\":\"2500-0640\",\"url\":\"https://elibrary.ru/item.asp?id=28843943\",\"doi\":\"10.23885/2500-0640-2017-13-1-18-24\",\"abstract\":\"Одной из важнейших концепций использования сегнетоэлектрических гетероструктур в микроэлектронике является энергонезависимая память (FeRAM), где в качестве подзатворного диэлектрика в полевом транзисторе используется сегнетоэлектрическая пленка. Вторым важным применением сегнетоэлектрических пленок является их использование при создании принципиально новых микроэлектромеханических устройств (МЕМС). Реализация МЕМС с использованием сегнетоэлектрических наноразмерных пленок в качестве активного элемента по своим параметрам в десятки раз будет превосходить существующие аналоги. В последние годы вопросам стабильности поляризованного состояния и динамики переключения поляризации придается большое значение. В данной работе впервые приведены результаты по исследованию эффекта поля в структуре металл - сегнетоэлектрик - полупроводник, где в качестве сегнетоэлектрика использованы многослойные сегнетоэлектрические слои. Использование многослойных сегнетоэлектрических гетероструктур приводит к самосогласованию поверхностных состояний на границах полупроводник - сегнетоэлектрик и сегнетоэлектрик - сегнетоэлектрик с переключаемой под действием внешнего поля спонтанной поляризацией. Это позволяет создать устойчивое поляризованное состояние с незначительной ее релаксацией.\",\"language\":\"ru\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Наука Юга России\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Стрюков\"],\"firstnames\":[\"Д.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бирюков\"],\"firstnames\":[\"С.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]}],\"year\":\"2017\",\"keywords\":\"Двумерные Напряжения, Двухслойные Сегнетоэлектрики, Сегнетоэлектрическая Пленка, Структура, Эффект Поля\",\"pages\":\"18–24\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\A5UM2STP\\\\\\\\Стрюков и др. - 2017 - Эффект Поля В Структуре Металл - Сегнетоэлектрик -.pdf:application/pdf\",\"bibtex\":\"@article{__2017-5,\\n\\ttitle = {Эффект поля в структуре металл - сегнетоэлектрик - полупроводник с использованием многослойного сегнетоэлектрика},\\n\\tvolume = {13},\\n\\tissn = {2500-0640},\\n\\turl = {https://elibrary.ru/item.asp?id=28843943},\\n\\tdoi = {10.23885/2500-0640-2017-13-1-18-24},\\n\\tabstract = {Одной из важнейших концепций использования сегнетоэлектрических гетероструктур в микроэлектронике является энергонезависимая память (FeRAM), где в качестве подзатворного диэлектрика в полевом транзисторе используется сегнетоэлектрическая пленка. Вторым важным применением сегнетоэлектрических пленок является их использование при создании принципиально новых микроэлектромеханических устройств (МЕМС). Реализация МЕМС с использованием сегнетоэлектрических наноразмерных пленок в качестве активного элемента по своим параметрам в десятки раз будет превосходить существующие аналоги. В последние годы вопросам стабильности поляризованного состояния и динамики переключения поляризации придается большое значение. В данной работе впервые приведены результаты по исследованию эффекта поля в структуре металл - сегнетоэлектрик - полупроводник, где в качестве сегнетоэлектрика использованы многослойные сегнетоэлектрические слои. Использование многослойных сегнетоэлектрических гетероструктур приводит к самосогласованию поверхностных состояний на границах полупроводник - сегнетоэлектрик и сегнетоэлектрик - сегнетоэлектрик с переключаемой под действием внешнего поля спонтанной поляризацией. Это позволяет создать устойчивое поляризованное состояние с незначительной ее релаксацией.},\\n\\tlanguage = {ru},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Наука Юга России},\\n\\tauthor = {Стрюков, Д. В. and Мухортов, В. М. and Бирюков, С. В. and Головко, Ю. И.},\\n\\tyear = {2017},\\n\\tkeywords = {Двумерные Напряжения, Двухслойные Сегнетоэлектрики, Сегнетоэлектрическая Пленка, Структура, Эффект Поля},\\n\\tpages = {18--24},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\A5UM2STP\\\\\\\\Стрюков и др. - 2017 - Эффект Поля В Структуре Металл - Сегнетоэлектрик -.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Стрюков, Д. В.\",\"Мухортов, В. М.\",\"Бирюков, С. В.\",\"Головко, Ю. И.\"],\"key\":\"__2017-5\",\"id\":\"__2017-5\",\"bibbaseid\":\"-----2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=28843943\"},\"keyword\":[\"Двумерные Напряжения\",\"Двухслойные Сегнетоэлектрики\",\"Сегнетоэлектрическая Пленка\",\"Структура\",\"Эффект Поля\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Экспериментальное и теоретическое исследование оптических антенн на основе наностержней ZnO покрытых тонкой пленкой серебра\",\"issn\":\"0033-8494\",\"url\":\"https://www.libnauka.ru/item.php?doi=10.7868/S0033849417110055\",\"doi\":\"10.7868/S0033849417110055\",\"language\":\"ru\",\"number\":\"12\",\"urldate\":\"2023-11-11\",\"journal\":\"Радиотехника и электроника\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лерер\"],\"firstnames\":[\"А.М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головачева\"],\"firstnames\":[\"Е.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"В.\",\"Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Цветянский\"],\"firstnames\":[\"Е.\",\"А.\"],\"suffixes\":[]}],\"year\":\"2017\",\"pages\":\"1173–1181\",\"bibtex\":\"@article{__2017-6,\\n\\ttitle = {Экспериментальное и теоретическое исследование оптических антенн на основе наностержней {ZnO} покрытых тонкой пленкой серебра},\\n\\tissn = {0033-8494},\\n\\turl = {https://www.libnauka.ru/item.php?doi=10.7868/S0033849417110055},\\n\\tdoi = {10.7868/S0033849417110055},\\n\\tlanguage = {ru},\\n\\tnumber = {12},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Радиотехника и электроника},\\n\\tauthor = {Кайдашев, Е. М. and Лерер, А.М. and Головачева, Е. В. and Кайдашев, В. Е. and Лянгузов, Н.В. and Цветянский, Е. А.},\\n\\tyear = {2017},\\n\\tpages = {1173--1181},\\n}\\n\\n\",\"author_short\":[\"Кайдашев, Е. М.\",\"Лерер, А.\",\"Головачева, Е. В.\",\"Кайдашев, В. Е.\",\"Лянгузов, Н.\",\"Цветянский, Е. А.\"],\"key\":\"__2017-6\",\"id\":\"__2017-6\",\"bibbaseid\":\"------zno-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.libnauka.ru/item.php?doi=10.7868/S0033849417110055\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Структура, динамика решетки и диэлектрические характеристики пленок Sr$_{\\\\textrm{0.5}}$Ba$_{\\\\textrm{0.5}}$Nb$_{\\\\textrm{2}}$O$_{\\\\textrm{6}}$\",\"volume\":\"59\",\"issn\":\"0367-3294\",\"url\":\"https://journals.ioffe.ru/articles/44376\",\"doi\":\"10.21883/FTT.2017.05.44376.382\",\"abstract\":\"Методом высокочастотного напыления в атмосфере кислорода получены пленки твердого раствора Sr 0.5 Ba 0.5 Nb 2 O 6 на подложке (111)Pt/(001)Si. Изучены их деполяризованные спектры комбинационного рассеяния света, структура и диэлектрические характеристики в широком диапазоне температур. Установлено, что пленки однофазны, обладают структурой тетрагональной вольфрамовой бронзы, имеют ярко выраженную аксиальную текстуру с осью 001, направленной перпендикулярно поверхности подложки. Показано, что в интервале температур 300-425 K в материале пленки происходит размытый фазовый переход в состояние сегнетоэлектрика-релаксора. Обсуждаются возможные причины выявленных закономерностей. Работа выполнена в рамках реализации государственного задания на 2016 г N 007-01114-16 ПР (проект N 0256-2014-0002) и гранта РФФИ N 16-32-60095 мол\\\\_а\\\\_дк. DOI: 10.21883/FTT.2017.05.44376.382\",\"language\":\"ru\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Павленко\"],\"firstnames\":[\"А.В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Захарченко\"],\"firstnames\":[\"И.Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Анохин\"],\"firstnames\":[\"А.С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Куприна\"],\"firstnames\":[\"Ю.А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Киселева\"],\"firstnames\":[\"Л.И\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.И.\"],\"suffixes\":[]}],\"year\":\"2017\",\"pages\":\"888\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\BGRS77V9\\\\\\\\Павленко и др. - 2017 - Структура, динамика решетки и диэлектрические хара.pdf:application/pdf\",\"bibtex\":\"@article{__2017-7,\\n\\ttitle = {Структура, динамика решетки и диэлектрические характеристики пленок {Sr}$_{\\\\textrm{0.5}}${Ba}$_{\\\\textrm{0.5}}${Nb}$_{\\\\textrm{2}}${O}$_{\\\\textrm{6}}$},\\n\\tvolume = {59},\\n\\tissn = {0367-3294},\\n\\turl = {https://journals.ioffe.ru/articles/44376},\\n\\tdoi = {10.21883/FTT.2017.05.44376.382},\\n\\tabstract = {Методом высокочастотного напыления в атмосфере кислорода получены пленки твердого раствора Sr\\n              0.5\\n              Ba\\n              0.5\\n              Nb\\n              2\\n              O\\n              6\\n              на подложке (111)Pt/(001)Si. Изучены их деполяризованные спектры комбинационного рассеяния света, структура и диэлектрические характеристики в широком диапазоне температур. Установлено, что пленки однофазны, обладают структурой тетрагональной вольфрамовой бронзы, имеют ярко выраженную аксиальную текстуру с осью 001, направленной перпендикулярно поверхности подложки. Показано, что в интервале температур 300-425 K в материале пленки происходит размытый фазовый переход в состояние сегнетоэлектрика-релаксора. Обсуждаются возможные причины выявленных закономерностей. Работа выполнена в рамках реализации государственного задания на 2016 г N 007-01114-16 ПР (проект N 0256-2014-0002) и гранта РФФИ N 16-32-60095 мол{\\\\textbackslash}\\\\_а{\\\\textbackslash}\\\\_дк. DOI: 10.21883/FTT.2017.05.44376.382},\\n\\tlanguage = {ru},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Павленко, А.В. and Захарченко, И.Н. and Анохин, А.С. and Куприна, Ю.А. and Киселева, Л.И and Юзюк, Ю.И.},\\n\\tyear = {2017},\\n\\tpages = {888},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\BGRS77V9\\\\\\\\Павленко и др. - 2017 - Структура, динамика решетки и диэлектрические хара.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Павленко, А.\",\"Захарченко, И.\",\"Анохин, А.\",\"Куприна, Ю.\",\"Киселева, Л.\",\"Юзюк, Ю.\"],\"key\":\"__2017-7\",\"id\":\"__2017-7\",\"bibbaseid\":\"------srtextrm05batextrm05nbtextrm2otextrm6-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/44376\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Получение, структура и диэлектрические свойства керамики и тонких поликристаллических пленок PbMg$_{\\\\textrm{1/3}}$Nb$_{\\\\textrm{2/3}}$O$_{\\\\textrm{3}}$ на подложке Si(001)\",\"volume\":\"13\",\"issn\":\"2500-0640\",\"url\":\"https://elibrary.ru/item.asp?id=29946411\",\"doi\":\"10.23885/2500-0640-2017-13-3-27-33\",\"abstract\":\"Методом газоразрядного RF-напыления в атмосфере чистого кислорода осуществлено напыление пленок сегнетоэлектрика-релаксора PbMg1/3Nb2/3O3 (PMN) на подложки (001)Si (p-тип). PMN-пленки являются поликристаллическими с параметрами ячейки, близкими к объемному материалу PMN. Следов примесных фаз в обоих объектах не выявлено. Количественный анализ характеристического рентгеновского спектра образцов показал, что соотношение катионного состава по Pb и Nb в пленке соответствует составу распыляемой мишени. Проведены измерения температурно-частотных зависимостей относительной диэлектрической проницаемости (ε/ε0) и тангенса угла диэлектрических потерь (tg δ) керамики PMN. При комнатной температуре керамике свойственны высокие значения ε/ε0 ≈ 5500 и низкие tg δ ≈ 0,02, при этом дисперсия ε/ε0 в исследуемом диапазоне f отсутствовала, а температура Бёрнса составила ≈300 °С. При электронно-микроскопическом исследовании поверхности и скола гетероструктуры PMN/Si установлено, что пленка однофазная, поликристаллическая с характерным размером кристаллитов 50... 70 нм, при этом следов присутствия переходного слоя оксида кремния на границе раздела пленка - подложка не выявлено. Проведены исследования вольт-фарадных характеристик гетероструктуры PMN/Si. Обсуждаются причины выявленных аномалий.\",\"language\":\"ru\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Наука Юга России\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Павленко\"],\"firstnames\":[\"А.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Новиковский\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Смотраков\"],\"firstnames\":[\"В.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ковтун\"],\"firstnames\":[\"А.\",\"П.\"],\"suffixes\":[]}],\"year\":\"2017\",\"keywords\":\"Диэлектрическая Проницаемость, Магнониобат Свинца, Релаксор, Тонкие Пленки\",\"pages\":\"27–33\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\K4J6BNEW\\\\\\\\Павленко и др. - 2017 - ПОЛУЧЕНИЕ, СТРУКТУРА И ДИЭЛЕКТРИЧЕСКИЕ СВОЙСТВА КЕ.pdf:application/pdf\",\"bibtex\":\"@article{__2017-8,\\n\\ttitle = {Получение, структура и диэлектрические свойства керамики и тонких поликристаллических пленок {PbMg}$_{\\\\textrm{1/3}}${Nb}$_{\\\\textrm{2/3}}${O}$_{\\\\textrm{3}}$ на подложке {Si}(001)},\\n\\tvolume = {13},\\n\\tissn = {2500-0640},\\n\\turl = {https://elibrary.ru/item.asp?id=29946411},\\n\\tdoi = {10.23885/2500-0640-2017-13-3-27-33},\\n\\tabstract = {Методом газоразрядного RF-напыления в атмосфере чистого кислорода осуществлено напыление пленок сегнетоэлектрика-релаксора PbMg1/3Nb2/3O3 (PMN) на подложки (001)Si (p-тип). PMN-пленки являются поликристаллическими с параметрами ячейки, близкими к объемному материалу PMN. Следов примесных фаз в обоих объектах не выявлено. Количественный анализ характеристического рентгеновского спектра образцов показал, что соотношение катионного состава по Pb и Nb в пленке соответствует составу распыляемой мишени. Проведены измерения температурно-частотных зависимостей относительной диэлектрической проницаемости (ε/ε0) и тангенса угла диэлектрических потерь (tg δ) керамики PMN. При комнатной температуре керамике свойственны высокие значения ε/ε0 ≈ 5500 и низкие tg δ ≈ 0,02, при этом дисперсия ε/ε0 в исследуемом диапазоне f отсутствовала, а температура Бёрнса составила ≈300 °С. При электронно-микроскопическом исследовании поверхности и скола гетероструктуры PMN/Si установлено, что пленка однофазная, поликристаллическая с характерным размером кристаллитов 50... 70 нм, при этом следов присутствия переходного слоя оксида кремния на границе раздела пленка - подложка не выявлено. Проведены исследования вольт-фарадных характеристик гетероструктуры PMN/Si. Обсуждаются причины выявленных аномалий.},\\n\\tlanguage = {ru},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Наука Юга России},\\n\\tauthor = {Павленко, А. В. and Лянгузов, Н. В. and Новиковский, Н. В. and Смотраков, В. Г. and Ковтун, А. П.},\\n\\tyear = {2017},\\n\\tkeywords = {Диэлектрическая Проницаемость, Магнониобат Свинца, Релаксор, Тонкие Пленки},\\n\\tpages = {27--33},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\K4J6BNEW\\\\\\\\Павленко и др. - 2017 - ПОЛУЧЕНИЕ, СТРУКТУРА И ДИЭЛЕКТРИЧЕСКИЕ СВОЙСТВА КЕ.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Павленко, А. В.\",\"Лянгузов, Н. В.\",\"Новиковский, Н. В.\",\"Смотраков, В. Г.\",\"Ковтун, А. П.\"],\"key\":\"__2017-8\",\"id\":\"__2017-8\",\"bibbaseid\":\"-----pbmgtextrm13nbtextrm23otextrm3si001-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=29946411\"},\"keyword\":[\"Диэлектрическая Проницаемость\",\"Магнониобат Свинца\",\"Релаксор\",\"Тонкие Пленки\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"Особенности фазового перехода в сегнетоэлектрической сверхрешетке BaTiO$_{\\\\textrm{3}}$/SrTiO$_{\\\\textrm{3}}$\",\"url\":\"https://elibrary.ru/item.asp?id=29647718\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"publisher\":\"Российский государственный педагогический университет им. А. И. Герцена\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Разумная\"],\"firstnames\":[\"А.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Горьковая\"],\"firstnames\":[\"Е.\",\"Д.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Тихонов\"],\"firstnames\":[\"Ю.\",\"А.\"],\"suffixes\":[]}],\"year\":\"2017\",\"keywords\":\"⛔ No DOI found\",\"bibtex\":\"@inproceedings{__2017-9,\\n\\ttitle = {Особенности фазового перехода в сегнетоэлектрической сверхрешетке {BaTiO}$_{\\\\textrm{3}}$/{SrTiO}$_{\\\\textrm{3}}$},\\n\\turl = {https://elibrary.ru/item.asp?id=29647718},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tpublisher = {Российский государственный педагогический университет им. А. И. Герцена},\\n\\tauthor = {Разумная, А. Г. and Горьковая, Е. Д. and Тихонов, Ю. А.},\\n\\tyear = {2017},\\n\\tkeywords = {⛔ No DOI found},\\n}\\n\\n\",\"author_short\":[\"Разумная, А. Г.\",\"Горьковая, Е. Д.\",\"Тихонов, Ю. А.\"],\"key\":\"__2017-9\",\"id\":\"__2017-9\",\"bibbaseid\":\"---batiotextrm3srtiotextrm3-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=29647718\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"Оптические Свойства Тонких Пленок BSn50\",\"url\":\"https://elibrary.ru/item.asp?id=29401602\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"publisher\":\"Российский государственный педагогический университет им. А. И. Герцена\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Павленко\"],\"firstnames\":[\"А.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Михейкин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Изюмский\"],\"firstnames\":[\"К.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ревинский\"],\"firstnames\":[\"Ю.\",\"В.\"],\"suffixes\":[]}],\"year\":\"2017\",\"keywords\":\"⛔ No DOI found\",\"bibtex\":\"@inproceedings{__2017-10,\\n\\ttitle = {Оптические Свойства Тонких Пленок {BSn50}},\\n\\turl = {https://elibrary.ru/item.asp?id=29401602},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tpublisher = {Российский государственный педагогический университет им. А. И. Герцена},\\n\\tauthor = {Широков, В. Б. and Павленко, А. В. and Михейкин, А. С. and Изюмский, К. С. and Ревинский, Ю. В.},\\n\\tyear = {2017},\\n\\tkeywords = {⛔ No DOI found},\\n}\\n\\n\",\"author_short\":[\"Широков, В. Б.\",\"Павленко, А. В.\",\"Михейкин, А. С.\",\"Изюмский, К. С.\",\"Ревинский, Ю. В.\"],\"key\":\"__2017-10\",\"id\":\"__2017-10\",\"bibbaseid\":\"-----bsn50-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=29401602\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"Многослойные структуры мультиферроик-сегнетоэлектрик: КРС исследования\",\"shorttitle\":\"Многослойные Структуры Мультиферроик-Сегнетоэлектрик\",\"url\":\"https://elibrary.ru/item.asp?id=29647696\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"publisher\":\"Российский государственный педагогический университет им. А. И. Герцена\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Анохин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Разумная\"],\"firstnames\":[\"А.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]}],\"year\":\"2017\",\"keywords\":\"⛔ No DOI found\",\"bibtex\":\"@inproceedings{__2017-11,\\n\\ttitle = {Многослойные структуры мультиферроик-сегнетоэлектрик: КРС исследования},\\n\\tshorttitle = {Многослойные Структуры Мультиферроик-Сегнетоэлектрик},\\n\\turl = {https://elibrary.ru/item.asp?id=29647696},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tpublisher = {Российский государственный педагогический университет им. А. И. Герцена},\\n\\tauthor = {Анохин, А. С. and Разумная, А. Г. and Головко, Ю. И. and Мухортов, В. М.},\\n\\tyear = {2017},\\n\\tkeywords = {⛔ No DOI found},\\n}\\n\\n\",\"author_short\":[\"Анохин, А. С.\",\"Разумная, А. Г.\",\"Головко, Ю. И.\",\"Мухортов, В. М.\"],\"key\":\"__2017-11\",\"id\":\"__2017-11\",\"bibbaseid\":\"-----2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=29647696\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"Магнитодиэлектрические свойства керамики LSMO/GeO$_{\\\\textrm{2}}$\",\"url\":\"https://elibrary.ru/item.asp?id=29647737\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"publisher\":\"Российский государственный педагогический университет им. А. И. Герцена\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Кабиров\"],\"firstnames\":[\"Ю.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гавриляченко\"],\"firstnames\":[\"В.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Богатин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Яценко\"],\"firstnames\":[\"В.\",\"К.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Пруцакова\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Чебанова\"],\"firstnames\":[\"Е.\",\"В.\"],\"suffixes\":[]}],\"year\":\"2017\",\"keywords\":\"⛔ No DOI found\",\"bibtex\":\"@inproceedings{__2017-12,\\n\\ttitle = {Магнитодиэлектрические свойства керамики {LSMO}/{GeO}$_{\\\\textrm{2}}$},\\n\\turl = {https://elibrary.ru/item.asp?id=29647737},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tpublisher = {Российский государственный педагогический университет им. А. И. Герцена},\\n\\tauthor = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Богатин, А. С. and Яценко, В. К. and Пруцакова, Н. В. and Чебанова, Е. В.},\\n\\tyear = {2017},\\n\\tkeywords = {⛔ No DOI found},\\n}\\n\\n\",\"author_short\":[\"Кабиров, Ю. В.\",\"Гавриляченко, В. Г.\",\"Богатин, А. С.\",\"Яценко, В. К.\",\"Пруцакова, Н. В.\",\"Чебанова, Е. В.\"],\"key\":\"__2017-12\",\"id\":\"__2017-12\",\"bibbaseid\":\"------lsmogeotextrm2-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=29647737\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Динамика решетки в пленках ниобата бария-стронция <i>Т </i>= 300-700 К\",\"volume\":\"13\",\"issn\":\"2500-0640\",\"url\":\"https://elibrary.ru/item.asp?id=29760083\",\"doi\":\"10.23885/2500-0640-2017-13-2-21-28\",\"abstract\":\"Методом газоразрядного RF-напыления в атмосфере чистого кислорода осуществлено напыление пленки твердого раствора сегнетоэлектрика-релаксора Ba0,5Sr0,5Nb2O6 (BSN-50) на предварительно подготовленную подложку (111)Pt/(001)Si. Пленке BSN-50 свойственна аксиальная текстура, основные элементы (Ba, Sr, Nb) по ее толщине распределены равномерно, а количественный анализ характеристического рентгеновского спектра показал, что соотношение катионного состава соответствует составу BSN-50. При исследовании температурных зависимостей относительной диэлектрической проницаемости (ε′/ε0) и остаточной поляризации (PR) гетероструктуры Al/BSN-50/Pt/Si установлено, что фазовый переход из сегнетоэлектрической в параэлектрическую фазу достаточно сильно размыт (ширина максимума ε′/ε0(Тm) на полувысоте ΔT = 263 K) и происходит при температуре ~427 К, намного превышающей температуру максимума диэлектрической проницаемости Tm = 334 K... Методом газоразрядного RF-напыления в атмосфере чистого кислорода осуществлено напыление пленки твердого раствора сегнетоэлектрика-релаксора Ba0,5Sr0,5Nb2O6 (BSN-50) на предварительно подготовленную подложку (111)Pt/(001)Si. Пленке BSN-50 свойственна аксиальная текстура, основные элементы (Ba, Sr, Nb) по ее толщине распределены равномерно, а количественный анализ характеристического рентгеновского спектра показал, что соотношение катионного состава соответствует составу BSN-50. При исследовании температурных зависимостей относительной диэлектрической проницаемости (ε′/ε0) и остаточной поляризации (PR) гетероструктуры Al/BSN-50/Pt/Si установлено, что фазовый переход из сегнетоэлектрической в параэлектрическую фазу достаточно сильно размыт (ширина максимума ε′/ε0(Тm) на полувысоте ΔT = 263 K) и происходит при температуре ~427 К, намного превышающей температуру максимума диэлектрической проницаемости Tm = 334 K. В диапазоне температур 300-700 K методом спектроскопии комбинационного рассеяния света изучена динамика решетки пленки BSN-50. Наибольший вклад в интенсивность спектра пленки BSN вносят три широкие полосы в районе 230 cm-1, 630 cm-1 и 850 cm-1, каждая из которых состоит из набора линий (всего 13 мод). Температурная зависимость частоты и полуширины полосы 630 cm-1 в спектре комбинационного рассеяния пленки BSN показывают четкую аномалию при сегнетоэлектрическом фазовом переходе.\",\"language\":\"ru\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Наука Юга России\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Анохин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Павленко\"],\"firstnames\":[\"А.\",\"В.\"],\"suffixes\":[]}],\"year\":\"2017\",\"keywords\":\"Диэлектрическая Проницаемость, Пленки, Спектроскопия Крс\",\"pages\":\"21–28\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\TM7MF7DI\\\\\\\\Анохин и др. - 2017 - ДИНАМИКА РЕШЕТКИ В ПЛЕНКАХ НИОБАТА БАРИЯ - СТРОНЦИ.pdf:application/pdf\",\"bibtex\":\"@article{__2017-13,\\n\\ttitle = {Динамика решетки в пленках ниобата бария-стронция \\\\textit{Т }= 300-700 К},\\n\\tvolume = {13},\\n\\tissn = {2500-0640},\\n\\turl = {https://elibrary.ru/item.asp?id=29760083},\\n\\tdoi = {10.23885/2500-0640-2017-13-2-21-28},\\n\\tabstract = {Методом газоразрядного RF-напыления в атмосфере чистого кислорода осуществлено напыление пленки твердого раствора сегнетоэлектрика-релаксора Ba0,5Sr0,5Nb2O6 (BSN-50) на предварительно подготовленную подложку (111)Pt/(001)Si. Пленке BSN-50 свойственна аксиальная текстура, основные элементы (Ba, Sr, Nb) по ее толщине распределены равномерно, а количественный анализ характеристического рентгеновского спектра показал, что соотношение катионного состава соответствует составу BSN-50. При исследовании температурных зависимостей относительной диэлектрической проницаемости (ε′/ε0) и остаточной поляризации (PR) гетероструктуры Al/BSN-50/Pt/Si установлено, что фазовый переход из сегнетоэлектрической в параэлектрическую фазу достаточно сильно размыт (ширина максимума ε′/ε0(Тm) на полувысоте ΔT = 263 K) и происходит при температуре {\\\\textasciitilde}427 К, намного превышающей температуру максимума диэлектрической проницаемости Tm = 334 K...\\n\\nМетодом газоразрядного RF-напыления в атмосфере чистого кислорода осуществлено напыление пленки твердого раствора сегнетоэлектрика-релаксора Ba0,5Sr0,5Nb2O6 (BSN-50) на предварительно подготовленную подложку (111)Pt/(001)Si. Пленке BSN-50 свойственна аксиальная текстура, основные элементы (Ba, Sr, Nb) по ее толщине распределены равномерно, а количественный анализ характеристического рентгеновского спектра показал, что соотношение катионного состава соответствует составу BSN-50. При исследовании температурных зависимостей относительной диэлектрической проницаемости (ε′/ε0) и остаточной поляризации (PR) гетероструктуры Al/BSN-50/Pt/Si установлено, что фазовый переход из сегнетоэлектрической в параэлектрическую фазу достаточно сильно размыт (ширина максимума ε′/ε0(Тm) на полувысоте ΔT = 263 K) и происходит при температуре {\\\\textasciitilde}427 К, намного превышающей температуру максимума диэлектрической проницаемости Tm = 334 K. В диапазоне температур 300-700 K методом спектроскопии комбинационного рассеяния света изучена динамика решетки пленки BSN-50. Наибольший вклад в интенсивность спектра пленки BSN вносят три широкие полосы в районе 230 cm-1, 630 cm-1 и 850 cm-1, каждая из которых состоит из набора линий (всего 13 мод). Температурная зависимость частоты и полуширины полосы 630 cm-1 в спектре комбинационного рассеяния пленки BSN показывают четкую аномалию при сегнетоэлектрическом фазовом переходе.},\\n\\tlanguage = {ru},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Наука Юга России},\\n\\tauthor = {Анохин, А. С. and Лянгузов, Н. В. and Павленко, А. В.},\\n\\tyear = {2017},\\n\\tkeywords = {Диэлектрическая Проницаемость, Пленки, Спектроскопия Крс},\\n\\tpages = {21--28},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\TM7MF7DI\\\\\\\\Анохин и др. - 2017 - ДИНАМИКА РЕШЕТКИ В ПЛЕНКАХ НИОБАТА БАРИЯ - СТРОНЦИ.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Анохин, А. С.\",\"Лянгузов, Н. В.\",\"Павленко, А. В.\"],\"key\":\"__2017-13\",\"id\":\"__2017-13\",\"bibbaseid\":\"---ii300700-2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=29760083\"},\"keyword\":[\"Диэлектрическая Проницаемость\",\"Пленки\",\"Спектроскопия Крс\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Dynamics of field-induced polarization reversal in thin strained perovskite ferroelectric films with <i>с</i>-oriented polarization\",\"volume\":\"91\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.91.144110\",\"doi\":\"10.1103/PhysRevB.91.144110\",\"abstract\":\"The field-induced polarization reversal in the c-oriented ferroelectric phase of strained perovskite film has been studied. We show that in addition to the conventional longitudinal switching mechanism, when the c-oriented polarization vector changes its modulus, the longitudinal-transversal and transversal mechanisms when the perpendicular component of polarization is dynamically admixed are possible. The latter process can occur either via the straight-abrupt or initially continues polarization turnover scenario. We specified the obtained results for the case of PbTiO3 and BaTiO3 ferroelectrics and propose the experimental methods for their investigation.\",\"number\":\"14\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Baudry\"],\"firstnames\":[\"Laurent\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Luk'yanchuk\"],\"firstnames\":[\"Igor\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"Anna\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2015\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"144110\",\"file\":\"Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\TC6IA8BZ\\\\\\\\Baudry и др. - 2015 - Dynamics of field-induced polarization reversal in.pdf:application/pdf\",\"bibtex\":\"@article{baudry_dynamics_2015,\\n\\ttitle = {Dynamics of field-induced polarization reversal in thin strained perovskite ferroelectric films with \\\\textit{с}-oriented polarization},\\n\\tvolume = {91},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.91.144110},\\n\\tdoi = {10.1103/PhysRevB.91.144110},\\n\\tabstract = {The field-induced polarization reversal in the c-oriented ferroelectric phase of strained perovskite film has been studied. We show that in addition to the conventional longitudinal switching mechanism, when the c-oriented polarization vector changes its modulus, the longitudinal-transversal and transversal mechanisms when the perpendicular component of polarization is dynamically admixed are possible. The latter process can occur either via the straight-abrupt or initially continues polarization turnover scenario. We specified the obtained results for the case of PbTiO3 and BaTiO3 ferroelectrics and propose the experimental methods for their investigation.},\\n\\tnumber = {14},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Baudry, Laurent and Luk'yanchuk, Igor A. and Razumnaya, Anna},\\n\\tmonth = apr,\\n\\tyear = {2015},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {144110},\\n\\tfile = {Отправленная версия:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\TC6IA8BZ\\\\\\\\Baudry и др. - 2015 - Dynamics of field-induced polarization reversal in.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Baudry, L.\",\"Luk'yanchuk, I. A.\",\"Razumnaya, A.\"],\"key\":\"baudry_dynamics_2015\",\"id\":\"baudry_dynamics_2015\",\"bibbaseid\":\"baudry-lukyanchuk-razumnaya-dynamicsoffieldinducedpolarizationreversalinthinstrainedperovskiteferroelectricfilmswithiiorientedpolarization-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.91.144110\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Вынужденный пироэффект в планарном поле\",\"volume\":\"59\",\"issn\":\"0367-3294\",\"url\":\"https://journals.ioffe.ru/articles/44377\",\"doi\":\"10.21883/FTT.2017.05.44377.397\",\"abstract\":\"Исследованы действие вынужденной деформации и влияние планарного электрического поля на основное состояние сегнетоэлектрических тонких пленок Ba0.7Sr0.3O3, осажденных на (001)-ориентированные кубические подложки. Для значений вынужденной деформации, соответствующих различным основным состояниям, построена зависимость пироэлектрического коэффициента от величины электрического поля Ex в плоскости пленки. В областях, где пленка может работать в режиме диэлектрического болометра, наблюдается значение поля, при котором пирокоэффициент достигает экстремального значения. Существует значение вынужденной деформации, при котором пироэффект проявляется наиболее ярко. Работа выполнена за счет средств Российского научного фонда (грант N 14-12-00258). DOI: 10.21883/FTT.2017.05.44377.397\",\"language\":\"ru\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Разумная\"],\"firstnames\":[\"А.Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.И.\"],\"suffixes\":[]}],\"year\":\"2017\",\"pages\":\"892\",\"file\":\"Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\WFDZMDZ3\\\\\\\\Широков и др. - 2017 - Вынужденный пироэффект в планарном поле.pdf:application/pdf\",\"bibtex\":\"@article{__2017-14,\\n\\ttitle = {Вынужденный пироэффект в планарном поле},\\n\\tvolume = {59},\\n\\tissn = {0367-3294},\\n\\turl = {https://journals.ioffe.ru/articles/44377},\\n\\tdoi = {10.21883/FTT.2017.05.44377.397},\\n\\tabstract = {Исследованы действие вынужденной деформации и влияние планарного электрического поля на основное состояние сегнетоэлектрических тонких пленок Ba0.7Sr0.3O3, осажденных на (001)-ориентированные кубические подложки. Для значений вынужденной деформации, соответствующих различным основным состояниям, построена зависимость пироэлектрического коэффициента от величины электрического поля Ex в плоскости пленки. В областях, где пленка может работать в режиме диэлектрического болометра, наблюдается значение поля, при котором пирокоэффициент достигает экстремального значения. Существует значение вынужденной деформации, при котором пироэффект проявляется наиболее ярко. Работа выполнена за счет средств Российского научного фонда (грант N 14-12-00258). DOI: 10.21883/FTT.2017.05.44377.397},\\n\\tlanguage = {ru},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Широков, В.Б. and Разумная, А.Г. and Юзюк, Ю.И.},\\n\\tyear = {2017},\\n\\tpages = {892},\\n\\tfile = {Полный текст:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\WFDZMDZ3\\\\\\\\Широков и др. - 2017 - Вынужденный пироэффект в планарном поле.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Широков, В.\",\"Разумная, А.\",\"Юзюк, Ю.\"],\"key\":\"__2017-14\",\"id\":\"__2017-14\",\"bibbaseid\":\"----2017\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/44377\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":8,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Theory of the formation of P$_{\\\\textrm{4{\\\\textless}sub{\\\\textgreater}1}}$32\\\\textless/sub\\\\textgreater(P$_{\\\\textrm{4{\\\\textless}sub{\\\\textgreater}3}}$32\\\\textless/sub\\\\textgreater)-phase spinels\",\"volume\":\"61\",\"issn\":\"1562-689X\",\"url\":\"https://doi.org/10.1134/S1063774516020280\",\"doi\":\"10.1134/S1063774516020280\",\"abstract\":\"A group-theoretical, thermodynamic, and structural study of the formation of P4132(P4332) spinel modification has been performed. In particular, the occurrence of unique hyper-kagome atomic order is analyzed. The critical order parameter inducing a phase transition is established. It is shown that the calculated structure of the low-symmetry P4132(P4332) phase is formed as a result of displacements of atoms of all types and due to the cation and anion ordering. The problem of the occurrence of unique hyper-kagome atomic order in the structures of P4132(P4332) spinel modifications is considered theoretically. It is proven within the Landau theory of phase transitions that the P4132(P4332) phase can be formed from the high-symmetry Fd3m phase with an ideal spinel structure only as a result of first-order phase transition. Therefore, the formation of hyper-kagome sublattice in the P4132(P4332) phase is accompanied by a significant transformation of the spinel structure.\",\"language\":\"en\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Crystallography Reports\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"M.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2016\",\"keywords\":\"Crystallography Report, Ible Representation, Multicritical Point, Spinel Structure, Unusual Physical Property\",\"pages\":\"159–169\",\"bibtex\":\"@article{talanov_theory_2016,\\n\\ttitle = {Theory of the formation of {P}$_{\\\\textrm{4{\\\\textless}sub{\\\\textgreater}1}}$32{\\\\textless}/sub{\\\\textgreater}({P}$_{\\\\textrm{4{\\\\textless}sub{\\\\textgreater}3}}$32{\\\\textless}/sub{\\\\textgreater})-phase spinels},\\n\\tvolume = {61},\\n\\tissn = {1562-689X},\\n\\turl = {https://doi.org/10.1134/S1063774516020280},\\n\\tdoi = {10.1134/S1063774516020280},\\n\\tabstract = {A group-theoretical, thermodynamic, and structural study of the formation of P4132(P4332) spinel modification has been performed. In particular, the occurrence of unique hyper-kagome atomic order is analyzed. The critical order parameter inducing a phase transition is established. It is shown that the calculated structure of the low-symmetry P4132(P4332) phase is formed as a result of displacements of atoms of all types and due to the cation and anion ordering. The problem of the occurrence of unique hyper-kagome atomic order in the structures of P4132(P4332) spinel modifications is considered theoretically. It is proven within the Landau theory of phase transitions that the P4132(P4332) phase can be formed from the high-symmetry Fd3m phase with an ideal spinel structure only as a result of first-order phase transition. Therefore, the formation of hyper-kagome sublattice in the P4132(P4332) phase is accompanied by a significant transformation of the spinel structure.},\\n\\tlanguage = {en},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Crystallography Reports},\\n\\tauthor = {Talanov, V. M. and Talanov, M. V. and Shirokov, V. B.},\\n\\tmonth = mar,\\n\\tyear = {2016},\\n\\tkeywords = {Crystallography Report, Ible Representation, Multicritical Point, Spinel Structure, Unusual Physical Property},\\n\\tpages = {159--169},\\n}\\n\\n\",\"author_short\":[\"Talanov, V. M.\",\"Talanov, M. V.\",\"Shirokov, V. B.\"],\"key\":\"talanov_theory_2016\",\"id\":\"talanov_theory_2016\",\"bibbaseid\":\"talanov-talanov-shirokov-theoryoftheformationofptextrm4textlesssubtextgreater132textlesssubtextgreaterptextrm4textlesssubtextgreater332textlesssubtextgreaterphasespinels-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1063774516020280\"},\"keyword\":[\"Crystallography Report\",\"Ible Representation\",\"Multicritical Point\",\"Spinel Structure\",\"Unusual Physical Property\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Structure of Cs$_{\\\\textrm{4}}$(HSO$_{\\\\textrm{4}}$)$_{\\\\textrm{3}}$(H$_{\\\\textrm{2}}$PO$_{\\\\textrm{4}}$) single crystals\",\"volume\":\"61\",\"issn\":\"1562-689X\",\"url\":\"https://doi.org/10.1134/S1063774516010119\",\"doi\":\"10.1134/S1063774516010119\",\"abstract\":\"Single crystals of Cs4(HSO4)3(H2PO4) are synthesized and studied for the first time. The new compound is found in the course of studies of the phase diagram of the CsHSO4–CsH2PO4–H2O triple system. Data on the atomic crystal structure of single-crystalline and powder specimens, as well as on structural phase transitions, are obtained.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Crystallography Reports\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Makarova\"],\"firstnames\":[\"I.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grebenev\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vasil’ev\"],\"firstnames\":[\"I.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dmitricheva\"],\"firstnames\":[\"E.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Komornikov\"],\"firstnames\":[\"V.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dolbinina\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheikin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2016\",\"keywords\":\"Crystallography Report, High Protonic Conductivity, Potassium Atom, Structural Phase Transition, Thermal Vibration\",\"pages\":\"18–23\",\"bibtex\":\"@article{makarova_structure_2016,\\n\\ttitle = {Structure of {Cs}$_{\\\\textrm{4}}$({HSO}$_{\\\\textrm{4}}$)$_{\\\\textrm{3}}$({H}$_{\\\\textrm{2}}${PO}$_{\\\\textrm{4}}$) single crystals},\\n\\tvolume = {61},\\n\\tissn = {1562-689X},\\n\\turl = {https://doi.org/10.1134/S1063774516010119},\\n\\tdoi = {10.1134/S1063774516010119},\\n\\tabstract = {Single crystals of Cs4(HSO4)3(H2PO4) are synthesized and studied for the first time. The new compound is found in the course of studies of the phase diagram of the CsHSO4–CsH2PO4–H2O triple system. Data on the atomic crystal structure of single-crystalline and powder specimens, as well as on structural phase transitions, are obtained.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Crystallography Reports},\\n\\tauthor = {Makarova, I. P. and Grebenev, V. V. and Vasil’ev, I. I. and Dmitricheva, E. V. and Komornikov, V. A. and Dolbinina, V. V. and Mikheikin, A. S.},\\n\\tmonth = jan,\\n\\tyear = {2016},\\n\\tkeywords = {Crystallography Report, High Protonic Conductivity, Potassium Atom, Structural Phase Transition, Thermal Vibration},\\n\\tpages = {18--23},\\n}\\n\\n\",\"author_short\":[\"Makarova, I. P.\",\"Grebenev, V. V.\",\"Vasil’ev, I. I.\",\"Dmitricheva, E. V.\",\"Komornikov, V. A.\",\"Dolbinina, V. V.\",\"Mikheikin, A. S.\"],\"key\":\"makarova_structure_2016\",\"id\":\"makarova_structure_2016\",\"bibbaseid\":\"makarova-grebenev-vasilev-dmitricheva-komornikov-dolbinina-mikheikin-structureofcstextrm4hsotextrm4textrm3htextrm2potextrm4singlecrystals-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1063774516010119\"},\"keyword\":[\"Crystallography Report\",\"High Protonic Conductivity\",\"Potassium Atom\",\"Structural Phase Transition\",\"Thermal Vibration\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Physical properties of Ba$_{\\\\textrm{0.8}}$Sr$_{\\\\textrm{0.2}}$TiO$_{\\\\textrm{3}}$ thin films\",\"volume\":\"58\",\"issn\":\"1090-6460\",\"url\":\"https://doi.org/10.1134/S1063783416100346\",\"doi\":\"10.1134/S1063783416100346\",\"abstract\":\"The behavior of material constants in ferroelectric Ba0.8Sr0.2TiO3 thin films is studied depending on the misfit strain at room temperature in the context of nonlinear thermodynamic potential of the phenomenological theory. Some constants are found to undergo drastic changes with the alternating strain at the interfaces. The gathered results allow one to evaluate the material constants for a specific film and to outline the direction in searching the ways to synthesize films with the needed properties.\",\"language\":\"en\",\"number\":\"10\",\"urldate\":\"2023-11-11\",\"journal\":\"Physics of the Solid State\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kalinchuk\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shakhovoi\"],\"firstnames\":[\"R.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2016\",\"pages\":\"2035–2039\",\"bibtex\":\"@article{shirokov_physical_2016-1,\\n\\ttitle = {Physical properties of {Ba}$_{\\\\textrm{0.8}}${Sr}$_{\\\\textrm{0.2}}${TiO}$_{\\\\textrm{3}}$ thin films},\\n\\tvolume = {58},\\n\\tissn = {1090-6460},\\n\\turl = {https://doi.org/10.1134/S1063783416100346},\\n\\tdoi = {10.1134/S1063783416100346},\\n\\tabstract = {The behavior of material constants in ferroelectric Ba0.8Sr0.2TiO3 thin films is studied depending on the misfit strain at room temperature in the context of nonlinear thermodynamic potential of the phenomenological theory. Some constants are found to undergo drastic changes with the alternating strain at the interfaces. The gathered results allow one to evaluate the material constants for a specific film and to outline the direction in searching the ways to synthesize films with the needed properties.},\\n\\tlanguage = {en},\\n\\tnumber = {10},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physics of the Solid State},\\n\\tauthor = {Shirokov, V. B. and Kalinchuk, V. V. and Shakhovoi, R. A. and Yuzyuk, Yu. I.},\\n\\tmonth = oct,\\n\\tyear = {2016},\\n\\tpages = {2035--2039},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Kalinchuk, V. V.\",\"Shakhovoi, R. A.\",\"Yuzyuk, Y. I.\"],\"key\":\"shirokov_physical_2016-1\",\"id\":\"shirokov_physical_2016-1\",\"bibbaseid\":\"shirokov-kalinchuk-shakhovoi-yuzyuk-physicalpropertiesofbatextrm08srtextrm02tiotextrm3thinfilms-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1134/S1063783416100346\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Phase transition in ferroelectric BaTiO$_{\\\\textrm{3}}$/SrTiO$_{\\\\textrm{3}}$ superlattice: Raman spectroscopy studies\",\"volume\":\"501\",\"issn\":\"0015-0193\",\"shorttitle\":\"Phase transition in ferroelectric BaTiO3/SrTiO3 superlattice\",\"url\":\"https://doi.org/10.1080/00150193.2016.1199201\",\"doi\":\"10.1080/00150193.2016.1199201\",\"abstract\":\"BaTiO3/SrTiO3 superlattice has been grown on (001)MgO substrate by pulsed laser deposition. The unit cell parameters of BaTiO3 and SrTiO3 layers and modulation period have been determined using X-ray diffraction. It was found that BaTiO3 and SrTiO3 layers revealed the pseudo-tetragonal distortion with out-of-plane and in-plane polarization, respectively. Electrostatic interaction of the alternating layers leads to the polarization rotations and to the symmetry lowering of the superlattice to orthorhombic or monoclinic with partial depolarization of the Raman spectra. It was found that the phase transition to the paraelectric phase occurs at ∼480 K.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zakharchenko\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tikhonov\"],\"firstnames\":[\"Yu.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ortega\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kumar\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"R.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lukyanchuk\"],\"firstnames\":[\"I.\",\"A.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2016\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2016.1199201\",\"keywords\":\"Raman spectroscopy, soft mode, superlattices\",\"pages\":\"61–69\",\"bibtex\":\"@article{razumnaya_phase_2016,\\n\\ttitle = {Phase transition in ferroelectric {BaTiO}$_{\\\\textrm{3}}$/{SrTiO}$_{\\\\textrm{3}}$ superlattice: {Raman} spectroscopy studies},\\n\\tvolume = {501},\\n\\tissn = {0015-0193},\\n\\tshorttitle = {Phase transition in ferroelectric {BaTiO3}/{SrTiO3} superlattice},\\n\\turl = {https://doi.org/10.1080/00150193.2016.1199201},\\n\\tdoi = {10.1080/00150193.2016.1199201},\\n\\tabstract = {BaTiO3/SrTiO3 superlattice has been grown on (001)MgO substrate by pulsed laser deposition. The unit cell parameters of BaTiO3 and SrTiO3 layers and modulation period have been determined using X-ray diffraction. It was found that BaTiO3 and SrTiO3 layers revealed the pseudo-tetragonal distortion with out-of-plane and in-plane polarization, respectively. Electrostatic interaction of the alternating layers leads to the polarization rotations and to the symmetry lowering of the superlattice to orthorhombic or monoclinic with partial depolarization of the Raman spectra. It was found that the phase transition to the paraelectric phase occurs at ∼480 K.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Razumnaya, A. G. and Yuzyuk, Yu. I. and Zakharchenko, I. N. and Tikhonov, Yu. A. and Ortega, N. and Kumar, A. and Katiyar, R. S. and El Marssi, M. and Lukyanchuk, I. A.},\\n\\tmonth = sep,\\n\\tyear = {2016},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/00150193.2016.1199201},\\n\\tkeywords = {Raman spectroscopy, soft mode, superlattices},\\n\\tpages = {61--69},\\n}\\n\\n\",\"author_short\":[\"Razumnaya, A. G.\",\"Yuzyuk, Y. I.\",\"Zakharchenko, I. N.\",\"Tikhonov, Y. A.\",\"Ortega, N.\",\"Kumar, A.\",\"Katiyar, R. S.\",\"El Marssi, M.\",\"Lukyanchuk, I. A.\"],\"key\":\"razumnaya_phase_2016\",\"id\":\"razumnaya_phase_2016\",\"bibbaseid\":\"razumnaya-yuzyuk-zakharchenko-tikhonov-ortega-kumar-katiyar-elmarssi-etal-phasetransitioninferroelectricbatiotextrm3srtiotextrm3superlatticeramanspectroscopystudies-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/00150193.2016.1199201\"},\"keyword\":[\"Raman spectroscopy\",\"soft mode\",\"superlattices\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"M$_{\\\\textrm{m}}$H$_{\\\\textrm{n}}$(XO$_{\\\\textrm{4}}$)$_{\\\\textrm{(m + n)/2}}$ crystals: structure, phase transitions, hydrogen bonds, conductivity. II. Structure and properties of Cs$_{\\\\textrm{3}}$(HSO$_{\\\\textrm{4}}$)$_{\\\\textrm{2}}$(H$_{\\\\textrm{2}}$PO$_{\\\\textrm{4}}$) and Cs$_{\\\\textrm{4}}$(HSO$_{\\\\textrm{4}}$)$_{\\\\textrm{3}}$(H$_{\\\\textrm{2}}$PO$_{\\\\textrm{4}}$) single crystals\",\"volume\":\"72\",\"copyright\":\"Copyright (c) 2016 International Union of Crystallography\",\"issn\":\"2052-5206\",\"shorttitle\":\"MmHn(XO4)(m + n)/2 crystals\",\"url\":\"http://scripts.iucr.org/cgi-bin/paper?bp5085\",\"doi\":\"10.1107/S2052520615023069\",\"abstract\":\"Cs3(HSO4)2(H2PO4) and Cs4(HSO4)3(H2PO4) single crystals were obtained for the first time based on a systematic study of the phase diagram of the CsHSO4–CsH2PO4–H2O ternary system. To reveal the structural conditionality for anomalies in physical properties, including dielectric and optical properties, diffraction studies of the crystal structure of Cs3(HSO4)2(H2PO4) and Cs4(HSO4)3(H2PO4) were performed, and their common structural features and differences were analyzed.\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Acta Crystallographica Section B: Structural Science, Crystal Engineering and Materials\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Makarova\"],\"firstnames\":[\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grebenev\"],\"firstnames\":[\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dmitricheva\"],\"firstnames\":[\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vasiliev\"],\"firstnames\":[\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Komornikov\"],\"firstnames\":[\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dolbinina\"],\"firstnames\":[\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"A.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2016\",\"note\":\"Number: 1 Publisher: International Union of Crystallography\",\"pages\":\"133–141\",\"bibtex\":\"@article{makarova_mmhnxo4m_2016,\\n\\ttitle = {M$_{\\\\textrm{m}}${H}$_{\\\\textrm{n}}$({XO}$_{\\\\textrm{4}}$)$_{\\\\textrm{(m + n)/2}}$ crystals: structure, phase transitions, hydrogen bonds, conductivity. {II}. {Structure} and properties of {Cs}$_{\\\\textrm{3}}$({HSO}$_{\\\\textrm{4}}$)$_{\\\\textrm{2}}$({H}$_{\\\\textrm{2}}${PO}$_{\\\\textrm{4}}$) and {Cs}$_{\\\\textrm{4}}$({HSO}$_{\\\\textrm{4}}$)$_{\\\\textrm{3}}$({H}$_{\\\\textrm{2}}${PO}$_{\\\\textrm{4}}$) single crystals},\\n\\tvolume = {72},\\n\\tcopyright = {Copyright (c) 2016 International Union of Crystallography},\\n\\tissn = {2052-5206},\\n\\tshorttitle = {{MmHn}({XO4})(m + n)/2 crystals},\\n\\turl = {http://scripts.iucr.org/cgi-bin/paper?bp5085},\\n\\tdoi = {10.1107/S2052520615023069},\\n\\tabstract = {Cs3(HSO4)2(H2PO4) and Cs4(HSO4)3(H2PO4) single crystals were obtained for the first time based on a systematic study of the phase diagram of the CsHSO4–CsH2PO4–H2O ternary system. To reveal the structural conditionality for anomalies in physical properties, including dielectric and optical properties, diffraction studies of the crystal structure of Cs3(HSO4)2(H2PO4) and Cs4(HSO4)3(H2PO4) were performed, and their common structural features and differences were analyzed.},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Acta Crystallographica Section B: Structural Science, Crystal Engineering and Materials},\\n\\tauthor = {Makarova, I. and Grebenev, V. and Dmitricheva, E. and Vasiliev, I. and Komornikov, V. and Dolbinina, V. and Mikheykin, A.},\\n\\tmonth = feb,\\n\\tyear = {2016},\\n\\tnote = {Number: 1\\nPublisher: International Union of Crystallography},\\n\\tpages = {133--141},\\n}\\n\\n\",\"author_short\":[\"Makarova, I.\",\"Grebenev, V.\",\"Dmitricheva, E.\",\"Vasiliev, I.\",\"Komornikov, V.\",\"Dolbinina, V.\",\"Mikheykin, A.\"],\"key\":\"makarova_mmhnxo4m_2016\",\"id\":\"makarova_mmhnxo4m_2016\",\"bibbaseid\":\"makarova-grebenev-dmitricheva-vasiliev-komornikov-dolbinina-mikheykin-mtextrmmhtextrmnxotextrm4textrmmn2crystalsstructurephasetransitionshydrogenbondsconductivityiistructureandpropertiesofcstextrm3hsotextrm4textrm2htextrm2potextrm4andcstextrm4hsotextrm4textrm3htextrm2potextrm4singlecrystals-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://scripts.iucr.org/cgi-bin/paper?bp5085\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Domain structures and correlated out-of-plane and in-plane polarization reorientations in Pb(Zr$_{\\\\textrm{0.96}}$Ti$_{\\\\textrm{0.04}}$)O$_{\\\\textrm{3}}$ single crystal via piezoresponse force microscopy\",\"volume\":\"6\",\"issn\":\"2158-3226\",\"url\":\"https://doi.org/10.1063/1.4962991\",\"doi\":\"10.1063/1.4962991\",\"abstract\":\"Pb(Zr1-xTix)O3 single crystal with a low titanium content (x = 4%) was studied by the piezoresponse force microscopy (PFM) and X-ray diffraction (XRD). The XRD studies showed that the crystal faces are orthogonal to the principal cubic axes and confirmed the existence of an intermediate phase between the high-temperature paraelectric (PE) phase and the low-temperature antiferroelectric (AFE) one. A significant temperature hysteresis of phase transitions was observed by the XRD: On heating, the AFE state transforms into the intermediate one at about 373 K and the PE phase appears at 508 K, whereas on cooling the intermediate phase forms at 503 K and persists down to at least 313 K. The PFM investigation was focused on the intermediate phase and involved measurements of both out-of-plane and in-plane electromechanical responses of the (001)-oriented crystal face. The PFM images revealed the presence of polarization patterns switchable by an applied electric field, which confirms the ferroelectric character of the intermediate phase. Importantly, two types of regular domain structures were found, which differ by the spatial orientation of domain walls. The reconstruction of polarization configurations in the observed domain structures showed that one of them is a purely ferroelectric 180° structure with domain walls orthogonal to the crystal surface and parallel to one of the ⟨111⟩ pseudocubic directions. Another one is a ferroelectric-ferroelastic domain structure with the 71° walls parallel to the \\\\101\\\\ or \\\\011\\\\ crystallographic planes. Remarkably, this domain structure shows correlated out-of-plane and in-plane polarization reorientations after the poling with the aid of the microscope tip.\",\"number\":\"9\",\"urldate\":\"2023-11-11\",\"journal\":\"AIP Advances\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Andreeva\"],\"firstnames\":[\"N.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pertsev\"],\"firstnames\":[\"N.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Andronikova\"],\"firstnames\":[\"D.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Filimonov\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontiev\"],\"firstnames\":[\"N.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vakhrushev\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2016\",\"pages\":\"095211\",\"file\":\"Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\QV2ANVMG\\\\\\\\Andreeva и др. - 2016 - Domain structures and correlated out-of-plane and .pdf:application/pdf\",\"bibtex\":\"@article{andreeva_domain_2016,\\n\\ttitle = {Domain structures and correlated out-of-plane and in-plane polarization reorientations in {Pb}({Zr}$_{\\\\textrm{0.96}}${Ti}$_{\\\\textrm{0.04}}$){O}$_{\\\\textrm{3}}$ single crystal via piezoresponse force microscopy},\\n\\tvolume = {6},\\n\\tissn = {2158-3226},\\n\\turl = {https://doi.org/10.1063/1.4962991},\\n\\tdoi = {10.1063/1.4962991},\\n\\tabstract = {Pb(Zr1-xTix)O3 single crystal with a low titanium content (x = 4\\\\%) was studied by the piezoresponse force microscopy (PFM) and X-ray diffraction (XRD). The XRD studies showed that the crystal faces are orthogonal to the principal cubic axes and confirmed the existence of an intermediate phase between the high-temperature paraelectric (PE) phase and the low-temperature antiferroelectric (AFE) one. A significant temperature hysteresis of phase transitions was observed by the XRD: On heating, the AFE state transforms into the intermediate one at about 373 K and the PE phase appears at 508 K, whereas on cooling the intermediate phase forms at 503 K and persists down to at least 313 K. The PFM investigation was focused on the intermediate phase and involved measurements of both out-of-plane and in-plane electromechanical responses of the (001)-oriented crystal face. The PFM images revealed the presence of polarization patterns switchable by an applied electric field, which confirms the ferroelectric character of the intermediate phase. Importantly, two types of regular domain structures were found, which differ by the spatial orientation of domain walls. The reconstruction of polarization configurations in the observed domain structures showed that one of them is a purely ferroelectric 180° structure with domain walls orthogonal to the crystal surface and parallel to one of the ⟨111⟩ pseudocubic directions. Another one is a ferroelectric-ferroelastic domain structure with the 71° walls parallel to the \\\\{101\\\\} or \\\\{011\\\\} crystallographic planes. Remarkably, this domain structure shows correlated out-of-plane and in-plane polarization reorientations after the poling with the aid of the microscope tip.},\\n\\tnumber = {9},\\n\\turldate = {2023-11-11},\\n\\tjournal = {AIP Advances},\\n\\tauthor = {Andreeva, N. V. and Pertsev, N. A. and Andronikova, D. A. and Filimonov, A. V. and Leontiev, N. G. and Leontyev, I. N. and Vakhrushev, S. B.},\\n\\tmonth = sep,\\n\\tyear = {2016},\\n\\tpages = {095211},\\n\\tfile = {Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\QV2ANVMG\\\\\\\\Andreeva и др. - 2016 - Domain structures and correlated out-of-plane and .pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Andreeva, N. V.\",\"Pertsev, N. A.\",\"Andronikova, D. A.\",\"Filimonov, A. V.\",\"Leontiev, N. G.\",\"Leontyev, I. N.\",\"Vakhrushev, S. B.\"],\"key\":\"andreeva_domain_2016\",\"id\":\"andreeva_domain_2016\",\"bibbaseid\":\"andreeva-pertsev-andronikova-filimonov-leontiev-leontyev-vakhrushev-domainstructuresandcorrelatedoutofplaneandinplanepolarizationreorientationsinpbzrtextrm096titextrm004otextrm3singlecrystalviapiezoresponseforcemicroscopy-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.4962991\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Determining the valence state of manganese ions in complex oxides La$_{\\\\textrm{1–x}}$Ca$_{\\\\textrm{x}}$MnO$_{\\\\textrm{3}}$ (x = 0.5, 0.7, 0.85, and 0.9) based on Mn2p and Mn3s X-ray photoelectron spectra\",\"volume\":\"80\",\"issn\":\"1934-9432\",\"url\":\"https://doi.org/10.3103/S1062873816060125\",\"doi\":\"10.3103/S1062873816060125\",\"abstract\":\"The valence state of manganese ions in complex oxides La1–xCaxMnO3 (x = 0.5, 0.7, 0.85, and 0.9) is studied on the basis of Mn2p and Mn3s X-ray photoelectron spectra. It is shown that manganese ions have the valence of Mn3+ and Mn4+ in the studied compounds. The relative Mn3+/Mn4+ content is determined.\",\"language\":\"en\",\"number\":\"6\",\"urldate\":\"2023-11-11\",\"journal\":\"Bulletin of the Russian Academy of Sciences: Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Googlev\"],\"firstnames\":[\"K.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kozakov\"],\"firstnames\":[\"A.\",\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kochur\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nikolskii\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zvolenskaya\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2016\",\"pages\":\"638–640\",\"bibtex\":\"@article{googlev_determining_2016,\\n\\ttitle = {Determining the valence state of manganese ions in complex oxides {La}$_{\\\\textrm{1–x}}${Ca}$_{\\\\textrm{x}}${MnO}$_{\\\\textrm{3}}$ (x = 0.5, 0.7, 0.85, and 0.9) based on {Mn2p} and {Mn3s} {X}-ray photoelectron spectra},\\n\\tvolume = {80},\\n\\tissn = {1934-9432},\\n\\turl = {https://doi.org/10.3103/S1062873816060125},\\n\\tdoi = {10.3103/S1062873816060125},\\n\\tabstract = {The valence state of manganese ions in complex oxides La1–xCaxMnO3 (x = 0.5, 0.7, 0.85, and 0.9) is studied on the basis of Mn2p and Mn3s X-ray photoelectron spectra. It is shown that manganese ions have the valence of Mn3+ and Mn4+ in the studied compounds. The relative Mn3+/Mn4+ content is determined.},\\n\\tlanguage = {en},\\n\\tnumber = {6},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Bulletin of the Russian Academy of Sciences: Physics},\\n\\tauthor = {Googlev, K. A. and Kozakov, A. T. and Kochur, A. G. and Nikolskii, A. V. and Torgashev, V. I. and Zvolenskaya, A. A.},\\n\\tmonth = jun,\\n\\tyear = {2016},\\n\\tpages = {638--640},\\n}\\n\\n\",\"author_short\":[\"Googlev, K. A.\",\"Kozakov, A. T.\",\"Kochur, A. G.\",\"Nikolskii, A. V.\",\"Torgashev, V. I.\",\"Zvolenskaya, A. A.\"],\"key\":\"googlev_determining_2016\",\"id\":\"googlev_determining_2016\",\"bibbaseid\":\"googlev-kozakov-kochur-nikolskii-torgashev-zvolenskaya-determiningthevalencestateofmanganeseionsincomplexoxideslatextrm1xcatextrmxmnotextrm3x0507085and09basedonmn2pandmn3sxrayphotoelectronspectra-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.3103/S1062873816060125\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Composition dependence of the diffuse scattering in cubic PbZr$_{\\\\textrm{1-x}}$Ti$_{\\\\textrm{x}}$O$_{\\\\textrm{3}}$\",\"volume\":\"503\",\"issn\":\"0015-0193\",\"url\":\"https://doi.org/10.1080/00150193.2016.1217723\",\"doi\":\"10.1080/00150193.2016.1217723\",\"abstract\":\"The results of the experimental study of the diffuse scattering in ferroelectric solid solutions PbZr1-xTixO3 are reported. We have used X-ray diffraction to characterize the diffuse scattering in six single-crystals with . The comparison of diffuse intensity maps in almost pure lead zirconate and PbZr1-xTixO3 compounds with significant titanium doping shows that increasing lead titanate concentration gradually scales down the shape anisotropy of the scattering, but some details of the diffuse scattering that are not observed in pure PbTiO3 still remain.\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Bronwald\"],\"firstnames\":[\"Iurii\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Andronikova\"],\"firstnames\":[\"Daria\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Burkovsky\"],\"firstnames\":[\"Roman\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Chernyshev\"],\"firstnames\":[\"Dmitry\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontiev\"],\"firstnames\":[\"N.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontiev\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ye\"],\"firstnames\":[\"Zuo-Guang\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Vakhrushev\"],\"firstnames\":[\"Sergey\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2016\",\"note\":\"Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2016.1217723\",\"keywords\":\"diffuse scattering, Lead zirconat-titanate, morphotropic phase boundary, PZT\",\"pages\":\"45–51\",\"bibtex\":\"@article{bronwald_composition_2016,\\n\\ttitle = {Composition dependence of the diffuse scattering in cubic {PbZr}$_{\\\\textrm{1-x}}${Ti}$_{\\\\textrm{x}}${O}$_{\\\\textrm{3}}$},\\n\\tvolume = {503},\\n\\tissn = {0015-0193},\\n\\turl = {https://doi.org/10.1080/00150193.2016.1217723},\\n\\tdoi = {10.1080/00150193.2016.1217723},\\n\\tabstract = {The results of the experimental study of the diffuse scattering in ferroelectric solid solutions PbZr1-xTixO3 are reported. We have used X-ray diffraction to characterize the diffuse scattering in six single-crystals with . The comparison of diffuse intensity maps in almost pure lead zirconate and PbZr1-xTixO3 compounds with significant titanium doping shows that increasing lead titanate concentration gradually scales down the shape anisotropy of the scattering, but some details of the diffuse scattering that are not observed in pure PbTiO3 still remain.},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Bronwald, Iurii and Andronikova, Daria and Burkovsky, Roman and Chernyshev, Dmitry and Leontiev, N. G. and Leontiev, I. N. and Ye, Zuo-Guang and Vakhrushev, Sergey},\\n\\tmonth = oct,\\n\\tyear = {2016},\\n\\tnote = {Publisher: Taylor \\\\& Francis\\n\\\\_eprint: https://doi.org/10.1080/00150193.2016.1217723},\\n\\tkeywords = {diffuse scattering, Lead zirconat-titanate, morphotropic phase boundary, PZT},\\n\\tpages = {45--51},\\n}\\n\\n\",\"author_short\":[\"Bronwald, I.\",\"Andronikova, D.\",\"Burkovsky, R.\",\"Chernyshev, D.\",\"Leontiev, N. G.\",\"Leontiev, I. N.\",\"Ye, Z.\",\"Vakhrushev, S.\"],\"key\":\"bronwald_composition_2016\",\"id\":\"bronwald_composition_2016\",\"bibbaseid\":\"bronwald-andronikova-burkovsky-chernyshev-leontiev-leontiev-ye-vakhrushev-compositiondependenceofthediffusescatteringincubicpbzrtextrm1xtitextrmxotextrm3-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1080/00150193.2016.1217723\"},\"keyword\":[\"diffuse scattering\",\"Lead zirconat-titanate\",\"morphotropic phase boundary\",\"PZT\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Bi$_{\\\\textrm{1-x}}$Ca$_{\\\\textrm{x}}$FeO$_{\\\\textrm{3-δ}}$ (0 ≤ x ≤ 1) ceramics: Crystal structure, phase and elemental composition, and chemical bonding from X-ray diffraction, Raman scattering, Mössbauer, and X-ray photoelectron spectra\",\"volume\":\"664\",\"issn\":\"0925-8388\",\"shorttitle\":\"Bi1-xCaxFeO3-δ (0 ≤ x ≤ 1) ceramics\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0925838815320314\",\"doi\":\"10.1016/j.jallcom.2015.12.241\",\"abstract\":\"An integrated study of samples of Bi1−хCaхFeO3-δ (BCFO) system for 0 ≤ x ≤ 1 (step 0.1) is performed using X-ray diffraction (XRD), Raman scattering, Mössbauer spectroscopy, and X-ray photoelectron spectroscopy (XPS). Measured elemental compositions of samples were found to deviate substantially from nominal ones. X-ray structure analysis discovered a continuous series of solid solutions with perovskite structure (or its derivatives) on the interval of nominal Ca content 0 ≤ x ≤ 0.9. However, the analysis of the data from all the methods used, limits the region of single phase samples (in presence of insignificant amount of foreign ones) to nominal Ca content interval 0.1 \\\\textless x \\\\textless 0.4. No Fe4+ ions are discovered upon substitution of Bi3+ by Ca2+, neither by Mössbauer spectroscopy, nor by XPS. Charge compensation in Bi1−хCaхFeO3-δ takes place mostly via creation of oxygen vacancies. Charge transfer satellites position in Ca2p XPS is shown to be sensitive to a number of oxygen ions in the immediate environment of Ca.\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Alloys and Compounds\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kozakov\"],\"firstnames\":[\"A.\",\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kochur\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Googlev\"],\"firstnames\":[\"K.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kubrin\"],\"firstnames\":[\"S.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Trotsenko\"],\"firstnames\":[\"V.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bush\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nikolskii\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2016\",\"keywords\":\"XPS, Mössbauer spectroscopy, Elemental composition, Vacancies, XRD, BiCaFeO, BiFeO, CaFeO, Phase analysis, Raman scattering\",\"pages\":\"392–405\",\"bibtex\":\"@article{kozakov_bi1-xcaxfeo3-_2016,\\n\\ttitle = {Bi$_{\\\\textrm{1-x}}${Ca}$_{\\\\textrm{x}}${FeO}$_{\\\\textrm{3-δ}}$ (0 ≤ x ≤ 1) ceramics: {Crystal} structure, phase and elemental composition, and chemical bonding from {X}-ray diffraction, {Raman} scattering, {Mössbauer}, and {X}-ray photoelectron spectra},\\n\\tvolume = {664},\\n\\tissn = {0925-8388},\\n\\tshorttitle = {Bi1-{xCaxFeO3}-δ (0 ≤ x ≤ 1) ceramics},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0925838815320314},\\n\\tdoi = {10.1016/j.jallcom.2015.12.241},\\n\\tabstract = {An integrated study of samples of Bi1−хCaхFeO3-δ (BCFO) system for 0 ≤ x ≤ 1 (step 0.1) is performed using X-ray diffraction (XRD), Raman scattering, Mössbauer spectroscopy, and X-ray photoelectron spectroscopy (XPS). Measured elemental compositions of samples were found to deviate substantially from nominal ones. X-ray structure analysis discovered a continuous series of solid solutions with perovskite structure (or its derivatives) on the interval of nominal Ca content 0 ≤ x ≤ 0.9. However, the analysis of the data from all the methods used, limits the region of single phase samples (in presence of insignificant amount of foreign ones) to nominal Ca content interval 0.1 {\\\\textless} x {\\\\textless} 0.4. No Fe4+ ions are discovered upon substitution of Bi3+ by Ca2+, neither by Mössbauer spectroscopy, nor by XPS. Charge compensation in Bi1−хCaхFeO3-δ takes place mostly via creation of oxygen vacancies. Charge transfer satellites position in Ca2p XPS is shown to be sensitive to a number of oxygen ions in the immediate environment of Ca.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Alloys and Compounds},\\n\\tauthor = {Kozakov, A. T. and Kochur, A. G. and Torgashev, V. I. and Googlev, K. A. and Kubrin, S. P. and Trotsenko, V. G. and Bush, A. A. and Nikolskii, A. V.},\\n\\tmonth = apr,\\n\\tyear = {2016},\\n\\tkeywords = {XPS, Mössbauer spectroscopy, Elemental composition, Vacancies, XRD, BiCaFeO, BiFeO, CaFeO, Phase analysis, Raman scattering},\\n\\tpages = {392--405},\\n}\\n\\n\",\"author_short\":[\"Kozakov, A. T.\",\"Kochur, A. G.\",\"Torgashev, V. I.\",\"Googlev, K. A.\",\"Kubrin, S. P.\",\"Trotsenko, V. G.\",\"Bush, A. A.\",\"Nikolskii, A. V.\"],\"key\":\"kozakov_bi1-xcaxfeo3-_2016\",\"id\":\"kozakov_bi1-xcaxfeo3-_2016\",\"bibbaseid\":\"kozakov-kochur-torgashev-googlev-kubrin-trotsenko-bush-nikolskii-bitextrm1xcatextrmxfeotextrm30x1ceramicscrystalstructurephaseandelementalcompositionandchemicalbondingfromxraydiffractionramanscatteringmssbauerandxrayphotoelectronspectra-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0925838815320314\"},\"keyword\":[\"XPS\",\"Mössbauer spectroscopy\",\"Elemental composition\",\"Vacancies\",\"XRD\",\"BiCaFeO\",\"BiFeO\",\"CaFeO\",\"Phase analysis\",\"Raman scattering\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Bandlike electrical transport in Pr$_{\\\\textrm{1-x}}$Ca$_{\\\\textrm{x}}$MnO$_{\\\\textrm{3}}$ manganites\",\"volume\":\"93\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.93.184303\",\"doi\":\"10.1103/PhysRevB.93.184303\",\"abstract\":\"The conductivity and dielectric permittivity spectra of polycrystalline manganites Pr1−xCaxMnO3 with x=0.3, 0.4, and 0.5 have been measured in a broad frequency range (5–3000cm−1) down to low temperatures. From the dispersion analysis the existence of a Drude component can be established that is associated with small polarons coherently moving within a band several meV wide. The temperature-dependent conductivity shows an activated behavior with an activation energy of approximately 165 meV above 170 K and 4.8 meV below 120 K. The change in the activation energy is assigned to the onset of magnetic order at 120 K. In all three samples an absorption band is discovered at 40–60cm−1 that is associated with the transition between Stark-split Pr3+ electron states which gain optical activity due to coupling to acoustical phonons.\",\"number\":\"18\",\"urldate\":\"2023-11-11\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kadyrov\"],\"firstnames\":[\"L.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhang\"],\"firstnames\":[\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"E.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Anzin\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Trotsenko\"],\"firstnames\":[\"V.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"B.\",\"P.\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2016\",\"note\":\"Publisher: American Physical Society\",\"pages\":\"184303\",\"bibtex\":\"@article{kadyrov_bandlike_2016,\\n\\ttitle = {Bandlike electrical transport in {Pr}$_{\\\\textrm{1-x}}${Ca}$_{\\\\textrm{x}}${MnO}$_{\\\\textrm{3}}$ manganites},\\n\\tvolume = {93},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.93.184303},\\n\\tdoi = {10.1103/PhysRevB.93.184303},\\n\\tabstract = {The conductivity and dielectric permittivity spectra of polycrystalline manganites Pr1−xCaxMnO3 with x=0.3, 0.4, and 0.5 have been measured in a broad frequency range (5–3000cm−1) down to low temperatures. From the dispersion analysis the existence of a Drude component can be established that is associated with small polarons coherently moving within a band several meV wide. The temperature-dependent conductivity shows an activated behavior with an activation energy of approximately 165 meV above 170 K and 4.8 meV below 120 K. The change in the activation energy is assigned to the onset of magnetic order at 120 K. In all three samples an absorption band is discovered at 40–60cm−1 that is associated with the transition between Stark-split Pr3+ electron states which gain optical activity due to coupling to acoustical phonons.},\\n\\tnumber = {18},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Kadyrov, L. S. and Zhang, T. and Zhukova, E. S. and Anzin, V. B. and Trotsenko, V. G. and Torgashev, V. I. and Dressel, M. and Gorshunov, B. P.},\\n\\tmonth = may,\\n\\tyear = {2016},\\n\\tnote = {Publisher: American Physical Society},\\n\\tpages = {184303},\\n}\\n\\n\",\"author_short\":[\"Kadyrov, L. S.\",\"Zhang, T.\",\"Zhukova, E. S.\",\"Anzin, V. B.\",\"Trotsenko, V. G.\",\"Torgashev, V. I.\",\"Dressel, M.\",\"Gorshunov, B. P.\"],\"key\":\"kadyrov_bandlike_2016\",\"id\":\"kadyrov_bandlike_2016\",\"bibbaseid\":\"kadyrov-zhang-zhukova-anzin-trotsenko-torgashev-dressel-gorshunov-bandlikeelectricaltransportinprtextrm1xcatextrmxmnotextrm3manganites-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.93.184303\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Эффекты изменения стехиометрии LaMnO$_{\\\\textrm{3}}$\",\"volume\":\"80\",\"issn\":\"0367-6765\",\"url\":\"https://elibrary.ru/item.asp?id=26160197\",\"doi\":\"10.7868/S0367676516060284\",\"abstract\":\"Установлено, что в результате синтеза LaMnO3 из разных прекурсоров, приготовленных методом твердофазной реакции и методами совместного осаждения и сорбции, в зависимости от температур синтеза образуются перовскитовые фазы с разными отклонениями от стехиометрии, что приводит к существованию при комнатной температуре фаз разной симметрии: орторомбической (твердофазный синтез) и ромбоэдрической (влажные методы синтеза).\",\"language\":\"ru\",\"number\":\"6\",\"urldate\":\"2023-11-11\",\"journal\":\"Известия Российской Академии Наук. Серия Физическая\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Рудская\"],\"firstnames\":[\"А.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Чаговец\"],\"firstnames\":[\"С.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ананьева\"],\"firstnames\":[\"Е.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Куприянов\"],\"firstnames\":[\"М.\",\"Ф.\"],\"suffixes\":[]}],\"year\":\"2016\",\"pages\":\"807\",\"bibtex\":\"@article{__2016-2,\\n\\ttitle = {Эффекты изменения стехиометрии {LaMnO}$_{\\\\textrm{3}}$},\\n\\tvolume = {80},\\n\\tissn = {0367-6765},\\n\\turl = {https://elibrary.ru/item.asp?id=26160197},\\n\\tdoi = {10.7868/S0367676516060284},\\n\\tabstract = {Установлено, что в результате синтеза LaMnO3 из разных прекурсоров, приготовленных методом твердофазной реакции и методами совместного осаждения и сорбции, в зависимости от температур синтеза образуются перовскитовые фазы с разными отклонениями от стехиометрии, что приводит к существованию при комнатной температуре фаз разной симметрии: орторомбической (твердофазный синтез) и ромбоэдрической (влажные методы синтеза).},\\n\\tlanguage = {ru},\\n\\tnumber = {6},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Известия Российской Академии Наук. Серия Физическая},\\n\\tauthor = {Рудская, А. Г. and Чаговец, С. В. and Ананьева, Е. В. and Куприянов, М. Ф.},\\n\\tyear = {2016},\\n\\tpages = {807},\\n}\\n\\n\",\"author_short\":[\"Рудская, А. Г.\",\"Чаговец, С. В.\",\"Ананьева, Е. В.\",\"Куприянов, М. Ф.\"],\"key\":\"__2016-2\",\"id\":\"__2016-2\",\"bibbaseid\":\"----lamnotextrm3-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://elibrary.ru/item.asp?id=26160197\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Электрические свойства и структура новых слоистых оксидов 26,5 ( , , )\",\"url\":\"http://ivdon.ru/ru/magazine/archive/n4y2016/3820\",\"abstract\":\"Сетевой научный журнал «Инженерный вестник Дона»\",\"language\":\"ru\",\"urldate\":\"2023-11-11\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Чупахина\"],\"firstnames\":[\"Т.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мельникова\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гырдасова\"],\"firstnames\":[\"О.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Никитина\"],\"firstnames\":[\"Ю.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гавриляченко\"],\"firstnames\":[\"В.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кабиров\"],\"firstnames\":[\"Ю.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Пруцакова\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Чебанова\"],\"firstnames\":[\"Е.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Русакова\"],\"firstnames\":[\"Е.\",\"Б.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2016\",\"keywords\":\"⛔ No DOI found\",\"file\":\"Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\2RRFFXDG\\\\\\\\3820.html:text/html\",\"bibtex\":\"@article{__2016-3,\\n\\ttitle = {Электрические свойства и структура новых слоистых оксидов 26,5 ( , , )},\\n\\turl = {http://ivdon.ru/ru/magazine/archive/n4y2016/3820},\\n\\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\\n\\tlanguage = {ru},\\n\\turldate = {2023-11-11},\\n\\tauthor = {Чупахина, Т. И. and Мельникова, Н. В. and Гырдасова, О. И. and Никитина, Ю. А. and Гавриляченко, В. Г. and Кабиров, Ю. В. and Пруцакова, Н. В. and Чебанова, Е. В. and Русакова, Е. Б.},\\n\\tmonth = oct,\\n\\tyear = {2016},\\n\\tkeywords = {⛔ No DOI found},\\n\\tfile = {Snapshot:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\2RRFFXDG\\\\\\\\3820.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Чупахина, Т. И.\",\"Мельникова, Н. В.\",\"Гырдасова, О. И.\",\"Никитина, Ю. А.\",\"Гавриляченко, В. Г.\",\"Кабиров, Ю. В.\",\"Пруцакова, Н. В.\",\"Чебанова, Е. В.\",\"Русакова, Е. Б.\"],\"key\":\"__2016-3\",\"id\":\"__2016-3\",\"bibbaseid\":\"--------etal-265-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://ivdon.ru/ru/magazine/archive/n4y2016/3820\"},\"keyword\":[\"⛔ No DOI found\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Особенности низкочастотной колебательной динамики и низкотемпературная теплоемкость двустенных углеродных нанотрубок\",\"volume\":\"58\",\"url\":\"http://journals.ioffe.ru/articles/43055\",\"abstract\":\"Построена континуальная модель низкочастотной динамики двустенной углеродной нанотрубки. В рамках предложенного подхода рассмотрено образование низкочастотной части фононного спектра двустенной нанотрубки из фононных спектров образующих ее одностенных нанотрубок. Рассмотрено влияние окружения на фононный спектр одиночной двустенной углеродной нанотрубки. Предложен комбинированный способ оценки коэффициентов ван-дер-ваальсова взаимодействия между стенками нанотрубки на основе спектроскопических данных и известных величин упругих модулей графита. Также рассчитана низкотемпературная удельная теплоемкость двустенных углеродных нанотрубок, которая в области применимости модели (T\\\\textless35 K) оказывается значительно меньше, чем сумма удельных теплоемкостей двух образующих ее индивидуальных одностенных нанотрубок. Работа выполнена при поддержке Российского научного фонда (грант N 15-12-10004).\",\"language\":\"ru\",\"number\":\"5\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Авраменко\"],\"firstnames\":[\"М.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Рошаль\"],\"firstnames\":[\"С.\",\"Б.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2016\",\"pages\":\"979–986\",\"file\":\"Физика твердого тела:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\7ERGJUQT\\\\\\\\43055.html:text/html\",\"bibtex\":\"@article{__2016-4,\\n\\ttitle = {Особенности низкочастотной колебательной динамики и низкотемпературная теплоемкость двустенных углеродных нанотрубок},\\n\\tvolume = {58},\\n\\turl = {http://journals.ioffe.ru/articles/43055},\\n\\tabstract = {Построена континуальная модель низкочастотной динамики двустенной углеродной нанотрубки. В рамках предложенного подхода рассмотрено образование низкочастотной части фононного спектра двустенной нанотрубки из фононных спектров образующих ее одностенных нанотрубок. Рассмотрено влияние окружения на фононный спектр одиночной двустенной углеродной нанотрубки. Предложен комбинированный способ оценки коэффициентов ван-дер-ваальсова взаимодействия между стенками нанотрубки на основе спектроскопических данных и известных величин упругих модулей графита. Также рассчитана низкотемпературная удельная теплоемкость двустенных углеродных нанотрубок, которая в области применимости модели (T{\\\\textless}35 K) оказывается значительно меньше, чем сумма удельных теплоемкостей двух образующих ее индивидуальных одностенных нанотрубок. Работа выполнена при поддержке Российского научного фонда (грант N 15-12-10004).},\\n\\tlanguage = {ru},\\n\\tnumber = {5},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Авраменко, М. В. and Рошаль, С. Б.},\\n\\tmonth = apr,\\n\\tyear = {2016},\\n\\tpages = {979--986},\\n\\tfile = {Физика твердого тела:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\7ERGJUQT\\\\\\\\43055.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Авраменко, М. В.\",\"Рошаль, С. Б.\"],\"key\":\"__2016-4\",\"id\":\"__2016-4\",\"bibbaseid\":\"---2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/43055\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Рентгеноэлектронное и мессбауэровское исследования валентного состояния ионов переходных металлов в керамиках Co$_{\\\\textrm{1-x}}$Fe$_{\\\\textrm{x}}$Cr$_{\\\\textrm{2}}$O4 (x=0.1,0.2, 0.5)\",\"volume\":\"58\",\"url\":\"http://journals.ioffe.ru/articles/42621\",\"abstract\":\"Валентное состояние ионов переходных металлов в системе Сo1-xFexCr2O4 (x = 0.1, 0.2, 0.5) изучено с помощью рентгеновской фотоэлектронной и мессбауэровской спектроскопии. Показано присутствие в этой системе ионов Fe2+ и Fe3+. Относительные содержания Fe3+/Fe2+ определены путем подгонки экспериментальных Fe2p-спектров суперпозицией теоретических спектров Fe2+ и Fe3+, а также методом мессбауэровской спектроскопии. Работа выполнена при частичной поддержке Минобрнауки РФ проект 1880 и в рамках проектной части государственного задания Департамента науки и технологий Минобрнауки России N 3.1137.2014К, а также соглашения N 14.607.21.0110 от 27.11.2014 г., уникальный идентификатор соглашения RFMEFI60714X0110.\",\"language\":\"ru\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Кочур\"],\"firstnames\":[\"А.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гуглев\"],\"firstnames\":[\"К.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Козаков\"],\"firstnames\":[\"А.\",\"Т.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кубрин\"],\"firstnames\":[\"С.\",\"П.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Никольский\"],\"firstnames\":[\"А.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Торгашев\"],\"firstnames\":[\"В.\",\"И.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2015\",\"pages\":\"108–113\",\"file\":\"Физика твердого тела:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\39KQTSIS\\\\\\\\42621.html:text/html\",\"bibtex\":\"@article{__2015,\\n\\ttitle = {Рентгеноэлектронное и мессбауэровское исследования валентного состояния ионов переходных металлов в керамиках {Co}$_{\\\\textrm{1-x}}${Fe}$_{\\\\textrm{x}}${Cr}$_{\\\\textrm{2}}${O4} (x=0.1,0.2, 0.5)},\\n\\tvolume = {58},\\n\\turl = {http://journals.ioffe.ru/articles/42621},\\n\\tabstract = {Валентное состояние ионов переходных металлов в системе Сo1-xFexCr2O4 (x = 0.1, 0.2, 0.5) изучено с помощью рентгеновской фотоэлектронной и мессбауэровской спектроскопии. Показано присутствие в этой системе ионов Fe2+ и Fe3+. Относительные содержания Fe3+/Fe2+ определены путем подгонки экспериментальных Fe2p-спектров суперпозицией теоретических спектров Fe2+ и Fe3+, а также методом мессбауэровской спектроскопии. Работа выполнена при частичной поддержке Минобрнауки РФ проект 1880 и в рамках проектной части государственного задания Департамента науки и технологий Минобрнауки России N 3.1137.2014К, а также соглашения N 14.607.21.0110 от 27.11.2014 г., уникальный идентификатор соглашения RFMEFI60714X0110.},\\n\\tlanguage = {ru},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Кочур, А. Г. and Гуглев, К. А. and Козаков, А. Т. and Кубрин, С. П. and Никольский, А. В. and Торгашев, В. И.},\\n\\tmonth = dec,\\n\\tyear = {2015},\\n\\tpages = {108--113},\\n\\tfile = {Физика твердого тела:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\39KQTSIS\\\\\\\\42621.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Кочур, А. Г.\",\"Гуглев, К. А.\",\"Козаков, А. Т.\",\"Кубрин, С. П.\",\"Никольский, А. В.\",\"Торгашев, В. И.\"],\"key\":\"__2015\",\"id\":\"__2015\",\"bibbaseid\":\"------cotextrm1xfetextrmxcrtextrm2o4x010205-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/42621\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Положительное магнитосопротивление композитов La$_{\\\\textrm{0.7}}$Sr$_{\\\\textrm{0.3}}$MnO$_{\\\\textrm{3}}$/C при комнатной температуре\",\"volume\":\"58\",\"url\":\"http://journals.ioffe.ru/articles/43238\",\"abstract\":\"Синтезированы двухфазные композиты xLa0.7Sr0.3MnO3/(100-x)C (x=5-85 mass/%). Изучены их магниторезистивные свойства в магнитных полях от 0 до 15 kOe. При комнатной температуре значения положительного изотропного магнитосопротивления для образцов с x=50-60 mass% достигают 15%. Работа выполнена при финансовой поддержке РФФИ (проект N 14-03-00103).\",\"language\":\"ru\",\"number\":\"7\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Кабиров\"],\"firstnames\":[\"Ю.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гавриляченко\"],\"firstnames\":[\"В.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Богатин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гавриляченко\"],\"firstnames\":[\"Т.\",\"В.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2016\",\"pages\":\"1263–1265\",\"bibtex\":\"@article{__2016-5,\\n\\ttitle = {Положительное магнитосопротивление композитов {La}$_{\\\\textrm{0.7}}${Sr}$_{\\\\textrm{0.3}}${MnO}$_{\\\\textrm{3}}$/{C} при комнатной температуре},\\n\\tvolume = {58},\\n\\turl = {http://journals.ioffe.ru/articles/43238},\\n\\tabstract = {Синтезированы двухфазные композиты xLa0.7Sr0.3MnO3/(100-x)C (x=5-85 mass/\\\\%). Изучены их магниторезистивные свойства в магнитных полях от 0 до 15 kOe. При комнатной температуре значения положительного изотропного магнитосопротивления для образцов с x=50-60 mass\\\\% достигают 15\\\\%. Работа выполнена при финансовой поддержке РФФИ (проект N 14-03-00103).},\\n\\tlanguage = {ru},\\n\\tnumber = {7},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Богатин, А. С. and Лянгузов, Н. В. and Гавриляченко, Т. В.},\\n\\tmonth = jun,\\n\\tyear = {2016},\\n\\tpages = {1263--1265},\\n}\\n\\n\",\"author_short\":[\"Кабиров, Ю. В.\",\"Гавриляченко, В. Г.\",\"Богатин, А. С.\",\"Лянгузов, Н. В.\",\"Гавриляченко, Т. В.\"],\"key\":\"__2016-5\",\"id\":\"__2016-5\",\"bibbaseid\":\"-----latextrm07srtextrm03mnotextrm3c-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/43238\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Отрицательная магниторезистивность композитной керамики (1-x)La$_{\\\\textrm{0.7}}$Sr$_{\\\\textrm{0.3}}$MnO$_{\\\\textrm{3}}$/x(GeO$_{\\\\textrm{2}}$, Li$_{\\\\textrm{4}}$P$_{\\\\textrm{2}}$O$_{\\\\textrm{7}}$)\",\"volume\":\"42\",\"url\":\"http://journals.ioffe.ru/articles/43008\",\"abstract\":\"Синтезированы керамические композиты (1-x)La0.7Sr0.3MnO3/x(GeO2) и (1-x)La0.7Sr0.3MnO3/x(Li4P2 O7), где x=0.1-0.3, отличающиеся высокими значениями отрицательной изотропной магниторезистивности (MR) при комнатной температуре. В композите, где в качестве барьерной компоненты с массовой долей 20% использован GeO2, MR=15% в магнитном поле 18 kOe, а в композите с Li4P2O7 при тех же условиях MR=16%.\",\"language\":\"ru\",\"number\":\"6\",\"urldate\":\"2023-11-11\",\"journal\":\"Письма в ЖТФ\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Кабиров\"],\"firstnames\":[\"Ю.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гавриляченко\"],\"firstnames\":[\"В.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Богатин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гавриляченко\"],\"firstnames\":[\"Т.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Медведев\"],\"firstnames\":[\"Б.\",\"С.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2016\",\"pages\":\"1–5\",\"file\":\"Письма в журнал технической физики:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\4JRHC3G5\\\\\\\\43008.html:text/html\",\"bibtex\":\"@article{__2016-6,\\n\\ttitle = {Отрицательная магниторезистивность композитной керамики (1-x){La}$_{\\\\textrm{0.7}}${Sr}$_{\\\\textrm{0.3}}${MnO}$_{\\\\textrm{3}}$/x({GeO}$_{\\\\textrm{2}}$, {Li}$_{\\\\textrm{4}}${P}$_{\\\\textrm{2}}${O}$_{\\\\textrm{7}}$)},\\n\\tvolume = {42},\\n\\turl = {http://journals.ioffe.ru/articles/43008},\\n\\tabstract = {Синтезированы керамические композиты (1-x)La0.7Sr0.3MnO3/x(GeO2) и (1-x)La0.7Sr0.3MnO3/x(Li4P2 O7), где x=0.1-0.3, отличающиеся высокими значениями отрицательной изотропной магниторезистивности (MR) при комнатной температуре. В композите, где в качестве барьерной компоненты с массовой долей 20\\\\% использован GeO2, MR=15\\\\% в магнитном поле 18 kOe, а в композите с Li4P2O7 при тех же условиях MR=16\\\\%.},\\n\\tlanguage = {ru},\\n\\tnumber = {6},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Письма в ЖТФ},\\n\\tauthor = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Богатин, А. С. and Лянгузов, Н. В. and Гавриляченко, Т. В. and Медведев, Б. С.},\\n\\tmonth = feb,\\n\\tyear = {2016},\\n\\tpages = {1--5},\\n\\tfile = {Письма в журнал технической физики:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\4JRHC3G5\\\\\\\\43008.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Кабиров, Ю. В.\",\"Гавриляченко, В. Г.\",\"Богатин, А. С.\",\"Лянгузов, Н. В.\",\"Гавриляченко, Т. В.\",\"Медведев, Б. С.\"],\"key\":\"__2016-6\",\"id\":\"__2016-6\",\"bibbaseid\":\"------1xlatextrm07srtextrm03mnotextrm3xgeotextrm2litextrm4ptextrm2otextrm7-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/43008\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Одношаговый синтез магниторезистивных композитных материалов La$_{\\\\textrm{0.7}}$Sr$_{\\\\textrm{0.3}}$MnO$_{\\\\textrm{3}}$/GeO$_{\\\\textrm{2}}$\",\"url\":\"https://fundamental-research.ru/ru/article/view?id=40689\",\"language\":\"ru\",\"number\":\"9\",\"urldate\":\"2023-11-11\",\"journal\":\"Технические науки\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Кабиров\"],\"firstnames\":[\"Ю.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гавриляченко\"],\"firstnames\":[\"В.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Пруцакова\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гуда\"],\"firstnames\":[\"А.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Попов\"],\"firstnames\":[\"Ю.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Чебанова\"],\"firstnames\":[\"Е.\",\"В.\"],\"suffixes\":[]}],\"month\":\"September\",\"year\":\"2016\",\"pages\":\"26–30\",\"file\":\"ОДНОШАГОВЫЙ СИНТЕЗ МАГНИТОРЕЗИСТИВНЫХ КОМПОЗИТНЫХ МАТЕРИАЛОВ LA0.7SR0.3MNO3/GEO2 - Фундаментальные исследования (научный журнал):C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\T72K4G94\\\\ǐew.html:text/html\",\"bibtex\":\"@article{__2016-7,\\n\\ttitle = {Одношаговый синтез магниторезистивных композитных материалов {La}$_{\\\\textrm{0.7}}${Sr}$_{\\\\textrm{0.3}}${MnO}$_{\\\\textrm{3}}$/{GeO}$_{\\\\textrm{2}}$},\\n\\turl = {https://fundamental-research.ru/ru/article/view?id=40689},\\n\\tlanguage = {ru},\\n\\tnumber = {9},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Технические науки},\\n\\tauthor = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Пруцакова, Н. В. and Гуда, А. А. and Попов, Ю. В. and Чебанова, Е. В.},\\n\\tmonth = sep,\\n\\tyear = {2016},\\n\\tpages = {26--30},\\n\\tfile = {ОДНОШАГОВЫЙ СИНТЕЗ МАГНИТОРЕЗИСТИВНЫХ КОМПОЗИТНЫХ МАТЕРИАЛОВ LA0.7SR0.3MNO3/GEO2 - Фундаментальные исследования (научный журнал):C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\T72K4G94\\\\\\\\view.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Кабиров, Ю. В.\",\"Гавриляченко, В. Г.\",\"Пруцакова, Н. В.\",\"Гуда, А. А.\",\"Попов, Ю. В.\",\"Чебанова, Е. В.\"],\"key\":\"__2016-7\",\"id\":\"__2016-7\",\"bibbaseid\":\"------latextrm07srtextrm03mnotextrm3geotextrm2-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://fundamental-research.ru/ru/article/view?id=40689\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Влияние механизмов роста на деформацию элементарной ячейки и переключение поляризации в гетероструктурах титаната бария-стронция на оксиде магния\",\"volume\":\"86\",\"url\":\"http://journals.ioffe.ru/articles/42648\",\"abstract\":\"Исследованы влияние механизмов роста на деформацию ячейки и связанное с этим изменение свойств монокристаллических пленок Ba0.8Sr0.2TiO3, выращенных на подложках MgO по механизмам роста Франка-Ван дер Мерве и Вольмера-Вебера. Показано, что деформация ячейки существенно зависит от толщины пленки и в значительной мере определяется механизмами роста. Установлено, что в рамках одной пары пленка-подложка можно варьировать напряжения в пленке от двумерно-растягивающих до сжимающих за счет изменения механизмов роста и толщины пленки.\",\"language\":\"ru\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Журнал технической физики\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бирюков\"],\"firstnames\":[\"С.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Анохин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2015\",\"pages\":\"93–98\",\"file\":\"Журнал технической физики:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\RVFMF3E9\\\\\\\\42648.html:text/html\",\"bibtex\":\"@article{__2015-1,\\n\\ttitle = {Влияние механизмов роста на деформацию элементарной ячейки и переключение поляризации в гетероструктурах титаната бария-стронция на оксиде магния},\\n\\tvolume = {86},\\n\\turl = {http://journals.ioffe.ru/articles/42648},\\n\\tabstract = {Исследованы влияние механизмов роста на деформацию ячейки и связанное с этим изменение свойств монокристаллических пленок Ba0.8Sr0.2TiO3, выращенных на подложках MgO по механизмам роста Франка-Ван дер Мерве и Вольмера-Вебера. Показано, что деформация ячейки существенно зависит от толщины пленки и в значительной мере определяется механизмами роста. Установлено, что в рамках одной пары пленка-подложка можно варьировать напряжения в пленке от двумерно-растягивающих до сжимающих за счет изменения механизмов роста и толщины пленки.},\\n\\tlanguage = {ru},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Журнал технической физики},\\n\\tauthor = {Мухортов, В. М. and Головко, Ю. И. and Бирюков, С. В. and Анохин, А. С. and Юзюк, Ю. И.},\\n\\tmonth = dec,\\n\\tyear = {2015},\\n\\tpages = {93--98},\\n\\tfile = {Журнал технической физики:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\RVFMF3E9\\\\\\\\42648.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Мухортов, В. М.\",\"Головко, Ю. И.\",\"Бирюков, С. В.\",\"Анохин, А. С.\",\"Юзюк, Ю. И.\"],\"key\":\"__2015-1\",\"id\":\"__2015-1\",\"bibbaseid\":\"------2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/42648\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Valence state of transition metal ions in Co$_{\\\\textrm{1−x}}$Fe$_{\\\\textrm{x}}$Cr$_{\\\\textrm{2}}$O$_{\\\\textrm{4}}$ (x=0.1, 0.2, 0.5) ceramics from X-ray photoelectron and Mössbauer spectroscopy data\",\"volume\":\"636\",\"issn\":\"0925-8388\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0925838815005903\",\"doi\":\"10.1016/j.jallcom.2015.02.150\",\"abstract\":\"Ceramics with nominal composition Co1−xFexCr2O4 (x=0.1, 0.2, 0.5) are synthesized via a solid state reaction method. Crystal structure of samples is studied with X-ray diffraction. Actual elemental composition is determined using X-ray microanalysis and X-ray photoelectron spectroscopy (XPS). Samples’ morphology is studied with scanning electron microscopy. Valence state of the Co, Fe and Cr ions is determined from 2p X-ray photoelectron spectra and Mössbauer spectra. XPS are assigned based on calculations with allowance for the multiplet splitting, crystal field, and the charge-transfer effects. Cobalt ions are found to be bivalent in tetrahedral coordination; chromium ions are trivalent in octahedral coordination. Fe ions are mostly in trivalent states, although Fe2+ ions are also present in significant amounts. Fe2+ ions are in tetrahedral coordination while Fe3+ ions occupy both tetrahedral and octahedral sites. Bulk and near-surface elemental compositions of the ceramic grains are noticeably different. Relative Fe3+/Fe2+ contents are the same in the volume and at the surface of the samples; relative number of Fe3+ ions increases upon the increase of x. A model of partly inverse spinel structure is suggested where the atoms of iron substitute both Co and Cr atoms.\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Alloys and Compounds\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kochur\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kozakov\"],\"firstnames\":[\"A.\",\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Googlev\"],\"firstnames\":[\"K.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kubrin\"],\"firstnames\":[\"S.\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nikolskii\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bush\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shkuratov\"],\"firstnames\":[\"V.\",\"Ya.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shevtsova\"],\"firstnames\":[\"S.\",\"I.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2015\",\"keywords\":\"X-ray diffraction, XPS, CoFeCrO ceramics, Ions valence state, Mössbauer spectroscopy, X-ray microanalysis\",\"pages\":\"241–248\",\"bibtex\":\"@article{kochur_valence_2015,\\n\\ttitle = {Valence state of transition metal ions in {Co}$_{\\\\textrm{1−x}}${Fe}$_{\\\\textrm{x}}${Cr}$_{\\\\textrm{2}}${O}$_{\\\\textrm{4}}$ (x=0.1, 0.2, 0.5) ceramics from {X}-ray photoelectron and {Mössbauer} spectroscopy data},\\n\\tvolume = {636},\\n\\tissn = {0925-8388},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0925838815005903},\\n\\tdoi = {10.1016/j.jallcom.2015.02.150},\\n\\tabstract = {Ceramics with nominal composition Co1−xFexCr2O4 (x=0.1, 0.2, 0.5) are synthesized via a solid state reaction method. Crystal structure of samples is studied with X-ray diffraction. Actual elemental composition is determined using X-ray microanalysis and X-ray photoelectron spectroscopy (XPS). Samples’ morphology is studied with scanning electron microscopy. Valence state of the Co, Fe and Cr ions is determined from 2p X-ray photoelectron spectra and Mössbauer spectra. XPS are assigned based on calculations with allowance for the multiplet splitting, crystal field, and the charge-transfer effects. Cobalt ions are found to be bivalent in tetrahedral coordination; chromium ions are trivalent in octahedral coordination. Fe ions are mostly in trivalent states, although Fe2+ ions are also present in significant amounts. Fe2+ ions are in tetrahedral coordination while Fe3+ ions occupy both tetrahedral and octahedral sites. Bulk and near-surface elemental compositions of the ceramic grains are noticeably different. Relative Fe3+/Fe2+ contents are the same in the volume and at the surface of the samples; relative number of Fe3+ ions increases upon the increase of x. A model of partly inverse spinel structure is suggested where the atoms of iron substitute both Co and Cr atoms.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Alloys and Compounds},\\n\\tauthor = {Kochur, A. G. and Kozakov, A. T. and Googlev, K. A. and Kubrin, S. P. and Nikolskii, A. V. and Torgashev, V. I. and Bush, A. A. and Shkuratov, V. Ya. and Shevtsova, S. I.},\\n\\tmonth = jul,\\n\\tyear = {2015},\\n\\tkeywords = {X-ray diffraction, XPS, CoFeCrO ceramics, Ions valence state, Mössbauer spectroscopy, X-ray microanalysis},\\n\\tpages = {241--248},\\n}\\n\\n\",\"author_short\":[\"Kochur, A. G.\",\"Kozakov, A. T.\",\"Googlev, K. A.\",\"Kubrin, S. P.\",\"Nikolskii, A. V.\",\"Torgashev, V. I.\",\"Bush, A. A.\",\"Shkuratov, V. Y.\",\"Shevtsova, S. I.\"],\"key\":\"kochur_valence_2015\",\"id\":\"kochur_valence_2015\",\"bibbaseid\":\"kochur-kozakov-googlev-kubrin-nikolskii-torgashev-bush-shkuratov-etal-valencestateoftransitionmetalionsincotextrm1xfetextrmxcrtextrm2otextrm4x010205ceramicsfromxrayphotoelectronandmssbauerspectroscopydata-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0925838815005903\"},\"keyword\":[\"X-ray diffraction\",\"XPS\",\"CoFeCrO ceramics\",\"Ions valence state\",\"Mössbauer spectroscopy\",\"X-ray microanalysis\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Valence state of manganese and iron ions in La$_{\\\\textrm{1−x}}$A$_{\\\\textrm{x}}$MnO$_{\\\\textrm{3}}$ (A = Ca, Sr) and Bi$_{\\\\textrm{1−x}}$Sr$_{\\\\textrm{x}}$FeO$_{\\\\textrm{3}}$ systems from Mn2p, Mn3s, Fe2p and Fe3s X-ray photoelectron spectra. Effect of delocalization on Fe3s spectra splitting\",\"volume\":\"647\",\"issn\":\"0925-8388\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0925838815302772\",\"doi\":\"10.1016/j.jallcom.2015.06.161\",\"abstract\":\"La1−xCaxMnO3 (x = 0.5, 0.7, 0.85, 0.95) ceramic samples are synthesized by solid state reaction method. Mn3s and Mn2p X-ray photoelectron spectra (XPS) of La1−xCaxMnO3, and Fe3s-spectra of Bi1−xSrxFeO3 (0 ≤ x ≤ 1) are measured at room temperature. Both Mn3+ and Mn4+ ions are discovered in La1−xCaxMnO3 similarly to the case of Fe3+ and Fe4+ found earlier in Bi1−xSrxFeO3 ceramics. Relative Mn3+/Mn4+ contents are determined by fitting measured Mn2p spectra with combinations of Mn2p spectra of compounds containing tri- and quadrivalent Mn ions. Relative portion of Mn4+ is shown to increase with the increase of x. Fe3s spectrum splitting in Bi1−xSrxFeO3 increases with x in contrast to the Mn3s-spectrum splitting in La1−xCaxMnO3 and La1−xSrxMnO3. Anomalous behavior of Fe3s splitting is explained in the frame of the model of partly itinerant 3d-electrons by strong effect of 3d electron delocalization on electron correlation interaction in final state of 3s photoabsorption.\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Alloys and Compounds\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kozakov\"],\"firstnames\":[\"A.\",\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kochur\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Googlev\"],\"firstnames\":[\"K.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nikolskii\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Trotsenko\"],\"firstnames\":[\"V.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bush\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2015\",\"keywords\":\"XPS, BiSrFeO, Delocalization, Electron correlation, Fe3s, Itinerant 3d electrons, LaAMnO (A = Ca,Sr), Mn2p, Mn3s\",\"pages\":\"947–955\",\"bibtex\":\"@article{kozakov_valence_2015,\\n\\ttitle = {Valence state of manganese and iron ions in {La}$_{\\\\textrm{1−x}}${A}$_{\\\\textrm{x}}${MnO}$_{\\\\textrm{3}}$ ({A} = {Ca}, {Sr}) and {Bi}$_{\\\\textrm{1−x}}${Sr}$_{\\\\textrm{x}}${FeO}$_{\\\\textrm{3}}$ systems from {Mn2p}, {Mn3s}, {Fe2p} and {Fe3s} {X}-ray photoelectron spectra. {Effect} of delocalization on {Fe3s} spectra splitting},\\n\\tvolume = {647},\\n\\tissn = {0925-8388},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0925838815302772},\\n\\tdoi = {10.1016/j.jallcom.2015.06.161},\\n\\tabstract = {La1−xCaxMnO3 (x = 0.5, 0.7, 0.85, 0.95) ceramic samples are synthesized by solid state reaction method. Mn3s and Mn2p X-ray photoelectron spectra (XPS) of La1−xCaxMnO3, and Fe3s-spectra of Bi1−xSrxFeO3 (0 ≤ x ≤ 1) are measured at room temperature. Both Mn3+ and Mn4+ ions are discovered in La1−xCaxMnO3 similarly to the case of Fe3+ and Fe4+ found earlier in Bi1−xSrxFeO3 ceramics. Relative Mn3+/Mn4+ contents are determined by fitting measured Mn2p spectra with combinations of Mn2p spectra of compounds containing tri- and quadrivalent Mn ions. Relative portion of Mn4+ is shown to increase with the increase of x. Fe3s spectrum splitting in Bi1−xSrxFeO3 increases with x in contrast to the Mn3s-spectrum splitting in La1−xCaxMnO3 and La1−xSrxMnO3. Anomalous behavior of Fe3s splitting is explained in the frame of the model of partly itinerant 3d-electrons by strong effect of 3d electron delocalization on electron correlation interaction in final state of 3s photoabsorption.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Alloys and Compounds},\\n\\tauthor = {Kozakov, A. T. and Kochur, A. G. and Googlev, K. A. and Nikolskii, A. V. and Torgashev, V. I. and Trotsenko, V. G. and Bush, A. A.},\\n\\tmonth = oct,\\n\\tyear = {2015},\\n\\tkeywords = {XPS, BiSrFeO, Delocalization, Electron correlation, Fe3s, Itinerant 3d electrons, LaAMnO (A = Ca,Sr), Mn2p, Mn3s},\\n\\tpages = {947--955},\\n}\\n\\n\",\"author_short\":[\"Kozakov, A. T.\",\"Kochur, A. G.\",\"Googlev, K. A.\",\"Nikolskii, A. V.\",\"Torgashev, V. I.\",\"Trotsenko, V. G.\",\"Bush, A. A.\"],\"key\":\"kozakov_valence_2015\",\"id\":\"kozakov_valence_2015\",\"bibbaseid\":\"kozakov-kochur-googlev-nikolskii-torgashev-trotsenko-bush-valencestateofmanganeseandironionsinlatextrm1xatextrmxmnotextrm3acasrandbitextrm1xsrtextrmxfeotextrm3systemsfrommn2pmn3sfe2pandfe3sxrayphotoelectronspectraeffectofdelocalizationonfe3sspectrasplitting-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0925838815302772\"},\"keyword\":[\"XPS\",\"BiSrFeO\",\"Delocalization\",\"Electron correlation\",\"Fe3s\",\"Itinerant 3d electrons\",\"LaAMnO (A = Ca\",\"Sr)\",\"Mn2p\",\"Mn3s\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"The cooperative Jahn–Teller effect and anti-isostructural phases in Ni$_{\\\\textrm{1−x}}$Co$_{\\\\textrm{x}}$Cr$_{\\\\textrm{2}}$O$_{\\\\textrm{4}}$ solid solutions: Synchrotron X-ray diffraction study\",\"volume\":\"86\",\"issn\":\"0022-3697\",\"shorttitle\":\"The cooperative Jahn–Teller effect and anti-isostructural phases in Ni1−xCoxCr2O4 solid solutions\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0022369715001651\",\"doi\":\"10.1016/j.jpcs.2015.06.015\",\"abstract\":\"A low-temperature high-resolution powder diffraction study has been carried out on a system of Ni1−xCoxCr2O4 solid solutions with x≤0.1 down to 5K. The tetragonal phase (I41/amd) with c/a\\\\textless1 was experimentally observed in Ni0.9Co0.1Cr2O4 below ∼64K. The new phase is anti-isostructural to the well-known tetragonal phase of NiCr2O4. A unified phenomenological model has been applied to structural phase transitions in Ni1−xCoxCr2O4 solid solutions. It shows that the appearing of such a phase is justified from a structural point of view. Analysis of atomic displacements confirms predictions of the symmetry-based model-free consideration.\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Physics and Chemistry of Solids\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bush\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Cervellino\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dmitriev\"],\"firstnames\":[\"V.\",\"P.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2015\",\"keywords\":\"A. Ceramics, C. X-ray diffraction, D. Crystal field, D. Crystal structure, D. Phase transitions\",\"pages\":\"42–48\",\"bibtex\":\"@article{mikheykin_cooperative_2015,\\n\\ttitle = {The cooperative {Jahn}–{Teller} effect and anti-isostructural phases in {Ni}$_{\\\\textrm{1−x}}${Co}$_{\\\\textrm{x}}${Cr}$_{\\\\textrm{2}}${O}$_{\\\\textrm{4}}$ solid solutions: {Synchrotron} {X}-ray diffraction study},\\n\\tvolume = {86},\\n\\tissn = {0022-3697},\\n\\tshorttitle = {The cooperative {Jahn}–{Teller} effect and anti-isostructural phases in {Ni1}−{xCoxCr2O4} solid solutions},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0022369715001651},\\n\\tdoi = {10.1016/j.jpcs.2015.06.015},\\n\\tabstract = {A low-temperature high-resolution powder diffraction study has been carried out on a system of Ni1−xCoxCr2O4 solid solutions with x≤0.1 down to 5K. The tetragonal phase (I41/amd) with c/a{\\\\textless}1 was experimentally observed in Ni0.9Co0.1Cr2O4 below ∼64K. The new phase is anti-isostructural to the well-known tetragonal phase of NiCr2O4. A unified phenomenological model has been applied to structural phase transitions in Ni1−xCoxCr2O4 solid solutions. It shows that the appearing of such a phase is justified from a structural point of view. Analysis of atomic displacements confirms predictions of the symmetry-based model-free consideration.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Physics and Chemistry of Solids},\\n\\tauthor = {Mikheykin, A. S. and Torgashev, V. I. and Yuzyuk, Yu. I. and Bush, A. A. and Talanov, V. M. and Cervellino, A. and Dmitriev, V. P.},\\n\\tmonth = nov,\\n\\tyear = {2015},\\n\\tkeywords = {A. Ceramics, C. X-ray diffraction, D. Crystal field, D. Crystal structure, D. Phase transitions},\\n\\tpages = {42--48},\\n}\\n\\n\",\"author_short\":[\"Mikheykin, A. S.\",\"Torgashev, V. I.\",\"Yuzyuk, Y. I.\",\"Bush, A. A.\",\"Talanov, V. M.\",\"Cervellino, A.\",\"Dmitriev, V. P.\"],\"key\":\"mikheykin_cooperative_2015\",\"id\":\"mikheykin_cooperative_2015\",\"bibbaseid\":\"mikheykin-torgashev-yuzyuk-bush-talanov-cervellino-dmitriev-thecooperativejahntellereffectandantiisostructuralphasesinnitextrm1xcotextrmxcrtextrm2otextrm4solidsolutionssynchrotronxraydiffractionstudy-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0022369715001651\"},\"keyword\":[\"A. Ceramics\",\"C. X-ray diffraction\",\"D. Crystal field\",\"D. Crystal structure\",\"D. Phase transitions\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"series\":\"Special Issue on Electronic Crystals (ECRYS-2014)\",\"title\":\"Terahertz-infrared spectroscopy of overdoped manganites La$_{\\\\textrm{1−x}}$Ca$_{\\\\textrm{x}}$MnO$_{\\\\textrm{3}}$\",\"volume\":\"460\",\"issn\":\"0921-4526\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0921452614009041\",\"doi\":\"10.1016/j.physb.2014.11.070\",\"abstract\":\"Terahertz and infrared spectra of dielectric permittivity and optical conductivity of overdoped manganites La1−xCaxMnO3 (0.5≤x≤1) have been measured at frequencies ν from 4cm−1 to 700cm−1 and at temperatures T from 5K to 300K. The samples were prepared in the form of bulk polycrystals (ceramics) and epitaxial films (free-standing and on MgO substrates). Strongly asymmetric absorption bands have been found in the compounds which are in charge-ordered state (0.5\\\\textlessx\\\\textless0.85) and have commensurate calcium doping. The bands are located close to the position of lowest energy van Hove singularity of the folded Brillouin zone. The bands are associated with a boson peak, i.e., with the excess of lattice acoustical vibrational states over the standard Debye contribution (~ν2). In addition, Raman scattering measurements on ceramic samples have been conducted, which confirmed our assignment of the bands’ origin. We firmly identify contribution to the low energy spectra due to quasi-free charge carriers. In the paramagnetic phase all samples show a Drude-like response corresponding to the band type of charge transport. At low temperatures, for the range of dopings 0.5≤x\\\\textless0.85, the conductivity spectra show signatures of variable-range hopping mechanisms of transport.\",\"urldate\":\"2023-11-11\",\"journal\":\"Physica B: Condensed Matter\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kadyrov\"],\"firstnames\":[\"Lenar\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"Elena\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"Victor\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"Boris\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"Anatoly\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Motovilova\"],\"firstnames\":[\"Elizaveta\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fischgrabe\"],\"firstnames\":[\"Florian\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Moshnyaga\"],\"firstnames\":[\"Vasily\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhang\"],\"firstnames\":[\"Tao\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kremer\"],\"firstnames\":[\"Reinhard\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pracht\"],\"firstnames\":[\"Uwe\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zapf\"],\"firstnames\":[\"Sina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pokorný\"],\"firstnames\":[\"Jan\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Untereiner\"],\"firstnames\":[\"Gabriele\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kamba\"],\"firstnames\":[\"Stanislav\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"Martin\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2015\",\"keywords\":\"Raman spectroscopy, Manganites, Terahertz spectroscopy\",\"pages\":\"199–201\",\"bibtex\":\"@article{kadyrov_terahertz-infrared_2015,\\n\\tseries = {Special {Issue} on {Electronic} {Crystals} ({ECRYS}-2014)},\\n\\ttitle = {Terahertz-infrared spectroscopy of overdoped manganites {La}$_{\\\\textrm{1−x}}${Ca}$_{\\\\textrm{x}}${MnO}$_{\\\\textrm{3}}$},\\n\\tvolume = {460},\\n\\tissn = {0921-4526},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0921452614009041},\\n\\tdoi = {10.1016/j.physb.2014.11.070},\\n\\tabstract = {Terahertz and infrared spectra of dielectric permittivity and optical conductivity of overdoped manganites La1−xCaxMnO3 (0.5≤x≤1) have been measured at frequencies ν from 4cm−1 to 700cm−1 and at temperatures T from 5K to 300K. The samples were prepared in the form of bulk polycrystals (ceramics) and epitaxial films (free-standing and on MgO substrates). Strongly asymmetric absorption bands have been found in the compounds which are in charge-ordered state (0.5{\\\\textless}x{\\\\textless}0.85) and have commensurate calcium doping. The bands are located close to the position of lowest energy van Hove singularity of the folded Brillouin zone. The bands are associated with a boson peak, i.e., with the excess of lattice acoustical vibrational states over the standard Debye contribution ({\\\\textasciitilde}ν2). In addition, Raman scattering measurements on ceramic samples have been conducted, which confirmed our assignment of the bands’ origin. We firmly identify contribution to the low energy spectra due to quasi-free charge carriers. In the paramagnetic phase all samples show a Drude-like response corresponding to the band type of charge transport. At low temperatures, for the range of dopings 0.5≤x{\\\\textless}0.85, the conductivity spectra show signatures of variable-range hopping mechanisms of transport.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Physica B: Condensed Matter},\\n\\tauthor = {Kadyrov, Lenar S. and Zhukova, Elena S. and Torgashev, Victor I. and Gorshunov, Boris P. and Prokhorov, Anatoly S. and Motovilova, Elizaveta A. and Fischgrabe, Florian and Moshnyaga, Vasily and Zhang, Tao and Kremer, Reinhard and Pracht, Uwe and Zapf, Sina and Pokorný, Jan and Untereiner, Gabriele and Kamba, Stanislav and Dressel, Martin},\\n\\tmonth = mar,\\n\\tyear = {2015},\\n\\tkeywords = {Raman spectroscopy, Manganites, Terahertz spectroscopy},\\n\\tpages = {199--201},\\n}\\n\\n\",\"author_short\":[\"Kadyrov, L. S.\",\"Zhukova, E. S.\",\"Torgashev, V. I.\",\"Gorshunov, B. P.\",\"Prokhorov, A. S.\",\"Motovilova, E. A.\",\"Fischgrabe, F.\",\"Moshnyaga, V.\",\"Zhang, T.\",\"Kremer, R.\",\"Pracht, U.\",\"Zapf, S.\",\"Pokorný, J.\",\"Untereiner, G.\",\"Kamba, S.\",\"Dressel, M.\"],\"key\":\"kadyrov_terahertz-infrared_2015\",\"id\":\"kadyrov_terahertz-infrared_2015\",\"bibbaseid\":\"kadyrov-zhukova-torgashev-gorshunov-prokhorov-motovilova-fischgrabe-moshnyaga-etal-terahertzinfraredspectroscopyofoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0921452614009041\"},\"keyword\":[\"Raman spectroscopy\",\"Manganites\",\"Terahertz spectroscopy\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Phenomenological theory of phase transitions in epitaxial Ba$_{\\\\textrm{x}}$Sr$_{\\\\textrm{1−x}}$TiO$_{\\\\textrm{3}}$ thin films on (111)-oriented cubic substrates\",\"volume\":\"118\",\"issn\":\"0021-8979\",\"url\":\"https://doi.org/10.1063/1.4926788\",\"doi\":\"10.1063/1.4926788\",\"abstract\":\"A phenomenological thermodynamic theory of BaxSr1−xTiO3 (BST-x) thin films epitaxially grown on (111)-oriented cubic substrates is developed using the Landau-Devonshire approach. The group-theoretical analysis of the low-symmetry phases was performed taking into account two order parameters: the polarization related to ionic shifts in polar zone-center F1u mode and the out-of-phase rotation of TiO6 octahedra corresponding to the R25 zone-boundary mode in the parent cubic phase Pm3¯m. The eight-order thermodynamic potential for BST-x solid solutions was developed and analyzed. We constructed the “concentration-misfit strain” phase diagram for BST-x thin films at room temperature and found that polar rhombohedral R3m phase with the polarization normal to the substrate is stable for x &gt; 0.72 and negative misfit strains, while ferroelectric monoclinic C2 and Cm phases with in-plane polarization are stable for much smaller x and positive or slightly negative misfit strains. We constructed the “temperature-misfit strain” phase diagrams for several concentrations (x = 1, 0.8, 0.6, 0.4, and 0.2). Systematic changes of the phase transition lines between the paraelectric and ferroelectric phases are discussed. The phase diagrams are useful for practical applications in thin-film engineering.\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Journal of Applied Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shakhovoy\"],\"firstnames\":[\"R.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2015\",\"pages\":\"024101\",\"bibtex\":\"@article{shirokov_phenomenological_2015,\\n\\ttitle = {Phenomenological theory of phase transitions in epitaxial {Ba}$_{\\\\textrm{x}}${Sr}$_{\\\\textrm{1−x}}${TiO}$_{\\\\textrm{3}}$ thin films on (111)-oriented cubic substrates},\\n\\tvolume = {118},\\n\\tissn = {0021-8979},\\n\\turl = {https://doi.org/10.1063/1.4926788},\\n\\tdoi = {10.1063/1.4926788},\\n\\tabstract = {A phenomenological thermodynamic theory of BaxSr1−xTiO3 (BST-x) thin films epitaxially grown on (111)-oriented cubic substrates is developed using the Landau-Devonshire approach. The group-theoretical analysis of the low-symmetry phases was performed taking into account two order parameters: the polarization related to ionic shifts in polar zone-center F1u mode and the out-of-phase rotation of TiO6 octahedra corresponding to the R25 zone-boundary mode in the parent cubic phase Pm3¯m. The eight-order thermodynamic potential for BST-x solid solutions was developed and analyzed. We constructed the “concentration-misfit strain” phase diagram for BST-x thin films at room temperature and found that polar rhombohedral R3m phase with the polarization normal to the substrate is stable for x \\\\&gt; 0.72 and negative misfit strains, while ferroelectric monoclinic C2 and Cm phases with in-plane polarization are stable for much smaller x and positive or slightly negative misfit strains. We constructed the “temperature-misfit strain” phase diagrams for several concentrations (x = 1, 0.8, 0.6, 0.4, and 0.2). Systematic changes of the phase transition lines between the paraelectric and ferroelectric phases are discussed. The phase diagrams are useful for practical applications in thin-film engineering.},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Journal of Applied Physics},\\n\\tauthor = {Shirokov, V. B. and Shakhovoy, R. A. and Razumnaya, A. G. and Yuzyuk, Yu. I.},\\n\\tmonth = jul,\\n\\tyear = {2015},\\n\\tpages = {024101},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Shakhovoy, R. A.\",\"Razumnaya, A. G.\",\"Yuzyuk, Y. I.\"],\"key\":\"shirokov_phenomenological_2015\",\"id\":\"shirokov_phenomenological_2015\",\"bibbaseid\":\"shirokov-shakhovoy-razumnaya-yuzyuk-phenomenologicaltheoryofphasetransitionsinepitaxialbatextrmxsrtextrm1xtiotextrm3thinfilmson111orientedcubicsubstrates-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1063/1.4926788\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"In Situ Studies of LaMnO$_{\\\\textrm{3}}$ Phases Formation When used of Different Precursors\",\"url\":\"https://www.semanticscholar.org/paper/In-Situ-Studies-of-LaMnO-3-Phases-Formation-When-of-Rudskaya-Kofanova/3b5d3dfeb83398cd0265cf3d59a70448d257bdf0\",\"abstract\":\"LaMnO3 specimens were synthesized with using of different precursors on X-ray diffractometer (method in situ). It was established that the cubic nanoand microcrystalline perovskite phases starts to form in the temperature range 400 – 600 °C. Synthesized LaMnO3 specimens at room temperature have stoichiometric and nonstoichiometric perovskite-type phases of different symmetry: Pnma (solid state synthesis) and R 3 c (wet methods of precursors’ preparation – sorption, co-precipitation and sol-gel)\",\"urldate\":\"2023-11-11\",\"journal\":\"International Journal of Advanced Research in Chemical Science\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Rudskaya\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kofanova\"],\"firstnames\":[\"N.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kupriyanov\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"year\":\"2015\",\"file\":\"Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\FT2R3G3W\\\\\\\\Rudskaya и др. - 2015 - In Situ Studies of LaMnO 3 Phases Formation When u.pdf:application/pdf\",\"bibtex\":\"@article{rudskaya_situ_2015,\\n\\ttitle = {In {Situ} {Studies} of {LaMnO}$_{\\\\textrm{3}}$ {Phases} {Formation} {When} used of {Different} {Precursors}},\\n\\turl = {https://www.semanticscholar.org/paper/In-Situ-Studies-of-LaMnO-3-Phases-Formation-When-of-Rudskaya-Kofanova/3b5d3dfeb83398cd0265cf3d59a70448d257bdf0},\\n\\tabstract = {LaMnO3 specimens were synthesized with using of different precursors on X-ray diffractometer (method in situ). It was established that the cubic nanoand microcrystalline perovskite phases starts to form in the temperature range 400 – 600 °C. Synthesized LaMnO3 specimens at room temperature have stoichiometric and nonstoichiometric perovskite-type phases of different symmetry: Pnma (solid state synthesis) and R 3 c (wet methods of precursors’ preparation – sorption, co-precipitation and sol-gel)},\\n\\turldate = {2023-11-11},\\n\\tjournal = {International Journal of Advanced Research in Chemical Science},\\n\\tauthor = {Rudskaya, A. and Kofanova, N. B. and Kupriyanov, M.},\\n\\tyear = {2015},\\n\\tfile = {Full Text PDF:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\FT2R3G3W\\\\\\\\Rudskaya и др. - 2015 - In Situ Studies of LaMnO 3 Phases Formation When u.pdf:application/pdf},\\n}\\n\\n\",\"author_short\":[\"Rudskaya, A.\",\"Kofanova, N. B.\",\"Kupriyanov, M.\"],\"key\":\"rudskaya_situ_2015\",\"id\":\"rudskaya_situ_2015\",\"bibbaseid\":\"rudskaya-kofanova-kupriyanov-insitustudiesoflamnotextrm3phasesformationwhenusedofdifferentprecursors-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.semanticscholar.org/paper/In-Situ-Studies-of-LaMnO-3-Phases-Formation-When-of-Rudskaya-Kofanova/3b5d3dfeb83398cd0265cf3d59a70448d257bdf0\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Fine structure of the X-ray photoelectron Ni 2$_{\\\\textrm{p}}$ spectrum in Ni$_{\\\\textrm{1–x}}$Co$_{\\\\textrm{x}}$Cr$_{\\\\textrm{2}}$O$_{\\\\textrm{4}}$ compounds\",\"volume\":\"79\",\"issn\":\"1934-9432\",\"url\":\"https://doi.org/10.3103/S106287381511012X\",\"doi\":\"10.3103/S106287381511012X\",\"abstract\":\"An interpretation of the components of the fine structure of X-ray photoelectron Ni $$\\\\2_\\\\\\\\p_\\\\3/1,1/2\\\\\\\\\\\\\\\\$$spectra of Ni1–xCoxCr2O4 solid solutions (x = 0.8, 0.5, 0.3, 0.02, 0.01, 0.005, 0.0) is given. It is shown that the A and B components of the fine structure in Ni $$\\\\2_\\\\\\\\p_\\\\3/2\\\\\\\\\\\\\\\\$$spectra originate from the Ni2+ ions located in the octahedral and tetrahedral environments, respectively. The fraction of Ni2+ ions that occupy octahedral positions in ceramics of different composition is determined.\",\"language\":\"en\",\"number\":\"11\",\"urldate\":\"2023-11-11\",\"journal\":\"Bulletin of the Russian Academy of Sciences: Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kozakov\"],\"firstnames\":[\"A.\",\"T.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kochur\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Googlev\"],\"firstnames\":[\"K.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nikolskii\"],\"firstnames\":[\"A.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shevcova\"],\"firstnames\":[\"S.\",\"I.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2015\",\"keywords\":\"Cr2O4 Solid Solution, Divalent Nickel, Hedral Position, Octahedral Crystal Field, Octahedral Position\",\"pages\":\"1371–1375\",\"bibtex\":\"@article{kozakov_fine_2015,\\n\\ttitle = {Fine structure of the {X}-ray photoelectron {Ni} 2$_{\\\\textrm{p}}$ spectrum in {Ni}$_{\\\\textrm{1–x}}${Co}$_{\\\\textrm{x}}${Cr}$_{\\\\textrm{2}}${O}$_{\\\\textrm{4}}$ compounds},\\n\\tvolume = {79},\\n\\tissn = {1934-9432},\\n\\turl = {https://doi.org/10.3103/S106287381511012X},\\n\\tdoi = {10.3103/S106287381511012X},\\n\\tabstract = {An interpretation of the components of the fine structure of X-ray photoelectron Ni \\\\$\\\\$\\\\{2\\\\_\\\\{\\\\{p\\\\_\\\\{3/1,1/2\\\\}\\\\}\\\\}\\\\}\\\\$\\\\$spectra of Ni1–xCoxCr2O4 solid solutions (x = 0.8, 0.5, 0.3, 0.02, 0.01, 0.005, 0.0) is given. It is shown that the A and B components of the fine structure in Ni \\\\$\\\\$\\\\{2\\\\_\\\\{\\\\{p\\\\_\\\\{3/2\\\\}\\\\}\\\\}\\\\}\\\\$\\\\$spectra originate from the Ni2+ ions located in the octahedral and tetrahedral environments, respectively. The fraction of Ni2+ ions that occupy octahedral positions in ceramics of different composition is determined.},\\n\\tlanguage = {en},\\n\\tnumber = {11},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Bulletin of the Russian Academy of Sciences: Physics},\\n\\tauthor = {Kozakov, A. T. and Kochur, A. G. and Googlev, K. A. and Nikolskii, A. V. and Torgashev, V. I. and Shevcova, S. I.},\\n\\tmonth = nov,\\n\\tyear = {2015},\\n\\tkeywords = {Cr2O4 Solid Solution, Divalent Nickel, Hedral Position, Octahedral Crystal Field, Octahedral Position},\\n\\tpages = {1371--1375},\\n}\\n\\n\",\"author_short\":[\"Kozakov, A. T.\",\"Kochur, A. G.\",\"Googlev, K. A.\",\"Nikolskii, A. V.\",\"Torgashev, V. I.\",\"Shevcova, S. I.\"],\"key\":\"kozakov_fine_2015\",\"id\":\"kozakov_fine_2015\",\"bibbaseid\":\"kozakov-kochur-googlev-nikolskii-torgashev-shevcova-finestructureofthexrayphotoelectronni2textrmpspectruminnitextrm1xcotextrmxcrtextrm2otextrm4compounds-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.3103/S106287381511012X\"},\"keyword\":[\"Cr2O4 Solid Solution\",\"Divalent Nickel\",\"Hedral Position\",\"Octahedral Crystal Field\",\"Octahedral Position\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Emergence of the sub-THz central peak at phase transitions in artificial BaTiO$_{\\\\textrm{3}}$/(Ba,Sr)TiO$_{\\\\textrm{3}}$ superlattices\",\"volume\":\"9\",\"copyright\":\"© 2015 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim\",\"issn\":\"1862-6270\",\"url\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssr.201409505\",\"doi\":\"10.1002/pssr.201409505\",\"abstract\":\"A prominent central peak in the sub-THz frequency range was observed in the Raman spectra of BaTiO3/(Ba,Sr)TiO3 (BT/BST) superlattice grown on (001)MgO substrate. Both soft and central mode show an anomaly around 200 K and 280 K, which can be correlated with orthorhombic to monoclinic phase transition of BST and BT, respectively. The observed temperature dependence of the central mode enabled us to explain rather broad temperature dependence of the dielectric permittivity previously observed in BT/BST superlattices. (© 2015 WILEY-VCH Verlag GmbH &Co. KGaA, Weinheim)\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"physica status solidi (RRL) – Rapid Research Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Tikhonov\"],\"firstnames\":[\"Yu.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zakharchenko\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ortega\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kumar\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"R.\",\"S.\"],\"suffixes\":[]}],\"year\":\"2015\",\"note\":\"_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssr.201409505\",\"keywords\":\"Raman spectroscopy, ferroelectrics, BaTiO3, phase transitions, soft mode, superlattices\",\"pages\":\"68–71\",\"bibtex\":\"@article{tikhonov_emergence_2015,\\n\\ttitle = {Emergence of the sub-{THz} central peak at phase transitions in artificial {BaTiO}$_{\\\\textrm{3}}$/({Ba},{Sr}){TiO}$_{\\\\textrm{3}}$ superlattices},\\n\\tvolume = {9},\\n\\tcopyright = {© 2015 WILEY-VCH Verlag GmbH \\\\& Co. KGaA, Weinheim},\\n\\tissn = {1862-6270},\\n\\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssr.201409505},\\n\\tdoi = {10.1002/pssr.201409505},\\n\\tabstract = {A prominent central peak in the sub-THz frequency range was observed in the Raman spectra of BaTiO3/(Ba,Sr)TiO3 (BT/BST) superlattice grown on (001)MgO substrate. Both soft and central mode show an anomaly around 200 K and 280 K, which can be correlated with orthorhombic to monoclinic phase transition of BST and BT, respectively. The observed temperature dependence of the central mode enabled us to explain rather broad temperature dependence of the dielectric permittivity previously observed in BT/BST superlattices. (© 2015 WILEY-VCH Verlag GmbH \\\\&Co. KGaA, Weinheim)},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {physica status solidi (RRL) – Rapid Research Letters},\\n\\tauthor = {Tikhonov, Yu. A. and Razumnaya, A. G. and Torgashev, V. I. and Zakharchenko, I. N. and Yuzyuk, Yu. I. and El Marssi, M. and Ortega, N. and Kumar, A. and Katiyar, R. S.},\\n\\tyear = {2015},\\n\\tnote = {\\\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssr.201409505},\\n\\tkeywords = {Raman spectroscopy, ferroelectrics, BaTiO3, phase transitions, soft mode, superlattices},\\n\\tpages = {68--71},\\n}\\n\\n\",\"author_short\":[\"Tikhonov, Y. A.\",\"Razumnaya, A. G.\",\"Torgashev, V. I.\",\"Zakharchenko, I. N.\",\"Yuzyuk, Y. I.\",\"El Marssi, M.\",\"Ortega, N.\",\"Kumar, A.\",\"Katiyar, R. S.\"],\"key\":\"tikhonov_emergence_2015\",\"id\":\"tikhonov_emergence_2015\",\"bibbaseid\":\"tikhonov-razumnaya-torgashev-zakharchenko-yuzyuk-elmarssi-ortega-kumar-etal-emergenceofthesubthzcentralpeakatphasetransitionsinartificialbatiotextrm3basrtiotextrm3superlattices-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssr.201409505\"},\"keyword\":[\"Raman spectroscopy\",\"ferroelectrics\",\"BaTiO3\",\"phase transitions\",\"soft mode\",\"superlattices\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Electrochemically Synthesized Pt/Al$_{\\\\textrm{2}}$O$_{\\\\textrm{3}}$ Oxidation Catalysts\",\"volume\":\"146\",\"issn\":\"1572-879X\",\"url\":\"https://doi.org/10.1007/s10562-015-1651-z\",\"doi\":\"10.1007/s10562-015-1651-z\",\"abstract\":\"Pt/γ–Al2O3 catalysts made by fast and simple electrochemical dispersion method were characterized using X-ray absorption spectroscopy, CO chemisorption, transmission electron microscopy and X-ray diffraction, and compared with an impregnated catalyst with respect to oxidation of CO and NO. A combination of techniques revealed average particle sizes of 3–4 nm for 0.81–3.8 wt% Pt/γ–Al2O3 catalysts. Electrochemically prepared materials demonstrated catalytic activity comparable to that of conventional impregnated catalyst and reasonable stability.\",\"language\":\"en\",\"number\":\"2\",\"urldate\":\"2023-11-11\",\"journal\":\"Catalysis Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Doronkin\"],\"firstnames\":[\"Dmitry\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kuriganova\"],\"firstnames\":[\"Aleksandra\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Leontyev\"],\"firstnames\":[\"Igor\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Baier\"],\"firstnames\":[\"Sina\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lichtenberg\"],\"firstnames\":[\"Henning\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnova\"],\"firstnames\":[\"Nina\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Grunwaldt\"],\"firstnames\":[\"Jan-Dierk\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2016\",\"keywords\":\"DOC, Electrochemical dispersion, Oxidation, Platinum\",\"pages\":\"452–463\",\"bibtex\":\"@article{doronkin_electrochemically_2016,\\n\\ttitle = {Electrochemically {Synthesized} {Pt}/{Al}$_{\\\\textrm{2}}${O}$_{\\\\textrm{3}}$ {Oxidation} {Catalysts}},\\n\\tvolume = {146},\\n\\tissn = {1572-879X},\\n\\turl = {https://doi.org/10.1007/s10562-015-1651-z},\\n\\tdoi = {10.1007/s10562-015-1651-z},\\n\\tabstract = {Pt/γ–Al2O3 catalysts made by fast and simple electrochemical dispersion method were characterized using X-ray absorption spectroscopy, CO chemisorption, transmission electron microscopy and X-ray diffraction, and compared with an impregnated catalyst with respect to oxidation of CO and NO. A combination of techniques revealed average particle sizes of 3–4 nm for 0.81–3.8 wt\\\\% Pt/γ–Al2O3 catalysts. Electrochemically prepared materials demonstrated catalytic activity comparable to that of conventional impregnated catalyst and reasonable stability.},\\n\\tlanguage = {en},\\n\\tnumber = {2},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Catalysis Letters},\\n\\tauthor = {Doronkin, Dmitry E. and Kuriganova, Aleksandra B. and Leontyev, Igor N. and Baier, Sina and Lichtenberg, Henning and Smirnova, Nina V. and Grunwaldt, Jan-Dierk},\\n\\tmonth = feb,\\n\\tyear = {2016},\\n\\tkeywords = {DOC, Electrochemical dispersion, Oxidation, Platinum},\\n\\tpages = {452--463},\\n}\\n\\n\",\"author_short\":[\"Doronkin, D. E.\",\"Kuriganova, A. B.\",\"Leontyev, I. N.\",\"Baier, S.\",\"Lichtenberg, H.\",\"Smirnova, N. V.\",\"Grunwaldt, J.\"],\"key\":\"doronkin_electrochemically_2016\",\"id\":\"doronkin_electrochemically_2016\",\"bibbaseid\":\"doronkin-kuriganova-leontyev-baier-lichtenberg-smirnova-grunwaldt-electrochemicallysynthesizedptaltextrm2otextrm3oxidationcatalysts-2016\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://doi.org/10.1007/s10562-015-1651-z\"},\"keyword\":[\"DOC\",\"Electrochemical dispersion\",\"Oxidation\",\"Platinum\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Direct transition from the rhombohedral ferroelectric to the paraelectric phase in a (Ba,Sr)TiO$_{\\\\textrm{3}}$ thin film on a (111)MgO substrate\",\"volume\":\"112\",\"issn\":\"0295-5075\",\"url\":\"https://dx.doi.org/10.1209/0295-5075/112/47001\",\"doi\":\"10.1209/0295-5075/112/47001\",\"abstract\":\"A heteroepitaxial (200 nm thick) (BST) thin film was deposited on a (111)MgO substrate using rf sputtering. X-ray diffraction examinations confirmed epitaxial growth and rhombohedral symmetry of the film ( and ) at room temperature. Polarized Raman spectra of the film were studied in the temperature range from 100 to 420 K. In contrast to a BST thin film grown on (001)MgO, the observed linear temperature dependence of the squared soft mode frequency suggests the displacive character of the ferroelectric-paraelectric phase transition in a BST thin film on (111)MgO.\",\"language\":\"en\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Europhysics Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Anokhin\"],\"firstnames\":[\"A.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lyanguzov\"],\"firstnames\":[\"N.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Stryukov\"],\"firstnames\":[\"D.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bunina\"],\"firstnames\":[\"O.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golovko\"],\"firstnames\":[\"Yu\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mukhortov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Marssi\"],\"firstnames\":[\"M.\",\"El\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2015\",\"note\":\"Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica\",\"pages\":\"47001\",\"bibtex\":\"@article{anokhin_direct_2015,\\n\\ttitle = {Direct transition from the rhombohedral ferroelectric to the paraelectric phase in a ({Ba},{Sr}){TiO}$_{\\\\textrm{3}}$ thin film on a (111){MgO} substrate},\\n\\tvolume = {112},\\n\\tissn = {0295-5075},\\n\\turl = {https://dx.doi.org/10.1209/0295-5075/112/47001},\\n\\tdoi = {10.1209/0295-5075/112/47001},\\n\\tabstract = {A heteroepitaxial (200 nm thick) (BST) thin film was deposited on a (111)MgO substrate using rf sputtering. X-ray diffraction examinations confirmed epitaxial growth and rhombohedral symmetry of the film ( and ) at room temperature. Polarized Raman spectra of the film were studied in the temperature range from 100 to 420 K. In contrast to a BST thin film grown on (001)MgO, the observed linear temperature dependence of the squared soft mode frequency suggests the displacive character of the ferroelectric-paraelectric phase transition in a BST thin film on (111)MgO.},\\n\\tlanguage = {en},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Europhysics Letters},\\n\\tauthor = {Anokhin, A. S. and Yuzyuk, Yu I. and Lyanguzov, N. V. and Razumnaya, A. G. and Stryukov, D. V. and Bunina, O. A. and Golovko, Yu I. and Shirokov, V. B. and Mukhortov, V. M. and Marssi, M. El},\\n\\tmonth = nov,\\n\\tyear = {2015},\\n\\tnote = {Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica},\\n\\tpages = {47001},\\n}\\n\\n\",\"author_short\":[\"Anokhin, A. S.\",\"Yuzyuk, Y. I.\",\"Lyanguzov, N. V.\",\"Razumnaya, A. G.\",\"Stryukov, D. V.\",\"Bunina, O. A.\",\"Golovko, Y. I.\",\"Shirokov, V. B.\",\"Mukhortov, V. M.\",\"Marssi, M. E.\"],\"key\":\"anokhin_direct_2015\",\"id\":\"anokhin_direct_2015\",\"bibbaseid\":\"anokhin-yuzyuk-lyanguzov-razumnaya-stryukov-bunina-golovko-shirokov-etal-directtransitionfromtherhombohedralferroelectrictotheparaelectricphaseinabasrtiotextrm3thinfilmona111mgosubstrate-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1209/0295-5075/112/47001\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Control of acoustic properties of a BaTiO$_{\\\\textrm{3}}$ thin film by a planar electric field\",\"volume\":\"111\",\"issn\":\"0295-5075\",\"url\":\"https://dx.doi.org/10.1209/0295-5075/111/16002\",\"doi\":\"10.1209/0295-5075/111/16002\",\"abstract\":\"An influence of a planar electric field on material coefficients of a barium titanate film has been studied. Electric-field dependences of dielectric constants, elastic and piezoelectric moduli were built for the (001)-oriented film on a cubic substrate with a misfit strain value equal to . It was revealed that an electromechanical coupling coefficient, k11, has a maximum at some value of the electric field, which depends on the clamping stress. The misfit strain dependence of the maximum value of the k11 coefficient was studied at strains below (c-phase).\",\"language\":\"en\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Europhysics Letters\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"Vladimir\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kalinchuk\"],\"firstnames\":[\"Valery\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shakhovoy\"],\"firstnames\":[\"Roman\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yury\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2015\",\"note\":\"Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica\",\"pages\":\"16002\",\"bibtex\":\"@article{shirokov_control_2015,\\n\\ttitle = {Control of acoustic properties of a {BaTiO}$_{\\\\textrm{3}}$ thin film by a planar electric field},\\n\\tvolume = {111},\\n\\tissn = {0295-5075},\\n\\turl = {https://dx.doi.org/10.1209/0295-5075/111/16002},\\n\\tdoi = {10.1209/0295-5075/111/16002},\\n\\tabstract = {An influence of a planar electric field on material coefficients of a barium titanate film has been studied. Electric-field dependences of dielectric constants, elastic and piezoelectric moduli were built for the (001)-oriented film on a cubic substrate with a misfit strain value equal to . It was revealed that an electromechanical coupling coefficient, k11, has a maximum at some value of the electric field, which depends on the clamping stress. The misfit strain dependence of the maximum value of the k11 coefficient was studied at strains below (c-phase).},\\n\\tlanguage = {en},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Europhysics Letters},\\n\\tauthor = {Shirokov, Vladimir and Kalinchuk, Valery and Shakhovoy, Roman and Yuzyuk, Yury},\\n\\tmonth = jul,\\n\\tyear = {2015},\\n\\tnote = {Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica},\\n\\tpages = {16002},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V.\",\"Kalinchuk, V.\",\"Shakhovoy, R.\",\"Yuzyuk, Y.\"],\"key\":\"shirokov_control_2015\",\"id\":\"shirokov_control_2015\",\"bibbaseid\":\"shirokov-kalinchuk-shakhovoy-yuzyuk-controlofacousticpropertiesofabatiotextrm3thinfilmbyaplanarelectricfield-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://dx.doi.org/10.1209/0295-5075/111/16002\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"series\":\"Proceedings of the 16th International Conference on the Physics of Light–Matter Coupling in Nanostructures, PLMCN 2015 (Medellín, Colombia), 3-8 February, 2015\",\"title\":\"Coexistence of the soft mode and sub-THz central peak in ferroelectric BaTiO$_{\\\\textrm{3}}$/(Ba,Sr)TiO$_{\\\\textrm{3}}$ superlattices\",\"volume\":\"87\",\"issn\":\"0749-6036\",\"url\":\"https://www.sciencedirect.com/science/article/pii/S0749603615301117\",\"doi\":\"10.1016/j.spmi.2015.07.038\",\"abstract\":\"Near- and sub-Terahertz dynamics of soft and Debye-type central modes was studied by the polarized Raman spectroscopy in ferroelectric BaTiO3/Ba0.3Sr0.7TiO3 (BT/BST) superlattice in the temperature range of 80–400K where system undergoes the series of phase transitions: paraelectric-tetragonal–monoclinic in BT layers and paraelectric-orthorhombic-monoclinic in BST layers. It was shown that temperature evolution of these modes can be described within the model of coexisted damped harmonic oscillator and Debye relaxator. The occurrence of the pronounced central mode can explain the recently observed relaxor-like dielectric anomaly in such superlattice.\",\"urldate\":\"2023-11-11\",\"journal\":\"Superlattices and Microstructures\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Razumnaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Tikhonov\"],\"firstnames\":[\"Yu.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Yuzyuk\"],\"firstnames\":[\"Yu.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zakharchenko\"],\"firstnames\":[\"I.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"V.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ortega\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kumar\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"R.\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Lukyanchuk\"],\"firstnames\":[\"I.\",\"A.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2015\",\"keywords\":\"Ferroelectrics, Raman spectroscopy, Debye relaxator, Phase transitions, Soft mode, Superlattice\",\"pages\":\"19–24\",\"bibtex\":\"@article{razumnaya_coexistence_2015,\\n\\tseries = {Proceedings of the 16th {International} {Conference} on the {Physics} of {Light}–{Matter} {Coupling} in {Nanostructures}, {PLMCN} 2015 ({Medellín}, {Colombia}), 3-8 {February}, 2015},\\n\\ttitle = {Coexistence of the soft mode and sub-{THz} central peak in ferroelectric {BaTiO}$_{\\\\textrm{3}}$/({Ba},{Sr}){TiO}$_{\\\\textrm{3}}$ superlattices},\\n\\tvolume = {87},\\n\\tissn = {0749-6036},\\n\\turl = {https://www.sciencedirect.com/science/article/pii/S0749603615301117},\\n\\tdoi = {10.1016/j.spmi.2015.07.038},\\n\\tabstract = {Near- and sub-Terahertz dynamics of soft and Debye-type central modes was studied by the polarized Raman spectroscopy in ferroelectric BaTiO3/Ba0.3Sr0.7TiO3 (BT/BST) superlattice in the temperature range of 80–400K where system undergoes the series of phase transitions: paraelectric-tetragonal–monoclinic in BT layers and paraelectric-orthorhombic-monoclinic in BST layers. It was shown that temperature evolution of these modes can be described within the model of coexisted damped harmonic oscillator and Debye relaxator. The occurrence of the pronounced central mode can explain the recently observed relaxor-like dielectric anomaly in such superlattice.},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Superlattices and Microstructures},\\n\\tauthor = {Razumnaya, A. G. and Tikhonov, Yu. A. and Yuzyuk, Yu. I. and Zakharchenko, I. N. and Torgashev, V. I. and Ortega, N. and Kumar, A. and Katiyar, R. S. and El Marssi, M. and Lukyanchuk, I. A.},\\n\\tmonth = nov,\\n\\tyear = {2015},\\n\\tkeywords = {Ferroelectrics, Raman spectroscopy, Debye relaxator, Phase transitions, Soft mode, Superlattice},\\n\\tpages = {19--24},\\n}\\n\\n\",\"author_short\":[\"Razumnaya, A. G.\",\"Tikhonov, Y. A.\",\"Yuzyuk, Y. I.\",\"Zakharchenko, I. N.\",\"Torgashev, V. I.\",\"Ortega, N.\",\"Kumar, A.\",\"Katiyar, R. S.\",\"El Marssi, M.\",\"Lukyanchuk, I. A.\"],\"key\":\"razumnaya_coexistence_2015\",\"id\":\"razumnaya_coexistence_2015\",\"bibbaseid\":\"razumnaya-tikhonov-yuzyuk-zakharchenko-torgashev-ortega-kumar-katiyar-etal-coexistenceofthesoftmodeandsubthzcentralpeakinferroelectricbatiotextrm3basrtiotextrm3superlattices-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.sciencedirect.com/science/article/pii/S0749603615301117\"},\"keyword\":[\"Ferroelectrics\",\"Raman spectroscopy\",\"Debye relaxator\",\"Phase transitions\",\"Soft mode\",\"Superlattice\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Фазовые переходы в двух- и трехкомпонентных сверхрешетках перовскитов\",\"volume\":\"57\",\"url\":\"http://journals.ioffe.ru/articles/41506\",\"abstract\":\"Исследовано температурное поведение поляризационных спектров комбинационного рассеяния света двухслойной BaTiO3/Ba0.5Sr0.5TiO3 и трехслойной BaTiO3/Ba0.5Sr0.5TiO3/SrTiO3 сверхрешеток, полученных методом импульсного лазерного напыления на подложках (001)MgO. Установлено, что в трехслойной сверхрешетке частота мягкой моды E(TO) при комнатной температуре значительно выше (94 cm-1), чем в двухслойной (70 cm-1), что свидетельствует об увеличении двумерных напряжений в эпитаксиальных слоях трехслойной сверхрешетки. Анализ температурной зависимости интегральной интенсивности мягкой моды E(TO) позволяет предполагать, что в сверхрешетке BaTiO3/Ba0.5Sr0.5TiO3 переход из сегнетоэлектрической в параэлектрическую фазу происходит при ~540 K, а в сверхрешетке BaTiO3/Ba0.5Sr0.5TiO3/SrTiO3 температура фазового перехода повышается до ~ 610 K из-за деформаций эпитаксиальных слоев. Работа выполнена за счет гранта Российского научного фонда (проект N 14-12-00258).\",\"language\":\"ru\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Тихонов\"],\"firstnames\":[\"Ю.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Разумная\"],\"firstnames\":[\"А.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Маслова\"],\"firstnames\":[\"О.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Захарченко\"],\"firstnames\":[\"И.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ortega\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kumar\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"R.\",\"S.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2015\",\"pages\":\"475–480\",\"bibtex\":\"@article{__2015-2,\\n\\ttitle = {Фазовые переходы в двух- и трехкомпонентных сверхрешетках перовскитов},\\n\\tvolume = {57},\\n\\turl = {http://journals.ioffe.ru/articles/41506},\\n\\tabstract = {Исследовано температурное поведение поляризационных спектров комбинационного рассеяния света двухслойной BaTiO3/Ba0.5Sr0.5TiO3 и трехслойной BaTiO3/Ba0.5Sr0.5TiO3/SrTiO3 сверхрешеток, полученных методом импульсного лазерного напыления на подложках (001)MgO. Установлено, что в трехслойной сверхрешетке частота мягкой моды E(TO) при комнатной температуре значительно выше (94 cm-1), чем в двухслойной (70 cm-1), что свидетельствует об увеличении двумерных напряжений в эпитаксиальных слоях трехслойной сверхрешетки. Анализ температурной зависимости интегральной интенсивности мягкой моды E(TO) позволяет предполагать, что в сверхрешетке BaTiO3/Ba0.5Sr0.5TiO3 переход из сегнетоэлектрической в параэлектрическую фазу происходит при {\\\\textasciitilde}540 K, а в сверхрешетке BaTiO3/Ba0.5Sr0.5TiO3/SrTiO3 температура фазового перехода повышается до {\\\\textasciitilde} 610 K из-за деформаций эпитаксиальных слоев. Работа выполнена за счет гранта Российского научного фонда (проект N 14-12-00258).},\\n\\tlanguage = {ru},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Тихонов, Ю. А. and Разумная, А. Г. and Маслова, О. А. and Захарченко, И. Н. and Юзюк, Ю. И. and Ortega, N. and Kumar, A. and Katiyar, R. S.},\\n\\tmonth = feb,\\n\\tyear = {2015},\\n\\tpages = {475--480},\\n}\\n\\n\",\"author_short\":[\"Тихонов, Ю. А.\",\"Разумная, А. Г.\",\"Маслова, О. А.\",\"Захарченко, И. Н.\",\"Юзюк, Ю. И.\",\"Ortega, N.\",\"Kumar, A.\",\"Katiyar, R. S.\"],\"key\":\"__2015-2\",\"id\":\"__2015-2\",\"bibbaseid\":\"-----ortega-kumar-katiyar--2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/41506\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Зависимость свойств эпитаксиальных тонких пленок титаната бария-стронция при изменении толщины\",\"volume\":\"57\",\"url\":\"Зависимость свойств эпитаксиальных тонких пленок титаната бария-стронция при изменении толщины\",\"abstract\":\"Проведены исследования гетероэпитаксиальных тонких пленок BaxSr1-xTiO3 различной толщины в параэлектрической фазе при температуре 600oC. Параметры решетки пленки показывают нелинейную зависимость от толщины. С уменьшением толщины происходит увеличение вынужденной деформации и увеличивается объем элементарной ячейки. Поведение вынужденной деформации при изменении толщины хорошо описывается в модели двойного электрического слоя, образовавшегося в процессе синтеза пленки на границе с подложкой. Работа выполнена при поддержке РФФИ (гранты N 13-02-00251а, 13-02-12085-ОФИ_М и 13-01-90619 Арм_а).\",\"language\":\"ru\",\"number\":\"8\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Janolin\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dkhil\"],\"firstnames\":[\"B.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2015\",\"pages\":\"1503–1508\",\"bibtex\":\"@article{__2015-3,\\n\\ttitle = {Зависимость свойств эпитаксиальных тонких пленок титаната бария-стронция при изменении толщины},\\n\\tvolume = {57},\\n\\turl = {Зависимость свойств эпитаксиальных тонких пленок титаната бария-стронция при изменении толщины},\\n\\tabstract = {Проведены исследования гетероэпитаксиальных тонких пленок BaxSr1-xTiO3 различной толщины в параэлектрической фазе при температуре 600oC. Параметры решетки пленки показывают нелинейную зависимость от толщины. С уменьшением толщины происходит увеличение вынужденной деформации и увеличивается объем элементарной ячейки. Поведение вынужденной деформации при изменении толщины хорошо описывается в модели двойного электрического слоя, образовавшегося в процессе синтеза пленки на границе с подложкой. Работа выполнена при поддержке РФФИ (гранты N 13-02-00251а, 13-02-12085-ОФИ\\\\_М и 13-01-90619 Арм\\\\_а).},\\n\\tlanguage = {ru},\\n\\tnumber = {8},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Широков, В. Б. and Головко, Ю. И. and Мухортов, В. М. and Юзюк, Ю. И. and Janolin, P. E. and Dkhil, B.},\\n\\tmonth = jul,\\n\\tyear = {2015},\\n\\tpages = {1503--1508},\\n}\\n\\n\",\"author_short\":[\"Широков, В. Б.\",\"Головко, Ю. И.\",\"Мухортов, В. М.\",\"Юзюк, Ю. И.\",\"Janolin, P. E.\",\"Dkhil, B.\"],\"key\":\"__2015-3\",\"id\":\"__2015-3\",\"bibbaseid\":\"----janolin-dkhil--2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://bibbase.org/f/NkS9m4R3ieFPicBbH/Зависимость%20свойств%20эпитаксиальных%20тонких%20пленок%20титаната%20бария-стронция%20при%20изменении%20толщины\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Структуры капсидов сферических вирусов как квазикристаллические укладки\",\"volume\":\"57\",\"url\":\"http://journals.ioffe.ru/articles/41613\",\"abstract\":\"Рассматрены вирусные сферические оболочки с икосаэдрической симметрией как квазикристаллические укладки. Аналогично известной теории квазиэквивалентности Каспара и Клуга данный подход также минимизирует количество конформаций, необходимых белковой молекуле для образования связей с соседями в оболочке, но основан на отличных геометрических принципах. Предполагается, что центры белковых молекул находятся в вершинах плиток с одинаковыми ребрами, а количество разных сортов плиток минимально. Получены идеализированные координаты симметрийно-неэквивалентных позиций протеинов в шести различных типах капсидов. Подход описывает единообразно как структуры, удовлетворяющие хорошо известной геометрической модели Каспара и Клуга, так и противоречащие ей. Работа выполнена при поддержке РФФИ (грант N 13-02-12085офи_м). В.Л. благодарит Labex NUMEV за финансовую поддержку.\",\"language\":\"ru\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Коневцова\"],\"firstnames\":[\"О.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лорман\"],\"firstnames\":[\"В.\",\"Л.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Рошаль\"],\"firstnames\":[\"С.\",\"Б.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2015\",\"pages\":\"790–795\",\"bibtex\":\"@article{__2015-4,\\n\\ttitle = {Структуры капсидов сферических вирусов как квазикристаллические укладки},\\n\\tvolume = {57},\\n\\turl = {http://journals.ioffe.ru/articles/41613},\\n\\tabstract = {Рассматрены вирусные сферические оболочки с икосаэдрической симметрией как квазикристаллические укладки. Аналогично известной теории квазиэквивалентности Каспара и Клуга данный подход также минимизирует количество конформаций, необходимых белковой молекуле для образования связей с соседями в оболочке, но основан на отличных геометрических принципах. Предполагается, что центры белковых молекул находятся в вершинах плиток с одинаковыми ребрами, а количество разных сортов плиток минимально. Получены идеализированные координаты симметрийно-неэквивалентных позиций протеинов в шести различных типах капсидов. Подход описывает единообразно как структуры, удовлетворяющие хорошо известной геометрической модели Каспара и Клуга, так и противоречащие ей. Работа выполнена при поддержке РФФИ (грант N 13-02-12085офи\\\\_м). В.Л. благодарит Labex NUMEV за финансовую поддержку.},\\n\\tlanguage = {ru},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Коневцова, О. В. and Лорман, В. Л. and Рошаль, С. Б.},\\n\\tmonth = mar,\\n\\tyear = {2015},\\n\\tpages = {790--795},\\n}\\n\\n\",\"author_short\":[\"Коневцова, О. В.\",\"Лорман, В. Л.\",\"Рошаль, С. Б.\"],\"key\":\"__2015-4\",\"id\":\"__2015-4\",\"bibbaseid\":\"----2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/41613\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Материальные константы тонких пленок титаната бария\",\"volume\":\"57\",\"url\":\"http://journals.ioffe.ru/articles/42109\",\"abstract\":\"Нелинейные свойства титаната бария приводят к изменению материальных постоянных линейных уравнений пьезоэффекта для тонких пленок. На основе потенциала Ландау феноменологической теории исследовано поведение материальных постоянных монокристаллических тонких пленок титаната бария при комнатной температуре в зависимости от величины вынужденной деформации. Большинство материальных постоянных при изменении деформации испытывают аномалии на границах фаз. Внутри r-фазы некоторые упругие и электроупругие постоянные достигают экстремума. Полученные результаты позволяют определить направление поиска для получения пленок с необходимыми свойствами. Работа выполнена при финансовой поддержке Российского научного фонда, грант N 14-19-01676.\",\"language\":\"ru\",\"number\":\"8\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Калинчук\"],\"firstnames\":[\"В.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Шаховой\"],\"firstnames\":[\"Р.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]}],\"month\":\"July\",\"year\":\"2015\",\"pages\":\"1509–1514\",\"bibtex\":\"@article{__2015-5,\\n\\ttitle = {Материальные константы тонких пленок титаната бария},\\n\\tvolume = {57},\\n\\turl = {http://journals.ioffe.ru/articles/42109},\\n\\tabstract = {Нелинейные свойства титаната бария приводят к изменению материальных постоянных линейных уравнений пьезоэффекта для тонких пленок. На основе потенциала Ландау феноменологической теории исследовано поведение материальных постоянных монокристаллических тонких пленок титаната бария при комнатной температуре в зависимости от величины вынужденной деформации. Большинство материальных постоянных при изменении деформации испытывают аномалии на границах фаз. Внутри r-фазы некоторые упругие и электроупругие постоянные достигают экстремума. Полученные результаты позволяют определить направление поиска для получения пленок с необходимыми свойствами. Работа выполнена при финансовой поддержке Российского научного фонда, грант N 14-19-01676.},\\n\\tlanguage = {ru},\\n\\tnumber = {8},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Широков, В. Б. and Калинчук, В. В. and Шаховой, Р. А. and Юзюк, Ю. И.},\\n\\tmonth = jul,\\n\\tyear = {2015},\\n\\tpages = {1509--1514},\\n}\\n\\n\",\"author_short\":[\"Широков, В. Б.\",\"Калинчук, В. В.\",\"Шаховой, Р. А.\",\"Юзюк, Ю. И.\"],\"key\":\"__2015-5\",\"id\":\"__2015-5\",\"bibbaseid\":\"-----2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/42109\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Критическое рассеяние синхротронного излучения в цирконате-титанате свинца с малой концентрацией титана\",\"volume\":\"57\",\"url\":\"http://journals.ioffe.ru/articles/42491\",\"abstract\":\"Методом рассеяния синхротронного излучения исследовано диффузное рассеяние в монокристалле цирконата-титаната свинца с концентрацией титана 0.7 at.%. Измерения проводились как в окрестности центра зоны Бриллюэна, так и в M-точке. В параэлектрической фазе вблизи центра зоны Бриллюэна выявлено сильно анизотропное диффузное рассеяние, анизотропия диффузного рассеяния сходна с наблюдаемой ранее в чистом цирконате свинца. Температурная зависимость этого диффузного рассеяния имеет критический вид с температурой Tc~ 480 K. Диффузное рассеяние в окрестности M-точки слабо зависит от температуры, причем эта зависимость имеет различный характер в M-точках с различными индексами. Д.А. Андроникова благодарит за финансовую поддержку Правительство РФ (грант N 14.Б25.31.0025), С.Б. Вахрушев и Ю.А. Бронвальд благодарят РФФИ за финансовую поддержу в рамках научного проекта N 14-02-01208.\",\"language\":\"ru\",\"number\":\"12\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Андроникова\"],\"firstnames\":[\"Д.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Босак\"],\"firstnames\":[\"А.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бронвальд\"],\"firstnames\":[\"Ю.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бурковский\"],\"firstnames\":[\"Р.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Вахрушев\"],\"firstnames\":[\"С.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Леонтьев\"],\"firstnames\":[\"Н.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Леонтьев\"],\"firstnames\":[\"И.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Таганцев\"],\"firstnames\":[\"А.\",\"К.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Филимонов\"],\"firstnames\":[\"А.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Чернышов\"],\"firstnames\":[\"Д.\",\"Ю.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2015\",\"pages\":\"2368–2373\",\"file\":\"Физика твердого тела:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\AKG5ZVNI\\\\\\\\42491.html:text/html\",\"bibtex\":\"@article{__2015-6,\\n\\ttitle = {Критическое рассеяние синхротронного излучения в цирконате-титанате свинца с малой концентрацией титана},\\n\\tvolume = {57},\\n\\turl = {http://journals.ioffe.ru/articles/42491},\\n\\tabstract = {Методом рассеяния синхротронного излучения исследовано диффузное рассеяние в монокристалле цирконата-титаната свинца с концентрацией титана 0.7 at.\\\\%. Измерения проводились как в окрестности центра зоны Бриллюэна, так и в M-точке. В параэлектрической фазе вблизи центра зоны Бриллюэна выявлено сильно анизотропное диффузное рассеяние, анизотропия диффузного рассеяния сходна с наблюдаемой ранее в чистом цирконате свинца. Температурная зависимость этого диффузного рассеяния имеет критический вид с температурой Tc{\\\\textasciitilde} 480 K. Диффузное рассеяние в окрестности M-точки слабо зависит от температуры, причем эта зависимость имеет различный характер в M-точках с различными индексами. Д.А. Андроникова благодарит за финансовую поддержку Правительство РФ (грант N 14.Б25.31.0025), С.Б. Вахрушев и Ю.А. Бронвальд благодарят РФФИ за финансовую поддержу в рамках научного проекта N 14-02-01208.},\\n\\tlanguage = {ru},\\n\\tnumber = {12},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Андроникова, Д. А. and Босак, А. А. and Бронвальд, Ю. А. and Бурковский, Р. Г. and Вахрушев, С. Б. and Леонтьев, Н. Г. and Леонтьев, И. Н. and Таганцев, А. К. and Филимонов, А. В. and Чернышов, Д. Ю.},\\n\\tmonth = nov,\\n\\tyear = {2015},\\n\\tpages = {2368--2373},\\n\\tfile = {Физика твердого тела:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\AKG5ZVNI\\\\\\\\42491.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Андроникова, Д. А.\",\"Босак, А. А.\",\"Бронвальд, Ю. А.\",\"Бурковский, Р. Г.\",\"Вахрушев, С. Б.\",\"Леонтьев, Н. Г.\",\"Леонтьев, И. Н.\",\"Таганцев, А. К.\",\"Филимонов, А. В.\",\"Чернышов, Д. Ю.\"],\"key\":\"__2015-6\",\"id\":\"__2015-6\",\"bibbaseid\":\"--------etal--2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/42491\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Сегнетоэлектрическая сверхрешетка на основе твердых растворов титаната бария-стронция\",\"volume\":\"57\",\"url\":\"http://journals.ioffe.ru/articles/42408\",\"abstract\":\"Сверхрешетка состава Ba0.8Sr0.2TiO3/Ba0.4Sr0.6TiO3 выращена методом высокочастотного катодного распыления на подложке (001)MgO. С помощью рентгеновской дифракции определены параметры элементарных ячеек слоев сверхрешетки по нормали к подложке, период модуляции и ориентационные соотношения между пленкой и подложкой. На основе температурной зависимости поляризованных спектров комбинационного рассеяния света обнаружено, что наблюдается ужесточение мягкой моды E(TO) от 79 до 97 cm-1 в интервале температур 80-350 K. Характерных признаков последовательности фазовых переходов, которые имеют место в объемных образцах твердых растворов титаната бария-стронция аналогичных составов, не обнаружено, а переход из сегнетоэлектрической в параэлектрическую фазу в сверхрешетке происходит при температуре ~350 K. Работа выполнена за счет средств Российского научного фонда (проект N 14-12-00258).\",\"language\":\"ru\",\"number\":\"11\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Разумная\"],\"firstnames\":[\"А.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Головко\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Мухортов\"],\"firstnames\":[\"В.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2015\",\"pages\":\"2181–2185\",\"bibtex\":\"@article{__2015-7,\\n\\ttitle = {Сегнетоэлектрическая сверхрешетка на основе твердых растворов титаната бария-стронция},\\n\\tvolume = {57},\\n\\turl = {http://journals.ioffe.ru/articles/42408},\\n\\tabstract = {Сверхрешетка состава Ba0.8Sr0.2TiO3/Ba0.4Sr0.6TiO3 выращена методом высокочастотного катодного распыления на подложке (001)MgO. С помощью рентгеновской дифракции определены параметры элементарных ячеек слоев сверхрешетки по нормали к подложке, период модуляции и ориентационные соотношения между пленкой и подложкой. На основе температурной зависимости поляризованных спектров комбинационного рассеяния света обнаружено, что наблюдается ужесточение мягкой моды E(TO) от 79 до 97 cm-1 в интервале температур 80-350 K. Характерных признаков последовательности фазовых переходов, которые имеют место в объемных образцах твердых растворов титаната бария-стронция аналогичных составов, не обнаружено, а переход из сегнетоэлектрической в параэлектрическую фазу в сверхрешетке происходит при температуре {\\\\textasciitilde}350 K. Работа выполнена за счет средств Российского научного фонда (проект N 14-12-00258).},\\n\\tlanguage = {ru},\\n\\tnumber = {11},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Разумная, А. Г. and Головко, Ю. И. and Лянгузов, Н. В. and Юзюк, Ю. И. and Широков, В. Б. and Мухортов, В. М. and El Marssi, M.},\\n\\tmonth = oct,\\n\\tyear = {2015},\\n\\tpages = {2181--2185},\\n}\\n\\n\",\"author_short\":[\"Разумная, А. Г.\",\"Головко, Ю. И.\",\"Лянгузов, Н. В.\",\"Юзюк, Ю. И.\",\"Широков, В. Б.\",\"Мухортов, В. М.\",\"El Marssi, M.\"],\"key\":\"__2015-7\",\"id\":\"__2015-7\",\"bibbaseid\":\"------elmarssi--2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/42408\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Магниторезистивность стеклокомпозитов La$_{\\\\textrm{0.7}}$Sr$_{\\\\textrm{0.3}}$MnO$_{\\\\textrm{3}}$/ Sb$_{\\\\textrm{2}}$O$_{\\\\textrm{3}}$ при комнатной температуре\",\"volume\":\"57\",\"url\":\"http://journals.ioffe.ru/articles/41214\",\"abstract\":\"Синтезированы керамические композиты La0.7Sr0.3MnO3/Sb2O3 с различными массовыми соотношениями компонентов. Исследованы их магниторезистивные свойства в слабых магнитных полях. Значения отрицательной изотропной магниторезистивности при комнатной температуре для композитов 90% La0.7Sr0.3MnO3/10%Sb2O3 составляют -1.2% при 0.25 kOe и -14% при 20 kOe. Рост магниторезистивности при увеличении поля имеет черты релаксационного процесса. Работа выполнена при финансовой поддержке проекта РФФИ N 14-03-00103.\",\"language\":\"ru\",\"number\":\"1\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Кабиров\"],\"firstnames\":[\"Ю.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гавриляченко\"],\"firstnames\":[\"В.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Чупахина\"],\"firstnames\":[\"Т.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гавриляченко\"],\"firstnames\":[\"Т.\",\"В.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2014\",\"pages\":\"16–18\",\"bibtex\":\"@article{__2014-7,\\n\\ttitle = {Магниторезистивность стеклокомпозитов {La}$_{\\\\textrm{0.7}}${Sr}$_{\\\\textrm{0.3}}${MnO}$_{\\\\textrm{3}}$/ {Sb}$_{\\\\textrm{2}}${O}$_{\\\\textrm{3}}$ при комнатной температуре},\\n\\tvolume = {57},\\n\\turl = {http://journals.ioffe.ru/articles/41214},\\n\\tabstract = {Синтезированы керамические композиты La0.7Sr0.3MnO3/Sb2O3 с различными массовыми соотношениями компонентов. Исследованы их магниторезистивные свойства в слабых магнитных полях. Значения отрицательной изотропной магниторезистивности при комнатной температуре для композитов 90\\\\% La0.7Sr0.3MnO3/10\\\\%Sb2O3 составляют -1.2\\\\% при 0.25 kOe и -14\\\\% при 20 kOe. Рост магниторезистивности при увеличении поля имеет черты релаксационного процесса. Работа выполнена при финансовой поддержке проекта РФФИ N 14-03-00103.},\\n\\tlanguage = {ru},\\n\\tnumber = {1},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Чупахина, Т. И. and Гавриляченко, Т. В.},\\n\\tmonth = dec,\\n\\tyear = {2014},\\n\\tpages = {16--18},\\n}\\n\\n\",\"author_short\":[\"Кабиров, Ю. В.\",\"Гавриляченко, В. Г.\",\"Чупахина, Т. И.\",\"Гавриляченко, Т. В.\"],\"key\":\"__2014-7\",\"id\":\"__2014-7\",\"bibbaseid\":\"----latextrm07srtextrm03mnotextrm3sbtextrm2otextrm3-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/41214\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"Broadband spectroscopy of H$_{\\\\textrm{2}}$O molecule confined in nano-cages of crystal lattice: Low-energy dynamics and incipient ferroelectric behavior\",\"shorttitle\":\"Broadband spectroscopy of H2O molecule confined in nano-cages of crystal lattice\",\"url\":\"https://ieeexplore.ieee.org/document/7327553?arnumber=7327553\",\"doi\":\"10.1109/IRMMW-THz.2015.7327553\",\"abstract\":\"Broadband (1 Hz to 100 THz) dielectric response of water-containing beryl crystals was measured at temperatures from 300 K down to 0.3 K. The low-energy dynamics of H2O molecules confined within nano-cages of the crystalline lattice was studied. We observe a THz-range soft mode indicating an incipient ferroelectric behavior due to interacting dipole moments of confined water molecules.\",\"urldate\":\"2023-11-11\",\"booktitle\":\"2015 40th International Conference on Infrared, Millimeter, and Terahertz waves (IRMMW-THz)\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Torgashev\"],\"firstnames\":[\"Victor\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorshunov\"],\"firstnames\":[\"Boris\",\"P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Zhukova\"],\"firstnames\":[\"Elena\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Savinov\"],\"firstnames\":[\"Maxim\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kadlec\"],\"firstnames\":[\"Christelle\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kadlec\"],\"firstnames\":[\"Filip\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Skoromets\"],\"firstnames\":[\"Volodymyr\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokleška\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Thomas\"],\"firstnames\":[\"Victor\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fursenko\"],\"firstnames\":[\"Dmitry\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pestrjakov\"],\"firstnames\":[\"Efim\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Uskov\"],\"firstnames\":[\"Vladimir\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shakurov\"],\"firstnames\":[\"Gil'man\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kremer\"],\"firstnames\":[\"Reinhard\",\"K.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kadyrov\"],\"firstnames\":[\"Lenar\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Belyanchikov\"],\"firstnames\":[\"Mikhail\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Prokhorov\"],\"firstnames\":[\"Anatoliy\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gorelik\"],\"firstnames\":[\"Vladimir\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dressel\"],\"firstnames\":[\"Martin\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2015\",\"note\":\"ISSN: 2162-2035\",\"pages\":\"1–2\",\"bibtex\":\"@inproceedings{torgashev_broadband_2015,\\n\\ttitle = {Broadband spectroscopy of {H}$_{\\\\textrm{2}}${O} molecule confined in nano-cages of crystal lattice: {Low}-energy dynamics and incipient ferroelectric behavior},\\n\\tshorttitle = {Broadband spectroscopy of {H2O} molecule confined in nano-cages of crystal lattice},\\n\\turl = {https://ieeexplore.ieee.org/document/7327553?arnumber=7327553},\\n\\tdoi = {10.1109/IRMMW-THz.2015.7327553},\\n\\tabstract = {Broadband (1 Hz to 100 THz) dielectric response of water-containing beryl crystals was measured at temperatures from 300 K down to 0.3 K. The low-energy dynamics of H2O molecules confined within nano-cages of the crystalline lattice was studied. We observe a THz-range soft mode indicating an incipient ferroelectric behavior due to interacting dipole moments of confined water molecules.},\\n\\turldate = {2023-11-11},\\n\\tbooktitle = {2015 40th {International} {Conference} on {Infrared}, {Millimeter}, and {Terahertz} waves ({IRMMW}-{THz})},\\n\\tauthor = {Torgashev, Victor I. and Gorshunov, Boris P. and Zhukova, Elena S. and Savinov, Maxim and Kadlec, Christelle and Kadlec, Filip and Skoromets, Volodymyr and Prokleška, J. and Thomas, Victor G. and Fursenko, Dmitry A. and Pestrjakov, Efim V. and Uskov, Vladimir V. and Shakurov, Gil'man S. and Kremer, Reinhard K. and Kadyrov, Lenar S. and Belyanchikov, Mikhail A. and Prokhorov, Anatoliy S. and Gorelik, Vladimir S. and Dressel, Martin},\\n\\tmonth = aug,\\n\\tyear = {2015},\\n\\tnote = {ISSN: 2162-2035},\\n\\tpages = {1--2},\\n}\\n\\n\",\"author_short\":[\"Torgashev, V. I.\",\"Gorshunov, B. P.\",\"Zhukova, E. S.\",\"Savinov, M.\",\"Kadlec, C.\",\"Kadlec, F.\",\"Skoromets, V.\",\"Prokleška, J.\",\"Thomas, V. G.\",\"Fursenko, D. A.\",\"Pestrjakov, E. V.\",\"Uskov, V. V.\",\"Shakurov, G. S.\",\"Kremer, R. K.\",\"Kadyrov, L. S.\",\"Belyanchikov, M. A.\",\"Prokhorov, A. S.\",\"Gorelik, V. S.\",\"Dressel, M.\"],\"key\":\"torgashev_broadband_2015\",\"id\":\"torgashev_broadband_2015\",\"bibbaseid\":\"torgashev-gorshunov-zhukova-savinov-kadlec-kadlec-skoromets-prokleka-etal-broadbandspectroscopyofhtextrm2omoleculeconfinedinnanocagesofcrystallatticelowenergydynamicsandincipientferroelectricbehavior-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://ieeexplore.ieee.org/document/7327553?arnumber=7327553\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Влияние процессов самоорганизации, дефектов, примесей, а также автокаталитических процессов на параметры пленок и наностержней ZnO\",\"volume\":\"49\",\"url\":\"https://journals.ioffe.ru/articles/42455\",\"abstract\":\"Исследовано влияние параметров нанесения пленок ZnO на различные материалы подложек при использовании магнетронного распыления на переменном токе в газовой смеси аргона и кислорода. Наблюдалось явление самоорганизации, приводящее к неизменности морфологии поверхности пленок ZnO при варьировании материалов подложки и параметров нанесения. Параметры спектров макро- и микрофотолюминесценции исследованных пленок ZnO незначительно отличались от параметров спектров фотолюминесценции объемных кристаллов ZnO, полученных методом гидротермального роста. Наличие интенсивного излучения с малой величиной FWHM в разных областях спектра дает возможность рассматривать пленки ZnO, полученные магнетронным распылением, легированные РЗИ, как перспективный материал при создании оптоэлектронных приборов, работающих в широком спектральном диапазоне. Возможность реализации магнитного упорядочения при легировании РЗИ существенно расширяет функциональные возможности пленок ZnO. Параметры спектров фотолюминесценции наностержней ZnO определяются геометрическими параметрами, концентрацией и типом введенных примесей.\",\"language\":\"ru\",\"number\":\"11\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика и техника полупроводников\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Мездрогина\"],\"firstnames\":[\"М.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Еременко\"],\"firstnames\":[\"М.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Петров\"],\"firstnames\":[\"В.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Теруков\"],\"firstnames\":[\"Е.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Левицкий\"],\"firstnames\":[\"В.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2015\",\"pages\":\"1521–1530\",\"file\":\"Физика и техника полупроводников:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\5XEFAQZX\\\\\\\\42455.html:text/html\",\"bibtex\":\"@article{__2015-8,\\n\\ttitle = {Влияние процессов самоорганизации, дефектов, примесей, а также автокаталитических процессов на параметры пленок и наностержней {ZnO}},\\n\\tvolume = {49},\\n\\turl = {https://journals.ioffe.ru/articles/42455},\\n\\tabstract = {Исследовано влияние параметров нанесения пленок ZnO на различные материалы подложек при использовании магнетронного распыления на переменном токе в газовой смеси аргона и кислорода. Наблюдалось явление самоорганизации, приводящее к неизменности морфологии поверхности пленок ZnO при варьировании материалов подложки и параметров нанесения. Параметры спектров макро- и микрофотолюминесценции исследованных пленок ZnO незначительно отличались от параметров спектров фотолюминесценции объемных кристаллов ZnO, полученных методом гидротермального роста. Наличие интенсивного излучения с малой величиной FWHM в разных областях спектра дает возможность рассматривать пленки ZnO, полученные магнетронным распылением, легированные РЗИ, как перспективный материал при создании оптоэлектронных приборов, работающих в широком спектральном диапазоне. Возможность реализации магнитного упорядочения при легировании РЗИ существенно расширяет функциональные возможности пленок ZnO. Параметры спектров фотолюминесценции наностержней ZnO определяются геометрическими параметрами, концентрацией и типом введенных примесей.},\\n\\tlanguage = {ru},\\n\\tnumber = {11},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика и техника полупроводников},\\n\\tauthor = {Мездрогина, М. М. and Еременко, М. В. and Петров, В. Н. and Теруков, Е. И. and Левицкий, В. С. and Кайдашев, Е. М. and Лянгузов, Н. В.},\\n\\tmonth = oct,\\n\\tyear = {2015},\\n\\tpages = {1521--1530},\\n\\tfile = {Физика и техника полупроводников:C\\\\:\\\\\\\\Users\\\\\\\\aleks\\\\\\\\Zotero\\\\\\\\storage\\\\\\\\5XEFAQZX\\\\\\\\42455.html:text/html},\\n}\\n\\n\",\"author_short\":[\"Мездрогина, М. М.\",\"Еременко, М. В.\",\"Петров, В. Н.\",\"Теруков, Е. И.\",\"Левицкий, В. С.\",\"Кайдашев, Е. М.\",\"Лянгузов, Н. В.\"],\"key\":\"__2015-8\",\"id\":\"__2015-8\",\"bibbaseid\":\"-------zno-2015\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://journals.ioffe.ru/articles/42455\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Особенности оптических фононов в спектрах комбинационного рассеяния массива вертикальных микростержней ZnO на кремнии\",\"volume\":\"56\",\"url\":\"http://journals.ioffe.ru/articles/26806\",\"abstract\":\"Исследованы поляризованные спектры комбинационного рассеяния массива вертикальных микростержней оксида цинка, синтезированного карботермическим методом на подложке Si (001). Длина стержней составляет 9±0.5 mum, а диаметр - 210±50 nm. Рентгенографические исследования подтвердили взаимную кристаллографическую ориентацию [001]ZnO\\\\textbar\\\\textbar[001]Si в направлении нормали к плоскости подложки. В спектрах комбинационного рассеяния света стержней наблюдаются запрещенные правилами отбора для монокристалла в геометрии x(yz)x-моды A1(TO) и Ehigh2 и в геометрии x(zz)x-мода E1(LO). Обнаружены квазимоды Q(TO) и Q(LO), спектральное положение которых смещается при изменении угла падения возбуждающего излучения. Путем сравнения спектрального сдвига квазимод с экспериментальными данными для монокристалла произведена оценка интервала углов распространения возбуждающего излучения в массиве стержней, составляющего ~25o при фиксированном угле падения. Работа выполнялась при финансовой поддержке Министерства образования и науки, тема N 2.5896 \\\"Развитие методов получения и исследование свойств полупроводниковых наноструктур для создания элементов устройств нанофотоники\\\".\",\"language\":\"ru\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Лянгузов\"],\"firstnames\":[\"Н.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Анохин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Левшов\"],\"firstnames\":[\"Д.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Кайдашев\"],\"firstnames\":[\"Е.\",\"М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Захарченко\"],\"firstnames\":[\"И.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Бунина\"],\"firstnames\":[\"О.\",\"А.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2014\",\"pages\":\"542–548\",\"bibtex\":\"@article{__2014-8,\\n\\ttitle = {Особенности оптических фононов в спектрах комбинационного рассеяния массива вертикальных микростержней {ZnO} на кремнии},\\n\\tvolume = {56},\\n\\turl = {http://journals.ioffe.ru/articles/26806},\\n\\tabstract = {Исследованы поляризованные спектры комбинационного рассеяния массива вертикальных микростержней оксида цинка, синтезированного карботермическим методом на подложке Si (001). Длина стержней составляет 9±0.5 mum, а диаметр - 210±50 nm. Рентгенографические исследования подтвердили взаимную кристаллографическую ориентацию [001]ZnO{\\\\textbar}{\\\\textbar}[001]Si в направлении нормали к плоскости подложки. В спектрах комбинационного рассеяния света стержней наблюдаются запрещенные правилами отбора для монокристалла в геометрии x(yz)x-моды A1(TO) и Ehigh2 и в геометрии x(zz)x-мода E1(LO). Обнаружены квазимоды Q(TO) и Q(LO), спектральное положение которых смещается при изменении угла падения возбуждающего излучения. Путем сравнения спектрального сдвига квазимод с экспериментальными данными для монокристалла произведена оценка интервала углов распространения возбуждающего излучения в массиве стержней, составляющего {\\\\textasciitilde}25o при фиксированном угле падения. Работа выполнялась при финансовой поддержке Министерства образования и науки, тема N 2.5896 \\\"Развитие методов получения и исследование свойств полупроводниковых наноструктур для создания элементов устройств нанофотоники\\\".},\\n\\tlanguage = {ru},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Лянгузов, Н. В. and Анохин, А. С. and Левшов, Д. И. and Кайдашев, Е. М. and Юзюк, Ю. И. and Захарченко, И. Н. and Бунина, О. А.},\\n\\tmonth = feb,\\n\\tyear = {2014},\\n\\tpages = {542--548},\\n}\\n\\n\",\"author_short\":[\"Лянгузов, Н. В.\",\"Анохин, А. С.\",\"Левшов, Д. И.\",\"Кайдашев, Е. М.\",\"Юзюк, Ю. И.\",\"Захарченко, И. Н.\",\"Бунина, О. А.\"],\"key\":\"__2014-8\",\"id\":\"__2014-8\",\"bibbaseid\":\"-------zno-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/26806\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Влияние редкоземельных ионов на диэлектрический отклик в стиллвеллитовых стеклах\",\"volume\":\"56\",\"url\":\"http://journals.ioffe.ru/articles/26789\",\"abstract\":\"Проведено сравнение экспериментально полученных спектров функции диэлектрического отклика стекол состава LnBGeO5 (Ln = La, Pr, Tb, Er, Sm) в терагерцевом и инфракрасном диапазонах. Выделены полосы поглощения и установлены их вклады в диэлектрическую проницаемость, определены контуры бозонного пика и зависимость диэлектрических потерь от типа редкоземельного иона. Работа выполнена при поддержке Министерства образования и науки РФ (грант N 11.G34.31.0027) и РФФИ (грант N 11-02-00810-а).\",\"language\":\"ru\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Командин\"],\"firstnames\":[\"Г.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Торгашев\"],\"firstnames\":[\"В.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Сигаев\"],\"firstnames\":[\"В.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Савинков\"],\"firstnames\":[\"В.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лотарев\"],\"firstnames\":[\"С.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Породинков\"],\"firstnames\":[\"О.\",\"Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Спектор\"],\"firstnames\":[\"И.\",\"Е.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2014\",\"pages\":\"435–441\",\"bibtex\":\"@article{__2014-9,\\n\\ttitle = {Влияние редкоземельных ионов на диэлектрический отклик в стиллвеллитовых стеклах},\\n\\tvolume = {56},\\n\\turl = {http://journals.ioffe.ru/articles/26789},\\n\\tabstract = {Проведено сравнение экспериментально полученных спектров функции диэлектрического отклика стекол состава LnBGeO5 (Ln = La, Pr, Tb, Er, Sm) в терагерцевом и инфракрасном диапазонах. Выделены полосы поглощения и установлены их вклады в диэлектрическую проницаемость, определены контуры бозонного пика и зависимость диэлектрических потерь от типа редкоземельного иона. Работа выполнена при поддержке Министерства образования и науки РФ (грант N 11.G34.31.0027) и РФФИ (грант N 11-02-00810-а).},\\n\\tlanguage = {ru},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Командин, Г. А. and Торгашев, В. И. and Сигаев, В. Н. and Савинков, В. И. and Лотарев, С. В. and Породинков, О. Е. and Спектор, И. Е.},\\n\\tmonth = feb,\\n\\tyear = {2014},\\n\\tpages = {435--441},\\n}\\n\\n\",\"author_short\":[\"Командин, Г. А.\",\"Торгашев, В. И.\",\"Сигаев, В. Н.\",\"Савинков, В. И.\",\"Лотарев, С. В.\",\"Породинков, О. Е.\",\"Спектор, И. Е.\"],\"key\":\"__2014-9\",\"id\":\"__2014-9\",\"bibbaseid\":\"--------2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/26789\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Особенности ян-теллеровского перехода в твердых растворах Ni$_{\\\\textrm{1-x}}$Co$_{\\\\textrm{x}}$Cr$_{\\\\textrm{2}}$O$_{\\\\textrm{4}}$\",\"volume\":\"56\",\"url\":\"http://journals.ioffe.ru/articles/26843\",\"abstract\":\"Методами синхротронной порошковой рентгеновской дифракции исследована структура твердых растворов Ni1-xCоxCr2O4 в температурном интервале 90-350 K для составов с x=0; 0.005; 0.01; 0.015; 0.02; 0.1; 0.5; 0.8 и проведено уточнение их структур с помощью полнопрофильного анализа Ритвельда. На основе полученных данных построена T-x-фазовая диаграмма для твердых растворов в исследованном диапазоне температур и концентраций. Обнаруженные структурные фазовые переходы объяснены с точки зрения теории кристаллического поля и кооперативного эффекта Яна-Теллера. Оценена величина искажений полиэдров, являющихся причиной структурного фазового перехода. Обсуждается применимость феноменологической теории Ландау и возможность использования в качестве параметра порядка величины спонтанных деформаций\",\"language\":\"ru\",\"number\":\"4\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Михейкин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Чернышов\"],\"firstnames\":[\"Д.\",\"Ю.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Буш\"],\"firstnames\":[\"А.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Прохоров\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Дмитриев\"],\"firstnames\":[\"В.\",\"П.\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2014\",\"pages\":\"754–760\",\"bibtex\":\"@article{__2014-10,\\n\\ttitle = {Особенности ян-теллеровского перехода в твердых растворах {Ni}$_{\\\\textrm{1-x}}${Co}$_{\\\\textrm{x}}${Cr}$_{\\\\textrm{2}}${O}$_{\\\\textrm{4}}$},\\n\\tvolume = {56},\\n\\turl = {http://journals.ioffe.ru/articles/26843},\\n\\tabstract = {Методами синхротронной порошковой рентгеновской дифракции исследована структура твердых растворов Ni1-xCоxCr2O4 в температурном интервале 90-350 K для составов с x=0; 0.005; 0.01; 0.015; 0.02; 0.1; 0.5; 0.8 и проведено уточнение их структур с помощью полнопрофильного анализа Ритвельда. На основе полученных данных построена T-x-фазовая диаграмма для твердых растворов в исследованном диапазоне температур и концентраций. Обнаруженные структурные фазовые переходы объяснены с точки зрения теории кристаллического поля и кооперативного эффекта Яна-Теллера. Оценена величина искажений полиэдров, являющихся причиной структурного фазового перехода. Обсуждается применимость феноменологической теории Ландау и возможность использования в качестве параметра порядка величины спонтанных деформаций},\\n\\tlanguage = {ru},\\n\\tnumber = {4},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Михейкин, А. С. and Чернышов, Д. Ю. and Буш, А. А. and Прохоров, А. С. and Юзюк, Ю. И. and Дмитриев, В. П.},\\n\\tmonth = mar,\\n\\tyear = {2014},\\n\\tpages = {754--760},\\n}\\n\\n\",\"author_short\":[\"Михейкин, А. С.\",\"Чернышов, Д. Ю.\",\"Буш, А. А.\",\"Прохоров, А. С.\",\"Юзюк, Ю. И.\",\"Дмитриев, В. П.\"],\"key\":\"__2014-10\",\"id\":\"__2014-10\",\"bibbaseid\":\"------nitextrm1xcotextrmxcrtextrm2otextrm4-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/26843\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Фононные и магнонные возбуждения в спектрах комбинационного рассеяния света эпитаксиальной пленки феррита висмута\",\"volume\":\"56\",\"url\":\"http://journals.ioffe.ru/articles/41133\",\"abstract\":\"Эпитаксиальная пленка феррита висмута BiFeO3 на монокристаллической подложке (001)MgO получена методом импульсного лазерного напыления с использованием буферных слоев SrTiO3 и SrRuO3. При комнатной температуре поляризационные характеристики спектров комбинационного рассеяния света исследованной пленки BiFeO3 предполагают моноклинную симметрию. Проведены высокотемпературные (295-1100 K) исследования спектров комбинационного рассеяния света в области частот 20\\\\textlessnu\\\\textless1600 cm-1. Особое внимание уделено высокочастотной области, где наблюдаются полоса 610 cm-1, соответствующая максимуму плотности состояний магнонной ветви на границе зоны Бриллюэна, и интенсивная полоса в спектрах второго порядка с максимумом ~1250 cm-1, соответствующая плотности состояний двухмагнонных возбуждений. Установлено, что при повышении температуры интенсивность полосы ~1250 cm-1 линейно понижается и выше 650 K она отсутствует. Экстраполяция температурной зависимости интегральной интенсивности полосы 1250 cm-1 позволяет предполагать, что в данной пленке антиферромагнитный фазовый переход происходит при температуре ~670 K.\",\"language\":\"ru\",\"number\":\"12\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Кхабири\"],\"firstnames\":[\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Анохин\"],\"firstnames\":[\"А.\",\"С.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Разумная\"],\"firstnames\":[\"А.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Gueye\"],\"firstnames\":[\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Carcan\"],\"firstnames\":[\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Bouyanfif\"],\"firstnames\":[\"H.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Wolfman\"],\"firstnames\":[\"J.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Autret-Lambert\"],\"firstnames\":[\"C.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"El\",\"Marssi\"],\"firstnames\":[\"M.\"],\"suffixes\":[]}],\"month\":\"November\",\"year\":\"2014\",\"pages\":\"2420–2425\",\"bibtex\":\"@article{__2014-11,\\n\\ttitle = {Фононные и магнонные возбуждения в спектрах комбинационного рассеяния света эпитаксиальной пленки феррита висмута},\\n\\tvolume = {56},\\n\\turl = {http://journals.ioffe.ru/articles/41133},\\n\\tabstract = {Эпитаксиальная пленка феррита висмута BiFeO3 на монокристаллической подложке (001)MgO получена методом импульсного лазерного напыления с использованием буферных слоев SrTiO3 и SrRuO3. При комнатной температуре поляризационные характеристики спектров комбинационного рассеяния света исследованной пленки BiFeO3 предполагают моноклинную симметрию. Проведены высокотемпературные (295-1100 K) исследования спектров комбинационного рассеяния света в области частот 20{\\\\textless}nu{\\\\textless}1600 cm-1. Особое внимание уделено высокочастотной области, где наблюдаются полоса 610 cm-1, соответствующая максимуму плотности состояний магнонной ветви на границе зоны Бриллюэна, и интенсивная полоса в спектрах второго порядка с максимумом {\\\\textasciitilde}1250 cm-1, соответствующая плотности состояний двухмагнонных возбуждений. Установлено, что при повышении температуры интенсивность полосы {\\\\textasciitilde}1250 cm-1 линейно понижается и выше 650 K она отсутствует. Экстраполяция температурной зависимости интегральной интенсивности полосы 1250 cm-1 позволяет предполагать, что в данной пленке антиферромагнитный фазовый переход происходит при температуре {\\\\textasciitilde}670 K.},\\n\\tlanguage = {ru},\\n\\tnumber = {12},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Кхабири, Г. and Анохин, А. С. and Разумная, А. Г. and Юзюк, Ю. И. and Gueye, I. and Carcan, B. and Bouyanfif, H. and Wolfman, J. and Autret-Lambert, C. and El Marssi, M.},\\n\\tmonth = nov,\\n\\tyear = {2014},\\n\\tpages = {2420--2425},\\n}\\n\\n\",\"author_short\":[\"Кхабири, Г.\",\"Анохин, А. С.\",\"Разумная, А. Г.\",\"Юзюк, Ю. И.\",\"Gueye, I.\",\"Carcan, B.\",\"Bouyanfif, H.\",\"Wolfman, J.\",\"Autret-Lambert, C.\",\"El Marssi, M.\"],\"key\":\"__2014-11\",\"id\":\"__2014-11\",\"bibbaseid\":\"----gueye-carcan-bouyanfif-wolfman-etal--2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/41133\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Исследование сверхрешеток BaTiO$_{\\\\textrm{3}}$/(Ba$_{\\\\textrm{0.5}}$,Sr$_{\\\\textrm{0.5}}$)TiO$_{\\\\textrm{3}}$/ SrTiO$_{\\\\textrm{3}}$ методами рентгеновской дифракции и комбинационного рассеяния света\",\"volume\":\"56\",\"url\":\"http://journals.ioffe.ru/articles/26811\",\"abstract\":\"Методами рентгеновской дифрактометрии определены структурные характеристики сверхрешетки BaTiO3/(Ba0.5,Sr0.5)TiO3/SrTiO3 на подложке (001) MgO. Получены период модуляции, параметры элементарных ячеек слоев, составляющих сверхрешетку, оценены величины областей когерентного рассеяния и средние микродеформации в направлении, перпендикулярном поверхности. Проведено сравнение с характеристиками двухслойной сверхрешетки BaTiO3/(Ba0.5,Sr0.5)TiO3. В спектрах комбинационного рассеяния света обнаружено существенное смещение мягкой E(TO)-моды в трехслойной сверхрешетке по сравнению с ее положением в двухслойной. Обнаруженные эффекты связываются с существенным увеличением температуры перехода трехслойной сверхрешетки в параэлектрическую фазу.\",\"language\":\"ru\",\"number\":\"3\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Тихонов\"],\"firstnames\":[\"Ю.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Захарченко\"],\"firstnames\":[\"И.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Маслова\"],\"firstnames\":[\"О.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Юзюк\"],\"firstnames\":[\"Ю.\",\"И.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Ortega\"],\"firstnames\":[\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kumar\"],\"firstnames\":[\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Katiyar\"],\"firstnames\":[\"R.\",\"S.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2014\",\"pages\":\"573–576\",\"bibtex\":\"@article{__2014-12,\\n\\ttitle = {Исследование сверхрешеток {BaTiO}$_{\\\\textrm{3}}$/({Ba}$_{\\\\textrm{0.5}}$,{Sr}$_{\\\\textrm{0.5}}$){TiO}$_{\\\\textrm{3}}$/ {SrTiO}$_{\\\\textrm{3}}$ методами рентгеновской дифракции и комбинационного рассеяния света},\\n\\tvolume = {56},\\n\\turl = {http://journals.ioffe.ru/articles/26811},\\n\\tabstract = {Методами рентгеновской дифрактометрии определены структурные характеристики сверхрешетки BaTiO3/(Ba0.5,Sr0.5)TiO3/SrTiO3 на подложке (001) MgO. Получены период модуляции, параметры элементарных ячеек слоев, составляющих сверхрешетку, оценены величины областей когерентного рассеяния и средние микродеформации в направлении, перпендикулярном поверхности. Проведено сравнение с характеристиками двухслойной сверхрешетки BaTiO3/(Ba0.5,Sr0.5)TiO3. В спектрах комбинационного рассеяния света обнаружено существенное смещение мягкой E(TO)-моды в трехслойной сверхрешетке по сравнению с ее положением в двухслойной. Обнаруженные эффекты связываются с существенным увеличением температуры перехода трехслойной сверхрешетки в параэлектрическую фазу.},\\n\\tlanguage = {ru},\\n\\tnumber = {3},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Тихонов, Ю. А. and Захарченко, И. Н. and Маслова, О. А. and Юзюк, Ю. И. and Ortega, N. and Kumar, A. and Katiyar, R. S.},\\n\\tmonth = feb,\\n\\tyear = {2014},\\n\\tpages = {573--576},\\n}\\n\\n\",\"author_short\":[\"Тихонов, Ю. А.\",\"Захарченко, И. Н.\",\"Маслова, О. А.\",\"Юзюк, Ю. И.\",\"Ortega, N.\",\"Kumar, A.\",\"Katiyar, R. S.\"],\"key\":\"__2014-12\",\"id\":\"__2014-12\",\"bibbaseid\":\"----ortega-kumar-katiyar-batiotextrm3batextrm05srtextrm05tiotextrm3srtiotextrm3-2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/26811\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Температурная эволюция спектров диэлектрического отклика стиллвеллитоподобных стекол в терагерцевом и инфракрасном диапазонах\",\"volume\":\"56\",\"url\":\"http://journals.ioffe.ru/articles/26909\",\"abstract\":\"Измерены спектры пропускания и отражения стекла PrBGeO5 в терагерцевом и инфракрасном диапазонах. При низких температурах зарегистрированы рост диэлектрической проницаемости и появление узких линий резонансного типа в терагерцевом диапазоне. Рассчитаны спектры комплексной диэлектрической проницаемости по формулам Френеля и Крамерса-Кронига.\",\"language\":\"ru\",\"number\":\"6\",\"urldate\":\"2023-11-11\",\"journal\":\"Физика твердого тела\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Командин\"],\"firstnames\":[\"Г.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Породинков\"],\"firstnames\":[\"О.\",\"Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Гончаров\"],\"firstnames\":[\"Ю.\",\"Г.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Спектор\"],\"firstnames\":[\"И.\",\"Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Исхакова\"],\"firstnames\":[\"Л.\",\"Д.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Сигаев\"],\"firstnames\":[\"В.\",\"Н.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Лотарев\"],\"firstnames\":[\"С.\",\"В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Торгашев\"],\"firstnames\":[\"В.\",\"И.\"],\"suffixes\":[]}],\"month\":\"May\",\"year\":\"2014\",\"pages\":\"1152–1157\",\"bibtex\":\"@article{__2014-13,\\n\\ttitle = {Температурная эволюция спектров диэлектрического отклика стиллвеллитоподобных стекол в терагерцевом и инфракрасном диапазонах},\\n\\tvolume = {56},\\n\\turl = {http://journals.ioffe.ru/articles/26909},\\n\\tabstract = {Измерены спектры пропускания и отражения стекла PrBGeO5 в терагерцевом и инфракрасном диапазонах. При низких температурах зарегистрированы рост диэлектрической проницаемости и появление узких линий резонансного типа в терагерцевом диапазоне. Рассчитаны спектры комплексной диэлектрической проницаемости по формулам Френеля и Крамерса-Кронига.},\\n\\tlanguage = {ru},\\n\\tnumber = {6},\\n\\turldate = {2023-11-11},\\n\\tjournal = {Физика твердого тела},\\n\\tauthor = {Командин, Г. А. and Породинков, О. Е. and Гончаров, Ю. Г. and Спектор, И. Е. and Исхакова, Л. Д. and Сигаев, В. Н. and Лотарев, С. В. and Торгашев, В. И.},\\n\\tmonth = may,\\n\\tyear = {2014},\\n\\tpages = {1152--1157},\\n}\\n\\n\",\"author_short\":[\"Командин, Г. А.\",\"Породинков, О. Е.\",\"Гончаров, Ю. Г.\",\"Спектор, И. Е.\",\"Исхакова, Л. Д.\",\"Сигаев, В. Н.\",\"Лотарев, С. В.\",\"Торгашев, В. И.\"],\"key\":\"__2014-13\",\"id\":\"__2014-13\",\"bibbaseid\":\"---------2014\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://journals.ioffe.ru/articles/26909\"},\"metadata\":{\"authorlinks\":{}},\"downloads\":0,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Landau theory and self-assembly of spherical nanoclusters and nanoparticles with octahedral symmetry\",\"volume\":\"107\",\"issn\":\"2469-9950\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevB.107.024102\",\"doi\":\"10.1103/PhysRevB.107.024102\",\"number\":\"2\",\"journal\":\"Physical Review B\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Chalin\"],\"firstnames\":[\"D.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"S.\",\"B.\"],\"suffixes\":[]}],\"month\":\"January\",\"year\":\"2023\",\"keywords\":\"Q1\",\"pages\":\"024102\",\"bibtex\":\"@article{chalin_landau_2023,\\n\\ttitle = {Landau theory and self-assembly of spherical nanoclusters and nanoparticles with octahedral symmetry},\\n\\tvolume = {107},\\n\\tissn = {2469-9950},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevB.107.024102},\\n\\tdoi = {10.1103/PhysRevB.107.024102},\\n\\tnumber = {2},\\n\\tjournal = {Physical Review B},\\n\\tauthor = {Chalin, D. V. and Rochal, S. B.},\\n\\tmonth = jan,\\n\\tyear = {2023},\\n\\tkeywords = {Q1},\\n\\tpages = {024102},\\n}\\n\\n\",\"author_short\":[\"Chalin, D. V.\",\"Rochal, S. B.\"],\"key\":\"chalin_landau_2023\",\"id\":\"chalin_landau_2023\",\"bibbaseid\":\"chalin-rochal-landautheoryandselfassemblyofsphericalnanoclustersandnanoparticleswithoctahedralsymmetry-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevB.107.024102\"},\"keyword\":[\"Q1\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Integration of Cypoviruses into polyhedrin matrix\",\"volume\":\"5\",\"issn\":\"2516-0230\",\"url\":\"http://xlink.rsc.org/?DOI=D3NA00393K\",\"doi\":\"10.1039/D3NA00393K\",\"abstract\":\"Based on symmetry arguments we predict the architecture of the Cypovirus superstructure and propose an electrostatic mechanism for its disassembly in alkaline environment.\",\"number\":\"16\",\"journal\":\"Nanoscale Advances\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Konevtsova\"],\"firstnames\":[\"Olga\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golushko\"],\"firstnames\":[\"Ivan\",\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Podgornik\"],\"firstnames\":[\"Rudolf\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergei\",\"B.\"],\"suffixes\":[]}],\"year\":\"2023\",\"keywords\":\"Q1\",\"pages\":\"4140–4148\",\"bibtex\":\"@article{konevtsova_integration_2023,\\n\\ttitle = {Integration of {Cypoviruses} into polyhedrin matrix},\\n\\tvolume = {5},\\n\\tissn = {2516-0230},\\n\\turl = {http://xlink.rsc.org/?DOI=D3NA00393K},\\n\\tdoi = {10.1039/D3NA00393K},\\n\\tabstract = {Based on symmetry arguments we predict the architecture of the Cypovirus superstructure and propose an electrostatic mechanism for its disassembly in alkaline environment.},\\n\\tnumber = {16},\\n\\tjournal = {Nanoscale Advances},\\n\\tauthor = {Konevtsova, Olga V. and Golushko, Ivan Yu. and Podgornik, Rudolf and Rochal, Sergei B.},\\n\\tyear = {2023},\\n\\tkeywords = {Q1},\\n\\tpages = {4140--4148},\\n}\\n\\n\",\"author_short\":[\"Konevtsova, O. V.\",\"Golushko, I. Y.\",\"Podgornik, R.\",\"Rochal, S. B.\"],\"key\":\"konevtsova_integration_2023\",\"id\":\"konevtsova_integration_2023\",\"bibbaseid\":\"konevtsova-golushko-podgornik-rochal-integrationofcypovirusesintopolyhedrinmatrix-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://xlink.rsc.org/?DOI=D3NA00393K\"},\"keyword\":[\"Q1\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Topological properties and shape of proliferative and nonproliferative cell monolayers\",\"volume\":\"108\",\"issn\":\"2470-0045\",\"url\":\"https://link.aps.org/doi/10.1103/PhysRevE.108.024404\",\"doi\":\"10.1103/PhysRevE.108.024404\",\"number\":\"2\",\"journal\":\"Physical Review E\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Roshal\"],\"firstnames\":[\"Daria\",\"S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Azzag\"],\"firstnames\":[\"Karim\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Fedorenko\"],\"firstnames\":[\"Kirill\",\"K.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergei\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Baghdiguian\"],\"firstnames\":[\"Stephen\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2023\",\"keywords\":\"Q1\",\"pages\":\"024404\",\"bibtex\":\"@article{roshal_topological_2023,\\n\\ttitle = {Topological properties and shape of proliferative and nonproliferative cell monolayers},\\n\\tvolume = {108},\\n\\tissn = {2470-0045},\\n\\turl = {https://link.aps.org/doi/10.1103/PhysRevE.108.024404},\\n\\tdoi = {10.1103/PhysRevE.108.024404},\\n\\tnumber = {2},\\n\\tjournal = {Physical Review E},\\n\\tauthor = {Roshal, Daria S. and Azzag, Karim and Fedorenko, Kirill K. and Rochal, Sergei B. and Baghdiguian, Stephen},\\n\\tmonth = aug,\\n\\tyear = {2023},\\n\\tkeywords = {Q1},\\n\\tpages = {024404},\\n}\\n\\n\",\"author_short\":[\"Roshal, D. S.\",\"Azzag, K.\",\"Fedorenko, K. K.\",\"Rochal, S. B.\",\"Baghdiguian, S.\"],\"key\":\"roshal_topological_2023\",\"id\":\"roshal_topological_2023\",\"bibbaseid\":\"roshal-azzag-fedorenko-rochal-baghdiguian-topologicalpropertiesandshapeofproliferativeandnonproliferativecellmonolayers-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.aps.org/doi/10.1103/PhysRevE.108.024404\"},\"keyword\":[\"Q1\"],\"metadata\":{\"authorlinks\":{}},\"downloads\":1,\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Close packings of identical proteins in small spherical capsids and similar proteinaceous shells\",\"volume\":\"19\",\"issn\":\"1744-683X\",\"url\":\"http://xlink.rsc.org/?DOI=D3SM01106B\",\"doi\":\"10.1039/D3SM01106B\",\"abstract\":\"Analyzing anisotropy of protein shapes, we reveal energy and symmetry reasons controlling capsid structures, including their handedness and interprotein bonds.\",\"number\":\"44\",\"journal\":\"Soft Matter\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Rochal\"],\"firstnames\":[\"Sergei\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Konevtsova\"],\"firstnames\":[\"Olga\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Golushko\"],\"firstnames\":[\"Ivan\",\"Yu.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Podgornik\"],\"firstnames\":[\"Rudolf\"],\"suffixes\":[]}],\"year\":\"2023\",\"keywords\":\"Q1\",\"pages\":\"8649–8658\",\"bibtex\":\"@article{rochal_close_2023,\\n\\ttitle = {Close packings of identical proteins in small spherical capsids and similar proteinaceous shells},\\n\\tvolume = {19},\\n\\tissn = {1744-683X},\\n\\turl = {http://xlink.rsc.org/?DOI=D3SM01106B},\\n\\tdoi = {10.1039/D3SM01106B},\\n\\tabstract = {Analyzing anisotropy of protein shapes, we reveal energy and symmetry reasons controlling capsid structures, including their handedness and interprotein bonds.},\\n\\tnumber = {44},\\n\\tjournal = {Soft Matter},\\n\\tauthor = {Rochal, Sergei B. and Konevtsova, Olga V. and Golushko, Ivan Yu. and Podgornik, Rudolf},\\n\\tyear = {2023},\\n\\tkeywords = {Q1},\\n\\tpages = {8649--8658},\\n}\\n\\n\",\"author_short\":[\"Rochal, S. B.\",\"Konevtsova, O. V.\",\"Golushko, I. Y.\",\"Podgornik, R.\"],\"key\":\"rochal_close_2023\",\"id\":\"rochal_close_2023\",\"bibbaseid\":\"rochal-konevtsova-golushko-podgornik-closepackingsofidenticalproteinsinsmallsphericalcapsidsandsimilarproteinaceousshells-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://xlink.rsc.org/?DOI=D3SM01106B\"},\"keyword\":[\"Q1\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Thermodynamic analysis of electro-optic coefficients of ferroelectrics\",\"volume\":\"133\",\"issn\":\"0021-8979\",\"url\":\"https://pubs.aip.org/jap/article/133/6/063103/2871932/Thermodynamic-analysis-of-electro-optic\",\"doi\":\"10.1063/5.0137409\",\"abstract\":\"The electro-optic coefficients of ferroelectric materials were obtained by Landau thermodynamic theory. It is proved that if the permittivity tensor is diagonal, then some ratios of the electro-optical coefficients are equal to the ratios of its diagonal components. The dependence of electro-optic coefficients on the external electric field for single-crystal barium titanate was studied and discussed. It is shown that electro-optic coefficients are rather high for barium titanate due to a non-linear response of dielectric susceptibility to electric field strength.\",\"number\":\"6\",\"journal\":\"Journal of Applied Physics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kalinchuk\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2023\",\"keywords\":\"Q2\",\"bibtex\":\"@article{shirokov_thermodynamic_2023,\\n\\ttitle = {Thermodynamic analysis of electro-optic coefficients of ferroelectrics},\\n\\tvolume = {133},\\n\\tissn = {0021-8979},\\n\\turl = {https://pubs.aip.org/jap/article/133/6/063103/2871932/Thermodynamic-analysis-of-electro-optic},\\n\\tdoi = {10.1063/5.0137409},\\n\\tabstract = {The electro-optic coefficients of ferroelectric materials were obtained by Landau thermodynamic theory. It is proved that if the permittivity tensor is diagonal, then some ratios of the electro-optical coefficients are equal to the ratios of its diagonal components. The dependence of electro-optic coefficients on the external electric field for single-crystal barium titanate was studied and discussed. It is shown that electro-optic coefficients are rather high for barium titanate due to a non-linear response of dielectric susceptibility to electric field strength.},\\n\\tnumber = {6},\\n\\tjournal = {Journal of Applied Physics},\\n\\tauthor = {Shirokov, V. B. and Timoshenko, P. E. and Kalinchuk, V. V.},\\n\\tmonth = feb,\\n\\tyear = {2023},\\n\\tkeywords = {Q2},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Timoshenko, P. E.\",\"Kalinchuk, V. V.\"],\"key\":\"shirokov_thermodynamic_2023\",\"id\":\"shirokov_thermodynamic_2023\",\"bibbaseid\":\"shirokov-timoshenko-kalinchuk-thermodynamicanalysisofelectroopticcoefficientsofferroelectrics-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://pubs.aip.org/jap/article/133/6/063103/2871932/Thermodynamic-analysis-of-electro-optic\"},\"keyword\":[\"Q2\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"The role of elastic stress during thermomigration of liquid zones based on aluminum in silicon\",\"volume\":\"85\",\"issn\":\"18149146\",\"url\":\"http://ppp.mech.unn.ru/index.php/ppp/article/view/774\",\"doi\":\"10.32326/1814-9146-2023-85-3-426-436\",\"abstract\":\"The method of thermomigration of liquid zones based on aluminum makes it possible to create complex structures of closed channels with boundaries formed from p-n junctions in single-crystal silicon wafers. The channels are characterized by the uniformity of their properties, and the pn junctions are characterized by their sharpness. Such structures are used in high-current electronics, photovoltaics, and microelectromechanical converters. Volumetric deformation inside and outside the channel due to alloying of silicon with aluminum leads to the formation of mechanical stresses. The equilibrium shape of the channels formed at high temperatures is determined by the minimum elastic energy and depends on the material parameters and geometry of the structure. Within the framework of the linear theory of elasticity, the behavior of elastic energy during the formation of the structure of thermomigration channels at high temperatures doped with aluminum in a single-crystalline (001) cut disk was studied. The simulation was performed using the finite element method in the COMSOL Multiphysics mathematical package. The study was carried out for practically important structures in which the direction of the edges is oriented along the diagonal of the square. Only such structures do not have breaks during the process of thermomigration. Based on the calculation results, it was revealed that the minimum elastic energy corresponds to structures with different crystalline orientations inside the channel and outside it – in the main silicon matrix. The direction of the crystalline axes inside the channel, corresponding to the minimum elastic energy, is rotated by 45 degrees in the plane of the disk relative to the direction of the axes of the main matrix of the silicon crystal. In addition, calculations showed that with such a turn, the shape of the channels changes. The minimum elastic energy corresponds not to vertical structures, but to inclined ones. The angle of inclination of the pyramids depends on the width of the channels and the distance between them.\",\"number\":\"3\",\"journal\":\"Problems of Strength and Plasticity\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Seredin\"],\"firstnames\":[\"B.M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kalinchuk\"],\"firstnames\":[\"V.V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Popov\"],\"firstnames\":[\"V.P.\"],\"suffixes\":[]}],\"year\":\"2023\",\"keywords\":\"Q4\",\"pages\":\"426–436\",\"bibtex\":\"@article{shirokov_role_2023,\\n\\ttitle = {The role of elastic stress during thermomigration of liquid zones based on aluminum in silicon},\\n\\tvolume = {85},\\n\\tissn = {18149146},\\n\\turl = {http://ppp.mech.unn.ru/index.php/ppp/article/view/774},\\n\\tdoi = {10.32326/1814-9146-2023-85-3-426-436},\\n\\tabstract = {The method of thermomigration of liquid zones based on aluminum makes it possible to create complex structures of closed channels with boundaries formed from p-n junctions in single-crystal silicon wafers. The channels are characterized by the uniformity of their properties, and the pn junctions are characterized by their sharpness. Such structures are used in high-current electronics, photovoltaics, and microelectromechanical converters. Volumetric deformation inside and outside the channel due to alloying of silicon with aluminum leads to the formation of mechanical stresses. The equilibrium shape of the channels formed at high temperatures is determined by the minimum elastic energy and depends on the material parameters and geometry of the structure. Within the framework of the linear theory of elasticity, the behavior of elastic energy during the formation of the structure of thermomigration channels at high temperatures doped with aluminum in a single-crystalline (001) cut disk was studied. The simulation was performed using the finite element method in the COMSOL Multiphysics mathematical package. The study was carried out for practically important structures in which the direction of the edges is oriented along the diagonal of the square. Only such structures do not have breaks during the process of thermomigration. Based on the calculation results, it was revealed that the minimum elastic energy corresponds to structures with different crystalline orientations inside the channel and outside it – in the main silicon matrix. The direction of the crystalline axes inside the channel, corresponding to the minimum elastic energy, is rotated by 45 degrees in the plane of the disk relative to the direction of the axes of the main matrix of the silicon crystal. In addition, calculations showed that with such a turn, the shape of the channels changes. The minimum elastic energy corresponds not to vertical structures, but to inclined ones. The angle of inclination of the pyramids depends on the width of the channels and the distance between them.},\\n\\tnumber = {3},\\n\\tjournal = {Problems of Strength and Plasticity},\\n\\tauthor = {Shirokov, V.B. and Seredin, B.M. and Timoshenko, P.E. and Kalinchuk, V.V. and Popov, V.P.},\\n\\tyear = {2023},\\n\\tkeywords = {Q4},\\n\\tpages = {426--436},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V.\",\"Seredin, B.\",\"Timoshenko, P.\",\"Kalinchuk, V.\",\"Popov, V.\"],\"key\":\"shirokov_role_2023\",\"id\":\"shirokov_role_2023\",\"bibbaseid\":\"shirokov-seredin-timoshenko-kalinchuk-popov-theroleofelasticstressduringthermomigrationofliquidzonesbasedonaluminuminsilicon-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://ppp.mech.unn.ru/index.php/ppp/article/view/774\"},\"keyword\":[\"Q4\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Генерация поверхностных акустических волн сегнетоэлектрической пленкой BST при действии одноосной нагрузки\",\"issn\":\"2226-1869\",\"url\":\"https://ered.pstu.ru/index.php/mechanics/article/view/3765\",\"doi\":\"10.15593/perm.mech/2023.1.16\",\"abstract\":\"The electro-mechanical properties of a ferroelectric film of barium strontium titanate (BST) film located on a silicon substrate depend on applied external strain. A significant dependence is observed for concentrations close to values, where a phase transition for the ferroelectric film occurs. A model of single-crystal BST film near the phase transition under uniaxial strain is studied by the thermodynamic theory of phase transitions. The material properties of the film obtained by the model are used for numerical study of the excitation of Rayleigh' acoustic waves on the surface of the film-substrate heterostructure. Shifting the extrema of S-parameters, characterizing the efficiency of excitation of surface acoustic waves, is shown under the applied strain. The change of S-parameters for the first three resonances determined principally by the geometry of the interdigital electrodes is presented. The largest shift of resonant frequency is observed in a case of the second resonance that corresponds to Sezava wave.\",\"number\":\"1\",\"journal\":\"PNRPU Mechanics Bulletin\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Timoshenko\"],\"firstnames\":[\"P.\",\"E.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kalinchuk\"],\"firstnames\":[\"V.\",\"V.\"],\"suffixes\":[]}],\"month\":\"December\",\"year\":\"2023\",\"keywords\":\"Q3\",\"pages\":\"173–178\",\"bibtex\":\"@article{shirokov__2023,\\n\\ttitle = {Генерация поверхностных акустических волн сегнетоэлектрической пленкой {BST} при действии одноосной нагрузки},\\n\\tissn = {2226-1869},\\n\\turl = {https://ered.pstu.ru/index.php/mechanics/article/view/3765},\\n\\tdoi = {10.15593/perm.mech/2023.1.16},\\n\\tabstract = {The electro-mechanical properties of a ferroelectric film of barium strontium titanate (BST) film located on a silicon substrate depend on applied external strain. A significant dependence is observed for concentrations close to values, where a phase transition for the ferroelectric film occurs. A model of single-crystal BST film near the phase transition under uniaxial strain is studied by the thermodynamic theory of phase transitions. The material properties of the film obtained by the model are used for numerical study of the excitation of Rayleigh' acoustic waves on the surface of the film-substrate heterostructure. Shifting the extrema of S-parameters, characterizing the efficiency of excitation of surface acoustic waves, is shown under the applied strain. The change of S-parameters for the first three resonances determined principally by the geometry of the interdigital electrodes is presented. The largest shift of resonant frequency is observed in a case of the second resonance that corresponds to Sezava wave.},\\n\\tnumber = {1},\\n\\tjournal = {PNRPU Mechanics Bulletin},\\n\\tauthor = {Shirokov, V. B. and Timoshenko, P. E. and Kalinchuk, V. V.},\\n\\tmonth = dec,\\n\\tyear = {2023},\\n\\tkeywords = {Q3},\\n\\tpages = {173--178},\\n}\\n\\n\",\"author_short\":[\"Shirokov, V. B.\",\"Timoshenko, P. E.\",\"Kalinchuk, V. V.\"],\"key\":\"shirokov__2023\",\"id\":\"shirokov__2023\",\"bibbaseid\":\"shirokov-timoshenko-kalinchuk-bst-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://ered.pstu.ru/index.php/mechanics/article/view/3765\"},\"keyword\":[\"Q3\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Magnetic phase diagrams of the pyrochlore-based magnets: Landau theory\",\"volume\":\"575\",\"issn\":\"03048853\",\"url\":\"https://linkinghub.elsevier.com/retrieve/pii/S0304885323003669\",\"doi\":\"10.1016/j.jmmm.2023.170717\",\"journal\":\"Journal of Magnetism and Magnetic Materials\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"M.V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Pimenov\"],\"firstnames\":[\"M.S.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"V.M.\"],\"suffixes\":[]}],\"month\":\"June\",\"year\":\"2023\",\"keywords\":\"Q2\",\"pages\":\"170717\",\"bibtex\":\"@article{talanov_magnetic_2023,\\n\\ttitle = {Magnetic phase diagrams of the pyrochlore-based magnets: {Landau} theory},\\n\\tvolume = {575},\\n\\tissn = {03048853},\\n\\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0304885323003669},\\n\\tdoi = {10.1016/j.jmmm.2023.170717},\\n\\tjournal = {Journal of Magnetism and Magnetic Materials},\\n\\tauthor = {Talanov, M.V. and Shirokov, V.B. and Pimenov, M.S. and Talanov, V.M.},\\n\\tmonth = jun,\\n\\tyear = {2023},\\n\\tkeywords = {Q2},\\n\\tpages = {170717},\\n}\\n\\n\",\"author_short\":[\"Talanov, M.\",\"Shirokov, V.\",\"Pimenov, M.\",\"Talanov, V.\"],\"key\":\"talanov_magnetic_2023\",\"id\":\"talanov_magnetic_2023\",\"bibbaseid\":\"talanov-shirokov-pimenov-talanov-magneticphasediagramsofthepyrochlorebasedmagnetslandautheory-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://linkinghub.elsevier.com/retrieve/pii/S0304885323003669\"},\"keyword\":[\"Q2\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Symmetry-based prediction of the type-II multiferroics with pyrochlore structure\",\"volume\":\"14\",\"issn\":\"22208054\",\"url\":\"http://nanojournal.ifmo.ru/en/articles-2/volume14/14-2/physics/paper09/\",\"doi\":\"10.17586/2220-8054-2023-14-2-208-215\",\"number\":\"2\",\"journal\":\"Nanosystems: Physics, Chemistry, Mathematics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"V.M.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"M.V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.B.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2023\",\"keywords\":\"Q3\",\"pages\":\"208–215\",\"bibtex\":\"@article{talanov_symmetry-based_2023,\\n\\ttitle = {Symmetry-based prediction of the type-{II} multiferroics with pyrochlore structure},\\n\\tvolume = {14},\\n\\tissn = {22208054},\\n\\turl = {http://nanojournal.ifmo.ru/en/articles-2/volume14/14-2/physics/paper09/},\\n\\tdoi = {10.17586/2220-8054-2023-14-2-208-215},\\n\\tnumber = {2},\\n\\tjournal = {Nanosystems: Physics, Chemistry, Mathematics},\\n\\tauthor = {Talanov, V.M. and Talanov, M.V. and Shirokov, V.B.},\\n\\tmonth = apr,\\n\\tyear = {2023},\\n\\tkeywords = {Q3},\\n\\tpages = {208--215},\\n}\\n\\n\",\"author_short\":[\"Talanov, V.\",\"Talanov, M.\",\"Shirokov, V.\"],\"key\":\"talanov_symmetry-based_2023\",\"id\":\"talanov_symmetry-based_2023\",\"bibbaseid\":\"talanov-talanov-shirokov-symmetrybasedpredictionofthetypeiimultiferroicswithpyrochlorestructure-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://nanojournal.ifmo.ru/en/articles-2/volume14/14-2/physics/paper09/\"},\"keyword\":[\"Q3\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Spin-induced ferroelastics with pyrochlore lattices\",\"volume\":\"612\",\"issn\":\"0015-0193\",\"url\":\"https://www.tandfonline.com/doi/full/10.1080/00150193.2023.2211291\",\"doi\":\"10.1080/00150193.2023.2211291\",\"number\":\"1\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"M.\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"V.\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"V.\",\"M.\"],\"suffixes\":[]}],\"month\":\"August\",\"year\":\"2023\",\"keywords\":\"Q4\",\"pages\":\"1–9\",\"bibtex\":\"@article{talanov_spin-induced_2023,\\n\\ttitle = {Spin-induced ferroelastics with pyrochlore lattices},\\n\\tvolume = {612},\\n\\tissn = {0015-0193},\\n\\turl = {https://www.tandfonline.com/doi/full/10.1080/00150193.2023.2211291},\\n\\tdoi = {10.1080/00150193.2023.2211291},\\n\\tnumber = {1},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Talanov, M. V. and Shirokov, V. B. and Talanov, V. M.},\\n\\tmonth = aug,\\n\\tyear = {2023},\\n\\tkeywords = {Q4},\\n\\tpages = {1--9},\\n}\\n\\n\",\"author_short\":[\"Talanov, M. V.\",\"Shirokov, V. B.\",\"Talanov, V. M.\"],\"key\":\"talanov_spin-induced_2023\",\"id\":\"talanov_spin-induced_2023\",\"bibbaseid\":\"talanov-shirokov-talanov-spininducedferroelasticswithpyrochlorelattices-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.tandfonline.com/doi/full/10.1080/00150193.2023.2211291\"},\"keyword\":[\"Q4\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Spin order on the pyrochlore lattice: Magnetic crystallography, Landau thermodynamics and emergent phenomena\",\"volume\":\"259\",\"issn\":\"13596454\",\"url\":\"https://linkinghub.elsevier.com/retrieve/pii/S1359645423005177\",\"doi\":\"10.1016/j.actamat.2023.119187\",\"journal\":\"Acta Materialia\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"Mikhail\",\"V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shirokov\"],\"firstnames\":[\"Vladimir\",\"B.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Talanov\"],\"firstnames\":[\"Valeriy\",\"M.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2023\",\"keywords\":\"Q1\",\"pages\":\"119187\",\"bibtex\":\"@article{talanov_spin_2023,\\n\\ttitle = {Spin order on the pyrochlore lattice: {Magnetic} crystallography, {Landau} thermodynamics and emergent phenomena},\\n\\tvolume = {259},\\n\\tissn = {13596454},\\n\\turl = {https://linkinghub.elsevier.com/retrieve/pii/S1359645423005177},\\n\\tdoi = {10.1016/j.actamat.2023.119187},\\n\\tjournal = {Acta Materialia},\\n\\tauthor = {Talanov, Mikhail V. and Shirokov, Vladimir B. and Talanov, Valeriy M.},\\n\\tmonth = oct,\\n\\tyear = {2023},\\n\\tkeywords = {Q1},\\n\\tpages = {119187},\\n}\\n\\n\",\"author_short\":[\"Talanov, M. V.\",\"Shirokov, V. B.\",\"Talanov, V. M.\"],\"key\":\"talanov_spin_2023\",\"id\":\"talanov_spin_2023\",\"bibbaseid\":\"talanov-shirokov-talanov-spinorderonthepyrochlorelatticemagneticcrystallographylandauthermodynamicsandemergentphenomena-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://linkinghub.elsevier.com/retrieve/pii/S1359645423005177\"},\"keyword\":[\"Q1\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"Мультипорядок, термодинамика и кристаллохимия тетрагональной фазы MgTi$_{\\\\textrm{2}}$O$_{\\\\textrm{4}}$\",\"isbn\":\"978-5-901688-53-3\",\"url\":\"http://www.niic.nsc.ru/phocadownload/Conferences/2023/TiM-2023/2023 Tezisy Termodinamika.pdf#page=122\",\"doi\":\"10.26902/THERM_2023_101\",\"booktitle\":\"Термодинамика и материаловедение. Тезисы докладов XV Симпозиума с международным участием\",\"publisher\":\"NIIC SB RAS\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Таланов\"],\"firstnames\":[\"В.М.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Таланов\"],\"firstnames\":[\"М.В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Авакян\"],\"firstnames\":[\"Л.\",\"А.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]}],\"year\":\"2023\",\"pages\":\"121\",\"bibtex\":\"@inproceedings{__2023,\\n\\ttitle = {Мультипорядок, термодинамика и кристаллохимия тетрагональной фазы {MgTi}$_{\\\\textrm{2}}${O}$_{\\\\textrm{4}}$},\\n\\tisbn = {978-5-901688-53-3},\\n\\turl = {http://www.niic.nsc.ru/phocadownload/Conferences/2023/TiM-2023/2023 Tezisy Termodinamika.pdf#page=122},\\n\\tdoi = {10.26902/THERM_2023_101},\\n\\tbooktitle = {Термодинамика и материаловедение. Тезисы докладов {XV} Симпозиума с международным участием},\\n\\tpublisher = {NIIC SB RAS},\\n\\tauthor = {Таланов, В.М. and Таланов, М.В. and Авакян, Л. А. and Широков, В. Б.},\\n\\tyear = {2023},\\n\\tpages = {121},\\n}\\n\\n\",\"author_short\":[\"Таланов, В.\",\"Таланов, М.\",\"Авакян, Л. А.\",\"Широков, В. Б.\"],\"key\":\"__2023\",\"id\":\"__2023\",\"bibbaseid\":\"----mgtitextrm2otextrm4-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://www.niic.nsc.ru/phocadownload/Conferences/2023/TiM-2023/2023 Tezisy Termodinamika.pdf#page=122\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"Поверхностные эффекты в наноразмерных сегнетоэлектрических гетероструктурах\",\"booktitle\":\"XIII Всероссийский съезд по теоретической и прикладной механике. Санкт-Петербург, 21-25 августа\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Калинчук\"],\"firstnames\":[\"В.В.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Тимошенко\"],\"firstnames\":[\"П.Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.Б.\"],\"suffixes\":[]}],\"year\":\"2023\",\"pages\":\"Т.4, С.670–672\",\"bibtex\":\"@inproceedings{__2023-1,\\n\\ttitle = {Поверхностные эффекты в наноразмерных сегнетоэлектрических гетероструктурах},\\n\\tbooktitle = {{XIII} Всероссийский съезд по теоретической и прикладной механике. 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Санкт- Петербург, 21-25 августа\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Тимошенко\"],\"firstnames\":[\"П.Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Калинчук\"],\"firstnames\":[\"В.В.\"],\"suffixes\":[]}],\"year\":\"2023\",\"pages\":\"Т.4, С.741–743\",\"bibtex\":\"@inproceedings{__2023-2,\\n\\ttitle = {О перспективных для систем мониторинга слоистых структурах с сегнетоэлектрическим поверхностным слоем},\\n\\tdoi = {10.18720/SPBPU/2/id23-630},\\n\\tbooktitle = {{XIII} Всероссийский съезд по теоретической и прикладной механике. 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V. and Shirokov, V. B. and Talanov, V. M. and Aulov, M. S.},\\n\\tmonth = sep,\\n\\tyear = {2023},\\n\\tkeywords = {Q3},\\n\\tpages = {1263--1269},\\n}\\n\\n\",\"author_short\":[\"Talanov, M. V.\",\"Shirokov, V. B.\",\"Talanov, V. M.\",\"Aulov, M. S.\"],\"key\":\"talanov_multiorder_2023\",\"id\":\"talanov_multiorder_2023\",\"bibbaseid\":\"talanov-shirokov-talanov-aulov-multiorderandthestructuralmechanismofthelirhtextrm2otextrm4tetragonalphaseformation-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.springer.com/10.3103/S1062873823703136\"},\"keyword\":[\"Q3\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Определение электрооптических коэффициентов титаната бария\",\"volume\":\"510\",\"doi\":\"10.31857/S2686740023030148\",\"journal\":\"Доклады Российской Академии Наук. Физика, Технические науки\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Широков\"],\"firstnames\":[\"В.\",\"Б.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Тимошенко\"],\"firstnames\":[\"П.\",\"Е.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Калинчук\"],\"firstnames\":[\"В.\",\"В.\"],\"suffixes\":[]}],\"year\":\"2023\",\"pages\":\"38–43\",\"bibtex\":\"@article{__2023-3,\\n\\ttitle = {Определение электрооптических коэффициентов титаната бария},\\n\\tvolume = {510},\\n\\tdoi = {10.31857/S2686740023030148},\\n\\tjournal = {Доклады Российской Академии Наук. Физика, Технические науки},\\n\\tauthor = {Широков, В. Б. and Тимошенко, П. Е. and Калинчук, В. В.},\\n\\tyear = {2023},\\n\\tpages = {38--43},\\n}\\n\\n\",\"author_short\":[\"Широков, В. Б.\",\"Тимошенко, П. Е.\",\"Калинчук, В. В.\"],\"key\":\"__2023-3\",\"id\":\"__2023-3\",\"bibbaseid\":\"----2023\",\"role\":\"author\",\"urls\":{},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Photothermal Effect and Phase Transition in VO$_{\\\\textrm{2}}$ Enhanced by Plasmonic Particles\",\"volume\":\"16\",\"issn\":\"1996-1944\",\"url\":\"https://www.mdpi.com/1996-1944/16/7/2579\",\"doi\":\"10.3390/ma16072579\",\"abstract\":\"Phase change metasurfaces based on VO2, which are pre-heated with electric current and optically addressed by projected structured light hologram, are considered to become a new paradigm in programmed THz/middle IR flat optics. Macroscopic quasi-homogeneous arrays of Au nanoparticles show large near IR absorption and a significant photothermal effect capable of boosting a light-triggered switching of VO2 and are to be carefully examined. We propose a new approach to simultaneously probe the altered temperature and electric conductivity of a hybrid Au particle-VO2 film composite by monitoring a phase shift and attenuating a surface acoustic wave in a YX128° cut LiNbO3 substrate. The method shows a temperature resolution of 0.1 °C comparable with the best existing techniques for studying nanoobjects and surfaces. The laser-induced photothermal effects were characterized in a macroscopic array of Au nanostars (AuNSts) with different surface coverage. In a monolayer of 10 nm Au, coupled plasmonic nanoparticles were deposited on the LiNbO3 substrate. An optically triggered insulator-metal transition assisted by photothermal effect in AuNSts/VO2/TiO2/LiNbO3 composites was studied at varied light power. We believe that the proposed SAW-based method is of significant importance for the characterization and optimization of radiation absorbing or/and electrically heated elements of metasurfaces and other devices for lab-on-chip and optical communication/processor technology.\",\"number\":\"7\",\"journal\":\"Materials\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Kaydashev\"],\"firstnames\":[\"Vladimir\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Khlebtsov\"],\"firstnames\":[\"Boris\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kutepov\"],\"firstnames\":[\"Maxim\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nikolskiy\"],\"firstnames\":[\"Anatoliy\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kozakov\"],\"firstnames\":[\"Alexey\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Konstantinov\"],\"firstnames\":[\"Alexey\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mikheykin\"],\"firstnames\":[\"Alexey\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Karapetyan\"],\"firstnames\":[\"Gevork\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kaidashev\"],\"firstnames\":[\"Evgeni\"],\"suffixes\":[]}],\"month\":\"March\",\"year\":\"2023\",\"keywords\":\"Q2\",\"pages\":\"2579\",\"bibtex\":\"@article{kaydashev_photothermal_2023,\\n\\ttitle = {Photothermal Effect and Phase Transition in {VO}$_{\\\\textrm{2}}$ Enhanced by {Plasmonic} {Particles}},\\n\\tvolume = {16},\\n\\tissn = {1996-1944},\\n\\turl = {https://www.mdpi.com/1996-1944/16/7/2579},\\n\\tdoi = {10.3390/ma16072579},\\n\\tabstract = {Phase change metasurfaces based on VO2, which are pre-heated with electric current and optically addressed by projected structured light hologram, are considered to become a new paradigm in programmed THz/middle IR flat optics. Macroscopic quasi-homogeneous arrays of Au nanoparticles show large near IR absorption and a significant photothermal effect capable of boosting a light-triggered switching of VO2 and are to be carefully examined. We propose a new approach to simultaneously probe the altered temperature and electric conductivity of a hybrid Au particle-VO2 film composite by monitoring a phase shift and attenuating a surface acoustic wave in a YX128° cut LiNbO3 substrate. The method shows a temperature resolution of 0.1 °C comparable with the best existing techniques for studying nanoobjects and surfaces. The laser-induced photothermal effects were characterized in a macroscopic array of Au nanostars (AuNSts) with different surface coverage. In a monolayer of 10 nm Au, coupled plasmonic nanoparticles were deposited on the LiNbO3 substrate. An optically triggered insulator-metal transition assisted by photothermal effect in AuNSts/VO2/TiO2/LiNbO3 composites was studied at varied light power. We believe that the proposed SAW-based method is of significant importance for the characterization and optimization of radiation absorbing or/and electrically heated elements of metasurfaces and other devices for lab-on-chip and optical communication/processor technology.},\\n\\tnumber = {7},\\n\\tjournal = {Materials},\\n\\tauthor = {Kaydashev, Vladimir and Khlebtsov, Boris and Kutepov, Maxim and Nikolskiy, Anatoliy and Kozakov, Alexey and Konstantinov, Alexey and Mikheykin, Alexey and Karapetyan, Gevork and Kaidashev, Evgeni},\\n\\tmonth = mar,\\n\\tyear = {2023},\\n\\tkeywords = {Q2},\\n\\tpages = {2579},\\n}\\n\\n\",\"author_short\":[\"Kaydashev, V.\",\"Khlebtsov, B.\",\"Kutepov, M.\",\"Nikolskiy, A.\",\"Kozakov, A.\",\"Konstantinov, A.\",\"Mikheykin, A.\",\"Karapetyan, G.\",\"Kaidashev, 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A.S. and Mikheykin, A.S. and Belenov, S.V. and Guterman, E.V.},\\n\\tmonth = sep,\\n\\tyear = {2023},\\n\\tkeywords = {Q1},\\n\\tpages = {157539},\\n}\\n\\n\",\"author_short\":[\"Alekseenko, A.\",\"Pavlets, A.\",\"Mikheykin, A.\",\"Belenov, S.\",\"Guterman, E.\"],\"key\":\"alekseenko_integrated_2023\",\"id\":\"alekseenko_integrated_2023\",\"bibbaseid\":\"alekseenko-pavlets-mikheykin-belenov-guterman-theintegratedapproachtostudyingthemicrostructureofdealloyedptcucelectrocatalystsforpemfcs-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://linkinghub.elsevier.com/retrieve/pii/S0169433223012175\"},\"keyword\":[\"Q1\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Lattice dynamics and phase transitions peculiarities of Ba$_{\\\\textrm{x}}$Sr$_{\\\\textrm{1-x}}$TiO$_{\\\\textrm{3}}$ solid solutions with high Sr 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Jagadeesha and Pasha, Apsar and Al-Dossari, M. and EL-Gawaad, N. S. Abd and Abdulvakhidov, Kamaludin and Lyanguzov, Nikolay and Khadke, Uday Kumar},\\n\\tmonth = feb,\\n\\tyear = {2023},\\n\\tkeywords = {Q2},\\n\\tpages = {318},\\n}\\n\\n\",\"author_short\":[\"Angadi, V. J.\",\"Pasha, A.\",\"Al-Dossari, M.\",\"EL-Gawaad, N. S. A.\",\"Abdulvakhidov, K.\",\"Lyanguzov, N.\",\"Khadke, U. K.\"],\"key\":\"angadi_high-performance_2023\",\"id\":\"angadi_high-performance_2023\",\"bibbaseid\":\"angadi-pasha-aldossari-elgawaad-abdulvakhidov-lyanguzov-khadke-highperformancelpgsensingbehaviourofcocrtextrm2xcetextrmxotextrm4x0to002forsensorapplications-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.springer.com/10.1007/s10854-022-09725-1\"},\"keyword\":[\"Q2\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Evolution of the macroresponses during the transition from two-to six-component systems of the solid solutions with fundamentally different properties\",\"volume\":\"49\",\"issn\":\"02728842\",\"url\":\"https://linkinghub.elsevier.com/retrieve/pii/S0272884223019983\",\"doi\":\"10.1016/j.ceramint.2023.07.074\",\"number\":\"19\",\"journal\":\"Ceramics International\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Andryushin\"],\"firstnames\":[\"K.P.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Mazuritsky\"],\"firstnames\":[\"M.I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Galatova\"],\"firstnames\":[\"A.O.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Il'ina\"],\"firstnames\":[\"M.V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Soboleva\"],\"firstnames\":[\"O.I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nagaenko\"],\"firstnames\":[\"A.V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shilkina\"],\"firstnames\":[\"L.A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Dudkina\"],\"firstnames\":[\"S.I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Andryushina\"],\"firstnames\":[\"I.N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudskaya\"],\"firstnames\":[\"A.G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Khasbulatov\"],\"firstnames\":[\"S.V.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sadykov\"],\"firstnames\":[\"Kh.A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Reznichenko\"],\"firstnames\":[\"L.A.\"],\"suffixes\":[]}],\"month\":\"October\",\"year\":\"2023\",\"keywords\":\"Q1\",\"pages\":\"31265–31275\",\"bibtex\":\"@article{andryushin_evolution_2023,\\n\\ttitle = {Evolution of the macroresponses during the transition from two-to six-component systems of the solid solutions with fundamentally different properties},\\n\\tvolume = {49},\\n\\tissn = {02728842},\\n\\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0272884223019983},\\n\\tdoi = {10.1016/j.ceramint.2023.07.074},\\n\\tnumber = {19},\\n\\tjournal = {Ceramics International},\\n\\tauthor = {Andryushin, K.P. and Mazuritsky, M.I. and Galatova, A.O. and Il'ina, M.V. and Soboleva, O.I. and Nagaenko, A.V. and Shilkina, L.A. and Dudkina, S.I. and Andryushina, I.N. and Rudskaya, A.G. and Khasbulatov, S.V. and Sadykov, Kh.A. and Reznichenko, L.A.},\\n\\tmonth = oct,\\n\\tyear = {2023},\\n\\tkeywords = {Q1},\\n\\tpages = {31265--31275},\\n}\\n\\n\",\"author_short\":[\"Andryushin, K.\",\"Mazuritsky, M.\",\"Galatova, A.\",\"Il'ina, M.\",\"Soboleva, O.\",\"Nagaenko, A.\",\"Shilkina, L.\",\"Dudkina, S.\",\"Andryushina, I.\",\"Rudskaya, A.\",\"Khasbulatov, S.\",\"Sadykov, K.\",\"Reznichenko, L.\"],\"key\":\"andryushin_evolution_2023\",\"id\":\"andryushin_evolution_2023\",\"bibbaseid\":\"andryushin-mazuritsky-galatova-ilina-soboleva-nagaenko-shilkina-dudkina-etal-evolutionofthemacroresponsesduringthetransitionfromtwotosixcomponentsystemsofthesolidsolutionswithfundamentallydifferentproperties-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://linkinghub.elsevier.com/retrieve/pii/S0272884223019983\"},\"keyword\":[\"Q1\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"inproceedings\",\"type\":\"inproceedings\",\"title\":\"Parameters structure calculation of nonstoichiometric Pb(Mg$_{\\\\textrm{1-y}}$Nb$_{\\\\textrm{y}}$)O$_{\\\\textrm{3-z}}$ solid solutions\",\"url\":\"http://aip.scitation.org/doi/abs/10.1063/5.0115358\",\"doi\":\"10.1063/5.0115358\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Lebedinskaya\"],\"firstnames\":[\"Alla\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudskaya\"],\"firstnames\":[\"Angela\"],\"suffixes\":[]}],\"year\":\"2023\",\"pages\":\"040003\",\"bibtex\":\"@inproceedings{lebedinskaya_parameters_2023,\\n\\ttitle = {Parameters structure calculation of nonstoichiometric {Pb}({Mg}$_{\\\\textrm{1-y}}${Nb}$_{\\\\textrm{y}}$){O}$_{\\\\textrm{3-z}}$ solid solutions},\\n\\turl = {http://aip.scitation.org/doi/abs/10.1063/5.0115358},\\n\\tdoi = {10.1063/5.0115358},\\n\\tauthor = {Lebedinskaya, Alla and Rudskaya, Angela},\\n\\tyear = {2023},\\n\\tpages = {040003},\\n}\\n\\n\",\"author_short\":[\"Lebedinskaya, A.\",\"Rudskaya, A.\"],\"key\":\"lebedinskaya_parameters_2023\",\"id\":\"lebedinskaya_parameters_2023\",\"bibbaseid\":\"lebedinskaya-rudskaya-parametersstructurecalculationofnonstoichiometricpbmgtextrm1ynbtextrmyotextrm3zsolidsolutions-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"http://aip.scitation.org/doi/abs/10.1063/5.0115358\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Multifunctional Materials Based on the Solid Solutions of the (Na, K, Cd$_{\\\\textrm{0.5}}$)NbO$_{\\\\textrm{3}}$3 (KNN-Cd) System Modified with Rare Earth Elements: Crystal Structure, Microstructure, and Macroresponses\",\"volume\":\"6\",\"issn\":\"2571-6131\",\"url\":\"https://www.mdpi.com/2571-6131/6/1/21\",\"doi\":\"10.3390/ceramics6010021\",\"abstract\":\"Ceramic samples of polycomponent solid solutions (SSs) Na0.90K0.05Cd0.05NbO3 (Cd-modified KNN) and [(Na0.90K0.05Cd0.05)0.95REE0.05]NbO3, where REE = La, Pr, Tb, Dy, Ho, were obtained by the uniaxial hot pressing (UHP) method. The crystal lattice structures, morphological features of the microstructure, and dielectric and thermophysical properties of these ceramics have been investigated. For the first time, their strength characteristics (Young's modulus) and the critical stress intensity factor of the mode I Kic have been estimated. Photoluminescent properties have been compared in SSs [(Na0.90K0.05Cd0.05)0.95REE0.05]NbO3 in the visible wavelength range.\",\"number\":\"1\",\"journal\":\"Ceramics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Konstantin\"],\"firstnames\":[\"Andryushin\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Palatnikov\"],\"firstnames\":[\"Mikhail\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shilkina\"],\"firstnames\":[\"Lidiya\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Nagaenko\"],\"firstnames\":[\"Alexandr\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shcherbina\"],\"firstnames\":[\"Olga\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Smirnov\"],\"firstnames\":[\"Maxim\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Sidorov\"],\"firstnames\":[\"Nikolay\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Kubrin\"],\"firstnames\":[\"Stanislav\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudskaya\"],\"firstnames\":[\"Anzhela\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudskiy\"],\"firstnames\":[\"Daniil\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Reznichenko\"],\"firstnames\":[\"Larisa\"],\"suffixes\":[]}],\"month\":\"February\",\"year\":\"2023\",\"keywords\":\"Q2\",\"pages\":\"342–363\",\"bibtex\":\"@article{konstantin_multifunctional_2023,\\n\\ttitle = {Multifunctional {Materials} {Based} on the {Solid} {Solutions} of the ({Na}, {K}, {Cd}$_{\\\\textrm{0.5}}$){NbO}$_{\\\\textrm{3}}$3 ({KNN}-{Cd}) {System} {Modified} with {Rare} {Earth} {Elements}: {Crystal} {Structure}, {Microstructure}, and {Macroresponses}},\\n\\tvolume = {6},\\n\\tissn = {2571-6131},\\n\\turl = {https://www.mdpi.com/2571-6131/6/1/21},\\n\\tdoi = {10.3390/ceramics6010021},\\n\\tabstract = {Ceramic samples of polycomponent solid solutions (SSs) Na0.90K0.05Cd0.05NbO3 (Cd-modified KNN) and [(Na0.90K0.05Cd0.05)0.95REE0.05]NbO3, where REE = La, Pr, Tb, Dy, Ho, were obtained by the uniaxial hot pressing (UHP) method. The crystal lattice structures, morphological features of the microstructure, and dielectric and thermophysical properties of these ceramics have been investigated. For the first time, their strength characteristics (Young's modulus) and the critical stress intensity factor of the mode I Kic have been estimated. Photoluminescent properties have been compared in SSs [(Na0.90K0.05Cd0.05)0.95REE0.05]NbO3 in the visible wavelength range.},\\n\\tnumber = {1},\\n\\tjournal = {Ceramics},\\n\\tauthor = {Konstantin, Andryushin and Palatnikov, Mikhail and Shilkina, Lidiya and Nagaenko, Alexandr and Shcherbina, Olga and Smirnov, Maxim and Sidorov, Nikolay and Kubrin, Stanislav and Rudskaya, Anzhela and Rudskiy, Daniil and Reznichenko, Larisa},\\n\\tmonth = feb,\\n\\tyear = {2023},\\n\\tkeywords = {Q2},\\n\\tpages = {342--363},\\n}\\n\\n\",\"author_short\":[\"Konstantin, A.\",\"Palatnikov, M.\",\"Shilkina, L.\",\"Nagaenko, A.\",\"Shcherbina, O.\",\"Smirnov, M.\",\"Sidorov, N.\",\"Kubrin, S.\",\"Rudskaya, A.\",\"Rudskiy, D.\",\"Reznichenko, L.\"],\"key\":\"konstantin_multifunctional_2023\",\"id\":\"konstantin_multifunctional_2023\",\"bibbaseid\":\"konstantin-palatnikov-shilkina-nagaenko-shcherbina-smirnov-sidorov-kubrin-etal-multifunctionalmaterialsbasedonthesolidsolutionsofthenakcdtextrm05nbotextrm33knncdsystemmodifiedwithrareearthelementscrystalstructuremicrostructureandmacroresponses-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.mdpi.com/2571-6131/6/1/21\"},\"keyword\":[\"Q2\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"article\",\"type\":\"article\",\"title\":\"Radio-absorbing properties of (1- x )BiFeO$_{\\\\textrm{3-x}}$LaMnO$_{\\\\textrm{3}}$ (0.1 ≤ x ≤ 0.9) solid solutions\",\"volume\":\"606\",\"issn\":\"0015-0193\",\"url\":\"https://www.tandfonline.com/doi/full/10.1080/00150193.2023.2189843\",\"doi\":\"10.1080/00150193.2023.2189843\",\"number\":\"1\",\"journal\":\"Ferroelectrics\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Sidorenko\"],\"firstnames\":[\"E.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudskaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Babenko\"],\"firstnames\":[\"A.\",\"A.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Natkhin\"],\"firstnames\":[\"I.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Galatova\"],\"firstnames\":[\"A.\",\"O.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudsky\"],\"firstnames\":[\"D.\",\"I.\"],\"suffixes\":[]}],\"month\":\"April\",\"year\":\"2023\",\"keywords\":\"Q4\",\"pages\":\"50–60\",\"bibtex\":\"@article{sidorenko_radio-absorbing_2023,\\n\\ttitle = {Radio-absorbing properties of (1- x ){BiFeO}$_{\\\\textrm{3-x}}${LaMnO}$_{\\\\textrm{3}}$ (0.1 ≤ x ≤ 0.9) solid solutions},\\n\\tvolume = {606},\\n\\tissn = {0015-0193},\\n\\turl = {https://www.tandfonline.com/doi/full/10.1080/00150193.2023.2189843},\\n\\tdoi = {10.1080/00150193.2023.2189843},\\n\\tnumber = {1},\\n\\tjournal = {Ferroelectrics},\\n\\tauthor = {Sidorenko, E. N. and Rudskaya, A. G. and Babenko, A. A. and Natkhin, I. I. and Galatova, A. O. and Rudsky, D. I.},\\n\\tmonth = apr,\\n\\tyear = {2023},\\n\\tkeywords = {Q4},\\n\\tpages = {50--60},\\n}\\n\\n\",\"author_short\":[\"Sidorenko, E. N.\",\"Rudskaya, A. G.\",\"Babenko, A. A.\",\"Natkhin, I. I.\",\"Galatova, A. O.\",\"Rudsky, D. I.\"],\"key\":\"sidorenko_radio-absorbing_2023\",\"id\":\"sidorenko_radio-absorbing_2023\",\"bibbaseid\":\"sidorenko-rudskaya-babenko-natkhin-galatova-rudsky-radioabsorbingpropertiesof1xbifeotextrm3xlamnotextrm301x09solidsolutions-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://www.tandfonline.com/doi/full/10.1080/00150193.2023.2189843\"},\"keyword\":[\"Q4\"],\"metadata\":{\"authorlinks\":{}},\"html\":\"\"},{\"bibtype\":\"incollection\",\"type\":\"incollection\",\"title\":\"Investigation of the Microwave Properties of the Transparent Piezoceramics PLZT\",\"url\":\"https://link.springer.com/10.1007/978-3-031-21572-8_16\",\"author\":[{\"propositions\":[],\"lastnames\":[\"Sidorenko\"],\"firstnames\":[\"E.\",\"N.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudskaya\"],\"firstnames\":[\"A.\",\"G.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Natkhin\"],\"firstnames\":[\"I.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Rudsky\"],\"firstnames\":[\"D.\",\"I.\"],\"suffixes\":[]},{\"propositions\":[],\"lastnames\":[\"Shpanko\"],\"firstnames\":[\"S.\",\"P.\"],\"suffixes\":[]}],\"year\":\"2023\",\"doi\":\"10.1007/978-3-031-21572-8_16\",\"pages\":\"189–196\",\"bibtex\":\"@incollection{sidorenko_investigation_2023,\\n\\ttitle = {Investigation of the {Microwave} {Properties} of the {Transparent} {Piezoceramics} {PLZT}},\\n\\turl = {https://link.springer.com/10.1007/978-3-031-21572-8_16},\\n\\tauthor = {Sidorenko, E. N. and Rudskaya, A. G. and Natkhin, I. I. and Rudsky, D. I. and Shpanko, S. P.},\\n\\tyear = {2023},\\n\\tdoi = {10.1007/978-3-031-21572-8_16},\\n\\tpages = {189--196},\\n}\\n\",\"author_short\":[\"Sidorenko, E. N.\",\"Rudskaya, A. G.\",\"Natkhin, I. I.\",\"Rudsky, D. I.\",\"Shpanko, S. P.\"],\"key\":\"sidorenko_investigation_2023\",\"id\":\"sidorenko_investigation_2023\",\"bibbaseid\":\"sidorenko-rudskaya-natkhin-rudsky-shpanko-investigationofthemicrowavepropertiesofthetransparentpiezoceramicsplzt-2023\",\"role\":\"author\",\"urls\":{\"Paper\":\"https://link.springer.com/10.1007/978-3-031-21572-8_16\"},\"metadata\":{\"authorlinks\":{}},\"html\":\"\"}],\n      metadata: {\"authorlinks\":{}},\n      ownerID: undefined\n    };\n  </script>\n\n  <script type=\"text/javascript\">\n  var site$;\n  if (typeof $ != 'undefined') {\n    console.log('existing jquery: storing and then restoring');\n    site$ = $;\n    $ = null;\n  }\n  </script>\n\n  <script src=\"https://ajax.googleapis.com/ajax/libs/jquery/2.2.4/jquery.min.js\">\n  </script>\n  <script type=\"text/javascript\">\n  if (site$) {\n    console.log('existing jquery: avoiding conflict and restoring');\n    bb$ = $.noConflict(true);\n    $ = site$;\n  } else {\n    bb$ = $;\n  }\n  </script>\n\n  <script src=\"//bibbase.org/js/bibbase.min.js\"\n          type=\"text/javascript\">\n  </script>\n\n  <script type=\"text/javascript\"\n          src=\"https://cdnjs.cloudflare.com/ajax/libs/mathjax/2.7.1/MathJax.js?config=TeX-AMS-MML_HTMLorMML\">\n  </script>\n  <script type=\"text/x-mathjax-config\">\n    MathJax.Hub.Config({tex2jax: {inlineMath: [['$','$'], ['\\\\(','\\\\)']]},\n                        skipTags: [\"body\"],\n                        processClass: \"bibbase_paper\"});\n  </script>\n\n  <style>\n  @media print {\n    .dontprint {\n        display: none !important;\n    }\n\n  .bibbase_group {\n    background-color: #E0E0E0;\n    font-style: italic;\n    font-size: larger;\n    text-shadow: 0px 0px 3px #FFFFFF;\n    border-radius: 4px 4px 4px 4px;\n    -moz-border-radius: 4px 4px 4px 4px;\n    -webkit-border-radius: 4px;\n    padding: 5px 40px 5px;\n    margin-top: 10px;\n    margin-bottom: 5px;\n    cursor: pointer;\n  }\n\n  .bibbase_paper {\n    margin-bottom: 5px;\n  }\n\n  }\n  </style>\n\n  \n  <div style=\"float: right; margin-right: 10px; margin-top: 10px; text-align: right; font-size: 12px\">\n    generated by\n    <a href=\"//bibbase.org\"\n       onclick=\"trackOutboundLink('bibbase', 'logo clicked', window.location.href, '//bibbase.org'); return false;\">\n      <img src=\"//bibbase.org/img/logo.svg\"\n           style=\"vertical-align: middle; margin-left: 3px; height: 16px;\"/\n           alt=\"bibbase.org\"\n           title=\"BibBase – The easiest way to maintain your publications page.\"\n        ></a>\n    \n  </div>\n  \n\n  <div id=\"bibbase_header\" class=\"dontprint\" style=\"\">\n\n    <ul class=\"nav nav-pills\" style=\"margin: 0px;\">\n\n      <li class=\"dropdown\" id=\"groupby_dropdown\">\n      <a class=\"dropdown-toggle\"\n         data-toggle=\"dropdown\"\n         href=\"#\">\n          Group by\n          <b class=\"caret\"></b>\n      </a>\n      <ul class=\"dropdown-menu\">\n        <li class=\"groupby year\"><a onclick=\"groupby('year')\">\n            Year</a>\n        </li>\n        <li class=\"groupby author\"><a onclick=\"groupby('author_short')\">\n            Author</a>\n        </li>\n        <li class=\"groupby type\"><a onclick=\"groupby('type')\">\n            Type</a>\n        </li>\n        <li class=\"groupby keyword\"><a onclick=\"groupby('keyword')\">\n            Keyword</a>\n        </li>\n        <li class=\"groupby downloads\"><a onclick=\"groupby('downloads')\">\n            Downloads</a>\n        </li>\n      </ul>\n      </li>\n\n\n      <li class=\"dropdown\" id=\"menu_dropdown\">\n      <a class=\"dropdown-toggle\"\n         data-toggle=\"dropdown\"\n         href=\"#\" alt=\"controls\">\n          <i class=\"fa fa-reorder\" alt=\"controls\"></i>\n          <b class=\"caret\"></b>\n      </a>\n      <ul class=\"dropdown-menu\">\n        <li>\n          <a onclick=\"toggleAll()\">\n            <i class=\"fa fa-chevron-down fa-fw\"></i> Expand/Collapse All\n          </a>\n        </li>\n        <li>\n          <a download=\"nanokafedra2002-2023.bib\" href=\"data:text/bibtex;base64,@article{konevtsova_hidden_2019,
	title = {Hidden symmetry of the anomalous bluetongue virus capsid and its role in the infection process},
	volume = {15},
	issn = {1744-6848},
	url = {https://pubs.rsc.org/en/content/articlelanding/2019/sm/c9sm01335k},
	doi = {10.1039/C9SM01335K},
	abstract = {Clear understanding of the principles that control the arrangement of proteins and their self-assembly into viral shells is very important for the development of antiviral strategies. Here we consider the structural peculiarities and hidden symmetry of the anomalous bluetongue virus (BTV) capsid. Each of its three concentric shells violates the paradigmatic geometrical model of Caspar and Klug, which is otherwise well suited to describe most of the known icosahedral viral shells. As we show, three icosahedral spherical lattices, which are commensurate with each other and possess locally hexagonal (primitive or honeycomb) order, underlie the proteinaceous shells of the BTV capsid. This interpretation of the multishelled envelope allows us to discuss the so-called “symmetry mismatch” between its layers. We also analyze the structural stability of the considered spherical lattices on the basis of the classical theory of spherical packing and relate the proximity of the outer spherical lattice to destabilization with the fact that during infection of the cell VP2 trimers are detached from the surface of the BTV capsid. An electrostatic mechanism that can assist in this detachment is discussed in detail.},
	language = {en},
	number = {38},
	urldate = {2023-11-11},
	journal = {Soft Matter},
	author = {Konevtsova, Olga V. and Roshal, Daria S. and Božič, Anže Lošdorfer and Podgornik, Rudolf and Rochal, Sergey},
	month = oct,
	year = {2019},
	note = {Publisher: The Royal Society of Chemistry},
	pages = {7663--7671},
}



@inproceedings{belyanchikov_hertz--terahertz_2019,
	title = {Hertz-to-terahertz dielectric response of nanoconfined water molecules},
	url = {https://ieeexplore.ieee.org/document/8873987},
	doi = {10.1109/IRMMW-THz.2019.8873987},
	abstract = {Broad-band dielectric spectroscopy, heat capacity measurements and molecular dynamic simulations are applied to study excitations of interacting electric dipoles spatially arranged in a network with an inter-dipole distance of 5-10 Å. The dipoles with magnitude of 1.85 Debye are represented by single H2O molecules located in voids (0.5 nm size) formed by ions of the crystal lattice of cordierite. We discover emergence of nontrivial disordered paraelectric phase of dipolar system with signs of phase transition below 3 K.},
	urldate = {2023-11-11},
	booktitle = {2019 44th {International} {Conference} on {Infrared}, {Millimeter}, and {Terahertz} {Waves} ({IRMMW}-{THz})},
	author = {Belyanchikov, M. and Savinov, M. and Bednyakov, P. and Bedran, Z. and Thomas, V. and Torgashev, V. and Prokhorov, A. and Loidl, A. and Lunkenheimer, P. and Zhukova, E. and Uykur, E. and Dressel, M. and Gorshunov, B.},
	month = sep,
	year = {2019},
	note = {ISSN: 2162-2035},
	pages = {1--3},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\DNQPGUUM\\Belyanchikov и др. - 2019 - Hertz-to-terahertz dielectric response of nanoconf.pdf:application/pdf;IEEE Xplore Abstract Record:C\:\\Users\\aleks\\Zotero\\storage\\RR6G2M8H\\8873987.html:text/html},
}



@article{andronikova_structural_2019,
	title = {Structural {Peculiarities} of the {Intermediate} {Phase} in {Zr}-{Rich} {Lead} {Zirconate} {Titanate}},
	volume = {61},
	issn = {1090-6460},
	url = {https://doi.org/10.1134/S1063783419100056},
	doi = {10.1134/S1063783419100056},
	abstract = {This paper presents the results of X-ray diffraction studies on a single crystal of lead zirconate titanate PbZr0.993Ti0.007O3 in the region of existence of an intermediate ferroelectric phase. In addition to the known superstructure reflections of the M type qM = \$\${\textbackslash}left{\textbackslash}\{ \{{\textbackslash}frac\{1\}\{2\},{\textbackslash}frac\{1\}\{2\},0\} {\textbackslash}right{\textbackslash}\}\$\$and the first-order satellite reflections qM + \{δ, δ, δ\}, unknown second-order satellites have been observed near qM and near the Bragg reflections. Structural model of regular system of antiphase domains is used for diffraction calculation. The model is shown to describe the first- and second-orders satellite reflections in the vicinity of qM, but it cannot explain the appearance of satellites around the main Bragg peaks. A possible origin of the system of the superstructures observed in the intermediate phase is discussed.},
	language = {en},
	number = {10},
	urldate = {2023-11-11},
	journal = {Physics of the Solid State},
	author = {Andronikova, D. A. and Bronwald, I. A. and Leontyev, N. G. and Leontyev, I. N. and Chernyshov, D. Yu. and Filimonov, A. V. and Vakhrushev, S. B.},
	month = oct,
	year = {2019},
	keywords = {ferroelectrics, phase transitions, and crystal structure, perovskite structure, X-ray scattering},
	pages = {1772--1778},
}



@article{rochal_chirality_2019,
	title = {Chirality manifestation in elastic coupling between the layers of double-walled carbon nanotubes},
	volume = {11},
	issn = {2040-3372},
	url = {https://pubs.rsc.org/en/content/articlelanding/2019/nr/c9nr03853a},
	doi = {10.1039/C9NR03853A},
	abstract = {The search for new relatively easy physicochemical methods for the structural identification of carbon nanotubes represents a key challenge. Here, analyzing the experimental data on double-walled carbon nanotubes (DWCNTs) obtained by us and taken from the literature, we have expressed the magnitude of elastic coupling between two tubular walls forming a DWCNT as a simple function dependent not only on DWCNT diameters but also on the difference between the chirality angles of the constituent nanotubes. To get this quite unexpected result, which allows us to relate more precisely the structural parameters of a DWCNT with frequencies of its radial breathing-like modes (RBLM), we have developed a new model for the RBLM dynamics that takes into account a possible deposition of water molecules from ambient air onto the DWCNT surface. The model constructed allows us to predict the higher prevalence of DWCNTs comprising two walls with identical handedness. The application of the results obtained for the identification of DWCNTs is also considered.},
	language = {en},
	number = {34},
	urldate = {2023-11-11},
	journal = {Nanoscale},
	author = {Rochal, Sergei and Levshov, Dmitry and Avramenko, Marina and Arenal, Raul and Cao, Thi Thanh and Nguyen, Van Chuc and Sauvajol, Jean-Louis and Paillet, Matthieu},
	month = aug,
	year = {2019},
	note = {Publisher: The Royal Society of Chemistry},
	pages = {16092--16102},
	file = {Supplementary Information PDF:C\:\\Users\\aleks\\Zotero\\storage\\EJHII2SI\\Rochal и др. - 2019 - Chirality manifestation in elastic coupling betwee.pdf:application/pdf},
}



@article{levi_dynamic_2019,
	title = {Some dynamic features of ferroelectric thin films},
	volume = {1260},
	issn = {1742-6596},
	url = {https://dx.doi.org/10.1088/1742-6596/1260/9/092004},
	doi = {10.1088/1742-6596/1260/9/092004},
	abstract = {The dynamic problem of the surface acoustic wave propagation in a thin-film structure is investigated. The propagation of plane waves in the film-substrate structure is considered. Thin film is made of barium titanate oxide, and solid substrate is made of magnesium oxide. Ferroelectric film is subjected to misfit strain because of the deposition. Assumed that the solid substrate retains its properties due to the large difference in the hardness of the materials. Built Green function, obtained phase velocities and electromechanical coupling coefficients in the C-phase of BaTiO3. The present investigation is of practical interest for developing high-frequencies smart ferroelectric devices for engineering applications.},
	language = {en},
	number = {9},
	urldate = {2023-11-11},
	journal = {Journal of Physics: Conference Series},
	author = {Levi, M. O. and Kalinchuk, V. V. and Shirokov, V. B.},
	month = aug,
	year = {2019},
	note = {Publisher: IOP Publishing},
	pages = {092004},
	file = {IOP Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\7XMUB7ZU\\Levi и др. - 2019 - Some dynamic features of ferroelectric thin films.pdf:application/pdf},
}



@article{chalin_low-frequency_2019,
	title = {Low-frequency phonon dynamics and related thermal properties of axially stressed single-walled carbon nanotubes},
	volume = {31},
	issn = {0953-8984},
	url = {https://dx.doi.org/10.1088/1361-648X/ab285c},
	doi = {10.1088/1361-648X/ab285c},
	abstract = {Synthesis temperatures of composite materials are usually far less than the ones of their use, thus carbon nanotubes (CNTs) embedded into a polymer matrix undergo significant axial stress. We develop a continuous theory, which describes the dynamics of stressed single-walled (SW-) CNTs and predicts their low-frequency phonon spectra. The changes in dispersion laws of SWCNT low-frequency phonon modes due to the axial stress of different signs are discussed. Then, the results obtained are used to analyze low-temperature (T {\textless} 70 K) heat capacity and thermal conductivity of individual nanotubes. We demonstrate that compressive stress leads to increase in heat capacity CV of an individual SWCNT, while tensile stress causes CV to decrease. In the latter case at T → 0 heat capacity diminishes according to a linear law T instead of a power one T1/2. Nevertheless, according to our results, axial stress hardly affects low-temperature thermal conductance of SWCNTs. Influence of investigated effects on the corresponding macroscopic properties of CNT-based composite materials are also discussed.},
	language = {en},
	number = {42},
	urldate = {2023-11-11},
	journal = {Journal of Physics: Condensed Matter},
	author = {Chalin, Dmitrii and Avramenko, Marina and Parmeggiani, Andrea and Rochal, Sergei},
	month = jul,
	year = {2019},
	note = {Publisher: IOP Publishing},
	pages = {425302},
}



@article{alyabyeva_influence_2019,
	title = {Influence of chemical substitution on broadband dielectric response of barium-lead {M}-type hexaferrite},
	volume = {21},
	issn = {1367-2630},
	url = {https://dx.doi.org/10.1088/1367-2630/ab2476},
	doi = {10.1088/1367-2630/ab2476},
	abstract = {We report on the electrodynamic properties of the single crystalline lead-substituted M-type barium hexaferrite, Ba0.3Pb0.7Fe12O19, performed in the broad frequency range including radio-frequency, terahertz and sub-terahertz bands, which are particularly important for the development of microelectronic devices. We demonstrate how changing on a molecular level the chemical characteristics (composition, intermolecular interaction, spin-orbital interaction) of lead-substituted M-type hexaferrite influences its radio-frequency and terahertz electrodynamic response. Our results indicate a critical temperature range, 50 K {\textless} T {\textless} 70 K, where significant changes of the electrodynamic response occur that are interpreted as freezing of dynamical oscillations of bi-pyramidal Fe(2b) ions. In the range 5–300 K, the heat capacity shows no sign of any phase transition and is solely determined by electron and phonon contributions. An anomalous electrodynamic response is detected at 1–2 THz that features a rich set of absorption resonances which are associated with electronic transitions within the fine-structured Fe2+ ground state and are visualized in the spectra due to magnetostriction and electron–phonon interaction. We show that lead substitution of barium in barium hexaferrite, BaFe12O19, leads to the emergence of a pronounced dielectric and magnetic relaxational dynamics at radio-frequencies and that both dynamics have the same characteristic relaxation times, thus evidencing the bi-relaxor-like nature of Ba0.3Pb0.7Fe12O19. We associate the origin of the relaxations as connected with the motion of magnetic domain walls. In order to unveil crucial influence of chemical substitution on electrodynamic characteristics of the compound, we analyze our results on substituted compound in comparison with the data available for pristine barium (BaFe12O19) and pristine lead (PbFe12O19) hexaferrites. The obtained spectroscopic data on the dielectric properties of Ba0.3Pb0.7Fe12O19 provide insight into fundamental phenomena responsible for the absorption mechanisms of the compound and demonstrates that chemical ionic substitution is an effective tool to tune the dielectric properties of the whole family of hexaferrites.},
	language = {en},
	number = {6},
	urldate = {2023-11-11},
	journal = {New Journal of Physics},
	author = {Alyabyeva, Liudmila N. and Torgashev, Victor I. and Zhukova, Elena S. and Vinnik, Denis A. and Prokhorov, Anatoliy S. and Gudkova, Svetlana A. and Góngora, David Rivas and Ivek, Tomislav and Tomić, Silvia and Novosel, Nikolina and Starešinić, Damir and Dominko, Damir and Jagličić, Zvonko and Dressel, Martin and Zherebtsov, Dmitry A. and Gorshunov, Boris P.},
	month = jun,
	year = {2019},
	note = {Publisher: IOP Publishing},
	pages = {063016},
	file = {IOP Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\4XWDRV9S\\Alyabyeva и др. - 2019 - Influence of chemical substitution on broadband di.pdf:application/pdf},
}



@article{talanov_group-theoretical_2019,
	title = {Group-{Theoretical} {Classification} of {Aristotypes} of {Cation} and {Anion} {Orders} in {Perovskites}},
	volume = {64},
	issn = {1562-689X},
	url = {https://doi.org/10.1134/S1063774519030258},
	doi = {10.1134/S1063774519030258},
	abstract = {A group-theoretical classification of cation and anion orders of crystals with a perovskite structure is presented. Aristotypes are idealized structures (phases), from which the low-symmetry ordered modifications of perovskites are formed as a result of rotations and deformation of octahedra, as well as the cooperative Jahn–Teller effect and other physical phenomena. Seven aristotype classes have been distinguished, which are characterized by the atomic ordering in each of Wyckoff positions and simultaneous atomic ordering in several positions. The critical and secondary (improper) order parameters, describing the formation of ordered structures, are determined. The classification proposed makes it possible to systematize a variety of known phases, establish genetic structural links between low-symmetry ordered structures, and design new materials.},
	language = {en},
	number = {3},
	urldate = {2023-11-11},
	journal = {Crystallography Reports},
	author = {Talanov, M. V. and Talanov, V. M. and Shirokov, V. B.},
	month = may,
	year = {2019},
	pages = {386--391},
}



@article{lukyanchuk_ferroelectric_2019,
	title = {Ferroelectric multiple-valued logic units},
	volume = {543},
	issn = {0015-0193},
	url = {https://doi.org/10.1080/00150193.2019.1592436},
	doi = {10.1080/00150193.2019.1592436},
	abstract = {Employing many-valued logic (MVL) data processing allows to dramatically increase the performance of computing circuits. Here we propose to employ ferroelectrics for the material implementation of MVL units basing on their ability to pin the polarization as a sequence of multi-stable states. Two conceptual ideas are considered. As the first system, we suggest using the strained ferroelectric films that can host the polarization states, allowing the effective field-induced multilevel switching between them. As the second one, we propose to employ the ferroelectric nano-samples that confine the topologically protected polarization textures, which may be used as MVL structural elements. We demonstrate that these systems are suitable for engineering of the 3-, 4- and even 5-level logic units and consider the circuit design for such elements.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Ferroelectrics},
	author = {Lukyanchuk, Igor and Zaitseva, Elena and Levashenko, Vitaly and Kvassay, Miroslav and Kondovych, Svitlana and Tikhonov, Yuri and Baudry, Laurent and Razumnaya, Anna},
	month = apr,
	year = {2019},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/00150193.2019.1592436},
	keywords = {Ferroelectrics, switching, domain, hysteresis, multiple-valued logic, skyrmion, topological structures, vortex},
	pages = {213--221},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\VXZHNBRF\\Lukyanchuk и др. - 2019 - Ferroelectric multiple-valued logic units.pdf:application/pdf},
}



@article{gorkovaya_properties_2019,
	title = {Properties of the low-frequency phonon spectra of ferroelectric barium titanate-based heterostructures},
	volume = {543},
	issn = {0015-0193},
	url = {https://doi.org/10.1080/00150193.2019.1592446},
	doi = {10.1080/00150193.2019.1592446},
	abstract = {Polarized Raman spectra of the epitaxial Ba0.5Sr0.5TiO3 film, bi-color BaTiO3/Ba0.5Sr0.5TiO3 superlattice and tri-color BaTiO3/Ba0.5Sr0.5TiO3/SrTiO3 superlattice were studied in a broad temperature range of 80–700 K. Based on the temperature dependence of the polar modes we determined the phase transitions temperatures in the studied heterostructures. In the sub-THz frequency range of the Y(XZ)Y¯spectra, we revealed the coexistence of the Debye-type central peak and soft mode in bi-color BaTiO3/Ba0.5Sr0.5TiO3 superlattice.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Ferroelectrics},
	author = {Gor’kovaya, E. D. and Tikhonov, Yu. A. and Torgashev, V. I. and Mikheykin, A. S. and Lukyanchuk, I. A. and Mezzane, D. and Ortega, N. and Kumar, A. and Katiyar, R. S. and Razumnaya, A. G.},
	month = apr,
	year = {2019},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/00150193.2019.1592446},
	keywords = {Raman spectroscopy, soft mode, central peak, superlattice, thin film},
	pages = {36--47},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\PCXC4STE\\Gor’kovaya и др. - 2019 - Properties of the low-frequency phonon spectra of .pdf:application/pdf},
}



@article{roshal_ph-induced_2019,
	title = {{pH}-induced morphological changes of proteinaceous viral shells},
	volume = {9},
	copyright = {2019 The Author(s)},
	issn = {2045-2322},
	url = {https://www.nature.com/articles/s41598-019-41799-6},
	doi = {10.1038/s41598-019-41799-6},
	abstract = {Changes in environmental pH can induce morphological changes in empty proteinaceous shells of bacteriophages in vitro that are very similar to changes occurring in viral capsids in vivo after encapsidation of DNA. These changes in capsid shape and size cannot be explained with a simple elastic model alone. We propose a new theoretical framework that combines the elasticity of thin icosahedral shells with the pH dependence of capsid charge distribution. Minimization of the sum of elastic and electrostatic free energies leads to equilibrium shapes of viral shells that depend on a single elastic parameter and the detailed configuration of the imbedded protein charges. Based on the in vitro shell reconstructions of bacteriophage HK97 we elucidate the details of how the reversible transition between Prohead II and Expansion Intermediate II states of the HK97 procapsid is induced by pH changes, as well as some other features of the bacteriophage maturation.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Scientific Reports},
	author = {Roshal, D. and Konevtsova, O. and Lošdorfer Božič, A. and Podgornik, R. and Rochal, S.},
	month = mar,
	year = {2019},
	note = {Number: 1
Publisher: Nature Publishing Group},
	keywords = {Biological physics, Molecular self-assembly},
	pages = {5341},
	file = {Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\MGU2DMMM\\Roshal и др. - 2019 - pH-induced morphological changes of proteinaceous .pdf:application/pdf},
}



@article{lerer_absorbing_2019,
	title = {Absorbing {Two}-{Dimensionally} {Periodic} {Structures} on {New} {Plasmonic} {Materials}},
	volume = {61},
	issn = {1573-9120},
	url = {https://doi.org/10.1007/s11141-019-09938-1},
	doi = {10.1007/s11141-019-09938-1},
	abstract = {We study theoretically two-dimensionally periodic gratings of plasmonic strips on substrates which contain dielectric and plasmonic layers. The developed electrodynamic model is based on solving the vector integro-differential equation of diffraction by three-dimensional dielectric bodies by the Galerkin method. It is shown that at the resonant frequencies of the surface plasmon polariton, these structures absorb almost 100\% of the energy of the incident radiation in a wide wavelength range. The use of nonmetal plasmonic materials makes it possible to create a wideband absorber of infrared waves.},
	language = {en},
	number = {11},
	urldate = {2023-11-11},
	journal = {Radiophysics and Quantum Electronics},
	author = {Lerer, A. M. and Golovacheva, E. V. and Ivanova, I. N. and Makhno, V. V. and Timoshenko, P. E.},
	month = apr,
	year = {2019},
	pages = {801--805},
}



@article{faddeev_electrocatalytic_2019,
	title = {Electrocatalytic {Properties} of {Rh}/{C} and {Pt}-{Rh}/{C} {Catalysts} {Fabricated} by the {Method} of {Electrochemical} {Dispersion}},
	volume = {55},
	issn = {1608-3342},
	url = {https://doi.org/10.1134/S1023193519030066},
	doi = {10.1134/S1023193519030066},
	abstract = {The Pt/C, Rh/C, and Pt-Rh/C catalytic systems with uniform distribution of metal phase over the surface of carbon support and an average size of Pt and Rh nanoparticles of 7.3 and 6.5 nm, respectively, are fabricated by the method of electrochemical dispersion of metals in the aqueous electrolytes containing Na+. It is shown that the double-layer potential E = 300 mV (RHE) is the optimal potential of CO adsorption for determining the electrochemically active surface area of Pt/C, Rh/C, and Pt-Rh/C catalysts by the method of oxidative desorption of CO. The introduction of Rh into the Pt/C catalyst enables us to increase the specific activity and reduce the potential of the onset of methanol oxidation.},
	language = {en},
	number = {4},
	urldate = {2023-11-11},
	journal = {Russian Journal of Electrochemistry},
	author = {Faddeev, N. A. and Kuriganova, A. B. and Leont′ev, I. N. and Smirnova, N. V.},
	month = apr,
	year = {2019},
	keywords = {electrochemical dispersion, fuel cell, electrocatalysis, platinum, rhodium},
	pages = {346--350},
}



@article{southern_federal_university_high-pressure_2019,
	title = {High-pressure container for the research of phase transitions of ferroelectrics under variable hydrostatic pressure, electric field strength and temperature},
	volume = {8},
	issn = {22254293},
	url = {http://red.jfop.ru/jfop-1901-022029},
	doi = {10.25210/jfop-1901-022029},
	number = {1},
	urldate = {2023-11-11},
	journal = {Физические основы приборостроения},
	author = {{Southern Federal University} and Leontiev, I.N. and Panich, A.E. and {Southern Federal University} and Smotrakov, V.G. and {Southern Federal University} and Fesenko, O.E. and {Southern Federal University}},
	month = mar,
	year = {2019},
	pages = {22--29},
}



@article{hanani_enhancement_2019,
	series = {Materials {Science} for {Green} {Energy} {Ifran} {City}},
	title = {Enhancement of dielectric properties of lead-free {BCZT} ferroelectric ceramics by grain size engineering},
	volume = {127},
	issn = {0749-6036},
	url = {https://www.sciencedirect.com/science/article/pii/S0749603617323121},
	doi = {10.1016/j.spmi.2018.03.004},
	abstract = {Lead-free Ba0.85Ca0.15Ti0.9Zr0.1O3 (BCZT) ceramics had attracted much attention for the fabrication of microelectronic devices by virtue of their excellent dielectric, ferroelectric and piezoelectric properties. To understand the effects of both mean grain size and grain size distribution on the dielectric properties of lead-free Ba0.85Ca0.15Ti0.9Zr0.1O3 (BCZT) ferroelectric relaxors, an original method was proposed. It is based on the surfactant-assisted solvothermal processing coupled with low-temperature conventional sintering at 1250 °C. In this way, three highly dense BCZT with different mean grain size and dissimilar grain size distribution were designed. A significant increase of dielectric properties was obtained by a control of grain size and densification process. The dielectric constants measured were ranged from 5370 to 9646 and the dielectric loss was enhanced by 70\%. Surprisingly, it was evidenced that there is unequivocal link between mean grain size with dielectric properties. Indeed, it was found that the presence of high density of refined grains leads to an improvement of dielectric properties due to an enhancement of densification. This work may provide a new strategy to design ferroelectric materials with enhanced properties.},
	urldate = {2023-11-11},
	journal = {Superlattices and Microstructures},
	author = {Hanani, Z. and Mezzane, D. and Amjoud, M. and Fourcade, S. and Razumnaya, A. G. and Luk'yanchuk, I. A. and Gouné, M.},
	month = mar,
	year = {2019},
	keywords = {BCZT, Dielectric, Ferroelectric, Lead-free, Microstructure, Relaxor},
	pages = {109--117},
	file = {Принятая версия:C\:\\Users\\aleks\\Zotero\\storage\\ZTGFIZUV\\Hanani и др. - 2019 - Enhancement of dielectric properties of lead-free .pdf:application/pdf;ScienceDirect Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\AEC2RSBJ\\S0749603617323121.html:text/html},
}



@article{lukyanchuk_harnessing_2019,
	title = {Harnessing ferroelectric domains for negative capacitance},
	volume = {2},
	copyright = {2019 The Author(s)},
	issn = {2399-3650},
	url = {https://www.nature.com/articles/s42005-019-0121-0},
	doi = {10.1038/s42005-019-0121-0},
	abstract = {A pressing quest for overcoming Boltzmann tyranny in low-power nanoscale electronics ignited an extensive search for the devices possessing the negative circuit constants. The emergent concept of the ferroelectric-based negative capacitance triggered then the explosive activity in the field. However, most of the research addressed transient negative capacitance, leaving the basic question of the existence of the steady-state negative capacitance unresolved. Here, we show that the ferroelectric nanodot capacitor hosts a stable two-domain state realizing the static reversible negative capacitance device thus opening routes for the extensive use of the negative capacitance in domain wall-based nanoelectronics.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Communications Physics},
	author = {Luk’yanchuk, I. and Tikhonov, Y. and Sené, A. and Razumnaya, A. and Vinokur, V. M.},
	month = feb,
	year = {2019},
	note = {Number: 1
Publisher: Nature Publishing Group},
	keywords = {Ferroelectrics and multiferroics, interfaces and thin films, Surfaces},
	pages = {1--6},
	file = {Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\T4E6X2XN\\Luk’yanchuk и др. - 2019 - Harnessing ferroelectric domains for negative capa.pdf:application/pdf},
}



@article{kocharian_ferromagnetism_2019,
	title = {Ferromagnetism and {Giant} {Paramagnetism} of {Copper} {Nanoparticles} in {Carbon} {Matrix}},
	volume = {55},
	issn = {1941-0069},
	url = {https://ieeexplore.ieee.org/document/8476555},
	doi = {10.1109/TMAG.2018.2862413},
	abstract = {Systematic X-ray diffraction, transmission electron microscopy (TEM), Raman and magnetic measurements were performed to study the structural and magnetic properties of copper nanoparticles (NPs) in carbon matrix. The weight concentration of Cu in carbon matrix is 8 wt\%. The carbon-coated core-shell structures with bimodal size distribution with 4 and 300 nm average sizes of NPs are confirmed by scanning electron microscopy and TEM. Our results on magnetization carried out by vibrational magnetometer for copper NPs provide a strong evidence for coexistence of ferromagnetism and giant paramagnetism in wide range of temperature and magnetic field. The magnetic susceptibility at T = 10 K shows high value of giant paramagnetism with χ = 5×10-5 emu/gCuOe while ferromagnetic behavior with hysteresis is preserved up to the room temperature.},
	number = {2},
	urldate = {2023-11-11},
	journal = {IEEE Transactions on Magnetics},
	author = {Kocharian, Armen and Gyulasaryan, Harutyun and Estiphanos, Medhanie and Avramenko, Marina and Nelms, Katherine and Bernal, Oscar and Sharoyan, Eduard and Manukyan, Aram},
	month = feb,
	year = {2019},
	note = {Conference Name: IEEE Transactions on Magnetics},
	pages = {1--4},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\DCWF2WPV\\Kocharian и др. - 2019 - Ferromagnetism and Giant Paramagnetism of Copper N.pdf:application/pdf;IEEE Xplore Abstract Record:C\:\\Users\\aleks\\Zotero\\storage\\CA3E5JSV\\8476555.html:text/html},
}



@article{andronikova_incommensurate_2019,
	title = {Incommensurate instability and diffuse scattering at {Brillouin} zone boundary in {Zr}-rich lead zirconate titanate},
	volume = {538},
	issn = {0015-0193},
	url = {https://doi.org/10.1080/00150193.2019.1569987},
	doi = {10.1080/00150193.2019.1569987},
	abstract = {Detailed study of the X-ray diffuse scattering in the paraelectric phase of the PbZr0.985Ti0.015O3 was carried out. We concentrated on the analysis of the scattering peculiarities in the vicinities of M- and R- points of the Brillouin zone. We have observed a critical increase of the diffuse scattering at the position Q ≈ (0.47 + h 0.53 + k l) slightly aside of M point on cooling to the intermediate phase. We attribute observed critical scattering to a mixed mode containing both oxygen octahedral tilts and antiparallel cationic displacements. Tentative conclusion is made describing earlier reported complicated set of the satellite peaks around M-point as the result of the soft-mode driven incommensurate phase transition.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Ferroelectrics},
	author = {Andronikova, D. A. and Bronwald, Iu. A. and Leontiev, I. N. and Leontiev, N. G. and Chernyshov, D. Yu. and Filimonov, A. V. and Vakhrushev, S. B.},
	month = jan,
	year = {2019},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/00150193.2019.1569987},
	keywords = {phase transitions, diffuse scattering, Ferroelectricity},
	pages = {65--73},
}



@article{kuriganova_new_2019,
	title = {New {Electrochemical} {Approach} for the {Synthesis} of {Pd}-{PdO}/{C} {Electrocatalyst} and {Application} to {Formic} {Acid} {Electrooxidation}},
	volume = {4},
	copyright = {© 2019 Wiley-VCH Verlag GmbH \& Co. KGaA, Weinheim},
	issn = {2365-6549},
	url = {https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201901628},
	doi = {10.1002/slct.201901628},
	abstract = {Pd-PdO/C catalyst for formic acid electrooxidation has been synthesized via electrochemical dispersion of Pd foil electrodes under pulse alternating current conditions in NaCl aqueous electrolyte. About 35 wt\% of the as-prepared Pd-PdO/C specimen is PdO as revealed by X-ray diffraction. The microstructural characteristics and catalytic activity of the synthesized Pd/C catalyst have been compared with those of a Pt/C catalyst prepared under the same conditions. Pd nanoparticles of Pd-PdO/C catalyst exhibit smaller average dimensions and narrower particle size distribution – 7.4±0.5 nm and 1.9±0.5 respectively for Pd and PdO particles. The process of ethanol electrooxidation on the catalyst was characterized by high overvoltage (up to 800 mV). The overvoltage of the formic acid electrochemical oxidation on Pd/C is 590 mV less than on Pt/C.},
	language = {en},
	number = {29},
	urldate = {2023-11-11},
	journal = {ChemistrySelect},
	author = {Kuriganova, Alexandra B. and Faddeev, Nikita A. and Leontyev, Igor N. and Allix, Mathieu and Rakhmatullin, Aydar and Smirnova, Nina V.},
	year = {2019},
	note = {\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/slct.201901628},
	keywords = {alternating current, electrochemical dispersion, formic acid, fuel cell, Pd/C},
	pages = {8390--8393},
	file = {Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\QME9WT8N\\slct.html:text/html},
}



@article{pimonov_anomalous_2019,
	title = {Anomalous small viral shells and simplest polyhedra with icosahedral symmetry: the rhombic triacontahedron case},
	volume = {75},
	copyright = {Copyright (c) 2019 International Union of Crystallography},
	issn = {2053-2733},
	shorttitle = {Anomalous small viral shells and simplest polyhedra with icosahedral symmetry},
	url = {https://journals.iucr.org/a/issues/2019/01/00/eo5089/},
	doi = {10.1107/S2053273318015656},
	abstract = {The symmetry of the capsomers forming a viral shell determines the polyhedron underlying the shell structure. If the capsid is self-assembled from dimers, this is the rhombic triacontahedron with 30 equivalent rhombic faces.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Acta Crystallographica Section A: Foundations and Advances},
	author = {Pimonov, V. V. and Konevtsova, O. V. and Rochal, S. B.},
	month = jan,
	year = {2019},
	note = {Number: 1
Publisher: International Union of Crystallography},
	pages = {135--141},
}



@article{__2019,
	title = {Тепловые флуктуации и резонансные свойства сканирующих зондов на основе углеродных нанотрубок},
	volume = {61},
	issn = {0367-3294},
	url = {https://journals.ioffe.ru/articles/47244},
	doi = {10.21883/FTT.2019.03.47244.237},
	abstract = {AbstractThe design of cantilevers and microelectromechanical systems based on carbon nanotubes necessitates a thorough study of their thermal fluctuations and resonance properties. This work aims at the simulation of thermal fluctuations and power spectral density for single-walled carbon nanotubes in the context of the continuous model of elastic cylindrical membranes with nonmacroscopic thicknesses. The conditions imposed on the geometry of this probe and providing its stable operation, as well as the high lateral resolution determined by only the radius of the nanotube independently on its thermal vibrations, are found, as well. The most intensive resonance modes, making the greatest contribution to the thermal fluctuations of carbon nanotubes, are established, and their frequencies are found analytically.
          , 
            Проектирование кантилеверов и микроэлектромеханических систем с использованием углеродных нанотрубок неразрывно связано с изучением их тепловых флуктуаций и резонансных свойств. В настоящей работе для одностенных углеродных нанотрубок производится расчет тепловых флуктуаций и спектральной плотности интенсивности колебаний в рамках континуальной модели упругих цилиндрических мембран, не обладающих макроскопической толщиной. Найдены налагаемые на геометрию такого зонда условия, выполнение которых обеспечивает как стабильность его работы, так и высокое латеральное разрешение, определяющееся только радиусом нанотрубки и не зависящее от величины ее тепловых колебаний. Определены самые интенсивные резонансные моды, дающие наибольший вклад в тепловые флуктуации углеродных нанотрубок, а также получено аналитическое выражение для их частот.},
	language = {ru},
	number = {3},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Чалин, Д.В. and Авраменко, М.В.},
	year = {2019},
	pages = {514},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\GE9CNIBE\\Чалин и Авраменко - 2019 - Тепловые флуктуации и резонансные свойства сканиру.pdf:application/pdf},
}



@article{chernysheva_synthesis_2018,
	title = {Synthesis of {Co3O4}/{CoOOH} via electrochemical dispersion using a pulse alternating current method for lithium-ion batteries and supercapacitors},
	volume = {86},
	issn = {1293-2558},
	url = {https://www.sciencedirect.com/science/article/pii/S129325581830551X},
	doi = {10.1016/j.solidstatesciences.2018.10.005},
	abstract = {We report a convenient, low-cost and ecofriendly approach for the fabrication of a Co3O4/CoOOH electrode material intended for lithium ion batteries (LIBs) and supercapacitors (SCs) using the electrochemical dispersion of the cobalt foil through the pulse alternating current (PAC) method. The synthesized material is a Co3O4/CoOOH composite (with about 10–15 wt\% CoOOH) in the form of nanosheets with a length of approximately 200 nm and a thickness of 10–20 nm. It is found to exhibit high reversible discharge specific capacities and good cycling behavior while tested as the anode material in LIBs. Measuring the reversible capacitance at high (2C) and low (C/20) cycling rates gives the values of 610 mAh g−1 and 1030 mAh g−1, respectively. The specimen possesses excellent performance as the electrode for SCs with the retention of capacitance up to 98\% at the current density increasing from 0.5 to 10 A g−1. After 1000 cycles at a current density of 10 A g−1 the electrode maintains about 90\% of its initial capacitance which evidences the long cycle life. Hence, electrochemically prepared Co3O4/CoOOH seems to be a promising candidate for high-performance LIBs and SCs applications.},
	urldate = {2023-11-11},
	journal = {Solid State Sciences},
	author = {Chernysheva, Daria and Vlaic, Codruta and Leontyev, Igor and Pudova, Lyudmila and Ivanov, Svetlozar and Avramenko, Marina and Allix, Mathieu and Rakhmatullin, Aydar and Maslova, Olga and Bund, Andreas and Smirnova, Nina},
	month = dec,
	year = {2018},
	pages = {53--59},
	file = {ScienceDirect Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\9GU5I35X\\S129325581830551X.html:text/html},
}



@article{kulbakov_non-isothermal_2018,
	title = {Non-isothermal decomposition of platinum acetylacetonate as a cost-efficient and {Size}-{Controlled} {Synthesis} of {Pt}/{C} nanoparticles},
	volume = {117},
	issn = {1566-7367},
	url = {https://www.sciencedirect.com/science/article/pii/S1566736718303686},
	doi = {10.1016/j.catcom.2018.08.022},
	abstract = {A simple two-stage synthesis of Pt/C nanoparticles based on the non-isothermal decomposition of platinum acetylacetonate is presented. It allows not only production of Pt nanoparticles, but also their sizes control during the synthesis. The heating rate is the key factor for tuning the average Pt nanoparticle size. The electrochemical surface area of produced nanoparticles enlarges with rising heating rate, which can enrich 103 m2/g. The growth dynamics of Pt/C nanoparticles is tracked via in-situ XRD. Furthermore, the electrocatalytic activity of Pt/C catalysts is studied as a function of platinum particle size in cases of ethanol electro-oxidation and oxygen reduction reactions.},
	urldate = {2023-11-11},
	journal = {Catalysis Communications},
	author = {Kulbakov, Anton A. and Kuriganova, Alexandra B. and Allix, Mathieu and Rakhmatullin, Aydar and Smirnova, NinaV. and Maslova, Olga A. and Leontyev, Igor N.},
	month = dec,
	year = {2018},
	keywords = {Pt/C, In-situ, Pt acetylacetonate, Size control, Thermal decomposition},
	pages = {14--18},
}



@article{pryadchenko_effect_2018,
	title = {Effect of {Thermal} {Treatment} on the {Atomic} {Structure} and {Electrochemical} {Characteristics} of {Bimetallic} {PtCu} {Core}–{Shell} {Nanoparticles} in {PtCu}/{C} {Electrocatalysts}},
	volume = {122},
	issn = {1932-7447},
	url = {https://doi.org/10.1021/acs.jpcc.8b03696},
	doi = {10.1021/acs.jpcc.8b03696},
	abstract = {Supported PtCu/C electrocatalysts containing core–shell bimetallic PtCu nanoparticles were synthesized by sequential chemical reduction of Cu2+ and Pt(IV) in a carbon suspension, prepared on the basis of ethylene glycol–water solvent, and then treated at different temperatures in the range from 250 to 350 °C. The structural characterization of “as-prepared” PtCu nanoparticles and of those obtained after the thermal treatments was performed by transmission electron microscopy, X-ray diffraction, and Pt L3- and Cu K-edge extended X-ray absorption fine structure spectroscopy. The atomic cluster models of PtCu nanoparticles before and after the thermal treatment, reflecting the character of the components’ distribution, were generated. The electrochemical performance of the obtained PtCu/C electrocatalysts in oxygen reduction reaction was studied by cycling and linear voltammetry.},
	number = {30},
	urldate = {2023-11-11},
	journal = {The Journal of Physical Chemistry C},
	author = {Pryadchenko, Vasiliy V. and Belenov, Sergey V. and Shemet, Darya B. and Srabionyan, Vasiliy V. and Avakyan, Leon A. and Volochaev, Vadim A. and Mikheykin, Alexey S. and Bdoyan, Karina E. and Zizak, Ivo and Guterman, Vladimir E. and Bugaev, Lusegen A.},
	month = aug,
	year = {2018},
	note = {Publisher: American Chemical Society},
	pages = {17199--17210},
}



@article{kuriganova_ptirc_2018,
	title = {{PtIr}/{C} {Catalysts} {Synthesized} by {Electrochemical} {Dispersion} {Method} for {Proton} {Exchange} {Membrane} {Fuel} {Cells}},
	volume = {54},
	issn = {1608-3342},
	url = {https://doi.org/10.1134/S1023193518060113},
	doi = {10.1134/S1023193518060113},
	abstract = {PtIr/C electrocatalyst with the metal phase uniformly distributed over the carbon support surface and the average size of PtIr nanoparticles of 5.9 nm is synthesized by electrochemical dispersion of Pt90Ir10 alloy under the action of alternating pulse current. It is shown that the presence of iridium within the composition of a Pt/C catalyst lowers down the overpotential of CO oxidation and increases catalyst’s specific activity with respect to electrochemical oxidation of ethanol.},
	language = {en},
	number = {6},
	urldate = {2023-11-11},
	journal = {Russian Journal of Electrochemistry},
	author = {Kuriganova, A. B. and Leont’ev, I. N. and Smirnova, N. V.},
	month = jun,
	year = {2018},
	keywords = {electrochemical dispersion, fuel cell, electrocatalysis, platinum, iridium},
	pages = {561--565},
}



@article{dmitriev_crystallography_2018,
	title = {Crystallography {Based} on {Synchrotron} {Radiation}: {Experiments} of {Russian} {Users} of the {ESRF} {BM01} {Diffraction} {Beam} {Line}},
	volume = {12},
	issn = {1819-7094},
	shorttitle = {Crystallography {Based} on {Synchrotron} {Radiation}},
	url = {https://doi.org/10.1134/S1027451018030084},
	doi = {10.1134/S1027451018030084},
	abstract = {The review deals with studies carried out at the BM01 diffraction beam line of the European Synchrotron Radiation Facility. X-ray diffraction analysis of single-crystal proton conductors demonstrates the possibilities of a precise diffraction experiment in which phase transitions associated with the release of crystallization water and transformation of the network of hydrogen contacts are investigated. Scanning of reciprocal space with the help of a 2D detector enables us to determine the new phase symmetry in a thin-film multiferroic sample based on bismuth ferrite (the given phase is stable only under thin-film conditions). A combination of Bragg and diffusion scattering processes is employed to investigate the interdependence between the structure and dynamics of a crystal lattice and the physical properties of a relaxor material with a perovskite-like structure. The complementarity and synergy of neutron and synchrotron experiments are demonstrated using the combined study of materials from the manganese-silicide group, which has revealed a nontrivial relationship between magnetic and crystallographic chiralities in noncollinear magnets. Although the given review is limited to only a few experiments carried out by Russian scientists at the BM01 beam line, they still illustrate a variety of problems that can be solved using a modern diffraction station where the bending magnet of a third-generation synchrotron is employed as the synchrotron radiation source.},
	language = {en},
	number = {3},
	urldate = {2023-11-11},
	journal = {Journal of Surface Investigation: X-ray, Synchrotron and Neutron Techniques},
	author = {Dmitriev, V. P. and Chernyshov, D. Yu. and Dyadkin, V. A. and Makarova, I. P. and Leontyev, I. N. and Andronikova, D. A. and Bronwald, I. and Burkovsky, R. G. and Vakhrushev, S. B. and Filimonov, A. V. and Grigoriev, S. V.},
	month = may,
	year = {2018},
	keywords = {crystallography, synchrotron X-ray diffraction, X-ray analysis},
	pages = {395--407},
}



@article{shirokov_optical_2018,
	title = {Optical {Properties} of {Barium} {Strontium} {Niobate} {SBN61} {Films}},
	volume = {60},
	issn = {1090-6460},
	url = {https://doi.org/10.1134/S1063783418050293},
	doi = {10.1134/S1063783418050293},
	abstract = {Heteroepitaxial Sr0.61Ba0.39Nb2O6 films have been formed on MgO(001) substrates by RF deposition in an oxygen atmosphere. The film orientation with respect to the substrate is investigated using X-ray diffraction. The permittivity dispersion parameters in the visible range are determined by measuring optical transmission spectra. The films are found to have a wider band gap and a smaller refractive index as compared with the single-crystal material.},
	language = {en},
	number = {5},
	urldate = {2023-11-11},
	journal = {Physics of the Solid State},
	author = {Shirokov, V. B. and Pavlenko, A. V. and Stryukov, D. V. and Revinskii, Yu. V.},
	month = may,
	year = {2018},
	pages = {1005--1010},
}



@article{kuriganova_electrochemically_2018,
	title = {Electrochemically synthesized {Pt}-based catalysts with different carbon supports for proton exchange membrane fuel cell applications},
	volume = {28},
	issn = {0959-9436},
	url = {https://www.sciencedirect.com/science/article/pii/S0959943618301834},
	doi = {10.1016/j.mencom.2018.07.036},
	abstract = {The Pt/C catalysts containing various types of carbon support were prepared via electrochemical oxidation/dispersion. Their different catalytic activity in CO-stripping and ethanol electrooxidation was revealed.},
	number = {4},
	urldate = {2023-11-11},
	journal = {Mendeleev Communications},
	author = {Kuriganova, Alexandra B. and Leontyev, Igor N. and Maslova, Olga A. and Smirnova, Nina V.},
	month = jul,
	year = {2018},
	pages = {444--446},
}



@article{shirokov_electric-field-dependent_2018,
	title = {Electric-field-dependent mechanical and electrical properties of barium strontium titanate films for tunable device applications},
	volume = {657},
	issn = {0040-6090},
	url = {https://www.sciencedirect.com/science/article/pii/S0040609018302918},
	doi = {10.1016/j.tsf.2018.04.029},
	abstract = {Developing the novel electric field tunable, reconfigurable, adaptive and frequency-agile microwave devices with specific properties involves technological and scientific activities in the studying of material properties. Measurements of its properties could be a difficult and expensive issue, especially when it concerns thin-film ferroelectrics. Their electromechanical properties change significantly under applied DC bias field. The material coefficients of barium strontium titanate thin films are still unknown; therefore, it is expedient to carry out their calculations. In the present paper, the linear equations of piezoelectric effect have been written for thin barium strontium titanate films under DC bias electric field in paraelectric phase (induced piezoelectric effect) based on the grand potential of Landau theory of phase transitions. The dependence of material constants for thin films of Ba0.65Sr0.35TiO3 (BST65) on the applied planar field at different lattice misfit strains has been studied for this phase. All induced piezoelectric moduli show extreme behavior during field alteration. Elastic moduli show similar abnormal behavior. The alterations increase as misfit strain is approaching the critical value.},
	urldate = {2023-11-11},
	journal = {Thin Solid Films},
	author = {Shirokov, V. B. and Kalinchuk, V. V. and Timoshenko, P. E.},
	month = jul,
	year = {2018},
	keywords = {Phenomenological theory, Phase transitions, Barium strontium titanate, Ferroelectric thin film},
	pages = {8--15},
}



@inproceedings{kaydashev_macroscopic_2018,
	title = {Macroscopic monolayer of plasmon coupled gold nanoparticles on mirror for fluorescence enhancement},
	volume = {10716},
	url = {https://www.spiedigitallibrary.org/conference-proceedings-of-spie/10716/107161F/Macroscopic-monolayer-of-plasmon-coupled-gold-nanoparticles-on-mirror-for/10.1117/12.2315071.full},
	doi = {10.1117/12.2315071},
	abstract = {We study an ability of a large quasi-homogeneous monolayer of Au plasmon coupled nanoparticles separated from continuous Au film by polymer spacer to enhance a fluorescence of adsorbed molecular species. A fluorescence response of Methylene Blue molecules is studied as a function of polymer film thickness. A change of plasmonic properties of a system, its ability to enhance a fluorescence and the possible heating of a structure upon light absorption are discussed.},
	urldate = {2023-11-11},
	booktitle = {Saratov {Fall} {Meeting} 2017: {Optical} {Technologies} in {Biophysics} and {Medicine} {XIX}},
	publisher = {SPIE},
	author = {Kaydashev, V. E. and Zolotukhin, P. and Belanova, A. and Anokhin, A. S. and Zharinov, V. S. and Kaidashev, E. M.},
	month = apr,
	year = {2018},
	pages = {357--363},
}



@inproceedings{kaydashev_sers_2018,
	title = {{SERS} of {Methylene} {Blue} induced by plasmonic coupled nanoparticle arrays},
	volume = {10716},
	url = {https://www.spiedigitallibrary.org/conference-proceedings-of-spie/10716/107161E/SERS-of-Methylene-Blue-induced-by-plasmonic-coupled-nanoparticle-arrays/10.1117/12.2315007.full},
	doi = {10.1117/12.2315007},
	abstract = {We study the surface enhanced Raman scattering of Methylene Blue (MB) dye molecules induced by large quasihomogeneous arrays of plasmon coupled 5-8 nm Au nanoparticle separated by distances less than 10 nm. Also, the variation of the fluorescence enhancement/SERS properties for as-prepared coupled particles and agglomerated particles obtained upon heat treatment and percolation-like films is analyzed for two measurement protocols, i.e. when measured through the solution and for a monolayer of MB molecules chemisorbed on a surface.},
	urldate = {2023-11-11},
	booktitle = {Saratov {Fall} {Meeting} 2017: {Optical} {Technologies} in {Biophysics} and {Medicine} {XIX}},
	publisher = {SPIE},
	author = {Kaydashev, V. E. and Lyanguzov, N. V. and Anokhin, A. S. and Chernishov, A. and Kaidashev, E. M.},
	month = apr,
	year = {2018},
	pages = {350--356},
}



@article{shirokov_properties_2018,
	title = {Properties of {Thin} {Films} of {Barium}–{Strontium} {Titanate} {Solid} {Solutions} by {Induced} {Piezoelectric} {Effect}},
	volume = {63},
	issn = {1562-6903},
	url = {https://doi.org/10.1134/S1028335818040092},
	doi = {10.1134/S1028335818040092},
	abstract = {Piezoelectric effect equations have been derived by linearizing the nonlinear equations of state of a thin film existing in a paraelectric phase in the presence of an external electrical field (induced piezoelectric effect). The behavior of the piezoelectric and elastic constants of thin films of a solid barium–strontium titanate solution BST065 (x = 0.65) in a planar field at different misfit strain values has been studied numerically.},
	language = {en},
	number = {4},
	urldate = {2023-11-11},
	journal = {Doklady Physics},
	author = {Shirokov, V. B. and Kalinchuk, V. V. and Timoshenko, P. E.},
	month = apr,
	year = {2018},
	pages = {142--146},
}



@article{popov_computational_2018,
	title = {Computational study of the shift of the {G} band of double-walled carbon nanotubes due to interlayer interactions},
	volume = {97},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.97.165417},
	doi = {10.1103/PhysRevB.97.165417},
	abstract = {The interactions between the layers of double-walled carbon nanotubes induce a measurable shift of the G bands relative to the isolated layers. While experimental data on this shift in freestanding double-walled carbon nanotubes has been reported in the past several years, a comprehensive theoretical description of the observed shift is still lacking. The prediction of this shift is important for supporting the assignment of the measured double-walled nanotubes to particular nanotube types. Here, we report a computational study of the G-band shift as a function of the semiconducting inner layer radius and interlayer separation. We find that with increasing interlayer separation, the G band shift decreases, passes through zero and becomes negative, and further increases in absolute value for the wide range of considered inner layer radii. The theoretical predictions are shown to agree with the available experimental data within the experimental uncertainty.},
	number = {16},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Popov, Valentin N. and Levshov, Dmitry I. and Sauvajol, Jean-Louis and Paillet, Matthieu},
	month = apr,
	year = {2018},
	note = {Publisher: American Physical Society},
	pages = {165417},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\VT7RDBBS\\Popov и др. - 2018 - Computational study of the shift of the G band of .pdf:application/pdf},
}



@article{timoshenko_finite-element_2018,
	title = {Finite-element analysis of scattering parameters of surface acoustic wave bandpass filter formed on barium titanate thin film},
	volume = {9},
	issn = {1947-5411},
	url = {https://doi.org/10.1080/19475411.2018.1447045},
	doi = {10.1080/19475411.2018.1447045},
	abstract = {The frequency dependence of scattering parameters of interdigital surface acoustic wave transducers placed on ferroelectric barium titanate (BaTiO3) epitaxial film in c-phase coated over magnesium oxide has been studied using the finite-element method (FEM) approach along with the perfectly matched layer (PML) technique. The interdigital transducer which has a comb-like structure with aluminum electrodes excites the mechanical wave. The distance between the fingers allows tuning the frequency properties of the wave propagation. The magnesium oxide is taken as the substrate. The two-dimensional model of two-port surface acoustic wave filter is created to calculate scattering parameters and to show how to design the fixture in COMSOLTM. Some practical computational challenges of finite element modeling of SAW devices in COMSOLTM are shown. The effect of lattice misfit strain on acoustic properties of heterostructures of BaTiO3 epitaxial film in c-phase at room temperature is discussed in present article for two low-frequency surface acoustic resonances.},
	number = {2},
	urldate = {2023-11-11},
	journal = {International Journal of Smart and Nano Materials},
	author = {Timoshenko, Pavel E. and Kalinchuk, Valery V. and Shirokov, Vladimir B.},
	month = apr,
	year = {2018},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/19475411.2018.1447045},
	keywords = {thin films, ferroelectrics, COMSOL, finite element method (FEM), SAW filters},
	pages = {88--98},
	file = {Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\AAZMSR86\\Timoshenko и др. - 2018 - Finite-element analysis of scattering parameters o.pdf:application/pdf},
}



@article{ulyankina_large-scale_2018,
	title = {Large-scale synthesis of {ZnO} nanostructures by pulse electrochemical method and their photocatalytic properties},
	volume = {76},
	issn = {1369-8001},
	url = {https://www.sciencedirect.com/science/article/pii/S1369800117320528},
	doi = {10.1016/j.mssp.2017.12.011},
	abstract = {In this paper, we report a simple environment-friendly and large-scale approach to synthesis of highly crystalline zinc oxide nanostructures using pulse alternating current (PAC). The morphological results demonstrate flower-like architectures of nanoparticle-based and nanorod-based zinc oxide (ZnO-NPs and ZnO-NRs) obtained in KCl and NaCl as electrolytes. The photocatalytic activity of the obtained materials was performed in methylene blue dye degradation reaction under UV light irradiation. A high efficiency of {\textasciitilde} 90\% within 60min with excellent rate constant (k = 0.0386min−1) was observed in the presence of ZnO-NPs synthesized in 2M KCl which is attributed to the larger specific surface area (27m2g−1), total pore volume and more defective structure.},
	urldate = {2023-11-11},
	journal = {Materials Science in Semiconductor Processing},
	author = {Ulyankina, Anna and Leontyev, Igor and Avramenko, Marina and Zhigunov, Denis and Smirnova, Nina},
	month = mar,
	year = {2018},
	keywords = {Electrochemical synthesis, Nanocrystalline materials, Photocatalytic activity, Pulse alternating current, Semiconductors, ZnO},
	pages = {7--13},
}



@article{mikheykin_nature_2018,
	title = {Nature of {Local} {Symmetry} {Violations} of {Ions} in the {Magnetic} {Subsystem} of {Magnetoplumbite} {Crystal}, {According} to {Raman} {Scattering} {Spectroscopy} {Data}},
	volume = {82},
	issn = {1934-9432},
	url = {https://doi.org/10.3103/S1062873818030140},
	doi = {10.3103/S1062873818030140},
	abstract = {The structure of an M-type lead hexaferrite (magnetoplumbite) crystal is studied via the diffraction of synchrotron radiation. The crystal model contains two iron ions positions with dynamic disorder. The dynamics of the crystal lattice in the temperature range of 80 to 775 K is studied by Raman scattering. Particular attention is given to the discussing the nature of the local disorder of iron ions in the trigonal bipyramidal environment of oxygen ions.},
	language = {en},
	number = {3},
	urldate = {2023-11-11},
	journal = {Bulletin of the Russian Academy of Sciences: Physics},
	author = {Mikheykin, A. S. and Anokhin, A. S. and Torgashev, V. I. and Zhukova, E. S. and Gorshunov, B. P. and Prokhorov, A. S. and Bush, A. A.},
	month = mar,
	year = {2018},
	pages = {266--268},
}



@article{shirokov_piezoelectric_2018,
	title = {Piezoelectric coefficients of the barium-strontium titanate film on a (111)-oriented substrate},
	volume = {324},
	issn = {1757-899X},
	url = {https://dx.doi.org/10.1088/1757-899X/324/1/012006},
	doi = {10.1088/1757-899X/324/1/012006},
	abstract = {Within the framework of the phenomenological theory of phase transitions, we consider properties of the Ba0.8Sr0.2TiO3 (BST80) film grown on a (111)-oriented cubic substrate. The film was revealed to exhibit three ferroelectric phases with different orientations of spontaneous polarization. It is shown that some piezoelectric moduli should demonstrate anomalous behavior near the phase boundaries.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {IOP Conference Series: Materials Science and Engineering},
	author = {Shirokov, V. B. and Shakhovoy, R. A. and Pan’kin, A. V. and Kalinchuk, V. V.},
	month = mar,
	year = {2018},
	note = {Publisher: IOP Publishing},
	pages = {012006},
	file = {IOP Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\74MIZ5W7\\Shirokov и др. - 2018 - Piezoelectric coefficients of the barium-strontium.pdf:application/pdf},
}



@inproceedings{zhilin_growth_2018,
	address = {Cham},
	series = {Springer {Proceedings} in {Physics}},
	title = {Growth and {Study} of {Zinc} {Oxide} {Nanorods} {Arrays} on {Piezoelectric} {Substrates}},
	isbn = {978-3-319-78919-4},
	doi = {10.1007/978-3-319-78919-4_2},
	abstract = {Our studies have shown the possibility of using the thermal synthesisSynthesismethod from Zn vapors to obtain ZnO nanorodsZnO nanorods (ZnO NRs)arrays as a sensitive element for UV radiation SAW sensors. The piezoelectricPiezoelectricproperties of the LiNbO3 substrate typically degrade upon nanorods growth at elevated temperature. This limitation is solved by using additional annealing of prepared structureStructureat 550 °C in an oxygen atmosphere. The obtained ZnO NRs were investigated by scanning electron microscopy and photoluminescence.},
	language = {en},
	booktitle = {Advanced {Materials}},
	publisher = {Springer International Publishing},
	author = {Zhilin, D. A. and Karapetyan, G. Y. and Kutepov, M. E. and Minasyan, T. A. and Yatsenko, V. I. and Kaidashev, E. M.},
	editor = {Parinov, Ivan A. and Chang, Shun-Hsyung and Gupta, Vijay K.},
	year = {2018},
	keywords = {Carbothermal Method, LiNbO3 Substrate, structureStructure, synthesisSynthesis, Zinc Oxide Nanorod Arrays},
	pages = {25--31},
}



@article{kulbakov_situ_2018,
	title = {In {Situ} {Investigation} of {Non}-{Isothermal} {Decomposition} of {Pt} {Acetylacetonate} as {One}-{Step} {Size}-{Controlled} {Synthesis} of {Pt} {Nanoparticles}},
	volume = {215},
	copyright = {© 2018 WILEY-VCH Verlag GmbH \& Co. KGaA, Weinheim},
	issn = {1862-6319},
	url = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssa.201800488},
	doi = {10.1002/pssa.201800488},
	abstract = {Interest in the development of state-of-the-art methods for synthesis of Pt nanoparticles is dictated by both unique properties of platinum itself and the wide range of platinum nanoparticles applications. Platinum acetylacetonate and platinum nanoparticles produced by the thermal decomposition of Pt(acac)2 are studied via in situ X-ray diffraction and Raman spectroscopy, thermal gravimetry, scanning (SEM), and transmission electronic microscopy (TEM). The experiments are made at heating rates of 1 and 5 K min−1. A comparative analysis of SEM, TEM, and XRD data highlights the formation of coarse Pt particles with sizes of ≈60–160 nm, which are composed of nanoparticles with dimensions of 1.9 and 4.1 nm for 1 K min−1- and 5 K min−1-heating rates, respectively. The desirable average size of nanoparticles upon their synthesis can thus be achieved by a simple tuning of the heating rate of acetylacetate thermal decomposition. The present results open up the possibility to use a trivial non-isothermal thermal decomposition method in the synthesis of both supported and unsupported nanoparticles of predetermined size for other chemical elements such as Pd, Ni, Co, etc. from their acetylacetonates.},
	language = {en},
	number = {23},
	urldate = {2023-11-11},
	journal = {physica status solidi (a)},
	author = {Kulbakov, Anton A. and Allix, Mathieu and Rakhmatullin, Aydar and Mikheykin, Alexey S. and Popov, Yuri V. and Smirnova, Nina V. and Maslova, Olga and Leontyev, Igor N.},
	year = {2018},
	note = {\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssa.201800488},
	keywords = {in situ characterizations, platinum acetylacetonate, Pt nanoparticles, thermal decomposition},
	pages = {1800488},
}



@article{novikova_influence_2018,
	title = {Influence of {Carbon} {Support} on {Catalytic} {Layer} {Performance} of {Proton} {Exchange} {Membrane} {Fuel} {Cells}},
	volume = {9},
	issn = {1868-5994},
	url = {https://doi.org/10.1007/s12678-017-0416-4},
	doi = {10.1007/s12678-017-0416-4},
	abstract = {Pt-based catalysts supported onto various carbon nanotubes (CNTs) and carbon black Vulcan XC-72 have been studied in this work. The samples have been prepared via electrochemical dispersion technique. The carbon nanotubes exhibit the mesoporous morphology with the pore size of 5—30 nm, while Vulcan XC-72 support exhibits a microporous structure. The agglomeration of Pt particles (5—7 nm) is found to be more extended at the carbon nanotubes compared to the carbon black. The examination of the synthesized catalysts in a catalytic membrane electrode assembly layer reveals that CNTs favor a power density higher than in the carbon black support owing to a more suitable porous structure of the catalyst layer. Moreover, the maximum characteristics of membrane electrode assembly are obtained for few-walled carbon nanotubes with a broad carbon having size distribution.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Electrocatalysis},
	author = {Novikova, Ksenia and Kuriganova, Alexandra and Leontyev, Igor and Gerasimova, Ekaterina and Maslova, Olga and Rakhmatullin, Aydar and Smirnova, Nina and Dobrovolsky, Yuri},
	month = jan,
	year = {2018},
	keywords = {Carbon nanotubes, Carbon support, Catalytic layer structure, PEM fuel cell, Pt/C},
	pages = {22--30},
}



@article{leontyev_evaluation_2018,
	title = {On the {Evaluation} of the {Average} {Crystalline} {Size} and {Surface} {Area} of {Platinum} {Catalyst} {Nanoparticles}},
	volume = {255},
	copyright = {© 2018 WILEY-VCH Verlag GmbH \& Co. KGaA, Weinheim},
	issn = {1521-3951},
	url = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201800240},
	doi = {10.1002/pssb.201800240},
	abstract = {In the present work, the effect of grain size distribution on the diffraction profile shape is inspected via analysis of the mutual ratio of Lorentz and Gauss components in pseudo-Voigt function which is used for simulating X-ray profiles of nanoparticles. As established from the plotted dependences, the error in the average Pt nanoparticles size determination reaches 56\% and the discrepancy between calculated Pt nanoparticle surface areas attains 60\%. Furthermore, the determination error becomes greater with increasing the Lorentz contribution to pseudo-Voigt function, or, in fact, with enlarging particle size distribution. The empirically found electrochemical surface area of Pt/C electrocatalyst is compared with that evaluated from XRD data using the Scherrer formula and particle size distribution data analysis.},
	language = {en},
	number = {10},
	urldate = {2023-11-11},
	journal = {physica status solidi (b)},
	author = {Leontyev, Igor N. and Kuriganova, Alexandra B. and Allix, Mathieu and Rakhmatullin, Aydar and Timoshenko, Pavel E. and Maslova, Olga A. and Mikheykin, Alexey S. and Smirnova, Nina V.},
	year = {2018},
	note = {\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201800240},
	keywords = {X-ray diffraction, Pt/C, average nanoparticle size, catalysts, specific surface area},
	pages = {1800240},
}



@article{rochal_commensurability_2018,
	title = {Commensurability between protein nanotubes in contractile ejection nanomachines},
	volume = {10},
	issn = {2040-3372},
	url = {https://pubs.rsc.org/en/content/articlelanding/2018/nr/c7nr06940e},
	doi = {10.1039/C7NR06940E},
	abstract = {Contractile ejection nanomachines being sheath–tube assemblies create an opening in the cell membrane to translocate molecules or ions across it. Here, on the most structurally investigated examples of the bacteriophage T4 tail and pyocin R2, we show that the rearrangement of the sheath structure resulting in its contraction and twist occurs in such a way that the contracted sheath becomes commensurate with the inner tube. This fact dictates the previously unknown simple geometrical relationship between the nanotube symmetries. Using the Frank and van der Merwe classical theory of commensurability, we study an interaction between two protein nanotubes forming such nanomachines and obtain an expression for the corresponding energy, which depends on the tube structures and their mutual arrangement. The appearance of commensurability between the contracted sheath and the inner tube decreases both the interaction energy and the total energy of the system. It improves the nanomachine efficiency, since the energy gain obtained increases the torque of the inner tube piercing the cell membrane.},
	language = {en},
	number = {2},
	urldate = {2023-11-11},
	journal = {Nanoscale},
	author = {Rochal, Sergey B. and Roshal, Daria S. and Myasnikova, Anna E. and Lorman, Vladimir L.},
	month = jan,
	year = {2018},
	note = {Publisher: The Royal Society of Chemistry},
	pages = {758--764},
	file = {Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\J2A5BG4M\\Rochal и др. - 2018 - Commensurability between protein nanotubes in cont.pdf:application/pdf;Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\TABA9EAQ\\Rochal и др. - 2018 - Commensurability between protein nanotubes in cont.pdf:application/pdf},
}



@article{ulyankina_copper_2018,
	series = {Semiconductor materials for green energy and environmental applications},
	title = {Copper oxides for energy storage application: {Novel} pulse alternating current synthesis},
	volume = {73},
	issn = {1369-8001},
	shorttitle = {Copper oxides for energy storage application},
	url = {https://www.sciencedirect.com/science/article/pii/S1369800117313975},
	doi = {10.1016/j.mssp.2017.08.001},
	abstract = {Copper oxide powders (CuOx) were reported to be electrochemically obtained under pulse alternating current by a facile and inexpensive one-pot method. The effect of the synthesis conditions on the copper electrode oxidation rate and product morphology and composition was studied. The CuOx products were characterized by X-ray powder diffraction (XRD), Raman spectroscopy, X-ray absorption near-edge structure (XANES) spectroscopy, energy dispersive spectroscopy (EDS), scanning electron microscopy (SEM) and transmission electron microscopy (TEM). Depending on the synthesis conditions, the powders reveal different morphologies and composition, such as Cu2O octahedra, Cu2O decorated with CuO or Cu2O-CuO bilayered composite. Cyclic voltammetry and charge-discharge measurements were used to study the electrochemical energy conversion properties of the materials. The results of the electrocatalytic study indicate that the powder with Cu2O-CuO bilayered polyhedra is suitable for use in methanol oxidation; and the powder with Cu2O octahedra has shown a good specific capacitance for supercapacitors.},
	urldate = {2023-11-11},
	journal = {Materials Science in Semiconductor Processing},
	author = {Ulyankina, A. and Leontyev, I. and Maslova, O. and Allix, M. and Rakhmatullin, A. and Nevzorova, N. and Valeev, R. and Yalovega, G. and Smirnova, N.},
	month = jan,
	year = {2018},
	pages = {111--116},
}



@article{levshov_photoluminescence_2017,
	title = {Photoluminescence from an individual double-walled carbon nanotube},
	volume = {96},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.96.195410},
	doi = {10.1103/PhysRevB.96.195410},
	abstract = {We report direct and unambiguous evidence of the existence of inner semiconducting tube (ISCT) photoluminescence (PL) from measurements performed on four individual freestanding index-identified double-walled carbon nanotubes (DWNTs). Based on thorough Rayleigh scattering, Raman scattering, and PL experiments, we are able to demonstrate that the ISCT PL is observed with a quantum yield estimated to be a few 10−6 independent of the semiconducting or metallic nature of the outer tube. This result is mainly attributed to ultrafast exciton transfer from the inner to outer tube. Furthermore, by carrying out PL excitation experiments on the (14,1)@(15,12) DWNT, we show that the ISCT PL can be detected through the optical excitation of the outer tube, indicating that the exciton transfer can also occur in the opposite way.},
	number = {19},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Levshov, Dmitry I. and Parret, Romain and Tran, Huy-Nam and Michel, Thierry and Cao, Thi Thanh and Nguyen, Van Chuc and Arenal, Raul and Popov, Valentin N. and Rochal, Sergei B. and Sauvajol, Jean-Louis and Zahab, Ahmed-Azmi and Paillet, Matthieu},
	month = nov,
	year = {2017},
	note = {Publisher: American Physical Society},
	pages = {195410},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\6UGH2Z3Z\\Levshov и др. - 2017 - Photoluminescence from an individual double-walled.pdf:application/pdf;APS Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\4XVAB652\\PhysRevB.96.html:text/html},
}



@article{motovilov_observation_2017,
	title = {Observation of dielectric universalities in albumin, cytochrome {C} and {Shewanella} oneidensis {MR}-1 extracellular matrix},
	volume = {7},
	copyright = {2017 The Author(s)},
	issn = {2045-2322},
	url = {https://www.nature.com/articles/s41598-017-15693-y},
	doi = {10.1038/s41598-017-15693-y},
	abstract = {The electrodynamics of metals is well understood within the Drude conductivity model; properties of insulators and semiconductors are governed by a gap in the electronic states. But there is a great variety of disordered materials that do not fall in these categories and still respond to external field in an amazingly uniform manner. At radiofrequencies delocalized charges yield a frequency-independent conductivity σ1(ν) whose magnitude exponentially decreases while cooling. With increasing frequency, dispersionless conductivity starts to reveal a power-law dependence σ1(ν)∝νswith s {\textless} 1 caused by hopping charge carriers. At low temperatures, such Universal Dielectric Response can cross over to another universal regime with nearly constant loss ε″∝σ1/ν = const. The powerful research potential based on such universalities is widely used in condensed matter physics. Here we study the broad-band (1–1012 Hz) dielectric response of Shewanella oneidensis MR-1 extracellular matrix, cytochrome C and serum albumin. Applying concepts of condensed matter physics, we identify transport mechanisms and a number of energy, time, frequency, spatial and temperature scales in these biological objects, which can provide us with deeper insight into the protein dynamics.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Scientific Reports},
	author = {Motovilov, K. A. and Savinov, M. and Zhukova, E. S. and Pronin, A. A. and Gagkaeva, Z. V. and Grinenko, V. and Sidoruk, K. V. and Voeikova, T. A. and Barzilovich, P. Yu and Grebenko, A. K. and Lisovskii, S. V. and Torgashev, V. I. and Bednyakov, P. and Pokorný, J. and Dressel, M. and Gorshunov, B. P.},
	month = nov,
	year = {2017},
	note = {Number: 1
Publisher: Nature Publishing Group},
	keywords = {Biomaterials – proteins, Polymers},
	pages = {15731},
	file = {Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\4QFUHD76\\Motovilov и др. - 2017 - Observation of dielectric universalities in albumi.pdf:application/pdf},
}



@article{chalin_simple_2017,
	title = {Simple theory of low-temperature thermal conductivity in single- and double-walled carbon nanotubes},
	volume = {96},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.96.155413},
	doi = {10.1103/PhysRevB.96.155413},
	abstract = {Low-temperature phonon thermal conductance (PTC) of any 1D system increases proportionally to the temperature. However, here we show that in single- and double-walled carbon nanotubes (CNTs), starting from 3–6 K, the PTC increases faster than the linear function, since the low-frequency modes of dispersion curves, which do not tend to zero together with the wave vector, are excited. To develop the PTC theory, we combine the Landauer's ballistic approach with the simple continuous model proposed for the calculation of the low-frequency phonon spectra of both free nanotubes and those interacting with an environment. The approach obtained is valid not only for commensurate double-walled CNTs, but also for incommensurate ones. The temperature-dependent relation between the PTC of double-walled CNT and those of its constituent SWNTs is obtained and discussed. The low-temperature heat transfer in bulk materials originated from CNTs is also considered and the upper limit of thermal conductivity of such materials is determined. We argue that the ideal material consisting of CNTs can challenge diamond only when the mean length of its defect-free nanotubes reaches at least one hundred of micrometers.},
	number = {15},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Chalin, D. V. and Avramenko, M. V. and Rochal, S. B.},
	month = oct,
	year = {2017},
	note = {Publisher: American Physical Society},
	pages = {155413},
}



@article{konevtsova_quasicrystalline_2017,
	title = {Quasicrystalline and crystalline types of local protein order in capsids of small viruses},
	volume = {29},
	issn = {0953-8984},
	url = {https://dx.doi.org/10.1088/1361-648X/aa7211},
	doi = {10.1088/1361-648X/aa7211},
	abstract = {Like metal alloys and micellar systems in soft matter, the viral capsid structures can be of crystalline and quasicrystalline types. We reveal the local quasicrystalline order of proteins in small spherical viral capsids using their nets of dodecahedral type. We show that the structure of some of the viral shells is well described in terms of a chiral pentagonal tiling, whose nodes coincide with centers of mass of protein molecules. The chiral protein packing found in these capsids originates from the pentagonal Penrose tiling (PPT), due to a specific phason reconstruction needed to fit the protein order at the adjacent dodecahedron faces. Via examples of small spherical viral shells and geminate capsid of a Maize Streak virus, we discuss the benefits and shortcomings of the usage of a dodecahedral net in comparison to icosahedral one, which is commonly applied for the modeling of viral shells with a crystalline local order.},
	language = {en},
	number = {28},
	urldate = {2023-11-11},
	journal = {Journal of Physics: Condensed Matter},
	author = {Konevtsova, O. V. and Pimonov, V. V. and Lorman, V. L. and Rochal, S. B.},
	month = jun,
	year = {2017},
	note = {Publisher: IOP Publishing},
	pages = {284002},
}



@article{akbaeva_dielectric_2017,
	title = {Dielectric spectrum of multicomponent relaxor ceramics based on {PZT}},
	volume = {509},
	issn = {0015-0193},
	url = {https://doi.org/10.1080/00150193.2017.1290499},
	doi = {10.1080/00150193.2017.1290499},
	abstract = {The dielectric spectrum of multicomponent relaxor ceramic based on PZT was studied. In non-polarized sample, Debye-type dispersion region is found with the dispersion frequency of the order of 106 Hz. During polarization of the sample, this dispersion is suppressed. It is assumed that upon cooling from the paraphrase, without applied electric field, the relaxor ceramics transition to the dipole glass state occurs. Polarization converts it into a ferroelectric state, which is confirmed by characteristic piezoresonance response in the dielectric spectrum.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Ferroelectrics},
	author = {Akbaeva, G.M. and Sitalo, E.I. and Gavrilyachenko, V.G. and Panchenko, E.M.},
	month = mar,
	year = {2017},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/00150193.2017.1290499},
	keywords = {dielectric properties, Lead zirconate titanate, relaxor},
	pages = {10--13},
}



@article{rochal_static_2017,
	title = {Static and dynamic hidden symmetries of icosahedral viral capsids},
	volume = {9},
	issn = {2040-3372},
	url = {https://pubs.rsc.org/en/content/articlelanding/2017/nr/c7nr04020b},
	doi = {10.1039/C7NR04020B},
	abstract = {Viral shells self-assemble from identical proteins, which tend to form equivalent environments in the resulting assembly. However, in icosahedral capsids containing more than 60 proteins, they are enforced to occupy not only the symmetrically equivalent locations but also the quasi-equivalent ones. Due to this important fact, static and dynamic symmetries of viral shells can include additional hidden components. Here, developing the Caspar and Klug ideas concerning the quasi-equivalence of protein environments, we derive the simplest hexagonal tilings, that in principle could correspond to the local protein order in viral shells, and apply the resulting theory to nucleocytoplasmic large dsDNA viruses. In addition, analyzing the dynamic symmetry of the P22 viral shell, we demonstrate that the collective critical modes responsible for the protein reorganization during the procapsid maturation are approximately equivalent to the normal modes of the isotropic spherical membrane with O(3) symmetry. Furthermore, we establish the relationship between the dynamic symmetry of the P22 procapsid and the protein arrangement regularities that appear only in the mature capsid.},
	language = {en},
	number = {34},
	urldate = {2023-11-11},
	journal = {Nanoscale},
	author = {Rochal, Sergey B. and Konevtsova, Olga V. and Lorman, Vladimir L.},
	month = aug,
	year = {2017},
	note = {Publisher: The Royal Society of Chemistry},
	pages = {12449--12460},
	file = {Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\BKZZ384I\\Rochal и др. - 2017 - Static and dynamic hidden symmetries of icosahedra.pdf:application/pdf},
}



@article{shpanko_anticorrosion_2017,
	title = {Anticorrosion properties and physicochemical characteristics of organic films based on heterocyclic imidazole derivative},
	volume = {53},
	issn = {2070-206X},
	url = {https://doi.org/10.1134/S207020511702023X},
	doi = {10.1134/S207020511702023X},
	language = {en},
	number = {2},
	urldate = {2023-11-11},
	journal = {Protection of Metals and Physical Chemistry of Surfaces},
	author = {Shpan’ko, S. P. and Sidorenko, E. N. and Semenchev, A. F. and Lyanguzov, N. V. and Anisimova, V. A.},
	month = mar,
	year = {2017},
	pages = {335--342},
}



@article{tran_intrinsic_2017,
	title = {Intrinsic phonon properties of double-walled carbon nanotubes*},
	volume = {8},
	issn = {2043-6262},
	url = {https://dx.doi.org/10.1088/2043-6254/aa5957},
	doi = {10.1088/2043-6254/aa5957},
	abstract = {Double-walled carbon nanotubes (DWNT) are made of two concentric and weakly van der Waals coupled single-walled carbon nanotubes (SWNT). DWNTs are the simplest systems for studying the mechanical and electronic interactions between concentric carbon layers. In this paper we review recent results concerning the intrinsic features of phonons of DWNTs obtained from Raman experiments performed on index-identified DWNTs. The effect of the interlayer distance on the strength of the mechanical and electronic coupling between the layers, and thus on the frequencies of the Raman-active modes, namely the radial breathing-like modes (RBLMs) and G-modes, are evidenced and discussed.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Advances in Natural Sciences: Nanoscience and Nanotechnology},
	author = {Tran, H. N. and Levshov, D. I. and Nguyen, V. C. and Paillet, M. and Arenal, R. and Than, X. T. and Zahab, A. A. and Yuzyuk, Y. I. and Phan, N. M. and Sauvajol, J.-L. and Michel, T.},
	month = mar,
	year = {2017},
	note = {Publisher: IOP Publishing},
	pages = {015018},
	file = {IOP Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\5JJ685FU\\Tran и др. - 2017 - Intrinsic phonon properties of double-walled carbo.pdf:application/pdf},
}



@article{shirokov_tunable_2017,
	title = {Tunable pyroelectric properties of barium strontium titanate thin films},
	volume = {29},
	issn = {0953-8984},
	url = {https://dx.doi.org/10.1088/1361-648X/aa5711},
	doi = {10.1088/1361-648X/aa5711},
	abstract = {We studied the influence of the induced strain and applied electric field on the ground state of ferroelectric Ba0.7Sr0.3TiO3 thin films, deposited on the cubic (0 0 1) substrate. The dependence of the pyroelectric coefficient on the applied field is calculated for the different values of the induced strain. We found that tuning of the misfit strain in the film under the dielectric bolometer mode by the proper selection of substrate makes it possible to create the structures with very large values of the pyroelectric coefficient.},
	language = {en},
	number = {18},
	urldate = {2023-11-11},
	journal = {Journal of Physics: Condensed Matter},
	author = {Shirokov, V. B. and Razumnaya, A. G. and Yuzyuk, Yu I.},
	month = mar,
	year = {2017},
	note = {Publisher: IOP Publishing},
	pages = {185701},
}



@article{karapetyan_use_2017,
	title = {Use of multiple acoustic reflections to enhance {SAW} {UV} photo-detector sensitivity},
	volume = {26},
	issn = {0964-1726},
	url = {https://dx.doi.org/10.1088/1361-665X/26/3/035029},
	doi = {10.1088/1361-665X/26/3/035029},
	abstract = {A new approach to enhance the sensitivity of existing SAW UV-visible photo-detectors based on the monitoring of the multiple reflections of the acoustic waves in the Fourier transform of the frequency response (S21) is demonstrated. By using this concept, it is possible to monitor the UV-visible light in a wide intensity range from very high to ultralow. We present a strategy to obtain an ultrafast SAW UV photo-detector with millisecond response by tuning the deposition conditions of the ZnO film and using the multiple-reflections concept.},
	language = {en},
	number = {3},
	urldate = {2023-11-11},
	journal = {Smart Materials and Structures},
	author = {Karapetyan, G. Y. and Kaydashev, V. E. and Zhilin, D. A. and Minasyan, T. A. and Abdulvakhidov, K. G. and Kaidashev, E. M.},
	month = feb,
	year = {2017},
	note = {Publisher: IOP Publishing},
	pages = {035029},
}



@article{leontyev_thermal_2017,
	title = {Thermal expansion coefficient of carbon-supported {Pt} nanoparticles: {In}-situ {X}-ray diffraction study},
	volume = {254},
	copyright = {© 2017 WILEY-VCH Verlag GmbH \& Co. KGaA, Weinheim},
	issn = {1521-3951},
	shorttitle = {Thermal expansion coefficient of carbon-supported {Pt} nanoparticles},
	url = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201600695},
	doi = {10.1002/pssb.201600695},
	abstract = {The thermal expansion of carbon-supported Pt nanoparticles with different particle size has been studied in-situ via X-ray diffraction at temperatures from 100 to 300 K. The thermal expansion coefficient (TEC) of investigated Pt/C nanoparticles is always superior to that of bulk Pt. When the grain size D decreases from 11 to 3 nm, the TEC nonlinearly increases by about 1.66 × 10−6 K−1 which corresponds to a variation of ∼20\% from bulk Pt. The obtained experimental dependence of TEC for Pt/C nanoparticles has been interpreted using different theoretical approaches. A comparison of the considered models with the experimental data reveals the best agreement from the binding order–length–strength model with the size dependence of TEC experimentally found in carbon-supported Pt nanoparticles.},
	language = {en},
	number = {5},
	urldate = {2023-11-11},
	journal = {physica status solidi (b)},
	author = {Leontyev, I. N. and Kulbakov, A. A. and Allix, M. and Rakhmatullin, A. and Kuriganova, A. B. and Maslova, O. A. and Smirnova, N. V.},
	year = {2017},
	note = {\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201600695},
	keywords = {X-ray diffraction, platinum, nanoparticles, surface relaxation, thermal expansion},
	pages = {1600695},
}



@article{razumnaya_unexpectedly_2017,
	title = {Unexpectedly high {Curie} temperature in weakly strained ferroelectric film},
	volume = {254},
	copyright = {© 2016 WILEY-VCH Verlag GmbH \& Co. KGaA, Weinheim},
	issn = {1521-3951},
	url = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201600413},
	doi = {10.1002/pssb.201600413},
	abstract = {Polarized Raman spectra of the epitaxial Ba0.4Sr0.6TiO3 film grown on MgO substrate with thickness of 600 nm were studied in a broad temperature range of 80–600 K and the phase transition from paraelectric to tetragonal ferroelectric phase was observed at about 500 K. This critical temperature is substantially higher than that calculated from the lattice-mismatch strain theory. In addition, the predicted from the theory low-temperature orthorhombic and rhombohedral phases were not observed. We ascribe the strengthening of the tetragonal ferroelectric phase to the effect of the interface-induced build-in electric field resulted from the interface-accumulated charges.},
	language = {en},
	number = {4},
	urldate = {2023-11-11},
	journal = {physica status solidi (b)},
	author = {Razumnaya, Anna G. and Mikheykin, Alexey S. and Lukyanchuk, Igor A. and Shirokov, Vladimir B. and Golovko, Yury I. and Mukhortov, Vladimir M. and Marssi, Mimoun El and Yuzyuk, Yury I.},
	year = {2017},
	note = {\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201600413},
	keywords = {thin films, Raman spectroscopy, strain, BaTiO3, soft mode, Curie temperature, ferroelectric transition},
	pages = {1600413},
}



@article{levshov_interlayer_2017,
	title = {Interlayer {Interaction} {Effects} on the {G} {Modes} in {Double}-{Walled} {Carbon} {Nanotubes} {With} {Different} {Electronic} {Configurations}},
	volume = {254},
	copyright = {© 2017 WILEY-VCH Verlag GmbH \& Co. KGaA, Weinheim},
	issn = {1521-3951},
	url = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201700251},
	doi = {10.1002/pssb.201700251},
	abstract = {We present experimental measurements of the features of G band in individual index-identified free-standing double-walled carbon nanotubes. We examine Raman spectra of different electronic configurations of DWNTs, namely: SC@SC, SC@M, M@SC, M@M, and clearly establish that, as in SWNTs, the profile of LO G-mode of each layer is broad (narrow) when the layer is metallic (semiconducting). The dependence of G-modes on the diameter and inter-layer distance in several SC@SC, SC@M, M@SC, M@M index-identified DWNTs is reported. We find, that, independently of the metallic or semiconducting nature of the layers, the frequencies of LO and TO G-mode of the inner and outer layers shift significantly with respect to the frequencies of the same modes in the constituent SWNTs.},
	language = {en},
	number = {11},
	urldate = {2023-11-11},
	journal = {physica status solidi (b)},
	author = {Levshov, Dmitry I. and Tran, Huy-Nam and Michel, Thierry and Cao, Thi Thanh and Nguyen, Van Chuc and Arenal, Raul and Popov, Valentin N. and Sauvajol, Jean-Louis and Zahab, Ahmed-Azmi and Paillet, Matthieu},
	year = {2017},
	note = {\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201700251},
	keywords = {Raman spectroscopy, double-walled carbon nanotubes, interlayer interaction},
	pages = {1700251},
}



@article{kuriganova_one-step_2017,
	title = {One-step {Simultaneous} {Synthesis} of {Graphene} and {Pt} {Nanoparticles} under the {Action} of {Pulsed} {Alternating} {Current} and {Electrochemical} {Performance} of {Pt}/{Graphene} {Catalysts}},
	volume = {2},
	copyright = {© 2017 Wiley-VCH Verlag GmbH \& Co. KGaA, Weinheim},
	issn = {2365-6549},
	url = {https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201701186},
	doi = {10.1002/slct.201701186},
	abstract = {Pt/graphene electrocatalyst for fuel elements has been obtained via the simultaneously electrochemical dispersion of Pt foil and expanded graphite by applying the alternating current. Raman spectroscopy and transmission electron microscopy (TEM) have revealed multilayered structure of graphene (3-5 layers) with linear defects of graphene sheets near 1 μm. The microstructural characteristics and catalytic activity of synthesized Pt/graphene catalyst have been compared with those of Pt/Vulcan catalyst prepared under the same conditions. Pt nanoparticles of Pt/Graphene catalyst exhibit smaller average dimensions and narrower particle size distribution. It follows from the electrochemical study that the electrochemical surface area of Pt/graphene catalyst is 2.5 times higher than for Pt/Vulcan. Besides this, the activity in the electrooxidation of methanol and the stability of Pt/graphene catalyst are found to be superior to the analogous parameters of Pt/Vulcan specimen.},
	language = {en},
	number = {24},
	urldate = {2023-11-11},
	journal = {ChemistrySelect},
	author = {Kuriganova, Alexandra B. and Leontyev, Igor N. and Avramenko, Marina V. and Popov, Yuri and Maslova, Olga A. and Koval, Olga Yu. and Smirnova, Nina V.},
	year = {2017},
	note = {\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/slct.201701186},
	keywords = {electrochemical dispersion, fuel cell, platinum, Graphene, Pt/graphene catalysts},
	pages = {6979--6983},
}



@article{__2017,
	title = {Формирование магнитных никелевых наночастиц и изменения матрицы фталоцианина никеля при допировании натрием},
	volume = {87},
	issn = {0044-4642},
	url = {http://journals.ioffe.ru/articles/44998},
	doi = {10.21883/JTF.2017.10.44998.2149},
	language = {ru},
	number = {10},
	urldate = {2023-11-11},
	journal = {Журнал технической физики},
	author = {Колпачева, Н.А. and Авраменко, М.В. and Авакян, Л.А. and Зубавичус, Я.В. and Мирзаханян, А.А. and Манукян, А.С. and Шароян, Э.Г. and Бугаев, Л.А.},
	year = {2017},
	pages = {1532},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\EXHSE7C9\\Колпачева и др. - 2017 - Формирование магнитных никелевых наночастиц и изме.pdf:application/pdf},
}



@article{__2017-1,
	title = {Экспериментальное исследование динамики решетки индивидуальных полупроводниковых двустенных углеродных нанотрубок: тангенциальные {G}-моды},
	volume = {59},
	issn = {0367-3294},
	shorttitle = {Экспериментальное исследование динамики решетки индивидуальных полупроводниковых двустенных углеродных нанотрубок},
	url = {https://journals.ioffe.ru/articles/44057},
	doi = {10.21883/FTT.2017.02.44057.274},
	abstract = {Проведены исследования тангенциальных G-мод индивидуальных полупроводниковых двустенных углеродных нанотрубок методом резонансной спектроскопии комбинационного рассеяния света в широком диапазоне длин волн лазерного возбуждения. Индивидуальные подвешенные нанотрубки синтезированы методом химического осаждения из парогазовой фазы. Индексы хиральности (n,m) нанотрубок определялись методами электронной дифракции и просвечивающей электронной микроскопии высокого разрешения. В спектрах комбинационного рассеяния двустенных нанотрубок наблюдается существенный сдвиг тангенциальных мод в сравнении с аналогичными модами одностенных нанотрубок. Показано, что величина сдвига зависит от межслойного расстояния и от величины ван-дер-ваальсова взаимодействия между слоями двустенной нанотрубки. Исследование выполнено за счет гранта Российского фонда фундаментальных исследований (проект N 15-02-08340). DOI: 10.21883/FTT.2017.02.44057.274},
	language = {ru},
	number = {2},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Левшов, Д.И. and Tran, H.N. and Слабодян, Ю.С. and Осадчий, А.В. and Рошаль, С.Б. and Юзюк, Ю.И.},
	year = {2017},
	pages = {328},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\CPU38V3F\\Левшов и др. - 2017 - Экспериментальное исследование динамики решетки ин.pdf:application/pdf},
}



@article{ulyankina_electrochemical_2017,
	title = {Electrochemical {Synthesis} and {Photocatalytic} {Activity} of {Differently} {Shaped} {CuOx} {Particles}},
	volume = {13},
	issn = {2297-3400},
	url = {https://www.scientific.net/NHC.13.330},
	doi = {10.4028/www.scientific.net/NHC.13.330},
	abstract = {CuOx powders with diff erently shaped particles were firstly prepared via an electrochemical method by oxidation and dispersion of copper electrodes in an electrolyte solution under pulse alternating current (PAC). By means of X-ray diffraction (XRD) and scanning electron microscopy (SEM) the current density is found to have an influence on the morphology and composition of CuOx particles. Photocatalytic efficiency of CuOx towards methyl orange (MO) degradation under visible light was investigated. The prepared polyhedral particles show the best photocatalytic activity of 81 \% towards MO comparing to octahedral and spherical particles with 70 and 61 \%, respectively.},
	language = {en},
	urldate = {2023-11-11},
	journal = {Nano Hybrids and Composites},
	author = {Ulyankina, Anna and Leontyev, Igor and Smirnova, Nina V.},
	year = {2017},
	note = {Publisher: Trans Tech Publications Ltd},
	pages = {330--333},
}



@article{__2017-2,
	title = {Особенности тангенциальных мод в спектрах комбинационного рассеяния света одностенных полупроводниковых углеродных нанотрубок большого диаметра},
	volume = {59},
	issn = {0367-3294},
	url = {https://journals.ioffe.ru/articles/44173},
	doi = {10.21883/FTT.2017.03.44173.137},
	abstract = {Методом резонансной спектроскопии комбинационного рассеяния света в широком диапазоне длин волн лазерного возбуждения исследована динамика решетки и оптические свойства индивидуальных полупроводниковых одностенных углеродных нанотрубок с диаметрами более 2.0 nm. Индивидуальные подвешенные нанотрубки синтезированы методом химического осаждения из парогазовой фазы. Индексы хиральности (n,m) нанотрубок определялись методом электронной дифракции. Обнаружена зависимость отношения абсолютных интенсивностей поперечной и продольной оптических тангенциальных мод как от энергии возбуждения, так и от структурных параметров нанотрубок (диаметра и хирального угла). Наблюдаемые зависимости отличаются от спектральных данных, полученных ранее для индивидуальных полупроводниковых структурно идентифицированных нанотрубок с диаметрами менее 1.1 nm. Работа выполнена за счет гранта Российского научного фонда (проект N 15-12-10004). DOI: 10.21883/FTT.2017.03.44173.137},
	language = {ru},
	number = {3},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Левшов, Д.И. and Слабодян, Ю.С. and Тонких, А.А. and Michel, T. and Рошаль, С.Б. and Юзюк, Ю.И.},
	year = {2017},
	pages = {575},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\RFCMW9MW\\Левшов и др. - 2017 - Особенности тангенциальных мод в спектрах комбинац.pdf:application/pdf},
}



@article{karapetyan_gya_investigation_2016,
	title = {Investigation of the {Wireless} {Reading} from {Signal} {Passive} {SAW} {Sensors} with {Reflective} {Interdigital} {Transducers}},
	url = {https://elibrary.ru/item.asp?id=43958874},
	language = {en},
	urldate = {2023-11-11},
	author = {Karapetyan G.ya. and Dneprovsky, V. G. and Kaidashev, E. M.},
	year = {2016},
	note = {Publisher: Южный федеральный университет},
}



@article{nikolaev_design_2016,
	title = {Design of {Construction} {Elements} for {Piezoelectric} {Resonators} and {Chemisensors} {Based} on {Zinc} {Oxide} {Nanorods}},
	url = {https://elibrary.ru/item.asp?id=44011645},
	language = {en},
	urldate = {2023-11-11},
	author = {Nikolaev, A. L. and Kazmina, M. A. and Minasyan, T. A. and Kaidashev, V. E. and Karapetyan G.ya. and Kaidashev, E. M.},
	year = {2016},
	note = {Publisher: Южный федеральный университет},
}



@article{lerer_refractive_2016,
	title = {Refractive {Properties} of {Nanorod}-{Type} {2D} {Photonic} {Crystals}},
	url = {https://elibrary.ru/item.asp?id=43962934},
	language = {en},
	urldate = {2023-11-11},
	author = {Lerer, A. M. and Timoshenko, P. E. and Golovacheva, E. V. and Kaidashev, E. M.},
	year = {2016},
	note = {Publisher: Южный федеральный университет},
}



@patent{___ru__nodate,
	title = {Способ измерения физических величин с помощью датчиков на поверхностных акустических волнах},
	url = {https://findpatent.ru/patent/262/2629892.html},
	number = {RU 2629892},
	author = {{Минасян Тигран Арменович (RU)} and {Кайдашев Евгений Михайлович (RU)} and {Кайдашев Владимир Евгеньевич (RU)} and {Карапетьян Геворк Яковлевич (RU)}},
}



@article{levshov_accurate_2017,
	title = {Accurate determination of the chiral indices of individual carbon nanotubes by combining electron diffraction and {Resonant} {Raman} spectroscopy},
	volume = {114},
	issn = {0008-6223},
	url = {https://www.sciencedirect.com/science/article/pii/S0008622316310570},
	doi = {10.1016/j.carbon.2016.11.076},
	abstract = {The experimental approach combining high resolution transmission electron microscopy (HRTEM), electron diffraction (ED) and resonant Raman spectroscopy (RRS) on the same free-standing individual carbon nanotubes (CNT) is the most efficient method to determine unambiguously the intrinsic features of the Raman-active phonons. In this paper, we review the main results obtained by the approach regarding the intrinsic features of the phonons of single-walled (SWNT) and double-walled carbon nanotubes (DWNT). First, we detail the different methods to identify the structure of SWNTs and DWNTs from the analysis of their electron diffraction patterns (EDP). In the following, we remind the principal features of the Raman response of SWNTs, unambiguously index-identified by ED. A special attention is devoted to the effect of the inter-layer interaction on the frequencies of the Raman-active phonons in index-identified DWNTs. The information obtained on index-identified SWNT and DWNT allows us to propose Raman criteria, which help identifying CNT when the ED fails to propose a single assignment. The efficiency of the Raman criteria as the complement to the ED information for the index-assignment of a few SWNTs and DWNTs is shown. The same approach to index-assign a triple-walled carbon nanotube (TWNT), by combining ED and RRS information, is reported.},
	urldate = {2023-11-11},
	journal = {Carbon},
	author = {Levshov, D. I. and Tran, H. N. and Paillet, M. and Arenal, R. and Than, X. T. and Zahab, A. A. and Yuzyuk, Y. I. and Sauvajol, J. -L. and Michel, T.},
	month = apr,
	year = {2017},
	pages = {141--159},
	file = {Принятая версия:C\:\\Users\\aleks\\Zotero\\storage\\2BU26V7I\\Levshov и др. - 2017 - Accurate determination of the chiral indices of in.pdf:application/pdf;Принятая версия:C\:\\Users\\aleks\\Zotero\\storage\\75XGRBXA\\Levshov и др. - 2017 - Accurate determination of the chiral indices of in.pdf:application/pdf},
}



@article{zhukova_crucial_2016,
	title = {Crucial influence of crystal site disorder on dynamical spectral response in artificial magnetoplumbites},
	volume = {62},
	issn = {1293-2558},
	url = {https://www.sciencedirect.com/science/article/pii/S1293255816305465},
	doi = {10.1016/j.solidstatesciences.2016.10.012},
	abstract = {High quality PbFe12O19 single crystals were grown by a solution-melt crystallization technique and characterized by synchrotron radiation diffraction structural studies, Mössbauer, Raman and infrared spectral measurements. In the terahertz and sub-terahertz range two absorption bands are observed, which are associated with the dynamics of structurally disordered lead and iron ions. We develop a structural model that comprises Fe2+ ions at the (1/2 × 4e) (0, 0, z) position with bipyramidal oxygen environment, and Pb ions at the (24l) (x, y, z) position with generic strongly distorted 12 vertex polyhedron of oxygen. The atomic displacement ellipsoids of the oxygen surrounding the lead ion are stretched towards the Pb ion within the plane perpendicular to the hexagonal axis. The suggested model is in full agreement with the local symmetry of the Fe2 and Pb ions and with the chemical composition of the sample determined by X-ray analysis.},
	urldate = {2023-11-11},
	journal = {Solid State Sciences},
	author = {Zhukova, E. S. and Mikheykin, A. S. and Torgashev, V. I. and Bush, A. A. and Yuzyuk, Yu. I. and Sashin, A. E. and Prokhorov, A. S. and Dressel, M. and Gorshunov, B. P.},
	month = dec,
	year = {2016},
	keywords = {X-ray diffraction, Hexaferrites, Magnetoplumbite, Single crystal, Terahertz-infrared spectroscopy},
	pages = {13--21},
}



@article{roshal_assembly_2016,
	title = {Assembly of the most topologically regular two-dimensional micro and nanocrystals with spherical, conical, and tubular shapes},
	volume = {94},
	url = {https://link.aps.org/doi/10.1103/PhysRevE.94.052605},
	doi = {10.1103/PhysRevE.94.052605},
	abstract = {We consider how to control the extension of curvature-induced defects in the hexagonal order covering different curved surfaces. In these frames we propose a physical mechanism for improving structures of two-dimensional spherical colloidal crystals (SCCs). For any SCC comprising of about 300 or less particles the mechanism transforms all extended topological defects (ETDs) in the hexagonal order into the point disclinations. Perfecting the structure is carried out by successive cycles of the particle implantation and subsequent relaxation of the crystal. The mechanism is potentially suitable for obtaining colloidosomes with better selective permeability. Our approach enables modeling the most topologically regular tubular and conical two-dimensional nanocrystals including various possible polymorphic forms of the HIV viral capsid. Different HIV-like shells with an arbitrary number of structural units (SUs) and desired geometrical parameters are easily formed. Faceting of the obtained structures is performed by minimizing the suggested elastic energy.},
	number = {5},
	urldate = {2023-11-11},
	journal = {Physical Review E},
	author = {Roshal, D. S. and Konevtsova, O. V. and Myasnikova, A. E. and Rochal, S. B.},
	month = nov,
	year = {2016},
	note = {Publisher: American Physical Society},
	pages = {052605},
}



@article{tonkikh_optical_2016,
	title = {Optical properties and charge transfer effects in single-walled carbon nanotubes filled with functionalized adamantane molecules},
	volume = {109},
	issn = {0008-6223},
	url = {https://www.sciencedirect.com/science/article/pii/S0008622316306261},
	doi = {10.1016/j.carbon.2016.07.053},
	abstract = {The filling of single-walled carbon nanotube films with 1-adamantanemethanol and 1-bromoadamantane molecules was carried out by a gas-phase procedure. Optical absorption and Raman spectroscopies revealed the effects of charge transfer for samples treated with 1-bromoadamantane. Using density functional simulations we show that the charge transfer takes place when bromine is detached from the carbon cage and accepts electrons as free-standing atoms or as polybromide structures. Transmission electron microscope images confirm the presence of individual bromine atoms inside carbon nanotubes, treated with 1-bromoadamantane molecules. The observed charge transfer is, therefore, a marker of the dehalogenization reaction, a critical step in the synthesis process of narrow 1D sp3 nanostructures.},
	urldate = {2023-11-11},
	journal = {Carbon},
	author = {Tonkikh, A. A. and Rybkovskiy, D. V. and Orekhov, A. S. and Chernov, A. I. and Khomich, A. A. and Ewels, C. P. and Kauppinen, E. I. and Rochal, S. B. and Chuvilin, A. L. and Obraztsova, E. D.},
	month = nov,
	year = {2016},
	pages = {87--97},
}



@article{andronikova_pre-transitional_2016,
	title = {Pre-transitional evolution of central peaks and transverse acoustic phonon branch in single crystal lead zirconate titanate with {Ti} concentration 0.7\%},
	volume = {769},
	issn = {1742-6596},
	url = {https://dx.doi.org/10.1088/1742-6596/769/1/012070},
	doi = {10.1088/1742-6596/769/1/012070},
	abstract = {Inelastic X-ray scattering measurements have been done to study the lattice dynamics in lead zirconate titanate solid solution with 0.7\% of PbTiO3. The temperature evolution of central peak and low-energy transverse phonon branches has been traced. Temperature dependent in-plane transverse polarized acoustic phonon branch in {\textless}1 1 0{\textgreater} direction has been revealed. The central peaks of two types have been found. The central peak at small wave vectors can be attributed to the relaxational-type soft ferroelectric mode, while the latter at Q = (1.5 -0.5 0) could be linked to the formation of M-superstructure in the intermediate ferroelectric phase.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Journal of Physics: Conference Series},
	author = {Andronikova, D. A. and Bronwald, I. A. and Burkovsky, R. G. and Leontiev, I. N. and Leontiev, N. G. and Bosak, A. A. and Filimonov, A. V. and Vakhrushev, S. B.},
	month = nov,
	year = {2016},
	note = {Publisher: IOP Publishing},
	pages = {012070},
	file = {IOP Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\77XA23P4\\Andronikova и др. - 2016 - Pre-transitional evolution of central peaks and tr.pdf:application/pdf},
}



@article{rochal_hidden_2016,
	title = {Hidden symmetry of small spherical viruses and organization principles in “anomalous” and double-shelled capsid nanoassemblies},
	volume = {8},
	issn = {2040-3372},
	url = {https://pubs.rsc.org/en/content/articlelanding/2016/nr/c6nr04930c},
	doi = {10.1039/C6NR04930C},
	abstract = {We propose the principles of structural organization in spherical nanoassemblies with icosahedral symmetry constituted by asymmetric protein molecules. The approach modifies the paradigmatic geometrical Caspar and Klug (CK) model of icosahedral viral capsids and demonstrates the common origin of both the “anomalous” and conventional capsid structures. In contrast to all previous models of “anomalous” viral capsids the proposed modified model conserves the basic structural principles of the CK approach and reveals the common hidden symmetry underlying all small viral shells. We demonstrate the common genesis of the “anomalous” and conventional capsids and explain their structures in the same frame. The organization principles are derived from the group theory analysis of the positional order on the spherical surface. The relationship between the modified CK geometrical model and the theory of two-dimensional spherical crystallization is discussed. We also apply the proposed approach to complex double-shelled capsids and capsids with protruding knob-like proteins. The introduced notion of commensurability for the concentric nanoshells explains the peculiarities of their organization and helps to predict analogous, but yet undiscovered, double-shelled viral capsid nanostructures.},
	language = {en},
	number = {38},
	urldate = {2023-11-11},
	journal = {Nanoscale},
	author = {Rochal, S. B. and Konevtsova, O. V. and Myasnikova, A. E. and Lorman, V. L.},
	month = sep,
	year = {2016},
	note = {Publisher: The Royal Society of Chemistry},
	pages = {16976--16988},
}



@article{anokhin_phase_2016,
	title = {Phase transitions in barium–strontium titanate films on {MgO} substrates with various orientations},
	volume = {58},
	issn = {1090-6460},
	url = {https://doi.org/10.1134/S1063783416100048},
	doi = {10.1134/S1063783416100048},
	abstract = {A comparative study of the lattice dynamic upon phase transitions in a polycrystalline Ba0.8Sr0.2TiO3 (BST) film on a Pt substrate and in epitaxial BST films grown on various sections of an MgO substrate has been performed by Raman spectroscopy. It has been found that different sequences of phase transitions take place in these films. The BST/Pt films demonstrate the same sequence of phase transitions that is observed in the bulk ceramics. The hardening of a soft mode in BST/(001)MgO and BST/Pt films shows that the transition from the tetragonal ferroelectric phase to the paraelectric phase has features of the displacement-type phase transition and also the order–disorder phase transition. When approaching the ferroelectric transition temperature, the soft mode in the BST/(111)MgO film is softened, following the Cockran law, which indicates the displacement-type phase transition.},
	language = {en},
	number = {10},
	urldate = {2023-11-11},
	journal = {Physics of the Solid State},
	author = {Anokhin, A. S. and Razumnaya, A. G. and Yuzyuk, Yu. I. and Golovko, Yu. I. and Mukhortov, V. M.},
	month = oct,
	year = {2016},
	pages = {2027--2034},
}



@article{gorshunov_incipient_2016,
	title = {Incipient ferroelectricity of water molecules confined to nano-channels of beryl},
	volume = {7},
	copyright = {2016 The Author(s)},
	issn = {2041-1723},
	url = {https://www.nature.com/articles/ncomms12842},
	doi = {10.1038/ncomms12842},
	abstract = {Water is characterized by large molecular electric dipole moments and strong interactions between molecules; however, hydrogen bonds screen the dipole–dipole coupling and suppress the ferroelectric order. The situation changes drastically when water is confined: in this case ordering of the molecular dipoles has been predicted, but never unambiguously detected experimentally. In the present study we place separate H2O molecules in the structural channels of a beryl single crystal so that they are located far enough to prevent hydrogen bonding, but close enough to keep the dipole–dipole interaction, resulting in incipient ferroelectricity in the water molecular subsystem. We observe a ferroelectric soft mode that causes Curie–Weiss behaviour of the static permittivity, which saturates below 10 K due to quantum fluctuations. The ferroelectricity of water molecules may play a key role in the functioning of biological systems and find applications in fuel and memory cells, light emitters and other nanoscale electronic devices.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Nature Communications},
	author = {Gorshunov, B. P. and Torgashev, V. I. and Zhukova, E. S. and Thomas, V. G. and Belyanchikov, M. A. and Kadlec, C. and Kadlec, F. and Savinov, M. and Ostapchuk, T. and Petzelt, J. and Prokleška, J. and Tomas, P. V. and Pestrjakov, E. V. and Fursenko, D. A. and Shakurov, G. S. and Prokhorov, A. S. and Gorelik, V. S. and Kadyrov, L. S. and Uskov, V. V. and Kremer, R. K. and Dressel, M.},
	month = sep,
	year = {2016},
	note = {Number: 1
Publisher: Nature Publishing Group},
	keywords = {Ferroelectrics and multiferroics, Electronic devices, Electronic properties and materials},
	pages = {12842},
	file = {Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\QJNV8X4R\\Gorshunov и др. - 2016 - Incipient ferroelectricity of water molecules conf.pdf:application/pdf},
}



@article{lerer_dispersion_2016,
	title = {Dispersion characteristics of optical waveguides based on {ZnO} nanorods},
	volume = {61},
	issn = {1555-6557},
	url = {https://doi.org/10.1134/S1064226916060140},
	doi = {10.1134/S1064226916060140},
	abstract = {Using the method of separation of variables in the cylindrical coordinate system, the problem of propagation of electromagnetic waves in a 2D periodic lattice of ZnO nanwaveguides covered with a thin metal film is solved. Comparison of calculation results with results of simulation with the use of the COMSOL Multiphysics™ package based on the finite-element method is performed. The obtained results are used for forecasting the resonance wavelengths of a 2D periodic lattice of ZnO nanorods grown on a dielectric substrate.},
	language = {en},
	number = {6},
	urldate = {2023-11-11},
	journal = {Journal of Communications Technology and Electronics},
	author = {Lerer, A. M. and Timoshenko, P. E. and Chernikova, T. Yu.},
	month = jun,
	year = {2016},
	pages = {619--623},
}



@inproceedings{zhukova_terahertz_2016,
	title = {Terahertz dynamics of nanoconfined water molecules},
	url = {https://ieeexplore.ieee.org/document/7758778},
	doi = {10.1109/IRMMW-THz.2016.7758778},
	abstract = {We performed spectroscopic studies of water-containing beryl crystals. At terahertz frequencies, we observed a strongly temperature-dependent spectral feature, corresponding to a collective excitation caused by dipole-dipole interactions between separate H2O molecules. We associate the excitation with a soft mode signaling an incipient ferroelectric state within the water molecular subsystem. Single-particle excitations of nanocaged H2O molecules are also observed at terahertz and infrared frequencies; using DFT analysis, their origin is assigned to translational and librational vibrational states.},
	urldate = {2023-11-11},
	booktitle = {2016 41st {International} {Conference} on {Infrared}, {Millimeter}, and {Terahertz} waves ({IRMMW}-{THz})},
	author = {Zhukova, Elena S. and Belyanchikov, Mikhail A. and Torgashev, Victor I. and Thomas, Victor G. and Savinov, Maksim and Kadlec, Christelle and Kadlec, Filip and Prokhorov, Anatoly S. and Kadyrov, Lenar S. and Petzelt, Jan and Ostapchuk, Tatyana and Fursenko, Dmitry A. and Thomas, Pavel V. and Shakurov, Gilman S. and Dressel, Martin and Gorshunov, Boris P.},
	month = sep,
	year = {2016},
	note = {ISSN: 2162-2035},
	pages = {1--2},
}



@inproceedings{motovilov_issue_2016,
	title = {On the issue of universal dielectric responses in proteins},
	url = {https://ieeexplore.ieee.org/document/7758865},
	doi = {10.1109/IRMMW-THz.2016.7758865},
	abstract = {Ac conductivity and dielectric permittivity of bovine serum albumin, cytochrome c and extracellular matrix synthesized by electrogenic bacteria Shewanella oneidensis MR-1 are measured at frequencies 1-1012 Hz and temperatures 10-300 K. Two types of conductivity mechanisms are observed as well as nearly constant loss (NCL) phenomenon, universal dielectric response (UDR) and signatures of boson peak depending on the temperature and water/ion contents in the samples.},
	urldate = {2023-11-11},
	booktitle = {2016 41st {International} {Conference} on {Infrared}, {Millimeter}, and {Terahertz} waves ({IRMMW}-{THz})},
	author = {Motovilov, Konstantin A. and Pronin, Aleksei A. and Zhukova, Elena S. and Gagkaeva, Zarina V. and Torgashev, Victor I. and Savinov, Maxim and Grinenko, Vadim and Belyanchikov, Mikhail A. and Grebenko, Artem K. and Sidoruk, Konstantin V. and Dressel, Martin and Gorshunov, Boris P.},
	month = sep,
	year = {2016},
	note = {ISSN: 2162-2035},
	pages = {1--1},
}



@article{lerer_optical_2016,
	title = {Optical {Nanowaveguides} {Based} on {Zinc} {Oxide} {Plasmonic} {Materials}},
	volume = {741},
	issn = {1742-6596},
	url = {https://dx.doi.org/10.1088/1742-6596/741/1/012159},
	doi = {10.1088/1742-6596/741/1/012159},
	abstract = {The numerical study of nanowaveguides containing ZO, AZO, GZO and other materials are studied in infrared range. The dispersion relation for the waveguides contained an arbitrary number of layers are solved numerically. The integral-differential equations in vector form of the electromagnetic waves propagation in nanowaveguides containing a finite width plasmon films are calculated by the Galerkin’ method and the effective dielectric constants method. The opportunity of surface plasmon-polariton propagation with a large deceleration ratio are shown.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Journal of Physics: Conference Series},
	author = {Lerer, A. M. and Timoshenko, P. E. and Chernikova, T. Yu and Kaidashev, E. M. and Puzanov, A. S.},
	month = aug,
	year = {2016},
	note = {Publisher: IOP Publishing},
	pages = {012159},
	file = {IOP Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\V8WUEVR3\\Lerer и др. - 2016 - Optical Nanowaveguides Based on Zinc Oxide Plasmon.pdf:application/pdf},
}



@article{shirokov_phenomenological_2016,
	title = {Phenomenological theory of uniaxial relaxor ferroelectrics},
	volume = {28},
	issn = {0953-8984},
	url = {https://dx.doi.org/10.1088/0953-8984/28/39/395902},
	doi = {10.1088/0953-8984/28/39/395902},
	abstract = {A phenomenological thermodynamic theory of uniaxial relaxor strontium barium niobate is developed using the Landau–Devonshire approach with two order parameters. The fourth-order thermodynamic potential allowed to explain the shape of the polarization hysteresis loops experimentally observed at different temperatures. We show that the broad maximum of the dielectric permittivity is not related to the phase transition and arise due to the coupling between polarization and true order parameter which has antiferroelectric nature. We found that the phase transition temperature is much higher than the maximum of the dielectric permittivity and very likely corresponds to so-called Burn’s temperature. True order parameter has no simple relation with polar modes.},
	language = {en},
	number = {39},
	urldate = {2023-11-11},
	journal = {Journal of Physics: Condensed Matter},
	author = {Shirokov, V. B. and Pavlenko, A. V. and Yuzyuk, Yu I.},
	month = aug,
	year = {2016},
	note = {Publisher: IOP Publishing},
	pages = {395902},
}



@article{shirokov_physical_2016,
	title = {Physical states and properties of barium titanate films in a plane electric field},
	volume = {61},
	issn = {1090-6525},
	url = {https://doi.org/10.1134/S1063784216070240},
	doi = {10.1134/S1063784216070240},
	abstract = {The influence of a plane electric field on the phase states of barium titanate thin films under the conditions of forced deformation has been studied. The field dependence of a complete set of material constants has been taken in the region of the c-phase, where polarization losses are absent. The material constants are calculated using equations of the piezoelectric effect derived by linearizing the nonlinear equations of state from the phenomenological; theory for barium titanate. It has been shown that there is a critical value of the field at which the electromechanical coupling coefficient reaches a maximum.},
	language = {en},
	number = {7},
	urldate = {2023-11-11},
	journal = {Technical Physics},
	author = {Shirokov, V. B. and Kalinchuk, V. V. and Shakhovoi, R. A. and Yuzyuk, Yu. I.},
	month = jul,
	year = {2016},
	pages = {1073--1078},
}



@article{konevtsova_theory_2016,
	title = {Theory of morphological transformation of viral capsid shell during the maturation process in the {HK97} bacteriophage and similar viruses},
	volume = {93},
	url = {https://link.aps.org/doi/10.1103/PhysRevE.93.052412},
	doi = {10.1103/PhysRevE.93.052412},
	abstract = {We consider the symmetry and physical origin of collective displacement modes playing a crucial role in the morphological transformation during the maturation of the HK97 bacteriophage and similar viruses. It is shown that the experimentally observed hexamer deformation and pentamer twist in the HK97 procapsid correspond to the simplest irreducible shear strain mode of a spherical shell. We also show that the icosahedral faceting of the bacteriophage capsid shell is driven by the simplest irreducible radial displacement field. The shear field has the rotational icosahedral symmetry group I while the radial field has the full icosahedral symmetry Ih. This difference makes their actions independent. The radial field sign discriminates between the icosahedral and the dodecahedral shapes of the faceted capsid shell, thus making the approach relevant not only for the HK97-like viruses but also for the parvovirus family. In the frame of the Landau-Ginzburg formalism we propose a simple phenomenological model valid for the first reversible step of the HK97 maturation process. The calculated phase diagram illustrates the discontinuous character of the virus shape transformation. The characteristics of the virus shell faceting and expansion obtained in the in vitro and in vivo experiments are related to the decrease in the capsid shell thickness and to the increase of the internal capsid pressure.},
	number = {5},
	urldate = {2023-11-11},
	journal = {Physical Review E},
	author = {Konevtsova, O. V. and Lorman, V. L. and Rochal, S. B.},
	month = may,
	year = {2016},
	note = {Publisher: American Physical Society},
	pages = {052412},
	file = {Принятая версия:C\:\\Users\\aleks\\Zotero\\storage\\UA4NGX4T\\Konevtsova и др. - 2016 - Theory of morphological transformation of viral ca.pdf:application/pdf},
}



@article{talanov_phenomenological_2016,
	title = {Phenomenological thermodynamics and the structure formation mechanism of the {CuTi2S4} rhombohedral phase},
	volume = {18},
	issn = {1463-9084},
	url = {https://pubs.rsc.org/en/content/articlelanding/2016/cp/c6cp00387g},
	doi = {10.1039/C6CP00387G},
	abstract = {The theory of structural phase transition in CuTi2S4 is proposed. The symmetry of order parameters, thermodynamics and the mechanism of the atomic structure formation of the rhombohedral Cu–Ti–thiospinel have been studied. The critical order parameter inducing the phase transition has been found. Within the Landau theory of phase transitions, it is shown that the phase state may change from the high-symmetry cubic disordered Fdm phase to the low-symmetry ordered rhombohedral Rm phase as a result of phase transition of the first order close to the second order. It is shown that the rhombohedral structure of CuTi2S4 is formed as a result of the displacements of all types of atoms and the ordering of Cu-atoms (1 : 1 order type in tetrahedral spinel sites), Ti-atoms (1 : 1 : 6 order type in octahedral spinel sites), and S-atoms (1 : 1 : 3 : 3 order type). The Cu- and Ti-atoms form metal nanoclusters which are named a “bunch” of dimers. The “bunch” of dimers in CuTi2S4 is a new type of self-organization of atoms in frustrated spinel-like structures. It is shown that Ti-atoms also form other types of metal nanoclusters: trimers and tetrahedra.},
	language = {en},
	number = {15},
	urldate = {2023-11-11},
	journal = {Physical Chemistry Chemical Physics},
	author = {Talanov, Michail V. and Shirokov, Vladimir B. and Talanov, Valery M.},
	month = apr,
	year = {2016},
	note = {Publisher: The Royal Society of Chemistry},
	pages = {10600--10606},
	file = {Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\IESXZ2EA\\Talanov и др. - 2016 - Phenomenological thermodynamics and the structure .pdf:application/pdf},
}



@article{mirzakhanyan_characterization_2016,
	title = {Characterization of zinc and zinc cyanide nanoparticles in carbon matrices prepared by solid-phase pyrolysis of zinc-phthalocyanine},
	volume = {51},
	issn = {1934-9378},
	url = {https://doi.org/10.3103/S1068337216020134},
	doi = {10.3103/S1068337216020134},
	abstract = {Using solid-phase pyrolysis of Zn-phthalocyanine (ZnC32H16N8), we have prepared zinc and zinc cyanide nanoparticles in carbon matrices with a zinc concentration of 3 at \%. The structure and composition of samples were investigated by the methods of scanning electron microscopy, X-ray diffraction, and Raman spectroscopy. It is shown that at low pyrolysis temperature (700°C) only the Zn nanoparticles are formed, whereas at higher temperature (900°C) a certain amount of Zn(CN)2 nanoparticles are also synthesized. The mean diameter of nanoparticles is about 150 nm, and their size distribution has a logarithmically normal shape.},
	language = {en},
	number = {2},
	urldate = {2023-11-11},
	journal = {Journal of Contemporary Physics (Armenian Academy of Sciences)},
	author = {Mirzakhanyan, A. A. and Manukyan, A. S. and Gyulasaryan, H. T. and Ginoyan, A. K. and Nurijanyan, M. Kh. and Yuzyuk, Yu. I. and Kaniukov, E. Yu. and Sharoyan, E. G.},
	month = apr,
	year = {2016},
	keywords = {X-ray diffraction, Raman shift, SEM images, size distribution, solid-phase pyrolysis, zinc and zinc cyanide nanoparticles},
	pages = {191--195},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\MAWN25GC\\Mirzakhanyan и др. - 2016 - Characterization of zinc and zinc cyanide nanopart.pdf:application/pdf},
}



@article{bokova-sirosh_investigation_2016,
	title = {Investigation of defectiveness of multiwalled carbon nanotubes produced with {Fe}–{Co} catalysts of different composition},
	volume = {10},
	issn = {1934-2608, 1934-2608},
	url = {https://www.spiedigitallibrary.org/journals/journal-of-nanophotonics/volume-10/issue-1/012526/Investigation-of-defectiveness-of-multiwalled-carbon-nanotubes-produced-with-FeCo/10.1117/1.JNP.10.012526.full},
	doi = {10.1117/1.JNP.10.012526},
	abstract = {We have performed a study of CVD multiwalled carbon nanotubes (MWCNTs) produced with Fe–Co catalysts with a variable ratio of active metals. The Raman data were considered in combination with the temperature dependence of MWCNT conductivity. The data analysis is based on the point that the value of I2D/ID ratio correlates with the graphene fragment size. The fragments are considered as building blocks of MWCNTs. We showed that MWCNT defectiveness depends on the ratio of bimetallic active components in the Fe–Co catalyst. Thus, the ratio of I2D/ID increases and the D-mode intensity decreases while the Fe content in the catalyst increases. This also points to the reduction of defect number in the bigger graphene fragments. These results correlate with the data on conductivity temperature dependence. Namely, the increase of Fe content in the active component of the Fe–Co catalyst results in the increase of charge carrier concentration, which, in turn, indicates a decrease in MWCNT defectiveness.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Journal of Nanophotonics},
	author = {Bokova-Sirosh, Sofya N. and Kuznetsov, Vladimir L. and Romanenko, Anatoly I. and Kazakova, Mariya A. and Krasnikov, Dmitry V. and Tkachev, Evgeniy N. and Yuzyuk, Yuri I. and Obraztsova, Elena D.},
	month = mar,
	year = {2016},
	note = {Publisher: SPIE},
	pages = {012526},
}



@article{rochal_soft_2016,
	title = {Soft spherical nanostructures with a dodecagonal quasicrystal-like order},
	volume = {12},
	issn = {1744-6848},
	url = {https://pubs.rsc.org/en/content/articlelanding/2016/sm/c5sm02265g},
	doi = {10.1039/C5SM02265G},
	abstract = {We develop a theory which predicts curvature-related structural peculiarities of soft spherical nanostructures with a dodecagonal local arrangement of subunits. Spherical templates coated with a thin film of a soft quasicrystal (QC)-forming material constitute the most promising direction to realize these nanostructures. Disordered and perfect spherical nanostructures are simulated using two approaches. The first of them models a random QC-like spherical nanostructure with extended curvature-induced topological defects similar to scars in colloidal spherical crystals. The second approach is inspired by the physics of viral capsids. It deals with the most regular spherical nanostructures with a local QC-like order derived from three well-known planar dodecagonal tilings. We explain how the additional QC-like degrees of freedom assist the nanostructure stabilization and determine the point defect number and location without extended scar formation. Unusual for nanoassemblies snub cube geometry is shown to be the most energetically favorable global organization of these spherical QC nanostructures.},
	language = {en},
	number = {4},
	urldate = {2023-11-11},
	journal = {Soft Matter},
	author = {Rochal, S. B. and Konevtsova, O. V. and Shevchenko, I. A. and Lorman, V. L.},
	month = jan,
	year = {2016},
	note = {Publisher: The Royal Society of Chemistry},
	pages = {1238--1247},
}



@article{mukhortov_effect_2016,
	title = {Effect of growth mechanisms on the deformation of a unit cell and polarization reversal in barium–strontium titanate heterostructures on magnesium oxide},
	volume = {61},
	issn = {1090-6525},
	url = {https://doi.org/10.1134/S106378421601014X},
	doi = {10.1134/S106378421601014X},
	abstract = {The effect of a growth mechanism on the unit cell strain and the related change in the properties of single-crystal Ba0.8Sr0.2TiO3 films grown on MgO substrates according to the Frank–van der Merwe and Volmer–Weber growth mechanisms is studied. The unit cell strain is shown to depend substantially on the film thickness and the growth mechanism. It is found that the same film–substrate pair can be used to vary stresses in the film from two-dimensional tensile to compressive stresses due to a change in the growth mechanism and the film thickness.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Technical Physics},
	author = {Mukhortov, V. M. and Golovko, Yu. I. and Biryukov, S. V. and Anokhin, A. and Yuzyuk, Yu. I.},
	month = jan,
	year = {2016},
	keywords = {Strontium Titanate, Growth Mechanism, Paraelectric Phase, Remanent Polarization, Substrate Plane},
	pages = {91--96},
}



@article{roshal_relaxation_2016,
	title = {Relaxation of interstitials in spherical colloidal crystals},
	volume = {75},
	issn = {1386-9477},
	url = {https://www.sciencedirect.com/science/article/pii/S1386947715302174},
	doi = {10.1016/j.physe.2015.09.036},
	abstract = {Spherical colloidal crystals (CCs) self-assemble on the interface between two liquids. These 2D structures unconventionally combine local hexagonal order and spherical geometry. Nowadays CCs are actively studied by altering their structures. However, the statistical analysis of such experiments results is limited by uniqueness of self-assembled structures and their short lifetime. Here we perform numerical experiments to investigate pathways of CC structure relaxation after the intrusion of interstitial. The process is simulated in the frames of overdamped molecular dynamics method. The relaxation occurs due to interaction with extended topological defects (ETDs) mandatory induced in spherical CCs by their intrinsic Gaussian curvature. Types of relaxation pathways are classified and their probabilities are estimated in the low-temperature region. To analyze the structural changes during the relaxation we use a parent phase approach allowing us to describe the global organization of spherical order. This organization is preserved by only the most typical relaxation pathway resulting in filling one of vacancies integrated inside the ETD areas. In contrast with this pathway the other ones shift the ETDs centers and can strongly reconstruct the internal structure of ETDs. Temperature dependence of the relaxation processes and the mechanism of dislocation unbinding are discussed. Common peculiarities in relaxation of spherical structures and particular fragments of planar hexagonal lattice are found.},
	urldate = {2023-11-11},
	journal = {Physica E: Low-dimensional Systems and Nanostructures},
	author = {Roshal, D. S. and Myasnikova, A. E. and Rochal, S. B.},
	month = jan,
	year = {2016},
	keywords = {Topological defects, Self-assembly, Interstitial, Parent phase, Relaxation, Spherical colloidal crystals},
	pages = {295--301},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\BC5X78BR\\Roshal и др. - 2016 - Relaxation of interstitials in spherical colloidal.pdf:application/pdf},
}



@article{__2016,
	title = {Электрофизические свойства шестикомпонентного состава сегнетомягкой керамики на основе ЦТС},
	volume = {80},
	issn = {0367-6765},
	url = {https://elibrary.ru/item.asp?doi=10.7868/S0367676516090039},
	doi = {10.7868/S0367676516090039},
	abstract = {Изучены свойства шестикомпонентного состава сегнетомягкой керамики на основе ЦТС. Установлено, что этот состав проявляет свойства сегнетоэлектрика-релаксора. В сегнетоэлекрической фазе материала обнаружен фазовый переход между двумя ромбоэдрическими фазами R3c → R3m. Поляризация образцов постоянным электрическим полем при охлаждении через точку Кюри расширяет температурный интервал существования фазы R3m по сравнению с поляризацией при комнатной температуре.},
	language = {ru},
	number = {9},
	urldate = {2023-11-11},
	journal = {Известия Российской Академии Наук. Серия Физическая},
	author = {Акбаева, Г. М. and Гавриляченко, В. Г. and Захаров, Ю. Н. and Лутохин, А. Г.},
	year = {2016},
	pages = {1179--1182},
}



@article{levshov_study_2015,
	title = {Study of collective radial breathing-like modes in double-walled carbon nanotubes: combination of continuous two-dimensional membrane theory and {Raman} spectroscopy},
	volume = {10},
	issn = {1934-2608, 1934-2608},
	shorttitle = {Study of collective radial breathing-like modes in double-walled carbon nanotubes},
	url = {https://www.spiedigitallibrary.org/journals/journal-of-nanophotonics/volume-10/issue-1/012502/Study-of-collective-radial-breathing-like-modes-in-double-walled/10.1117/1.JNP.10.012502.full},
	doi = {10.1117/1.JNP.10.012502},
	abstract = {Radial breathing modes (RBMs) are widely used for the atomic structure characterization and index assignment of single-walled carbon nanotubes (SWNTs) from resonant Raman spectroscopy. However, for double-walled carbon nanotubes (DWNTs), the use of conventional ωRBM(d) formulas is complicated due to the van der Waals interaction between the layers, which strongly affects the frequencies of radial modes and leads to new collective vibrations. This paper presents an alternative way to theoretically study the collective radial breathing-like modes (RBLMs) of DWNTs and to account for interlayer interaction, namely the continuous two-dimensional membrane theory. We obtain an analytical ωRBLM(do,di) relation, being the equivalent of the conventional ωRBM(d) expressions, established for SWNTs. We compare our theoretical predictions with Raman data, measured on individual index-identified suspended DWNTs, and find a good agreement between experiment and theory. Moreover, we show that the interlayer coupling in individual DWNTs strongly depends on the interlayer distance, which is manifested in the frequency shifts of the RBLMs with respect to the RBMs of the individual inner and outer tubes. In terms of characterization, this means that the combination of Raman spectroscopy data and predictions of continuous membrane theory may give additional criteria for the index identification of DWNTs, namely the interlayer distance.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Journal of Nanophotonics},
	author = {Levshov, Dmitry I. and Avramenko, Marina V. and Than, Xuan-Tinh and Michel, Thierry and Arenal, Raul and Paillet, Matthieu and Rybkovskiy, Dmitry V. and Osadchy, Alexander V. and Rochal, Sergei B. and Yuzyuk, Yuri I. and Sauvajol, Jean-Louis},
	month = sep,
	year = {2015},
	note = {Publisher: SPIE},
	pages = {012502},
}



@article{wang_novel_2007,
	title = {Novel nanostructures of {ZnO} for nanoscale photonics, optoelectronics, piezoelectricity, and sensing},
	volume = {88},
	issn = {0947-8396, 1432-0630},
	url = {http://link.springer.com/10.1007/s00339-007-3942-8},
	doi = {10.1007/s00339-007-3942-8},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Applied Physics A},
	author = {Wang, Z.L.},
	month = may,
	year = {2007},
	pages = {7--15},
}



@inproceedings{lerer_dispersion_2016-1,
	address = {Cham},
	series = {Springer {Proceedings} in {Physics}},
	title = {Dispersion {Characteristics} of {Zinc} {Oxide} {Nanorods} {Coated} with {Thin} {Silver} {Layer} and {Organized} in {Two}-{Dimensional} {Uniform} {Arrays}},
	isbn = {978-3-319-26324-3},
	doi = {10.1007/978-3-319-26324-3_22},
	abstract = {The problem on electromagnetic waves propagation in a two-dimensional periodic array of zinc oxide nano-waveguides covered with a thin metal film is solved by the method of variables separationMethod of variables separationin cylindrical coordinates. The numerical results obtained by the method are in good agreement with the results computed by the commercial software COMSOL MultiphysicsTM over all optical range and have minor deviations for the wavelength range close to the critical wavelength. Resonances located at the amplitude-frequency characteristics of optical nano-antennas may be interpreted as resonances of circular bilayer nano-wave-guide segments with the ZnO core covered with thin metal shell. The results may also be used to predict the resonance wavelength of two-dimensional periodic arrays of ZnO nanorodsZnO nanorods, coated with a thin metal layer and grown on a dielectric substrate.},
	language = {en},
	booktitle = {Advanced {Materials}},
	publisher = {Springer International Publishing},
	author = {Lerer, A. M. and Timoshenko, P. E. and Kaidashev, E. M. and Puzanov, A. S. and Chernikova, T. Y.},
	editor = {Parinov, Ivan A. and Chang, Shun-Hsyung and Topolov, Vitaly Yu.},
	year = {2016},
	keywords = {Complex Dielectric Constant, Critical Wavelength, Resonant Wavelength, Thin Metal Film, Unknown Coefficient},
	pages = {317--327},
}



@article{shirokov_anomalous_2015,
	title = {Anomalous change in the material moduli of thin films of barium titanate},
	volume = {56},
	issn = {1573-8620},
	url = {https://doi.org/10.1134/S0021894415060218},
	doi = {10.1134/S0021894415060218},
	abstract = {A method is proposed to determine the moduli of thin ferroelectric films subjected to forced deformation due to the mismatch between the crystal lattice sizes of the film and substrate materials and the difference of their thermal expansion coefficients. Models of single-crystal films of barium titanate are studied using the eighth-degree Landau thermodynamic potential. It is shown that in the considered range of forced strain of the barium titanate film, three main states exist: a tetragonal phase (c phase) of 4mm symmetry with spontaneous polarization directed along the normal to the film plane; an orthorhombic phase (aa phase) of 2 mm symmetry with polarization oriented along the diagonal plane of the film; monoclinic phase (r phase) of Cmsymmetry with the intermediate direction of polarization. All phases are separated by the lines of transitions of the second kind. Dependences of the elastic, electric and piezoelectric moduli on the magnitude of forced strain are plotted. It is shown that at the phase boundaries there is an anomalous change in the constants of the ferroelectric film and in the region of existence of the r phase, some moduli reach extreme values.},
	language = {en},
	number = {6},
	urldate = {2023-11-11},
	journal = {Journal of Applied Mechanics and Technical Physics},
	author = {Shirokov, V. B. and Kalinchuk, V. V. and Shakhovoi, R. A. and Yuzyuk, Yu. I.},
	month = nov,
	year = {2015},
	keywords = {thin films, elastic moduli, ferroelectrics, forced strain, material constants, piezoelectric moduli},
	pages = {1103--1110},
}



@article{leontyev_characterization_2015,
	title = {Characterization of the electrocatalytic activity of carbon-supported platinum-based catalysts by thermal gravimetric analysis},
	volume = {25},
	issn = {0959-9436},
	url = {https://www.sciencedirect.com/science/article/pii/S0959943615002229},
	doi = {10.1016/j.mencom.2015.11.024},
	abstract = {Investigations of carbon-supported Pt, Pt3Co, and Pt3Ni electrocatalysts using thermal gravimetric analysis (TGA) in combination with electrochemical measurements of the membrane electrode assemblies (MEA) for proton exchange membrane fuel cells have demonstrated that the onset temperature of the carbon support thermal oxidation and apparent activation energy of this reaction decrease in the following orders: Pt(20\%)/C {\textgreater} Pt(35\%)/C {\textgreater} Pt(46\%)/C and Pt3Ni/C {\textgreater} Pt3Co/C {\textgreater} Pt/C, while MEA power density increases. Thus, TGA can be used as a simple and express technique for analysis of the electrocatalytic activity of carbon-supported Pt-based catalysts for proton exchange membrane fuel cells.},
	number = {6},
	urldate = {2023-11-11},
	journal = {Mendeleev Communications},
	author = {Leontyev, Igor N. and Leontyeva, Daria V. and Kuriganova, Alexandra B. and Popov, Yurii V. and Maslova, Olga A. and Glebova, Nadezhda V. and Nechitailov, Andrei A. and Zelenina, Natalia K. and Tomasov, Alexander A. and Hennet, Louis and Smirnova, Nina V.},
	month = nov,
	year = {2015},
	pages = {468--469},
}



@article{golushko_complex_2015,
	title = {Complex instability of axially compressed tubular lipid membrane with controlled spontaneous curvature},
	volume = {38},
	issn = {1292-895X},
	url = {https://doi.org/10.1140/epje/i2015-15112-6},
	doi = {10.1140/epje/i2015-15112-6},
	abstract = {Tubular lipid membranes (TLMs) are formed by an external pulling force from artificial or biological bilayer vesicles and can be subsequently stabilized by incorporating proteins or amphiphilic polymers into the lipid bilayer. The arising spontaneous curvature of the lipid sheet allows switching off the pulling force without TLM destabilization. However, here we show that during this process two different thermal fluctuation modes drastically increase their amplitudes making fluctuations of the TLM much greater than its radius. Due to the system’s proximity to the critical fluctuation point, a weak axial compressive force is sufficient to destabilize the TLM. Its absolute value is shown to be much smaller than that of the pulling force required for the initial lipid nanotube formation. Induced complex instability was studied in the frame of Landau phase transition theory. The process involves two consecutive second-order phase transitions and leads to the tube deformation combining annular corrugation with completely unconventional chiral buckling.},
	language = {en},
	number = {10},
	urldate = {2023-11-11},
	journal = {The European Physical Journal E},
	author = {Golushko, I. Yu. and Rochal, S. B. and Lorman, V. L.},
	month = oct,
	year = {2015},
	keywords = {Living systems: Biological Matter},
	pages = {112},
}



@article{levshov_interlayer_2015,
	title = {Interlayer {Dependence} of {G}-{Modes} in {Semiconducting} {Double}-{Walled} {Carbon} {Nanotubes}},
	volume = {119},
	issn = {1932-7447},
	url = {https://doi.org/10.1021/acs.jpcc.5b05888},
	doi = {10.1021/acs.jpcc.5b05888},
	abstract = {A double-walled carbon nanotube (DWNT), a coaxial composite of two single-walled carbon nanotubes (SWNT), provides a unique model to study interactions between the two constituent SWNTs. Combining high resolution transmission electron microscopy (HRTEM), electron diffraction (ED), and resonant Raman scattering (RRS) experiments on the same individual suspended DWNT is the ultimate way to relate unambiguously its atomic structure, defined by the chiral indices of the coaxial outer/inner SWNTs, and its Raman-active vibration modes. This approach is used to investigate the intertube distance dependence of the G-modes of individual index-identified DWNTs composed of two semiconducting SWNTs. We state the main features of the dependence of the G-mode frequencies on the distance between the inner and outer layers: (i) When the interlayer distance is larger than the nominal van der Waals distance (close to 0.34 nm), a downshift of the inner-layer G-modes with respect to the G-modes in the equivalent SWNTs is measured. (ii) The amplitude of the downshift depends on the interlayer distance, or in other words, on the negative pressure felt by the inner layer in DWNT. (iii) No shift is observed for an intertube distance close to 0.34 nm.},
	number = {40},
	urldate = {2023-11-11},
	journal = {The Journal of Physical Chemistry C},
	author = {Levshov, D. I. and Michel, T. and Arenal, R. and Tran, H. N. and Than, T. X. and Paillet, M. and Yuzyuk, Yu. I. and Sauvajol, J.-L.},
	month = oct,
	year = {2015},
	note = {Publisher: American Chemical Society},
	pages = {23196--23202},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\M5V5TPZR\\Levshov и др. - 2015 - Interlayer Dependence of G-Modes in Semiconducting.pdf:application/pdf},
}



@article{shirokov_problem_2015,
	title = {The problem of determining elastic constants of thin ferroelectric films},
	volume = {60},
	issn = {1562-6903},
	url = {https://doi.org/10.1134/S1028335815080108},
	doi = {10.1134/S1028335815080108},
	abstract = {A method of determining the constants of the linear equations of the piezoelectric effect dependent on the external conditions is proposed for thin ferroelectric films on the basis of the Landau potential of the phenomenological theory of phase transitions. By the example of single-crystalline barium—titanate thin films, the behavior of material constants is investigated in dependence on the value of the misfit strain. The investigation of material equations is implemented on the basis of the Landau potential of the eighth degree at room temperature. The substantial difference in the elastic, electric, and piezoelectric properties of a thin film from those of a bulk material is shown; the anomalous behavior of constants on the phase boundaries and the extremal behavior inside the r-phase is revealed.},
	language = {en},
	number = {8},
	urldate = {2023-11-11},
	journal = {Doklady Physics},
	author = {Shirokov, V. B. and Kalinchuk, V. V. and Shakhovoy, R. A. and Yuzyuk, Yu. I.},
	month = aug,
	year = {2015},
	keywords = {Barium Titanate, DOKLADY Physic, Elastic Constant, Misfit Strain, Piezoelectric Effect},
	pages = {349--354},
}



@inproceedings{motovilov_terahertz_2015,
	title = {Terahertz and infrared spectroscopy of bacterial nanofilaments},
	url = {https://ieeexplore.ieee.org/document/7327875},
	doi = {10.1109/IRMMW-THz.2015.7327875},
	abstract = {By means of terahertz and infrared (THz, IR) spectroscopies we have measured the dielectric response of nano-filaments of electrogenic bacteria Shewanella oneidensis MR-1 in a wide frequency and temperature ranges. THz-far-IR spectra are dominated by absorption due to bound water. At helium temperatures and at sub-THz frequencies a boson-peak-like excitation is detected that is typical for disordered materials. The observation is in agreement with the heat capacity measurements.},
	urldate = {2023-11-11},
	booktitle = {2015 40th {International} {Conference} on {Infrared}, {Millimeter}, and {Terahertz} waves ({IRMMW}-{THz})},
	author = {Motovilov, Konstantin A. and Gagkaeva, Zarina V. and Kadyrov, Lenar S. and Zhukova, Elena S. and Tobokhova, Aiyyna S. and Torgashev, Victor I. and Savinov, Maxim and Grinenko, Vadim and Belyanchikov, Mikhail A. and Sidoruk, Konstantin V. and Dressel, Martin and Gorshunov, Boris P.},
	month = aug,
	year = {2015},
	note = {ISSN: 2162-2035},
	pages = {1--2},
}



@article{yohannes_effect_2015,
	title = {Effect of ethylene glycol on electrochemical and morphological features of platinum electrodeposits from chloroplatinic acid},
	volume = {45},
	issn = {1572-8838},
	url = {https://doi.org/10.1007/s10800-015-0820-5},
	doi = {10.1007/s10800-015-0820-5},
	abstract = {The aim of this work was to investigate the morphology, average size, and the electrochemical behavior of platinum nanoparticles electrodeposited from water and mixed water–ethylene glycol solutions of the electrolyte of H2PtCl6 and H2SO4 at a rotating disk electrode coated with Vulcan XC-72 carbon powder. Cyclic voltammetry and linear sweep voltammetry were used to determine the electrochemically active surface area (ESA) and oxygen reduction reaction (ORR) activity of the prepared Pt/C materials, respectively. XRD and scanning electron microscopy were used to study the influence of the electrodeposition methods applied on the morphology of platinum particles deposited in water and mixed water–ethylene glycol solutions. The average size of Pt crystallites was in the range of ca. 6–10 nm, and the average size of deposited Pt particles was in the range of ca. 30–150 nm. It was found that the presence of ethylene glycol in the electrolyte solution increased the overpotential of electrodeposition and it also strongly affected the morphology of Pt deposits when constant current electrodeposition was employed. Moreover, it was shown that pulse current electrodeposition is a more effective method compared to constant current electrodeposition method for the preparation of the Pt/Vulcan electrode with high ESA of Pt and enhanced catalytic activity toward ORR. The results obtained concerning the morphology and the spatial distribution of platinum particles electrodeposited on the surface of carbon support at different conditions demonstrate new possibilities to improve synthesis of Pt/C by electrodeposition methods.},
	language = {en},
	number = {6},
	urldate = {2023-11-11},
	journal = {Journal of Applied Electrochemistry},
	author = {Yohannes, Weldegebriel and Belenov, S. V. and Guterman, V. E. and Skibina, L. M. and Volotchaev, V. A. and Lyanguzov, N. V.},
	month = jun,
	year = {2015},
	keywords = {Platinum, Electrocatalyst, Galvanostatic electrodeposition, ORR, Vulcan XC-72},
	pages = {623--633},
}



@article{avramenko_vibrational_2015,
	title = {Vibrational heat capacity of carbon nanotubes at low and ultra-low temperatures},
	volume = {68},
	issn = {1386-9477},
	url = {https://www.sciencedirect.com/science/article/pii/S138694771400472X},
	doi = {10.1016/j.physe.2014.12.033},
	abstract = {To measure a heat capacity of a single carbon nanotube is impossible nowadays and experiments are performed with the nanotubes bundles. However, the existing theories of carbon nanotubes heat capacity do not take into account an interaction between an individual nanotube and its environment. Here we show that due to this fact the known theories overestimate the heat capacity in the ultra-low temperature limit. In this region the main contribution to heat capacity of a single free nanotube is caused by the bending phonon mode with a quadratic dispersion. At T=1K different known models of the phonon dynamics lead to the theoretical specific heat which is at least 10 times greater than the experimentally measured value. To overcome this contradiction we take into account the interaction between an individual nanotube and its environment. As a result, the nanotube loses its Goldstone degrees of freedom and essential reconstruction of the lowest-energy part of its phonon spectrum occurs. The theory proposed explains experimental data on thermal capacity in the ultra-low temperature range and simultaneously demonstrates better agreement with experiments in the region 2.5K{\textless}T{\textless}40K than the preceding models.},
	urldate = {2023-11-11},
	journal = {Physica E: Low-dimensional Systems and Nanostructures},
	author = {Avramenko, M. V. and Golushko, I. Yu. and Myasnikova, A. E. and Rochal, S. B.},
	month = apr,
	year = {2015},
	keywords = {2D membranes, Carbon nanotubes, Heat capacity, Low temperatures, Phonon spectrum, Pinning},
	pages = {133--139},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\QUQ3BBJ9\\Avramenko и др. - 2015 - Vibrational heat capacity of carbon nanotubes at l.pdf:application/pdf},
}



@article{chernovyants_synthesis_2015,
	title = {Synthesis and structure of interaction products of quinoline-2({1H})-thione with molecular iodine},
	volume = {139},
	issn = {1386-1425},
	url = {https://www.sciencedirect.com/science/article/pii/S1386142514018551},
	doi = {10.1016/j.saa.2014.12.075},
	abstract = {The behavior of quinoline-2(1H)-thione, which is a potential antithyroid drug toward molecular iodine, was investigated. The ability of quinoline-2(1H)-thione to form the outer-sphere charge-transfer complex C9H7NS·I2 with iodine molecular in dilute chloroform solution has been studied by UV–vis spectroscopy (lgβ=3.85). The crystal structure of the new salt 2-(quinoline-2-yldisulfanyl)quinolinium triiodide – product of irreversible oxidation of quinoline-2(1H)-thione was determined by X-ray diffraction. The 2-(quinoline-2-yldisulfanyl)quinolinium cations form dimers through π–π–stacking interaction between quinoline rings. Strong intramolecular interactions are observed between iodine – sulfur atoms and iodine – hydrogen atoms with shortened contacts (less of sum of van der Waals contacts). It is noteworthy that two perfectly centrosymmetrical anions I3− form a very short contact I(3)⋯I(3′) 3.7550(5) so we can state the formation of the dianion I62−. Therefore the formation and topology of polyiodide species depend on the characteristics, such as shape, size and charge, etc., of the counter cation, 2-(quinoline-2-yldisulfanyl)quinolinium, which is considered as templating agent.},
	urldate = {2023-11-11},
	journal = {Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy},
	author = {Chernov’yants, Margarita S. and Starikova, Zoya A. and Kolesnikova, Tatiana S. and Karginova, Anastasia O. and Lyanguzov, Nikolay V.},
	month = mar,
	year = {2015},
	keywords = {X-ray diffraction, Raman spectroscopy, 2-(quinoline-2-yldisulfanyl)quinolinium triiodide, Charge-transfer complex, IR, Quinoline-2(1)-thione},
	pages = {533--538},
}



@article{roshal_slightly_2015,
	title = {Slightly broken icosahedral symmetry advances {Thomson} problem},
	volume = {379},
	issn = {0375-9601},
	url = {https://www.sciencedirect.com/science/article/pii/S0375960114011682},
	doi = {10.1016/j.physleta.2014.11.039},
	abstract = {To advance Thomson problem we generalize physical principles suggested by Caspar and Klug (CK) to model icosahedral capsids. Proposed simplest distortions of the CK spherical arrangements yield new-type trial structures very close to the lowest energy ones. In the region 600≤N≤1000, where N is the number of particles in the structure, we found 40 new spherical crystals with the lowest ever seen energies and curvature-induced topological defects being not the well-known elongated scars but flatten pentagons. These crystals have N values prohibited in the CK model and demonstrate a new way to combine the local hexagonal order and spherical geometry.},
	number = {4},
	urldate = {2023-11-11},
	journal = {Physics Letters A},
	author = {Roshal, D. S. and Myasnikova, A. E. and Rochal, S. B.},
	month = feb,
	year = {2015},
	keywords = {Topological defects, Caspar and Klug theory, Self-assembly, Spherical crystals, Thomson problem, Viral capsids},
	pages = {372--376},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\I3PW53KV\\Roshal и др. - 2015 - Slightly broken icosahedral symmetry advances Thom.pdf:application/pdf},
}



@article{anokhin_difference_2015,
	title = {Difference {Raman} spectroscopy of {DNA} molecules},
	volume = {584},
	issn = {1742-6596},
	url = {https://dx.doi.org/10.1088/1742-6596/584/1/012022},
	doi = {10.1088/1742-6596/584/1/012022},
	abstract = {In this paper the micro-Raman spectra of calf DNA for different points of DNA sample have been recorded. The Raman spectra were made with help of difference Raman spectroscopy technique. Raman spectra were recorded with high spatial resolution from different points of the wet and dry samples in different spectral range (100÷4000cm−1) using two lasers: argon (514.5 nm) and helium -neon (632.8 nm). The significant differences in the Raman spectra for dry and wet DNA and for different points of DNA molecules were observed. The obtained data on difference Raman scattering spectra of DNA molecules may be used for identification of DNA types and for analysis of genetic information associated with the molecular structure of this molecule.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Journal of Physics: Conference Series},
	author = {Anokhin, Andrey S. and Gorelik, Vladimir S. and Dovbeshko, Galina I. and Pyatyshev, Alexander Yu and Yuzyuk, Yury I.},
	month = jan,
	year = {2015},
	pages = {012022},
	file = {IOP Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\B6MCEJV5\\Anokhin и др. - 2015 - Difference Raman spectroscopy of DNA molecules.pdf:application/pdf},
}



@article{shirokov_anomalies_2014,
	title = {Anomalies of piezoelectric coefficients in barium titanate thin films},
	volume = {108},
	issn = {0295-5075},
	url = {https://dx.doi.org/10.1209/0295-5075/108/47008},
	doi = {10.1209/0295-5075/108/47008},
	abstract = {Modeling of electromechanical devices involves the use of different material coefficients, whose measurement is a difficult task, especially when the problem concerns thin films. Required coefficients of thin films could be found theoretically, using known values of the bulk constants. Electromechanical coefficients of barium titanate thin films are still unknown; therefore, it is expedient to carry out their calculations. We give here the full set of electromechanical coefficients of barium titanate thin films for the whole range of technologically available misfit strains. In the present paper, piezoelectric coefficients as functions of a misfit strain were calculated. It was revealed that piezoelectric coefficients exhibit anomalies at phase boundaries and inside the monoclinic r-phase as well. The obtained results allow finding the required values of the thin-film parameters, varying the misfit strain.},
	language = {en},
	number = {4},
	urldate = {2023-11-11},
	journal = {Europhysics Letters},
	author = {Shirokov, Vladimir and Kalinchuk, Valery and Shakhovoy, Roman and Yuzyuk, Yury},
	month = nov,
	year = {2014},
	note = {Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica},
	pages = {47008},
}



@article{gorshunov_thzir_2014,
	title = {{THz}–{IR} spectroscopy of single {H2O} molecules confined in nanocage of beryl crystal lattice},
	volume = {87},
	issn = {0141-1594},
	url = {https://doi.org/10.1080/01411594.2014.954247},
	doi = {10.1080/01411594.2014.954247},
	abstract = {We have measured the terahertz–infrared (3–7000 cm−1) spectra of the optical conductivity of iron-doped single crystals of beryl, (Mn,Fe):Be3Al2Si6O18, that contain lone water molecules isolated within nanometer-sized cages formed by the ions of beryl crystal lattice. By comparing the spectra with those of dehydrated crystals, we exclude phonon resonances and reconstruct the spectra determined exclusively by vibrations of the water molecules. At liquid-helium temperatures, well-known intramolecular H2O modes are observed above 1000 cm−1 and accompanied with satellite resonances that are combinations of intramolecular and external vibrations of H2O molecules. At terahertz frequencies, a broad bump centred around 20 cm−1 (at 5 K) is observed with three rather narrow resonances at its high-frequency shoulder (38, 42 and 46 cm−1). The origin of these low-energy excitations is discussed.},
	number = {10-11},
	urldate = {2023-11-11},
	journal = {Phase Transitions},
	author = {Gorshunov, Boris P. and Zhukova, Elena S. and Torgashev, Victor I. and Motovilova, Elizaveta A. and Lebedev, Vladimir V. and Prokhorov, Anatoly S. and Shakurov, Gil’man S. and Kremer, Reinhard K. and Uskov, Vladimir V. and Pestrjakov, Efim V. and Thomas, Victor G. and Fursenko, Dimitri A. and Kadlec, Christelle and Kadlec, Filip and Dressel, Martin},
	month = nov,
	year = {2014},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/01411594.2014.954247},
	keywords = {nano-confined water molecule, terahertz spectroscopy},
	pages = {966--972},
}



@article{mikheykin_high_2014,
	title = {High pressure x-ray diffraction study of nickel–copper chromites solid solutions},
	volume = {26},
	issn = {0953-8984},
	url = {https://dx.doi.org/10.1088/0953-8984/26/50/505401},
	doi = {10.1088/0953-8984/26/50/505401},
	abstract = {A high-pressure synchrotron radiation diffraction study has been carried out on Ni1−xCuxCr2O4 solid solutions. Observed pressure-controlled phase transitions, along with data previously collected for temperature-induced phase transitions, are analyzed in the framework of the unified phenomenological model that results in mapping of the generic phase diagram for the whole family of Ni1−xCuxCr2O4 solid solutions.},
	language = {en},
	number = {50},
	urldate = {2023-11-11},
	journal = {Journal of Physics: Condensed Matter},
	author = {Mikheykin, A. S. and Torgashev, V. I. and Talanov, V. M. and Bush, A. A. and Chernyshov, D. and Yuzyuk, I. Yu and Dmitriev, V. P.},
	month = nov,
	year = {2014},
	note = {Publisher: IOP Publishing},
	pages = {505401},
}



@article{zhilin_photoelectric_2014,
	title = {Photoelectric properties of {MSM} structure based on {ZnO} nanorods, received by thermal evaporation and carbothermal syntesis},
	volume = {541},
	issn = {1742-6596},
	url = {https://dx.doi.org/10.1088/1742-6596/541/1/012038},
	doi = {10.1088/1742-6596/541/1/012038},
	abstract = {Photoelectric characteristics of metal-semiconductor-metal (MSM) structures: Au/ZnO(nanorods)/ZnO(film)/ZnO(nanorods)/Au were investigated. Synthesis of ZnO nanorods (NR's) was carried out by two different methods, such as catalyst-free carbothermal synthesis (t = 950°C, precursor – ZnO:C) and catalyst-free thermal evaporation of metallic Zn (t = 600°C, precursor Zn). Photoluminescence spectra have shown that the ZnO NR's obtained by means of thermal evaporation technique have a lower concentration of point defects related with oxygen vacancies, than ZnO NR's prepared by carbothermal synthesis. MSM structure with ZnO NR's obtained by thermal evaporation technique have photosensitivity 97 mA/W at 325 nm illumination and 44 mA/W at 518 nm illumination at a bias 5V. For MSM structure with ZnO NR's obtained by method of carbothermal synthesis, the photosensitivity values were 22 mA/W, and 103 mA/W, respectively.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Journal of Physics: Conference Series},
	author = {Zhilin, D. A. and Lyanguzov, N. V. and Nikolaev, L. A. and Pushkariov, V. I. and Kaidashev, E. M.},
	month = oct,
	year = {2014},
	pages = {012038},
	file = {IOP Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\49KV5PK9\\Zhilin и др. - 2014 - Photoelectric properties of MSM structure based on.pdf:application/pdf},
}



@article{talanov_combined_2014,
	title = {Combined atomic ordering in the {A} and {B} sublattices of perovskite structure},
	volume = {59},
	issn = {1562-689X},
	url = {https://doi.org/10.1134/S1063774514050198},
	doi = {10.1134/S1063774514050198},
	abstract = {The simultaneous ordering of cations in the A and B sublattices of cubic perovskite structure has been investigated by the group-theoretical method. It is found that 147 ordered phases may exist. Among them, there may be 121 phases with simultaneous cation ordering in the 1(a)- and 1(c) positions of perovskite structure. It is shown that 53 phases are described by improper order parameters related to cation ordering, the formation of 56 phases is related to improper rotations of octahedra, and 15 phases are improper ferroelectrics. Calculated structures of some types of ordered low-symmetry perovskite modifications are presented.},
	language = {en},
	number = {5},
	urldate = {2023-11-11},
	journal = {Crystallography Reports},
	author = {Talanov, M. V. and Shirokov, V. B. and Talanov, V. M.},
	month = sep,
	year = {2014},
	keywords = {Crystallography Report, Group Theoretical Method, Permutation Representation, Perovskite, Perovskite Structure},
	pages = {662--678},
}



@article{talanov_group-theoretical_2014,
	title = {Group-theoretical study of cationic ordering in perovskite structure},
	volume = {59},
	issn = {1562-689X},
	url = {https://doi.org/10.1134/S1063774514050186},
	doi = {10.1134/S1063774514050186},
	abstract = {Atomic ordering in the structure of cubic perovskite has been investigated by the group-theoretical method. The possibility of existence of 13 ordered phases in the 1(a) position (including four binary, two ternary, and five quaternary cationic superstructures) and 13 phases with different types of ordering in the 1(b) position (including four binary, two ternary, and five quaternary cationic superstructures) is established. Calculated structures of some types of ordered low-symmetry perovskite modifications are reported.},
	language = {en},
	number = {5},
	urldate = {2023-11-11},
	journal = {Crystallography Reports},
	author = {Talanov, V. M. and Talanov, M. V. and Shirokov, V. B.},
	month = sep,
	year = {2014},
	keywords = {Crystallography Report, Perovskite, Perovskite Structure, CaCu, Central Atom},
	pages = {650--661},
}



@inproceedings{timoshenko_scattering_2014,
	title = {Scattering of magnetostatic waves by defects of the surface of a ferromagnetic film},
	volume = {1},
	url = {https://ieeexplore.ieee.org/document/6958761},
	doi = {10.1109/APEDE.2014.6958761},
	abstract = {The solution for the diffraction problem of scattering of magnetostatic waves by an arbitrary shallow defect situated under the surface of a ferromagnetic film magnetized at an arbitrary angle is obtained in the quasi-static approximation. Expressions for the energy flux density of scattered magnetostatic waves in the far-field zone are found.},
	urldate = {2023-11-11},
	booktitle = {2014 {International} {Conference} on {Actual} {Problems} of {Electron} {Devices} {Engineering} ({APEDE})},
	author = {Timoshenko, P. E. and Babichev, R. K. and Vyatkina, S. A.},
	month = sep,
	year = {2014},
	pages = {279--283},
}



@inproceedings{timoshenko_finite_2014,
	title = {Finite element simulation of surface acoustic waves excited in barium-strontium titanate films fabricated on magnesium oxide substrate by interdigital transducers},
	volume = {1},
	url = {https://ieeexplore.ieee.org/document/6958762},
	doi = {10.1109/APEDE.2014.6958762},
	abstract = {In this paper, we present study on surface acoustic waves excited in barium — strontium titanate films fabricated on magnesium oxide substrate by interdigital transducers. The surface acoustic waves propagation was simulated by using COMSOL Multiphysics™. The presence of bias, since the oscillations are not considered as sagittal polarized, is the principal difference between considered problem and standard problem that implemented in many finite element packages. The calculations of mechanic displacement and electric field potential for the first Eigen frequencies for different planes are shown. The methods of modeling in COMSOL Multiphysics™ software package are presented in this paper can be used for calculations of other systems that have different complex configuration.},
	urldate = {2023-11-11},
	booktitle = {2014 {International} {Conference} on {Actual} {Problems} of {Electron} {Devices} {Engineering} ({APEDE})},
	author = {Timoshenko, P. E. and Kalinchuk, V. V. and Shirokov, V. B. and Levi, M. O. and Pan'kin, A. V. and Donets, A. V.},
	month = sep,
	year = {2014},
	pages = {283--289},
}



@article{pushkariov_synthesis_2014,
	title = {Synthesis and characterization of {ZnO} nanorods obtained by catalyst-free thermal technique},
	volume = {541},
	issn = {1742-6596},
	url = {https://dx.doi.org/10.1088/1742-6596/541/1/012031},
	doi = {10.1088/1742-6596/541/1/012031},
	abstract = {ZnO nanorod arrays have been synthesized on silicon wafers by catalyst free thermal vapor deposition with different temperature values. Vertical-aligned ZnO nanostructures were grown at the quite low temperatures by this method. Modification of the method allowed to place silicon substrates in areas with different ratios of concentrations Ar and O2 molecules in the vapor phase. Photoluminescence spectroscopy and electron microscopy studies have shown that morphologies and optical properties of nanorods depends on different ratios of concentrations of the molecules in the vapor phase.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Journal of Physics: Conference Series},
	author = {Pushkariov, V. I. and Nikolaev, A. L. and Kaidashev, E. M.},
	month = oct,
	year = {2014},
	pages = {012031},
	file = {IOP Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\7WR58HGN\\Pushkariov и др. - 2014 - Synthesis and characterization of ZnO nanorods obt.pdf:application/pdf},
}



@article{puzikov_pulsed_2014,
	title = {Pulsed laser deposition and investigation of antimony-doped {ZnO} films},
	volume = {541},
	issn = {1742-6596},
	url = {https://dx.doi.org/10.1088/1742-6596/541/1/012004},
	doi = {10.1088/1742-6596/541/1/012004},
	abstract = {We have investigated the influence of oxygen partial pressure, temperature of synthesis and annealing conditions on nanocsrystallineSb-doped thin films, grown by pulsed laser deposition. It is shown that the minimum resistivity ( 8·10−3Ω·cm) and the maximum carriers density ( 2·1019 cm-3) corresponds to the pressure range 5·10−3-7·10−3 mbar, to the temperature 550 ° C and in situ annealing at 700 °C.Also we show the features of the crystal lattice's dynamics, which are found in the Raman research.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Journal of Physics: Conference Series},
	author = {Puzikov, A. S. and Lyanguzov, N. V. and Kaidashev, E. M.},
	month = oct,
	year = {2014},
	pages = {012004},
	file = {IOP Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\H6J3GSQ8\\Puzikov и др. - 2014 - Pulsed laser deposition and investigation of antim.pdf:application/pdf},
}



@inproceedings{nistratov_experimental_2014,
	title = {Experimental investigation of magnetostatic backward volume waves excited by the narrow transducer},
	volume = {1},
	url = {https://ieeexplore.ieee.org/document/6958745},
	doi = {10.1109/APEDE.2014.6958745},
	abstract = {The results of experimental investigation of diffraction profiles of magnetostatic backward volume waves (MSBVW) exited by the linear transducer with finite length located at the surface of ferrite-dielectric structure are presented. The comparison of experimental data obtained and theoretical calculations is reported.},
	urldate = {2023-11-11},
	booktitle = {2014 {International} {Conference} on {Actual} {Problems} of {Electron} {Devices} {Engineering} ({APEDE})},
	author = {Nistratov, N. P. and Vyatkina, S. A. and Babichev, R. K. and Timoshenko, P. E.},
	month = sep,
	year = {2014},
	pages = {199--204},
}



@article{zhukova_vibrational_2014,
	title = {Vibrational states of a water molecule in a nano-cavity of beryl crystal lattice},
	volume = {140},
	issn = {0021-9606},
	url = {https://doi.org/10.1063/1.4882062},
	doi = {10.1063/1.4882062},
	abstract = {Low-energy excitations of a single water molecule are studied when confined within a nano-size cavity formed by the ionic crystal lattice. Optical spectra are measured of manganese doped beryl single crystal Mn:Be3Al2Si6O18, that contains water molecules individually isolated in 0.51 nm diameter voids within the crystal lattice. Two types of orientation are distinguished: water-I molecules have their dipole moments aligned perpendicular to the c axis and dipole moments of water-II molecules are parallel to the c-axis. The optical conductivity σ(ν) and permittivity ɛ′(ν) spectra are recorded in terahertz and infrared ranges, at frequencies from several wavenumbers up to ν = 7000 cm−1, at temperatures 5–300 K and for two polarizations, when the electric vector E of the radiation is parallel and perpendicular to the c-axis. Comparative experiments on as-grown and on dehydrated samples allow to identify the spectra of σ(ν) and ɛ′(ν) caused exclusively by water molecules. In the infrared range, well-known internal modes ν1, ν2, and ν3 of the H2O molecule are observed for both polarizations, indicating the presence of water-I and water-II molecules in the crystal. Spectra recorded below 1000 cm−1 reveal a rich set of highly anisotropic features in the low-energy response of H2O molecule in a crystalline nano-cavity. While for E∥c only two absorption peaks are detected, at ∼90 cm−1 and ∼160 cm−1, several absorption bands are discovered for E⊥c, each consisting of narrower resonances. The bands are assigned to librational (400–500 cm−1) and translational (150–200 cm−1) vibrations of water-I molecule that is weakly coupled to the nano-cavity “walls.” A model is presented that explains the “fine structure” of the bands by a splitting of the energy levels due to quantum tunneling between the minima in a six-well potential relief felt by a molecule within the cavity.},
	number = {22},
	urldate = {2023-11-11},
	journal = {The Journal of Chemical Physics},
	author = {Zhukova, Elena S. and Torgashev, Victor I. and Gorshunov, Boris P. and Lebedev, Vladimir V. and Shakurov, Gil'man S. and Kremer, Reinhard K. and Pestrjakov, Efim V. and Thomas, Victor G. and Fursenko, Dimitry A. and Prokhorov, Anatoly S. and Dressel, Martin},
	month = jun,
	year = {2014},
	pages = {224317},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\776RNGVS\\Zhukova и др. - 2014 - Vibrational states of a water molecule in a nano-c.pdf:application/pdf},
}



@article{leontyev_size_2014,
	title = {Size dependence of the lattice parameters of carbon supported platinum nanoparticles: {X}-ray diffraction analysis and theoretical considerations},
	volume = {4},
	issn = {2046-2069},
	shorttitle = {Size dependence of the lattice parameters of carbon supported platinum nanoparticles},
	url = {https://pubs.rsc.org/en/content/articlelanding/2014/ra/c4ra04809a},
	doi = {10.1039/C4RA04809A},
	abstract = {Carbon supported Pt nanoparticles with diameters ranging from 2 to 28 nm have been studied using X-ray diffraction. The unit cell parameter of synthesized Pt/C nanoparticles is always lower than that of bulk Pt. By decreasing the average particle size D to approximately 2 nm, the unit cell parameter a nonlinearly decreases by about 0.03 Å which corresponds to a variation of 0.7\% in comparison to bulk Pt, and the size effect is predominant for sizes ranging from 2 to 10 nm. The dependence a(1/D) is approximated well using a straight line with a slope of −0.0555 ± 0.0067 nm−1 and an intercept of −3.9230 ± 0.0017 Å. For interpreting the obtained experimental dependence of the unit cell parameter of Pt/C nanoparticles, four different theoretical approaches such as the thermal vacancy mechanism, continuous-medium model, Laplace pressure, and bond order–length–strength correlation mechanism, were used. Comparison of the calculated dependencies, based on the above models, with the experimental ones, shows that the continuous-medium model agrees best with the experimentally found unit cell parameter dependence of our carbon supported Pt nanoparticles.},
	language = {en},
	number = {68},
	urldate = {2023-11-11},
	journal = {RSC Advances},
	author = {Leontyev, I. N. and Kuriganova, A. B. and Leontyev, N. G. and Hennet, L. and Rakhmatullin, A. and Smirnova, N. V. and Dmitriev, V.},
	month = aug,
	year = {2014},
	note = {Publisher: The Royal Society of Chemistry},
	pages = {35959--35965},
}



@article{janolin_strain_2014,
	title = {Strain engineering of perovskite thin films using a single substrate},
	volume = {26},
	issn = {0953-8984},
	url = {https://dx.doi.org/10.1088/0953-8984/26/29/292201},
	doi = {10.1088/0953-8984/26/29/292201},
	abstract = {Combining temperature-dependent x-ray diffraction, Raman spectroscopy and first-principles-based effective Hamiltonian calculations, we show that varying the thickness of (Ba0.8Sr0.2)TiO3 (BST) thin films deposited on the same single substrate (namely, MgO) enables us to change not only the magnitude but also the sign of the misfit strain. Such previously overlooked control of the strain allows several properties of these films (e.g. Curie temperature, symmetry of ferroelectric phases, dielectric response) to be tuned and even optimized. Surprisingly, such desired control of the strain (and of the resulting properties) originates from an effect that is commonly believed to be detrimental to functionalities of films, namely the existence of misfit dislocations. The present study therefore provides a novel route to strain engineering, as well as leading us to revisit common beliefs.},
	language = {en},
	number = {29},
	urldate = {2023-11-11},
	journal = {Journal of Physics: Condensed Matter},
	author = {Janolin, P.-E. and Anokhin, A. S. and Gui, Z. and Mukhortov, V. M. and Golovko, Yu I. and Guiblin, N. and Ravy, S. and Marssi, M. El and Yuzyuk, Yu I. and Bellaiche, L. and Dkhil, B.},
	month = jun,
	year = {2014},
	note = {Publisher: IOP Publishing},
	pages = {292201},
}



@article{roshal_extended_2014,
	title = {Extended topological defects as sources and outlets of dislocations in spherical hexagonal crystals},
	volume = {378},
	issn = {0375-9601},
	url = {https://www.sciencedirect.com/science/article/pii/S0375960114002941},
	doi = {10.1016/j.physleta.2014.03.037},
	abstract = {Extended topological defects (ETDs) arising in spherical hexagonal crystals due to their curvature are considered. These prevalent defects carry a unit total topological charge and are surrounded by scalene pentagonal boundaries. Topological peculiarities of reactions between ETDs and dislocations are considered. Similarly to boundaries of the usual planar crystalline order the ETDs emit and absorb the dislocations without preservation of their dislocational charge. Dislocations located inside the ETD area lose it and the enforced ETD decay can proceed in different ways without conservation of the total Burgers vector of the dislocations emitted.},
	number = {21},
	urldate = {2023-11-11},
	journal = {Physics Letters A},
	author = {Roshal, D. S. and Petrov, K. Yu. and Myasnikova, A. E. and Rochal, S. B.},
	month = apr,
	year = {2014},
	keywords = {Colloidal crystals, Curvature, Disclinations, Dislocations, Spherical structures, Topological defects},
	pages = {1548--1552},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\VVC82RZB\\Roshal и др. - 2014 - Extended topological defects as sources and outlet.pdf:application/pdf},
}



@article{baudry_longitudinal_2014,
	title = {Longitudinal and {Transversal} {Polarization} {Switching} in {Strained} {Ferroelectrics}},
	volume = {461},
	issn = {0015-0193},
	url = {https://doi.org/10.1080/00150193.2014.889528},
	doi = {10.1080/00150193.2014.889528},
	abstract = {Using the multicomponent Landau-Devonshire functional we study the field-induced polarization switching in c-oriented ferroelectric phase of epitaxial perovskite film and found that two different regimes are possible: (i) longitudinal switching with change of the polarization modulus and (ii) transversal switching with virtual admixing of the a-component of polarization. The results are specified for the case of barium titanate oxide BaTiO3where the crossover line between two types of switching is found at strain-temperature phase diagram.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Ferroelectrics},
	author = {Baudry, L. and Luk’yanchuk, I. A. and Razumnaya, A.},
	month = mar,
	year = {2014},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/00150193.2014.889528},
	keywords = {Ferroelectric thin films, strain, switching},
	pages = {22--28},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\XAP4K9W5\\Baudry и др. - 2014 - Longitudinal and Transversal Polarization Switchin.pdf:application/pdf},
}



@article{zhukova_quantum_2014,
	title = {Quantum behaviour of water molecule in gemstone: terahertz fingerprints},
	volume = {486},
	issn = {1742-6596},
	shorttitle = {Quantum behaviour of water molecule in gemstone},
	url = {https://dx.doi.org/10.1088/1742-6596/486/1/012019},
	doi = {10.1088/1742-6596/486/1/012019},
	abstract = {We have shown that a weak interaction of a lone H2O molecule with the ‘‘walls’’ of nano-sized crystalline cage of gemstone (beryl) results in emergence of a rich set of molecular vibrational states. By analogy with translational and librational bands in liquid water and ice corresponding absorption bands are explained as due to translational (T) and librational (L) movements of the H2O molecule which is hydrogen bonded to the cage walls. In beryl crystal lattice, however, the six-fold symmetry of the cage brings about additional effect of splitting of the T and L bands into fine structure due to tunnelling within the six-well potential relief. The presented results will be of use for analysis of more complicated systems with confined water molecules like H2O chains in carbon nano-tubes, molecular clusters in e.g. zeolites, clays, silica gels and other natural or synthetic frameworks, as well as for interfacial water in biological systems.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Journal of Physics: Conference Series},
	author = {Zhukova, Elena S. and Gorshunov, Boris P. and Torgashev, Victor I. and Lebedev, Vladimir V. and Shakurov, Gil'man S. and Kremer, Reinhard K. and Pestrjakov, Efim V. and Thomas, Victor G. and Fursenko, Dimitry A. and Dressel, Martin},
	month = mar,
	year = {2014},
	pages = {012019},
	file = {IOP Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\E6MX2SN9\\Zhukova и др. - 2014 - Quantum behaviour of water molecule in gemstone t.pdf:application/pdf},
}



@article{talanov_atomic_2014,
	title = {Atomic order in the spinel structure – a group-theoretical analysis},
	volume = {70},
	copyright = {Copyright (c) 2014 International Union of Crystallography},
	issn = {2053-2733},
	url = {http://scripts.iucr.org/cgi-bin/paper?kx5021},
	doi = {10.1107/S2053273313027605},
	abstract = {Group-theoretical methods of the Landau theory of phase transitions are used to investigate the structures of ordered spinels. The possibility of the existence is determined of 305 phases with different types of order in Wyckoff position 8a (including seven binary and seven ternary cation substructures), 537 phases in Wyckoff position 16d (including eight binary and 11 ternary cation substructures), 595 phases in Wyckoff position 32e (including seven binary and four ternary anion substructures) and 549 phases with simultaneous ordering in Wyckoff positions 8a and 16d (including five substructures with binary order in tetrahedral and octahedral sublattices, two substructures with ternary order in both spinel sublattices, and nine substructures with different combined types of binary and ternary order). Theoretical results and experimental data are compared. Calculated structures of the spread types of ordered low-symmetry spinel modifications are given.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Acta Crystallographica Section A: Foundations and Advances},
	author = {Talanov, V. M. and Shirokov, V. B.},
	month = jan,
	year = {2014},
	note = {Number: 1
Publisher: International Union of Crystallography},
	pages = {49--63},
}



@article{ponomareva_effect_2014,
	title = {Effect of thermal annealing on the surface of sol-gel prepared oxide film studied by atomic force microscopy and {Raman} spectroscopy},
	volume = {40},
	issn = {1608-313X},
	url = {https://doi.org/10.1134/S1087659614010192},
	doi = {10.1134/S1087659614010192},
	abstract = {In this work, we have investigated the surface topography evolution of sol-gel deposited SiO2-SnO2 nanocomposite films annealed in the temperature range 200–600°C. The fractal dimension of atomic force microscopy images of the films was determined by the cube counting method and the triangulation method. The fractal dimension was shown to be an appropriate and easy to use tool for the characterization of nanosized thin film structures. Raman spectroscopy revealed the formation of a SiO2 cage-like structure at 400°C and SnO2 crystallization above 500°C.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Glass Physics and Chemistry},
	author = {Ponomareva, A. A. and Moshnikov, V. A. and Maslova, O. A. and Yuzyuk, Yu. I. and Suchaneck, G.},
	month = jan,
	year = {2014},
	keywords = {nanocomposite SiO2-SnO2, the sol-gel method},
	pages = {99--105},
}



@article{gorshunov_boson_2014,
	title = {Boson peak in manganites},
	volume = {486},
	issn = {1742-6596},
	url = {https://dx.doi.org/10.1088/1742-6596/486/1/012001},
	doi = {10.1088/1742-6596/486/1/012001},
	abstract = {After the phase transition occurs in manganites La1-xCaxMnO3 (x ≥ 0.5) into a dielectric phase with charge order, right below the corresponding temperature of TCO = 240 K a series of absorption lines appear in the terahertz spectral range, only in case of commensurate x values. We show that the lines originate from acoustic phonons that become optically active by folding of the Brillouin zone. At even lower temperatures, a strongly asymmetric extra absorption band develops at frequencies around 20 cm−1 – 30 cm−1 corresponding to the position of the lowest-energy van Hove singularity in the reduced Brillouin zone. The band is assigned to the Boson Peak, i.e. to the excess of lattice vibrational states over the standard Debye contribution. The folded phonons and the boson peak do not show up for incommensurate calcium.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Journal of Physics: Conference Series},
	author = {Gorshunov, Boris P. and Zhukova, Elena S. and Torgashev, Victor I. and Kadyrov, Lenar S. and Motovilova, Elizaveta A. and Fischgrabe, Florian and Moshnyaga, Vasiliy and Zhang, Tao and Kremer, Reinhard and Pracht, Uwe and Zapf, Sina and Dressel, Martin},
	month = mar,
	year = {2014},
	pages = {012001},
	file = {IOP Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\MKBKK4JA\\Gorshunov и др. - 2014 - Boson peak in manganites.pdf:application/pdf},
}



@article{levshov_coupled_2014,
	title = {Coupled {Vibrations} in {Index}-{Identified} {Carbon} {Nanotubes}},
	volume = {1700},
	issn = {0272-9172, 1946-4274},
	url = {https://www.cambridge.org/core/journals/mrs-online-proceedings-library-archive/article/abs/coupled-vibrations-in-indexidentified-carbon-nanotubes/2DD3B289A28698521E4E64C11E70F0DB},
	doi = {10.1557/opl.2014.574},
	abstract = {Combining high resolution transmission electron spectroscopy, electron diffraction, and resonant Raman spectroscopy experiments on the same suspended (free-standing) individual carbon nanotubes is the ultimate approach to relate unambiguously the structure and the intrinsic phonon features of these nano-systems.By using this approach, the effect of coupling between nanotubes on the phonons is investigated in two model nano-systems: (i) a bundle of two non-identical SWNTs (inhomogeneous dimer), (ii) double-walled carbon nanotubes.},
	language = {en},
	urldate = {2023-11-11},
	journal = {MRS Online Proceedings Library (OPL)},
	author = {Levshov, Dmitry and Michel, Thierry and Paillet, Matthieu and Than, Xuan Tinh and Tran, Huy Nam and Arenal, Raul and Rahmani, Abdelali and Boutahir, Mourad and Zahab, Ahmed-Azmi and Sauvajol, Jean-Louis},
	month = jan,
	year = {2014},
	note = {Publisher: Cambridge University Press},
	keywords = {C, nanoscale, Raman spectroscopy},
	pages = {69--77},
}



@article{rochal_two-dimensional_2013,
	title = {Two-dimensional elasticity determines the low-frequency dynamics of single- and double-walled carbon nanotubes},
	volume = {88},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.88.235435},
	doi = {10.1103/PhysRevB.88.235435},
	abstract = {We develop a continuous theory of low-frequency dynamics for nanotubes with walls constituted by single-atom monolayer, the topological elasticity of which is not related to its vanishing macroscopic thickness. The applicability region of the theory proposed includes all truly two-dimensional materials such as graphene and MoS2. New comprehensive interpretation and analytical expressions for low-frequency modes in single-walled carbon nanotube (SWCNT) are given. The theory unambiguously relates the radial breathing modes of SWCNT and breathinglike modes of the double-walled carbon nanotube (DWCNT). The existing Raman data on DWCNTs are fitted better than in the frame of previous models.},
	number = {23},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Rochal, S. B. and Lorman, V. L. and Yuzyuk, Yu. I.},
	month = dec,
	year = {2013},
	note = {Publisher: American Physical Society},
	pages = {235435},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\IBZ3DB87\\Rochal и др. - 2013 - Two-dimensional elasticity determines the low-freq.pdf:application/pdf},
}



@article{leontyeva_electrochemical_2013,
	title = {Electrochemical dispergation as a simple and effective technique toward preparation of {NiO} based nanocomposite for supercapacitor application},
	volume = {114},
	issn = {0013-4686},
	url = {https://www.sciencedirect.com/science/article/pii/S0013468613019725},
	doi = {10.1016/j.electacta.2013.10.031},
	abstract = {NiO/C nanocomposite was prepared directly by means a one-step electrochemical technique based on electrochemical dispergation of nickel by the alternating current. The prepared material was well characterized using different analytical techniques such as X-ray diffraction, Raman spectroscopy, scanning electron microscopy, and N2 adsorption/desorption. The X-ray diffraction and Raman scattering investigations of the freshly prepared sample confirmed the formation of β-NiO. The morphology of synthesized NiO/C can be described as dispersed on carbon support nano-leaves consisting of tightly packed array of nanoparticles (around 10nm in diam) with length of 500–2000nm and ∼20nm thick. NiO/C composite possesses high specific surface area of 137m2g−1 and a micro–meso–macroporous structure with a distribution of the pore size from 1 to 200nm. The electrochemical properties of the nanostructured NiO/C were investigated using cyclic voltammetry (CV) and galvanostatic charge-discharge tests. The synthesized NiO/C composite exhibited pseudo-capacitive behavior with the mass capacitance value as high as 1012Fg−1 and 750Fg−1 measured from CV and discharge curves, respectively. Compared with the theoretical specific capacitance of NiO 2573Fg−1, the degree of electrochemical utilization is 97\% for NiO in the synthesized NiO/C composite. The superior electrochemical performance is attributed to the hierarchically porous structure of the synthesized NiO/C, its with a high specific surface area as well as a wide pore size distribution. Considering the excellent performance and facile preparation, this NiO/C composite should have great potential for application in energy storage and conversion devices.},
	urldate = {2023-11-11},
	journal = {Electrochimica Acta},
	author = {Leontyeva, D. V. and Leontyev, I. N. and Avramenko, M. V. and Yuzyuk, Yu. I. and Kukushkina, Yu. A. and Smirnova, N. V.},
	month = dec,
	year = {2013},
	keywords = {Electrochemical capacitors, Nanoplatelets, Nanostructured materials, Nickel oxide},
	pages = {356--362},
}



@article{__2013,
	title = {{УФ} фотоприемник на основе наностержней и пленок оксида цинка},
	url = {http://www.ivdon.ru/magazine/archive/n4y2013/1883},
	abstract = {Сетевой научный журнал «Инженерный вестник Дона»},
	language = {ru},
	urldate = {2023-11-11},
	author = {Жилин, Д. А. and Лянгузов, Н. В. and Кайдашев, Е. М.},
	month = aug,
	year = {2013},
}



@article{__2013-1,
	title = {Импульсное лазерное напыление наноструктур},
	url = {http://www.ivdon.ru/magazine/archive/n4y2013/1885},
	abstract = {Сетевой научный журнал «Инженерный вестник Дона»},
	language = {ru},
	urldate = {2023-11-11},
	author = {Несветаев, Д. Г. and Кайдашев, Е. М. and Пузиков, А. С.},
	month = aug,
	year = {2013},
}



@article{konevtsova_unconventional_2013,
	title = {Unconventional {Landau} theory of quasicrystalline structure formation},
	volume = {377},
	issn = {0375-9601},
	url = {https://www.sciencedirect.com/science/article/pii/S0375960113002417},
	doi = {10.1016/j.physleta.2013.03.006},
	abstract = {We propose an unconventional theory which unifies the description of quasicrystal thermodynamics and quasicrystal structure formation by combining the Landau theory of crystallization and the cluster approach to quasicrystals. The theory is illustrated on the example of pentagonal Penrose quasilattice. It employs the notion of non-linear order parameter dependent on the atomic coordinates which was developed in the theory of reconstructive phase transitions. The coordinates of the quasilattice nodes are calculated by minimizing the Landau free energy with the constraint imposed by internal organization of clusters. The correspondence is shown between the theory proposed and the conventional projection method.},
	number = {16},
	urldate = {2023-11-11},
	journal = {Physics Letters A},
	author = {Konevtsova, O. V. and Rochal, S. B. and Lorman, V. L.},
	month = jul,
	year = {2013},
	keywords = {Cluster approach, Constrained minimization, Landau crystallization theory, Non-linear order parameter, Quasicrystal},
	pages = {1215--1220},
}



@article{gorshunov_quantum_2013,
	title = {Quantum {Behavior} of {Water} {Molecules} {Confined} to {Nanocavities} in {Gemstones}},
	volume = {4},
	url = {https://doi.org/10.1021/jz400782j},
	doi = {10.1021/jz400782j},
	abstract = {When water is confined to nanocavities, its quantum mechanical behavior can be revealed by terahertz spectroscopy. We place H2O molecules in the nanopores of a beryl crystal lattice and observe a rich and highly anisotropic set of absorption lines in the terahertz spectral range. Two bands can be identified, which originate from translational and librational motions of the water molecule isolated within the cage; they correspond to the analogous broad bands in liquid water and ice. In the present case of well-defined and highly symmetric nanocavities, the observed fine structure can be explained by macroscopic tunneling of the H2O molecules within a six-fold potential caused by the interaction of the molecule with the cavity walls.},
	number = {12},
	urldate = {2023-11-11},
	journal = {The Journal of Physical Chemistry Letters},
	author = {Gorshunov, Boris P. and Zhukova, Elena S. and Torgashev, Victor I. and Lebedev, Vladimir V. and Shakurov, Gil’man S. and Kremer, Reinhard K. and Pestrjakov, Efim V. and Thomas, Victor G. and Fursenko, Dimitry A. and Dressel, Martin},
	month = jun,
	year = {2013},
	note = {Publisher: American Chemical Society},
	pages = {2015--2020},
}



@article{__2013-2,
	title = {Электронные методы структурного анализа индивидуальных углеродных нанотрубок},
	url = {http://www.ivdon.ru/magazine/archive/n4y2013/2006},
	abstract = {Сетевой научный журнал «Инженерный вестник Дона»},
	language = {ru},
	urldate = {2023-11-11},
	author = {Левшов, Д. И. and Авраменко, М. В.},
	month = jun,
	year = {2013},
}



@article{__2013-3,
	title = {Топологические дефекты в двумерных сферических кристаллах},
	url = {http://www.ivdon.ru/magazine/archive/n3y2013/1844},
	abstract = {Сетевой научный журнал «Инженерный вестник Дона»},
	language = {ru},
	urldate = {2023-11-11},
	author = {Петров, К. Ю. and Шевченко, И. А.},
	month = apr,
	year = {2013},
}



@article{avramenko_symmetry_2013,
	title = {Symmetry of the carbon nanotube modes and their origin from the phonon branches of graphene},
	volume = {87},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.87.035407},
	doi = {10.1103/PhysRevB.87.035407},
	abstract = {A group-theory method to relate the spectra of tubular and parent planar structures is elaborated. The spectra correlation is obtained using a virtual intermediate planar periodic structure, which has a local symmetry coinciding with that of the tube surface. The method is applied to deduce the zone-center phonon modes of carbon nanotubes from the dispersion branches of the graphene monolayer. The results obtained open an additional way for experimental indexing of the carbon nanotubes by means of Raman spectroscopy, and the origin of the Raman-active modes in the achiral nanotubes is determined. We demonstrate that the number of modes in the G band and the relation between their frequencies are governed by the nanotube type. The proposed theory can be easily explored to understand the phonon and electron spectra of many other tubular structures (boron nitride, transition metal dichalcogenides) which have emerged in the past decade.},
	number = {3},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Avramenko, M. V. and Rochal, S. B. and Yuzyuk, Yu. I.},
	month = jan,
	year = {2013},
	note = {Publisher: American Physical Society},
	pages = {035407},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\S37AE8AD\\Avramenko и др. - 2013 - Symmetry of the carbon nanotube modes and their or.pdf:application/pdf},
}



@article{razumnaya_resistive_2013,
	title = {Resistive {Switching} {Hysteresis} in {Thin} {Films} of {Bismuth} {Ferrite}},
	volume = {444},
	issn = {0015-0193},
	url = {https://doi.org/10.1080/00150193.2013.790759},
	doi = {10.1080/00150193.2013.790759},
	abstract = {We have studied the resistive switching (RS) phenomenon in series of BiFeO3 thin films of thickness of 40 – 154 nm deposited by PLD technique on conducting Nb-doped substrate of SrTiO3 and with Pt top electrodes. It was found that 154 nm film demonstrates the interface-provided I–V characteristic of Schottky diode when the applied voltage does not exceed the threshold value Vd = 1.3 V. The RS phenomenon appears as the current hysteresis loop during the 0 → Vm → 0 → −Vm → 0 voltage sweep cycle, provided that the maximal stop-voltage Vm is larger than Vd. For thinner films neither diode-like I–V behavior nor substantial RS effect were observed. The results are interpreted in terms of the filamentary model of the mobile oxygen vacancies.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Ferroelectrics},
	author = {Razumnaya, A. and Gagou, Y. and Bouyanfif, H. and Carcan, B. and Allouche, B. and Wolfman, J. and Autret-Lambert, C. and Marssi, M. El and Mezzane, D. and Luk'yanchuk, I.},
	month = jan,
	year = {2013},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/00150193.2013.790759},
	keywords = {multiferroics, oxides, Resistive switching, thin films},
	pages = {183--189},
}



@article{akbaeva_phase_2013,
	title = {Phase {States} in {Multicomponent} {PZT}-{Based} {Materials} {Depending} on {Poling} {Conditions}},
	volume = {443},
	issn = {0015-0193},
	url = {https://doi.org/10.1080/00150193.2013.778616},
	doi = {10.1080/00150193.2013.778616},
	abstract = {Phase states of the PZT-based multicomponent solid solutions belonging to the rhombohedral area of the phase х-Т diagram with low coercive field values are considered. The solid-solution samples in the initial state are proved to be heterophase (R3c and P4mm mixtures) and reveal relaxor properties. The anomalies of dielectric characteristics obtained in poled samples are due to the R3c→R3m phase transition. The manifestations of relaxor properties above the temperature of the dielectric permittivity maximum are caused by the R3m phase in the P4mm and Pm3m phase mixture.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Ferroelectrics},
	author = {Akbaeva, G. M. and Kabirov, Yu. V. and Milov, E. V. and Gavrilyachenko, V. G.},
	month = jan,
	year = {2013},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/00150193.2013.778616},
	keywords = {phase transition, X-ray diffraction, Phase state, poling condition},
	pages = {57--62},
}



@article{levshov_comparative_2013,
	title = {Comparative {Raman} {Study} of {Individual} {Double}-{Walled} {Carbon} {Nanotubes} and {Single}-{Walled} {Carbon} {Nanotubes}},
	volume = {8},
	doi = {10.1166/jno.2013.1423},
	abstract = {In this paper, we compare the Raman responses obtained on individual suspended Single-Walled Carbon Nanotubes (SWNTs) and Double-Walled Carbon Nanotubes (DWNTs). We focus on the comparison of the frequencies, line widths, intensities and resonance conditions of the main Raman active
modes measured on an index-identified DWNT with those measured on SWNTs having atomic structures close to the inner and outer tubes of the DWNT. By this way, we state that the relation between the radial breathing mode frequencies and the diameters established for SWNTs do not work in DWNTs.
We found that resonance of only one tube can be sufficient to observe the response of the coupled layers in DWNTs. These results are understood in terms of mechanical coupling between the layers in DWNTs. We evidence that the spectral line widths of the Raman active modes are systematically
narrower for DWNTs compared to the corresponding SWNTs. Finally, we present the measurements of the G modes of two different DWNTs which behave in a different way. For the first one, the frequencies of the G modes are not significantly affected by the interaction between the
layers, while for the second one we evidence a downward shift of the LO and TO bands arising from the inner layer.},
	number = {1},
	journal = {Journal of Nanoelectronics and Optoelectronics},
	author = {Levshov, D. and Michel, T. and Than, T. and Paillet, M. and Arenal, R. and Jourdain, V. and Yuzyuk, Yu. I. and Sauvajol, J.-L.},
	month = jan,
	year = {2013},
	keywords = {ELECTRON DIFFRACTION, INDIVIDUAL DOUBLE-WALLED CARBON NANOTUBES, INDIVIDUAL SINGLE-WALLED CARBON NANOTUBES, RAMAN SPECTROSCOPY},
	pages = {9--15},
}



@inproceedings{__2013-4,
	title = {Структурные и электрокаталитические свойства катализаторов {Pt}/{C} и {Pt}–{Ni}/{C}, полученных методом электрохимического диспергирования},
	volume = {54},
	url = {http://www.maikonline.com/maik/showArticle.do?auid=VAHEB686WM&lang=ru},
	doi = {10.7868/S0453881113020147},
	abstract = {Semantic Scholar extracted view of "Структурные и электрокаталитические свойства катализаторов Pt/C и Pt–Ni/C, полученных методом электрохимического диспергирования" by Наталья Владимировна Смирнова et al.},
	language = {ru},
	urldate = {2023-11-11},
	booktitle = {Кинетика и катализ},
	author = {Смирнова, Н. В. and Куриганова, А. Б. and Леонтьева, Д. В. and Леонтьев, И. Н. and Михейкин, А. С.},
	year = {2013},
	note = {ISSN: 0453-8811
Issue: 2
Journal Abbreviation: Кинет. и катал.},
	pages = {265--272},
}



@article{__2013-5,
	title = {Синтез и свойства метаматериалов со структурой оболочка-ядро},
	issn = {2073-2562},
	url = {https://elibrary.ru/item.asp?id=18944350},
	abstract = {Синтезированы поликристаллические и керамические композитные материалы (КМ) Pt ( PbZrO 3 ) и CaCu 3 Ti 4 O 12 ( SrFe 12 O 19 ), архитектурно представляющие собой структуру оболочка—ядро. В первых из них обнаружен парамагнетизм, обусловленный появлением парамагнитных центров при взаимодействии атомов платины и матрицы. Композитная керамика на основе гексаферрита стронция SrFe 12 O 19, структурированная по типу оболочка—ядро материалом с колоссальным значением диэлектрической проницаемости CaCu 3 Ti 4 O 12, приготовлена с использованием традиционной керамической технологии. Приведены результаты электронно-микроскопических и электрофизических исследований объектов},
	language = {ru},
	number = {2 (130)},
	urldate = {2023-11-11},
	journal = {Конструкции Из Композиционных Материалов},
	author = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Гутерман, В. Е. and Залетов, В. Г. and Сидоренко, Е. Н. and Лянгузов, Н. В. and Панченко, Е. М.},
	year = {2013},
	keywords = {Гексаферрит Стронция, Композиты, Метаматериалы},
	pages = {37--42},
}



@article{mikheykin_compressibility_2012,
	title = {The compressibility of nanocrystalline {Pt}},
	volume = {101},
	issn = {0003-6951},
	url = {https://doi.org/10.1063/1.4758000},
	doi = {10.1063/1.4758000},
	abstract = {High-pressure behavior of carbon supported Pt nanoparticles (Pt/C) with an average particle size of 10.6 nm was investigated by in situ high-pressure synchrotron radiation x-ray diffraction up to 14 GPa at ambient temperature. Our results show that the compressibility of Pt/C nanoparticles decreases substantially as the particle size decreases. An interpretation based upon the available mechanisms of structural compliance in nanoscale vs bulk materials was proposed.},
	number = {17},
	urldate = {2023-11-11},
	journal = {Applied Physics Letters},
	author = {Mikheykin, A. S. and Dmitriev, V. P. and Chagovets, S. V. and Kuriganova, A. B. and Smirnova, N. V. and Leontyev, I. N.},
	month = oct,
	year = {2012},
	pages = {173111},
}



@article{__2012,
	title = {Исследование наностержней оксида цинка методом фотолюминесценции для оптимизации характеристик чувствительного элемента ПАВ сенсора},
	url = {http://ivdon.ru/magazine/archive/n4p1y2012/1178},
	abstract = {Сетевой научный журнал «Инженерный вестник Дона»},
	language = {ru},
	urldate = {2023-11-11},
	author = {Несветаев, Д. Г. and Лянгузов, Н. В. and Николаев, А. Л. and Кайдашев, Е. М.},
	month = aug,
	year = {2012},
}



@article{leontyev_new_2012,
	title = {New life of a forgotten method: {Electrochemical} route toward highly efficient {Pt}/{C} catalysts for low-temperature fuel cells},
	volume = {431-432},
	issn = {0926-860X},
	shorttitle = {New life of a forgotten method},
	url = {https://www.sciencedirect.com/science/article/pii/S0926860X12002268},
	doi = {10.1016/j.apcata.2012.04.025},
	abstract = {Driven by global environmental concerns, great efforts are currently made to develop novel, cheap and practical means for producing highly efficient electrocatalysts, specifically for the low-temperature fuel-cell applications. Employing an old but yet unexplored method based on electrochemical dispergation of platinum by the alternating current, we show that the freshly prepared Pt/C catalysts exhibit greatly enhanced catalytic activity (up to 350\% for oxygen reduction and up to 200\% for ethylene glycol oxidation) as compared with that of a commercially available counterpart (E-TEK). A key role in these reactions is attributed to a specific nanoparticle morphology. These findings should provide a revival of an ancient but simple and efficient electrochemical process and motivate further researches in the field.},
	urldate = {2023-11-11},
	journal = {Applied Catalysis A: General},
	author = {Leontyev, Igor and Kuriganova, Aleksandra and Kudryavtsev, Yuri and Dkhil, Brahim and Smirnova, Nina},
	month = jul,
	year = {2012},
	keywords = {Electrocatalysis, Oxygen reduction reaction (ORR), X-ray diffraction (XRD), Low-temperature fuel cell, Platinum nanoparticles, Shape},
	pages = {120--125},
}



@article{__2012-1,
	title = {Исследование влияния адсорбции моноокиси углерода на характеристики линии задержки на ПАВ с чувствительным элементом из наностержней оксида цинка},
	url = {http://ivdon.ru/ru/magazine/archive/n4p1y2012/1189},
	abstract = {Сетевой научный журнал «Инженерный вестник Дона»},
	language = {ru},
	urldate = {2023-11-11},
	author = {Карапетьян, Г. Я. and Николаев, А. Л. and Лянгузов, Н. В. and Несветаев, Д. Г. and Кайдашев, Е. М.},
	month = jul,
	year = {2012},
}



@article{timoshenko_diffraction_2012,
	title = {Diffraction of surface magnetostatic waves by surface cavities on ferromagnetic film},
	volume = {57},
	issn = {1555-6557},
	url = {https://doi.org/10.1134/S1064226912060137},
	doi = {10.1134/S1064226912060137},
	abstract = {The diffraction problem of the scattering of surface magnetostatic waves by shallow rectangular and circular cavities on the surface of a ferromagnetic film that is tangentially magnetized with respect to the surface is numerically analyzed in the magnetostatic approximation.},
	language = {en},
	number = {7},
	urldate = {2023-11-11},
	journal = {Journal of Communications Technology and Electronics},
	author = {Timoshenko, P. E. and Ivanov, V. N. and Babichev, R. K. and Shloma, A. V.},
	month = jul,
	year = {2012},
	keywords = {Circular Cavity, Lower Lobe, Rectangular Cavity, Reflection Coefficient, Surface Cavity},
	pages = {726--733},
}



@article{manukyan_nickel_2012,
	title = {Nickel nanoparticles in carbon structures prepared by solid-phase pyrolysis of nickel-phthalocyanine},
	volume = {14},
	issn = {1572-896X},
	url = {https://doi.org/10.1007/s11051-012-0982-6},
	doi = {10.1007/s11051-012-0982-6},
	abstract = {By using a modified method of solid-phase pyrolysis of metal-phthalocyanines, we have synthesized ferromagnetic Ni nanoparticles in different carbon structures: amorphous carbon plates, multiwall carbon nanotubes, carbon fibers, and graphitized capsules. The composition, structure and morphology of prepared composite materials have been studied by energy dispersive X-ray microanalysis, scanning and transmission electron microscopy, and X-ray diffraction technique. It has been found that the sizes of nickel nanoparticles (10–500 nm) and the type of carbon structures strongly depend on the pyrolysis conditions. By using the X-band ferromagnetic resonance measurements, we have revealed features of the temperature dependence of resonance spectra of single-domain and multi-domain Ni nanoparticles in Ni/C composites.},
	language = {en},
	number = {7},
	urldate = {2023-11-11},
	journal = {Journal of Nanoparticle Research},
	author = {Manukyan, A. S. and Mirzakhanyan, A. A. and Badalyan, G. R. and Shirinyan, G. H. and Fedorenko, A. G. and Lianguzov, N. V. and Yuzyuk, Yu I. and Bugaev, L. A. and Sharoyan, E. G.},
	month = jun,
	year = {2012},
	keywords = {Carbon nanostructures, Magnetic properties, Nickel nanoparticles, Nickel-phthalocyanine, Solid-phase pyrolysis},
	pages = {982},
}



@article{__2012-2,
	title = {Пассивный беспроводный датчик на поверхностных акустических волнах для измерения параметров газовых и жидких сред},
	url = {http://ivdon.ru/magazine/archive/n2y2012/770},
	abstract = {Сетевой научный журнал «Инженерный вестник Дона»},
	language = {ru},
	urldate = {2023-11-11},
	author = {Карапетьян, Г. Я. and Днепровский, В. Г. and Багдасарян, А. С. and Багдасарян, С. А. and Николаев, А. Л. and Кайдашев, Е. М.},
	month = mar,
	year = {2012},
}



@article{__2012-3,
	title = {Тригональная хиральная и гексагональная двумерные квазикристаллические укладки},
	url = {http://ivdon.ru/magazine/archive/n2y2012/816},
	abstract = {Сетевой научный журнал «Инженерный вестник Дона»},
	language = {ru},
	urldate = {2023-11-11},
	author = {Рошаль, Д. С. and Рошаль, С. Б.},
	month = jan,
	year = {2012},
}



@article{konevtsova_chiral_2012,
	title = {Chiral {Quasicrystalline} {Order} and {Dodecahedral} {Geometry} in {Exceptional} {Families} of {Viruses}},
	volume = {108},
	url = {https://link.aps.org/doi/10.1103/PhysRevLett.108.038102},
	doi = {10.1103/PhysRevLett.108.038102},
	abstract = {On the example of exceptional families of viruses we (i) show the existence of a completely new type of matter organization in nanoparticles, in which the regions with a chiral pentagonal quasicrystalline order of protein positions are arranged in a structure commensurate with the spherical topology and dodecahedral geometry, (ii) generalize the classical theory of quasicrystals (QCs) to explain this organization, and (iii) establish the relation between local chiral QC order and nonzero curvature of the dodecahedral capsid faces.},
	number = {3},
	urldate = {2023-11-11},
	journal = {Physical Review Letters},
	author = {Konevtsova, O. V. and Rochal, S. B. and Lorman, V. L.},
	month = jan,
	year = {2012},
	note = {Publisher: American Physical Society},
	pages = {038102},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\T2BMSVJV\\Konevtsova и др. - 2012 - Chiral Quasicrystalline Order and Dodecahedral Geo.pdf:application/pdf},
}



@article{firsova_femtosecond_2012,
	title = {Femtosecond {Infrared} {Laser} {Annealing} of {PZT} {Films} on a {Metal} {Substrate}},
	volume = {433},
	issn = {0015-0193},
	url = {https://doi.org/10.1080/00150193.2012.696459},
	doi = {10.1080/00150193.2012.696459},
	abstract = {The quazi-amorphous PbZrTiO2 (PZT) precursor film on a platinized silicon substrate is annealed by femtosecond laser at the wavelength falling into transparency band of PZT. Two areas are found within the laser spot: ferroelectric perovskite revealing strong hysteresis and coercivity in piezoelectric response and paraelectric with low piezoresponse and the absence of hysteresis and coercivity. Annealing takes place through platinum absorbing laser irradiation and acting as a heat source for transparent film on top of it.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Ferroelectrics},
	author = {Firsova, N. Yu. and Mishina, E. D. and Sigov, A. S. and Senkevich, S. V. and Pronin, I. P. and Kholkin, A. and Bdikin, I. and Yuzyuk, Yu. I.},
	month = jan,
	year = {2012},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/00150193.2012.696459},
	keywords = {thin films, Raman scattering, ferroelectric, femtosecond laser annealing, piezoelectric, second harmonic generation, Sol-gel},
	pages = {164--169},
}



@article{maslova_diagnostics_2012,
	title = {Diagnostics of {Carbonaceous} {Nanomaterial} “{Taunit}” by {Raman} {Spectroscopy}},
	volume = {7},
	doi = {10.1166/jno.2012.1225},
	abstract = {Crystalline structure perfection of carbonaceous nanomaterial (CNM) “Taunit” which constitutes the multi-walled nanotubes was studied using a Raman spectroscopy technique. CNM “Taunit” was synthesized by MOCVD method. The pristine material, the samples annealed
at different temperatures and the samples functionalized by Pt-catalyst nanoparticles were investigated. It has been found that “Taunit” belongs to the poorly organized carbon materials but its crystalline structure was observed to order while the annealing temperature increased.
D1 and G Raman band (at 1350 and 1580 cm–1, respectively) intensity ratios were calculated to estimate the crystal structure ordering of CNM “Taunit”. The investigation of the influence of functionalization by the catalyst nanoparticles shows that Pt-catalyst
precipitation on the surface of MWNTs leads to the increase of the defect band intensity due to an appearance of lattice defects.},
	number = {1},
	journal = {Journal of Nanoelectronics and Optoelectronics},
	author = {Maslova, O. A. and Mikheykin, A. S. and Leontiev, I. N. and Yuzyuk, Yu. I. and Tkachev, A. G.},
	month = jan,
	year = {2012},
	keywords = {RAMAN SPECTROSCOPY, CRYSTALLINE STRUCTURE ORDERING, D- AND G-BAND INTENSITIES RATIOS, MULTI-WALLED CARBON NANOTUBES, PT-CATALYST NANOPARTICLES},
	pages = {95--98},
}



@article{levshov_raman_2012,
	title = {Raman {Study} of {Uniaxial} {Strain} in {Individual} {Single}-{Wall} {Carbon} {Nanotubes} {Induced} by {Temperature} {Changes}},
	volume = {7},
	doi = {10.1166/jno.2012.1221},
	abstract = {We report the temperature dependence of the Raman spectra of a gelatine-based composite material doped with single-walled carbon nanotubes (SWNT@gelatin). On decreasing the temperature from 290 to 20 K a significant up-shift of the G-mode and no changes in the radial breathing modes
are observed. This behaviour cannot be understood by pure thermal effects. We explain these results in terms of an uniaxial strain of the nanotubes induced by the thermal expansion mismatch between the nanotubes and the surrounding matrix.},
	number = {1},
	journal = {Journal of Nanoelectronics and Optoelectronics},
	author = {Levshov, D. I. and Yuzyuk, Yu. I. and Michel, T. and Voisin, C. and Alvarez, L. and Berger, S. and Roussignol, P. and Sauvajol, J.-L.},
	month = jan,
	year = {2012},
	keywords = {RAMAN SPECTROSCOPY, COMPOSITES, SINGLE-WALLED CARBON NANOTUBES, UNIAXIAL STRAIN},
	pages = {77--80},
}



@article{ivanov_enhanced_2012,
	title = {Enhanced {Magnetization} and {Ferroelectric} {Switching} in {Multiferroic} {BST}/{BNFO} {Superstructures}},
	volume = {433},
	issn = {0015-0193},
	url = {https://doi.org/10.1080/00150193.2012.696448},
	doi = {10.1080/00150193.2012.696448},
	abstract = {Multiferroic BaSrTiO3/NdBiFeO3 (BST/BNFO) mulilayers with 3 nm and 6 nm layer thickness demonstrate superlattice structure in the XRD patterns. The break of the spin cycloide and interface strain results in ferromagnetic behavior and enhancement of magnetization. The total thickness of BNFO is varied in the range of 50–60 nm, and saturation magnetization is varied in the range of 50-60 emu/cm3, which is an order of magnitude higher than reported for BaTiO3/BiFeO3 superstructure [1]. Polarization hysteresis loop were obtained by second harmonic generation technique and show significant electro-optical switchability. Both magnetization and ferroelectric polarization possess bulk rather than interface localization.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Ferroelectrics},
	author = {Ivanov, M. S. and Sherstyuk, N. E. and Mishina, E. D. and Sigov, A. S. and Mukhortov, V. M. and Moshnyaga, V. T.},
	month = jan,
	year = {2012},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/00150193.2012.696448},
	keywords = {thin films, superlattice, polarization, Multiferroic, second harmonic generation, magnetization},
	pages = {158--163},
}



@article{__2011,
	title = {Селективный рост массивов наностержней гидротермальным методом на кремнии},
	url = {http://ivdon.ru/magazine/archive/n1y2012/684},
	abstract = {Сетевой научный журнал «Инженерный вестник Дона»},
	language = {ru},
	urldate = {2023-11-11},
	author = {Ступко, М. Ю. and Лянгузов, Н. В. and Николаев, А. Л. and Кайдашев, Е. М.},
	month = dec,
	year = {2011},
}



@article{__2011-1,
	title = {Исследование роста наностержней в методике карботермического синтеза на тонкопленочных подслоях},
	url = {http://ivdon.ru/magazine/archive/n1y2012/683/},
	abstract = {Сетевой научный журнал «Инженерный вестник Дона»},
	language = {ru},
	urldate = {2023-11-11},
	author = {Лянгузов, Н. В.},
	month = dec,
	year = {2011},
}



@misc{noauthor_notitle_nodate,
	url = {http://www.maikonline.com/maik/showArticle.do?auid=VAH1QBBBMQ},
	urldate = {2023-11-11},
	file = {maikonline.com/maik/showArticle.do?auid=VAH1QBBBMQ:C\:\\Users\\aleks\\Zotero\\storage\\APT4EU54\\showArticle.html:text/html},
}



@misc{noauthor_notitle_nodate-1,
	url = {http://www.maikonline.com/maik/showArticle.do?auid=VAH4QS914Q&lang=ru},
	urldate = {2023-11-11},
	file = {maikonline.com/maik/showArticle.do?auid=VAH4QS914Q&lang=ru:C\:\\Users\\aleks\\Zotero\\storage\\ZC6HN8U9\\showArticle.html:text/html},
}



@misc{noauthor_notitle_nodate-2,
	url = {http://www.maikonline.com/maik/showArticle.do?auid=VAGWQ43GB0&lang=ru},
	urldate = {2023-11-11},
	file = {maikonline.com/maik/showArticle.do?auid=VAGWQ43GB0&lang=ru:C\:\\Users\\aleks\\Zotero\\storage\\22TTF2JJ\\showArticle.html:text/html},
}



@misc{noauthor_notitle_nodate-3,
	url = {http://www.maikonline.com/maik/showArticle.do?auid=VAGZTLODNH},
	urldate = {2023-11-11},
	file = {maikonline.com/maik/showArticle.do?auid=VAGZTLODNH:C\:\\Users\\aleks\\Zotero\\storage\\9FI6SVHU\\showArticle.html:text/html},
}



@inproceedings{mirzakhanyan_raman_2011,
	title = {Raman spectra of nickel-carbon nanocomposites},
	volume = {7998},
	url = {https://www.spiedigitallibrary.org/conference-proceedings-of-spie/7998/79981B/Raman-spectra-of-nickel-carbon-nanocomposites/10.1117/12.890940.full},
	doi = {10.1117/12.890940},
	abstract = {By using the solid-phase pyrolysis of phthalocyanines the nickel-carbon nanocomposites have been synthesized. The composition, structure, and morphology of samples were investigated by scanning electron microscopy and Raman spectroscopy. The first-order Raman shifts of prepared materials were measured with laser excitation at 514.5 nm in the frequency range from 900 to 2000 cm$^{\textrm{-1}}$. It is shown that the degree of graphitization in nanocomposites essentially depends on the pyrolysis temperature. By analyzing the intensity ratio of Raman D- and G-bands the mean sizes of graphitic nanocrystallites in prepared samples were estimated.},
	urldate = {2023-11-11},
	booktitle = {International {Conference} on {Laser} {Physics} 2010},
	publisher = {SPIE},
	author = {Mirzakhanyan, Armen A. and Manukyan, Aram S. and Badalyan, George R. and Khachatryan, Tatevik K. and Maslova, Olga A. and Yuzyuk, Yurii I. and Bugaev, Lusegen A. and Sharoyan, Eduard G.},
	month = mar,
	year = {2011},
	pages = {346--349},
}



@article{levshov_experimental_2011,
	title = {Experimental {Evidence} of a {Mechanical} {Coupling} between {Layers} in an {Individual} {Double}-{Walled} {Carbon} {Nanotube}},
	volume = {11},
	issn = {1530-6984},
	url = {https://doi.org/10.1021/nl2026234},
	doi = {10.1021/nl2026234},
	abstract = {We perform transmission electron microscopy, electron diffraction, and Raman scattering experiments on an individual suspended double-walled carbon nanotube (DWCNT). The first two techniques allow the unambiguous determination of the DWCNT structure: (12,8)@(16,14). However, the low-frequency features in the Raman spectra cannot be connected to the derived layer diameters d by means of the 1/d power law, widely used for the diameter dependence of the radial-breathing mode of single-walled nanotubes. We discuss this disagreement in terms of mechanical coupling between the layers of the DWCNT, which results in collective vibrational modes. Theoretical predictions for the breathing-like modes of the DWCNT, originating from the radial-breathing modes of the layers, are in a very good agreement with the observed Raman spectra. Moreover, the mechanical coupling qualitatively explains the observation of Raman lines of breathing-like modes, whenever only one of the layers is in resonance with the laser energy.},
	number = {11},
	urldate = {2023-11-11},
	journal = {Nano Letters},
	author = {Levshov, D. and Than, T. X. and Arenal, R. and Popov, V. N. and Parret, R. and Paillet, M. and Jourdain, V. and Zahab, A. A. and Michel, T. and Yuzyuk, Yu. I. and Sauvajol, J.-L.},
	month = nov,
	year = {2011},
	note = {Publisher: American Chemical Society},
	pages = {4800--4804},
}



@article{leontyev_catalytic_2011,
	title = {Catalytic {Activity} of {Carbon}-{Supported} {Pt} {Nanoelectrocatalysts}. {Why} {Reducing} the {Size} of {Pt} {Nanoparticles} is {Not} {Always} {Beneficial}},
	volume = {115},
	issn = {1932-7447},
	url = {https://doi.org/10.1021/jp1109477},
	doi = {10.1021/jp1109477},
	abstract = {Carbon-supported Pt catalysts prepared by the impregnation method in water−dimethyl sulfoxide (DMSO) solutions were investigated. Using X-ray diffraction (XRD) technique for estimation of the particle size and shapes, we show that morphology of the Pt/C catalysts depends strongly on the DMSO content in the solutions. The average particles size reduces and a shape of the Pt nanocrystals changes from a truncated octahedron to a cuboctahedron and eventually to a truncated cube with increasing DMSO concentration in the reaction mixture. Antibate effects of the size and shape cause nonmonotonic dependence of the catalytic activity for the oxygen reduction reaction (ORR) with electric current maximum at an average particle size of 2.7 nm.},
	number = {13},
	urldate = {2023-11-11},
	journal = {The Journal of Physical Chemistry C},
	author = {Leontyev, I. N. and Belenov, S. V. and Guterman, V. E. and Haghi-Ashtiani, P. and Shaganov, A. P. and Dkhil, B.},
	month = apr,
	year = {2011},
	note = {Publisher: American Chemical Society},
	pages = {5429--5434},
}



@article{__2011-2,
	title = {Наноразмерные сегнетоэлектрические пленки {Ba}$_{\textrm{0.8}}${Sr}$_{\textrm{0.2}}${TiO}$_{\textrm{3}}$ на подложках {MgO}},
	volume = {12},
	issn = {1999-8465},
	url = {https://www.elibrary.ru/item.asp?id=16220258},
	abstract = {Методом просвечивающей электронной микроскопии высокого разрешения проведены исследования и анализ дефектной микроструктуры монокристаллических сегнетоэлектрических наноразмерных пленок Ba0.8Sr0.2TiO3, выращенных методом магнетронного распыления мишени на подложках MgO. Выявлено в пленке наличие дислокаций с векторами Бюргерса {\textless}100{\textgreater}и 1/2{\textless}110{\textgreater} и границы блоков.},
	language = {ru},
	number = {5},
	urldate = {2023-11-11},
	journal = {Наукоемкие Технологии},
	author = {Жигалина, О. М. and Мухортов, В. М. and Головко, Ю. И. and Чувилин, A. Л. and Кускова, А. Н.},
	year = {2011},
	keywords = {Тонкие Сегнетоэлектрические Пленки, Электронная Микроскопия Высокого Разрешения},
	pages = {23--25},
}



@article{ishioka_coherent_2010,
	title = {Coherent optical phonons of {ZnO} under near resonant photoexcitation},
	volume = {22},
	issn = {0953-8984},
	url = {https://dx.doi.org/10.1088/0953-8984/22/46/465803},
	doi = {10.1088/0953-8984/22/46/465803},
	abstract = {Ultrafast electron–phonon coupling dynamics in ZnO are investigated by degenerate pump–probe reflectivity measurements using near resonant 400 nm light. Because of the below-gap excitation, photocarriers are excited primarily from deep levels of intrinsic point defects. At least six coherent phonon modes, including two E2 modes and their combination, longitudinal optical (LO) mode and its overtone (2LO), are observed. Unlike the previous resonant Raman studies using 325 nm light, the intensity of the polar LO phonons is only moderately enhanced by the Fröhlich interaction. The non-polar E2 phonons decay considerably faster than under visible excitation, indicative of strong deformation potential interaction with photocarriers. The overdamped oscillation centered at around 20 THz is tentatively attributed to the upper branch of the plasmon–phonon coupled mode. The pump-polarization dependence of the phonon amplitudes is consistent with the impulsive Raman generation.},
	language = {en},
	number = {46},
	urldate = {2023-11-11},
	journal = {Journal of Physics: Condensed Matter},
	author = {Ishioka, K. and Petek, H. and Kaydashev, V. E. and Kaidashev, E. M. and Misochko, O. V.},
	month = nov,
	year = {2010},
	pages = {465803},
}



@article{monnier_long-range_2010,
	title = {Long-{Range} {Protein} {Coupling} {Mediated} by {Critical} {Low}-{Energy} {Modes} of {Tubular} {Lipid} {Membranes}},
	volume = {105},
	url = {https://link.aps.org/doi/10.1103/PhysRevLett.105.028102},
	doi = {10.1103/PhysRevLett.105.028102},
	abstract = {We develop a theory of a resonant effect in protein-membrane coupling taking place in the vicinity of instabilities in tubular lipid membranes (TLMs) under longitudinal force and pressure difference constraints. Two critical low-energy modes defining the stability domain boundaries are found. We show that these modes mediate long-range TLM-protein coupling and interactions between absorbed proteins. Besides, TLM mechanical instabilities strongly influence protein desorption and protein cluster nucleation on TLMs. Model predictions can be tested over a large spectrum of mechanochemical conditions.},
	number = {2},
	urldate = {2023-11-11},
	journal = {Physical Review Letters},
	author = {Monnier, Sylvain and Rochal, Sergei B. and Parmeggiani, Andrea and Lorman, Vladimir L.},
	month = jul,
	year = {2010},
	note = {Publisher: American Physical Society},
	pages = {028102},
	file = {APS Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\22HMBNIH\\PhysRevLett.105.html:text/html},
}



@article{__2010,
	title = {Спектры комбинационного рассеяния углеродного наноматериала "Таунит"},
	volume = {5},
	issn = {1992-7223, 1993-4068},
	url = {https://www.elibrary.ru/item.asp?id=15271362},
	abstract = {Изучены спектры комбинационного рассеяния света (КРС) образцов углеродного наноматериала (УНМ) «Таунит», отожженных при различных температурах. Кроме того, исследовалось влияние наночастиц катализатора Pt с размерами 3-6 нм на спектры КРС УНМ «Таунит». Было обнаружено, что «Таунит» относится к углеродным материалам с нарушенной степенью организации, однако с ростом температуры отжига наблюдалось упорядочение его кристаллической структуры. Показано, что осаждение частиц платинового катализатора на поверхность УНМ «Таунит» приводит к увеличению интенсивности дефектной полосы в спектрах КРС из-за появления некоторого количества дефектов кристаллической решеткиRaman spectra of carbonaceous nanomaterial (CNM) «Taunit» samples annealed at different temperatures were studied. Also influence Pt-catalyst nanoparticles with the size distribution 3-6 nm on the Raman spectra of CNM «Taunit» was studied. It was found that «Taunit» belonged to poorly organized CNM but the its crystalline structure ordering was observed with increasing of annealing temperature. It is shown that Pt-catalyst precipitation on the surface of CNM «Taunit» leads to increasing of the defect band intensity due to appearance of some crystal lattice defects.},
	language = {ru},
	number = {9-10},
	urldate = {2023-11-11},
	journal = {Российские Нанотехнологии},
	author = {Маслова, О. А. and Михейкин, А. С. and Леонтьев, И. Н. and Юзюк, Ю. И. and Ткачев, А. Г.},
	year = {2010},
	pages = {89--93},
}



@article{leontyev_xrd_2010,
	title = {{XRD} and electrochemical investigation of particle size effects in platinum-cobalt cathode electrocatalysts for oxygen reduction},
	volume = {500},
	issn = {0925-8388},
	url = {https://www.sciencedirect.com/science/article/pii/S0925838810008091},
	doi = {10.1016/j.jallcom.2010.04.018},
	abstract = {Pt-Co/C electrocatalysts with Pt loadings close to 30wt.\% prepared by the impregnation method in water–ethylene glycol solutions were investigated by X-ray diffraction and correlated with electrochemical measurements. We show that composition of the binary solvent controls the average particle size and its distribution. The unit cell parameter of the Pt3Co alloy decreases nonlinearly with decreasing particle size. The ORR activity of the prepared Pt-Co/C catalysts in H2SO4 solution enhances with decreasing particle size and unit cell parameter as well as with narrowing of the particle size distribution. Corrosion treatment of the synthesized Pt-Co/C materials brings about an increase of ca. 1nm in the average grain size accompanied by broadening of the grain size distribution and a decrease in the Co content. All of the synthesized Pt-Co/C materials show higher ORR activities compared with commercial Pt/C electrocatalysts.},
	number = {2},
	urldate = {2023-11-11},
	journal = {Journal of Alloys and Compounds},
	author = {Leontyev, I. N. and Guterman, V. E. and Pakhomova, E. B. and Timoshenko, P. E. and {A.V.Guterman} and Zakharchenko, I. N. and Petin, G. P. and Dkhil, B.},
	month = jun,
	year = {2010},
	keywords = {Grain size distribution, Electrocatalysis, Oxygen reduction reaction (ORR), Platinum alloy, X-ray diffraction (XRD)},
	pages = {241--246},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\RVNSSP3Z\\Leontyev и др. - 2010 - XRD and electrochemical investigation of particle .pdf:application/pdf;ScienceDirect Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\VESEAEDH\\S0925838810008091.html:text/html},
}



@article{lorenz_self-organized_2010,
	title = {Self-organized growth of {ZnO}-based nano- and microstructures},
	volume = {247},
	copyright = {Copyright © 2010 WILEY-VCH Verlag GmbH \& Co. KGaA, Weinheim},
	issn = {1521-3951},
	url = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.200945514},
	doi = {10.1002/pssb.200945514},
	abstract = {ZnO-based nano- and micro-structures with controlled orientation, size, and lateral density were grown by specially designed two-step pulsed laser deposition and direct carbothermal growth, respectively. Different substrate orientations and nucleation layers allow well-defined tuning of growth direction and lateral arrangement of the wires. As a result, axial MgZnOZnO nano quantum dots and homogeneous radial nano core-shell quantum well structures are demonstrated. Donor and acceptor doping of nano- and microwires influence considerably both electrical characteristics as well as morphology including branching. Field effect transistors with n- and p-type wire channel and nanowire p–n junctions seem to prove a reproducible p-type conductivity of phosphorous-doped ZnO wires. Single ZnO wire (309 nm thick, 3.99 µm high) grown on pyramidal base with controlled lateral density by tuning the ZnO template layer in a two-step PLD process.},
	language = {en},
	number = {6},
	urldate = {2023-11-11},
	journal = {physica status solidi (b)},
	author = {Lorenz, Michael and Rahm, Andreas and Cao, Bingqiang and Zúñiga-Pérez, Jesús and Kaidashev, Evgeni M. and Zhakarov, Nikolai and Wagner, Gerald and Nobis, Thomas and Czekalla, Christian and Zimmermann, Gregor and Grundmann, Marius},
	year = {2010},
	note = {\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.200945514},
	keywords = {72.80.Ey, 73.21.Fg, 78.67.Bf, 81.05.Dz, 81.16.Dn, 81.16.Mk},
	pages = {1265--1281},
	file = {Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\6WSS5J7I\\pssb.html:text/html},
}



@article{timoshenko_impedance_2009,
	title = {Impedance of the microstrip line for magnetostatic backward volume waves},
	volume = {52},
	issn = {1573-9120},
	url = {https://doi.org/10.1007/s11141-010-9197-9},
	doi = {10.1007/s11141-010-9197-9},
	abstract = {We study excitation of magnetostatic backward volume waves on the microstrip line. The relation between the current density in the line and the normal component of the magnetic induction is found. The impedance of the line per unit length, i.e., its reactance and radiation resistance per unit length, is represented as a functional of the current density. The dependence of the operating-wave radiation resistance on the transverse size of the line and the width of the dielectric gap is studied. The radiation resistances of multistrip array and meander-type converters of magnetostatic backward volume waves are calculated},
	language = {en},
	number = {12},
	urldate = {2023-11-11},
	journal = {Radiophysics and Quantum Electronics},
	author = {Timoshenko, P. E. and Babicheva, E. R. and Ivanov, V. N. and Zubkov, V. I.},
	month = dec,
	year = {2009},
	keywords = {Ferrite, Frequency Dependence, Radiation Resistance, Side Lobe, Unit Length},
	pages = {892--899},
}



@article{rochal_theory_2009,
	title = {Theory of a reconstructive structural transformation in capsids of icosahedral viruses},
	volume = {80},
	url = {https://link.aps.org/doi/10.1103/PhysRevE.80.051905},
	doi = {10.1103/PhysRevE.80.051905},
	abstract = {A theory of a reconstructive structural transformation in icosahedral capsid shells is developed for a whole family of virulent human viruses. It is shown that the reversible rearrangement of proteins during the virus maturation transformation is driven by the variation in the wave number l associated with the protein density distribution function. The collective displacement field of protein centers from their positions in the initial (procapsid) and the final (capsid) two-dimensional icosahderal structures is derived. The amplitude of the displacement field is shown to be small and it minimizes the calculated free energy of the transformation. The theory allows us to propose a continuous thermodynamical mechanism of the reconstructive procapsid-to-capsid transformation. In the frame of the density-wave approach, we also propose to take an equivalent plane-wave vector as a common structural feature for different icosahedral capsid shells formed by the same proteins. Using these characteristics, we explain the relation between the radii of the procapsid and capsid shells and generalize it to the case of the viral capsid polymorphism.},
	number = {5},
	urldate = {2023-11-11},
	journal = {Physical Review E},
	author = {Rochal, S. B. and Lorman, V. L.},
	month = nov,
	year = {2009},
	note = {Publisher: American Physical Society},
	pages = {051905},
}



@article{leontyev_particle_2009,
	title = {Particle size effect in carbon supported {Pt}–{Co} alloy electrocatalysts prepared by the borohydride method: {XRD} characterization},
	volume = {357},
	issn = {0926-860X},
	shorttitle = {Particle size effect in carbon supported {Pt}–{Co} alloy electrocatalysts prepared by the borohydride method},
	url = {https://www.sciencedirect.com/science/article/pii/S0926860X08007874},
	doi = {10.1016/j.apcata.2008.12.023},
	abstract = {Pt3Co/C electrocatalysts prepared by wet synthesis method from water–ethylene glycol solutions of Pt and Co precursors were investigated by X-ray diffraction in conjunction with electrochemical measurements. It was shown that varying the binary solvent composition is an effective means of control over the average nanoparticle size and the grain size distribution. It was found that unit cell parameter of the Pt3Co/C electrocatalysts decreases nonlinearly with decreasing particle size. The activity of the prepared Pt3Co/C catalysts for the oxygen reduction reaction (ORR) in H2SO4 solution enhances with decrease in the particle size, the unit cell parameter, and the dispersion of the grain size distribution. All samples studied show higher catalytic activities in comparison with the commercial Pt/C materials.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Applied Catalysis A: General},
	author = {Leontyev, I. N. and Chernyshov, D. Yu. and Guterman, V. E. and Pakhomova, E. V. and Guterman, A. V.},
	month = mar,
	year = {2009},
	keywords = {X-ray diffraction, Grain size distribution, Oxygen reduction, Pt–Co alloy, Size effects},
	pages = {1--4},
	file = {ScienceDirect Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\356CZ2CX\\S0926860X08007874.html:text/html},
}



@article{martinand-mari_topological_2009,
	title = {Topological {Control} of {Life} and {Death} in {Non}-{Proliferative} {Epithelia}},
	volume = {4},
	issn = {1932-6203},
	url = {https://journals.plos.org/plosone/article?id=10.1371/journal.pone.0004202},
	doi = {10.1371/journal.pone.0004202},
	abstract = {Programmed cell death is one of the most fascinating demonstrations of the plasticity of biological systems. It is classically described to act upstream of and govern major developmental patterning processes (e.g. inter-digitations in vertebrates, ommatidia in Drosophila). We show here the first evidence that massive apoptosis can also be controlled and coordinated by a pre-established pattern of a specific ‘master cell’ population. This new concept is supported by the development and validation of an original model of cell patterning. Ciona intestinalis eggs are surrounded by a three-layered follicular organization composed of 60 elongated floating extensions made of as many outer and inner cells, and indirectly spread through an extracellular matrix over 1200 test cells. Experimental and selective ablation of outer and inner cells results in the abrogation of apoptosis in respective remaining neighbouring test cells. In addition incubation of outer/inner follicular cell-depleted eggs with a soluble extract of apoptotic outer/inner cells partially restores apoptosis to apoptotic-defective test cells. The 60 inner follicular cells were thus identified as ‘apoptotic master’ cells which collectively are induction sites for programmed cell death of the underlying test cells. The position of apoptotic master cells is controlled by topological constraints exhibiting a tetrahedral symmetry, and each cell spreads over and can control the destiny of 20 smaller test cells, which leads to optimized apoptosis signalling.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {PLOS ONE},
	author = {Martinand-Mari, Camille and Maury, Benoit and Rousset, François and Sahuquet, Alain and Mennessier, Gérard and Rochal, Sergei and Lorman, Vladimir and Mangeat, Paul and Baghdiguian, Stephen},
	year = {2009},
	note = {Publisher: Public Library of Science},
	keywords = {Apoptosis, Apoptotic signaling cascade, Chorion, Ciona intestinalis, Eggs, Fertilization, Ova, Symmetry},
	pages = {e4202},
	file = {Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\U26F6JVM\\Martinand-Mari и др. - 2009 - Topological Control of Life and Death in Non-Proli.pdf:application/pdf},
}



@article{ankiewicz_magnetic_2009,
	title = {Magnetic and structural properties of transition metal doped zinc-oxide nanostructures},
	volume = {246},
	copyright = {Copyright © 2009 WILEY-VCH Verlag GmbH \& Co. KGaA, Weinheim},
	issn = {1521-3951},
	url = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.200880581},
	doi = {10.1002/pssb.200880581},
	abstract = {We report on the magnetic and structural properties of two types of nanostructures doped with Co or Mn, namely, ZnO nanowires and colloidal ZnO nanocrystals. Electron paramagnetic resonance (EPR) spectra have been measured and analysed to extract information on the incorporation of the ions in the lattice. A detailed analysis by means of simulations of the experimental EPR spectra confirms that the transition metal (TM) ions were mainly incorporated as TM2+, occupying the Zn2+ sites in the wurtzite structure of ZnO. Furthermore, for both types of nanostructures, the EPR spectra are composed of more than one signal, revealing locally distorted environments or core-shell structures, proved by surface modifications via inorganic coatings. (© 2009 WILEY-VCH Verlag GmbH \& Co. KGaA, Weinheim)},
	language = {en},
	number = {4},
	urldate = {2023-11-11},
	journal = {physica status solidi (b)},
	author = {Ankiewicz, Amélia O. and Gehlhoff, Wolfgang and Martins, Joana S. and Pereira, Ângela S. and Pereira, Sérgio and Hoffmann, Axel and Kaidashev, Evgeni M. and Rahm, Andreas and Lorenz, Michael and Grundmann, Marius and Carmo, Maria C. and Trindade, Tito and Sobolev, Nikolai A.},
	year = {2009},
	note = {\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.200880581},
	keywords = {61.72.Vv, 68.65.La, 75.50.Pp, 76.30.Fc, 81.07.Bc},
	pages = {766--770},
}



@book{___2009,
	title = {Обработка и визуализация данных физических экспериментов с помощью пакета {Origin}},
	isbn = {978-5-397-00183-0},
	url = {https://urss.ru/cgi-bin/db.pl?lang=Ru&blang=ru&page=Book&id=81481&list=Found},
	abstract = {Настоящее учебно-методическое пособие на конкретных примерах учит приемам обработки спектров с помощью пакета Origin. Рассматриваются типичные задачи, наиболее часто встречающиеся на практике.

Пособие может использоваться при изучении дисциплин общего и специального физического практикума студентами направлений "Нанотехнология", "Физика" и других физических направлений и специальностей. Оно будет полезно всем, кому по роду своей деятельности приходится иметь дело с анализом спектров.},
	author = {{Исакова О.П.} and {Тарасевич Ю.Ю.} and {Юзюк Ю.И.}},
	year = {2009},
}



@article{czekalla_spatial_2008,
	title = {Spatial fluctuations of optical emission from single {ZnO}/{MgZnO} nanowire quantum wells},
	volume = {19},
	issn = {0957-4484},
	url = {https://dx.doi.org/10.1088/0957-4484/19/11/115202},
	doi = {10.1088/0957-4484/19/11/115202},
	abstract = {MgZnO/ZnO quantum wells on top of ZnO nanowires were grown by pulsed laser deposition. Ensembles of spatially fluctuating and narrow cathodoluminescence peaks with single widths down to 1 meV were found at the spectral position of the quantum well emission at 4 K. In addition, the number of these narrow QW peaks increases with increasing excitation power in micro-photoluminescence, thus pointing to quantum-dot-like emission centers. Indeed, laterally strained areas of about 5 nm diameter were identified at the quantum well positions on top of the nanowires by high-resolution transmission electron microscopy.},
	language = {en},
	number = {11},
	urldate = {2023-11-11},
	journal = {Nanotechnology},
	author = {Czekalla, C. and Guinard, J. and Hanisch, C. and Cao, B. Q. and Kaidashev, E. M. and Boukos, N. and Travlos, A. and Renard, J. and Gayral, B. and Dang, D. Le Si and Lorenz, M. and Grundmann, M.},
	month = feb,
	year = {2008},
	pages = {115202},
}



@article{kaidashev_structure_2008,
	title = {Structure and optical properties of {ZnO} nanowires fabricated by pulsed laser deposition on {GaN}/{Si}(111) films with the use of {Au} and {NiO} catalysts},
	volume = {72},
	issn = {1062-8738, 1934-9432},
	url = {http://link.springer.com/10.3103/S1062873808080315},
	doi = {10.3103/S1062873808080315},
	language = {en},
	number = {8},
	urldate = {2023-11-11},
	journal = {Bulletin of the Russian Academy of Sciences: Physics},
	author = {Kaidashev, E. M. and Lorenz, M. and Lenzner, J. and Ramm, A. and Nobis, T. and Grundmann, M. and Zakharov, N. and Kozakov, A. T. and Shevtsova, S. I. and Abdulvakhidov, K. G. and Kaidashev, V. E.},
	month = aug,
	year = {2008},
	pages = {1129--1131},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\TPG4HECU\\Kaidashev и др. - 2008 - Structure and optical properties of ZnO nanowires .pdf:application/pdf},
}



@article{schmidt-grund_vacuum_2008,
	title = {Vacuum {Ultraviolet} {Dielectric} {Function} and {Band} {Structure} of {ZnO}},
	volume = {53},
	issn = {0374-4884},
	url = {http://www.jkps.or.kr/journal/DOIx.php?id=10.3938/jkps.53.88},
	doi = {10.3938/jkps.53.88},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Journal of the Korean Physical Society},
	author = {Schmidt-Grund, Rüdiger and Rheinländer, Bernd and Kaidashev, Evgeni M. and Lorenz, Michael and Grundmann, Marius and Fritsch, Daniel and Schubert, Mathias M. and Schmidt, Heidemarie and Herzinger, Craig M.},
	month = jul,
	year = {2008},
	pages = {88--93},
}



@incollection{grundmann_growth_2008,
	title = {Growth and {Characterization} of {ZnO} {Nano}- and {Microstructures}},
	isbn = {978-0-08-046325-4},
	url = {https://linkinghub.elsevier.com/retrieve/pii/B9780080463254000098},
	language = {en},
	urldate = {2023-11-11},
	booktitle = {Handbook of {Self} {Assembled} {Semiconductor} {Nanostructures} for {Novel} {Devices} in {Photonics} and {Electronics}},
	publisher = {Elsevier},
	author = {Grundmann, Marius and Rahm, Andreas and Nobis, Thomas and Lorenz, Michael and Czekalla, Christian and Kaidashev, Evgeni M. and Lenzner, Jörg and Boukos, Nikos and Travlos, Anastasios},
	year = {2008},
	doi = {10.1016/B978-0-08-046325-4.00009-8},
	pages = {293--323},
}



@book{___2008,
	title = {Введение в химию и физику наноструктур и наноструктурированных материалов},
	isbn = {978-5-91327-029-0},
	publisher = {Москва: Академия Естествознания},
	author = {{Таланов В.М.} and {Ерейская Г.П.} and {Юзюк Ю.И.}},
	year = {2008},
}



@article{mishina_switchable_2007,
	title = {Switchable nonlinear metalloferroelectric photonic crystals},
	volume = {91},
	issn = {0003-6951},
	url = {https://doi.org/10.1063/1.2762284},
	doi = {10.1063/1.2762284},
	abstract = {Two types of low-voltage electroswitchable nonlinear photonic crystals were fabricated providing spatial-frequency control of second harmonic generation radiation of visible light. A two-dimensional photonic crystal was fabricated by focused ion beam etching of a ferroelectric BaSrTiO3 thin film and switched by an electric field applied by an interdigital electrode system, which simultaneously acted as a one-dimensional photonic crystal. The fabricated device operated at a second harmonic wavelength around 400nm with an efficiency incomparably higher than in the case of linear optics.},
	number = {4},
	urldate = {2023-11-11},
	journal = {Applied Physics Letters},
	author = {Mishina, E. and Zaitsev, A. and Ilyin, N. and Sherstyuk, N. and Sigov, A. and Golovko, Yu. and Muhortov, V. and Kolesnikov, A. and Lozovik, Yu. and Yemtsova, M. and Rasing, Th.},
	month = jul,
	year = {2007},
	pages = {041107},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\UJII4ECH\\Mishina и др. - 2007 - Switchable nonlinear metalloferroelectric photonic.pdf:application/pdf},
}



@article{rahm_growth_2006,
	title = {Growth and characterization of {Mn}- and {Co}-doped {ZnO} nanowires},
	volume = {156},
	issn = {1436-5073},
	url = {https://doi.org/10.1007/s00604-006-0602-1},
	doi = {10.1007/s00604-006-0602-1},
	abstract = {We report on the high-pressure pulsed laser deposition growth of zinc oxide nanowires containing about 0.2 at.\% Co and 0.5 at.\% Mn by NiO and Au catalyst. Scanning electron microscopy and X-ray diffraction measurements revealed arrays of parallel-standing nanowires with hexagonal cross section and uniform in-plane epitaxial relations without rotational domains. Elemental analysis was carried out using particle induced X-ray emission and Q-band electron spin resonance. The valence of the incorporated Mn was determined to be 2+. Atomic and magnetic force microscopy measurements indicate that Mn is incorporated preferentially at the nanowire boundaries.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Microchimica Acta},
	author = {Rahm, Andreas and Kaidashev, Evgeni M. and Schmidt, Heidemarie and Diaconu, Mariana and Pöppl, Andreas and Böttcher, Rolf and Meinecke, Christoph and Butz, Tilman and Lorenz, Michael and Grundmann, Marius},
	month = nov,
	year = {2006},
	keywords = {Key words: Zinc oxide; pulsed laser deposition; nanowire; transition metal.},
	pages = {21--25},
}



@inproceedings{nobis_whispering_2005,
	address = {Dordrecht},
	series = {{NATO} {Science} {Series} {II}: {Mathematics}, {Physics} and {Chemistry}},
	title = {Whispering {Gallery} {Modes} in {Hexagonal} {Zinc} {Oxide} {Micro}- and {Nanocrystals}},
	isbn = {978-1-4020-3475-6},
	doi = {10.1007/1-4020-3475-X_8},
	abstract = {The resonator properties of zinc oxide (ZnO) micro- and nanocrystals grown by a novel high pressure pulsed laser deposition process have been investigated at room temperature by cathodoluminescence (CL), spatially resolved CL-imaging and polarization resolved micro-photoluminescence (μ-PL) within the visible spectral range. The spectra exhibit a series of comparatively sharp and almost equidistant resonance lines. Using a simple plane wave interference model and taking into account the spectral characteristic n(ω) of the refractive index of ZnO, we can unambiguously attribute those lines to whispering gallery modes (WGMs) of a two dimensional hexagonal resonator. The predicted resonator diameters agree well with the measured crystal sizes. Tapered, high aspect ratio ZnO nanoneedles furthermore allow systematic investigations of the WGMs as a function of cavity diameter D down to zero. Hence, the transition from a multi-mode to a single mode cavity is directly observed. μ-PL experiments demonstrate that the WGMs are mainly TM polarized.},
	language = {en},
	booktitle = {Zinc {Oxide} — {A} {Material} for {Micro}- and {Optoelectronic} {Applications}},
	publisher = {Springer Netherlands},
	author = {Nobis, Thomas and Kaidashev, Evgeni M. and Rahm, Andreas and Lorenz, Michael and Grundmann, Marius},
	editor = {Nickel, Norbert H. and Terukov, Evgenii},
	year = {2005},
	keywords = {microcrystal, nanocavity, nanostructure, polarization, Whispering gallery modes},
	pages = {83--98},
}



@article{nobis_whispering_2004,
	title = {Whispering {Gallery} {Modes} in {Nanosized} {Dielectric} {Resonators} with {Hexagonal} {Cross} {Section}},
	volume = {93},
	url = {https://link.aps.org/doi/10.1103/PhysRevLett.93.103903},
	doi = {10.1103/PhysRevLett.93.103903},
	abstract = {The size dependence of whispering gallery modes in dielectric resonators with hexagonal cross section has been observed within the visible spectral range for cavity diameters comparable to the light wavelength. As a model system single, tapered, high aspect ratio zinc oxide nanoneedles were analyzed. They enable systematic investigations as a function of the resonator diameter down to the nanometer regime. A simple plane wave interference model without free parameter describes the spectral positions and the linewidths of the modes in good agreement with the experiment.},
	number = {10},
	urldate = {2023-11-11},
	journal = {Physical Review Letters},
	author = {Nobis, Thomas and Kaidashev, Evgeni M. and Rahm, Andreas and Lorenz, Michael and Grundmann, Marius},
	month = sep,
	year = {2004},
	note = {Publisher: American Physical Society},
	pages = {103903},
}



@article{nobis_spatially_2004,
	title = {Spatially {Inhomogeneous} {Impurity} {Distribution} in {ZnO} {Micropillars}},
	volume = {4},
	issn = {1530-6984},
	url = {https://doi.org/10.1021/nl049889y},
	doi = {10.1021/nl049889y},
	abstract = {Using ZnO a variety of micro- and nanostructures can be fabricated. We investigate hexagonal micropillars grown by high pressure pulsed laser deposition on sapphire with spatially and spectrally resolved cathodoluminescence. We demonstrate that the impurity and defect incorporation is strongly inhomogeneous, at least under the present growth conditions, dramatically influencing the optical properties.},
	number = {5},
	urldate = {2023-11-11},
	journal = {Nano Letters},
	author = {Nobis, Thomas and Kaidashev, Evgeni M. and Rahm, Andreas and Lorenz, Michael and Lenzner, Jörg and Grundmann, Marius},
	month = may,
	year = {2004},
	note = {Publisher: American Chemical Society},
	pages = {797--800},
}



@article{bundesmann_infrared_2004,
	series = {The 3rd {International} {Conference} on {Spectroscopic} {Ellipsometry}},
	title = {Infrared dielectric functions and crystal orientation of a-plane {ZnO} thin films on r-plane sapphire determined by generalized ellipsometry},
	volume = {455-456},
	issn = {0040-6090},
	url = {https://www.sciencedirect.com/science/article/pii/S0040609003018285},
	doi = {10.1016/j.tsf.2003.11.226},
	abstract = {Generalized infrared spectroscopic ellipsometry for wave numbers from 370 to 1200 cm−1 was applied to study the anisotropic dielectric response of wurtzite-type ZnO thin films grown on r-plane sapphire. Combined wavelength-by-wavelength analysis of data measured at multiple sample in-plane orientations allows for simultaneous extraction of the dielectric function (DF) tensor, the film thickness and the respective ZnO c-axis orientation, specifically in relation to the sapphire substrate. For anisotropic materials and use of generalized ellipsometry, the correlation problem between thickness and DF does not exist. Subsequent line shape analysis of ordinary and extraordinary DFs provides complete A1- and E1-symmetry longitudinal and transverse optical phonon-mode and broadening parameters, together with the static dielectric constants. The epitaxial relations from the ellipsometry data analysis are (11−20)ZnO∣∣(01−12)sapphire and [0001]ZnO∣∣[0−111]sapphire, which was confirmed by XRD measurements.},
	urldate = {2023-11-11},
	journal = {Thin Solid Films},
	author = {Bundesmann, C. and Ashkenov, N. and Schubert, M. and Rahm, A. and Wenckstern, H. v. and Kaidashev, E. M. and Lorenz, M. and Grundmann, M.},
	month = may,
	year = {2004},
	keywords = {-Plane ZnO, Epitaxial relation, Generalized infrared spectroscopic ellipsometry, Phonon modes},
	pages = {161--166},
}



@article{von_wenckstern_lateral_2003,
	title = {Lateral homogeneity of {Schottky} contacts on n-type {ZnO}},
	volume = {84},
	issn = {0003-6951},
	url = {https://doi.org/10.1063/1.1638898},
	doi = {10.1063/1.1638898},
	abstract = {The electrical properties of Schottky contacts (SCs) produced ex situ on n-type ZnO single crystals and epitaxial thin films were investigated. Electron beam induced current imaging was used to study lateral variations of the current induced in the space charge region of the SC. Further, the effective barrier height was determined by current–voltage and capacitance–voltage measurements. Pd contacts prepared on ZnO thin films that had undergone treatment in a plasma-enhanced chemical vapor deposition with nitrous oxide (N2O) as ambient gas are laterally homogeneous with an effective barrier height of (600±30) meV.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Applied Physics Letters},
	author = {von Wenckstern, H. and Kaidashev, E. M. and Lorenz, M. and Hochmuth, H. and Biehne, G. and Lenzner, J. and Gottschalch, V. and Pickenhain, R. and Grundmann, M.},
	month = dec,
	year = {2003},
	pages = {79--81},
}



@article{bundesmann_raman_2003,
	title = {Raman scattering in {ZnO} thin films doped with {Fe}, {Sb}, {Al}, {Ga}, and {Li}},
	volume = {83},
	issn = {0003-6951},
	url = {https://doi.org/10.1063/1.1609251},
	doi = {10.1063/1.1609251},
	abstract = {Polarized micro-Raman measurements were performed to study the phonon modes of Fe, Sb, Al, Ga, and Li doped ZnO thin films, grown by pulsed-laser deposition on c-plane sapphire substrates. Additional modes at about 277, 511, 583, and 644 cm−1, recently assigned to N incorporation [A. Kaschner et al., Appl. Phys. Lett. 80, 1909 (2002)], were observed for Fe, Sb, and Al doped films, intentionally grown without N. The mode at 277 cm−1 occurs also for Ga doped films. These modes thus cannot be related directly to N incorporation. Instead, we suggest host lattice defects as their origin. Further additional modes at 531, 631, and 720 cm−1 seem specific for the Sb, Ga, and Fe dopants, respectively. Li doped ZnO did not reveal additional modes.},
	number = {10},
	urldate = {2023-11-11},
	journal = {Applied Physics Letters},
	author = {Bundesmann, C. and Ashkenov, N. and Schubert, M. and Spemann, D. and Butz, T. and Kaidashev, E. M. and Lorenz, M. and Grundmann, M.},
	month = sep,
	year = {2003},
	pages = {1974--1976},
}



@article{ashkenov_infrared_2002,
	title = {Infrared dielectric functions and phonon modes of high-quality {ZnO} films},
	volume = {93},
	issn = {0021-8979},
	url = {https://doi.org/10.1063/1.1526935},
	doi = {10.1063/1.1526935},
	abstract = {Infrared dielectric function spectra and phonon modes of high-quality, single crystalline, and highly resistive wurtzite ZnO films were obtained from infrared (300–1200 cm−1) spectroscopic ellipsometry and Raman scattering studies. The ZnO films were deposited by pulsed-laser deposition on c-plane sapphire substrates and investigated by high-resolution x-ray diffraction, high-resolution transmission electron microscopy, and Rutherford backscattering experiments. The crystal structure, phonon modes, and dielectric functions are compared to those obtained from a single-crystal ZnO bulk sample. The film ZnO phonon mode frequencies are highly consistent with those of the bulk material. A small redshift of the longitudinal optical phonon mode frequencies of the ZnO films with respect to the bulk material is observed. This is tentatively assigned to the existence of vacancy point defects within the films. Accurate long-wavelength dielectric constant limits of ZnO are obtained from the infrared ellipsometry analysis and compared with previously measured near-band-gap index-of-refraction data using the Lyddane–Sachs–Teller relation. The ZnO model dielectric function spectra will become useful for future infrared ellipsometry analysis of free-carrier parameters in complex ZnO-based heterostructures.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Journal of Applied Physics},
	author = {Ashkenov, N. and Mbenkum, B. N. and Bundesmann, C. and Riede, V. and Lorenz, M. and Spemann, D. and Kaidashev, E. M. and Kasic, A. and Schubert, M. and Grundmann, M. and Wagner, G. and Neumann, H. and Darakchieva, V. and Arwin, H. and Monemar, B.},
	month = dec,
	year = {2002},
	pages = {126--133},
}



@article{kaidashev_high_2003,
	title = {High electron mobility of epitaxial {ZnO} thin films on c-plane sapphire grown by multistep pulsed-laser deposition},
	volume = {82},
	issn = {0003-6951},
	url = {https://doi.org/10.1063/1.1578694},
	doi = {10.1063/1.1578694},
	abstract = {A multistep pulsed-laser deposition (PLD) process is presented for epitaxial, nominally undoped ZnO thin films of total thickness of 1 to 2 μm on c-plane sapphire substrates. We obtain reproducibly high electron mobilities from 115 up to 155 cm2/V s at 300 K in a narrow carrier concentration range from 2 to 5×1016 cm−3. The key issue of the multistep PLD process is the insertion of 30-nm-thin ZnO relaxation layers deposited at reduced substrate temperature. The high-mobility samples show atomically flat surface structure with grain size of about 0.5–1 μm, whereas the surfaces of low-mobility films consist of clearly resolved hexagonally faceted columnar grains of only 200-nm size, as shown by atomic force microscopy. Structurally optimized PLD ZnO thin films show narrow high-resolution x-ray diffraction peak widths of the ZnO(0002) ω- and 2Θ-scans as low as 151 and 43 arcsec, respectively, and narrow photoluminescence linewidths of donor-bound excitons of 1.7 meV at 2 K.},
	number = {22},
	urldate = {2023-11-11},
	journal = {Applied Physics Letters},
	author = {Kaidashev, E. M. and Lorenz, M. and von Wenckstern, H. and Rahm, A. and Semmelhack, H.-C. and Han, K.-H. and Benndorf, G. and Bundesmann, C. and Hochmuth, H. and Grundmann, M.},
	month = may,
	year = {2003},
	pages = {3901--3903},
}



@article{molodtsova_fabrication_2023,
	title = {Fabrication of nano-{In}$_{\textrm{2}}${O}$_{\textrm{3}}$ phase junction by pulse alternating current synthesis for enhanced photoelectrochemical performance: {Unravelling} the role of synthetic conditions},
	volume = {49},
	issn = {02728842},
	shorttitle = {Fabrication of nano-{In2O3} phase junction by pulse alternating current synthesis for enhanced photoelectrochemical performance},
	url = {https://linkinghub.elsevier.com/retrieve/pii/S0272884222043309},
	doi = {10.1016/j.ceramint.2022.11.293},
	language = {en},
	number = {7},
	urldate = {2023-11-11},
	journal = {Ceramics International},
	author = {Molodtsova, Tatyana and Gorshenkov, Mikhail and Kolesnikov, Evgeny and Leontyev, Igor and Kaichev, Vasily and Zhigunov, Denis and Faddeev, Nikita and Kuriganova, Alexandra and Smirnova, Nina},
	month = apr,
	year = {2023},
	keywords = {Q1},
	pages = {10986--10992},
}



@article{kuriganova_pulse_2022,
	title = {Pulse {Electrolysis} {Technique} for {Preparation} of {Bimetal} {Tin}-{Containing} {Electrocatalytic} {Materials}},
	volume = {12},
	issn = {2073-4344},
	url = {https://www.mdpi.com/2073-4344/12/11/1444},
	doi = {10.3390/catal12111444},
	abstract = {Platinum–tin-containing materials are the most popular catalysts for processes occurring in fuel cells with direct ethanol oxidation. Pulse electrolysis based on the electrochemical dispersion of platinum electrodes under the influence of alternating pulse current in an alkaline electrolyte made it possible to introduce the tin component into the catalyst in the form of a dopant, an alloy with platinum, and in the form of an oxide phase and evaluate the effect of the form in which tin is present in the catalyst on its microstructural and electrocatalytic characteristics. The introduction of tin into the catalyst generally increases the rate of ethanol electrooxidation; however, with the most prominent effect observed when tin is present in form of an oxide.},
	language = {en},
	number = {11},
	urldate = {2023-11-11},
	journal = {Catalysts},
	author = {Kuriganova, Alexandra and Kubanova, Marina and Leontyev, Igor and Molodtsova, Tatiana and Smirnova, Nina},
	month = nov,
	year = {2022},
	pages = {1444},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\BTS2JHFX\\Kuriganova и др. - 2022 - Pulse Electrolysis Technique for Preparation of Bi.pdf:application/pdf},
}



@article{gerasimova_role_2022,
	title = {Role of the {Potential} {Range} during {Stress} {Testing} of {Platinum}-{Containing} {Electrocatalysts} at {Elevated} {Temperature}},
	volume = {12},
	issn = {2073-4344},
	url = {https://www.mdpi.com/2073-4344/12/10/1179},
	doi = {10.3390/catal12101179},
	abstract = {The durability of low temperature proton exchange membrane fuel cell (PEMFC) catalysts crucially affects their lifetime. The choice of carbon support is important in terms of increasing the stability of catalysts. In this research, Pt/C samples were obtained using the polyol synthesis method on two types of carbon supports: the standard support, Vulcan XC-72, and carbon support with a high degree of graphitization, ECS-002402. One method for assessing structural characteristics is through transmission electron microscopy (TEM), according to which materials G1 and G2 showed an average nanoparticle size of 3.7 and 4.2 nm, respectively. On all catalysts, the oxygen reduction reaction proceeded according to the four electron mechanism. Durability was assessed by changes in ESA and activity in the ORR after 1000 cycles, with changes in the upper potential values: 0.7; 1.0; 1.2; and 1.4 V. After accelerated stress testing, the G1 material showed the greatest residual activity at a potential of 1.4 V (165 A/g (Pt). Based on the results of comparing various ADT protocols, the optimal mode of 0.4 and 1.4 V was chosen, and should be used for further studies comparing the durability of Pt/C catalysts.},
	language = {en},
	number = {10},
	urldate = {2023-11-11},
	journal = {Catalysts},
	author = {Gerasimova, Irina and Belenov, Sergey and Lyanguzov, Nikolai and Pankov, Ilya and Tolstunov, Mikhail and Pavlets, Angelina},
	month = oct,
	year = {2022},
	pages = {1179},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\IERK75HA\\Gerasimova и др. - 2022 - Role of the Potential Range during Stress Testing .pdf:application/pdf;Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\G3CGGG63\\Gerasimova и др. - 2022 - Role of the Potential Range during Stress Testing .pdf:application/pdf},
}



@article{andryushin_influence_2022,
	title = {The {Influence} of the {Elemental} {Composition}, {Crystal} {Structure}, and {Grain} {Structure} of the {Ferro}-{Piezoceramics} of {Various} {Degrees} of the {Ferro}-{Hardness} on the {Stability} of the {Polarized} {State}},
	volume = {15},
	issn = {1996-1944},
	url = {https://www.mdpi.com/1996-1944/15/6/2118},
	doi = {10.3390/ma15062118},
	abstract = {Ferro-piezoceramic materials (FPCM) with different degrees of ferrohardness were fabricated by double solid-phase synthesis followed by the sintering technique using hot pressing method. The X-ray studies carried out in a wide temperature range showed that with increasing temperature, each of the studied FPCM undergoes a series of phase transformations, accompanied by a change in the symmetry of the unit cell. In this case, near the phase transition to the nonpolar cubic phase, in each of the FPCM, the formation of a fuzzy symmetry region is observed, which is characterized by weak distortions and temperature–time instability of the crystal structure. The study of the piezoelectric modulus d33 in the quasi-static regime as a function of temperature made it possible to reveal the different nature of its behavior in materials of various degrees of ferrohardness. It was shown that the conservation of the state in ferrosoft materials above the Curie temperature is associated with the relaxation nature of the change in their properties, the existence of a region of fuzzy symmetry (noncubic phase) in them above the Curie temperature, and increased inertia of the system. The expediency of taking into account the presented results in the development of electromechanical converters based on FPCM of various degrees of ferrohardness, operated under temperature effects, including cyclic ones, was shown.},
	language = {en},
	number = {6},
	urldate = {2023-11-11},
	journal = {Materials},
	author = {Andryushin, Konstantin and Dudkina, Svetlana and Sahoo, Sushrisangita and Shilkina, Lidiya and Alyoshin, Vladimir and Triger, Ekaterina and Andryushina, Inna and Verbenko, Iliya and Rudskiy, Daniil and Rudskaya, Angela and Reznichenko, Larisa},
	month = mar,
	year = {2022},
	pages = {2118},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\G8H4F7ND\\Andryushin и др. - 2022 - The Influence of the Elemental Composition, Crysta.pdf:application/pdf;Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\J7PHWKJD\\Andryushin и др. - 2022 - The Influence of the Elemental Composition, Crysta.pdf:application/pdf},
}



@article{konevtsova_moire_2022,
	title = {Moiré patterns and carbon nanotube sorting},
	volume = {6},
	issn = {2399-1984},
	url = {https://iopscience.iop.org/article/10.1088/2399-1984/ac4a27},
	doi = {10.1088/2399-1984/ac4a27},
	abstract = {Abstract
            Moiré patterns (MPs), arising from the superposition of two lattices with close periods, are tightly related to the physicochemical properties of bilayer nanostructures. Here, we develop the theory of complex MPs emerging in twisted bilayer graphene and planar nets of double-walled nanotubes at significant relative twist and/or deformation of layers. The proposed theory clarifies the physicochemical regularities arising at sorting of single-walled carbon nanotubes (SWCNTs) by organic molecules, which self-assemble in regular coatings on both the tubes and planar graphene. We introduce and consider an outer tubular virtual lattice that is a parent structure for the deposited coating and due to this fact, its existence is crucial for the coating formation. As we show, such outer lattices exist only for successfully sorted SWCNTs and the superposition between the outer lattice and SWCNT forms a specific long-period MP. We explain known experimental results of SWCNT sorting by molecules of flavin group, poly(9,9-dioctylfluorene-2,7-diyl), and poly [(m-phenylenevinylene)-alt-(p-phenylenevinylene)]. Also, our approach points out other organic molecules and polymers suitable for effective carbon nanotube sorting.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Nano Futures},
	author = {Konevtsova, Olga V and Roshal, Daria S and Rochal, Sergei B},
	month = mar,
	year = {2022},
	pages = {015005},
}



@article{chalin_tight-binding_2022,
	title = {Tight-binding approximation for bilayer graphene and nanotube structures: {From} commensurability to incommensurability between the layers},
	volume = {105},
	issn = {2469-9950, 2469-9969},
	shorttitle = {Tight-binding approximation for bilayer graphene and nanotube structures},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.105.045402},
	doi = {10.1103/PhysRevB.105.045402},
	language = {en},
	number = {4},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Chalin, D. V. and Levshov, D. I. and Myasnikova, A. E. and Rochal, S. B.},
	month = jan,
	year = {2022},
	pages = {045402},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\MDNW4VT5\\Chalin и др. - 2022 - Tight-binding approximation for bilayer graphene a.pdf:application/pdf;Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\VM6EQJBB\\Chalin и др. - 2022 - Tight-binding approximation for bilayer graphene a.pdf:application/pdf},
}



@article{shirokov_efficiency_2022,
	title = {Efficiency of {Generation} of {Surface} {Acoustic} {Waves} in {Barium} {Strontium} {Titanate} {Thin} {Films}},
	volume = {69},
	issn = {0885-3010, 1525-8955},
	url = {https://ieeexplore.ieee.org/document/9744607/},
	doi = {10.1109/TUFFC.2022.3163610},
	number = {5},
	urldate = {2023-11-11},
	journal = {IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control},
	author = {Shirokov, Vladimir B. and Timoshenko, Pavel E. and Kalinchuk, Valery V.},
	month = may,
	year = {2022},
	pages = {1815--1820},
}



@article{roshal_random_2022,
	title = {Random nature of epithelial cancer cell monolayers},
	volume = {19},
	issn = {1742-5662},
	url = {https://royalsocietypublishing.org/doi/10.1098/rsif.2022.0026},
	doi = {10.1098/rsif.2022.0026},
	abstract = {Although the polygonal shape of epithelial cells has been drawing the attention of scientists for several centuries, only a decade and a half ago it was demonstrated that distributions of polygon types (DOPTs) are similar in proliferative epithelia of many different plant and animal species. In this study, we show that hyper-proliferation of cancer cells disrupts this universal paradigm and results in randomly organized epithelial structures. Examining non-synchronized and synchronized HeLa cervix cells, we suppose that the spread of cell sizes is the main parameter controlling the DOPT in the cancer cell monolayers. To test this hypothesis, we develop a theory of morphologically similar random polygonal packings. By analysing differences between tumoural and normal epithelial cell monolayers, we conclude that the latter have more ordered structures because of their lower proliferation rates and, consequently, more effective relaxation of mechanical stress associated with cell division and growth. To explain the structural features of normal proliferative epithelium, we take into account the spread of cell sizes in the monolayer. The proposed theory also rationalizes some highly ordered unconventional post-mitotic epithelia.},
	language = {en},
	number = {190},
	urldate = {2023-11-11},
	journal = {Journal of The Royal Society Interface},
	author = {Roshal, Daria S. and Martin, Marianne and Fedorenko, Kirill and Golushko, Ivan and Molle, Virginie and Baghdiguian, Stephen and Rochal, Sergei B.},
	month = may,
	year = {2022},
	pages = {20220026},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\9ZQ6KFAD\\Roshal и др. - 2022 - Random nature of epithelial cancer cell monolayers.pdf:application/pdf},
}



@article{andryushin_effects_2022,
	title = {The effects of the modification of the {BST}-system solid solutions with rare earth elements},
	volume = {48},
	issn = {02728842},
	url = {https://linkinghub.elsevier.com/retrieve/pii/S0272884221030534},
	doi = {10.1016/j.ceramint.2021.09.243},
	language = {en},
	number = {2},
	urldate = {2023-11-11},
	journal = {Ceramics International},
	author = {Andryushin, K.P. and Shilkina, L.A. and Khasbulatov, S.V. and Nagaenko, A.V. and Dudkina, S.I. and Andryushina, I.N. and Sadykov, KhA. and Verbenko, I.A. and Rudskaya, A.G. and Reznichenko, L.A.},
	month = jan,
	year = {2022},
	pages = {1642--1658},
}



@article{konevtsova_hidden_2023,
	title = {Hidden symmetry of the flavivirus protein shell and {pH}-controlled reconstruction of the viral surface},
	volume = {11},
	issn = {2047-4830, 2047-4849},
	url = {http://xlink.rsc.org/?DOI=D2BM01562E},
	doi = {10.1039/D2BM01562E},
	abstract = {A pH-induced change in the charge distribution of proteins leads to a structural transformation of the outer flavivirus shell, which violates the hidden symmetry of the mutual arrangement of proteins located on opposite sides of the lipid membrane.
          , 
            Using recent Zika virus structural data we reveal a hidden symmetry of protein order in immature and mature flavivirus shells, violating the Caspar–Klug paradigmatic model of capsid structures. We show that proteins of the outer immature shell layer exhibit trihexagonal tiling, while proteins from inner and outer layers conjointly form a double-shelled close-packed structure, based on a common triangular spherical lattice. Within the proposed structural model, we furthermore rationalize the structural organization of misassembled non-infectious subviral particles that have no inner capsid. We consider a pH-controlled structural reconstruction of the outer shell from the trimeric to the dimeric state, and demonstrate that this transition, occurring during the virus maturation, can be induced by changes in protein charges at lower pH, leading to a decrease in the electrostatic interaction free energy. This transition could also be assisted by electrostatic attraction of shell proteins to the interposed lipid membrane substrate separating the shells.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Biomaterials Science},
	author = {Konevtsova, Olga V. and Golushko, Ivan Yu. and Podgornik, Rudolf and Rochal, Sergei B.},
	year = {2023},
	keywords = {Q1},
	pages = {225--234},
}



@article{__2014,
	title = {Структура и динамика решетки твердых растворов (1-x){BiFeO}$_{\textrm{3}}$-{xANbO}$_{\textrm{3}}$ ({A}-{K}, {Na})},
	volume = {56},
	url = {http://journals.ioffe.ru/articles/40748},
	abstract = {Методами рентгеновской порошковой дифракции и комбинационного рассеяния света изучены структуры и динамические характеристики решеток составов двух систем твердых растворов мультиферроика BiFeO3 с сегнетоэлектриком KNbO3 и антисегнетоэлектриком NaNbO3: (1-x)BiFeO3-xKNbO3 и (1-x)BiFeO3-xNaNbO3. Для этих систем в составах с x=0.3, 0.5 и 0.7 при комнатной температуре определены симметрия, параметры элементарных ячеек. Из анализа колебательных спектров установлены последовательности ротационных искажений при изменении концентраций в этих системах твердых растворов.},
	language = {ru},
	number = {9},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Тесленко, П. Ю. and Разумная, А. Г. and Пономоренко, В. О. and Рудская, А. Г. and Назаренко, А. В. and Анохин, А. С. and Авраменко, М. В. and Левшов, Д. И. and Куприянов, М. Ф. and Юзюк, Ю. И.},
	month = aug,
	year = {2014},
	pages = {1804--18010},
}



@article{__2013-6,
	title = {Спектроскопия комбинационного рассеяния света как метод диагностики структуры индивидуальных углеродных нанотрубок},
	url = {http://www.ivdon.ru/magazine/archive/n4y2013/1972},
	abstract = {Сетевой научный журнал «Инженерный вестник Дона»},
	language = {ru},
	number = {4},
	urldate = {2023-11-11},
	author = {Левшов, Д. И. and Авраменко, М. В.},
	month = jul,
	year = {2013},
}



@article{__2013-7,
	title = {Низкотемпературный термический синтез наностержней оксида цинка из паров цинка без катализатора},
	url = {http://www.ivdon.ru/magazine/archive/n4y2013/1884},
	abstract = {Сетевой научный журнал «Инженерный вестник Дона»},
	language = {ru},
	urldate = {2023-11-11},
	author = {Пушкарев, В. И. and Лянгузов, Н. В. and Кайдашев, Е. М.},
	month = aug,
	year = {2013},
}



@article{__2007,
	title = {Фазовращатель на щелевой линии, нагруженный варакторами на основе наноразмерных пленок титаната бария-стронция},
	volume = {52},
	issn = {0033-8494},
	url = {http://naukarus.com/fazovraschatel-na-schelevoy-linii-nagruzhennoy-varaktorami-na-osnove-nanorazmernyh-plenok-titanata-bariya-strontsiya},
	abstract = {Реализован монолитный фазовращатель на щелевой линии передачи, периодически нагруженной сегнетоэлектрическими варакторами на основе наноразмерных пленок Bа0.8Sr0.2TiO3. Установлено, что при уменьшении толщины наноразмерной сегнетоэлектрической пленки, на основе которой реализованы варакторы, от 36 до 18 нм коэффициент качества фазовращателя в полосе частот от 12 до 13.5 ГГц возрастает более чем в два раза.},
	language = {ru},
	number = {11},
	urldate = {2023-11-11},
	journal = {Радиотехника и электроника},
	author = {Головко, Ю. И. and Масычев, С. И. and Мухортов, Вас.М. and Мухортов, Вл. М. and Чуб, А. В.},
	year = {2007},
	keywords = {⛔ No DOI found},
	file = {Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\NC57SS3Z\\fazovraschatel-na-schelevoy-linii-nagruzhennoy-varaktorami-na-osnove-nanorazmernyh-plenok-titan.html:text/html},
}



@article{__2006,
	title = {Новый датчик динамической деформации на основе тонких пьезоэлектрических пленок, полученных ионноплазменным напылением},
	volume = {58},
	issn = {1999-9429},
	url = {https://cyberleninka.ru/article/n/novyy-datchik-dinamicheskoy-deformatsii-na-osnove-tonkih-piezoelektricheskih-plenok-poluchennyh-ionnoplazmennym-napyleniem},
	language = {ru},
	number = {3},
	urldate = {2023-11-11},
	journal = {Известия Южного федерального университета. Технические науки},
	author = {Мухортов, Вл. М. and Мухортов, Вас.М. and Бирюков, С. В.},
	year = {2006},
	note = {Number: 3
Place: Россия, Ростов-на-Дону
Publisher: Федеральное государственное автономное образовательное учреждение высшего образования «Южный федеральный университет»},
	keywords = {⛔ No DOI found},
	pages = {221--227},
	file = {Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\D4V7B898\\В.м и др. - 2006 - Новый датчик динамической деформации на основе тон.pdf:application/pdf},
}



@article{__2014-1,
	title = {Анализ атомной структуры углеродных нанотрубок методами спектроскопии комбинационного рассеяния света и электронной дифракции},
	url = {http://www.ivdon.ru/ru/magazine/archive/N4y2014/2679},
	abstract = {Сетевой научный журнал «Инженерный вестник Дона»},
	language = {ru},
	number = {4},
	urldate = {2023-11-11},
	journal = {Инженерный Вестник Дона},
	author = {Левшов, Д. И. and Авраменко, М. В. and Пимонов, В. В.},
	month = jun,
	year = {2014},
	keywords = {⛔ No DOI found},
	pages = {1--11},
	file = {Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\8MAPFW2E\\2679.html:text/html},
}



@article{__2014-2,
	title = {Влияние эффектов окружения на колебательные свойства индивидуальных углеродных нанотрубок},
	url = {http://www.ivdon.ru/ru/magazine/archive/N4y2014/2680},
	abstract = {Сетевой научный журнал «Инженерный вестник Дона»},
	language = {ru},
	number = {4},
	urldate = {2023-11-11},
	journal = {Инженерный Вестник Дона},
	author = {Левшов, Д. И. and Авраменко, М. В. and Пимонов, В. В.},
	month = jun,
	year = {2014},
	keywords = {⛔ No DOI found},
	pages = {1--14},
	file = {Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\ZAP3J5ZW\\2680.html:text/html},
}



@article{__2014-3,
	title = {Температурная зависимость двухмагнонных возбуждений в пленках феррита висмута легированного неодимом},
	url = {http://www.ivdon.ru/ru/magazine/archive/N4y2014/2681},
	abstract = {Сетевой научный журнал «Инженерный вестник Дона»},
	language = {ru},
	urldate = {2023-11-11},
	author = {Кхабири, Г. and Разумная, А. Г. and Юзюк, Ю. И.},
	month = may,
	year = {2014},
	keywords = {⛔ No DOI found},
	file = {Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\NBC8JXKZ\\2681.html:text/html},
}



@article{kadyrov_terahertzinfrared_2014,
	title = {Terahertz–infrared electrodynamics of overdoped manganites {La}$_{\textrm{1–x}}${Ca}$_{\textrm{x}}${MnO}$_{\textrm{3}}$},
	volume = {87},
	issn = {0141-1594},
	url = {https://doi.org/10.1080/01411594.2014.953508},
	doi = {10.1080/01411594.2014.953508},
	abstract = {We have measured low-temperature terahertz and infrared spectra of La1–xCa xMnO3 with x = 0.5; 0.6; 2/3, 0.7; 3/4, 0.85; 0.9; 0.95; 0.98 and x = 1 in the form of ceramics and epitaxial films. In the charge-ordered state for commensurate dopings (x = 2/3 and 3/4), we observed an absorption band at frequencies corresponding to the position of the lowest energy van Hove singularity in the folded Brillouin zone. The band is assigned to the boson peak. We observed qualitatively the same boson peak in Raman spectra of La1/3Ca2/3MnO3 ceramics. In antiferromagnetic phase, for the 0.5 ≤ x {\textless} 0.85 range of doping, the conductivity mechanism gradually changes from a hopping-like transport at low temperatures to the Drude behavior at elevated temperatures in the paramagnetic phase. For 0.85 ≤ x {\textless} 1 (canted antiferromagnetic phase), the electrons behave as Drude-like carriers in the whole temperature interval 5–300 K.},
	number = {10-11},
	urldate = {2023-11-11},
	journal = {Phase Transitions},
	author = {Kadyrov, Lenar S. and Gorshunov, Boris P. and Zhukova, Elena S. and Torgashev, Victor I. and Prokhorov, Anatoly S. and Motovilova, Elizaveta A. and Fischgrabe, Florian and Moshnyaga, Vasily T. and Zhang, Tao and Kremer, Reinhard K. and Pracht, Uwe and Zapf, Sina and Pokorný, Jan and Untereiner, Gabriele and Kamba, Stanislav and Dressel, Martin},
	month = nov,
	year = {2014},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/01411594.2014.953508},
	keywords = {manganites, terahertz},
	pages = {1050--1059},
}



@article{yuzyuk_phase_2014,
	title = {Phase transitions in {BaTiO}$_{\textrm{3}}$ thin films and {BaTiO}$_{\textrm{3}}$/{BaZrO}$_{\textrm{3}}$ superlattices},
	volume = {116},
	issn = {0021-8979},
	url = {https://doi.org/10.1063/1.4901207},
	doi = {10.1063/1.4901207},
	abstract = {Using pulsed laser deposition, we grew a ferroelectric [BaTiO3]Λ/2/[BaZrO3]Λ/2 (BT/BZ) superlattice with a stacking periodicity of Λ = 256 Å and a BT single film on a La1/2Sr1/2CoO3-buffered (001)MgO substrate, and then studied the phase transitions of these materials. At room temperature, the polarized Raman spectra of the BT film corresponded to a ferroelectric orthorhombic C2V14 phase with the polar axis oriented in the plane of the substrate. A ferroelectric-paraelectric phase transition in the BT film occurred at ∼450 K. Upon cooling to ∼300 K, a phase transition to the monoclinic Cs3 phase occurred. These experimental results agree well with a theoretical “temperature-misfit strain” phase diagram of the BT film. We found no evidence of phase transitions in the BT/BZ superlattice below room temperature. The phase transition to the paraelectric phase in the BT/BZ superlattice increased in temperature because of lattice mismatch between the BT and BZ layers. A desirable Curie temperature can be tailored rather precisely by varying the layer thicknesses or the BT/BZ ratio in the superlattice. The BT/BZ superlattices are very good for device applications because their ferroelectric phase with in-plane polarization can remain stable at least from 0 K up to 723 K, and even at higher temperatures in superlattices with smaller periodicities.},
	number = {18},
	urldate = {2023-11-11},
	journal = {Journal of Applied Physics},
	author = {Yuzyuk, Yu. I. and Sakhovoy, R. A. and Maslova, O. A. and Shirokov, V. B. and Zakharchenko, I. N. and Belhadi, J. and El Marssi, M.},
	month = nov,
	year = {2014},
	pages = {184102},
}



@article{shirokov_optical_2014,
	title = {Optical properties of the {Ba}$_{\textrm{0.8}}${Sr}$_{\textrm{0.2}}${TiO}$_{\textrm{3}}$/({Bi}$_{\textrm{0.82}}$, {Nd}$_{\textrm{0.02}}$){FeO}$_{\textrm{3}}$ superlattice},
	volume = {59},
	issn = {1090-6525},
	url = {https://doi.org/10.1134/S1063784214040239},
	doi = {10.1134/S1063784214040239},
	abstract = {A Ba0.8Sr0.2TiO3/(Bi0.82, Nd0.02)FeO3 multilayer heteroepitaxial structure is prepared by successively depositing 20 Ba0.8Sr0.2TiO3 and (Bi0.82, Nd0.02)FeO3 layers, each 4 nm thick, using the method of rf sputtering. The layers grow on a single-crystal MgO substrate following the layer-by-layer mechanism. The structural perfection of the layers is examined by X-ray diffraction. The optical transmission is studied in the wavelength interval 200–1100 nm. The spectra are processed using a dispersion formula for the permittivity represented as a superposition of two oscillators with regard to relaxation. Such an approach allows us to separate direct and indirect transitions. The absorption edge of the superlattice for direct transitions is 80 nm wide and is estimated to be 3.78 eV.},
	language = {en},
	number = {4},
	urldate = {2023-11-11},
	journal = {Technical Physics},
	author = {Shirokov, V. B. and Golovko, Yu. I. and Mukhortov, V. M. and Revinskii, Yu. V.},
	month = apr,
	year = {2014},
	keywords = {Barium Strontium, Barium Strontium Titanate, Multilayer Structure, Strontium Titanate, Wavelength Interval},
	pages = {571--575},
}



@article{gagou_nature_2014,
	title = {On the nature of phase transitions in the tetragonal tungsten bronze {GdK}$_{\textrm{2}}${Nb}$_{\textrm{5}}${O}$_{\textrm{15}}$ ceramics},
	volume = {115},
	issn = {0021-8979},
	url = {https://doi.org/10.1063/1.4865741},
	doi = {10.1063/1.4865741},
	abstract = {Phase transitions in gadolinium potassium niobate GdK2Nb5O15 (GKN) ceramics have been investigated by x-ray diffraction, dielectric susceptibility, differential scanning calorimetry, and Raman scattering. The results of our complementary studies show that GKN exhibits two phase transitions at Tc1 = 238 °C and Tc2 = 375 °C attributed to the ferroelectric-antiferroelectric-paraelectric (FE-AFE-PE) phase transitions. According to the x-ray diffraction analysis, the FE and PE phases were refined in the polar P4bm and centrosymmetric P4/mbm space groups. For the intermediate phase, the structure is refined in the space group P4nc with doubling of the c unit cell parameter, which is compatible with an AFE phase. This result was confirmed by Raman spectroscopy since new low-frequency lines are activated in the AFE phase due to the Brillouin zone-folding effect, typical for the modulated phases. The presence of the AFE phase between the FE and PE phases and the complex nature of tetragonal tungsten bronze crystal structure can explain the large thermal hysteresis observed at the FE-AFE transition between heating and cooling cycle and the strong depression of the Curie-Weiss temperature T0. The semi-phenomenological Ising-like model based on the obtained experimental data is proposed to account for the observed FE-AFE-PE transition sequence.},
	number = {6},
	urldate = {2023-11-11},
	journal = {Journal of Applied Physics},
	author = {Gagou, Y. and Amira, Y. and Lukyanchuk, I. and Mezzane, D. and Courty, M. and Masquelier, C. and Yuzyuk, Yu. I. and El Marssi, M.},
	month = feb,
	year = {2014},
	pages = {064104},
	file = {Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\4WTIXGZJ\\On-the-nature-of-phase-transitions-in-the.html:text/html},
}



@article{mikheykin_lattice_2014,
	title = {Lattice anharmonicity and polar soft mode in ferrimagnetic {M}-type hexaferrite {BaFe}$_{\textrm{12}}${O}$_{\textrm{19}}$ single crystal},
	volume = {87},
	issn = {1434-6036},
	url = {https://doi.org/10.1140/epjb/e2014-50329-4},
	doi = {10.1140/epjb/e2014-50329-4},
	abstract = {The polar phonon modes in BaFe12O19 single crystal are studied in the temperature rangefrom 6 to 300 K by polarized infrared spectroscopy. The phonon spectrum of the crystal isstrongly anharmonic and unstable with respect to long-wavelength fluctuations ofthe dielectric permittivity along the hexagonal axis. Our results suggests that inBaFe12O19 hexaferrite symmetry lowering to the polar phase withthe space group P63mc can beexpected.},
	language = {en},
	number = {10},
	urldate = {2023-11-11},
	journal = {The European Physical Journal B},
	author = {Mikheykin, Alexey S. and Zhukova, Elena S. and Torgashev, Viktor I. and Razumnaya, Anna G. and Yuzyuk, Yury I. and Gorshunov, Boris P. and Prokhorov, Anatoly S. and Sashin, Aleksandr E. and Bush, Alexandr A. and Dressel, Martin},
	month = oct,
	year = {2014},
	keywords = {Solid State and Materials},
	pages = {232},
}



@article{li_investigations_2014,
	title = {Investigations of {Ba}$_{\textrm{x}}${Sr}$_{\textrm{1−x}}${TiO}$_{\textrm{3}}$ ceramics and powders prepared by direct current arc discharge technique},
	volume = {105},
	issn = {0003-6951},
	url = {https://doi.org/10.1063/1.4894456},
	doi = {10.1063/1.4894456},
	abstract = {BaxSr1−xTiO3 ceramics with x ranging from 0 to 1 were prepared by direct current arc discharge technique and studied by means of x-ray diffraction (XRD) and Raman spectroscopy. The cubic-tetragonal ferroelectric phase transition in BaxSr1−xTiO3 ceramics was found to occur at x ≈ 0.75. XRD investigation of as-grown BaTiO3 ceramics revealed co-existence of tetragonal and hexagonal modifications with a small amount of impurity phase BaTi4O9. No evidences of hexagonal phase were observed in Raman spectra of as-grown BaTiO3 ceramics, while Raman peaks related to hexagonal phase were clearly observed in the spectrum of fine-grain powders prepared from the same ceramics. A core-shell model for BaTiO3 ceramics prepared by direct current arc discharge technique is proposed. Absence of the hexagonal phase in any BaxSr1−xTiO3 solid solution with x \&lt; 1 is discussed in the frame of specific atomic arrangement.},
	number = {9},
	urldate = {2023-11-11},
	journal = {Applied Physics Letters},
	author = {Li, Shuangbin and Yao, Ying and Yuzyuk, Yu. I. and Jia, Yongzhong and Wang, Xiaohan and Xie, Shaolei and Jing, Yan},
	month = sep,
	year = {2014},
	pages = {092901},
}



@article{belhadi_highly_2014,
	title = {Highly constrained ferroelectric [{BaTiO}$_{\textrm{3}}$]$_{\textrm{(1−x)Λ}}$/[{BaZrO}$_{\textrm{3}}$]$_{\textrm{{xΛ}}}$ superlattices: {X}-ray diffraction and {Raman} spectroscopy},
	volume = {116},
	issn = {0021-8979},
	shorttitle = {Highly constrained ferroelectric [{BaTiO3}](1−x)Λ/[{BaZrO3}]{xΛ} superlattices},
	url = {https://doi.org/10.1063/1.4890513},
	doi = {10.1063/1.4890513},
	abstract = {We report an x-ray diffraction (XRD) and a Raman-scattering investigation of ferroelectric/paraelectric superlattices [BaTiO3] (1−x)Λ/[BaZrO3]xΛ for which the composition varied, 0.15 ≤ x ≤ 0.85, while the superlattice (SL) modulation period Λ was kept constant at about 100 Å. The samples were epitaxially grown by pulsed laser deposition on MgO substrates buffered with La0.5Sr0.5CoO3. Based on the XRD analysis and on polarized Raman spectra, we have showed that the large strain in SLs induced ferroelectricity in BaZrO3 (BZ) for all SLs, a material that is paraelectric in the bulk form at any temperature and in the single film. The induced polar axis in BZ layers is perpendicular to the plane of substrate while BaTiO3 (BT) layers exhibit in-plane polar orientation. Raman spectroscopy revealed a lattice ordering in SLs due to the misfit strain generated by the large lattice mismatch between the alternating BZ and BT layers. This strain induced a huge upward frequency of the lowest E(1TO) soft mode from 60 cm−1 in the BT single film to 215 cm−1 in the SL with x = 0.85. These results show that in spite of relatively large periodicity of SLs, they are highly constrained and the variation of BZ ratio allowed modifying strains between layers. The temperature dependence of the Raman spectra for BT0.3Λ/BZ0.7Λ and BT0.7Λ/BZ0.3Λ samples revealed giant shift of the ferroelectric phase transition. The phase transition temperature was found to be upshifted by about 300 °C with respect to BT single crystal.},
	number = {3},
	urldate = {2023-11-11},
	journal = {Journal of Applied Physics},
	author = {Belhadi, J. and El Marssi, M. and Gagou, Y. and Yuzyuk, Yu. I. and El Mendili, Y. and Raevski, I. P. and Bouyanfif, H. and Wolfman, J.},
	month = jul,
	year = {2014},
	pages = {034108},
}



@article{belhadi_giant_2014,
	title = {Giant increase of ferroelectric phase transition temperature in highly strained ferroelectric [{BaTiO}$_{\textrm{3}}$]$_{\textrm{0.{7Λ}}}$/[{BaZrO}$_{\textrm{3}}$]$_{\textrm{0.{3Λ}}}$ superlattice},
	volume = {106},
	issn = {0295-5075},
	url = {https://dx.doi.org/10.1209/0295-5075/106/17004},
	doi = {10.1209/0295-5075/106/17004},
	abstract = {We report epitaxial strain effects in the lead-free ferroelectric/paraelectric superlattice (SL) for a modulation period Λ of about 100 Å. We have demonstrated that the large strain in SL induces ferroelectricity in BaZrO3 layers, a material that is paraelectric at any temperature in the bulk form. The induced polar axis in BaZrO3 layers is perpendicular to the plane of the substrate while BaTiO3 layers exhibit in-plane polar orientation. Raman spectroscopy revealed a lattice ordering in SL due to the misfit strain generated by the large lattice mismatch between the alternating BaZrO3 and BaTiO3 layers. Such strain induces a huge upward frequency shift of the lowest E(1TO) soft mode from in the BaTiO3 single film to in the SL. The temperature of the ferroelectric phase transition in the SL was found to be upshifted by about with respect to the BaTiO3 single crystal.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Europhysics Letters},
	author = {Belhadi, J. and Marssi, M. El and Gagou, Y. and Yuzyuk, Yu I. and Raevski, I. P.},
	month = apr,
	year = {2014},
	note = {Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica},
	pages = {17004},
}



@article{kochur_chemical_2014,
	title = {Chemical bonding and valence state of 3d-metal ions in {Ni}$_{\textrm{1−x}}${Co}$_{\textrm{x}}${Cr}$_{\textrm{2}}${O}$_{\textrm{4}}$ spinels from {X}-ray diffraction and {X}-ray photoelectron spectroscopy data},
	volume = {195},
	issn = {0368-2048},
	url = {https://www.sciencedirect.com/science/article/pii/S0368204814001583},
	doi = {10.1016/j.elspec.2014.07.010},
	abstract = {Ni1−xCoxCr2O4 solid solution samples with х=0, 0.005, 0.01, 0.02, 0.3, 0.5, 0.8 and 1 are studied by the methods of X-ray diffraction and X-ray photoelectron spectroscopy (XPS). Ni2p3/2,1/2, Co2p3/2,1/2, Cr2p3/2,1/2, and O1s spectra are measured. The spectra are calculated with allowance for multiplet splitting, crystal field, and charge-transfer effect. Ni2+ ions are found to be present in tetrahedral and octahedral positions. Relative numbers of Ni2+ ions in tetrahedral and octahedral sites are determined via fitting the experimental spectra with superposition of the spectra of Ni2+ ions calculated in tetrahedral and octahedral crystal field. Cobalt ions are bivalent and occupy mostly tetrahedral sites. Chromium ions are trivalent and occupy predominantly octahedral positions. However, due to a defective lattice, the samples may contain Cr ions in non-equivalent states, either chemically or structurally.},
	urldate = {2023-11-11},
	journal = {Journal of Electron Spectroscopy and Related Phenomena},
	author = {Kochur, A. G. and Kozakov, A. T. and Googlev, K. A. and Mikheykin, A. S. and Torgashev, V. I. and Bush, A. A. and Nikolskii, A. V.},
	month = aug,
	year = {2014},
	keywords = {X-ray diffraction, Crystal structure, NiCoCrO spinels, Valence state, XPS},
	pages = {208--219},
}



@article{__2014-4,
	title = {Экспериментальное и теоретическое исследование массивов наностержней {ZnO}, покрытых пленкой серебра, как антенн оптического и ближнего ИК-диапазона},
	volume = {40},
	url = {http://journals.ioffe.ru/articles/27360},
	abstract = {Предложена новая конструкция оптической антенны - наностержень ZnO, покрытый тонкой металлической пленкой. Методами карботермического синтеза и магнетронного напыления получены решетки высокоориентированных перпендикулярно подложке наностержней оксида цинка, покрытых тонкой пленкой серебра. Решены задачи дифракции электромагнитных волн на одиночном металлодиэлектрическом нановибраторе, расположенном на границе раздела диэлектриков и на двумерно-периодической решетке нановибраторов. Проведено сравнение расчетов электродинамических характеристик оптических наноантенн различной длины с экспериментально полученными.},
	language = {ru},
	number = {7},
	urldate = {2023-11-11},
	journal = {Письма в ЖТФ},
	author = {Кайдашев, Е. М. and Лянгузов, Н. В. and Лерер, А. М. and Распопова, Е. А.},
	month = mar,
	year = {2014},
	pages = {79--86},
}



@article{__2013-8,
	title = {Оптические свойства эпитаксиальных тонких пленок {BiFeO3}},
	volume = {84},
	url = {http://journals.ioffe.ru/articles/27131},
	abstract = {Исследованы свойства наноразмерных пленок BiFeO3, допированных неодимом, на монокристаллических подложках оксида магния, полученных методом высокочастотного распыления по слоевому механизму роста. Структурное совершенство пленок изучено методами рентгеновской дифракции. Пропускание пленок различной толщины исследовано в диапазоне длин волн 200-1100 nm. Спектры обработаны с использованием дисперсионной формулы для диэлектрической проницаемости в виде суммы осцилляторов с учетом релаксации, что позволило выделить прямые и непрямые переходы. Край поглощения оценен для прямых переходов как 2.81 и 2.78 eV для пленок толщиной 14 и 60 nm соответственно.},
	language = {ru},
	number = {1},
	urldate = {2023-11-11},
	journal = {Журнал технической физики},
	author = {Широков, В. Б. and Головко, Ю. И. and Мухортов, В. М.},
	month = dec,
	year = {2013},
	pages = {104--108},
}



@inproceedings{__2019-1,
	address = {Тула},
	title = {Сферические упаковки в оболочках вирусов, эпителиальных монослоях и коллоидных кристаллах},
	shorttitle = {Алгебра, теория чисел и дискретная геометрия},
	url = {https://elibrary.ru/item.asp?id=39552125},
	language = {ru},
	urldate = {2023-11-11},
	booktitle = {Материалы {XVI} Международной конференции,  посвященной 80-летию со дня рождения  профессора Мишеля Деза},
	publisher = {Тульский государственный педагогический университет им. Л.Н. Толстого},
	author = {Рошаль, Д. С.},
	year = {2019},
	pages = {2},
}



@inproceedings{vakhrushev_temperature_2021,
	address = {St. Petersburg, Russian Federation},
	title = {Temperature {Evolution} of {Inelastic} {Synchrotron} {Radiation} {Scattering} in {PbZr} $_{\textrm{0.985}}${Ti}$_{\textrm{0.015}}${O}$_{\textrm{3}}$ in the {Vicinity} of {M}-{Point}},
	isbn = {978-1-66544-972-4},
	url = {https://ieeexplore.ieee.org/document/9614882/},
	doi = {10.1109/EExPolytech53083.2021.9614882},
	urldate = {2023-11-10},
	booktitle = {2021 {International} {Conference} on {Electrical} {Engineering} and {Photonics} ({EExPolytech})},
	publisher = {IEEE},
	author = {Vakhrushev, Sergey B. and Leontyev, Igor N. and Bosak, Alexey and Udovenko, Stanislav A. and Petroukhno, Konstantin A.},
	month = oct,
	year = {2021},
	pages = {143--145},
}



@article{redina_characteristics_2021,
	title = {Characteristics of {Carbon} {Nanotubes} {Synthesized} from {Methane} and {Acetylene} in the {Presence} of a {FeCl}$_{\textrm{3}}$ {Catalyst}},
	volume = {66},
	issn = {1063-7842, 1090-6525},
	url = {http://link.springer.com/10.1134/S106378422103021X},
	doi = {10.1134/S106378422103021X},
	language = {en},
	number = {3},
	urldate = {2023-11-10},
	journal = {Technical Physics},
	author = {Redina, A. G. and Avramenko, M. V. and Lyanguzov, N. V.},
	month = mar,
	year = {2021},
	pages = {445--452},
}



@article{__2014-5,
	title = {Исследование динамики решетки макро-, микро- и наноструктурированного титаната бария методом спектроскопии комбинационного рассеяния света},
	volume = {56},
	url = {http://journals.ioffe.ru/articles/26768},
	language = {ru},
	number = {2},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Маслова, О. А. and Широков, В. Б. and Юзюк, Ю. И. and Marssi, M. El and Jain, M. and Ortega, N. and Katiyar, R. S.},
	month = jan,
	year = {2014},
	pages = {308--314},
}



@article{__2013-9,
	title = {Динамический спектральный отклик твердых растворов висмут-стронциевого феррита {Bi}$_{\textrm{1-x}}${Sr}$_{\textrm{x}}${FeO}$_{\textrm{3-delta}}$ в диапазоне частот 0.3-200 {THz}},
	volume = {55},
	url = {http://journals.ioffe.ru/articles/1093},
	language = {ru},
	number = {7},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Анохин, А. С. and Разумная, А. Г. and Торгашев, В. И. and Троценко, В. Г. and Юзюк, Ю. И. and Буш, А. А. and Шкуратов, В. Я. and Горшунов, Б. П. and Жукова, Е. С. and Кадыров, Л. С. and Командин, Г. А.},
	month = jun,
	year = {2013},
	pages = {1320--1332},
}



@article{__2013-10,
	title = {Теплоемкость наноструктурированной керамики {BaTiO}$_{\textrm{3}}$},
	volume = {55},
	url = {http://journals.ioffe.ru/articles/1045},
	abstract = {Исследована температурная зависимость теплоемкости наноструктурированной керамики BaTiO3, полученной твердофазным методом, спеканию которой предшествовала обработка при комнатной температуре синтезированной шихты в наковальнях Бриджмена силовым воздействием в сочетании со сдвиговой деформацией. Обнаружено существенное размытие сегнетоэлектрического перехода и нелинейное убывание температуры фазового перехода с увеличением приложенного давления. Показано, что дефектная структура играет доминирующую роль в формировании физических свойств керамики.},
	language = {ru},
	number = {5},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Каллаев, С. Н. and Омаров, З. М. and Бакмаев, А. Г. and Абдулвахидов, К. Г.},
	month = apr,
	year = {2013},
	pages = {1011--1013},
}



@article{__2013-11,
	title = {Материальные константы твердых растворов ({Ba},{Sr}){TiO}$_{\textrm{3}}$},
	volume = {55},
	url = {http://journals.ioffe.ru/articles/998},
	abstract = {Феноменологическая теория твердого раствора использована для вычисления поведения материальных констант (упругих податливостей, восприимчивостей, пьезоэлектрических модулей, пироэлектрических коэффициентов) твердого раствора BaxSr1-xTiO3 во всей области изменения концентраций x при комнатной температуре. Для выделенных концентраций приведены константы феноменологического потенциала и численные значения материальных констант.},
	language = {ru},
	number = {4},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Широков, В. Б. and Юзюк, Ю. И. and Калинчук, В. В. and Леманов, В. В.},
	month = mar,
	year = {2013},
	pages = {709--714},
}



@article{__2013-12,
	title = {Теория кристаллизации Ландау и самосборка октагональных квазикристаллов},
	volume = {55},
	url = {http://journals.ioffe.ru/articles/1117},
	abstract = {Предложена теория кристаллизации квазикристаллических структур, не использующая для описания квазикристаллического порядка концепций многомерной кристаллографии. На примере структуры октагонального квазикристалла MnSiAl показано, что координаты узлов соответствующей квазикристаллической решетки (КР) можно рассчитать путем условной минимизации свободной энергии Ландау. Отказ от безусловной минимизации свободной энергии обосновывается особенностями локального атомного порядка в рассматриваемой структуре. Предложенная теория придает новый физический смысл традиционным понятиям многомерной кристаллографии и может быть также применена для объяснения образования квазикристаллических структур с другими КР.},
	language = {ru},
	number = {8},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Коневцова, О. В. and Рошаль, С. Б. and Лорман, В. Л.},
	month = jul,
	year = {2013},
	pages = {1488--1493},
}



@article{__2013-13,
	title = {Особенности диэлектрического спектра {CaCu}$_{\textrm{3}}${Ti}$_{\textrm{4}}${O}$_{\textrm{12}}$ в низкочастотном диапазоне},
	volume = {55},
	url = {http://journals.ioffe.ru/articles/1124},
	abstract = {Представлены диэлектрические спектры керамики CaCu3Ti4O12, отличающейся гигантскими значениями диэлектрической проницаемости. В высокочастотной части спектра в области 106-107 Hz проявляется дисперсия дебаевского типа с энергией активации 0.075 eV, а также характерное плато в частотной зависимости диэлектрической проницаемости в области 104-105 Hz. В низкочастотной части спектра наблюдается значительное увеличение фактора потерь varepsilon'', а при частоте менее 10-2 Hz в некоторых образцах обнаружен переход от импеданса емкостного типа к индуктивному. Обсуждаются причины такого перехода.},
	language = {ru},
	number = {8},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Гавриляченко, В. Г. and Кабиров, Ю. В. and Панченко, Е. М. and Ситало, Е. И. and Гавриляченко, Т. В. and Милов, Е. В. and Лянгузов, Н. В.},
	month = jul,
	year = {2013},
	pages = {1540--1543},
}



@article{gorshunov_boson_2013,
	title = {Boson peak in overdoped manganites {La}$_{\textrm{1-x}}${Ca}$_{\textrm{x}}${MnO}$_{\textrm{3}}$},
	volume = {87},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.87.245124},
	doi = {10.1103/PhysRevB.87.245124},
	abstract = {In the charge-ordered phase of strongly doped manganites La1−xCaxMnO3 (x≥0.5) absorption lines appear in the terahertz spectral range for commensurate x values right below the charge-ordering temperature. They are connected to acoustic phonons that become optically active by folding of the Brillouin zone. At lower temperatures a strongly asymmetric extra absorption band develops at frequencies corresponding to the position of the lowest-energy van Hove singularity in the reduced Brillouin zone. The band is assigned to the boson peak, i.e., to the excess of lattice vibrational states over the standard Debye contribution. The folded phonons and the boson peak do not show up for incommensurate calcium contents when no distinct Brillouin zone folding exists.},
	number = {24},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Gorshunov, B. and Zhukova, E. and Torgashev, V. I. and Kadyrov, L. S. and Motovilova, E. A. and Fischgrabe, F. and Moshnyaga, V. and Zhang, T. and Kremer, R. and Pracht, U. and Zapf, S. and Dressel, M.},
	month = jun,
	year = {2013},
	note = {Publisher: American Physical Society},
	pages = {245124},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\G3SEUD2M\\Gorshunov и др. - 2013 - Boson peak in overdoped manganites La\$ _ 1ensure.pdf:application/pdf},
}



@article{kozakov_chemical_2013,
	title = {Chemical bonding in the {Bi}$_{\textrm{1−x}}${Sr}$_{\textrm{x}}${FeO}$_{\textrm{3±y}}$ system by {X}-ray photoelectron and {Mössbauer} spectroscopy},
	volume = {189},
	issn = {0368-2048},
	url = {https://www.sciencedirect.com/science/article/pii/S0368204813001369},
	doi = {10.1016/j.elspec.2013.08.006},
	abstract = {Ceramic samples Bi1−xSrxFeO3±y are synthesized with 0≤x≤1 by the solid state reaction method. X-ray diffraction study of the samples is performed. Chemical bonding and the valence state of the Fe ions in the Bi1−xSrxFeO3±y ceramics are studied using X-ray photoelectron Fe2p-, Sr3d-, Bi4f-, and O1s-spectra, and Mössbauer spectroscopy. Fe2p-spectra for various ionic states of Fe are calculated in an isolated ion approximation. Considerable deviations of actual elemental compositions from nominal ones are discovered. Both Fe3+ and Fe4+ ions are found to be present in the samples with x{\textgreater}0. Relative Fe3+/Fe4+ contents are determined by comparing the parameters of experimental and theoretical Fe2p-spectra. Concentration of Fe4+ ions in the samples correlates with that of the Sr atoms.},
	urldate = {2023-11-11},
	journal = {Journal of Electron Spectroscopy and Related Phenomena},
	author = {Kozakov, A. T. and Kochur, A. G. and Torgashev, V. I. and Bush, A. A. and Shkuratov, V. Ya. and Kubrin, S. P. and Nikolskii, A. V. and Googlev, K. A.},
	month = aug,
	year = {2013},
	keywords = {X-ray diffraction, BiSrFeO ceramics, Fe valence state, Mössbauer spectra, X-ray photoelectron spectra},
	pages = {106--115},
}



@article{ortega_compositional_2013,
	title = {Compositional engineering of {BaTiO}$_{\textrm{3}}$/({Ba},{Sr}){TiO}$_{\textrm{3}}$ ferroelectric superlattices},
	volume = {114},
	issn = {0021-8979},
	url = {https://doi.org/10.1063/1.4820576},
	doi = {10.1063/1.4820576},
	abstract = {Epitaxial strain is one of the major factors influencing physical properties of artificial superlattice (SL) structures. One way to control the local stress in epitaxial films is altering the lattice parameters by doping. Superlattices of BT/Ba(1−x)SrxTiO3 (BT/BST) with x = (0, 0.3, 0.4, 0.5, 0.6, 0.7, 1) with a modulation period of about 80–90 Å were grown on La0.67Sr0.33MnO3 coated (100) MgO substrates by pulsed laser deposition technique. The modulated structure of the thin films was confirmed by x-ray diffraction, Raman spectroscopy, and transmission electron microscopy. The increase in Sr concentration in BST layers of the SLs results in an increase in in-plane (a) and out-plane (c) compressive/tensile misfit strains in the BT/BST layers, respectively. The highest value of the dielectric constant was obtained for BT/Ba0.3Sr0.7TiO3 (BT/BST3070) and BT/Ba0.7Sr0.3TiO3 (BT/BST7030) SLs. Slim, asymmetric, but well-saturated ferroelectric hysteresis loops were observed in all SLs. Additionally, BT/BST SLs exhibited exceptionally high electric field stress sustainability over a wide range of frequency (10 kHz) and temperature (80–350 K). Temperature-dependent dielectric and ferroelectric properties show a ferroelectric relaxor behavior when the Sr content is increased in the BST layer of the SLs. Analysis of polarization versus temperature data using Landau-Devonshire theory suggests a second-order ferroelectric phase transition in these SLs. This structure can therefore be attractive in the design of a new kind of dielectric device capable in both high power and high energy density applications.},
	number = {10},
	urldate = {2023-11-11},
	journal = {Journal of Applied Physics},
	author = {Ortega, N. and Kumar, Ashok and Resto, Oscar and Maslova, O. A. and Yuzyuk, Yu. I. and Scott, J. F. and Katiyar, Ram S.},
	month = sep,
	year = {2013},
	pages = {104102},
}



@article{kamenskyi_observation_2013,
	title = {Observation of an intersublattice exchange magnon in {CoCr}$_{\textrm{2}}${O}$_{\textrm{4}}$ and analysis of magnetic ordering},
	volume = {87},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.87.134423},
	doi = {10.1103/PhysRevB.87.134423},
	abstract = {We report on an investigation of optical properties of multiferroic CoCr2O4 at terahertz frequencies in magnetic fields up to 30 T. Below the ferrimagnetic transition (94 K), the terahertz response of CoCr2O4 is dominated by a magnon mode, which shows a steep magnetic-field dependence. We ascribe this mode to an exchange resonance between two magnetic sublattices with different g factors. In the framework of a simple two-sublattice model (the sublattices are formed by Co2+ and Cr3+ ions), we find the inter-sublattice coupling constant, λ=−(18±1) K, and trace the magnetization for each sublattice as a function of field. We show that the Curie temperature of the Cr3+ sublattice, Θ2 = (49±2) K, coincides with the temperature range, where anomalies of the dielectric and magnetic properties of CoCr2O4 have been reported in literature.},
	number = {13},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Kamenskyi, D. and Engelkamp, H. and Fischer, T. and Uhlarz, M. and Wosnitza, J. and Gorshunov, B. P. and Komandin, G. A. and Prokhorov, A. S. and Dressel, M. and Bush, A. A. and Torgashev, V. I. and Pronin, A. V.},
	month = apr,
	year = {2013},
	note = {Publisher: American Physical Society},
	pages = {134423},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\X6THP5XM\\Kamenskyi и др. - 2013 - Observation of an intersublattice exchange magnon .pdf:application/pdf;APS Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\3GBGXRM2\\PhysRevB.87.html:text/html},
}



@article{shakhovoy_phase_2013,
	title = {Phase {Diagrams} of {BaTiO}$_{\textrm{3}}$/{BaZrO}$_{\textrm{3}}$ {Superlattices}},
	volume = {444},
	issn = {0015-0193},
	url = {https://doi.org/10.1080/10584587.2013.785795},
	doi = {10.1080/10584587.2013.785795},
	abstract = {Temperature-misfit strain phase diagrams of BaTiO3/BaZrO3 superlattices were developed and an alteration of the “misfit strain-temperature” phase diagrams against the changing of ferroelectric layers volume fraction was investigated. The topology of developed phase diagrams is similar to that of single BaTiO3 film, but phase transition lines exhibit substation shifts. According to our approach, the main reason of this shift is the electrostatic interaction between the layers. It is revealed that only one polar phase remains stable in superlattices with volume fraction of BaTiO3 being less than 70\%.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Ferroelectrics},
	author = {Shakhovoy, R. A. and Shirokov, V. B. and Yuzyuk, Yu. I.},
	month = jan,
	year = {2013},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/10584587.2013.785795},
	keywords = {ferroelectric superlattices, Phenomenological theory},
	pages = {168--176},
}



@article{anokhin_raman_2013,
	title = {Raman and {X}-ray diffraction study of ({Ba},{Sr}){TiO}$_{\textrm{3}}$/({Bi},{Nd}){FeO}$_{\textrm{3}}$ multilayer heterostructures},
	volume = {545},
	issn = {0040-6090},
	url = {https://www.sciencedirect.com/science/article/pii/S0040609013013564},
	doi = {10.1016/j.tsf.2013.08.057},
	abstract = {We report synthesis, X-ray diffraction (XRD) and Raman scattering characterisation of epitaxial heterostructures containing alternating (Bi0.98Nd0.02)FeO3 (BNFO) and (Ba0.8Sr0.2TiO3) (BST) layers deposited on (100) MgO substrates. A significant shift of the BST soft mode and partial depolarisation in the Raman spectra of multilayer heterostructures caused by epitaxial strains were observed. Satellite peaks typical for superlattices were observed in the XRD patterns of multilayer heterostructures with layer thicknesses below 30nm. Raman spectra of the BNFO/BST superlattice with a modulation period of 10nm revealed hardening of the soft mode and a dominating symmetric-stretching mode at 705cm−1 due to distortion in FeO6 octahedra enforced by the epitaxial strain in the superlattice.},
	urldate = {2023-11-11},
	journal = {Thin Solid Films},
	author = {Anokhin, A. S. and Bunina, O. A. and Golovko, Yu I. and Mukhortov, V. M. and Yuzyuk, Yu I. and Simon, P.},
	month = oct,
	year = {2013},
	keywords = {Raman spectroscopy, Thin films, Multiferroics, Sputtering, X-ray diffraction superlattices},
	pages = {267--271},
}



@article{belboukhari_studies_2013,
	title = {Studies of {Diffuse} {Phase} {Transition} in {Ferroelectric} {Solid} {Solution} {Pb}$_{\textrm{1-x}}${K}$_{\textrm{2x}}${Nb}$_{\textrm{2}}${O}$_{\textrm{6}}$ (x = 0.1, 0.2, 0.25 and 0.3)},
	volume = {444},
	issn = {0015-0193},
	url = {https://doi.org/10.1080/00150193.2013.786619},
	doi = {10.1080/00150193.2013.786619},
	abstract = {New compositions of Tetragonal Tungsten Bronze (TTB) ferroelectrics Pb1-xK2xNb5O15 (PKN) with x = 0.1, 0.2, 0.25 and 0.3 were synthesized using the solid state reaction method. Structural and electrical properties were examined as a function of the ratio Pb/K using X-ray diffraction, Raman spectroscopy and dielectric measurements. The dielectric permittivity and the loss tangent of each composition have been measured in a frequency range 10 Hz–1 MH and in a temperatures range 25–600°C. It was shown that the Pb substitution induces the diffuse phase transition.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Ferroelectrics},
	author = {Belboukhari, A. and Abkhar, Z. and Choukri, E. and Gagou, Y. and Abdelmoula, N. and Elmoznine, R. and Mezzane, D. and Khemakhem, H. and Marssi, M. El and Razumnaya, A. and Raevski, I. and Luk'yanchuk, I.},
	month = jan,
	year = {2013},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/00150193.2013.786619},
	keywords = {dielectric spectroscopy, Ferroelectrics, phase transition, TTB compounds},
	pages = {116--124},
}



@article{komandin_terahertz-infrared_2013,
	title = {Terahertz-infrared spectra of the rare-earth scandate {DyScO}$_{\textrm{3}}$ single crystal},
	volume = {114},
	issn = {0021-8979},
	url = {https://doi.org/10.1063/1.4813496},
	doi = {10.1063/1.4813496},
	abstract = {Terahertz and infrared spectra of the optical response of DyScO3 single crystal are measured at temperatures from 5 K to 300 K for two different polarizations E‖[1¯01] and E‖[010], i.e., along the two crystallographic directions of the DyScO3 substrates used for growing of thin films and heterostructures. Detailed reference data on the terahertz dielectric characteristics of the DyScO3 substrate are presented. We discuss the mechanisms responsible for electromagnetic absorption. Phonon spectra are analyzed along with the results of group-theoretical analysis of the crystal structure. Besides phonon modes, additional resonance absorptions are found and assigned to the electronic transitions between Kramers doublets in the three lowest-energy terms of the Dy3+ ion.},
	number = {2},
	urldate = {2023-11-11},
	journal = {Journal of Applied Physics},
	author = {Komandin, G. A. and Zhukova, E. S. and Torgashev, V. I. and Boris, A. V. and Boris, A. A. and Motovilova, E. A. and Prokhorov, A. S. and Kadyrov, L. S. and Gorshunov, B. P. and Dressel, M.},
	month = jul,
	year = {2013},
	pages = {024102},
}



@article{__2013-14,
	title = {Индуцированный электрическим полем фазовый переход в релаксорной керамике на основе {PMN}--{PT}},
	volume = {55},
	url = {http://journals.ioffe.ru/articles/929},
	abstract = {Методами рентгеновской дифрактометрии и атомно-силовой микроскопии проанализированы механизмы формирования плато на зависимостях реверсивной диэлектрической проницаемости от величины напряженности внешнего электрического поля в керамическом образце системы yPZN-mPMN-nPNN-xPT (x=0,3, y =0.0982, m = 0.4541, n = 0.1477). Показано, что в электрических полях, соответствующих аномалии диэлектрической проницаемости, происходит индуцированный фазовый переход из гетерофазного (тетрагонального+псевдокубического) в монофазное (тетрагональное) состояние. При этом наблюдаются значительные деформации тетрагональной ячейки (до 0.1\%) и прекращение 90o-ных доменных переключений. Представлена качественная модель формирования наблюдаемой диэлектрической аномалии, основанная на выделении двух процессов, протекающих при увеличении напряженности электрического поля: роста полярных областей тетрагональной фазы и их переключения.},
	language = {ru},
	number = {2},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Таланов, М. В. and Бунина, О. А. and Бунин, М. А. and Захарченко, И. Н. and Резниченко, Л. А.},
	month = jan,
	year = {2013},
	pages = {288--294},
}



@article{zakharchenko_x-ray_2013,
	title = {X-ray {Diffraction} {Study} of {BaTiO}$_{\textrm{3}}$/({Ba}$_{\textrm{1-x}}${Sr}$_{\textrm{x}}$){TiO}$_{\textrm{3}}$ {Artificial} {Superlattices}},
	volume = {444},
	issn = {0015-0193},
	url = {https://doi.org/10.1080/00150193.2013.785833},
	doi = {10.1080/00150193.2013.785833},
	abstract = {We report x-ray diffraction investigation of two sets of artificial BaTiO3/Ba1-x Sr x TiO3 (BT/BST-x) superlattices (SLs) grown on MgO substrates. The first set of SLs was deposited with the constant periodicity (about 150 Å) and the variable Ba/Sr content in BST layers. In the second set, the modulation period Λ was varied between 30 Å {\textless} Λ {\textless} 110 Å while Ba content was equal 0 in BST layers. It is shown that, fabrication of the artificial SLs with variable composition of the constituting layers even with large modulation period may provide enhanced variation of the ferroelectric properties comparing to the SLs with variable layers thickness.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Ferroelectrics},
	author = {Zakharchenko, I. N. and Bunina, O. A. and Maslova, O. A. and Yuzyuk, Yu. I. and Ortega, N. and Kumar, A. and Katiyar, R. S.},
	month = jan,
	year = {2013},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/00150193.2013.785833},
	keywords = {ferroelectric superlattices, X-ray diffraction},
	pages = {1--8},
}



@article{__2013-15,
	title = {Методы синтеза {LaMnO}$_{\textrm{3}}$ (обзор)},
	url = {http://www.ivdon.ru/magazine/archive/n2y2013/1724},
	abstract = {Сетевой научный журнал «Инженерный вестник Дона»},
	language = {ru},
	urldate = {2023-11-11},
	author = {Рудская, А. Г. and Власенко, М. П. and Чаговец, С. В. and Назаренко, А. В. and Тесленко, П. Ю. and Разумная, А. Г. and Кофанова, Н. Б. and Куприянов, М. Ф.},
	month = jan,
	year = {2013},
}



@article{__2013-16,
	title = {Оптимизация карботермического синтеза массивов микро- и наностержней оксида цинка и их морфометрических параметров},
	volume = {39},
	url = {http://journals.ioffe.ru/articles/14597},
	abstract = {Исследовано влияние буферного давления Ar и расстояния до источника вещества на морфометрические параметры массивов вертикально ориентированных нано- и микростержней ZnO, синтезированных карботермическим методом на подложках Si(100) с тонкопленочным подслоем ZnO. Проведены системные исследования бескаталитического роста, а также влияния катализаторов роста, таких как Au и Cu, на процесс формирования и размеры стержней. Продемонстрировано, что катализатор играет роль лишь на начальном этапе, и не участвует в дальнейшем росте стержней в применяемых условиях синтеза. Показана возможность управления средними диаметрами, длинами и плотностью поверхностного распределения стержней в диапазонах 100-300 nm, 1.5-9 mum и 2.8-5.3· 108 cm-2 соответственно.},
	language = {ru},
	number = {17},
	urldate = {2023-11-11},
	journal = {Письма в ЖТФ},
	author = {Лянгузов, Н. В. and Кайдашев, Е. М. and Захарченко, И. Н. and Бунина, О. А.},
	month = aug,
	year = {2013},
	pages = {27--34},
}



@article{__2013-17,
	title = {Структура и динамика решетки гетероструктур на основе феррита висмута и титаната бария-стронция},
	volume = {55},
	url = {http://journals.ioffe.ru/articles/1254},
	abstract = {Исследования морфологии поверхности, параметров решетки и спектров комбинационного рассеяния выполнены на этапах последовательного формирования трехслойной гетероструктуры, состоящей из эпитаксиальных слоев Ba0.8Sr0.2TiO3 (BST) и (Bi0.98Nd0.02)FeO3 (BNFO). Методами рентгенографии определены структурные искажения, возникающие при последовательном осаждении слоев BST/BNFO/BST равной толщины. Обнаружено, что степень тетрагонального искажения пленки BST на MgO повышается после осаждения на ее поверхность пленки BNFO, что свидетельствует о появлении в BST сжимающих напряжений. На основании анализа поляризованных спектров КРС показано, что в слое BNFO наблюдается новое фазовое состояние, не реализующееся в объемных образцах. Показано, что в пленке BST, выращенной на поверхности BNFO степень тетрагональности оказывается выше, чем в такой же пленке, выращенной непосредственно на MgO.},
	language = {ru},
	number = {12},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Кхабири, Г. and Анохин, А. С. and Бунина, О. А. and Головко, Ю. И. and Мухортов, В. М. and Широков, В. Б. and Юзюк, Ю. И. and Simon, P.},
	month = nov,
	year = {2013},
	pages = {2383--2391},
}



@article{__2012-4,
	title = {Спектры комбинационного рассеяния керамик, пленок и сверхрешеток сегнетоэлектрических перовскитов (О б з о р)},
	url = {http://journals.ioffe.ru/articles/598},
	urldate = {2023-11-11},
	author = {Юзюк, Ю. И.},
	month = apr,
	year = {2012},
}



@article{__2012-5,
	title = {Сравнительное исследование пленки {BaTiO}$_{\textrm{3}}$ и сверхрешетки {BaTiO}$_{\textrm{3}}$/({Ba}$_{\textrm{0.7}}${Sr}$_{\textrm{0.3}}$){TiO}$_{\textrm{3}}$ методами дифракции рентгеновских лучей и спектроскопии комбинационного рассеяния света},
	volume = {54},
	abstract = {Проведено сравнительное исследование эпитаксиальной пленки BaTiO3 и сверхрешетки состава BaTiO3/(Ba0.7Sr0.3)TiO3, изготовленных методом импульсного лазерного осаждения на подложках (100) MgO. На основе данных рентгеновской дифрактометрии установлена полная параллельная ориентация пленки и подложки, определены период модуляции сверхрешетки Lambda=28 nm, параметры ячейки, усредненной по периоду Lambda, и параметры ячеек слоев сверхрешетки. Согласно рентгенографическим данным, ячейка однокомпонентной пленки BaTiO3 и усредненная по периоду Lambda ячейка сверхрешетки являются псевдокубическими, однако анализ поляризационных характеристик спектров комбинационного рассеяния света позволил предположить моноклинную симметрию (Px=Py\#0, Pz\#0) в пленке и сверхрешетке. Обсуждается трансформация компонент мягкой моды, обусловленная деформацией эпитаксиальных слоев, образующих сверхрешетку.},
	language = {ru},
	number = {8},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Маслова, О. А. and Захарченко, И. Н. and Бунина, О. А. and Юзюк, Ю. И. and Ortega, N. and Kumar, A. and Katiyar, R. S.},
	month = jul,
	year = {2012},
	pages = {1526--1532},
}



@article{__2012-6,
	title = {Влияние морфологии керамик {BiFeO}$_{\textrm{3}}$ на электродинамические свойства в терагерцевом диапазоне частот},
	volume = {54},
	url = {http://journals.ioffe.ru/articles/623},
	abstract = {Методами субмиллиметровой и инфракрасной Фурье-спектроскопии исследована природа вклада, дополнительного к фононному, в диэлектрическую проницаемость керамик феррита висмута. Выявлено, что его численное значение зависит от морфологических особенностей образцов, а природа обусловлена наличием дефектов и межкристаллитных границ. Отмечено влияние структурно-фазовых особенностей керамик феррита висмута на частоты линий антиферромагнитного резонанса.},
	language = {ru},
	number = {6},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Командин, Г. А. and Торгашев, В. И. and Волков, А. А. and Породинков, О. Е. and Пронин, А. А. and Исхакова, Л. Д. and Буш, А. А.},
	month = may,
	year = {2012},
	pages = {1120--1127},
}



@article{__2012-7,
	title = {Магнитный и диэлектрический отклик кобальт-хромовой шпинели {CoCr}$_{\textrm{2}}${O}$_{\textrm{4}}$ в терагерцевой области частот},
	volume = {54},
	url = {http://journals.ioffe.ru/articles/523},
	abstract = {Методами субмиллиметровой спектроскопии и инфракрасной Фурье-спектроскопии исследована природа фононных и магнонных мод в мультиферроике CoCr2O4 со структурой кубической шпинели. Впервые измерена температурная эволюция обменного оптического магнона в ферримагнитной (TC=94 K) и двух низкосимметричных (TS{\textasciitilde} 26 K, Tlock-in=14.5 K) фазах CoCr2O4 вплоть до T=5 K в нулевом магнитном поле. Показано, что зарегистрированный магнон не является ферримагнитным параметром порядка и, вероятнее всего, обусловлен прецессией спинов в подрешетках кобальта. В точках магнитных фазовых переходов осцилляторные параметры двух наиболее низкочастотных фононных мод проявляют аномальную температурную зависимость, что свидетельствует о значительном взаимодействии между магнитной и фононной подсистемами. На основании того, что параметр затухания фононной моды, обусловленной колебаниями тетраэдров CoO4, при переходе CoCr2O4 в состояние мультиферроика (T{\textless}TS) увеличивается на 25\%, сделано предположение о структурных изменениях в решетке с потерей пространственной центросимметричности среды.},
	language = {ru},
	number = {2},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Торгашев, В. И. and Прохоров, А. С. and Командин, Г. А. and Жукова, Е. С. and Анзин, В. Б. and Таланов, В. М. and Рабкин, Л. М. and Буш, А. А. and Dressel, M. and Горшунов, Б. П.},
	month = jan,
	year = {2012},
	pages = {330--339},
}



@article{_-_2012,
	title = {Нелинейно-оптическая микроскопия и спектроскопия сегнетоэлектрических и мультиферроидных материалов},
	volume = {54},
	url = {http://journals.ioffe.ru/articles/840},
	abstract = {Раcсмотрены особенности применения двухфотонной микроскопии и спектроскопии для исследования мультиферроидных и пьезоэлектрических наноразмерных структур. Для наноразмерных планарных мультислойных структур титанат бария-стронция/феррит висмута показано проявление в нелинейно-оптическом отклике локальных электроиндуцированного и магнитоиндуцированного вкладов в определенных спектральных диапазонах. Для пьезоэлектрических био-микротрубок пептидов показано, что максимальное значение интенсивности второй гармоники не меняется вдоль трубки, в то время как направление поляризации изменяется значительно.},
	language = {ru},
	number = {5},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Мишина, Е. Д. and Семин, С. В. and Швырков, К. В. and Кудрявцев, А. В. and Ильин, Н. А. and Шерстюк, Н. Э. and Мухортов, В. М.},
	month = apr,
	year = {2012},
	pages = {836--841},
}



@article{__2012-8,
	title = {Электропроводность и термо-э.д.с. кристаллов титаната свинца},
	volume = {54},
	url = {http://journals.ioffe.ru/articles/859},
	abstract = {Исследованы температурные зависимости коэффициента термо-э.д.с. alpha и удельной объемной электропроводности sigmaV в температурном интервале 400-550 K, где в кристаллах титаната свинца наблюдаются аномалии диэлектрической проницаемости varepsilon, не связанные с фазовым переходом. Установлено, что в указанном интервале температур alpha имеет максимум и во многих кристаллах меняет знак, при этом sigmaV снижается. Сделано предположение о том, что аномалии alpha и sigmaV, коррелирующие с аномалиями varepsilon, обусловлены термоактивацией ловушек электронов, что приводит к компенсации проводимости p-типа. Определены концентрация свободных носителей заряда и их дрейфовая подвижность в парафазе вблизи точки Кюри. Эти данные указывают на возможность полного внутреннего экранирования связанного заряда Ps.},
	language = {ru},
	number = {5},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Гавриляченко, В. Г. and Семенчев, А. Ф. and Авакян, Е. И. and Панченко, Е. М. and Мартыщенко, А. В.},
	month = apr,
	year = {2012},
	pages = {901--902},
}



@article{__2012-9,
	title = {Электродинамические характеристики стекол составов {LaBGeO}$_{\textrm{5}}$ и {LaBSiO}$_{\textrm{5}}$ в терагерцевом и ИК-диапазонах},
	volume = {54},
	url = {http://journals.ioffe.ru/articles/780},
	abstract = {Сравниваются методы расчета функций диэлектрического отклика разупорядоченных веществ по пропусканию (субмиллиметровый диапазон) и отражению (ИК диапазон) на примере функциональных стекол LaBGeO5 и LaBSiO5 со структурой стиллвеллита. В рамках четырехпараметрической факторизованной модели дисперсии определены диэлектрические параметры стекол LaBGeO5 и LaBSiO5 и выполнено соотнесение спектральных полос с фрагментами структуры.},
	language = {ru},
	number = {11},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Командин, Г. А. and Сигаев, В. Н. and Торгашев, В. И. and Лотарев, С. В. and Породинков, О. Е. and Спектор, И. Е.},
	month = oct,
	year = {2012},
	pages = {2058--2065},
}



@article{__2012-10,
	title = {Исследование сверхрешеток {BaTiO}$_{\textrm{3}}$/({Ba},{Sr}){TiO}$_{\textrm{3}}$ методом дифракции рентгеновских лучей},
	volume = {54},
	url = {http://journals.ioffe.ru/articles/878},
	abstract = {Методом дифракции рентгеновских лучей проведено исследование образцов сверхрешеток BaTiO3/ (Ba1-xSrx)TiO3 (ВТ/BST-x). Установлена полная параллельная ориентация всех пленок и подложки, определены периоды модуляции Lambda сверхрешеток, параметры ячейки, усредненной по периоду Lambda, и параметры отдельных компонент сверхрешеток.},
	language = {ru},
	number = {5},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Маслова, О. А. and Захарченко, И. Н. and Бунина, О. А. and Юзюк, Ю. И. and Ortega, N. and Kumar, A. and Katiyar, R. S.},
	month = apr,
	year = {2012},
	pages = {953--955},
}



@article{__2012-11,
	title = {Магнетронное и импульсное лазерное напыление наночастиц и несплошных пленок {Ag} и {Au} и исследование их оптических свойств},
	volume = {82},
	url = {http://journals.ioffe.ru/articles/10727},
	abstract = {Исследованы различные режимы получения наночастиц Ag и Au методами магнетронного и импульсного лазерного напыления и особенности спектров поглощения, связанные с плазмонными резонансами. Для получения наночастиц серебра малых размеров (5-10 nm) с большой плотностью поверхностного распределения определен оптимальный режим получения: повышенное давление аргона (2.5·10-2 Torr) и малое напряжение разряда (100 V). Массивы наночастиц Au, полученные методом импульского лазерного напыления, проявляют более высокую однородность при напылении на подложки при температуре 200oC в вакууме, нежели при комнатной температуре в атмосфере аргона. Показано, что положение максимума плазмонного поглощения сдвигается в область меньших длин волн при снижении значения эквивалентной толщины пленок металлов и зависит не только от данного значения, но и от типа подложки, которая определяет морфологические характеристики массивов наночастиц.},
	language = {ru},
	number = {10},
	urldate = {2023-11-11},
	journal = {Журнал технической физики},
	author = {Лянгузов, Н. В. and Кайдашев, В. Е. and Широков, В. Б. and Кайдашев, Е. М.},
	month = sep,
	year = {2012},
	pages = {90--95},
}



@article{__2012-12,
	title = {Фазовые переходы в поляризованных гетерофазных системах на основе цирконата-титаната свинца},
	volume = {54},
	url = {http://journals.ioffe.ru/articles/850},
	abstract = {Исследованы зависимости токов деполяризации, определены фазовые превращения между фазами R3c, R3m, P4mm и Pm3m в образцах пятикомпонентной гетерофазной сегнетокерамики на основе цирконата-титаната свинца.},
	language = {ru},
	number = {5},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Милов, Е. В. and Акбаева, Г. М. and Гавриляченко, В. Г. and Семенчев, А. Ф.},
	month = apr,
	year = {2012},
	pages = {878--879},
}



@article{bunina_structural_2012,
	title = {Structural {Properties} of {Composite} {Thin} {Films} {BiFeO}$_{\textrm{3}}$ - {Ba}$_{\textrm{0.8}}${Sr}$_{\textrm{0.2}}${TiO}$_{\textrm{3}}$},
	volume = {439},
	issn = {0015-0193},
	url = {https://doi.org/10.1080/00150193.2012.741920},
	doi = {10.1080/00150193.2012.741920},
	abstract = {The results of X-ray diffraction study of a new promising magnetoelectric composite films with alternating layers of barium strontium titanate and bismuth ferrite with layer thicknesses d = 6–200 nm are presented. All films show epitaxial growth on the MgO single crystals substrates. The 00L profiles for thick layered films (d {\textgreater} 15 nm) consist of the two reflections corresponding to the separate coherent scattering regions of composite layers. The XRD patterns of thin layered films testify the formation of superlattice. The mean microstrain and mean size of coherent scattering regions were determined using the Willamson-Hall approach.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Ferroelectrics},
	author = {Bunina, O. A. and Zakharchenko, I. N. and Golovko, Yu. I. and Mukhortov, V. M. and Stryukov, D. V. and Yuzyuk, Yu. I.},
	month = jan,
	year = {2012},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/00150193.2012.741920},
	keywords = {X-ray diffraction, superlattice, Thin films, magnetoelectric composite},
	pages = {67--73},
}



@article{bush_ferroelectricity_2012,
	title = {Ferroelectricity in spinel solid solution {Co}$_{\textrm{0.8}}${Ni}$_{\textrm{0.2}}${Cr}$_{\textrm{2}}${O}$_{\textrm{4}}$},
	volume = {85},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.85.214112},
	doi = {10.1103/PhysRevB.85.214112},
	abstract = {Temperature dependencies of dielectric permittivity and loss tangent (at frequencies 0.1–200 kHz) together with thermally stimulated depolarization currents, magnetization, and Mössbauer spectra of ceramic solid solutions Co1−xNixCr2O4 (x = 0, 0.2, 0.4, 0.6, 1.0) are studied at temperatures from 80 to 350 K. We find evidence of two reversible phase transitions located at T1 and T2 (220 and 245 K, respectively, for x = 0.2), of occurrence of pyroelectric properties below T2, as well as of a phase transition to magnetically ordered state of ferrimagnetic type (below 86 K for x = 0.2). The obtained results evidence that the compounds possess, additionally to magnetic, ferroelectric properties and are thus new members in the family of multiferroics.},
	number = {21},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Bush, A. A. and Shkuratov, V. Ya. and Kamentsev, K. E. and Prokhorov, A. S. and Zhukova, E. S. and Gorshunov, B. P. and Torgashev, V. I.},
	month = jun,
	year = {2012},
	note = {Publisher: American Physical Society},
	pages = {214112},
}



@article{druzhinina_raman_2012,
	title = {Raman {Spectra} of {PbFe}$_{\textrm{0.5}}${Nb}$_{\textrm{0.5}}${O}$_{\textrm{3}}${Multiferroic} {Single} {Crystals} and {Ceramics}},
	volume = {438},
	issn = {0015-0193},
	url = {https://doi.org/10.1080/00150193.2012.747391},
	doi = {10.1080/00150193.2012.747391},
	abstract = {Room temperature Raman spectra of both PbFe0.5Nb0.5O3 (PFN) single crystal and ceramics were found to contain 14 bands, namely 64, 130, 200, 265, 427, 488, 560, 703, 785, 861, 971, 1123, 1236, and 1383 cm−1. For the first time distinct anomalies in the temperature dependences of frequency and/or full width at half maximum were observed for some lines in the Raman spectra of PFN single crystal at both antiferromagnetic (≈150 K) and ferroelectric (≈350 K) phase transitions.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Ferroelectrics},
	author = {Druzhinina, N. S. and Yuzyuk, Yu. I. and Raevski, I. P. and Marssi, M. El and Laguta, V. V. and Raevskaya, S. I.},
	month = jan,
	year = {2012},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/00150193.2012.747391},
	keywords = {phase transition, ferroelectric, lead iron niobate, multiferroic, Raman spectra},
	pages = {107--114},
}



@article{ortega_ferroelectric_2012,
	title = {Ferroelectric and {Dielectric} {Properties} of {BaTiO}$_{\textrm{3}}$/{Ba}$_{\textrm{0.30}}${Sr}$_{\textrm{0.70}}${TiO}$_{\textrm{3}}$ {Superlattices}},
	volume = {134},
	issn = {1058-4587},
	url = {https://doi.org/10.1080/10584587.2012.673980},
	doi = {10.1080/10584587.2012.673980},
	abstract = {BaTiO3/Ba0.30Sr0.70TiO3 (BT/BST3070) artificial superlattice (SL) was fabricated by pulsed laser deposition on La0.67Sr0.33MnO3 (LSMO) coated (001) MgO substrates. Satellite reflections in X-ray diffraction are used to calculate the periodicity of SL structure indicates a period ∼14 nm. Cross polarized Raman spectra show upward shift of the E(1TO) soft mode, this is markedly changed with respect to its parent BT layer thin film. The BT/BST3070 SL illustrates high dielectric constant (1100-1300) and low loss tangent ({\textless}0.1) below to 104 Hz. Polarization and dielectric constant show strong switching behavior under applied external electric field with well saturated hysteresis loop and high dielectric tunability.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Integrated Ferroelectrics},
	author = {Ortega, N. and Kumar, Ashok and Yuzyuk, YU. I. and Scott, J. F. and Katiyar, Rams.},
	month = jan,
	year = {2012},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/10584587.2012.673980},
	keywords = {Superlattices, BT/BST, dielectric, ferroelectric, PLD},
	pages = {139--145},
}



@article{shakhovoy_ferroelectric_2012,
	title = {Ferroelectric {Q} and antiferroelectric {P} phases' coexistence and local phase transitions in oxygen-deficient {NaNb}$_{\textrm{3}}$ single crystal: micro-{Raman}, dielectric and dilatometric studies},
	volume = {43},
	copyright = {Copyright © 2012 John Wiley \& Sons, Ltd.},
	issn = {1097-4555},
	shorttitle = {Ferroelectric {Q} and antiferroelectric {P} phases' coexistence and local phase transitions in oxygen-deficient {NaNbO3} single crystal},
	url = {https://onlinelibrary.wiley.com/doi/abs/10.1002/jrs.3140},
	doi = {10.1002/jrs.3140},
	abstract = {Micro-Raman studies of oxygen-deficient gray-colored NaNbO3 single crystals have shown that at room temperature both antiferroelectric P and ferroelectric Q phases are present simultaneously as separate regions tens of micrometers in size. Phase transitions in P and Q regions have been elucidated by dielectric, dilatometric and micro-Raman studies. For the first time, the sequence of phase transitions between antiferroelectric phase P and ferroelectric Q and N phases has been revealed. Copyright © 2012 John Wiley \& Sons, Ltd.},
	language = {en},
	number = {8},
	urldate = {2023-11-11},
	journal = {Journal of Raman Spectroscopy},
	author = {Shakhovoy, R. A. and Raevskaya, S. I. and Shakhovaya, L. A. and Suzdalev, D. V. and Raevski, I. P. and Yuzyuk, Yu. I. and Semenchev, A. F. and El Marssi, M.},
	year = {2012},
	note = {\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/jrs.3140},
	keywords = {phase transition, ferroelectric, antiferroelectric, micro-Raman spectroscopy, sodium niobate},
	pages = {1141--1145},
	file = {Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\HWT6QGGA\\jrs.html:text/html},
}



@article{__2012-13,
	title = {Усиление комбинационного рассеяния локализованными плазмонами в наночастицах серебра на поверхности наностержней оксида цинка},
	volume = {82},
	url = {http://journals.ioffe.ru/articles/10726},
	abstract = {Исследованы особенности процесса магнетронного напыления наночастиц Ag на массивы наностержней ZnO. Боковые грани наностержней покрываются наночастицами с гораздо меньшей плотностью, нежели плоские поверхности при аналогичных временах напыления. Повышенная плотность частиц Ag наблюдается на ребрах боковых граней наностержней. Максимум плазмонного поглощения в синтезированных массивах наностержней, покрытых изолированными наночастицами Ag, лежит в диапазоне 450-500 nm. Возникновение локальных плазмонных возбуждений приводит к усилению интенсивности многофононных процессов с участием полярных мод ZnO в спектрах комбинационного рассеяния. С увеличением эквивалентной толщины пленок Ag возрастает сечение резонансного комбинационного рассеяния для обертонов фонона A1(LO).},
	language = {ru},
	number = {10},
	urldate = {2023-11-11},
	journal = {Журнал технической физики},
	author = {Кайдашев, В. Е. and Лянгузов, Н. В. and Юзюк, Ю. И. and Кайдашев, Е. М.},
	month = sep,
	year = {2012},
	pages = {85--89},
}



@article{__2012-14,
	title = {Оптические свойства эпитаксиальных тонких пленок {Ba}$_{\textrm{0.8}}${Sr}$_{\textrm{0.2}}${TiO}$_{\textrm{3}}$},
	volume = {82},
	url = {http://journals.ioffe.ru/articles/10654},
	abstract = {Исследованы свойства наноразмерных пленок (Ba0.8,Sr0.2)TiO3 на монокристаллических подложках окиси магния. Пленки изготовлены по методу высокочастотного распыления при осаждении по слоевому механизму роста. Измерения параметров решетки выполнены с помощью методов рентгеновской дифракции. Пропускание пленок различной толщины исследовано в диапазоне длин волн 190-1100 nm. При анализе экспериментальных оптических характеристик для определения коэффициента преломления и поглощения в дисперсионной формуле использованы дополнительные, релаксационные слагаемые, отражающие конечное время жизни осциллятора, что позволило более точно провести аппроксимацию экспериментальных данных.},
	language = {ru},
	number = {7},
	urldate = {2023-11-11},
	journal = {Журнал технической физики},
	author = {Широков, В. Б. and Головко, Ю. И. and Мухортов, В. М.},
	month = jun,
	year = {2012},
	pages = {79--84},
	file = {Журнал технической физики:C\:\\Users\\aleks\\Zotero\\storage\\8NHTT9Q2\\10654.html:text/html},
}



@article{__2012-15,
	title = {Использование различных катализаторов роста для лазерного напыления микро- и наностержней {ZnO}},
	volume = {82},
	url = {http://journals.ioffe.ru/articles/10579},
	abstract = {С помощью метода импульсного лазерного напыления получены микро- и наностержни ZnO с использованием различных катализаторов роста при температурах, близких к оптимальным для каждого типа катализатора. Сравнительный анализ оптических и структурных свойств полученных образцов показал, что при снижении температуры роста при использовании подложек Al2O3 (11-20) уменьшаются внутренние напряжения в стержнях, что приводит к улучшению структуры и оптических свойств. При использовании подложек GaN/Si такой эффект не наблюдается из-за сильных напряжений, вносимых разностью параметров решеток. При повышении температуры синтеза увеличиваются внутренние напряжения и концентрация точечных дефектов решетки, происходит релаксация правил отбора, и наблюдаются множественные обертоны фонона A1(LO). Получено качественное соответствие результатов расчетов деформаций кристаллической решетки, произведенных по параметру a элементарной ячейки и по сдвигу частоты фонона A1(LO). Исследование фотолюминесценции образцов показало, что снижение температуры синтеза уменьшает дефектность стержней ZnO и позволяет улучшить их оптические свойства для УФ-приложений.},
	language = {ru},
	number = {4},
	urldate = {2023-11-11},
	journal = {Журнал технической физики},
	author = {Лянгузов, Н. В. and Кайдашев, В. Е. and Захарченко, И. Н. and Куприна, Ю.А. and Бунина, О. А. and Юзюк, Ю. И. and Киселев, А. П. and Кайдашев, Е. М.},
	month = mar,
	year = {2012},
	pages = {108--116},
}



@article{bouyanfif_comparative_2012,
	title = {A comparative {Raman} study of 0.65({PbMg}$_{\textrm{1/3}}${Nb}$_{\textrm{2/3}}${O}$_{\textrm{3}}$) -0.35({PbTiO}$_{\textrm{3}}$) single crystal and thin film},
	volume = {85},
	issn = {1434-6036},
	url = {https://doi.org/10.1140/epjb/e2011-20484-3},
	doi = {10.1140/epjb/e2011-20484-3},
	abstract = {We report a comparative Raman study of 0.65(PbMg1/3Nb2/3O3)-0.35(PbTiO3) (PMN-0.35PT) single crystal and thin film. Raman spectra investigation indicates a change in bulk from the high temperature cubic to the tetragonal phase and then to the low temperature Mc monoclinic phase. The transition temperatures are in good agreement with the ones previously observed by dielectric measurements on the same sample. In contrast, we observe no phase transition to the monoclinic phase in the PMN-0.35PT 4000 Å thick film and only a cubic to tetragonal diffuse transition has been determined at high temperature. The enhanced stability of the tetragonal phase and the absence of low temperature monoclinic phase have been attributed to the in plane strain.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {The European Physical Journal B},
	author = {Bouyanfif, H. and El Marssi, M. and Lemée, N. and Le Marrec, F. and Karkut, M. G. and Dkhil, B. and Yuzyuk, Yu. I.},
	month = jan,
	year = {2012},
	keywords = {Solid State and Materials},
	pages = {35},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\ZDGC57TN\\Bouyanfif и др. - 2012 - A comparative Raman study of 0.65(PbMg13Nb23O3) .pdf:application/pdf},
}



@article{__2012-16,
	title = {Структурные изменения в жидкотвердых сплавах {Bi} + 44\% {Cd} и {Bi} + 43\% {Sn} под действием постоянного электрического тока},
	volume = {76},
	issn = {0367-6765},
	url = {https://elibrary.ru/item.asp?id=17845707},
	abstract = {Исследовано влияние постоянного электрического тока на параметры ячеек компонентов в жидкотвердых сплавах Bi + 44\% Cd и Bi + 43\% Sn. Обнаружено изменение параметров ячеек, связанное со структурными эффектами.},
	language = {ru},
	number = {7},
	urldate = {2023-11-11},
	journal = {Известия Российской Академии Наук. Серия Физическая},
	author = {Афашоков, В. З. and Ахкубеков, А. А. and Кабиров, Ю. В.},
	year = {2012},
	pages = {851},
}



@article{__2012-17,
	title = {Динамика решетки эпитаксиальной пленки титаната бария-стронция во внешнем электрическом поле},
	volume = {8},
	issn = {1813-4289},
	url = {https://elibrary.ru/item.asp?id=18062877},
	abstract = {Исследована динамика решетки тонкой гетероэпитаксиальной пленки (Ba0,8Sr0,2)TiO3 на кубиче- ской подложке MgO во внешнем электрическом поле. Приведено как феноменологическое описание поведения мягких мод на основе теории Ландау, так и подробный анализ данных комбинационного рассеяния света. Расщепление мягкой моды на компоненты и их частотная зависимость свидетель- ствуют о переходе в моноклинную фазу при приложении внешнего электрического поля в направле- нии, перпендикулярном спонтанной поляризации c-доменной пленки.},
	language = {ru},
	number = {3},
	urldate = {2023-11-11},
	journal = {Вестник Южного Научного Центра Ран},
	author = {Анохин, А. С. and Головко, Ю. И. and Широков, В. Б. and Мухортов, В. М. and Юзюк, Ю. И.},
	year = {2012},
	keywords = {Мягкая Мода, Сегнетоэлектрические Тонкие Пленки, Сегнетоэлектричество, Спектры Комбинационного Рассеяния Света},
	pages = {22--31},
}



@article{pronin_b-t_2012,
	title = {B-{T} phase diagram of {CoCr}$_{\textrm{2}}${O}$_{\textrm{4}}$ in magnetic fields up to 14 {T}},
	volume = {85},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.85.012101},
	doi = {10.1103/PhysRevB.85.012101},
	abstract = {We have measured the magnetization and specific heat of multiferroic CoCr2O4 in magnetic fields up to 14 T. The high-field magnetization measurements indicate a new phase transition at T∗=5–6 K. The phase between T∗ and the lock-in transition at 15 K is characterized by magnetic irreversibility. At higher magnetic fields, the irreversibility increases. Specific-heat measurements confirm the transition at T∗, and also show irreversible behavior. We construct a field-temperature phase diagram of CoCr2O4.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Pronin, A. V. and Uhlarz, M. and Beyer, R. and Fischer, T. and Wosnitza, J. and Gorshunov, B. P. and Komandin, G. A. and Prokhorov, A. S. and Dressel, M. and Bush, A. A. and Torgashev, V. I.},
	month = jan,
	year = {2012},
	note = {Publisher: American Physical Society},
	pages = {012101},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\AZP2XD73\\Pronin и др. - 2012 - \$B\$-\$T\$ phase diagram of CoCr\$ _ 2 \$O\$ _ 4 \$ in .pdf:application/pdf},
}



@article{ortega_effect_2011,
	title = {Effect of periodicity and composition in artificial {BaTiO}$_{\textrm{3}}$/({Ba},{Sr}){TiO}$_{\textrm{3}}$ superlattices},
	volume = {83},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.83.144108},
	doi = {10.1103/PhysRevB.83.144108},
	abstract = {We have prepared two series of BaTiO3/SrTiO3 (BT/ST) superlattices (SLs). In the first set, the modulation period (Λ) was varied from 136 to 16 Å, whereas in the second set ST was replaced with Ba(1−x)SrxTiO3 (BST) (0{\textless}x{\textless}1) with constant periodicity of ∼ 136 Å. A total stack height of 10 000 Å (1 μm) was maintained for both systems. The compositional changes give large spectral changes at x = 40\% where the lowest E mode in BT/BST SL becomes underdamped. X-ray-diffraction patterns and surface topography of the modulated period revealed a Stranski-Krastanov growth mechanism. The upward frequency shift of the E(1TO) in SLs with decrease in Λ or Ba concentration in the BST layer was attributed to the in-plane compressive stress induced by the lattice mismatch of the constituent layers. [N.B., here the notation E(1TO) or A1(2TO) simply designates the vibrational mode of E or A1 symmetry, with 1TO or 2TO designating the transverse optical branch that is lowest, 1, or second lowest, 2, in energy.] In the low-frequency region, the folded acoustic phonon doublets were observed. Since the low-frequency out-of-plane dielectric constant is directly related to the E(1TO) soft mode frequency, strain engineering in artificial SLs allowed us to modify their dielectric properties by varying either the Ba/Sr in BST sublayer concentration or the modulation periodicity in the superlattices.},
	number = {14},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Ortega, N. and Kumar, A. and Maslova, O. A. and Yuzyuk, Yu. I. and Scott, J. F. and Katiyar, R. S.},
	month = apr,
	year = {2011},
	note = {Publisher: American Physical Society},
	pages = {144108},
	file = {Принятая версия:C\:\\Users\\aleks\\Zotero\\storage\\56AU3DQI\\Ortega и др. - 2011 - Effect of periodicity and composition in artificia.pdf:application/pdf},
}



@article{anokhin_electric-field-induced_2011,
	title = {Electric-field-induced monoclinic phase in ({Ba},{Sr}){TiO}$_{\textrm{3}}$ thin film},
	volume = {109},
	issn = {0021-8979},
	url = {https://doi.org/10.1063/1.3573516},
	doi = {10.1063/1.3573516},
	abstract = {We have studied electric-field-induced symmetry lowering in the tetragonal (001)-oriented heteroepitaxial (Ba0.8Sr0.2)TiO3 thin film deposited on (001)MgO substrate. Polarized micro-Raman spectra were recorded from the film area in between two planar electrodes deposited on the film surface. Presence of c domains with polarization normal to the substrate was confirmed from polarized Raman study under zero field, while splitting and hardening of the E(TO) soft mode and polarization changes in the Raman spectra suggest monoclinic symmetry under external electric field.},
	number = {7},
	urldate = {2023-11-11},
	journal = {Journal of Applied Physics},
	author = {Anokhin, A. S. and Yuzyuk, Yu. I. and Golovko, Yu. I. and Mukhortov, V. M. and El Marssi, M.},
	month = apr,
	year = {2011},
	pages = {074111},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\R9PF7M4M\\Anokhin и др. - 2011 - Electric-field-induced monoclinic phase in (Ba,Sr).pdf:application/pdf},
}



@article{leontyev_orthorhombic_2011,
	title = {Orthorhombic polar {Nd}-doped {BiFeO}$_{\textrm{3}}$ thin film on {MgO} substrate},
	volume = {23},
	issn = {0953-8984},
	url = {https://dx.doi.org/10.1088/0953-8984/23/33/332201},
	doi = {10.1088/0953-8984/23/33/332201},
	abstract = {A Nd-doped BiFeO3 thin film deposited on MgO substrate was studied by synchrotron diffraction. The ferroelectric nature of the film is proven by in-plane remanent polarization measurement. The highest possible symmetry of the film is determined to be orthorhombic, within the Fm2m space group. Such a structure is rotated by 45° with respect to the substrate and is consistent with tilts of oxygen octahedra doubling the unit cell. This polar structure presents a rather unusual strain-accommodation mechanism.},
	language = {en},
	number = {33},
	urldate = {2023-11-11},
	journal = {Journal of Physics: Condensed Matter},
	author = {Leontyev, I. N. and Yuzyuk, Yu I. and Janolin, P.-E. and El-Marssi, M. and Chernyshov, D. and Dmitriev, V. and Golovko, Yu I. and Mukhortov, V. M. and Dkhil, B.},
	month = jul,
	year = {2011},
	pages = {332201},
}



@article{__2011-3,
	title = {Особенности структурных состояний в твердых растворах {BiFeO}$_{\textrm{3}}$-{YMnO}$_{\textrm{3}}$},
	volume = {53},
	url = {http://journals.ioffe.ru/articles/1518},
	abstract = {Обнаружено, что в твердых растворах (1-x)BiFeO3-xYMnO3 наблюдается следующая последовательность изменений фаз с увеличением x: R3c-{\textgreater} Pbnm-{\textgreater} C2-{\textgreater} Pnma-{\textgreater} P63cm. Установлено, что фазы Pbnm и Pnma различаются ориентацией атомных смещений и могут иметь антисегнетоэлектрические свойства. Работа поддержана грантом РФФИ N 10-03-00189-a. А.Г. Разумная благодарит Фонд содействия развитию малых форм предприятий в научно-технической сфере по программе У.М.Н.И.К. N 10170.},
	language = {ru},
	number = {8},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Назаренко, А. В. and Разумная, А. Г. and Куприянов, М. Ф. and Кабиров, Ю. В. and Рудская, А. Г. and Тесленко, П. Ю. and Кофанова, Н. Б.},
	month = jul,
	year = {2011},
	pages = {1523--1525},
}



@article{__2010-1,
	title = {Структура и фазовые переходы твердых растворов цирконата-гафната свинца},
	volume = {53},
	url = {http://journals.ioffe.ru/articles/1291},
	abstract = {Методом твердофазного синтеза из простых оксидов приготовлены твердые растворы двух антисегнетоэлектриков - цирконата и гафната свинца PbZr1-xHfxO3, x=0, 0.3, 0.5, 0.7, 1. Элементный состав образцов и их структура изучены методами рентгенофлуоресцентного анализа и рентгеновской дифракции. Определены фазовые изменения твердых растворов в области температур 20{\textless}t{\textless}300oC. Работа поддержана грантом РФФИ N 10-03-00189-a.},
	language = {ru},
	number = {1},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Кабиров, Ю. В. and Куприянов, М. Ф. and Петрович, Э. В. and Дуймакаев, Ш. И. and Пономоренко, В. О.},
	month = dec,
	year = {2010},
	pages = {110--113},
}



@article{__2011-4,
	title = {Спектры комбинационного рассеяния поликристаллических нанотрубок титаната висмута},
	volume = {53},
	url = {http://journals.ioffe.ru/articles/1557},
	abstract = {Исследованы спектры комбинационного рассеяния света нанотрубок титаната висмута Bi4Ti3O12 синтезированных темплатным методом на мембранах Al2O3. Полученные образцы представляли собой массив ориентированных нанотрубок со сросшимися гладкими стенками длиной около 50 mum. Толщина стенок нанотрубок варьировалась от 20 до 50 nm, а внутренний диаметр составлял около 200 nm. В спектрах комбинационного рассеяния света нанотрубок наблюдалось уширение линий, соответствующих валентным и деформационным колебаниям TiO6 октаэдров, а в низкочастотной области спектра, соответствующей колебаниям ионов Bi относительно кислородных октаэдров, наблюдалась трансформация, обусловленная сильными механическими напряжениями, возникающими при формировании нанотрубок.},
	language = {ru},
	number = {9},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Анохин, А. С. and Лянгузов, Н. В. and Рошаль, С. Б. and Юзюк, Ю. И. and Wang, Wen},
	month = sep,
	year = {2011},
	pages = {1768--1772},
}



@article{__2011-5,
	title = {Формирование физических свойств релаксорного сегнетоэлектрика {Pb}$_{\textrm{2}}${ScNbO}$_{\textrm{6}}$ методом механоактивации},
	volume = {37},
	url = {http://journals.ioffe.ru/articles/14334},
	abstract = {Изучен релаксорный сегнетоэлектрик Pb2ScNbO6 (PSN), полученный твердофазным методом, спеканию которого предшествовала обработка при комнатной температуре синтезированного порошка PSN в наковальнях Бриджмена силовым воздействием в сочетании со сдвиговой деформацией. Показано, что при интенсивных силовых воздействиях в сочетании со сдвиговой деформацией в PSN развиваются динамические рекристаллизационные процессы, вносящие существенный вклад в формирование физических свойств керамики.},
	language = {ru},
	number = {20},
	urldate = {2023-11-11},
	journal = {Письма в ЖТФ},
	author = {Убушаева, Э. Н. and Лихушина, Е. В. and Абдулвахидов, К. Г. and Витченко, М. А. and Абулвахидов, Б. К. and Широков, В. Б. and Лянгузов, Н. В. and Юзюк, Ю. И. and Кайдашев, Е. М. and Мардасова, И. В.},
	month = sep,
	year = {2011},
	pages = {23--30},
}



@article{__2011-6,
	title = {Исследование влияния толщины медного катализатора и пленочного подслоя на морфологию наностержней {ZnO}},
	volume = {37},
	url = {http://journals.ioffe.ru/articles/12488},
	abstract = {Исследовано влияние толщины пленочного подслоя ZnO, а также толщины пленок катализатора роста (Cu) на морфологию наностержней ZnO, выращенных на подложках a-Al2O3(11-20) карботермическим методом. Увеличение толщины пленки Cu приводит к увеличению диаметров, высоты и поверхностной плотности наностержней. Увеличение толщины пленочного подслоя ZnO приводит к возрастанию среднего диаметра и уменьшению длины и поверхностной плотности наностержней. Проведены исследования по влиянию температуры на процесс термического развала сверхтонких пленок меди, нанесенынх на подложки a-Al2O3. Исследованы фотолюминесцентные свойства массивов наностержней при высоких уровнях оптической накачки. Повышение плотности мощности накачки до 250-280 kW/cm2 приводит к сверхлюминесценции наностержней.},
	language = {ru},
	number = {5},
	urldate = {2023-11-11},
	journal = {Письма в ЖТФ},
	author = {Лянгузов, Н. В. and Кайдашев, В. Е. and Кайдашев, Е. М. and Абдулвахидов, К. Г.},
	month = feb,
	year = {2011},
	pages = {1--8},
}



@article{__2011-7,
	title = {Поверхностные акустические волны в тонких пленках титаната бария-стронция на подложках из оксида магния},
	volume = {37},
	url = {http://journals.ioffe.ru/articles/12492},
	abstract = {Установлено, что при использовании в устройстве на поверхностных акустических волнах в качестве активного элемента тонкой пленки титаната бария-стронция на подложке из оксида магния можно вдвое повысить рабочую частоту преобразователя за счет формирования в пленке периодической доменной структуры. Показано, что в тонкой сегнетоэлектрической пленке при стандартной структуре электродов эффективно возбуждается вторая гармоника поверхностной акустической волны. Путем изменения внешнего поляризующего напряжения на электродах пленки можно создавать преобразователи с электрически регулируемым коэффициентом электромеханической связи.},
	language = {ru},
	number = {5},
	urldate = {2023-11-11},
	journal = {Письма в ЖТФ},
	author = {Мухортов, В. М. and Бирюков, С. В. and Головко, Ю. И. and Карапетьян, Г. Я. and Масычев, С. И. and Мухортов, В.М.},
	month = feb,
	year = {2011},
	pages = {31--37},
}



@article{__2011-8,
	title = {Поляризация тонких пленок титаната бария-стронция при действии внешнего электрического поля},
	volume = {81},
	url = {http://journals.ioffe.ru/articles/10392},
	abstract = {В рамках простой феноменологической модели описано поведение поляризации тонкой пленки Ba0.8Sr0.2TiO3 во внешнем электрическом поле при планарной геометрии электродов. Для согласования с экспериментальными данными введено "поле Ван-дер-Ваальса" Ez, формируемое подложкой в направлении нормали к плоскости пленки. Оценка величины поля дает значение Ez=1.1· 108 V/m. Проанализирована фазовая диаграмма пленки Ba0.8Sr0.2TiO3 в плоскости Ez - misfit strain при комнатной температуре},
	language = {ru},
	number = {8},
	urldate = {2023-11-11},
	journal = {Журнал технической физики},
	author = {Широков, В. Б. and Бирюков, С. В. and Мухортов, В. М. and Юзюк, Ю. И.},
	month = jul,
	year = {2011},
	pages = {115--120},
}



@article{__2010-2,
	title = {Структура и динамика решетки гетероструктур на основе феррита висмута и титаната бария-стронция на подложке оксида магния},
	volume = {52},
	url = {https://journals.ioffe.ru/articles/1900},
	abstract = {Пленки феррита висмута, легированные неодимом, получены на монокристаллических подложках MgO с эпитаксиальным тонким (1-2 nm) подслоем титаната бария-стронция методом высокочастотного распыления керамических мишеней при повышенном парциальном давлении кислорода при температурах ниже температур сегнетоэлектрического и магнитного переходов. Методами дифракции рентгеновских лучей и спектроскопии комбинационного рассеяния света установлено, что в этих пленках феррита висмута реализуется новая фаза, которая не наблюдается в объемных образцах. Симметрия такой фазы моноклинная, элементарная ячейка содержит две формульные единицы, а вектор спонтанной поляризации отклоняется от направления [111]cub и может иметь различные компоненты вдоль осей x, y и z.},
	language = {ru},
	number = {7},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Головко, Ю. И. and Мухортов, В. М. and Бунина, О. А. and Захарченко, И. Н. and Анохин, А. С. and Широков, В. Б. and Юзюк, Ю. И.},
	month = jun,
	year = {2010},
	pages = {1336--1341},
	file = {Физика твердого тела:C\:\\Users\\aleks\\Zotero\\storage\\3AQF2CGA\\1900.html:text/html},
}



@article{__2010-3,
	title = {Тонкие сегнетоэлектрические пленки: получение и перспективы интеграции},
	volume = {52},
	url = {http://journals.ioffe.ru/articles/1789},
	abstract = {ассматриваются свойства тонких пленок (Ba,Sr)TiO3 и BiFeO3 и наноструктур на их основе. Пленки изготавливаются методом высокочастотного распыления в атмосфере кислорода с повышенным давлением, наноструктуры - методом фокусированного ионного травления; электрическое поле прикладывается в планарной структуре встречно-штыревых электродов. Исследуются структура, диэлектрические, электро-оптические и нелинейно-оптические свойства полученных образцов в широком диапазоне толщин и частот электрического поля. Показана высокая эффективность планарного переключения и его влияния на оптические свойства полученных структур. Наноструктурирование позволяет изменять диэлектрические и оптические свойства исследуемых материалов и таким образом увеличивать диапазон переключения функциональных параметров.},
	language = {ru},
	number = {4},
	urldate = {2023-11-11},
	journal = {Тонкие сегнетоэлектрические пленки: получение и перспективы интеграции},
	author = {Сигов, А. С. and Мишина, Е. Д. and Мухортов, В. М.},
	month = mar,
	year = {2010},
	pages = {709--717},
}



@article{__2010-4,
	title = {Диэлектрические спектры тонких пленок мультиферроика {Bi}$_{\textrm{0.98}}${Nd}$_{\textrm{0.02}}${FeO}$_{\textrm{3}}$ в терагерцевом диапазоне частот},
	volume = {52},
	url = {http://journals.ioffe.ru/articles/1956},
	abstract = {етодами субмиллиметровой спектроскопии на основе ламп обратной волны (ЛОВ) и инфракрасной Фурье-спектроскопии в диапазоне частот 8-1000 cm-1 при комнатной температуре измерены спектры пропускания и отражения тонких пленок мультиферроика Bi0.98Nd0.02FeO3 на подложках монокристаллического MgO. В рамках модели слоистой среды рассчитаны спектры комплексной диэлектрической проницаемости пленок. Обнаружены мощный рост потерь в области 30 cm-1 при уменьшении толщины пленок и обусловленное им пятикратное увеличение статической диэлектрической проницаемости (до 500 в пленке толщиной 32 nm). Явление обсуждается в рамках феноменологической теории фазовых переходов.},
	language = {ru},
	number = {9},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Командин, Г. А. and Торгашев, В. И. and Волков, А. А. and Породинков, О. Е. and Спектор, И. Е. and Мухортов, В. М.},
	month = sep,
	year = {2010},
	pages = {1717--1723},
	file = {Физика твердого тела:C\:\\Users\\aleks\\Zotero\\storage\\NZQTPGVK\\1956.html:text/html},
}



@article{__2010-5,
	title = {Спектры комбинационного рассеяния пленки титаната бария-стронция в электрических полях},
	volume = {74},
	issn = {0367-6765},
	url = {https://www.elibrary.ru/item.asp?id=15249715},
	abstract = {Исследованы поляризованные спектры комбинационного рассеяния гетероэпитаксиальной пленки титаната бариястронция на подложке MgO во внешнем электрическом поле, приложенном перпендикулярно направлению спонтанной поляризации. Частичная деполяризация, наблюдающаяся в спектрах, свидетельствует об индуцированном полем понижении симметрии кристаллической решетки.},
	language = {ru},
	number = {9},
	urldate = {2023-11-11},
	journal = {Известия Российской Академии Наук. Серия Физическая},
	author = {Анохин, А. С. and Юзюк, Ю. И. and Головко, Ю. И. and Мухортов, В. М.},
	year = {2010},
	keywords = {⛔ No DOI found},
	pages = {1282--1284},
}



@article{__2010-6,
	title = {Сегнетоэлектрические тонкие пленки {BiFeO}$_{\textrm{3}}$ с орторомбической структурой допированного {Nd}},
	volume = {74},
	issn = {0367-6765},
	url = {https://www.elibrary.ru/item.asp?id=15142299},
	abstract = {Методами дифракции рентгеновских лучей и рамановской спектроскопии определена орторомбическая симметрия (Fmm2, a = 7.914 A, b = 7.913 A и c = 7.937 A) эпитаксиальных пленок феррита висмута, допированного Nd, на подложках MgO.},
	language = {ru},
	number = {8},
	urldate = {2023-11-11},
	journal = {Известия Российской Академии Наук. Серия Физическая},
	author = {Леонтьев, И. Н. and Анохин, А. С. and Юзюк, Ю. И. and Головко, Ю. И. and Мухортов, В. М.},
	year = {2010},
	keywords = {⛔ No DOI found},
	pages = {1163--1165},
}



@article{__2010-7,
	title = {Влияние внутренних деформационных полей на управляемость наноразмерных сегнетоэлектрических пленок в планарном конденсаторе},
	volume = {80},
	url = {http://journals.ioffe.ru/articles/9945},
	abstract = {Рентгенодифракционными методами и просвечивающей электронной спектроскопией высокого разрешения исследованы наноразмерные сегнетоэлектрические гетероэпитаксиальные пленки Ba0.8Sr0.2TiO3, выращенные по слоевому механизму роста на подложках (100) MgO. Установлено, что при изменении толщины пленок релаксация напряжений происходит посредством образования дислокаций нсоответствия на границе раздела между пленкой и подложкой. Существует критическая толщина ({\textasciitilde}40 nm) пленок, ниже которой в пленках имеют место напряжения растяжения, а выше - напряжения сжатия. Приведены примеры влияния напряжений на диэлектрические характеристики пленок.},
	language = {ru},
	number = {3},
	urldate = {2023-11-11},
	journal = {Журнал технической физики},
	author = {Мухортов, В. М. and Головко, Ю. И. and Маматов, А. А. and Жигалина, О. М. and Кускова, А. Н. and Чувилин, A. Л.},
	month = feb,
	year = {2010},
	pages = {77--82},
}



@article{__2010-8,
	title = {Наноструктурированный мультиферроик {PbFe}$_{\textrm{0.5}}${Nb}$_{\textrm{0.5}}${O}$_{\textrm{3}}$ и его физические свойства},
	volume = {80},
	url = {http://journals.ioffe.ru/articles/10151},
	abstract = {Изучен поликристаллический мультиферроик PbFe0.5Nb0.5O3 (PEN), полученный твердофазным методом, спеканию которого предшествовала обработка при комнатной температуре синтезированного порошка PFN в наковальнях Бриджмена силовым воздействием в сочетании со сдвиговой деформацией (СВСД). Проведен сравнительный анализ электрофизических свойств и структурных параметров рабочих и эталонного образцов. Показано, что, начиная с величины СВСД, равной 200 MPa, доминирующую роль в формировании физических свойств играют точечные дефекты.},
	language = {ru},
	number = {11},
	urldate = {2023-11-11},
	journal = {Журнал технической физики},
	author = {Убушаева, Э. Н. and Абдулвахидов, К. Г. and Мардасова, И. В. and Абулвахидов, Б. К. and Витченко, М. А. and Амиров, А. А. and Батдалов, А. Б. and Гамзатов, А. Г.},
	month = oct,
	year = {2010},
	pages = {49--52},
	file = {Журнал технической физики:C\:\\Users\\aleks\\Zotero\\storage\\26FX65HJ\\10151.html:text/html},
}



@article{yuzyuk_ferroelectric_2010,
	title = {Ferroelectric {Q}-phase in a {NaNbO}$_{\textrm{3}}$ epitaxial thin film},
	volume = {96},
	issn = {0003-6951},
	url = {https://doi.org/10.1063/1.3437090},
	doi = {10.1063/1.3437090},
	abstract = {Epitaxial NaNbO3 thin films have been grown by pulsed laser deposition on cubic (00l) MgO substrate with epitaxial (La0.5Sr0.5)CoO3 buffer layer. Micro-Raman spectroscopy studies revealed that the ferroelectric Q phase (Pmc21, Z=4) is stable in a 250-nm-thick film in contrast to the antiferroelectric phase P (Pbma, Z=8) known to exist in the bulk single crystals and ceramics of undoped stoichiometric NaNbO3. Temperature-dependent Raman spectra indicate that the Q phase is stable over a wide temperature range (at least from 80 to 600 K), while the low-temperature ferroelectric rhombohedral phase N, typical for NaNbO3 single crystals, is not observed.},
	number = {22},
	urldate = {2023-11-11},
	journal = {Applied Physics Letters},
	author = {Yuzyuk, Yu. I. and Shakhovoy, R. A. and Raevskaya, S. I. and Raevski, I. P. and El Marssi, M. and Karkut, M. G. and Simon, P.},
	month = jun,
	year = {2010},
	pages = {222904},
}



@article{el_marssi_ferroelectric_2010,
	title = {Ferroelectric {BaTiO}$_{\textrm{3}}$/{BaZrO}$_{\textrm{3}}$ superlattices: {X}-ray diffraction, {Raman} spectroscopy, and polarization hysteresis loops},
	volume = {108},
	issn = {0021-8979},
	shorttitle = {Ferroelectric {BaTiO3}/{BaZrO3} superlattices},
	url = {https://doi.org/10.1063/1.3496620},
	doi = {10.1063/1.3496620},
	abstract = {Artificial superlattices (SLs) consisting of ferroelectric BaTiO3 (BT) and paraelectric BaZrO3 (BZ) have been growth by a pulsed laser deposition technique. The epitaxial BT and BZ layers with a periodicity from 16 Å to 1056 Å were sequentially deposited on (001) MgO substrate buffered with an oxide conducting layer of La1/2Sr1/2CoO3. The out-of-plane lattice parameters of the SLs constituents were determined by modeling of the x-ray diffractograms. The results indicate that the polar c-axis of the BT layers lies in the plane of the substrate and BZ layers exhibit enhanced tetragonal distortion which is induced by the mismatch between the alternating BZ and BT layers. The Raman data reinforces this interpretation and suggest a monoclinic phase in BT layers and polar phase in BZ layers. The Raman spectra give evidence of coupling between the constituent layers and a narrowing of the Raman peaks is attributed to a reduction in the disorder of the Ti4+ ions due to the epitaxial strain. This strain is responsible for the upward frequency shift in the soft modes, especially, the E(1TO) mode, which is markedly altered with respect to its analogs in BT-bulk crystal and BT thin film. Ferroelectric hysteresis loops measurements, confirmed the x-ray diffraction and Raman results, and revealed a clear ferroelectric behavior for the constrained SLs (32 Å≤Λ≤256 Å) while a weak ferroelectricity is observed for the large periods (Λ=500 Å and 1056 Å). This is attributed to the strain-induced ferroelectricity in BZ layers for the constrained SLs.},
	number = {8},
	urldate = {2023-11-11},
	journal = {Journal of Applied Physics},
	author = {El Marssi, M. and Gagou, Y. and Belhadi, J. and De Guerville, F. and Yuzyuk, Yu. I. and Raevski, I. P.},
	month = oct,
	year = {2010},
	pages = {084104},
}



@article{leontyev_ferroelectric_2010,
	title = {Ferroelectric {BaTiO}$_{\textrm{3}}$ single crystal under superstrong electric fields up to 55 {MV}/m: {A} comparative experimental and theoretical study},
	volume = {96},
	issn = {0003-6951},
	shorttitle = {Ferroelectric {BaTiO3} single crystal under superstrong electric fields up to 55 {MV}/m},
	url = {https://doi.org/10.1063/1.3386537},
	doi = {10.1063/1.3386537},
	abstract = {We investigated the effect of huge electric field up to E=55 MV/m on tetragonal ferroelectric phase of BaTiO3 single crystal. Both lattice parameters and the dielectric susceptibility along the polar axis were determined. The induced polarization shows a continuous increase up to 20\% of the spontaneous polarization. The longitudinal d33 and transverse d31 piezoelectric coefficients were also determined. The experimental data are described by a phenomenological approach. Interestingly, an intermediate critical electric field value of E∼25 MV/m was evidenced suggesting that the physics below and above this value are different.},
	number = {14},
	urldate = {2023-11-11},
	journal = {Applied Physics Letters},
	author = {Leontyev, I. N. and Fesenko, O. E. and Leontyev, N. G. and Dkhil, B.},
	month = apr,
	year = {2010},
	pages = {142904},
	file = {Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\ZP8445SF\\Ferroelectric-BaTiO3-single-crystal-under.html:text/html},
}



@article{__2010-9,
	title = {Фазовые переходы в {PbSc}$_{\textrm{0.5}}${Ta}$_{\textrm{0.5}}${O}$_{\textrm{3}}$},
	volume = {80},
	url = {http://journals.ioffe.ru/articles/9965},
	abstract = {Рентгенодифрактометрическим, электрофизическими и оптическими методами изучены разупорядоченные и частично упорядоченные сегнетоэлектрические монокристаллы PbSc0.5Ta0.5O3 в широком интервале значений температуры. В низкотемпературной области при T=-40oC обнаружен фазовый переход, который подтверждается как электрофизическими, так и рентгенодифрактометрическим методами.},
	language = {ru},
	number = {4},
	urldate = {2023-11-11},
	journal = {Журнал технической физики},
	author = {Абдулвахидов, К. Г. and Мардасова, И. В. and Мясникова, Т. П. and Витченко, М. А. and Ошаева, Э. Н.},
	month = mar,
	year = {2010},
	pages = {81--83},
}



@article{__2009,
	title = {Терагерцевые диэлектрические спектры тонких пленок ({Ba},{Sr}){TiO}$_{\textrm{3}}$},
	volume = {51},
	url = {https://journals.ioffe.ru/articles/2288},
	abstract = {Измерены спектры отражения и пропускания пленок Ba0.7Sr0.3TiO3 с толщинами 36 и 800 mum на подложке из MgO на частотах 8-1000 cm-1 при комнатной температуре. Методом моделирования извлечены диэлектрические параметры материала пленок. Найдена зависимость диэлектрической проницаемости от толщины пленки. Выявлено сильное влияние спектра поглощения излучения в подложке на расчетные диэлектрические спектры материала пленки. Показана необходимость учета при моделировании подфононных диэлектрических потерь в подложке.},
	language = {ru},
	number = {7},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Командин, Г. А. and Волков, А. А. and Спектор, И. Е. and Воротилов, К. А. and Мухортов, В. М.},
	month = jun,
	year = {2009},
	pages = {1280--1283},
}



@article{__2009-1,
	title = {Феноменологическое описание тонких пленок {SrTiO}$_{\textrm{3}}$},
	volume = {51},
	url = {https://journals.ioffe.ru/articles/2235},
	abstract = {Проведено вычисление констант феноменологического потенциала SrTiO3 с учетом последних экспериментальных данных. По сравнению с ранее приведенными значениями константы alpha11,alpha12,t44 изменены более чем на порядок. Рассчитаны фазовые T-P-диаграммы при действии одноосных - [001] и [110] - нагрузок. Построена фазовая диаграмма температура-деформация (misfit strain) тонкой пленки SrTiO3, на которой чисто сегнетоэлектрические фазы существуют при низких температурах.},
	language = {ru},
	number = {5},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Широков, В. Б. and Юзюк, Ю. И. and Леманов, В. В.},
	month = apr,
	year = {2009},
	pages = {972--978},
}



@article{de_guerville_soft_2006,
	title = {Soft mode dynamics and the reduction of {Ti}$^{\textrm{4+}}$ disorder in ferroelectric∕relaxor superlattices {BaTiO}$_{\textrm{3}}$ / {BaTi}$_{\textrm{0.68}}${Zr}$_{\textrm{0.32}}${O}$_{\textrm{3}}$},
	volume = {74},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.74.064107},
	doi = {10.1103/PhysRevB.74.064107},
	abstract = {We used pulsed laser deposition to grow a series of [BaTiO3]Λ∕2/[BaTi0.68Zr0.32O3]Λ∕2 (BTZ∕BT) superlattices (SL’s) with a modulation period Λ that varies between 16Å⩽Λ⩽1008Å; the total thickness is kept constant at about 4000Å. We determine the out-of-plane lattice parameters of the SL constituents by modeling the x-ray diffractograms of the SL’s. The results indicate that the polar c axis of the BT layers lies in the plane of the film. The Raman data reinforces this interpretation. The Raman spectra of SL’s give evidence of coupling between BT and BTZ layers and a narrowing of the Raman peaks suggest a reduction of the disorder of the Ti4+ ions due to the strain. This strain resulting from the lattice mismatch between the constituent layers is responsible for the upward frequency shift of the soft modes, especially the E(1TO) mode, which is markedly altered with respect to its analogs in BT-bulk crystals and BT film. This soft-mode behavior as a function of Λ indicates that the crystal structure of all SL’s is more rigid than in BTZ and BT single thin films.},
	language = {en},
	number = {6},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {De Guerville, F. and El Marssi, M. and Raevski, I. P. and Karkut, M. G. and Yuzyuk, Yu. I.},
	month = aug,
	year = {2006},
	note = {Publisher: American Physical Society},
	pages = {064107},
}



@article{shirokov_phenomenological_2009,
	title = {Phenomenological theory of phase transitions in epitaxial {Ba}$_{\textrm{x}}${Sr}$_{\textrm{1-x}}${TiO}$_{\textrm{3}}$ thin films},
	volume = {79},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.79.144118},
	doi = {10.1103/PhysRevB.79.144118},
	abstract = {A phenomenological thermodynamic theory of BaxSr1−xTiO3 (BST-x) thin films epitaxially grown on cubic substrates is developed using the Landau-Devonshire approach. The eighth-order thermodynamic potential for BaTiO3 (BT) single crystal and modified fourth-order potential for SrTiO3 single crystal were used as starting potentials for the end members of the solid solution with the aim to develop potential of BST-x solid solution valid at high temperatures. Several coefficients of these potentials for BT were changed to obtain reasonable agreement between theory and experimental phase diagram for BST-x (x{\textgreater}0.2) solid solutions. For low Ba content we constructed the specific phase diagram where five phases converge at the multiphase point (TN2=48 K, x=0.029) and all transitions are of the second order. The “concentration-misfit strain” phase diagrams for BST-x thin films at room temperature and “temperature-misfit strain” phase diagrams for particular concentrations are constructed and discussed. Near TN2 coupling between polarization and structural order parameter in the epitaxial film is modified considerably and large number of new phases not present in the bulk materials appear on the phase diagram.},
	number = {14},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Shirokov, V. B. and Yuzyuk, Yu. I. and Dkhil, B. and Lemanov, V. V.},
	month = apr,
	year = {2009},
	note = {Publisher: American Physical Society},
	pages = {144118},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\56FT9N2S\\Shirokov и др. - 2009 - Phenomenological theory of phase transitions in ep.pdf:application/pdf},
}



@article{__2008,
	title = {Микрорамановский отклик и осцилляторные параметры фононов в твердых растворах {Pb}$_{\textrm{1-x}}${Ca}$_{\textrm{x}}${TiO}$_{\textrm{3}}$ (0.40{\textless}x{\textless}0.62)},
	volume = {51},
	url = {https://journals.ioffe.ru/articles/2094},
	abstract = {Посредством температурных (295{\textless}T{\textless}650 K) исследований поляризованных спектров комбинационного рассеяния света в области частот 10{\textless}nu{\textless}1200 cm-1 на монокристаллическом образце твердого раствора Pb0.54Ca0.46TiO3 установлено существование по крейней мере одной особой температурной точки (Tc{\textasciitilde}392 K), в которой наблюдаются заметные аномалии осцилляторных параметров фононных мод. Аналогичные явления имеют место в растворах с 0.4{\textless}x{\textless}0.5. Резкий рост интенсивности спектральных линий, соответствующих волнам поляризации, при температурах сразу ниже Tc позволяет сделать вывод о трансформации Pb1-xCaxTiO3 (0.4{\textless}x{\textless}0.5) в полярное состояние, которое отсутствует в системе при концентрациях x{\textgreater}0.5.},
	language = {ru},
	number = {1},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Чабанюк, А. Н. and Торгашев, В. И. and Юзюк, Ю. И. and Леманов, В. В. and Simon, P.},
	month = dec,
	year = {2008},
	pages = {155--163},
}



@article{__2009-2,
	title = {Оптические и структурные свойства наностержней {ZnO}, полученных методом импульсного лазерного напыления без катализатора},
	volume = {79},
	url = {https://journals.ioffe.ru/articles/9840},
	abstract = {Методом импульсного лазерного напыления без использования катализатора на сапфире получены наностержни ZnO диаметром менее 10 nm. Исследованы структурные особенности наностержней методом комбинационного рассеяния при возбуждении в видимом и УФ-диапазонах. Изучены температурные зависимости экситонных спектров, а также поведение зеленой люминесценции в диапазоне 10-280 K. Интенсивность люминесценции полученных наностержней ZnO в экситонной области превышала зеленую люминесценцию в 7.8 раза при комнатной температуре.},
	language = {ru},
	number = {11},
	urldate = {2023-11-11},
	journal = {Журнал технической физики},
	author = {Кайдашев, В. Е. and Кайдашев, Е. М. and Peres, M. and Monteiro, T. and Correira, M. R. and Sobolev, N. A.},
	month = oct,
	year = {2009},
	pages = {45--49},
}



@article{__2009-3,
	title = {Исследование пьезоактивности тонких пленок цирконата-титаната свинца},
	volume = {79},
	url = {https://journals.ioffe.ru/articles/9770},
	abstract = {зучены особенности проявления пьезоактивности тонких сегнетоэлектрических пленок цирконата-титаната свинца, полученных высокочастотным катодным распылением мишеней стехиометрического состава. Установлено, что пленки обладают естественной униполярностью. Обсуждаются возможные причины этого явления. Экспериментально построено семейство петель пьезоэлектрического гистерезиса при различных значениях частоты и напряженности внешнего смещающего поля. Полученные зависимости сравниваются с классическими петлями диэлектрического гистерезиса},
	number = {8},
	urldate = {2023-11-11},
	journal = {Журнал технической физики},
	author = {Бирюков, С. В. and Головко, Ю. И. and Масычев, С. И. and Мухортов, В. М. and Шелепо, А. П.},
	month = jul,
	year = {2009},
	pages = {90--92},
}



@article{__2008-1,
	title = {Феноменологическое описание фазовых переходов в тонких пленках {BaTiO}$_{\textrm{3}}$},
	volume = {50},
	url = {https://journals.ioffe.ru/articles/2648},
	abstract = {Проведено феноменологическое описание фазовых переходов в тонких эпитаксиальных пленках BaTiO3 на основе потенциалов Ландау шестой и восьмой степеней. Обнаружена зависимость вида фазовой диаграммы от величины электрострикционного коэффициента Q12. Для разных значений коэффициента Q12, известных из литературы, приведены качественно различные фазовые диаграммы. Определена зависимость деформации несоответствия (misfit strain) пленки от степени тетрагональности пленки при комнатной температуре, что позволяет определить термодинамический путь на фазовой диаграмме для конкретной пленки. Построены зависимости спонтанной поляризации и диэлектрической проницаемости пленки от деформации несоответствия при комнатной температуре.},
	language = {ru},
	number = {5},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Широков, В. Б. and Юзюк, Ю. И. and Dkhil, B. and Леманов, В. В.},
	year = {2008},
	pages = {889--896},
	file = {Физика твердого тела:C\:\\Users\\aleks\\Zotero\\storage\\BKW4NGEV\\2648.html:text/html},
}



@article{__2008-2,
	title = {Фазовые переходы в наноразмерных эпитаксиальных сегнетоэлектрических пленках титаната бария-стронция},
	volume = {4},
	issn = {1813-4289},
	url = {http://naukarus.com/fazovye-perehody-v-nanorazmernyh-epitaksialnyh-segnetoelektricheskih-plenkah-titanata-bariya-strontsiya},
	abstract = {С использованием дифракции рентгеновского излучения исследованы температурные зависимости параметров решетки в нормальном и тангенциальном к подложке направлении эиитакси-альных пленок титаната бария-стронция разной толщины (от 6 до 980 нм), выращенных по слоевому механизму высокочастотным катодным распылением при повышенном давлении кислорода. Выявлена критическая толщина пленок (-50 нм), ниже которой в пленках существуют сжимающие напряжения, а выше - растягивающие напряжения. Во всем интервале толщин при изменении температуры от 780 до 100 К в пленках наблюдаются два размытых структурных фазовых перехода второго рода.},
	number = {2},
	urldate = {2023-11-11},
	journal = {Вестник Южного научного центра РАН},
	author = {Головко, Ю. И. and Маматов, А. А. and Мухортов, В. М.},
	year = {2008},
	keywords = {⛔ No DOI found},
	file = {Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\PWGKVDJ4\\fazovye-perehody-v-nanorazmernyh-epitaksialnyh-segnetoelektricheskih-plenkah-titanata-bariya-st.html:text/html},
}



@article{__2008-3,
	title = {Структурные фазовые переходы в наноразмерных сегнетоэлектрических пленках титаната бария--стронция},
	volume = {50},
	url = {https://journals.ioffe.ru/articles/2579},
	abstract = {С использованием метода дифракции рентгеновского излучения исследованы температурные зависимости параметров решетки в нормальном и тангенциальном к подложке направлениях эпитаксиальных пленок титаната бария-стронция разной толщины (от 6 до 960 nm), выращенных по слоевому механизму высокочастотным катодным распылением при повышенном давлении кислорода. Выявлена критическая толщина пленок ({\textasciitilde}50 nm), ниже которой в пленках существуют сжимающие, а выше - растягивающие напряжения. Во всем интервале толщин при изменении температуры от 780 до 100 K в пленках наблюдаются два размытых структурных фазовых перехода второго рода. При растягивающих напряжениях переходы могут соответствовать переходам из тетрагональной параэлектрической фазы в aa-фазу и далее в r-фазу, в то время как при сжимающих напряжениях переходы происходят из тетрагональной параэлектрической фазы в сегнетоэлектрическую c-фазу, а при дальнейшем понижении температуры - в r-фазу. Работа проводилась при финансовой поддержке Российского фонда фундаментальных исследований (гранты N 05-02-17191 и 06-02-16271). PACS: 77.80.-e, 64.70.Nd, 77.55.+f},
	language = {ru},
	number = {3},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Головко, Ю. И. and Мухортов, В. М. and Юзюк, Ю. И. and Janolin, P. E. and Dkhil, B.},
	year = {2008},
	pages = {467--471},
	file = {Физика твердого тела:C\:\\Users\\aleks\\Zotero\\storage\\GRNCX2XX\\2579.html:text/html},
}



@article{__2008-4,
	title = {Особенности рамановских спектров и фазовых состояний в твердых растворах {Pb}$_{\textrm{x}}${Sr}$_{\textrm{1}}$ $_{\textrm{-}}$ $_{\textrm{x}}${TiO}$_{\textrm{3}}$ с низким содержанием свинца},
	volume = {72},
	issn = {0367-6765},
	url = {https://www.elibrary.ru/item.asp?id=9934183},
	abstract = {Приведены результаты исследований микрорамановского спектрального отклика в твердых растворах PbxSr1 - xTiO3 (x = 0.005, 0.01, 0.02, 0.03, 0.04) в диапазоне частот 151200 см-1 при нескольких температурах между 10 и 300 К. Проведенное исследование позволило сделать вывод, что в твердых растворах PST область концентраций с x {\textless} 0.04 скорее всего следует рассматривать как гетерофазную.},
	language = {ru},
	number = {4},
	urldate = {2023-11-11},
	journal = {Известия Российской Академии Наук. Серия Физическая},
	author = {Торгашев, В. И. and Чабанюк, А. Н. and Юзюк, Ю. И. and Леманов, В. В. and Sauvajol, J. L.},
	year = {2008},
	keywords = {⛔ No DOI found},
	pages = {569--571},
}



@article{__2008-5,
	title = {Диэлектрические свойства пленок титаната бария-стронция нанометровой толщины},
	volume = {78},
	url = {https://journals.ioffe.ru/articles/9548},
	abstract = {Методами субмиллиметровой и инфракрасной спектроскопии в области частот 10{\textless}nu{\textless}3000 cm-1 впервые измерены спектры отражения R(nu) и пропускания T(nu) гетероэпитаксиальных пленок титаната бария-стронция различной толщины на подложках MgO. Путем моделирования экспериментальных спектров френелевскими формулами для слоистых сред определены спектры комплексной диэлектрической проницаемости varepsilon*(nu)=varepsilon'(nu)+ivarepsilon''(nu) пленок. Показано, что при уменьшении толщины до 10 nm в пленках возникают растягивающие напряжения в направлении, параллельном плоскости подложки, вызывающие возрастание в несколько раз диэлектрического вклада низкочастотной мягкой моды. PACS: 77.22.Ch, 77.22.Gm, 78.20.Ci, 71.28.+d},
	language = {ru},
	number = {11},
	urldate = {2023-11-11},
	journal = {Журнал технической физики},
	author = {Мигунов, С. Н. and Волков, А. А. and Командин, Г. А. and Лобанов, А. Н. and Горшунов, Б. П. and Головко, Ю. И. and Мухортов, В. М. and Юзюк, Ю. И.},
	year = {2008},
	pages = {99--103},
	file = {Журнал технической физики:C\:\\Users\\aleks\\Zotero\\storage\\WZE458EK\\9548.html:text/html},
}



@article{__2008-6,
	title = {Внутренние напряжения и деформационный фазовый переход в наноразмерных пленках титаната бария-стронция},
	volume = {53},
	issn = {0023-4761},
	url = {https://www.elibrary.ru/item.asp?id=9955581},
	abstract = {Установлено, что при изменении толщины гетероэпитаксиальных пленок Ba0.8Sr0.2TiO3, выращенных по слоевому механизму роста на подложках (100) MgO, существует критическая толщина пленок ( 50 нм), характерная тем, что внутренние деформационные поля в пленках толщиной ниже критической существенно меньше, чем в пленках толщиной выше критической. При толщине ниже критической имеют место напряжения растяжения, а при больших толщинах  напряжения сжатия. Существование критической толщины подтверждено рентгеноструктурными данными и рамановской спектроскопией.},
	language = {ru},
	number = {3},
	urldate = {2023-11-11},
	journal = {Кристаллография},
	author = {Мухортов, В. М. and Головко, Ю. И. and Юзюк, Ю. И. and Латуш, Л. Т. and Жигалина, О. М. and Кускова, А. Н.},
	year = {2008},
	keywords = {⛔ No DOI found},
	pages = {536--542},
}



@article{katiyar_stress_2007,
	series = {Raman {Spectroscopy} {Workshop} 2006},
	title = {Stress manipulation in ferroelectric thin films and superlattices},
	volume = {45},
	issn = {0924-2031},
	url = {https://www.sciencedirect.com/science/article/pii/S0924203107000537},
	doi = {10.1016/j.vibspec.2007.05.004},
	abstract = {The integration of ferroelectric oxides into microelectronic devices requires a better understanding of stress and size effects onto ferroelectric properties of epitaxial thin films and superlattices which are generally imposed by the underlying substrate due to misfits in their lattice parameters and their thermal expansion coefficients. We have utilized polarized micro-Raman spectroscopy to investigate such stress effects in epitaxially grown Ba0.7Sr0.3TiO3 (BST-0.3) thin films and BaTiO3/SrTiO3 (BT/ST) superlattices with different periodicities as a function of temperature. In BST-0.3 films, the mismatch of the thermal expansion coefficients of the film and the substrate induces significant two-dimensional (2D) clamping and governs the domain structure formation. Moreover, the 2D stresses increase the Curie temperature remarkably and even change the phase-transition sequence in thin films, creating new phases, which were never observed in bulk materials. It is shown that in the epitaxial BST-0.3 films and BT/ST superlattices the E(TO) soft mode is very sensitive internal probe of 2D clamping and can be used for precise characterization.},
	language = {en},
	number = {2},
	urldate = {2023-11-11},
	journal = {Vibrational Spectroscopy},
	author = {Katiyar, R. S. and Yuzyuk, Yu. I.},
	month = nov,
	year = {2007},
	keywords = {Ferroelectrics, Raman spectroscopy, Superlattices},
	pages = {108--111},
}



@article{mishina_polarization_2007,
	title = {Polarization {Switching} in {Ferroelectric} {Thin} {Films} {Studied} by {Optical} {Second} {Harmonic} {Generation}},
	volume = {92},
	issn = {1058-4587},
	url = {https://doi.org/10.1080/10584580701746913},
	doi = {10.1080/10584580701746913},
	abstract = {Domain configuration during polarization switching in ferroelectric thin films was studied by optical second harmonic generation on different time scales: quasistatic (0.1 Hz), low-frequency (0.1–1 kHz) and fast (0.1 GHz). It is shown that within the electric pulses of several tenth of nanoseconds domain configuration may be different from the equilibrium.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Integrated Ferroelectrics},
	author = {Mishina, Elena and Sherstyuk, Nataliya and Golovko, Yurii and Muhortov, Vladimir and Sigov, Alexandr},
	month = dec,
	year = {2007},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/10584580701746913},
	pages = {65--76},
}



@article{shirokov_phenomenological_2007,
	title = {Phenomenological theory of phase transitions in epitaxial {BaTiO}$_{\textrm{3}}$ thin films},
	volume = {75},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.75.224116},
	doi = {10.1103/PhysRevB.75.224116},
	abstract = {We develop a phenomenological thermodynamic theory of ferroelectric BaTiO3 (BT) thin films epitaxially grown on cubic substrates using the Landau-Devonshire eight-order potential. The constructed “misfit-temperature” phase diagram is asymmetrical. We found that the overall view of the phase diagram depends on the values of compliances used in calculations and we provide two qualitatively different diagrams. A thermodynamic path for BT film grown onto a particular substrate can be found using a plot of the room-temperature tetragonal distortion (c−a)∕a as a function of misfit strain.},
	language = {en},
	number = {22},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Shirokov, V. B. and Yuzyuk, Yu. I. and Dkhil, B. and Lemanov, V. V.},
	month = jun,
	year = {2007},
	note = {Publisher: American Physical Society},
	pages = {224116},
}



@article{ankiewicz_electron_2007,
	title = {Electron paramagnetic resonance in transition metal-doped {ZnO} nanowires},
	volume = {101},
	issn = {0021-8979},
	url = {https://doi.org/10.1063/1.2402095},
	doi = {10.1063/1.2402095},
	abstract = {The wide-band-gap zinc oxide-based diluted magnetic semiconductors currently attract considerable attention due to their possible use in spintronic devices. In this work, we studied ZnO nanowire samples synthesized on 10×10 mm2 a-plane sapphire substrates by high-pressure pulsed laser deposition. The samples were characterized by scanning electron microscopy (SEM) and electron paramagnetic resonance (EPR) in the X-band (≃9.3 GHz) from T=4 to 300 K. According to the SEM pictures, the nanowires exhibit a length of about 1 μm and are aligned perpendicular to the substrate surface. The structures have a hexagonal cross section and their diameter ranges from 60 nm up to 150 nm. For the lowest nominal concentrations of xMn=3 at. \% and xCo=5 at. \%, we detect the anisotropic EPR spectra of isolated Mn2+ (3d5, S6) and Co2+ (3d7, F4), respectively, on Zn sites. The detection of the well-resolved anisotropic spectra proves a coherent crystallographic orientation of the nanowires. The linewidth was larger than the best values reported in the literature. Nevertheless, it was possible to identify two different components, A and B, of the reported spectra. From the temperature dependence of the EPR intensity, we found that both components exhibit paramagnetic behavior and are present in a concentration ratio of NB∕NA=1.4. In the case of the Mn-doped ZnO wires, the linewidth increases with increasing Mn concentration due to the dipole-dipole interaction of the paramagnetic ions. At the highest used nominal concentration, xMn=10 at. \%, an additional broad single line is observed.},
	language = {en},
	number = {2},
	urldate = {2023-11-11},
	journal = {Journal of Applied Physics},
	author = {Ankiewicz, A. O. and Carmo, M. C. and Sobolev, N. A. and Gehlhoff, W. and Kaidashev, E. M. and Rahm, A. and Lorenz, M. and Grundmann, M.},
	month = jan,
	year = {2007},
	pages = {024324},
}



@article{__2007-1,
	title = {Геометрические эффекты в наноразмерных эпитаксиальных пленках титаната бария-стронция},
	volume = {77},
	url = {https://journals.ioffe.ru/articles/9249},
	abstract = {Исследованы наноразмерные (6−950 nm) эпитаксиальные пленки Ba0.8Sr0.2TiO3 на (001) MgO с целью
изучения влияния толщины пленки на особенности проявления сегнетоэлектрических свойств. Данные
комбинационного рассеяния света и рентгеновской дифрактометрии показывают, что при толщине пленки
∼ 70 nm происходит структурный фазовый переход, при котором резко изменяются параметры решетки
пленки.
Спектры комбинационного рассеяния света наноразмерных пленок подтвердили наличие в них сегне тоэлектрического состояния и изменение симметрии при переходе пленок через критическую толщину,
что проявилось в резком смещении пиков, соответствующих A1 (TO) и E (TO) компонентам мягкой
моды. В области толщины пленок {\textless} 100 nm в зависимости диэлектрической проницаемости от толщины
появляются два максимума при толщине ∼ 18 и ∼ 36 nm. Диэлектрическая нелинейность в области первого
максимума существенно больше, чем в области второго.},
	language = {ru},
	number = {10},
	urldate = {2023-11-11},
	journal = {Журнал технической физики},
	author = {Мухортов, В. М. and Колесников, В. В. and Головко, Ю. И. and Бирюков, С. В. and Маматов, А. А. and Юзюк, Ю. И.},
	year = {2007},
	keywords = {⛔ No DOI found},
	pages = {97--102},
}



@article{__2007-2,
	title = {Влияние механизма роста и термоупругих напряжений на динамику кристаллической решетки гетероэпитаксиальных пленок титаната бария-стронция},
	volume = {49},
	url = {https://journals.ioffe.ru/articles/3167},
	language = {ru},
	number = {9},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Юзюк, Ю. И. and Захарченко, И. Н. and Алёшин, В. А. and Леонтьев, И. Н. and Рабкин, Л. М. and Мухортов, В. М. and Simon, P.},
	year = {2007},
	keywords = {⛔ No DOI found},
	pages = {1676--1682},
}



@article{gupta_optical_2006,
	series = {Proceedings of the {International} {Conference} on {Materials} for {Advanced} {Technologies} ({ICMAT} 2005) {Symposium} {N}},
	title = {Optical phonon modes in {ZnO} nanorods on {Si} prepared by pulsed laser deposition},
	volume = {287},
	issn = {0022-0248},
	url = {https://www.sciencedirect.com/science/article/pii/S0022024805011619},
	doi = {10.1016/j.jcrysgro.2005.10.039},
	abstract = {An array of vertically aligned c-axis-oriented zinc oxide (ZnO) nanorods were fabricated at a low substrate temperature (500°C) without using any catalytic template on the Si substrate by pulsed laser deposition at a high pressure (1–5Torr). The successive deposition of ZnO nanoparticles one over the other during growth led to the formation of elongated and well-isolated nanorods with a diameter in the range 70–350nm and up to 14μm long. The influence of deposition parameters on the Raman phonon modes was investigated. The polarized Raman studies were carried out in the backward geometry with incident light (i) parallel and (ii) perpendicular to the nanorod length. The activation of lower and upper surface phonon modes were observed in the ZnO nanorods between the transverse optical (ωTO) and the longitudinal optical (ωLO) phonon frequencies. The lower surface mode observed at ∼475cm−1 is found to be predominant in the X(ZZ)X¯ configuration. The surface phonon modes were not found in the samples prepared at {\textgreater}600°C due to the coalescence process resulting in a continuous film. The agreement of polarized Raman spectra with single crystal data indicates the growth of good quality ZnO nanorods, and allows direct integration on Si without introducing contamination at the interface due to any catalytic material.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Journal of Crystal Growth},
	author = {Gupta, Vinay and Bhattacharya, P. and Yuzuk, Yu. I. and Sreenivas, K. and Katiyar, R. S.},
	month = jan,
	year = {2006},
	keywords = {A1. axis orientation, A1. Nanorods, A1. Raman scattering, A1. Surface phonon mode, A3. PLD, B2. Zinc oxide},
	pages = {39--43},
	file = {ScienceDirect Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\HR85BTQK\\S0022024805011619.html:text/html},
}



@article{_-_2006,
	title = {Ротационно-полярные структурные искажения в твердых растворах {Pb}$_{\textrm{1-x}}${Ca}$_{\textrm{x}}${TiO}$_{\textrm{3}}$ на основе данных спектроскопии комбинационного рассеяния света},
	volume = {48},
	url = {https://journals.ioffe.ru/articles/3406},
	abstract = {При проведении высокотемпературных (290−560 K) исследований поляризованных спектров комбинаци онного рассеяния света в области частот 6 {\textless}ν{\textless} 1200 cm−1 на монокристаллическом образце твердого
раствора Pb0.55Ca0.45TiO3 установлено существование трех особых температурных точек, по крайней мере
в двух из которых происходят структурные фазовые переходы. В рамках теории Ландау фазовых переходов
второго рода обсуждается допустимая топология фазовых диаграмм, качественно верно отражающая
экспериментальную ситуацию.},
	language = {ru},
	number = {5},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Торгашев, В. И. and Юзюк, Ю. И. and Широков, В. Б. and Леманов, В. В.},
	year = {2006},
	keywords = {⛔ No DOI found},
	pages = {864--873},
}



@article{__2006-1,
	title = {Концентрационный фазовый переход в твердых растворах {Pb}$_{\textrm{1-x}}${Ca}$_{\textrm{x}}${TiO}$_{\textrm{3}}$ по данным спектроскопии комбинационного рассеяния света},
	volume = {48},
	url = {https://journals.ioffe.ru/articles/3382},
	abstract = {Впервые на монокристаллических образцах твердых перовскитных растворов Pb1−xCaxTiO3 (составы:
x = 0, 0.03, 0.04, 0.15, 0.23, 0.28, 0.34, 0.38, 0.40, 0.45 и 0.50) получены поляризованные спектры
комбинационного рассеяния света и ИК отражения в области частот 6 {\textless}ν{\textless} 1200 cm−1 и температурах
290–620 K. Основное внимание уделено низкочастотной динамике решетки, где установлено аномальное
концентрационное поведение фононного спектрального отклика при 0.38 {\textless} x {\textless} 0.40. При комнатной
температуре в области x {\textgreater} 0.40 в твердых растворах Pb1−xCaxTiO3 реализуется новое фазовое состояние,
которое, вероятно, является полярным},
	language = {ru},
	number = {4},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Торгашев, В. И. and Юзюк, Ю. И. and Леманов, В. В. and Kuntscher, C. A.},
	year = {2006},
	keywords = {⛔ No DOI found},
	pages = {717--725},
}



@article{__2019-2,
	title = {Оптические свойства фотонных кристаллов на основе наностержней оксида цинка, покрытых тонкой пленкой плазмонного материала},
	volume = {1},
	url = {https://elibrary.ru/item.asp?id=39539483},
	abstract = {В данной работе исследовались зависимости оптических свойств фотонных кристаллов, представляющих двумерно-периодическую решетку наностержней оксида цинка от геометрических параметров и типов их тонкопленочного покрытия плазмонными материалами (Au, Ag, Cu, AZO, GZO, AGZO и т. п.). В расчетах учтены свойства металлов и диэлектриков в оптическом диапазоне. Характеристики двухмерно-периодических структур, образованных бесконечно длинными слоистыми цилиндрами на основе ZnO, рассчитаны методом разделения переменных в цилиндрической системе координат. Проведено сравнение полученных численных данных с результатами конечноэлементного моделирования.},
	language = {ru},
	urldate = {2023-11-11},
	journal = {Электроника И Микроэлектроника Свч},
	author = {Лерер, А. М. and Тимошенко, П. Е. and Головачева, Е. В. and Кайдашев, Е. М. and Турчин, А. С.},
	year = {2019},
	keywords = {Дифракция, Наностержни, Оксид Цинка, Оптические Наноантенны, Оптические Свойства, Плазмон-Поляритон, Плазмонный Резонанс, Фотонная Запрещенная Зона, Фотонный Кристалл, ⛔ No DOI found},
	pages = {209--213},
}



@article{__2017-3,
	title = {Уникальный атомный порядок гиперкагоме в геометрически фрустрированных иридиевых шпинелеподобных структурах},
	issn = {1026-3500, 2658-784X},
	url = {https://elibrary.ru/item.asp?id=30304556},
	abstract = {Представлен краткий авторский обзор результатов теоретического исследования уникального атомного и орбитального порядка гиперкагоме в геометрически фрустрированных иридиевых шпинелеподобных структурах. Установлен структурный механизм образования атомного порядка гиперкагоме. Показано, что фундаментальной структурной особенностью иридиевых шпинелеподобных структур является существование замкнутых контуров химических связей Ir-Ir, каждый из которых состоит из десяти атомов - декагонов. Высказано предположение, что декагоны обусловливают аномальные химические и физические свойства кристаллов. Сделан прогноз структурных типов кристаллов, в которых может существовать атомный порядок гиперкагоме.},
	language = {ru},
	number = {10},
	urldate = {2023-11-11},
	journal = {Известия Академии Наук. Серия Химическая},
	author = {Таланов, М. В. and Таланов, В. М. and Широков, В. Б.},
	year = {2017},
	keywords = {Геометрическая Фрустрация, Декагоны, Порядок Гиперкагоме, Упорядоченные Шпинели, ⛔ No DOI found},
	pages = {1719--1727},
}



@article{_-_2006-1,
	title = {Конечно-элементное моделирование в динамических задачах для упругих решеток микро- и нанокристаллов из оксида цинка},
	volume = {2},
	issn = {1813-4289},
	url = {https://www.elibrary.ru/item.asp?id=12884469},
	abstract = {Представлены результаты конечно-элементного моделирования процессов деформирования решетки нано- и микрокристаллов из оксида цинка. В рамках плоской теории электроупругости рассмотрены свободные и вынужденные колебания, а также нестационарные задачи для решетки микро- или нанокристаллов из оксида цинка, расположенных на подложке сапфира. Определены собственные частоты для системы решетка кристаллов - подложка, показано, что по найденному спектру большой системы (решетка - подложка) и спектру подложки можно определить первые собственные частоты одного нанокристалла. Это позволяет по экспериментальным данным для больших систем определить собственные частоты нанообъекта, которые непосредственно трудно определить другим способом. Знание собственных частот позволяет, в частности, судить о механических свойствах нанокристалла. Обсуждается возможность использования решеток нанокристаллов в качестве элементов наносенсоров.},
	language = {ru},
	number = {1},
	urldate = {2023-11-11},
	journal = {Вестник Южного Научного Центра Ран},
	author = {Еремеев, В. А. and Кайдашев, Е. М. and Соловьев, А. Н.},
	year = {2006},
	keywords = {⛔ No DOI found},
	pages = {10--15},
}



@article{__2017-4,
	title = {Влияние барьерных веществ на магниторезистивные свойства композитов на основе манганита лантана стронция},
	issn = {2073-8633},
	url = {https://elibrary.ru/item.asp?id=29911660},
	abstract = {Based on our own, as well as literary experimental data, the analysis of the Influence of a barrier material used to create heterogeneous composites based on La0.7Sr0.3MnO3 on their magnetoresistive properties is carried out. Such composites differ in existence of an isotropic negative magnitorezistivnost (MR) connected from backs - dependent tunneling of carriers in magnetic field. The largest value MR up to 15\% in the field of 15 kOe are shown when using glass-like GeO2 oxide at a percolation ratio of components.},
	language = {ru},
	number = {2 (45)},
	urldate = {2023-11-11},
	journal = {Инженерный Вестник Дона},
	author = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Богатин, А. С. and Чебанова, Е. В. and Пруцакова, Н. В. and Русакова, Е. Б.},
	year = {2017},
	keywords = {Барьерный Слой, Диэлектрическая Проницаемость, Керамика, Композитный Материал, Магниторезистивность, Манганит Лантана Стронция, Одношаговый Синтез, Порог Перколяции, Спиновая Поляризация, Туннелирование, ⛔ No DOI found},
	pages = {4},
}



@article{__2009-4,
	title = {Гетероэпитаксиальные плёнки мультиферроика феррита висмута, допированного неодимом},
	volume = {179},
	issn = {0042-1294},
	url = {https://ufn.ru/ru/articles/2009/8/k/},
	abstract = {Гетероэпитаксиальные плёнки мультиферроика феррита висмута, допированного неодимом, Мухортов В.М., Головко Ю.И., Юзюк Ю.И.},
	language = {ru},
	number = {8},
	urldate = {2023-11-11},
	journal = {Успехи физических наук},
	author = {Мухортов, В. М. and Головко, Ю. И. and Юзюк, Ю. И.},
	month = aug,
	year = {2009},
	keywords = {⛔ No DOI found},
	pages = {909--913},
	file = {Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\2X6KHVNX\\Мухортов и др. - 2009 - Гетероэпитаксиальные плёнки мультиферроика феррита.pdf:application/pdf},
}



@article{__2016-1,
	title = {Оптические наноантенны на новых плазмонных материалах на основе оксида цинка},
	volume = {1},
	url = {https://elibrary.ru/item.asp?id=26607463},
	language = {ru},
	urldate = {2023-11-11},
	journal = {Электроника И Микроэлектроника Свч},
	author = {Лерер, А. М. and Тимошенко, П. Е. and Головачева, Е. В. and Кайдашев, Е. М. and Пузанов, А. С.},
	year = {2016},
	keywords = {Дифракция, Оптические Наноантенны, Конечно-Элементное Моделирование, Фотонно-Кристаллические Структуры, Zno Наностержни, ⛔ No DOI found},
	pages = {279--282},
}



@article{___2005,
	title = {Особенности динамики переключения поляризации в тонких пленках цирконата–титаната–свинца},
	volume = {75},
	url = {https://journals.ioffe.ru/articles/viewPDF/8639},
	number = {5},
	journal = {Журнал технической физики},
	author = {{Мухортов В.М.} and {Колесников В.В.} and {Головко Ю.И.} and {Мащенко А.И.} and {Бирюков С.В.}},
	year = {2005},
	keywords = {⛔ No DOI found},
	pages = {126--131},
}



@article{__2007-3,
	title = {Магнитоэлектрические и нелинейно-оптические свойства пленок {BiFeO}$_{\textrm{3}}$, допированных неодимом},
	issn = {1813-8586},
	url = {https://www.elibrary.ru/item.asp?id=11693334},
	abstract = {Методом магнетронного распыления получены мо-нокристаллические и поликристаллические пленки фер-рита висмута. Показано, что монокристаллические пленки обладают высокими значениями остаточной по-ляризации и намагниченности насыщения. Наличие маг-нитоэлектрического взаимодействия подтверждено нели-нейно-оптическими измерениями.},
	language = {ru},
	number = {12},
	urldate = {2023-11-11},
	journal = {Нано- И Микросистемная Техника},
	author = {Кузнецов, М. А. and Мишина, Е. Д. and Морозов, А. И. and Сигов, А. С. and Головко, Ю. И. and Мухортов, В. М. and Мошняга, В. Т.},
	year = {2007},
	keywords = {⛔ No DOI found},
	pages = {20--22},
}



@article{__2005,
	title = {Спектры комбинационного рассеяния света титаната кадмия},
	volume = {47},
	url = {https://journals.ioffe.ru/articles/3735},
	abstract = {Впервые получены поляризованные спектры комбинационного рассеяния света монокристаллических
образцов CdTiO3 в области частот 5 {\textless}ν{\textless} 1000 cm$^{\textrm{−1}}$ при температурах 10−1200 K. Основное внима ние уделено низкочастотной области, где обнаружено аномальное температурное поведение нескольких
фононных мод. Высокотемпературными исследованиями выявлено существование четырех фононов с характерным для мягких мод поведением. Эти фононы отнесены к модам, восстанавливающим кубическую симметрию решетки. Экстраполяции их температурных зависимостей позволили выдвинуть гипотезу о существовании цепочки из трех гипотетических высокотемпературных фазовых переходов, аналогичных тем, что наблюдаются собственно в перовските CaTiO3. При температурах ниже 78 K спектр комбинационного рассеяния обогащается новыми линиями, появление которых связано с полярными искажениями ячейки. На низких частотах обнаружено три линии с аномальным поведением осцилляторных параметров, которое характерно для мягких мод в сегнетоэлектрических фазах. Предполагается возможность существования нескольких разных полярных состояний при низких температурах.},
	number = {2},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Торгашев, В. И. and Юзюк, Ю. И. and Широков, В. Б. and Леманов, В. В. and Спектор, И. Е.},
	year = {2005},
	keywords = {⛔ No DOI found},
	pages = {324--333},
	file = {Физика твердого тела:C\:\\Users\\aleks\\Zotero\\storage\\9NBHHWBQ\\3735.html:text/html;Физика твердого тела.pdf:C\:\\Users\\aleks\\Zotero\\storage\\3H3Z7B97\\Физика твердого тела.pdf:application/pdf},
}



@article{__2005-1,
	title = {Формирование доменной структуры под действием деформационных полей в наноразмерных пленках титаната бария-стронция},
	volume = {31},
	url = {http://elibrary.lt/resursai/Uzsienio%20leidiniai/ioffe/pztf/2005/23/pztf_t31v23_12.pdf},
	number = {23},
	urldate = {2023-11-11},
	journal = {Письма ЖТФ},
	author = {Мухортов, В. М. and Головко, Ю. И. and Колесников, В. В. and Бирюков, С. В.},
	year = {2005},
	keywords = {⛔ No DOI found},
	pages = {75--81},
}



@article{__2014-6,
	title = {Переключение поляризации в наноразмерных пленках титаната бария стронция},
	volume = {9},
	issn = {1992-7223, 1993-4068},
	url = {https://elibrary.ru/item.asp?id=21184158},
	abstract = {Исследовано переключение поляризации сегнетоэлектрических тонких пленок Ba0.8Sr0.2TiO3 толщиной 2–150 нм, осажденных на Si(111) с Pt подслоем. Критическим параметром при переключении поляризации является площадь сегнетоэлектрического кристаллита. Пленки толщиной 2 нм обладают сегнетоэлектрическими свойствами.Polarization switching in Ba0.8Sr0.2TiO3 ferroelectric 2–150 nm-thick thin films deposited on Pt coated Si(111) substrates was studied. The area of the ferroelectric crystallite is shown to be a critical parameter for polarization switching. The 2 nm-thick films possess ferroelectric properties.},
	language = {ru},
	number = {1-2},
	urldate = {2023-11-11},
	journal = {Российские Нанотехнологии},
	author = {Мухортов, В. М. and Сова, Е. М. and Широков, В. Б. and Головко, Ю. И. and Лянгузов, Н. В. and Юзюк, Ю. И.},
	year = {2014},
	keywords = {Кристаллит, Наноразмер, Наноразмерная Пленка, Поляризация, Сегнетоэлектрический, Титанат Бария Стронция, ⛔ No DOI found},
	pages = {55--58},
}



@article{tikhonov_comparative_2017,
	title = {A comparative {X}-ray diffraction study of ferroelectric thin films and superlattices},
	copyright = {© 2017 Taylor \& Francis Group, LLC},
	issn = {0015-0193},
	url = {https://www.tandfonline.com/doi/abs/10.1080/00150193.2017.1289764},
	abstract = {A number of ferroelectric thin films with various barium concentration and two sets of superlattices with different composition and number of constituent layers were investigated using X-ray diffra...},
	language = {EN},
	urldate = {2023-11-11},
	journal = {Ferroelectrics},
	author = {Tikhonov, Yu A. and Zakharchenko, I. N. and Razumnaya, A. G. and Yuzyuk, Y. I. and Pavunny, Sh and Ortega, N. and Kumar, A. and Katiyar, R. S.},
	month = feb,
	year = {2017},
	note = {Publisher: Taylor \& Francis},
	keywords = {⛔ No DOI found},
	file = {Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\VRJ96NXD\\full.html:text/html},
}



@article{noauthor__nodate,
	title = {Влияние механизма роста и термоупругих напряжений на динамику кристаллической решетки гетероэпитаксиальных пленок титаната бария--стронция},
	url = {https://journals.ioffe.ru/articles/3167},
	urldate = {2023-11-11},
}



@article{yuzyuk_stress_2007,
	title = {Stress alteration in heteroepitaxial ({Ba},{Sr}){TiO}$_{\textrm{3}}$/(001) {MgO} thin films via growth mechanism},
	volume = {40},
	issn = {0022-3727},
	url = {https://dx.doi.org/10.1088/0022-3727/40/14/025},
	doi = {10.1088/0022-3727/40/14/025},
	abstract = {We have studied stress effects in heteroepitaxial (Ba0.7Sr0.3)TiO3 thin films deposited by rf sputtering on (0 0 1) MgO substrates. By varying the deposition conditions, three-dimensional (3D) nucleation growth and layer-by-layer growth mechanisms were realized. X-ray diffraction (XRD) measurements revealed that tetragonal distortion and Curie temperature (Tc) depend on the growth mechanism. The frequency of the E(TO) soft mode in the polarized Raman spectra correlated with the value of two-dimensional stress, determined from XRD experiments. Temperature-dependent lattice parameters and Raman spectra revealed an upward shift of the Curie temperature. Two-dimensional compressive stress was found to be larger in the film grown by the 3D nucleation mechanism.},
	language = {en},
	number = {14},
	urldate = {2023-11-11},
	journal = {Journal of Physics D: Applied Physics},
	author = {Yuzyuk, Yu I. and Simon, P. and Zakharchenko, I. N. and Alyoshin, V. A. and Leontyev, I. N. and Mukhortov, V. M.},
	month = jun,
	year = {2007},
	pages = {4271},
}



@book{__2008-7,
	title = {Гетероструктуры на основе наноразмерных сегнетоэлектрических пленок: получение, свойства и применение},
	isbn = {978-5-902982-42-5},
	shorttitle = {Гетероструктуры на основе наноразмерных сегнетоэлектрических пленок},
	url = {https://rusneb.ru/catalog/000199_000009_004241648/},
	abstract = {«Гетероструктуры на основе наноразмерных сегнетоэлектрических пленок: получение, свойства и применение» (978-5-902982-42-5 (в пер.)) — Мухортов, Владимир Михайлович, 221, [1] с.. Издано: (2008). ✔Читать онлайн. ✔Адрес библиотеки с ближайшим печатным изданием ➤ RusNeb.ru.},
	language = {ru},
	urldate = {2023-11-11},
	author = {Мухортов, В. М. and Юзюк, Ю. И.},
	year = {2008},
	file = {Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\VMDT5IMU\\000199_000009_004241648.html:text/html},
}



@article{lorenz_mgxzn1xo0x02_2005,
	title = {Mg$_{\textrm{x}}${Zn}$_{\textrm{1−x}}${O}(0⩽x{\textless}0.2) nanowire arrays on sapphire grown by high-pressure pulsed-laser deposition},
	volume = {86},
	issn = {0003-6951},
	url = {https://doi.org/10.1063/1.1898433},
	doi = {10.1063/1.1898433},
	abstract = {MgxZn1−xO nanowires with Mg-content x from 0 to 0.2 have been grown by high-pressure pulsed-laser deposition (PLD) on gold-covered sapphire single crystals. The PLD process allows for a unique wide-range control of morphology, diameter, and composition of the MgxZn1−xO nanowires. The diameter of single ZnO wires could be varied between about 50 and 3000 nm, and the Mg content x of MgxZn1−xO wire arrays was controlled via the PLD gas pressure. The microscopic homogeneity of Mg content is displayed by cathodoluminescence (CL) imaging of the excitonic peak energy. The fluctuation of CL peak energy between individual wires is about an order of magnitude smaller than the alloy broadening.},
	number = {14},
	urldate = {2023-11-11},
	journal = {Applied Physics Letters},
	author = {Lorenz, M. and Kaidashev, E. M. and Rahm, A. and Nobis, Th. and Lenzner, J. and Wagner, G. and Spemann, D. and Hochmuth, H. and Grundmann, M.},
	month = mar,
	year = {2005},
	pages = {143113},
}



@article{jain_local_2005,
	title = {Local symmetry breaking in {Pb}$_{\textrm{x}}${Sr}$_{\textrm{1−x}}${TiO}$_{\textrm{3}}$ ceramics and composites studied by {Raman} spectroscopy},
	volume = {98},
	issn = {0021-8979},
	url = {https://doi.org/10.1063/1.1989434},
	doi = {10.1063/1.1989434},
	abstract = {Local symmetry breaking in PbxSr1−xTiO3 (PST) solid solutions was revealed by Raman spectroscopy below and above the ferroelectric phase-transition temperature. In the paraelectric phase, local symmetry breaking associated with the polar clusters localized mostly at grain boundaries in ceramic samples leads to the activation of the polar modes far above the dielectric maximum. This effect was found remarkably enhanced in the PST:MgO composites due to the compositional inhomogeneity of the grain boundaries and the intergrain stresses in the composite. In the ferroelectric phase, the degeneracy of the E(TO1) soft mode was lifted due to translational symmetry breaking in the solid solutions with x=0.2 and 0.3, where the substitution of Sr by Pb replaces partially the ionic bonding between the A cations and the oxygens by a stronger covalent bonding.},
	number = {2},
	urldate = {2023-11-11},
	journal = {Journal of Applied Physics},
	author = {Jain, M. and Yuzyuk, Yu. I. and Katiyar, R. S. and Somiya, Y. and Bhalla, A. S.},
	month = jul,
	year = {2005},
	pages = {024116},
}



@article{katiyar_polarized_2005,
	title = {Polarized {Raman} {Spectra} of {BaTiO}$_{\textrm{3}}$/{SrTiO}$_{\textrm{3}}$ {Superlattices}},
	volume = {329},
	issn = {0015-0193},
	url = {https://doi.org/10.1080/00150190500314833},
	doi = {10.1080/00150190500314833},
	abstract = {BaTiO 3 /SrTiO 3 superlattices were grown on (001)MgO substrates by pulsed-laser-deposition technique. The thickness of each layer varied from 6 to 25 unit cells. Polarization-dependent Raman spectra confirmed tetragonal symmetry of the superlattices with the polar axis being normal to the layers. The observed optic modes in the superlattices showed intermediate frequencies between corresponding bulk BaTiO 3 and SrTiO 3 values, while the E(TO 1 ) soft mode exhibited upward shift due to significant two-dimensional clamping caused by the lattice mismatch of the constituting layers. The observed downward shift of the soft mode revealed relaxation of two-dimensional stresses with increasing the stacking periodicity of the superlattices. The excitation of folded transverse acoustic phonons in the Raman spectra due to the new periodicity of the Brillouin zone was revealed. The observed data are quantitatively explained by a folding of the corresponding acoustic branch. It is shown that micro-Raman spectroscopy provides determination of a spatial variation of the layer thickness in graded superlattices. On leave from the Faculty of Physics, Rostov State University, Rostov-on-Don, Russia},
	number = {1},
	urldate = {2023-11-11},
	journal = {Ferroelectrics},
	author = {Katiyar, Ram S. and Yuzyuk†, Yu. I. and Das, R. R. and Bhattacharya, P. and Gupta, V.},
	month = dec,
	year = {2005},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/00150190500314833},
	pages = {3--12},
}



@article{das_folded_2004,
	title = {Folded acoustic phonons and soft mode dynamics in {BaTiO}$_{\textrm{3}}$/{SrTiO}$_{\textrm{3}}$ superlattices},
	volume = {69},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.69.132302},
	doi = {10.1103/PhysRevB.69.132302},
	abstract = {A series of BaTiO3/SrTiO3 superlattices with stacking periodicity of 6–10 unit cells were fabricated on (001)MgO substrates using pulsed-laser-deposition technique. Polarized Raman spectra revealed BaTiO3-like optical vibrations and confirmed tetragonal symmetry of the superlattices with the c axis being normal to the layers. Due to in-plane compressive stresses generated by the lattice mismatch of the constituting layers, the E(1TO) soft mode was underdamped and markedly shifted to higher frequencies with respect to its analogs in the bulk. The existence of perfect superlattice structure was evident from the observation of the folded acoustic phonons in Raman spectra. The frequencies of the folded phonons matched well with the calculated transverse-acoustic branches of the constituent materials. No phase transitions were revealed in the superlattices below room temperature, while phase transition to the paraelectric state is shifted up to 650–700 K and it is diffused.},
	number = {13},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Das, Rasmi R. and Yuzyuk, Yu. I. and Bhattacharya, P. and Gupta, V. and Katiyar, R. S.},
	month = apr,
	year = {2004},
	note = {Publisher: American Physical Society},
	pages = {132302},
}



@article{gupta_growth_2004,
	title = {Growth and characterization of c-axis oriented {LiNbO}$_{\textrm{3}}$ film on a transparent conducting {Al}:{ZnO} inter-layer on {Si}},
	volume = {19},
	issn = {2044-5326},
	shorttitle = {Growth and characterization of c-axis oriented {LiNbO3} film on a transparent conducting {Al}},
	url = {https://doi.org/10.1557/JMR.2004.0322},
	doi = {10.1557/JMR.2004.0322},
	abstract = {C-axis oriented lithium niobate (LiNbO3) films were deposited by pulsed-laser deposition on silicon using a transparent conducting interlayer of aluminum (Al)-doped zinc oxide (ZnO). Only two x-ray diffraction reflections corresponding to (006) and (0012) planes of LiNbO3 were observed in the films deposited at a 100-mTorr oxygen pressure and a 450–500 °C substrate temperature. Presence of sharp modes corresponding to E(TO) and A(LO), and absence of any superfluous peaks mainly around 900–905 cm−1 in the Raman spectra confirmed the formation of textured LiNbO3 film. Measured value of direct current and alternate current (AC) conductivities and dielectric constant are 8.6 × 10-12 Ω−1cm-1, 1.16 × 10-6 Ω−1cm-1, and 29.3, respectively, at room temperature. Behavior of dielectric constant and AC conductivity with frequency and temperature are close to the reported single-crystal data.},
	language = {en},
	number = {8},
	urldate = {2023-11-11},
	journal = {Journal of Materials Research},
	author = {Gupta, Vinay and Bhattacharya, P. and Yuzyuk, Yu. I. and Katiyar, R. S. and Tomar, Monika and Sreenivas, K.},
	month = aug,
	year = {2004},
	pages = {2235--2239},
}



@article{kholkin_raman_2004,
	title = {Raman scattering in sol–gel derived {PbTiO}$_{\textrm{3}}$ films modified with {Ca}},
	volume = {85},
	issn = {0254-0584},
	url = {https://www.sciencedirect.com/science/article/pii/S025405840400029X},
	doi = {10.1016/j.matchemphys.2004.01.001},
	abstract = {X-ray diffraction (XRD) and Raman scattering in sol–gel derived Pb1−xCaxTiO3 (PCT) thin films are studied as a function of Ca content x. It is found that Ca2+ addition to PbTiO3 films results in a gradual decrease of tetragonality of the perovskite lattice accompanied with a considerable modification of the Raman spectra. A significant difference in Raman spectra of PCT films and available reference data for single crystals (x=0) is explained in terms of the large internal stress, small grain size, and structural disorder produced by Ca2+ substitution. It is found that the shift of the frequency of ferroelectric soft mode correlates well with the variation of tetragonality for x≤xc=0.4. The concentration dependence of the shift is strongly non-linear being qualitatively different from that observed earlier in other A-site doped lead titanate-based systems. According to XRD data, the averaged crystal structure for xc≈0.4 appears as pseudo-cubic, while Raman scattering revealed short-range order tetragonal distortion. The structural characteristics of PCT films are linked to their electromechanical properties measured earlier by interferometric technique.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Materials Chemistry and Physics},
	author = {Kholkin, A. L and Bdikin, I and Yuzyuk, Yu. I and Almeida, A and Chaves, M. R and Calzada, M. L and Mendiola, J},
	month = may,
	year = {2004},
	keywords = {Ferroelectricity, Thin films, Raman spectroscopy and scattering, Sol–gel growth},
	pages = {176--179},
}



@article{korolkov_nanodimensional_2004,
	title = {Nanodimensional effects in the structure of epitaxial {YBa}$_{\textrm{2}}${Cu}$_{\textrm{3}}${O}$_{\textrm{7-y}}$ films},
	volume = {30},
	issn = {1090-6533},
	url = {https://doi.org/10.1134/1.1666963},
	doi = {10.1134/1.1666963},
	abstract = {We have studied the structure of YBa2Cu3O7−y(YBCO) high-Tcsuperconductor films obtained by deposition for various times under otherwise identical conditions. Thin YBCO films prepared by the nonaxial laser shadow deposition technique are epitaxial and have microstrains below 1×10−3. The main factor determining variations of the unit cell parameter c in the films is the difference of the crystal block size 〈D〉 in the direction normal to the film surface, which reflects the nanodimensional effects known in oxides.},
	language = {en},
	number = {2},
	urldate = {2023-11-11},
	journal = {Technical Physics Letters},
	author = {Korol’kov, D. S. and Kaidashev, E. M. and Abdulvakhidov, K. G. and Kupriyanov, M. F.},
	month = feb,
	year = {2004},
	keywords = {Block Size, Cell Parameter, Film Surface, Identical Condition, Oxide},
	pages = {135--137},
}



@article{prosandeev_lattice_2004,
	title = {Lattice dynamics in {PbMg}$_{\textrm{1/3}}${Nb}$_{\textrm{2/3}}${O}$_{\textrm{3}}$},
	volume = {70},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.70.134110},
	doi = {10.1103/PhysRevB.70.134110},
	abstract = {Lattice dynamics for five ordered PbMg1∕3Nb2∕3O3 supercells were calculated from first principles by the frozen phonon method. Maximal symmetries of all supercells are reduced by structural instabilities. Lattice modes corresponding to these instabilities, equilibrium ionic positions, and infrared reflectivity spectra were computed for all supercells. Results are compared with our experimental data for a chemically disordered PMN single crystal.},
	number = {13},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Prosandeev, S. A. and Cockayne, E. and Burton, B. P. and Kamba, S. and Petzelt, J. and Yuzyuk, Yu. and Katiyar, R. S. and Vakhrushev, S. B.},
	month = oct,
	year = {2004},
	note = {Publisher: American Physical Society},
	pages = {134110},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\GZG82Z22\\Prosandeev и др. - 2004 - Lattice dynamics in \$ mathrm PbMg _ 1∕3 mathrm.pdf:application/pdf;APS Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\T9HNHJSG\\PhysRevB.70.html:text/html},
}



@article{schmidt-grund_uvvuv_2004,
	series = {The 3rd {International} {Conference} on {Spectroscopic} {Ellipsometry}},
	title = {{UV}–{VUV} spectroscopic ellipsometry of ternary {Mg}$_{\textrm{x}}${Zn}$_{\textrm{1−x}}${O} (0≤x≤0.53) thin films},
	volume = {455-456},
	issn = {0040-6090},
	url = {https://www.sciencedirect.com/science/article/pii/S004060900301856X},
	doi = {10.1016/j.tsf.2003.11.249},
	abstract = {The ordinary optical dielectric functions of pulsed-laser-deposition grown wurtzite c-plane MgxZn1−xO (0≤x≤0.53) thin films have been determined by using spectroscopic ellipsometry in the photon energy range from 4.5 to 9.5 eV. The dielectric functions reveal features which resemble those previously detected in uniaxial AlGaN and identified as E1- and E2-type band-to-band transitions with no remarkable dependence of the transition energy on Mg content x. The E1- and E2-type transitions for ZnO are compared with pseudopotential band-structure calculations.},
	urldate = {2023-11-11},
	journal = {Thin Solid Films},
	author = {Schmidt-Grund, R. and Schubert, M. and Rheinländer, B. and Fritsch, D. and Schmidt, H. and Kaidashev, E. M. and Lorenz, M. and Herzinger, C. M. and Grundmann, M.},
	month = may,
	year = {2004},
	keywords = {Optical properties, Dielectric function, Ellipsometry, MgZnO, Vacuum ultraviolet, Zinc oxide (ZnO), ZnMgO},
	pages = {500--504},
	file = {ScienceDirect Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\E97NUBSQ\\S004060900301856X.html:text/html},
}



@article{spemann_ion_2004,
	series = {Proceedings of the {Sixteenth} {International} {Conference} on {Ion} {Beam} {Analysis}},
	title = {Ion beam analysis of epitaxial ({Mg}, {Cd})$_{\textrm{x}}${Zn}$_{\textrm{1−x}}${O} and {ZnO}:({Li}, {Al}, {Ga}, {Sb}) thin films grown on c-plane sapphire},
	volume = {219-220},
	issn = {0168-583X},
	shorttitle = {Ion beam analysis of epitaxial ({Mg}, {Cd}){xZn1}−{xO} and {ZnO}},
	url = {https://www.sciencedirect.com/science/article/pii/S0168583X0400223X},
	doi = {10.1016/j.nimb.2004.01.183},
	abstract = {In this study ZnO thin films, nominally undoped, doped with Li, Al, Ga and Sb and alloyed with Mg and Cd grown epitaxially on c-plane sapphire by pulsed laser deposition (PLD) were investigated. In order to correlate the optical and electrical properties, e.g. the band gap energy and carrier concentration, to the elemental composition, the films were analyzed by RBS, PIXE and PIGE using He+ and H+ ion beams. It was found that the element transfer from the PLD target to the film differs significantly for the individual doping and alloying elements, with concentration ratios between film and target ranging from ∼4\% for Li and Cd to ∼400\% for Ga. In general, the films exhibited a metal to oxygen ratio of 1:1, only the ZnO:Li films were slightly oxygen deficient. Furthermore, the crystalline quality of the films was investigated using ion channeling. The nominally undoped ZnO films which were deposited with low-temperature interlayers for lower lateral stress showed a normalized minimum RBS yield of χmin=3.3\% under channeling conditions. Whereas the incorporation of isovalent alloying atoms into the ZnO films leads to a slight degradation of the crystalline quality only, doping degrades the crystalline quality remarkably, even at low dopant concentrations.},
	urldate = {2023-11-11},
	journal = {Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms},
	author = {Spemann, D and Kaidashev, E. M and Lorenz, M and Vogt, J and Butz, T},
	month = jun,
	year = {2004},
	keywords = {Elemental composition, Thin films, Zinc oxide, Crystalline quality},
	pages = {891--896},
}



@article{yuzyuk_synchrotron_2004,
	title = {Synchrotron x-ray diffraction and {Raman} scattering investigations of ({Li}$_{\textrm{x}}${Na}$_{\textrm{1-x}}$){NbO}$_{\textrm{3}}$ solid solutions: {Evidence} of the rhombohedral phase},
	volume = {69},
	shorttitle = {Synchrotron x-ray diffraction and {Raman} scattering investigations of \$(\{{\textbackslash}mathrm\{{Li}\}\}\_\{x\}\{{\textbackslash}mathrm\{{Na}\}\}\_\{1{\textbackslash}ensuremath\{-\}x\})\{{\textbackslash}mathrm\{{NbO}\}\}\_\{3\}\$ solid solutions},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.69.144105},
	doi = {10.1103/PhysRevB.69.144105},
	abstract = {The (LixNa1−x)NbO3 perovskite solid solutions are investigated using synchrotron x-ray diffraction and Raman spectroscopy in order to clarify the structural changes in the concentration range 0{\textless}{\textasciitilde}x{\textless}{\textasciitilde}0.145 at room temperature. The orthorhombic antiferroelectric P phase (space group Pbma, Z=8) exists up to x=0.02 and in the concentration interval 0.02{\textless}{\textasciitilde}x{\textless}{\textasciitilde}0.03 we have confirmed a previously reported transition to the orthorhombic ferroelectric Q phase (space group P21ma, Z=4). It is found that the Q phase is stable up to x=0.145 but in the narrow concentration interval at x=0.12 the dominating (86.2\%) rhombohedral N phase (space group R3c, Z=2) coexists with the minor (13.8\%) Q phase at room temperature. The crystal structure of this rhombohedral N phase has been refined using Rietveld method. Detailed comparison with similar low-temperature phase of pure NaNbO3 showed that the NbO6 octahedra are slightly distorted in the solid solution with x=0.12 while they are rather regular in NaNbO3. Raman spectra showed drastic changes associated with the P−Q transition and revealed coexistence of the P and Q phases in the interval 0.02{\textless}{\textasciitilde}x{\textless}{\textasciitilde}0.03. Abrupt transformation of the Raman response and remarkable narrowing of the Nb-O stretching vibrations related to the existence of the rhombohedral N phase at x=0.12 were observed.},
	number = {14},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Yuzyuk, Yu. I. and Gagarina, E. and Simon, P. and Reznitchenko, L. A. and Hennet, L. and Thiaudière, D.},
	month = apr,
	year = {2004},
	note = {Publisher: American Physical Society},
	pages = {144105},
	file = {APS Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\BS8JEKPQ\\PhysRevB.69.html:text/html},
}



@article{lorenz_optical_2003,
	series = {Proceedings of the 9th {International} {Workshop} on {Oxide} {Electronics}},
	title = {Optical and electrical properties of epitaxial ({Mg},{Cd})$_{\textrm{x}}${Zn}$_{\textrm{1−x}}${O}, {ZnO}, and {ZnO}:({Ga},{Al}) thin films on c-plane sapphire grown by pulsed laser deposition},
	volume = {47},
	issn = {0038-1101},
	shorttitle = {Optical and electrical properties of epitaxial ({Mg},{Cd}){xZn1}−{xO}, {ZnO}, and {ZnO}},
	url = {https://www.sciencedirect.com/science/article/pii/S0038110103001989},
	doi = {10.1016/S0038-1101(03)00198-9},
	abstract = {A consistent set of epitaxial, n-type conducting ZnO thin films, nominally undoped, doped with Ga or Al, or alloyed with Mg or Cd, was grown by pulsed laser deposition (PLD) on single-crystalline c-plane sapphire (0001) substrates, and characterized by Hall measurement, and UV/VIS optical transmission spectroscopy. The optical band gap of undoped ZnO films at nearly 3.28 eV was shifted by alloying with Mg up to 4.5 eV and by alloying with Cd down to 3.18 eV, dependent on the alloy composition. In addition, highly doped ZnO:Al films show a blue-shifted optical absorption edge due to filling of electronic states in the conduction band. The Hall transport data of the PLD (Mg,Zn,Cd)O:(Ga,Al) thin films span a carrier concentration range of six orders of magnitude from 3×1014 to 3×1020 cm−3, which corresponds to a resistivity from 5×10−4 to 3×103 Ωcm. Structurally optimized, nominally undoped ZnO films grown with ZnO nucleation and top layer reached an electron mobility of 155 cm2/Vs (300 K), which is among the largest values reported for heteroepitaxial ZnO thin films so far. Finally, we succeeded in combining the low resistivity of ZnO:Ga and the band gap shift of MgZnO in MgZnO:Ga thin films. This results demonstrate the unique tunability of the optical and electrical properties of the ZnO-based wide-band gap material for future electronic devices.},
	number = {12},
	urldate = {2023-11-11},
	journal = {Solid-State Electronics},
	author = {Lorenz, M. and Kaidashev, E. M. and von Wenckstern, H. and Riede, V. and Bundesmann, C. and Spemann, D. and Benndorf, G. and Hochmuth, H. and Rahm, A. and Semmelhack, H. -C. and Grundmann, M.},
	month = dec,
	year = {2003},
	keywords = {Electrical properties, Optical properties, Pulsed laser deposition, Thin films, Wide-band gap material, Zinc oxide},
	pages = {2205--2209},
}



@article{misochko_time-resolved_2003,
	title = {A time-resolved optical study of the paramagnetic dielectric-ferromagnetic metal transition in {La}$_{\textrm{0.7}}${Ca}$_{\textrm{0.3}}${MnO}$_{\textrm{3}}$},
	volume = {97},
	issn = {1090-6509},
	url = {https://doi.org/10.1134/1.1625069},
	doi = {10.1134/1.1625069},
	abstract = {The relaxation dynamics of charge carriers in an epitaxial La0.7Ca0.3MnO3 film was studied by the light reflection method with a femtosecond time resolution in a wide temperature range. The relaxation of time-resolved photoinduced reflections was shown to be two-component in the whole temperature range including the paramagnetic dielectric-ferromagnetic metal transition at T ≈ 150–160 K. The fast relaxation component had a maximum lifetime (τ ∼ 500 ps) in the transition region, and its contribution to relaxation increased as temperature decreased. The lifetime of the slow component was minimum (τ ∼ 15 fs) in the transition region. In addition, fast oscillations assigned to coherent phonons appeared in photoinduced responses at T {\textless} 200 K. The dephasing time of these oscillations increased as temperature decreased, whereas their frequency changed insignificantly.},
	language = {en},
	number = {4},
	urldate = {2023-11-11},
	journal = {Journal of Experimental and Theoretical Physics},
	author = {Misochko, 1. O. V. and Kaidashev, E. M. and Georgiev, N. and Dekorsy, T. and Zakharchenko, I. N.},
	month = oct,
	year = {2003},
	keywords = {Charge Carrier, Elementary Particle, Time Resolution, Transition Region, Wide Temperature Range},
	pages = {788--793},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\JRJUDEGD\\Misochko и др. - 2003 - A time-resolved optical study of the paramagnetic .pdf:application/pdf},
}



@article{schmidt_dielectric_2003,
	title = {Dielectric functions (1 to 5 {eV}) of wurtzite {Mg}$_{\textrm{x}}${Zn}$_{\textrm{1−x}}${O} (x⩽0.29) thin films},
	volume = {82},
	issn = {0003-6951},
	url = {https://doi.org/10.1063/1.1565185},
	doi = {10.1063/1.1565185},
	abstract = {The optical dielectric functions for polarization perpendicular and parallel to the c-axis (optical axis) of pulsed-laser-deposition grown wurtzite MgxZn1−xO (0⩽x⩽0.29) thin films have been determined at room temperature using ellipsometry for photon energies from 1 to 5 eV. The dielectric functions reveal strong excitonic contributions for all Mg concentrations x. The band gap energies (E0A=3.369 eV for ZnO to 4.101 eV for x=0.29) show a remarkable blueshift. The exciton binding energy (61 meV for ZnO) decreases to approximately 50 meV for x≈0.17 and increases to approximately 58 meV for x=0.29. In contrast to ZnO, the MgxZn1−xO alloys are found uniaxial negative below the band gap energy, opposite to previously reported results.},
	number = {14},
	urldate = {2023-11-11},
	journal = {Applied Physics Letters},
	author = {Schmidt, R. and Rheinländer, B. and Schubert, M. and Spemann, D. and Butz, T. and Lenzner, J. and Kaidashev, E. M. and Lorenz, M. and Rahm, A. and Semmelhack, H. C. and Grundmann, M.},
	month = apr,
	year = {2003},
	pages = {2260--2262},
}



@article{yuzyuk_stress_2003,
	title = {Stress relaxation in heteroepitaxial ({Ba}, {Sr}){TiO}$_{\textrm{3}}$/(001) {MgO} thin film studied by micro-{Raman} spectroscopy},
	volume = {68},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.68.104104},
	doi = {10.1103/PhysRevB.68.104104},
	abstract = {The evolution of stresses in a heteroepitaxial (Ba0.7Sr0.3)TiO3/(001)MgO thin film was studied by means of micro-Raman spectroscopy. A small part of the substrate was gradually dissolved, then partially unsupported and completely free-standing areas of the film were studied in a side-view backscattering geometry. The E(TO) soft mode was used to estimate local stresses in the thin film. Our experiments revealed stress relaxation and the gradient of the tetragonal distortion in the partially unsupported ferroelectric thin film. The length scale over which the stress relaxes in the heteroepitaxial film was estimated. The thermal strain arising mostly due to the difference between the thermal-expansion coefficients of the film and the substrate governs the domain structure and induces enhanced tetragonality in the film studied. We found that the partially unsupported thin film is polarization graded due to the stress gradient along the film-substrate interface.},
	number = {10},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Yuzyuk, Yu. I. and Katiyar, R. S. and Alyoshin, V. A. and Zakharchenko, I. N. and Markov, D. A. and Sviridov, E. V.},
	month = sep,
	year = {2003},
	note = {Publisher: American Physical Society},
	pages = {104104},
}



@article{yuzyuk_phase_2003,
	title = {Phase transitions in ({Ba}$_{\textrm{0.7}}${Sr}$_{\textrm{0.3}}$){TiO}$_{\textrm{3}}$/(001){MgO} thin film studied by {Raman} scattering},
	volume = {93},
	issn = {0021-8979},
	url = {https://doi.org/10.1063/1.1574173},
	doi = {10.1063/1.1574173},
	abstract = {Polarized Raman spectra of heteroepitaxial (Ba0.7Sr0.3)TiO3 thin film deposited on the (001)MgO substrate have been studied in the broad temperature range from 30 to 1300 K. Our results show that the ferroelectric–paraelectric phase transition is markedly shifted to higher temperatures with respect to the bulk ceramics of the same composition. Because of the two-dimensional compressive stresses imposed on the film by the substrate, the symmetry of the paraelectric phase is found to be tetragonal well above the Curie temperature. Near the deposition temperature (1173 K), the thermoelastic compressive stresses vanish and Raman response suggests nearly cubic symmetry. Raman measurements below room temperature show clearly that the phase transition to the rhombohedral phase is completely suppressed and only one phase transition from the tetragonal to the monoclinic phase is revealed at ∼150 K.},
	number = {12},
	urldate = {2023-11-11},
	journal = {Journal of Applied Physics},
	author = {Yuzyuk, Yu. I. and Sauvajol, J. L. and Simon, P. and Lorman, V. L. and Alyoshin, V. A. and Zakharchenko, I. N. and Sviridov, E. V.},
	month = may,
	year = {2003},
	pages = {9930--9937},
}



@article{yuzyuk_comment_2003,
	title = {Comment on ``{Structural} ordering transition and repulsion of the giant {LO}-{TO} splitting in polycrystalline {Ba}$_{\textrm{x}}${Sr}$_{\textrm{1-x}}${TiO}$_{\textrm{3}}$},
	volume = {68},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.68.216101},
	doi = {10.1103/PhysRevB.68.216101},
	abstract = {Recently, Kuo et al. [S.-Y. Kuo, W.-Y. Liao, and W.-F. Hsieh, Phys. Rev. B 64, 224103 (2001)] reported a new structural ordering in sol-gel derived polycrystalline BaxSr1−xTiO3 around x≈0.4–0.5 at room temperature. We show that unpolarized Raman data obtained in this work were analyzed incorrectly. As a consequence, conclusions derived from Raman-scattering experiments in the above paper are questionable.},
	number = {21},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Yuzyuk, Yu. I. and Simon, P.},
	month = dec,
	year = {2003},
	note = {Publisher: American Physical Society},
	pages = {216101},
}



@article{bundesmann_infrared_2002,
	title = {Infrared dielectric functions and phonon modes of wurtzite {Mg}$_{\textrm{x}}${Zn}$_{\textrm{1−x}}${O} (x⩽0.2)},
	volume = {81},
	issn = {0003-6951},
	url = {https://doi.org/10.1063/1.1509862},
	doi = {10.1063/1.1509862},
	abstract = {Infrared dielectric function spectra and phonon modes with polarization parallel and perpendicular to the c axis of high quality, highly relaxed, and single crystalline wurtzite MgxZn1−xO films with 0⩽x⩽0.2 prepared by pulsed-laser deposition on c-plane sapphire substrates were obtained from infrared spectroscopic ellipsometry (380–1200 cm−1) and Raman scattering studies. A two-mode behavior is found for the modes with E1 symmetry, a lattice mode and an impurity-type mode are obtained for the A1 symmetry phonons. Model dielectric function spectra will become useful for future infrared ellipsometry analysis of complex MgxZn1−xO-based heterostructures.},
	number = {13},
	urldate = {2023-11-11},
	journal = {Applied Physics Letters},
	author = {Bundesmann, C. and Schubert, M. and Spemann, D. and Butz, T. and Lorenz, M. and Kaidashev, E. M. and Grundmann, M. and Ashkenov, N. and Neumann, H. and Wagner, G.},
	month = sep,
	year = {2002},
	pages = {2376--2378},
	file = {Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\MGX7XX67\\Infrared-dielectric-functions-and-phonon-modes-of.html:text/html},
}



@article{yuzyuk_polarization-dependent_2002,
	title = {Polarization-dependent {Raman} spectra of heteroepitaxial ({Ba}, {Sr}){TiO}$_{\textrm{3}}$/(001) {MgO} thin films},
	volume = {65},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.65.134107},
	doi = {10.1103/PhysRevB.65.134107},
	abstract = {We have studied the concentration dependence of the Raman spectra of heteroepitaxial (Ba1−xSrx)TiO3 (BST) (x=0, 0.15, 0.30, and 0.45) thin films deposited by rf sputtering on (001) MgO substrates. It is found that substitution of Ba by Sr leads to the distortions of the Ti-O bonds and causes the appearance of new bands in the Raman spectra near the bands corresponding to the Ti-O vibrations. The Sr incorporation induces relatively large shifts of the low-frequency Raman peaks attributed to ETO and A1TO components of the soft mode. The ETO soft mode in BST films becomes underdamped for x{\textgreater}{\textasciitilde}0.3 and is very sensitive to the two-dimensional compressive stresses.},
	number = {13},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Yuzyuk, Yu. I. and Alyoshin, V. A. and Zakharchenko, I. N. and Sviridov, E. V. and Almeida, A. and Chaves, M. R.},
	month = mar,
	year = {2002},
	note = {Publisher: American Physical Society},
	pages = {134107},
	file = {APS Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\DIUXSDGU\\PhysRevB.65.html:text/html},
}



@article{yuzyuk_stress_2002,
	title = {Stress effect on the ferroelectric-to-paraelectric phase transition in heteroepitaxial ({Ba}, {Sr}){TiO}$_{\textrm{3}}$/(001) {MgO} thin film studied by {Raman} scattering and x-ray diffraction},
	volume = {66},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.66.052103},
	doi = {10.1103/PhysRevB.66.052103},
	abstract = {We report experimental evidence for the stress-induced tetragonal symmetry of the paraelectric phase in heteroepitaxial (Ba0.7Sr0.3)TiO3 thin film deposited on the (001)MgO substrate. Our Raman and x-ray-diffraction data evidently show that symmetry of the paraelectric phase is tetragonal well above the Curie temperature due to the two-dimensional compressive stresses imposed on the film by the substrate. On approaching the deposition temperature the thermoelastic compressive stresses vanish and Raman measurements revealed cubic symmetry of the paraelectric phase.},
	number = {5},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Yuzyuk, Yu. I. and Simon, P. and Zakharchenko, I. N. and Alyoshin, V. A. and Sviridov, E. V.},
	month = aug,
	year = {2002},
	note = {Publisher: American Physical Society},
	pages = {052103},
	file = {APS Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\B9REP2NW\\PhysRevB.66.html:text/html},
}



@article{linnik_crystal_2021,
	title = {Crystal {Structure} and the {Spectral} {Response} of the {Ba}‐{Doped} {SrTiO}$_{\textrm{3}}$ {Incipient} {Ferroelectrics}},
	volume = {258},
	issn = {0370-1972, 1521-3951},
	url = {https://onlinelibrary.wiley.com/doi/10.1002/pssb.202100010},
	doi = {10.1002/pssb.202100010},
	abstract = {The crystal structure and lattice dynamics of quantum paraelectric Ba
                
                  x
                
                Sr
                
                  1−
                  x
                
                TiO
                3
                (
                x
                 = 0, 0.01, 0.02) solid solutions are studied using X‐ray diffraction (XRD), Raman and terahertz‐infrared (THz‐IR) spectroscopies in a temperature range of 4–300 K. XRD and Raman spectroscopy reveal the cubic‐to‐tetragonal nonpolar structural phase transition at about 100 K. At the same time, Raman spectra manifest the presence of polar modes, TO
                2
                and TO
                4
                , normally prohibited in paraelectric phase. Emergence of these modes indicates the appearance of the polar nanoregions in a broad temperature range. The modes become more intensive at low temperatures, and temperature dependence of their intensities on cooling reveals the kink‐like change of the slope from flat to steep, indicating on activation of polar nanoregions. The transmission THz‐IR spectra show that squared frequency of the polar TO
                1
                soft mode, responsible for ferroelectric transition, follows Cochran's behavior at high temperatures. However, at low temperatures, it doesn't vanish at extrapolated Curie temperature but saturates, demonstrating the plateau feature below 20 K. This behavior, coherent with known saturation of the dielectric constant, indicates that transition to ferroelectric phase in Ba
                
                  x
                
                Sr
                
                  1−
                  x
                
                TiO
                3
                is suppressed by quantum fluctuations and the system stays in quantum paraelectric state at very low temperatures.},
	language = {en},
	number = {7},
	urldate = {2023-11-10},
	journal = {physica status solidi (b)},
	author = {Linnik, Ekaterina D. and Lukyanchuk, Igor A. and Mikheykin, Alexey S. and Ragulya, Andrey V. and Gorshunov, Boris P. and Alyabyeva, Liudmila N. and Zhukov, Sergey S. and Mezzane, Daoud and Razumnaya, Anna G.},
	month = jul,
	year = {2021},
	pages = {2100010},
}



@article{lukyanchuk_ferroelectric_2022,
	title = {The ferroelectric field-effect transistor with negative capacitance},
	volume = {8},
	issn = {2057-3960},
	url = {https://www.nature.com/articles/s41524-022-00738-2},
	doi = {10.1038/s41524-022-00738-2},
	abstract = {Abstract
            Integrating ferroelectric negative capacitance (NC) into the field-effect transistor (FET) promises to break fundamental limits of power dissipation known as Boltzmann tyranny. However, realizing the stable static negative capacitance in the non-transient non-hysteretic regime remains a daunting task. The problem stems from the lack of understanding of how the fundamental origin of the NC due to the emergence of the domain state can be put in use for implementing the NC FET. Here we put forth an ingenious design for the ferroelectric domain-based field-effect transistor with the stable reversible static negative capacitance. Using dielectric coating of the ferroelectric capacitor enables the tunability of the negative capacitance improving tremendously the performance of the field-effect transistors.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {npj Computational Materials},
	author = {Luk’yanchuk, I. and Razumnaya, A. and Sené, A. and Tikhonov, Y. and Vinokur, V. M.},
	month = mar,
	year = {2022},
	pages = {52},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\RNZJZAMQ\\Luk’yanchuk и др. - 2022 - The ferroelectric field-effect transistor with neg.pdf:application/pdf;Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\NWIGDCZ5\\Luk’yanchuk и др. - 2022 - The ferroelectric field-effect transistor with neg.pdf:application/pdf},
}



@article{nikolaev_synthesis_2022,
	title = {Synthesis of {ZnO} nanorods for piezoelectric resonators and sensors},
	volume = {12},
	issn = {2010-135X, 2010-1368},
	url = {https://www.worldscientific.com/doi/abs/10.1142/S2010135X21600201},
	doi = {10.1142/S2010135X21600201},
	abstract = {Efficiency of the piezoelectric chemisensors may be considerably enhanced by use of zinc oxide nanorods as sensing elements. ZnO nanorod arrays being good piezoelectric materials possess large surface area, which provides extra benefits for chemisorption and photodetection. Highly oriented nanorod arrays are typically prepared onto highly crystalline substrates, whereas the nanorods growth onto metal contacts meets significant technological difficulties. In this paper, we report on carbothermal, electrochemical, and hydrothermal techniques of ZnO nanorod arrays synthesis on metal contacts. The optical and structural properties of the obtained nanorods were studied using scanning electron microscopy, X-ray diffraction (XRD), Raman spectroscopy, and luminescence spectroscopy. A reliable technique was developed for obtaining ohmic contact with the grown nanorods. I–U curves of prepared contact were studied. Carbothermal synthesis made it possible to obtain the most crystallinely perfect, homogeneous, and dense arrays of nanorods and control the concentration of point defects by changing the synthesis parameters over a wide range. The electrochemical synthesis demonstrated excellent results for synthesis of ZnO nanorods on the surface of resonator electrodes.},
	language = {en},
	number = {01},
	urldate = {2023-11-11},
	journal = {Journal of Advanced Dielectrics},
	author = {Nikolaev, A. L. and Kazmina, M. A. and Lyanguzov, N. V. and Abdulvakhidov, K. G. and Kaidashev, E. M.},
	month = feb,
	year = {2022},
	pages = {2160020},
}



@article{merselmiz_design_2022,
	title = {Design of lead-free {BCZT}-based ceramics with enhanced piezoelectric energy harvesting performances},
	volume = {24},
	issn = {1463-9076, 1463-9084},
	url = {http://xlink.rsc.org/?DOI=D1CP04723J},
	doi = {10.1039/D1CP04723J},
	abstract = {The benefits of the multiphase convergence strategy to design ferroelectric ceramics for piezoelectric energy harvesting applications over a broad temperature range.
          , 
            
              The design of lead-free ceramics for piezoelectric energy harvesting applications has become a hot topic. Among these materials, Ba
              0.85
              Ca
              0.15
              Zr
              0.10
              Ti
              0.90
              O
              3
              (BCZT) and BaTi
              0.89
              Sn
              0.11
              O
              3
              (BTSn) are considered as potential candidates due to their enhanced piezoelectric properties. Here, the structural, electrical, piezoelectric and piezoelectric energy harvesting properties of the (1 −
              x
              )Ba
              0.85
              Ca
              0.15
              Zr
              0.10
              Ti
              0.90
              O
              3
              −
              x
              BaTi
              0.89
              Sn
              0.11
              O
              3
              (
              x
              BTSn,
              x
              = 0.2, 0.4 and 0.6) system are investigated. A systematic study of the structural properties of the
              x
              BTSn samples was carried out using X-ray diffraction, Raman spectroscopy, and dielectric measurements. The addition of BTSn allows a successive phase transition, which broadens the application temperature range. The enhanced piezoelectric energy harvesting properties were found in the 0.2BTSn ceramic, where the large-signal and small-signal piezoelectric coefficients, piezoelectric voltage and the piezoelectric figure of merit reached 245 pm V
              −1
              , 228 pC N
              −1
              , 16.2 mV m N
              −1
              and 3.7 pm
              2
              N
              −1
              , respectively. Consequently, the combination of BCZT and BTSn could provide suitable lead-free materials with enhanced piezoelectric energy harvesting performances.},
	language = {en},
	number = {10},
	urldate = {2023-11-11},
	journal = {Physical Chemistry Chemical Physics},
	author = {Merselmiz, Soukaina and Hanani, Zouhair and Prah, Uroš and Mezzane, Daoud and Hajji, Lahoucine and Abkhar, Zahra and Spreitzer, Matjaž and Vengust, Damjan and Uršič, Hana and Fabijan, David and Razumnaya, Anna G. and Shapovalova, Olesia and Luk'yanchuk, Igor A. and Kutnjak, Zdravko},
	year = {2022},
	pages = {6026--6036},
}



@article{kuriganova_graphene_2022,
	title = {Graphene structures prepared via pulse alternating current technique},
	volume = {32},
	issn = {09599436},
	url = {https://linkinghub.elsevier.com/retrieve/pii/S0959943622001249},
	doi = {10.1016/j.mencom.2022.05.005},
	language = {en},
	number = {3},
	urldate = {2023-11-11},
	journal = {Mendeleev Communications},
	author = {Kuriganova, Alexandra B. and Leontyev, Igor N. and Avramenko, Marina V. and Faddeev, Nikita A. and Smirnova, Nina V.},
	month = may,
	year = {2022},
	pages = {308--310},
}



@article{shirokov_ferromagnetoelectric_2021,
	title = {Ferromagnetoelectric phases of hexaferrites: a group-theoretical analysis},
	volume = {77},
	issn = {2052-5206},
	shorttitle = {Ferromagnetoelectric phases of hexaferrites},
	url = {https://scripts.iucr.org/cgi-bin/paper?S2052520621007125},
	doi = {10.1107/S2052520621007125},
	abstract = {A symmetry-guided approach for designing and tailoring magnetoelectric and multiferroic hexaferrites is proposed. A group-theoretical study of the magnetoferroelectric structures of a hexagonal ferrite was carried out. The results were applied to M-, W- and Z-type hexaferrites. It is shown that the magnetic structure cannot be collinear in the main magnetic phase, with the direction of the magnetic moment along the hexagonal axis. Magnetic sublattices are shown in which cation substitution should lead to the formation of a multiferroic state. A thermodynamic model of a hexagonal ferroelectric ferrimagnet was constructed, in which isostructural phase transitions were observed.},
	number = {5},
	urldate = {2023-11-10},
	journal = {Acta Crystallographica Section B Structural Science, Crystal Engineering and Materials},
	author = {Shirokov, Vladimir Borisovich and Razumnaya, Anna Grigoryevna and Mikheykin, Alexey Sergeevich},
	month = oct,
	year = {2021},
	pages = {740--748},
}



@article{chalin_modeling_2021,
	title = {Modeling and live imaging of mechanical instabilities in the zebrafish aorta during hematopoiesis},
	volume = {11},
	issn = {2045-2322},
	url = {https://www.nature.com/articles/s41598-021-88667-w},
	doi = {10.1038/s41598-021-88667-w},
	abstract = {Abstract
            All blood cells originate from hematopoietic stem/progenitor cells (HSPCs). HSPCs are formed from endothelial cells (ECs) of the dorsal aorta (DA), via endothelial-to-hematopoietic transition (EHT). The zebrafish is a primary model organism to study the process in vivo. While the role of mechanical stress in controlling gene expression promoting cell differentiation is actively investigated, mechanisms driving shape changes of the DA and individual ECs remain poorly understood. We address this problem by developing a new DA micromechanical model and applying it to experimental data on zebrafish morphogenesis. The model considers the DA as an isotropic tubular membrane subjected to hydrostatic blood pressure and axial stress. The DA evolution is described as a movement in the dimensionless controlling parameters space: normalized hydrostatic pressure and axial stress. We argue that HSPC production is accompanied by two mechanical instabilities arising in the system due to the plane stress in the DA walls and show how a complex interplay between mechanical forces in the system drives the emerging morphological changes.},
	language = {en},
	number = {1},
	urldate = {2023-11-10},
	journal = {Scientific Reports},
	author = {Chalin, Dmitrii and Bureau, Charlotte and Parmeggiani, Andrea and Rochal, Sergei and Kissa, Karima and Golushko, Ivan},
	month = apr,
	year = {2021},
	pages = {9316},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\PXM8A3B8\\Chalin и др. - 2021 - Modeling and live imaging of mechanical instabilit.pdf:application/pdf},
}



@article{moysa_influence_2021,
	title = {The influence of the internal structure on the polarization properties of the solid solutions of the three-component system of the sodium – potassium – cadmium niobates},
	volume = {575},
	issn = {0015-0193, 1563-5112},
	url = {https://www.tandfonline.com/doi/full/10.1080/00150193.2021.1888228},
	doi = {10.1080/00150193.2021.1888228},
	language = {en},
	number = {1},
	urldate = {2023-11-10},
	journal = {Ferroelectrics},
	author = {Moysa, M. O. and Nagaenko, A. V. and Shilkina, L. A. and Andryushin, K. P. and Andryushina, I. N. and Reznichenko, L. A. and Rudskiy, D. I. and Rudskaya, A. G.},
	month = apr,
	year = {2021},
	pages = {64--74},
}



@article{vakhrushev_electric_2021,
	title = {Electric field control of antiferroelectric domain pattern},
	volume = {103},
	issn = {2469-9950, 2469-9969},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.103.214108},
	doi = {10.1103/PhysRevB.103.214108},
	language = {en},
	number = {21},
	urldate = {2023-11-10},
	journal = {Physical Review B},
	author = {Vakhrushev, S. B. and Andronikova, D. and Bronwald, Iu. and Koroleva, E. Yu. and Chernyshov, D. and Filimonov, A. V. and Udovenko, S. A. and Rudskoy, A. I. and Ishikawa, D. and Baron, A. Q. R. and Bosak, A. and Leontiev, I. N. and Tagantsev, Alexander K.},
	month = jun,
	year = {2021},
	pages = {214108},
}



@article{lukyanchuk_dynamics_2021,
	title = {Dynamics of polarization vortices revealed in a ferroelectric material},
	volume = {592},
	issn = {0028-0836, 1476-4687},
	url = {https://www.nature.com/articles/d41586-021-00887-2},
	doi = {10.1038/d41586-021-00887-2},
	language = {en},
	number = {7854},
	urldate = {2023-11-10},
	journal = {Nature},
	author = {Luk’yanchuk, Igor and Vinokur, Valerii M.},
	month = apr,
	year = {2021},
	pages = {359--360},
}



@article{kondovych_tip-induced_2021,
	title = {Tip-induced domain protrusion in ferroelectric films with in-plane polarization},
	volume = {129},
	issn = {0021-8979, 1089-7550},
	url = {https://pubs.aip.org/jap/article/129/5/054103/1080347/Tip-induced-domain-protrusion-in-ferroelectric},
	doi = {10.1063/5.0035950},
	abstract = {Charge manipulation and fabrication of stable domain patterns in ferroelectric materials by scanning probe microscopy open up broad avenues for the development of tunable electronics. Harnessing the polarization energy and electrostatic forces with specific geometry of the system enables producing the nanoscale domains by-design. Along with that, domain engineering requires mastery of underlying physical mechanisms that govern the domain formation. Here, we present a theoretical description of the domain formation by a scanning probe microscopy tip in a ferroelectric film with strong in-plane anisotropy of polarization. We demonstrate that local charge injection produces wedge-shaped domains that propagate along the anisotropy axis, whereas the tip-written lines of charge generate a comb-like domain structure. The results of our calculations agree with earlier experimental observations and allow for the optimization of the targeted domain structures.},
	language = {en},
	number = {5},
	urldate = {2023-11-10},
	journal = {Journal of Applied Physics},
	author = {Kondovych, S. and Gruverman, A. and Luk’yanchuk, I.},
	month = feb,
	year = {2021},
	pages = {054103},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\2AIGWX9B\\Kondovych и др. - 2021 - Tip-induced domain protrusion in ferroelectric fil.pdf:application/pdf},
}



@article{andryushin_reasons_2021,
	title = {Reasons for the {High} {Electrical} {Conductivity} of {Bismuth} {Ferrite} and {Ways} to {Minimize} {It}},
	volume = {11},
	issn = {2076-3417},
	url = {https://www.mdpi.com/2076-3417/11/3/1025},
	doi = {10.3390/app11031025},
	abstract = {The reasons for the high electrical conductivity of bismuth ferrite due to its natural composite structure, structural non-stoichiometry, redox processes, and the boundary position in the perovskite family have been considered. It has been shown that it is possible to significantly (2–3 orders of magnitude) reduce the conductivity of BiFeO3 by introducing large-sized ions of rare-earth elements (REE: La, Pr, Nd, Sm, Eu, Gd with 0.94 ≤ R¯ ≤ 1.04 Å) in amounts of up to 10 mol \%. An interpretation of the observed effects has been given. A consideration about the appropriateness of taking into account the presented results when developing devices using materials of the BiFeO3/REE type has been expressed.},
	language = {en},
	number = {3},
	urldate = {2023-11-10},
	journal = {Applied Sciences},
	author = {Andryushin, Konstantin and Sakhnenko, Vladimir and Turik, Anatoliy and Shilkina, Lidiya and Pavelko, Alexey and Dudkina, Svetlana and Rudskaya, Angela and Rudskiy, Daniil and Verbenko, Iliya and Hasbulatov, Sidek and Reznichenko, Larisa and Parinov, Ivan and Chang, Shun-Hsyung and Wang, Hung-Yu},
	month = jan,
	year = {2021},
	pages = {1025},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\6GVK6IPC\\Andryushin и др. - 2021 - Reasons for the High Electrical Conductivity of Bi.pdf:application/pdf},
}



@article{chernysheva_non-isothermal_2021,
	title = {Non-{Isothermal} {Decomposition} as {Efficient} and {Simple} {Synthesis} {Method} of {NiO}/{C} {Nanoparticles} for {Asymmetric} {Supercapacitors}},
	volume = {11},
	issn = {2079-4991},
	url = {https://www.mdpi.com/2079-4991/11/1/187},
	doi = {10.3390/nano11010187},
	abstract = {A series of NiO/C nanocomposites with NiO concentrations ranging from 10 to 90 wt\% was synthesized using a simple and efficient two-step method based on non-isothermal decomposition of Nickel(II) bis(acetylacetonate). X-ray diffraction (XRD) measurements of these NiO/C nanocomposites demonstrate the presence of β-NiO. NiO/C nanocomposites are composed of spherical particles distributed over the carbon support surface. The average diameter of nickel oxide spheres increases with the NiO content and are estimated as 36, 50 and 205 nm for nanocomposites with 10, 50 and 80 wt\% NiO concentrations, respectively. In turn, each NiO sphere contains several nickel oxide nanoparticles, whose average sizes are 7–8 nm. According to the tests performed using a three-electrode cell, specific capacitance (SC) of NiO/C nanocomposites increases from 200 to 400 F/g as the NiO content achieves a maximum of 60 wt\% concentration, after which the SC decreases. The study of the NiO/C composite showing the highest SC in three- and two-electrode cells reveals that its SC remains almost unchanged while increasing the current density, and the sample demonstrates excellent cycling stability properties. Finally, NiO/C (60\% NiO) composites are shown to be promising materials for charging quartz clocks with a power rating of 1.5 V (30 min).},
	language = {en},
	number = {1},
	urldate = {2023-11-10},
	journal = {Nanomaterials},
	author = {Chernysheva, Daria and Pudova, Ludmila and Popov, Yuri and Smirnova, Nina and Maslova, Olga and Allix, Mathieu and Rakhmatullin, Aydar and Leontyev, Nikolay and Nikolaev, Andrey and Leontyev, Igor},
	month = jan,
	year = {2021},
	pages = {187},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\A9ZZXP6R\\Chernysheva и др. - 2021 - Non-Isothermal Decomposition as Efficient and Simp.pdf:application/pdf},
}



@article{nikolaev_pulsed_2021,
	title = {Pulsed laser deposition of {Au} nanoparticles on {ZnO} nanostructures},
	volume = {1029},
	issn = {1757-8981, 1757-899X},
	url = {https://iopscience.iop.org/article/10.1088/1757-899X/1029/1/012064},
	doi = {10.1088/1757-899X/1029/1/012064},
	abstract = {Abstract
            Au nanoparticles and ultrathin gold films were obtained on the surface of thin (100 nm) ZnO films on Si (001) by pulsed laser deposition (PLD) at high argon pressure by sputtering a pure gold target with a CL3100 pulsed excimer laser (λ = 248 nm) at room temperature. The dependence of the size and distribution of nanoparticles on the argon pressure in the vacuum chamber (PAr), the power density of laser radiation (j), and the number of laser pulses (N) was investigated. Also, to obtain nanostructures, axial and non-axial deposition was used, where the substrate was located perpendicular and parallel to the plasma torch, respectively. Stable modes of obtaining gold nanoparticles with high uniformity and average size from 4 to 10 nm were demonstrated. The modes of stable and reproducible deposition of ultrathin Au films (23-42 nm) and percolation structures (18-20 nm) were also demonstrated. Thus, PLD is a reliable and flexible tool for obtaining nanoparticles and ultrathin Au films the average size and thickness of which can be predictably controlled by varying the deposition parameters. This technique is well suited for coating with gold nanoparticles the surface of nanostructured materials based on chemically active substances that are particularly sensitive to surface cleanliness, which cannot be coated by standard methods.},
	number = {1},
	urldate = {2023-11-10},
	journal = {IOP Conference Series: Materials Science and Engineering},
	author = {Nikolaev, A L and Kamencev, A S and Lyanguzov, N V and Aizikovich, S M},
	month = jan,
	year = {2021},
	pages = {012064},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\N97WGD4I\\Nikolaev и др. - 2021 - Pulsed laser deposition of Au nanoparticles on ZnO.pdf:application/pdf},
}



@article{alyabyeva_lead-substituted_2021,
	title = {Lead-substituted barium hexaferrite for tunable terahertz optoelectronics},
	volume = {13},
	issn = {1884-4049, 1884-4057},
	url = {https://www.nature.com/articles/s41427-021-00331-x},
	doi = {10.1038/s41427-021-00331-x},
	abstract = {Abstract
            
              Due to their outstanding dielectric and magnetic properties, hexaferrites are attracting ever-increasing attention for developing electronic components of next-generation communication systems. The complex crystal structure of hexaferrites and the critical dependences of their electric and magnetic properties on external factors, such as magnetic/electric fields, pressure, and doping, open ample opportunities for targeted tuning of these properties when designing specific devices. Here we explored the electromagnetic properties of lead-substituted barium hexaferrite, Ba
              
                1−
                x
              
              Pb
              
                x
              
              Fe
              12
              O
              19
              , a compound featuring an extremely rich set of physical phenomena that are inherent in the dielectric and magnetic subsystems and can have a significant effect on its electromagnetic response at terahertz frequencies. We performed the first detailed measurements of the temperature-dependent (5–300 K) dielectric response of single-crystalline Ba
              
                1−
                x
              
              Pb
              
                x
              
              Fe
              12
              O
              19
              in an extremely broad spectral range of 1 Hz–240 THz. We fully analyzed numerous phenomena with a corresponding wide distribution of specific energies that can affect the terahertz properties of the material. The most important fundamental finding is the observation of a ferroelectric-like terahertz excitation with an unusual temperature behavior of its frequency and strength. We suggest microscopic models that explain the origin of the excitation and its nonstandard temperature evolution. Several narrower terahertz excitations are associated with electronic transitions between the fine-structure components of the Fe
              2+
              ground state. The discovered radio-frequency relaxations are attributed to the response of magnetic domains. Gigahertz resonances are presumably of magnetoelectric origin. The obtained data on diverse electromagnetic properties of Ba
              
                1−
                x
              
              Pb
              
                x
              
              Fe
              12
              O
              19
              compounds provide information that makes the entire class of hexaferrites attractive for manufacturing electronic devices for the terahertz range.},
	language = {en},
	number = {1},
	urldate = {2023-11-10},
	journal = {NPG Asia Materials},
	author = {Alyabyeva, L. N. and Prokhorov, A. S. and Vinnik, D. A. and Anzin, V. B. and Ahmed, A. G. and Mikheykin, A. and Bednyakov, P. and Kadlec, C. and Kadlec, F. and De Prado, E. and Prokleška, J. and Proschek, P. and Kamba, S. and Pronin, A. V. and Dressel, M. and Abalmasov, V. A. and Dremov, V. V. and Schmid, S. and Savinov, M. and Lunkenheimer, P. and Gorshunov, B. P.},
	month = dec,
	year = {2021},
	pages = {63},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\3G3UAQ2R\\Alyabyeva и др. - 2021 - Lead-substituted barium hexaferrite for tunable te.pdf:application/pdf},
}



@article{chernysheva_one_2021,
	title = {One step simultaneous electrochemical synthesis of {NiO}/multilayer graphene nanocomposite as an electrode material for high performance supercapacitors},
	volume = {31},
	issn = {09599436},
	url = {https://linkinghub.elsevier.com/retrieve/pii/S0959943621000596},
	doi = {10.1016/j.mencom.2021.03.005},
	language = {en},
	number = {2},
	urldate = {2023-11-10},
	journal = {Mendeleev Communications},
	author = {Chernysheva, Daria V. and Leontyev, Igor N. and Avramenko, Marina V. and Lyanguzov, Nikolay V. and Grebenyuk, Tatyana I. and Smirnova, Nina V.},
	month = mar,
	year = {2021},
	pages = {160--162},
}



@article{nagaenko_influence_2021,
	title = {The influence of thermodynamic background on the phase picture, macroresponses and the effects of the temporary aging of lead titanium doped with alkaline earth metal oxides},
	volume = {47},
	issn = {02728842},
	url = {https://linkinghub.elsevier.com/retrieve/pii/S0272884220331928},
	doi = {10.1016/j.ceramint.2020.10.149},
	language = {en},
	number = {4},
	urldate = {2023-11-10},
	journal = {Ceramics International},
	author = {Nagaenko, A.V. and Andryushina, I.N. and Andryushin, K.P. and Shilkina, L.A. and Rudskaya, A.G. and Reznichenko, L.A.},
	month = feb,
	year = {2021},
	pages = {5639--5647},
}



@article{merselmiz_thermal-stability_2021,
	title = {Thermal-stability of the enhanced piezoelectric, energy storage and electrocaloric properties of a lead-free {BCZT} ceramic},
	volume = {11},
	issn = {2046-2069},
	url = {http://xlink.rsc.org/?DOI=D0RA09707A},
	doi = {10.1039/D0RA09707A},
	abstract = {High-thermal stability of the recovered energy density and significant electrocaloric temperature change over a broad temperature span in a lead-free BCZT ceramic.
          , 
            
              The lead-free Ba
              0.85
              Ca
              0.15
              Zr
              0.10
              Ti
              0.90
              O
              3
              (BCZT) relaxor ferroelectric ceramic has aroused much attention due to its enhanced piezoelectric, energy storage and electrocaloric properties. In this study, the BCZT ceramic was elaborated by the solid-state reaction route, and the temperature-dependence of the structural, electrical, piezoelectric, energy storage and electrocaloric properties was investigated. X-ray diffraction analysis revealed a pure perovskite phase, and the temperature-dependence of Raman spectroscopy, dielectric and ferroelectric measurements revealed the phase transitions in the BCZT ceramic. At room temperature, the strain and the large-signal piezoelectric coefficient
              
              reached a maximum of 0.062\% and 234 pm V
              −1
              , respectively. Furthermore, enhanced recovered energy density (
              W
              rec
              = 62 mJ cm
              −3
              ) and high-energy storage efficiency (
              η
              ) of 72.9\% at 130 °C were found. The BCZT ceramic demonstrated excellent thermal stability of the energy storage variation (ESV), less than ±5.5\% in the temperature range of 30–100 °C compared to other lead-free ceramics. The electrocaloric response in the BCZT ceramic was explored
              via
              the indirect approach by using the Maxwell relation. Significant electrocaloric temperature change (Δ
              T
              ) of 0.57 K over a broad temperature span (
              T
              span
              = 70 °C) and enhanced coefficient of performance (COP = 11) were obtained under 25 kV cm
              −1
              . The obtained results make the BCZT ceramic a suitable eco-friendly material for energy storage and solid-state electrocaloric cooling devices.},
	language = {en},
	number = {16},
	urldate = {2023-11-10},
	journal = {RSC Advances},
	author = {Merselmiz, Soukaina and Hanani, Zouhair and Mezzane, Daoud and Razumnaya, Anna G. and Amjoud, M'barek and Hajji, Lahoucine and Terenchuk, Svitlana and Rožič, Brigita and Luk'yanchuk, Igor A. and Kutnjak, Zdravko},
	year = {2021},
	pages = {9459--9468},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\AUJR9SKH\\Merselmiz и др. - 2021 - Thermal-stability of the enhanced piezoelectric, e.pdf:application/pdf},
}



@article{mikheykin_twin-boundary_2021,
	title = {Twin-boundary engineering and thickness effect on strontium-barium niobate thin films on {MgO} substrate},
	volume = {888},
	issn = {09258388},
	url = {https://linkinghub.elsevier.com/retrieve/pii/S0925838821029984},
	doi = {10.1016/j.jallcom.2021.161589},
	language = {en},
	urldate = {2023-11-10},
	journal = {Journal of Alloys and Compounds},
	author = {Mikheykin, A.S. and Shirokov, V.B. and Marssi, M. El and Mezzane, D. and Lyanguzov, N.V. and Pavlenko, A.V. and Stryukov, D.V. and Razumnaya, A.G.},
	month = dec,
	year = {2021},
	pages = {161589},
}



@article{ulyankina_photocatalytic_2021,
	title = {Photocatalytic degradation of ciprofloxacin in water at nano-{ZnO} prepared by pulse alternating current electrochemical synthesis},
	volume = {40},
	issn = {22147144},
	url = {https://linkinghub.elsevier.com/retrieve/pii/S2214714420306863},
	doi = {10.1016/j.jwpe.2020.101809},
	language = {en},
	urldate = {2023-11-10},
	journal = {Journal of Water Process Engineering},
	author = {Ulyankina, Anna and Molodtsova, Tatiana and Gorshenkov, Mikhail and Leontyev, Igor and Zhigunov, Denis and Konstantinova, Elizaveta and Lastovina, Tatiana and Tolasz, Jakub and Henych, Jiří and Licciardello, Nadia and Cuniberti, Gianaurelio and Smirnova, Nina},
	month = apr,
	year = {2021},
	pages = {101809},
}



@article{ahlskog_individual_2020,
	title = {Individual arc-discharge synthesized multiwalled carbon nanotubes probed with multiple measurement techniques},
	volume = {38},
	issn = {2166-2746, 2166-2754},
	url = {https://pubs.aip.org/jvb/article/38/4/042804/592550/Individual-arc-discharge-synthesized-multiwalled},
	doi = {10.1116/6.0000187},
	abstract = {Arc-discharge synthesized multiwalled carbon nanotubes (AD-MWNT), or related MWNTs, exhibit a good quality compared to the more common type of MWNT synthesized by catalytic chemical vapor deposition methods. Yet experimental measurements on these are rather few and typically have not correlated data from different measurement techniques. Here, the authors report Raman spectroscopy, scanning probe microscopy, conductivity measurements, and force microscopy on single AD-MWNTs. The results demonstrate the high quality of AD-MWNTs and are compatible with the view of them as the best approximation of MWNTs as an assembly of defect-free concentric individual single-walled carbon nanotubes. The authors also demonstrate conductance measurements over a step on the surface of an AD-MWNT, which is due to an abruptly broken outer layer(s), whereby the interlayer resistance is measured.},
	language = {en},
	number = {4},
	urldate = {2023-11-11},
	journal = {Journal of Vacuum Science \& Technology B, Nanotechnology and Microelectronics: Materials, Processing, Measurement, and Phenomena},
	author = {Ahlskog, Markus and Hokkanen, Matti J. and Levshov, Dmitry and Svensson, Krister and Volodin, Alexander and Van Haesendonck, Chris},
	month = jul,
	year = {2020},
	pages = {042804},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\76DFFX6C\\Ahlskog и др. - 2020 - Individual arc-discharge synthesized multiwalled c.pdf:application/pdf},
}



@article{chalin_band_2020,
	title = {Band structure and inter-tube optical transitions in double-walled carbon nanotubes},
	volume = {102},
	issn = {2469-9950, 2469-9969},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.102.115426},
	doi = {10.1103/PhysRevB.102.115426},
	language = {en},
	number = {11},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Chalin, D. V. and Rochal, S. B.},
	month = sep,
	year = {2020},
	pages = {115426},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\2XJKU38W\\Chalin и Rochal - 2020 - Band structure and inter-tube optical transitions .pdf:application/pdf},
}



@article{sadyrin_characterization_2020,
	title = {Characterization of {Enamel} and {Dentine} about a {White} {Spot} {Lesion}: {Mechanical} {Properties}, {Mineral} {Density}, {Microstructure} and {Molecular} {Composition}},
	volume = {10},
	issn = {2079-4991},
	shorttitle = {Characterization of {Enamel} and {Dentine} about a {White} {Spot} {Lesion}},
	url = {https://www.mdpi.com/2079-4991/10/9/1889},
	doi = {10.3390/nano10091889},
	abstract = {The study focuses on in vitro tracing of some fundamental changes that emerge in teeth at the initial stage of caries development using multiple approaches. The research was conducted on a mostly sound maxillary molar tooth but with a clearly visible natural proximal white spot lesion (WSL). Values of mineral density, reduced Young’s modulus, indentation hardness and creep as well as the molecular composition and surface microstructure of the WSL and bordering dentine area were studied. The results obtained were compared to those of sound enamel and dentine on the same tooth. A decrease of mechanical properties and mineral density both for the WSL and bordering dentine was detected in comparison to the sound counterparts, as well as increase of creep for the enamel WSL. Differences in molecular composition and surface microstructure (including the indenter impressions) were found and described. WSL induces a serious change in the state of not only the visually affected enamel but also surrounding visually intact enamel and dentine in its vicinity. The results provide the basis for future studies of efficacy of minimal invasive treatments of caries.},
	language = {en},
	number = {9},
	urldate = {2023-11-11},
	journal = {Nanomaterials},
	author = {Sadyrin, Evgeniy and Swain, Michael and Mitrin, Boris and Rzhepakovsky, Igor and Nikolaev, Andrey and Irkha, Vladimir and Yogina, Diana and Lyanguzov, Nikolay and Maksyukov, Stanislav and Aizikovich, Sergei},
	month = sep,
	year = {2020},
	pages = {1889},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\95JZJ5NP\\Sadyrin и др. - 2020 - Characterization of Enamel and Dentine about a Whi.pdf:application/pdf},
}



@article{kuriganova_comparison_2020,
	title = {A {Comparison} of “{Bottom}-{Up}” and “{Top}-{Down}” {Approaches} to the {Synthesis} of {Pt}/{C} {Electrocatalysts}},
	volume = {8},
	issn = {2227-9717},
	url = {https://www.mdpi.com/2227-9717/8/8/947},
	doi = {10.3390/pr8080947},
	abstract = {Three 40 wt \% Pt/C electrocatalysts prepared using two different approaches—the polyol process and electrochemical dispersion of platinum under pulse alternating current—and a commercial Pt/C catalyst (Johnson Matthey prod.) were examined via X-ray diffraction (XRD) and transmission electron microscopy (TEM). The stability characteristics of the Pt/C catalysts were studied via long-term cycling, revealing that, for all cycling modes, the best stability was achieved for the Pt/C catalyst with the largest platinum nanoparticle sizes, which was synthesized via electrochemical dispersion of platinum under pulse alternating current. Our results show that the mass and specific electrocatalytic activities of Pt/C catalysts toward ethanol electrooxidation are determined by the value of the electrochemically active Pt surface area in the catalysts.},
	language = {en},
	number = {8},
	urldate = {2023-11-11},
	journal = {Processes},
	author = {Kuriganova, Alexandra and Faddeev, Nikita and Gorshenkov, Mikhail and Kuznetsov, Dmitri and Leontyev, Igor and Smirnova, Nina},
	month = aug,
	year = {2020},
	pages = {947},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\86DZKUPG\\Kuriganova и др. - 2020 - A Comparison of “Bottom-Up” and “Top-Down” Approac.pdf:application/pdf},
}



@article{kuriganova_pac_2020,
	title = {{PAC} {Synthesis} and {Comparison} of {Catalysts} for {Direct} {Ethanol} {Fuel} {Cells}},
	volume = {8},
	issn = {2227-9717},
	url = {https://www.mdpi.com/2227-9717/8/6/712},
	doi = {10.3390/pr8060712},
	abstract = {Pt/C, PtMOn/C (M = Ni, Sn, Ti, and PtX/C (X = Rh, Ir) catalyst systems were prepared by using the pulse alternating current (PAC) technique. Physical and electrochemical parameters of samples were carried out by x-ray powder diffraction (XRD), transmission electron microscopy (TEM), and CO stripping. The catalytic activity of the synthesized samples for the ethanol electrooxidation reaction (EOR) was investigated. The XRD patterns of the samples showed the presence of diffraction peaks characteristic for Pt, NiO, SnO2, TiO2, Rh, and Ir. The TEM images indicate that the Pt, Rh, and PtIr (alloys) particles had a uniform distribution over the carbon surface in the Pt/C, PtRh/C, PtIr/C, and PtMOn/C (M = Ni, Sn, Ti) catalysts. The electrochemically active surface area of catalysts was determined by the CO-stripping method. The addition of a second element to Pt or the use of hybrid supported catalysts can evidently improve the EOR activity. A remarkable positive affecting shift of the onset potential for the EOR was observed as follows: PtSnO2/C {\textgreater} PtTiO2/C ≈ PtIr/C ≈ PtNiO/C {\textgreater} PtRh/C ≈ Pt/C. The addition of SnO2 to Pt/C catalyst led to the decrease of the onset potential and to significantly facilitate the EOR. The long-term cyclic stability of the synthesized catalysts was investigated. Thereby, the PtSnO2/C catalyst prepared by the PAC technique can be considered as a promising anode catalyst for direct ethanol fuel cells.},
	language = {en},
	number = {6},
	urldate = {2023-11-11},
	journal = {Processes},
	author = {Kuriganova, Alexandra and Chernysheva, Daria and Faddeev, Nikita and Leontyev, Igor and Smirnova, Nina and Dobrovolskii, Yury},
	month = jun,
	year = {2020},
	pages = {712},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\JUTMKRJV\\Kuriganova и др. - 2020 - PAC Synthesis and Comparison of Catalysts for Dire.pdf:application/pdf},
}



@article{roshal_crystal-like_2020,
	title = {Crystal-like order and defects in metazoan epithelia with spherical geometry},
	volume = {10},
	issn = {2045-2322},
	url = {https://www.nature.com/articles/s41598-020-64598-w},
	doi = {10.1038/s41598-020-64598-w},
	abstract = {Abstract
            Since Robert Hooke studied cork cell patterns in 1665, scientists have been puzzled by why cells form such ordered structures. The laws underlying this type of organization are universal, and we study them comparing the living and non-living two-dimensional systems self-organizing at the spherical surface. Such-type physical systems often possess trigonal order with specific elongated defects, scars and pleats, where the 5-valence and 7-valence vertices alternate. In spite of the fact that the same physical and topological rules are involved in the structural organization of biological systems, such topological defects were never reported in epithelia. We have discovered them in the follicular spherical epithelium of ascidians that are emerging models in developmental biology. Surprisingly, the considered defects appear in the epithelium even when the number of cells in it is significantly less than the previously known threshold value. We explain this result by differences in the cell sizes and check our hypothesis considering the self-assembly of different random size particles on the spherical surface. Scars, pleats and other complex defects found in ascidian samples can play an unexpected and decisive role in the permanent renewal and reorganization of epithelia, which forms or lines many tissues and organs in metazoans.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Scientific Reports},
	author = {Roshal, Daria S. and Azzag, Karim and Le Goff, Emilie and Rochal, Sergei B. and Baghdiguian, Stephen},
	month = may,
	year = {2020},
	pages = {7652},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\JI45G85W\\Roshal и др. - 2020 - Crystal-like order and defects in metazoan epithel.pdf:application/pdf;Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\J7BDDRP3\\Roshal и др. - 2020 - Crystal-like order and defects in metazoan epithel.pdf:application/pdf},
}



@inproceedings{kaydashev_surface_2020,
	address = {Saratov, Russian Federation},
	title = {Surface acoustic waves based method to study photothermal response of plasmonic nano-objects and metasurfaces},
	isbn = {978-1-5106-3718-4 978-1-5106-3719-1},
	url = {https://www.spiedigitallibrary.org/conference-proceedings-of-spie/11457/2559972/Surface-acoustic-waves-based-method-to-study-photothermal-response-of/10.1117/12.2559972.full},
	doi = {10.1117/12.2559972},
	urldate = {2023-11-11},
	booktitle = {Saratov {Fall} {Meeting} 2019: {Optical} and {Nano}-{Technologies} for {Biology} and {Medicine}},
	publisher = {SPIE},
	author = {Kaydashev, Vladimir E. and Timoshenko, Pavel and Kutepov, Maxim and Karapetyan, Gevork and Kirtaev, Roman and Kaidashev, Evgeni},
	editor = {Tuchin, Valery V. and Genina, Elina A.},
	month = apr,
	year = {2020},
	pages = {13},
}



@article{tikhonov_controllable_2020,
	title = {Controllable skyrmion chirality in ferroelectrics},
	volume = {10},
	issn = {2045-2322},
	url = {https://www.nature.com/articles/s41598-020-65291-8},
	doi = {10.1038/s41598-020-65291-8},
	abstract = {Abstract
            Chirality, an intrinsic handedness, is one of the most intriguing fundamental phenomena in nature. Materials composed of chiral molecules find broad applications in areas ranging from nonlinear optics and spintronics to biology and pharmaceuticals. However, chirality is usually an invariable inherent property of a given material that cannot be easily changed at will. Here, we demonstrate that ferroelectric nanodots support skyrmions the chirality of which can be controlled and switched. We devise protocols for realizing control and efficient manipulations of the different types of skyrmions. Our findings open the route for controlled chirality with potential applications in ferroelectric-based information technologies.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Scientific Reports},
	author = {Tikhonov, Yu. and Kondovych, S. and Mangeri, J. and Pavlenko, M. and Baudry, L. and Sené, A. and Galda, A. and Nakhmanson, S. and Heinonen, O. and Razumnaya, A. and Luk’yanchuk, I. and Vinokur, V. M.},
	month = may,
	year = {2020},
	pages = {8657},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\AXZJJ5II\\Tikhonov и др. - 2020 - Controllable skyrmion chirality in ferroelectrics.pdf:application/pdf},
}



@article{lukyanchuk_hopfions_2020,
	title = {Hopfions emerge in ferroelectrics},
	volume = {11},
	issn = {2041-1723},
	url = {https://www.nature.com/articles/s41467-020-16258-w},
	doi = {10.1038/s41467-020-16258-w},
	abstract = {Abstract
            Paradigmatic knotted solitons, Hopfions, that are characterized by topological Hopf invariant, attract an intense attention in the diverse areas of physics ranging from high-energy physics, cosmology and astrophysics to biology, magneto- and hydrodynamics and condensed matter physics. Yet, while being of broad interest, they remain elusive and under-explored. Here we demonstrate that Hopfions emerge as a basic configuration of polarization field in confined ferroelectric nanoparticles. Our findings establish that Hopfions are of fundamental importance for the electromagnetic behavior of the nanocomposits and can result in advanced functionalities of these materials.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Nature Communications},
	author = {Luk’yanchuk, I. and Tikhonov, Y. and Razumnaya, A. and Vinokur, V. M.},
	month = may,
	year = {2020},
	pages = {2433},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\B5GV9UWB\\Luk’yanchuk и др. - 2020 - Hopfions emerge in ferroelectrics.pdf:application/pdf},
}



@article{anokhin_lattice_2020,
	title = {Lattice {Dynamics} of the {Strontium} {Ferrotungstate} in the {Temperature} {Range} 300–700 {K}},
	volume = {62},
	issn = {1063-7834, 1090-6460},
	url = {http://link.springer.com/10.1134/S1063783420120033},
	doi = {10.1134/S1063783420120033},
	language = {en},
	number = {12},
	urldate = {2023-11-11},
	journal = {Physics of the Solid State},
	author = {Anokhin, A. S. and Razumnaya, A. G. and Pavlenko, A. V.},
	month = dec,
	year = {2020},
	pages = {2434--2438},
}



@article{kuriganova_electrochemical_2020,
	title = {Electrochemical dispersion technique for the preparation of {Sn}-doped {Pt} particles and their use as electrocatalysts},
	volume = {30},
	issn = {09599436},
	url = {https://linkinghub.elsevier.com/retrieve/pii/S0959943620302625},
	doi = {10.1016/j.mencom.2020.09.037},
	language = {en},
	number = {5},
	urldate = {2023-11-11},
	journal = {Mendeleev Communications},
	author = {Kuriganova, Alexandra B. and Leontyev, Igor N. and Ulyankina, Anna A. and Smirnova, Nina V.},
	month = sep,
	year = {2020},
	pages = {663--665},
}



@article{payod_2n4-rule_2020,
	title = {{2N}+4-rule and an atlas of bulk optical resonances of zigzag graphene nanoribbons},
	volume = {11},
	issn = {2041-1723},
	url = {https://www.nature.com/articles/s41467-019-13728-8},
	doi = {10.1038/s41467-019-13728-8},
	abstract = {Abstract
            
              Development of on-chip integrated carbon-based optoelectronic nanocircuits requires fast and non-invasive structural characterization of their building blocks. Recent advances in synthesis of single wall carbon nanotubes and graphene nanoribbons allow for their use as atomically precise building blocks. However, while cataloged experimental data are available for the structural characterization of carbon nanotubes, such an atlas is absent for graphene nanoribbons. Here we theoretically investigate the optical absorption resonances of armchair carbon nanotubes and zigzag graphene nanoribbons continuously spanning the tube (ribbon) transverse sizes from 0.5(0.4) nm to 8.1(12.8) nm. We show that the linear mapping is guaranteed between the tube and ribbon bulk resonance when the number of atoms in the tube unit cell is
              
                
                  \$\$2N+4\$\$
                  
                    2
                    N
                    +
                    4
                  
                
              
              , where
              
                
                  \$\$N\$\$
                  
                    N
                  
                
              
              is the number of atoms in the ribbon unit cell. Thus, an atlas of carbon nanotubes optical transitions can be mapped to an atlas of zigzag graphene nanoribbons.},
	language = {en},
	number = {1},
	urldate = {2023-11-10},
	journal = {Nature Communications},
	author = {Payod, Renebeth B. and Grassano, Davide and Santos, Gil Nonato C. and Levshov, Dmitry I. and Pulci, Olivia and Saroka, Vasil A.},
	month = jan,
	year = {2020},
	pages = {82},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\GVJGZB4S\\Payod и др. - 2020 - 2N+4-rule and an atlas of bulk optical resonances .pdf:application/pdf},
}



@article{shirokov_tunable_2020,
	title = {Tunable {Electromechanical} {Properties} of a {Barium} {Strontium} {Titanate} {Ferroelectric} {Film} {Under} a {Uniaxial} {Stress}},
	volume = {67},
	issn = {0885-3010, 1525-8955},
	url = {https://ieeexplore.ieee.org/document/9146729/},
	doi = {10.1109/TUFFC.2020.3011591},
	number = {12},
	urldate = {2023-11-11},
	journal = {IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control},
	author = {Shirokov, Vladimir Borisovich and Timoshenko, Pavel Evgenjevich and Pan'kin, Artyom Vital'yevich and Razumnaya, Anna Grigoryevna},
	month = dec,
	year = {2020},
	pages = {2704--2709},
}



@article{hanani_structural_2020,
	title = {Structural, dielectric, and ferroelectric properties of lead-free {BCZT} ceramics elaborated by low-temperature hydrothermal processing},
	volume = {31},
	issn = {0957-4522, 1573-482X},
	url = {https://link.springer.com/10.1007/s10854-020-03555-9},
	doi = {10.1007/s10854-020-03555-9},
	language = {en},
	number = {13},
	urldate = {2023-11-11},
	journal = {Journal of Materials Science: Materials in Electronics},
	author = {Hanani, Zouhair and Mezzane, Daoud and Amjoud, M’barek and Gagou, Yaovi and Hoummada, Khalid and Perrin, Carine and Razumnaya, Anna G. and Kutnjak, Zdravko and Bouzina, Adnane and Marssi, Mimoun El and Gouné, Mohamed and Rožič, Brigita},
	month = jul,
	year = {2020},
	pages = {10096--10104},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\ZEME2MZQ\\Hanani и др. - 2020 - Structural, dielectric, and ferroelectric properti.pdf:application/pdf},
}



@article{hanani_enhanced_2020,
	title = {Enhanced dielectric and electrocaloric properties in lead-free rod-like {BCZT} ceramics},
	volume = {9},
	issn = {2226-4108, 2227-8508},
	url = {http://link.springer.com/10.1007/s40145-020-0361-1},
	doi = {10.1007/s40145-020-0361-1},
	abstract = {Abstract
            
              Ba
              0.85
              Ca
              0.15
              Zr
              0.10
              Ti
              0.90
              O
              3
              (BCZT) lead-free ceramics demonstrated excellent dielectric, ferroelectric, and piezoelectric properties at the morphotropic phase boundary (MPB). So far, to study the effect of morphological changes on dielectric and ferroelectric properties in lead-free BCZT ceramics, researchers have mostly focused on the influence of spherical grain shape change. In this study, BCZT ceramics with rod-like grains and aspect ratio of about 10 were synthesized by surfactant-assisted solvothermal route. X-ray diffraction (XRD) and selected area electron diffraction (SAED) performed at room temperature confirm the crystallization of pure perovskite with tetragonal symmetry. Scanning electron microscopy (SEM) image showed that BCZT ceramics have kept the 1D rod-like grains with an average aspect ratio of about 4. Rod-like BCZT ceramics exhibit enhanced dielectric ferroelectric (ɛ
              r
              = 11,906, tanδ = 0.014,
              P
              r
              = 6.01 μgC/cm
              2
              , and
              E
              c
              = 2.46 kV/cm), and electrocaloric properties (Δ
              T
              = 0.492 K and gZ = 0.289 (K·mm)/kV at 17 kV/cm) with respect to spherical BCZT ceramics. Therefore, rod-like BCZT lead-free ceramics have good potential to be used in solid-state refrigeration technology.},
	language = {en},
	number = {2},
	urldate = {2023-11-11},
	journal = {Journal of Advanced Ceramics},
	author = {Hanani, Zouhair and Merselmiz, Soukaina and Danine, Abdelaadim and Stein, Nicolas and Mezzane, Daoud and Amjoud, M’barek and Lahcini, Mohammed and Gagou, Yaovi and Spreitzer, Matjaz and Vengust, Damjan and Kutnjak, Zdravko and El Marssi, Mimoun and Luk’yanchuk, Igor A. and Gouné, Mohamed},
	month = apr,
	year = {2020},
	pages = {210--219},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\PIFXGEQ5\\Hanani и др. - 2020 - Enhanced dielectric and electrocaloric properties .pdf:application/pdf},
}



@article{alyabyeva_terahertz-infrared_2020,
	title = {Terahertz-infrared spectroscopy of {Ti4}+-doped {M}-type barium hexaferrite},
	volume = {820},
	issn = {09258388},
	url = {https://linkinghub.elsevier.com/retrieve/pii/S0925838819346444},
	doi = {10.1016/j.jallcom.2019.153398},
	language = {en},
	urldate = {2023-11-11},
	journal = {Journal of Alloys and Compounds},
	author = {Alyabyeva, Liudmila and Yegiyan, Samvel and Torgashev, Victor and Prokhorov, Anatoly S. and Vinnik, Denis and Gudkova, Svetlana and Zherebtsov, Dmitry and Dressel, Martin and Gorshunov, Boris},
	month = apr,
	year = {2020},
	pages = {153398},
}



@article{hanani_thermally-stable_2020,
	title = {Thermally-stable high energy storage performances and large electrocaloric effect over a broad temperature span in lead-free {BCZT} ceramic},
	volume = {10},
	issn = {2046-2069},
	url = {http://xlink.rsc.org/?DOI=D0RA06116F},
	doi = {10.1039/D0RA06116F},
	abstract = {Thermally-stable recovered energy density and significant electrocaloric temperature change over a broad temperature span in BCZT ceramic elaborated by low-temperature hydrothermal processing.
          , 
            
              Ba
              0.85
              Ca
              0.15
              Zr
              0.10
              Ti
              0.90
              O
              3
              (BCZT) relaxor ferroelectric ceramics exhibit enhanced energy storage and electrocaloric performances due to their excellent dielectric and ferroelectric properties. In this study, the temperature-dependence of the structural and dielectric properties, as well as the field and temperature-dependence of the energy storage and the electrocaloric properties in BCZT ceramics elaborated at low-temperature hydrothermal processing are investigated. X-ray diffraction and Raman spectroscopy results confirmed the ferroelectric–paraelectric phase transition in the BCZT ceramic. At room temperature and 1 kHz, the dielectric constant and dielectric loss reached 5000 and 0.029, respectively. The BCZT ceramic showed a large recovered energy density (
              W
              rec
              ) of 414.1 mJ cm
              −3
              at 380 K, with an energy efficiency of 78.6\%, and high thermal-stability of
              W
              rec
              of 3.9\% in the temperature range of 340–400 K. The electrocaloric effect in BCZT was explored
              via
              an indirect approach following the Maxwell relation at 60 kV cm
              −1
              . The significant electrocaloric temperature change of 1.479 K at 367 K, a broad temperature span of 87 K, an enhanced refrigerant capacity of 140.33 J kg
              −1
              , and a high coefficient of performance of 6.12 obtained at 60 kV cm
              −1
              make BCZT ceramics potentially useful coolant materials in the development of future eco-friendly solid-state refrigeration technology.},
	language = {en},
	number = {51},
	urldate = {2023-11-11},
	journal = {RSC Advances},
	author = {Hanani, Zouhair and Merselmiz, Soukaina and Mezzane, Daoud and Amjoud, M'barek and Bradeško, Andraž and Rožič, Brigita and Lahcini, Mohammed and El Marssi, Mimoun and Ragulya, Andrey V. and Luk'yanchuk, Igor A. and Kutnjak, Zdravko and Gouné, Mohamed},
	year = {2020},
	pages = {30746--30755},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\3987HKNB\\Hanani и др. - 2020 - Thermally-stable high energy storage performances .pdf:application/pdf},
}



@article{timoshenko_finite-element_2020,
	title = {Finite-element {Modeling} of {SAW}-filters {Based} on {Thin} {Films} of {Barium} {Strontium} {Titanate}},
	volume = {17},
	issn = {1729-5459},
	url = {https://elibrary.ru/doi_resolution.asp?doi=10%2E31429%2Fvestnik%2D17%2D4%2D48%2D56},
	doi = {10.31429/vestnik-17-4-48-56},
	number = {4},
	urldate = {2023-11-11},
	journal = {Ecological Bulletin of Research Centers of the Black Sea Economic Cooperation},
	author = {Timoshenko, P.E. and Shirokov, V.B. and Kalinchuk, V.V.},
	year = {2020},
	pages = {48--56},
}



@article{konevtsova_irreversible_2020,
	title = {Irreversible and reversible morphological changes in the \textit{ϕ} 6 capsid and similar viral shells: symmetry and micromechanics},
	volume = {16},
	issn = {1744-683X, 1744-6848},
	shorttitle = {Irreversible and reversible morphological changes in the \textit{ϕ} 6 capsid and similar viral shells},
	url = {http://xlink.rsc.org/?DOI=D0SM01338B},
	doi = {10.1039/D0SM01338B},
	abstract = {We propose a new micromechanical model perfectly describing the capsid shapes and morphological transformations that occur between the states of the dodecahedral
              ϕ
              6 capsid and similar viral shells due to the sequential packaging of RNA segments.
            
          , 
            
              Understanding the physicochemical processes occurring in viruses during their maturation is of fundamental importance since only mature viruses can infect host cells. Here we consider the irreversible and reversible morphological changes that occur with the dodecahedral
              ϕ
              6 procapsid during the sequential packaging of 3 RNA segments forming the viral genome. It is shown that the dodecahedral shape of all the four observed capsid states is perfectly reproduced by a sphere radially deformed by only two irreducible spherical harmonics with icosahedral symmetry and wave numbers
              l
              = 6 and
              l
              = 10. The rotation of proteins around the 3-fold axes at the Procapsid → Intermediate 1 irreversible transformation is in fact also well described with the shear field containing only two irreducible harmonics with the same two wave numbers. The high stability of the Intermediate 1 state is discussed and the shapes of the Intermediate 2 state and Capsid (reversibly transforming back to the Intermediate 1 state) are shown to be mainly due to the isotropic pressure that the encapsidated RNA segments exert on the shell walls. The hidden symmetry of the capsid and the physicochemical features of the
              in vitro
              genome extraction from the viral shell are also elucidated.},
	language = {en},
	number = {40},
	urldate = {2023-11-11},
	journal = {Soft Matter},
	author = {Konevtsova, Olga V. and Roshal, Daria S. and Podgornik, Rudolf and Rochal, Sergei B.},
	year = {2020},
	pages = {9383--9392},
}



@article{konevtsova_carbon_2020,
	title = {Carbon nanotube sorting due to commensurate molecular wrapping},
	volume = {12},
	issn = {2040-3364, 2040-3372},
	url = {http://xlink.rsc.org/?DOI=D0NR03236K},
	doi = {10.1039/D0NR03236K},
	abstract = {Commensurate wrapping of carbon nanotubes ensures their selection by flavin group molecules.
          , 
            Single-walled carbon nanotubes (SWCNTs) can be sorted by their structural parameters using organic molecules and polymers: some of which, demonstrating a profound affinity only for specific nanotubes, form dense coatings on them. Here, analyzing well-known examples of flavin group molecules and those of 2,4-dichlorophenoxyacetic acid, we show for the first time that successful formation of the considered coatings depends on the ability of molecules to wrap around the SWCNT in a commensurate way. Commensurability provides a decrease in the free energy of the resulting bilayer system and makes the coating much more stable. Concurrently, it strongly relates the nanotube chiral vector with the geometric characteristics of the adhering molecules, which leads to revealed selection rules. If they are not satisfied, the deposition of molecules does not occur or is insignificant. The proposed theory unambiguously explains known experimental results on the formation of spiral wrappings of SWCNTs by flavin group molecules and points out other organic molecules and polymers suitable for effective CNT sorting.},
	language = {en},
	number = {29},
	urldate = {2023-11-11},
	journal = {Nanoscale},
	author = {Konevtsova, Olga V. and Roshal, Daria S. and Dmitriev, Vladimir P. and Rochal, Sergei B.},
	year = {2020},
	pages = {15725--15735},
}



@article{poullet_mechanical_2020,
	title = {Mechanical instabilities of aorta drive blood stem cell production: a live study},
	volume = {77},
	issn = {1420-9071},
	shorttitle = {Mechanical instabilities of aorta drive blood stem cell production},
	url = {https://doi.org/10.1007/s00018-019-03372-2},
	doi = {10.1007/s00018-019-03372-2},
	abstract = {During embryogenesis of all vertebrates, haematopoietic stem/progenitor cells (HSPCs) extrude from the aorta by a complex process named endothelial-to-haematopoietic transition (EHT). HSPCs will then colonize haematopoietic organs allowing haematopoiesis throughout adult life. The mechanism underlying EHT including the role of each aortic endothelial cell (EC) within the global aorta dynamics remains unknown. In the present study, we show for the first time that EHT involves the remodelling of individual cells within a collective migration of ECs which is tightly orchestrated, resulting in HSPCs extrusion in the sub-aortic space without compromising aorta integrity. By performing a cross-disciplinary study which combines high-resolution 4D imaging and theoretical analysis based on the concepts of classical mechanics, we propose that this complex developmental process is dependent on mechanical instabilities of the aorta preparing and facilitating the extrusion of HSPCs.},
	language = {en},
	number = {17},
	urldate = {2023-11-11},
	journal = {Cellular and Molecular Life Sciences},
	author = {Poullet, Nausicaa and Golushko, Ivan and Lorman, Vladimir and Travnickova, Jana and Bureau, Charlotte and Chalin, Dmitrii and Rochal, Sergei and Parmeggiani, Andrea and Kissa, Karima},
	month = sep,
	year = {2020},
	keywords = {4D microscopy, Endothelial-to-haematopoietic transition, Haematopoiesis, Modeling, Zebrafish},
	pages = {3453--3464},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\8C4TEQZS\\Poullet и др. - 2020 - Mechanical instabilities of aorta drive blood stem.pdf:application/pdf;Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\6C7BISAS\\Poullet и др. - 2020 - Mechanical instabilities of aorta drive blood stem.pdf:application/pdf},
}



@article{ahmed_effect_2019,
	title = {Effect of aluminium substitution on low energy electrodynamics of barium-lead {M}-type hexagonal ferrites},
	volume = {1389},
	issn = {1742-6596},
	url = {https://dx.doi.org/10.1088/1742-6596/1389/1/012044},
	doi = {10.1088/1742-6596/1389/1/012044},
	abstract = {We present the first detailed study of the terahertz-infrared dielectric response of single crystalline lead-substituted M-type barium hexaferrites doped with Al3+. The broadband spectra of complex dielectric permittivity ε*(v)=ε’(v)+iε"(v) of Ba0.8Pb0.2AlxFe12-xO19 with concentrations of the dopant x(Al)=1.2, 3, 3.3 are obtained for two principle polarizations using Fourier-transform infrared spectroscopy and terahertz time-domain spectroscopy in the temperature range from 4 to 300 K and at frequencies from 10 cm−1 up to 8000 cm−1. We observe a rich set of excitations and assign them to the electronic transitions within the ground state 5E of the 4-fold coordinated divalent iron and to phonon resonances. Effect of Al3+ cation substitution on low energy (terahertz) dielectric response and infrared phonon spectra of barium-lead M-type hexaferrites is analysed and discussed.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Journal of Physics: Conference Series},
	author = {Ahmed, Asmaa and Alyabyeva, Liudmila and Torgashev, Victor and Prokhorov, Anatoly S. and Vinnik, Denis and Dressel, Martin and Gorshunov, Boris},
	month = nov,
	year = {2019},
	note = {Publisher: IOP Publishing},
	pages = {012044},
	file = {IOP Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\F2HHUAX3\\Ahmed и др. - 2019 - Effect of aluminium substitution on low energy ele.pdf:application/pdf},
}



@article{mukhortov_structure_2019,
	title = {Structure, lattice dynamics, properties of bismuth titanate heterostructures},
	volume = {53},
	issn = {0022-3727},
	url = {https://dx.doi.org/10.1088/1361-6463/ab4bf6},
	doi = {10.1088/1361-6463/ab4bf6},
	abstract = {We investigated the epitaxial Bi4Ti3O12 (BTO) thin films with different thicknesses on a (0 0 1) MgO substrate with a Ba0.4Sr0.6TiO3 buffer layer (4 nm). The crystallographic axis [1 0 0] of Bi4Ti3O12 film is rotated on degrees relative to [1 0 0] MgO axis. When the thickness of Bi4Ti3O12 film is less than 40 nm, the unit cell of the film is compressed in the normal to the interface plane direction. In cases of large film thicknesses, the sign of strain changes and correspondingly the unit cell is stretched. Switched spontaneous polarization in the interface plane with 180° domain structure occurs at 10 nm film thickness and increases with a thickness up to 55 C cm−2. Changes in the Raman spectra of the Bi4Ti3O12 films indicates to increase of monoclinic distortion of the film unit cell in comparison with the bulk unit cell. The anisotropy of in-plane dielectric properties and the effect of internal strain on dielectric properties for the Bi4Ti3O12 films are confirmed by the study of the dielectric characteristics of the films.},
	language = {en},
	number = {3},
	urldate = {2023-11-11},
	journal = {Journal of Physics D: Applied Physics},
	author = {Mukhortov, V. M. and Golovko, Yu I. and Anokhin, A. S. and Stryukov, D. V. and Biryukov, S. V. and Timoshenko, P. E.},
	month = nov,
	year = {2019},
	note = {Publisher: IOP Publishing},
	pages = {035304},
}





@article{timoshenko_terahertz_2022,
	title = {Terahertz frequency selective surfaces using heterostructures based on two-dimensional diffraction grating of single-walled carbon nanotubes},
	volume = {14},
	issn = {1947-5411, 1947-542X},
	url = {https://www.tandfonline.com/doi/full/10.1080/19475411.2022.2148307},
	doi = {10.1080/19475411.2022.2148307},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {International Journal of Smart and Nano Materials},
	author = {Timoshenko, Pavel Evgenjevich and Lerer, Alexander and Rochal, Sergei Bernardovich},
	month = dec,
	year = {2022},
	keywords = {Q1},
	pages = {21--35},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\4F954CZU\\Timoshenko и др. - 2023 - Terahertz frequency selective surfaces using heter.pdf:application/pdf},
}



@article{talanov_vanadium_2018,
	title = {Vanadium clusters formation in geometrically frustrated spinel oxide {AlV}$_{\textrm{2}}${O}$_{\textrm{4}}$},
	volume = {74},
	copyright = {Copyright (c) 2018 International Union of Crystallography},
	issn = {2052-5206},
	url = {http://scripts.iucr.org/cgi-bin/paper?dq5028},
	doi = {10.1107/S2052520618007242},
	abstract = {The spinel oxide AlV2O4 is a unique material, in which the formation of clusters is accompanied by atomic, charge and orbital ordering and a rhombohedral lattice distortion. In this work a theory of the structural phase transition in AlV2O4 is proposed. This theory is based on the study of the order-parameter symmetry, thermodynamics, electron density distribution, crystal chemistry and mechanisms of formation of the atomic and orbital structures of the rhombohedral phase. It is established that the critical order parameter is transformed according to irreducible representation k9(τ4) (in Kovalev notation) of the Fd {\textbackslash}bar\{3\}m space group. Knowledge of the order-parameter symmetry allows us to show that the derived AlV2O4 rhombohedral structure is a result of displacements of all atom types and the ordering of Al atoms (1:1 order type in tetrahedral spinel sites), V atoms (1:1:6 order type in octahedral sites) and O atoms (1:1:3:3 order type), and the ordering of dxy, dxz and dyz orbitals. Application of the density functional theory showed that V atoms in the Kagomé sublattice formed separate trimers. Also, no sign of metallic bonding between separate vanadium trimers in the heptamer structure was found. The density functional theory study and the crystal chemical analysis of V—O bond lengths allowed us to assume the existence of dimers and trimers as main clusters in the structure of the AlV2O4 rhombohedral modification. The trimer model of the low-symmetry AlV2O4 structure is proposed. Within the Landau theory of phase transitions, typical diagrams of possible phase states are built. It is shown that phase states can be changed as a first-order phase transition close to the second order in the vicinity of tricritical points of the phase diagrams.},
	language = {en},
	number = {4},
	urldate = {2023-11-11},
	journal = {Acta Crystallographica Section B: Structural Science, Crystal Engineering and Materials},
	author = {Talanov, M. V. and Shirokov, V. B. and Avakyan, L. A. and Talanov, V. M. and Borlakov, K. S.},
	month = aug,
	year = {2018},
	note = {Number: 4
Publisher: International Union of Crystallography},
	pages = {337--353},
}



@article{kozakov_valence_2018,
	title = {Valence state of cations in manganites {Pr}$_{\textrm{1-x}}${Ca}$_{\textrm{x}}${MnO}$_{\textrm{3}}$ (0.3 ≤ x ≤ 0.5) from {X}-ray diffraction and {X}-ray photoelectron spectroscopy},
	volume = {740},
	issn = {0925-8388},
	url = {https://www.sciencedirect.com/science/article/pii/S0925838818300021},
	doi = {10.1016/j.jallcom.2018.01.002},
	abstract = {Polycrystalline Pr1-xCaxMnO3 (х = 0.3, 0.35, 04, 0.45, and 0.5) samples are synthesized by solid-state reaction method. Crystal structure of the samples is studied by X-ray diffraction method with Rietveld refinement. Diffraction patterns from all the samples are well indexed within the Pnma space group. It is shown that lattice parameters and unit cell volume decrease monotonically and O−Mn−O angles become closer to the ideal 180⁰ value upon the growth of x. Mn2p, Mn3s, Ca2p, Pr3d, Pr4d, and O1s X-ray photoelectron spectra are measured. Pr3d and Pr4d spectra are calculated in isolated ion approximation with approximate accounting for the charge transfer effect. Elemental compositions of samples are measured by the XPS method; they differ noticeably from the nominal ones. Charge compensation upon heterovalent Pr3+ → Ca2+ substitution is shown to realize via two mechanisms: creation of oxygen vacancies and formation of Mn4+ ions coexisting with Mn3+. Relative Mn4+/Mn3+ abundances are determined via decomposition of Mn2p and Mn3s XPS into contributions from the spectra of tri- and quadrivalent Mn ions. The amount of Mn4+ ions is shown to increase with Ca content x.},
	urldate = {2023-11-11},
	journal = {Journal of Alloys and Compounds},
	author = {Kozakov, A. T. and Kochur, A. G. and Trotsenko, V. G. and Nikolskii, A. V. and El Marssi, M. and Gorshunov, B. P. and Torgashev, V. I.},
	month = apr,
	year = {2018},
	keywords = {XPS, Manganites, Cations valence state, Elemental composition, Mn/Mn content, PCaMnO (PCMO) ceramics, Vacancies, XRD},
	pages = {132--142},
}



@article{trotsenko_temperature_2018,
	title = {Temperature {Behavior} of the {Rotational} {Order} {Parameters} in a {La}$_{\textrm{0.25}}${Ca}$_{\textrm{0.75}}${MnO}$_{\textrm{3}}$ {Solid} {Solution}},
	volume = {82},
	issn = {1934-9432},
	url = {https://doi.org/10.3103/S1062873818030310},
	doi = {10.3103/S1062873818030310},
	abstract = {The behavior of the crystal structure of a La0.25Ca0.75MnO3 solid solution in the temperature range of 80–725 K is studied. It is established that rotational structural distortions predominate during the transition to a charge-ordered state},
	language = {en},
	number = {3},
	urldate = {2023-11-11},
	journal = {Bulletin of the Russian Academy of Sciences: Physics},
	author = {Trotsenko, V. G. and Mikheykin, A. S. and Shirokov, V. B. and Razumnaya, A. G. and Bush, A. A. and Kadyrov, L. S. and El Marssi, M. and Gorshunov, B. P. and Torgashev, V. I.},
	month = mar,
	year = {2018},
	pages = {335--337},
}



@article{kabirov_effect_2018,
	title = {Effect of a magnetic field on the permittivity of 80\%{La}$_{\textrm{0.7}}${Sr}$_{\textrm{0.3}}${MnO}$_{\textrm{3}}$/20\%{GeO}$_{\textrm{2}}$ composite},
	volume = {60},
	issn = {1090-6460},
	url = {https://doi.org/10.1134/S1063783418010110},
	doi = {10.1134/S1063783418010110},
	abstract = {The dielectric properties of a magnetoresistive conducting two-phase 80\%La0.7Sr0.3MnO3/20\%GeO2 (wt \%) composite have been studied near the percolation threshold in magnetic fields from 0 to 15 kOe at frequencies of the measurement field from 5 kHz to 1 MHz. The samples have inductive impedances; i.e., their permittivities can be considered negative due to a high conductivity in this frequency range. The permittivity increases in magnitude in magnetic field, and the values of the magnetodielectric coefficient reach 23\% at room temperature. The reasons for the effect of magnetic field on the dielectric permittivity of samples are discussed.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Physics of the Solid State},
	author = {Kabirov, Yu. V. and Gavrilyachenko, V. G. and Bogatin, A. S. and Sitalo, E. I. and Yatsenko, V. K.},
	month = jan,
	year = {2018},
	pages = {60--63},
}



@article{gorshunov_collective_2018,
	title = {Collective {Infrared} {Excitation} in {LuB}$_{\textrm{12}}$ {Cage}-{Glass}},
	volume = {107},
	issn = {1090-6487},
	url = {https://doi.org/10.1134/S0021364018020029},
	doi = {10.1134/S0021364018020029},
	abstract = {By measuring room temperature infrared (40–35000 cm–1) reflectivity of metallic LuB12 single crystals with different isotopic compositions (natB, 10B, 11B), we find that to model the spectrum we had to introduce, additionally to Drude free-carrier component, a broad excitation with unusually large dielectric contribution (Δε = 8000 ± 4000), which is characterized by a non-Lorentzian lineshape. It is suggested that the origin of the excitation is connected with cooperative dynamics of Jahn–Teller active B12 molecules producing quasilocal vibrations (rattling modes) of caged lutetium ions. The coupling of the Lu3+ rattling motions with the charge carriers of conduction band is proposed to be the reason of strongly damped character of the excitation.},
	language = {en},
	number = {2},
	urldate = {2023-11-11},
	journal = {JETP Letters},
	author = {Gorshunov, B. P. and Zhukova, E. S. and Komandin, G. A. and Torgashev, V. I. and Muratov, A. V. and Aleshchenko, Yu. A. and Demishev, S. V. and Shitsevalova, N. Yu. and Filipov, V. B. and Sluchanko, N. E.},
	month = jan,
	year = {2018},
	pages = {100--105},
}



@patent{___ru__2017,
	title = {Пассивный беспроводный датчик ультрафиолетового излучения на поверхностных акустических волнах},
	url = {https://findpatent.ru/patent/261/2613590.html},
	number = {RU 2613590},
	author = {{Кайдашев Евгений Михайлович (RU)} and {Кайдашев Владимир Евгеньевич (RU)} and {Карапетьян Геворк Яковлевич (RU)} and {Жилин Денис Анатольевич (RU)}},
	month = mar,
	year = {2017},
}



@article{tikhonov_polarization_2022,
	title = {Polarization {Topology} at the {Nominally} {Charged} {Domain} {Walls} in {Uniaxial} {Ferroelectrics}},
	volume = {34},
	issn = {0935-9648, 1521-4095},
	url = {https://onlinelibrary.wiley.com/doi/10.1002/adma.202203028},
	doi = {10.1002/adma.202203028},
	abstract = {Abstract
            
              Ferroelectric domain walls provide a fertile environment for novel materials physics. If a polarization discontinuity arises, it can drive a redistribution of electronic carriers and changes in band structure, which often result in emergent 2D conductivity. If such a discontinuity is not tolerated, then its amelioration usually involves the formation of complex topological patterns, such as flux‐closure domains, dipolar vortices, skyrmions, merons, or Hopfions. The degrees of freedom required for the development of such patterns, in which dipolar rotation is a hallmark, are readily found in multiaxial ferroelectrics. In uniaxial ferroelectrics, where only two opposite polar orientations are possible, it has been assumed that discontinuities are unavoidable when antiparallel components of polarization meet. This perception has been borne out by the appearance of charged conducting domain walls in systems such as hexagonal manganites and lithium niobate. Here, experimental and theoretical investigations on lead germanate (Pb
              5
              Ge
              3
              O
              11
              ) reveal that polar discontinuities can be obviated at head‐to‐head and tail‐to‐tail domain walls by mutual domain bifurcation along two different axes, creating a characteristic saddle‐point domain wall morphology and associated novel dipolar topology, removing the need for screening charge accumulation and associated conductivity enhancement.},
	language = {en},
	number = {45},
	urldate = {2023-11-11},
	journal = {Advanced Materials},
	author = {Tikhonov, Yurii and Maguire, Jesi R. and McCluskey, Conor J. and McConville, James P. V. and Kumar, Amit and Lu, Haidong and Meier, Dennis and Razumnaya, Anna and Gregg, John Martin and Gruverman, Alexei and Vinokur, Valerii M. and Luk'yanchuk, Igor},
	month = nov,
	year = {2022},
	pages = {2203028},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\2JEF82TV\\Tikhonov и др. - 2022 - Polarization Topology at the Nominally Charged Dom.pdf:application/pdf},
}



@article{pavlenko_phase_2022,
	title = {Phase {Diagram} of a {Strained} {Ferroelectric} {Nanowire}},
	volume = {12},
	issn = {2073-4352},
	url = {https://www.mdpi.com/2073-4352/12/4/453},
	doi = {10.3390/cryst12040453},
	abstract = {Ferroelectric materials manifest unique dielectric, ferroelastic, and piezoelectric properties. A targeted design of ferroelectrics at the nanoscale is not only of fundamental appeal but holds the highest potential for applications. Compared to two-dimensional nanostructures such as thin films and superlattices, one-dimensional ferroelectric nanowires are investigated to a much lesser extent. Here, we reveal a variety of the topological polarization states, particularly the vortex and helical chiral phases, in loaded ferroelectric nanowires, which enable us to complete the strain–temperature phase diagram of the one-dimensional ferroelectrics. These phases are of prime importance for optoelectronics and quantum communication technologies.},
	language = {en},
	number = {4},
	urldate = {2023-11-11},
	journal = {Crystals},
	author = {Pavlenko, Maksim A. and Di Rino, Franco and Boron, Leo and Kondovych, Svitlana and Sené, Anaïs and Tikhonov, Yuri A. and Razumnaya, Anna G. and Vinokur, Valerii M. and Sepliarsky, Marcelo and Lukyanchuk, Igor A.},
	month = mar,
	year = {2022},
	pages = {453},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\9V22JHFK\\Pavlenko и др. - 2022 - Phase Diagram of a Strained Ferroelectric Nanowire.pdf:application/pdf;Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\NDRVUCFW\\Pavlenko и др. - 2022 - Phase Diagram of a Strained Ferroelectric Nanowire.pdf:application/pdf},
}



@article{rochal_packing_2022,
	title = {Packing and trimer-to-dimer protein reconstruction in icosahedral viral shells with a single type of symmetrical structural unit},
	volume = {4},
	issn = {2516-0230},
	url = {http://xlink.rsc.org/?DOI=D2NA00461E},
	doi = {10.1039/D2NA00461E},
	abstract = {Modelling morphological transformation in
              Flavivirus
              proteinaceous shells at maturation. Locally periodic arrangement of pr peptides makes the dimeric state energetically more favorable at a low pH level.
            
          , 
            
              Understanding the principles of protein packing and the mechanisms driving morphological transformations in virus shells (capsids) during their maturation can be pivotal for the development of new antiviral strategies. Here, we study how these principles and mechanisms manifest themselves in icosahedral viral capsids assembled from identical symmetric structural units (capsomeres). To rationalize such shells, we model capsomers as symmetrical groups of identical particles interacting with a short-range potential typical of the classic Tammes problem. The capsomere particles are assumed to retain their relative positions on the vertices of planar polygons placed on the spherical shell and to interact only with the particles from other capsomeres. Minimization of the interaction energy enforces equal distances between the nearest particles belonging to neighboring capsomeres and minimizes the number of different local environments. Thus, our model implements the Caspar and Klug quasi-equivalence principle and leads to packings strikingly similar to real capsids. We then study a reconstruction of protein trimers into dimers in a
              Flavivirus
              shell during its maturation, connecting the relevant structural changes with the modifications of the electrostatic charges of proteins, wrought by the oxidative switch in the bathing solution that is essential for the process. We highlight the key role of pr peptides in the shell reconstruction and show that the highly ordered arrangement of these subunits in the dimeric state is energetically favored at a low pH level. We also discuss the electrostatic mechanisms controlling the release of pr peptides in the last irreversible step of the maturation process.},
	language = {en},
	number = {21},
	urldate = {2023-11-11},
	journal = {Nanoscale Advances},
	author = {Rochal, Sergei B. and Konevtsova, Olga V. and Roshal, Daria S. and Božič, Anže and Golushko, Ivan Yu. and Podgornik, Rudolf},
	year = {2022},
	pages = {4677--4688},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\DB8I4DZC\\Rochal и др. - 2022 - Packing and trimer-to-dimer protein reconstruction.pdf:application/pdf;Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\7PKD38HX\\Rochal и др. - 2022 - Packing and trimer-to-dimer protein reconstruction.pdf:application/pdf},
}



@article{shirokov_thermodynamic_2022,
	title = {Thermodynamic theory of {Pb}$_{\textrm{x}}${Sr}$_{\textrm{1-x}}${TiO}$_{\textrm{3}}$ solid solutions},
	volume = {161},
	issn = {00223697},
	url = {https://linkinghub.elsevier.com/retrieve/pii/S0022369721004613},
	doi = {10.1016/j.jpcs.2021.110395},
	language = {en},
	urldate = {2023-11-11},
	journal = {Journal of Physics and Chemistry of Solids},
	author = {Shirokov, V.B. and Razumnaya, A.G. and Mikheykin, A.S.},
	month = feb,
	year = {2022},
	pages = {110395},
}



@article{abdulvakhidov_study_2022,
	title = {Study of the structural-phase state and physical properties of (1 − x)({CoFe}$_{\textrm{2}}${O}$_{\textrm{4}}$) − x({PbTiO}$_{\textrm{3}}$) compositions},
	volume = {128},
	issn = {0947-8396, 1432-0630},
	url = {https://link.springer.com/10.1007/s00339-022-05442-y},
	doi = {10.1007/s00339-022-05442-y},
	language = {en},
	number = {4},
	urldate = {2023-11-11},
	journal = {Applied Physics A},
	author = {Abdulvakhidov, Bashir and Li, Zhengyou and Abdulvakhidov, Kamaludin and Soldatov, Alexander and Nazarenko, Alexander and Kulbuzhev, Bashir and Mardasova, Irina and Lyanguzov, Nikolay and Sitalo, Evgeniy and Sadykov, Sadyk and Sirota, Marina and Dmitrenko, Ivan and Manukyan, Aram},
	month = apr,
	year = {2022},
	pages = {293},
}



@article{zahid_enhanced_2022,
	title = {Enhanced near-ambient temperature energy storage and electrocaloric effect in the lead-free {BaTi}$_{\textrm{0.89}}${Sn}$_{\textrm{0.11}}${O}$_{\textrm{3}}$ ceramic synthesized by sol–gel method},
	volume = {33},
	issn = {0957-4522, 1573-482X},
	url = {https://link.springer.com/10.1007/s10854-022-08233-6},
	doi = {10.1007/s10854-022-08233-6},
	language = {en},
	number = {16},
	urldate = {2023-11-11},
	journal = {Journal of Materials Science: Materials in Electronics},
	author = {Zahid, Marwa and Hadouch, Youness and Amjoud, M’barek and Mezzane, Daoud and Gouné, Mohamed and Hoummada, Khalid and Alimoussa, Abdelhadi and Razumnaya, Anna G. and Rožič, Brigita and Kutnjak, Zdravko},
	month = jun,
	year = {2022},
	pages = {12900--12911},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\JXG9ZCDZ\\Zahid и др. - 2022 - Enhanced near-ambient temperature energy storage a.pdf:application/pdf;Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\GCABVF4P\\Zahid и др. - 2022 - Enhanced near-ambient temperature energy storage a.pdf:application/pdf},
}



@article{zaitouni_enhanced_2022,
	title = {Enhanced electrocaloric and energy-storage properties of environment-friendly ferroelectric {Ba}$_{\textrm{0.9}}${Sr}$_{\textrm{0.1}}${Ti}$_{\textrm{1−x}}${Sn}$_{\textrm{x}}${O}$_{\textrm{3}}$ ceramics},
	volume = {31},
	issn = {23524928},
	url = {https://linkinghub.elsevier.com/retrieve/pii/S2352492822002227},
	doi = {10.1016/j.mtcomm.2022.103351},
	language = {en},
	urldate = {2023-11-11},
	journal = {Materials Today Communications},
	author = {Zaitouni, H. and Hajji, L. and Mezzane, D. and Choukri, E. and Razumnaya, A.G. and Gagou, Y. and Hoummada, K. and Alimoussa, A. and Rožič, B. and Črešnar, D. and El Marssi, M. and Kutnjak, Z.},
	month = jun,
	year = {2022},
	pages = {103351},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\24PCRTWA\\Zaitouni и др. - 2022 - Enhanced electrocaloric and energy-storage propert.pdf:application/pdf;Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\C3NG5P6W\\Zaitouni и др. - 2022 - Enhanced electrocaloric and energy-storage propert.pdf:application/pdf},
}



@article{hadouch_electrocaloric_2022,
	title = {Electrocaloric effect and high energy storage efficiency in lead-free {Ba}$_{\textrm{0.95}}${Ca}$_{\textrm{0.05}}${Ti}$_{\textrm{0.89}}${Sn}$_{\textrm{0.11}}${O}$_{\textrm{3}}$ ceramic elaborated by sol–gel method},
	volume = {33},
	issn = {0957-4522, 1573-482X},
	url = {https://link.springer.com/10.1007/s10854-021-07411-2},
	doi = {10.1007/s10854-021-07411-2},
	language = {en},
	number = {4},
	urldate = {2023-11-11},
	journal = {Journal of Materials Science: Materials in Electronics},
	author = {Hadouch, Youness and Ben Moumen, Said and Mezzourh, Hanane and Mezzane, Daoud and Amjoud, M’barek and Asbani, Bouchra and Razumnaya, Anna G. and Gagou, Yaovi and Rožič, Brigita and Kutnjak, Zdravko and El Marssi, Mimoun},
	month = feb,
	year = {2022},
	pages = {2067--2079},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\3DEEINNF\\Hadouch и др. - 2022 - Electrocaloric effect and high energy storage effi.pdf:application/pdf;Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\ECS5QNNK\\Hadouch и др. - 2022 - Electrocaloric effect and high energy storage effi.pdf:application/pdf},
}



@article{linnik_raman_2021,
	title = {Raman {Response} of {Quantum} {Critical} {Ferroelectric} {Pb}-{Doped} {SrTiO}$_{\textrm{3}}$},
	volume = {11},
	issn = {2073-4352},
	url = {https://www.mdpi.com/2073-4352/11/12/1469},
	doi = {10.3390/cryst11121469},
	abstract = {A quantum paraelectric SrTiO3 is a material situated in close proximity to a quantum critical point (QCP) of ferroelectric transition in which the critical temperature to the ferroelectric state is suppressed down to 0 K. However, the understanding of the behavior of the phase transition in the vicinity of this point remains challenging. Using the concentration x of Pb in solid solution Sr1−xPbxTiO3 (PSTx) as a tuning parameter and applying the combination of Raman and dielectric spectroscopy methods, we approach the QCP in PSTx and study the interplay of classical and quantum phenomena in the region of criticality. We obtain the critical temperature of PSTx and the evolution of the temperature-dependent dynamical properties of the system as a function of x to reveal the mechanism of the transition. We show that the ferroelectric transition occurs gradually through the emergence of the polar nanoregions inside the non-polar tetragonal phase with their further expansion on cooling. We also study the ferroelastic cubic-to-tetragonal structural transition, occurring at higher temperatures, and show that its properties are almost concentration-independent and not affected by the quantum criticality.},
	language = {en},
	number = {12},
	urldate = {2023-11-10},
	journal = {Crystals},
	author = {Linnik, Ekaterina D. and Mikheykin, Alexey S. and Rubi, Diego and Shirokov, Vladimir B. and Mezzane, Daoud and Kondovych, Svitlana V. and Lukyanchuk, Igor A. and Razumnaya, Anna G.},
	month = nov,
	year = {2021},
	pages = {1469},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\DT8BPF4T\\Linnik и др. - 2021 - Raman Response of Quantum Critical Ferroelectric P.pdf:application/pdf},
}



@article{weber_structural_2020,
	title = {Structural features of the {A}$_{\textrm{2}}${TiSi}$_{\textrm{2}}${O}$_{\textrm{8}}$ ( \textit{{A}} -{Ba} and {Pb}) compounds},
	volume = {10},
	issn = {2010-135X, 2010-1368},
	url = {https://www.worldscientific.com/doi/abs/10.1142/S2010135X20500228},
	doi = {10.1142/S2010135X20500228},
	abstract = {X-ray diffraction studies of synthesized Ba
              2
              TiSi
              2
              O
              8
              have shown that this compound has a fresnoite structure and is characterized by a polar phase [Formula: see text]4bm at room temperature. The synthesis of Pb
              2
              TiSi
              2
              O
              8
              in the fresnoite phase under the selected synthesis conditions has led to the formation of a perovskite tetragonal phase [Formula: see text]4mm corresponding to PbTiO
              3
              .},
	language = {en},
	number = {05},
	urldate = {2023-11-11},
	journal = {Journal of Advanced Dielectrics},
	author = {Weber, Svetlana and Lebedinskaya, Alla and Rudsky, Daniil and Kabirov, Yuri and Rudskaya, Anzhela and Kupriyanov, Michael},
	month = oct,
	year = {2020},
	pages = {2050022},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\CQ956RAJ\\Weber и др. - 2020 - Structural features of the A2TiSi2O8 ( A -B.pdf:application/pdf},
}



@article{shirokov_soft_2020,
	title = {Soft modes behavior in bilayer ({Ba},{Sr}){TiO}$_{\textrm{3}}$ /({Ba},{Sr}){TiO}$_{\textrm{3}}$ heterostructures},
	volume = {567},
	issn = {0015-0193, 1563-5112},
	url = {https://www.tandfonline.com/doi/full/10.1080/00150193.2020.1791593},
	doi = {10.1080/00150193.2020.1791593},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Ferroelectrics},
	author = {Shirokov, V. B. and Razumnaya, A. G.},
	month = oct,
	year = {2020},
	pages = {102--112},
}



@article{merselmiz_high_2020,
	title = {High energy storage efficiency and large electrocaloric effect in lead-free {BaTi}$_{\textrm{0.89}}${Sn}$_{\textrm{0.11}}${O}$_{\textrm{3}}$ ceramic},
	volume = {46},
	issn = {02728842},
	url = {https://linkinghub.elsevier.com/retrieve/pii/S027288422031823X},
	doi = {10.1016/j.ceramint.2020.06.163},
	language = {en},
	number = {15},
	urldate = {2023-11-11},
	journal = {Ceramics International},
	author = {Merselmiz, Soukaina and Hanani, Zouhair and Mezzane, Daoud and Spreitzer, Matjaž and Bradeško, Andraž and Fabijan, David and Vengust, Damjan and Amjoud, M’Barek and Hajji, Lahoucine and Abkhar, Zahra and Razumnaya, Anna G. and Rožič, Brigita and Luk'yanchuk, Igor A. and Kutnjak, Zdravko},
	month = oct,
	year = {2020},
	pages = {23867--23876},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\K8VED7CU\\Merselmiz и др. - 2020 - High energy storage efficiency and large electroca.pdf:application/pdf},
}



@article{razumnaya_built-electric_2020,
	title = {Built-in electric field induces polarization rotation in bilayer {BiFeO}$_{\textrm{3}}$/({Ba},{Sr}){TiO}$_{\textrm{3}}$ thin films},
	volume = {812},
	issn = {09258388},
	url = {https://linkinghub.elsevier.com/retrieve/pii/S0925838819334103},
	doi = {10.1016/j.jallcom.2019.152164},
	language = {en},
	urldate = {2023-11-11},
	journal = {Journal of Alloys and Compounds},
	author = {Razumnaya, A.G. and Mikheykin, A.S. and Stryukov, D.V. and Anokhin, A.S. and Pavlenko, A.V. and Shirokov, V.B. and Kaliteevski, M.A. and Mezzane, D. and Lukyanchuk, I.},
	month = jan,
	year = {2020},
	pages = {152164},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\5XSCX5X3\\Razumnaya и др. - 2020 - Built-in electric field induces polarization rotat.pdf:application/pdf},
}



@article{yegiyan_terahertz-infrared_2019,
	title = {Terahertz-infrared spectroscopy of single crystalline m-type hexaferrite {BaTi}$_{\textrm{x}}${Fe}$_{\textrm{12-x}}${O}$_{\textrm{19}}$},
	volume = {1389},
	issn = {1742-6596},
	url = {https://dx.doi.org/10.1088/1742-6596/1389/1/012038},
	doi = {10.1088/1742-6596/1389/1/012038},
	abstract = {We have studied polarization-dependent broad-band dielectric response of single-crystalline Ti-substituted barium hexaferrites BaTixFe12-xO19, x=0.64., 0.75, 1.1, in the frequency range from 10 to 8000 cm−1 and at temperatures from 5 to 300 K. In addition to a rich set of phonon resonances located at frequencies from 90 to 800 cm−1 we observed an unusual low-energy response (terahertz region, 10-100 cm−1) stemming from two different effects: relaxational process and second order spin-orbit coupling in Fe2+ ground state, that may set up new prospects for doped hexaferrites in terahertz technologies.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Journal of Physics: Conference Series},
	author = {Yegiyan, S. R. and Alyabyeva, L. N. and Torgashev, V. I. and Vinnik, D. A. and Gudkova, S. A. and Prokhorov, A. S. and Dressel, M. and Gorshunov, B. P.},
	month = nov,
	year = {2019},
	note = {Publisher: IOP Publishing},
	pages = {012038},
	file = {IOP Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\UWP6ZQD3\\Yegiyan и др. - 2019 - Terahertz-infrared spectroscopy of single crystall.pdf:application/pdf},
}



@article{boldyrev_structure_2019,
	title = {Structure, microstructure, dielectric and piezoelectric properties of (1-x-y){BiFeO}$_{\textrm{3}}$-{xPbFe}$_{\textrm{0.5}}${Nb}$_{\textrm{0.5}}${O}$_{\textrm{3}}$-{yPbTiO}$_{\textrm{3}}$ ceramics},
	volume = {45},
	issn = {0272-8842},
	url = {https://www.sciencedirect.com/science/article/pii/S0272884219310296},
	doi = {10.1016/j.ceramint.2019.04.204},
	abstract = {Ceramics of seven quasi-binary concentration sections of the ternary solid solution system (1-x-y)BiFeO3-xPbFe0.5Nb0.5O3-yPbTiO3 were prepared by the conventional solid-phase reaction method in the range of 0.05 ≤ x ≤ 0.325; 0.05 ≤ y ≤ 0.325. By using x-ray diffraction technique, the phase diagram of the system was constructed which was shown to contain the regions of tetragonal and rhombohedral symmetry and the morphotropic phase boundary between them. Grain morphology, dielectric and piezoelectric properties of selected solid solutions were investigated. The highest piezoelectric coefficient d33 = 50 pC/N was obtained. Dielectric characteristics of ceramics revealed ferroelectric relaxor behavior and region of diffuse phase transition from the paraelectric to ferroelectric phase in the temperature range of 600–800 K.},
	number = {12},
	urldate = {2023-11-11},
	journal = {Ceramics International},
	author = {Boldyrev, N. A. and Pavlenko, A. V. and Shilkina, L. A. and Nazarenko, A. V. and Bokov, A. A. and Reznichenko, L. A. and Rudskaya, A. G. and Panchenko, E. I.},
	month = aug,
	year = {2019},
	keywords = {Dielectric properties, Perovskites multiferroics, Piezoelectric properties, Solid solutions},
	pages = {14768--14774},
	file = {ScienceDirect Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\FR6CF252\\S0272884219310296.html:text/html},
}



@article{kabirov_piezoresistance_2019,
	title = {Piezoresistance and magnetoresistance of composites based on manganite {La}$_{\textrm{0.7}}${Sr}$_{\textrm{0.3}}${MnO}$_{\textrm{3}}$},
	volume = {9},
	issn = {2218-5046},
	url = {https://lettersonmaterials.com/en/Readers/Article.aspx?aid=15201},
	doi = {10.22226/2410-3535-2019-2-223-227},
	abstract = {The development of new sensitive multifunctional materials, which simultaneously react both to mechanical pressure and a constant magnetic field, is one of challenges of the modern materials science. In order to create materials that can simultaneously possess extrinsic piezoresistance and magnetoresistance, polymer composites based on La0.7Sr0.3MnO3 (LSMO) and low density polyethylene (LDPE) of composition (100‑x)LSMO / xLDPE at x = 7, 8, 9, 12, 15, 17, 18, 22 mass percent have been synthesized in this work. The composites have been synthesized at 170°C and a pressure of 50 MPa in the presence of hydrocarbons. The phase composition of the obtained samples has been studied by X-ray diffraction and infrared spectroscopy. Electric, piezoresistance and magnetoresistance properties of the samples have been studied. It has been found out that with increasing concentration of polyethylene, the electrical resistance of the samples also increases. It has been established that the percolation threshold of the composites is about 13 wt.\% of polyethylene. A maximum is observed in the dependence of the electrical resistance of the samples on the uniaxial pressure at a concentration of polyethylene near the percolation threshold at x =15 wt.\%. Samples with concentration of x =15 wt.\% of low density polyethylene show extrinsic piezoresistance of about 17 \% in the pressure range 0 – 270 kPa. Significant hysteresis is observed when considering the dependence of piezoresistance on pressure for all samples. The pressure sensitivity for a sample of 85 \%LSMO / 15 \%LDPE reaches 8.40 mΩ / Pa. The maximum values of the negative isotropic tunnel magnetoresistance of the composites 88 \%LSMO / 12 \%LDPE have values of about 2 \% in a 15 kOe magnetic field. We believe that the materials studied in the paper could be useful for designing multifunctional biosensors of mechanical pressure and constant magnetic field.},
	language = {en},
	number = {2},
	urldate = {2023-11-11},
	journal = {Letters on Materials},
	author = {Kabirov, Y. V. and Bogatin, A. S. and Sidorenko, E. N. and Belokobylsky, M. V. and Mikheikin, A. S. and Letovaltsev, A. O. and Bulanova, A. L. and Prutsakova, N. V.},
	month = may,
	year = {2019},
	note = {Publisher: Letters on Materials},
	pages = {223--227},
	file = {Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\KQGQ4KDV\\Kabirov и др. - 2019 - Piezoresistance and magnetoresistance of composite.pdf:application/pdf},
}



@article{hanani_phase_2019,
	title = {Phase transitions, energy storage performances and electrocaloric effect of the lead-free {Ba}$_{\textrm{0.85}}${Ca}$_{\textrm{0.15}}${Zr}$_{\textrm{0.10}}${Ti}$_{\textrm{0.90}}${O}$_{\textrm{3}}$ ceramic relaxor},
	volume = {30},
	issn = {1573-482X},
	url = {https://doi.org/10.1007/s10854-019-00946-5},
	doi = {10.1007/s10854-019-00946-5},
	abstract = {Lead-free Ba0.85Ca0.15Zr0.10Ti0.90O3 (BCZT) ceramic exhibits excellent dielectric, ferroelectric and piezoelectric properties at the morphotropic phase boundary (MPB). Previously, we demonstrated that the use of the anionic surfactant sodium dodecyl sulfate (SDS, NaC12H25SO4) could enhance the dielectric properties of BCZT ceramic using surfactant-assisted solvothermal processing [1]. In the present study, structural, dielectric, ferroelectric properties, as well as electrocaloric effect and energy storage performances of this BCZT ceramic were thoroughly investigated. X-ray diffraction (XRD) measurements revealed the presence of single perovskite phase at room temperature with the coexistence of orthorhombic and tetragonal symmetries. In-situ Raman spectroscopy results confirmed the existence of all phase transitions from rhombohedral through orthorhombic and tetragonal to cubic symmetries when the temperature varies as reported in undoped-BaTiO3. Evolution of energy storage performances with temperature have been investigated. BCZT ceramic exhibits a high energy storage efficiency of {\textasciitilde} 80\% at 120 °C. In addition, the electrocaloric responsivity was found to be 0.164 × 10−6 K·m/V at 363 K.},
	language = {en},
	number = {7},
	urldate = {2023-11-11},
	journal = {Journal of Materials Science: Materials in Electronics},
	author = {Hanani, Zouhair and Mezzane, Daoud and Amjoud, M’barek and Razumnaya, Anna G. and Fourcade, Sébastien and Gagou, Yaovi and Hoummada, Khalid and El Marssi, Mimoun and Gouné, Mohamed},
	month = apr,
	year = {2019},
	pages = {6430--6438},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\8NW2JEKW\\Hanani и др. - 2019 - Phase transitions, energy storage performances and.pdf:application/pdf},
}



@article{shirokov_phase_2019,
	title = {Phase transitions in {Bi}$_{\textrm{4}}${Ti}$_{\textrm{3}}${O}$_{\textrm{12}}$},
	volume = {75},
	copyright = {Copyright (c) 2019 International Union of Crystallography},
	issn = {2052-5206},
	url = {https://journals.iucr.org/b/issues/2019/06/00/dq5041/},
	doi = {10.1107/S2052520619011843},
	abstract = {A Landau-type phase diagram describing the temperature phase transitions in the layered perovskite ferroelectric Bi4Ti3O12 is constructed.},
	language = {en},
	number = {6},
	urldate = {2023-11-11},
	journal = {Acta Crystallographica Section B: Structural Science, Crystal Engineering and Materials},
	author = {Shirokov, V. B. and Talanov, M. V.},
	month = dec,
	year = {2019},
	note = {Number: 6
Publisher: International Union of Crystallography},
	pages = {978--986},
}



@article{kuriganova_investigation_2019,
	title = {{INVESTIGATION} {OF} {STRUCTURAL}, {MICROSTRUCTURAL} {AND} {ELECTROCHEMICAL} {CHARACTERISTICS} {OF} {Pt}/{SnO}$_{\textrm{x}}$-{C} {ELECTROCATALYSTS} {PREPARED} {VIA} {ELECTROCHEMICAL} {DISPERSION} {OF} {TIN} {AND} {PLATINUM}},
	volume = {62},
	issn = {2500-3070},
	url = {http://ctj-isuct.ru/article/view/1551},
	doi = {10.6060/ivkkt.20196209.5945},
	abstract = {Аннотация
					Порошки оксидов олова (SnOx) с различной структурой и составом и Pt/SnOx-C электрокатализаторы для топливных элементов с прямым окислением этанола были получены путем электрохимического диспергирования оловянных и платиновых электродов под действием импульсного переменного тока с использованием электролитов с различными типами анионов (Cl- и F-). Полученные порошки оксидов олова, композиционные носители SnOx-C и катализаторы Pt/SnOx-C были исследованы различными методами: рентгеновская дифракция, рамановская спектроскопия, сканирующая и просвечивающая электронная микроскопия. Наночастицы SnO2 со средним размером 5 - 8 нм были синтезированы в Cl- -содержащем растворе. В свою очередь, было обнаружено, что во F- - содержащем электролите были получены наночастицы SnO с выраженной анизотропией формы и размером частиц. Полученные оксиды олова использовались в качестве предшественников в синтезе Pt/SnOx-C катализаторов (загрузка Pt 20\%, D111 = 10,5-13,5 нм) также с применением технологии электрохимического диспергирования под действием импульсного переменного тока. Электрохимически активная площадь поверхности Pt/SnOx-C электрокатализаторов, определенная методом окислительной десорбции CO, составляла 13-15 м2г-1. Электрокаталитическую активность электрокатализаторов изучали для реакции электрохимического окисления этанола методами циклической вольтамперометрии с использованием вращающегося дискового электрода. Было обнаружено, что присутствие оксидов олова оказывает одинаковое влияние на реакции электрохимического окисления СО и этанола независимо от структурных особенностей их частиц.
{\textless}span style="opacity: 0;"{\textgreater} . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . {\textless}/span{\textgreater}},
	language = {ru-RU},
	number = {9},
	urldate = {2023-11-11},
	journal = {ИЗВЕСТИЯ ВЫСШИХ УЧЕБНЫХ ЗАВЕДЕНИЙ. СЕРИЯ «ХИМИЯ И ХИМИЧЕСКАЯ ТЕХНОЛОГИЯ»},
	author = {Kuriganova, Alexandra B. and Smirnova, Nina V. and Leontyev, Igor N. and Avramenko, Marina V.},
	month = aug,
	year = {2019},
	keywords = {Pt/C, оксиды олова, топливный элемент, электроокисление этанола, электрохимическое диспергирование},
	pages = {53--59},
	file = {Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\VKA94EMJ\\Kuriganova и др. - 2019 - INVESTIGATION OF STRUCTURAL, MICROSTRUCTURAL AND E.pdf:application/pdf},
}



@article{ulyankina_electrochemical_2019,
	title = {Electrochemical {Synthesis} of {TiO}$_{\textrm{2}}$ under {Pulse} {Alternating} {Current}: {Effect} of {Thermal} {Treatment} on the {Photocatalytic} {Activity}},
	volume = {4},
	copyright = {© 2019 Wiley-VCH Verlag GmbH \& Co. KGaA, Weinheim},
	issn = {2365-6549},
	shorttitle = {Electrochemical {Synthesis} of {TiO2} under {Pulse} {Alternating} {Current}},
	url = {https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201803367},
	doi = {10.1002/slct.201803367},
	abstract = {The current work aimed to study the effect of thermal treatment on the structural, optical, and photocatalytic properties of TiO2 nanoparticles synthesized by a novel large-scale electrochemical method using pulse alternating current (PAC). The obtained titania was characterized via XRD, TEM, XPS, UV-Vis DRS, PL, Raman and FTIR spectroscopy. The as-prepared TiO2 was found to be poorly crystallized and partly amorphous. Following thermal annealing, the anatase structure is developed at temperatures of 400–600 °C. The photoreactivity of the TiO2 nanoparticles was evaluated for the degradation of methylene blue (MB) and rhodamin B (RhB) dyes under UVA irradiation. As shown, the adsorption properties and photocatalytic activity of the as-prepared TiO2 strongly depend on the chemical nature of the dye. The enhanced photocatalytic performance for the MB and RhB degradation was observed for the sample annealed at 400 °C, which coincides with a balance between the degree of crystallinity, specific surface area, optical properties and efficiency of electron-hole pair separation.},
	language = {en},
	number = {6},
	urldate = {2023-11-11},
	journal = {ChemistrySelect},
	author = {Ulyankina, Anna and Avramenko, Marina and Kusnetsov, Denis and Firestein, Konstantin and Zhigunov, Denis and Smirnova, Nina},
	year = {2019},
	note = {\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/slct.201803367},
	keywords = {crystallinity, dye, electrochemical synthesis, photocatalysis, titanium dioxide},
	pages = {2001--2007},
	file = {Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\NQTKT7VJ\\slct.html:text/html},
}



@article{__2019-3,
	title = {Температурная зависимость фононных и магнонных мод в гетероструктурах мультиферроик - сегнетоэлектрик},
	issn = {2500-0640},
	url = {https://www.libnauka.ru/item.php?doi=10.7868/S25000640190103},
	doi = {10.7868/S25000640190103},
	abstract = {Пленки феррита висмута BiFeO выращены на монокристаллической подложке (001) MgO по блочному механизму роста методом высокочастотного катодного распыления с использованием в качестве буферного слоя сегнетоэлектрика BaSr \_ TiO при варьировании состава x. Изучение гетероструктур методом рентгеновской дифракции показало, что пленки характеризуются псевдотетрагональной симметрией при комнатной температуре. Определено, что степень тетрагонального искажения слоев BaSr \_ TiO возрастает с увеличением концентрации Ba, в то время как в слоях BiFeO она остается практически неизменной. Методом атомно-силовой микроскопии установлено, что пленки BiFeOвыросли по блочному механизму роста, причем блоки строго ориентированы относительно друг друга и кристаллографических осей подложки MgO. Высокотемпературные исследования спектров комбинационного рассеяния света в широком диапазоне температур 295-900 K и частот от 50 до 1600 смпоказали, что интенсивность полосы 1250 см, соответствующей плотности состояний двухмагнонных возбуждений, линейно понижается при повышении температуры. Анализ температурного поведения полосы 1250 см позволяет предполагать, что в изученных пленках BiFeO антиферромагнитный фазовый переход происходит в диапазоне температур 600-700 K. Использование сегнетоэлектрических буферных слоев BaSr \_ TiO с разной степенью тетрагонального искажения позволяет управлять деформацией пленок BiFeO, возникающей в результате несоответствия параметров решеток в смежных слоях, и тем самым искусственно варьировать свойства данных структур.},
	language = {ru},
	number = {1},
	urldate = {2023-11-11},
	journal = {Science in the South of Russia},
	author = {Бабарикин, Д.С. and Разумная, А.Г. and Стрюков, Д.В. and Анохин, А.С. and Михейкин, А.С. and Павленко, А.В. and Широков, В.Б. and Зинченко, С.П. and Мухортов, В.М.},
	year = {2019},
	pages = {21--30},
	file = {Бабарикин и др. - 2019 - Температурная зависимость фононных и магнонных мод.pdf:C\:\\Users\\aleks\\Zotero\\storage\\2GW49MUE\\Бабарикин и др. - 2019 - Температурная зависимость фононных и магнонных мод.pdf:application/pdf},
}



@article{maslova_characterization_2019,
	title = {Characterization of an {UO}$_{\textrm{2}}$ ceramic via {Raman} imaging and electron back-scattering diffraction},
	volume = {147},
	issn = {1044-5803},
	url = {https://www.sciencedirect.com/science/article/pii/S1044580318315651},
	doi = {10.1016/j.matchar.2018.11.006},
	abstract = {A surface state analysis of an UO2 ceramic is performed by combining Raman imaging and electron back-scattering diffraction. Special attention is paid to the behavior of the T2g band intensity versus the crystalline orientation. In order to clarify the origin of the T2g intensity variation in the appropriate Raman image, electron back-scattering diffraction (EBSD) measurements are carried out. EBSD data allow a theoretical estimation of the Raman T2g band intensities. Both maps have been compared in order to correlate them, and to distinguish regions where they are analogous, from those where some physical or chemical effects (stoichiometry, or strains) induce different behavior. More generally, this highlights the interest and the complementarity of combining Raman spectroscopy and EBSD for a better microstructure knowledge.},
	urldate = {2023-11-11},
	journal = {Materials Characterization},
	author = {Maslova, O. A. and Iltis, X. and Desgranges, L. and Ammar, M. R. and Genevois, C. and de Bilbao, E. and Canizarès, A. and Barannikova, S. A. and Leontyev, I. N. and Simon, P.},
	month = jan,
	year = {2019},
	keywords = {Crystalline orientation, Crystallographic indices, EBSD, Euler angles, Pole figures, Raman imaging, T band, UO},
	pages = {280--285},
	file = {ScienceDirect Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\IZ29TZSV\\S1044580318315651.html:text/html},
}



@article{k__2008,
	title = {{СТРУКТУРА} И ОПТИЧЕСКИЕ СВОЙСТВА {ZnO}-НАНОКРИСТАЛЛОВ, ПОЛУЧЕННЫХ МЕТОДОМ ИМПУЛЬСНОГО ЛАЗЕРНОГО НАПЫЛЕНИЯ НА ПЛЕНКАХ {GaN}/{Si}(111) С ИСПОЛЬЗОВАНИЕМ {Au}- И {NiO}-КАТАЛИЗАТОРОВ},
	volume = {72},
	issn = {0367-6765},
	url = {https://www.elibrary.ru/item.asp?id=11036052},
	abstract = {Исследован рост ZnO-нанокристаллов на пленочном подслое GaN/Si(111) методом импульсного лазерного напыления при высоком давлении аргона с использованием Au- и NiO-катализаторов. Использование низкотемпературного NiO-катализатора позволяет снизить оптимальную температуру роста с 900°C (в случае Au-катализатора) до T = 570°C и вырастить высокоориентированные в направлении оси c решетки ZnO-нанокристаллов диаметром 20 нм полностью свободных от дислокаций.},
	language = {ru},
	number = {8},
	urldate = {2023-11-11},
	journal = {Известия Российской Академии Наук. Серия Физическая},
	author = {Kайдашев, E. M. and Lorenz, M. and Lenzner, J. and Ramm, A. and Nobis, T. and Grundmann, M. and Zakharov, N. and Козаков, А. Т. and Шевцова, С. И. and Абдулвахидов, К. Г. and Кайдашев, В. Е.},
	year = {2008},
	keywords = {⛔ No DOI found},
	pages = {1195--1197},
}



@inproceedings{nazarenko_structure_2017,
	title = {{THE} {STRUCTURE} {AND} {PARAMAGNETISM} {OF} (1-x){BiFeO}$_{\textrm{3}}$ – {xYMnO}$_{\textrm{3}}$ {SOLID} {SOLUTIONS}},
	url = {https://elibrary.ru/item.asp?id=30471203},
	abstract = {In solid solutions of (1–x)BiFeO 3 –xYMnO 3 around x = 0.5 the monoclinic phase with C2 symmetry is detected. It was found that the Lande parameter values of the electronic paramagnetic resonance signals (g-factors) of compositions with 0 {\textless} x {\textless} 0.8 differ from g-factor of the free electron (g e = 2.0023) and depend on concentration of x with the maximum value for x = 0.5. Also paramagnetic parameters correlate with bond lengths and angles between Fe/Mn-centred octahedron in the perovskite structures.},
	language = {en},
	urldate = {2023-11-11},
	author = {Nazarenko, A. V. and Zaletov, V. G. and Kabirov Yu.v. and Chagovets, S. V. and Ananyeva, E. V. and Rudskaya, A. G. and Kupriyanov, M. F.},
	year = {2017},
	keywords = {Perovskite, (1-X)bifeo3 -Xymno3, Bifeo3, Epr, Multiferroics, Xrd, Ymno3, ⛔ No DOI found},
}



@article{kadyrov_terahertz_2017,
	title = {Terahertz spectroscopy of low-energy excitations in {Eu}$_{\textrm{0.42}}${Sr}$_{\textrm{0.58}}${MnO}$_{\textrm{3}}$},
	volume = {96},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.96.245120},
	doi = {10.1103/PhysRevB.96.245120},
	abstract = {The origin of low-energy excitations in the polycrystalline Eu0.42Sr0.58MnO3 manganite is explored by terahertz and infrared spectroscopies. The transition from the charge and/or orbital to antiferromagnetic order (TN=130−140K) is seen as smooth (spread over a temperature range from 50 to 100 K) decrease of free-carrier conductivity with the activation energy change from 86 meV (high temperatures) to 0.52 meV (low temperatures). A broad relaxation is observed at around 10cm−1 which we associate with the dynamics of free charge carriers in the presence of random localizing potential. We discover an absorption resonance at ≈50cm−1 below TN that is assigned to the formation of hybridized “acoustic phonon-magnon” quasiparticles.},
	number = {24},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Kadyrov, L. S. and Zhukova, E. S. and Torgashev, V. I. and Zhang, T. and Gagkaeva, Z. V. and Dressel, M. and Gorshunov, B. P.},
	month = dec,
	year = {2017},
	note = {Publisher: American Physical Society},
	pages = {245120},
	file = {APS Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\GFXPT7MJ\\PhysRevB.96.html:text/html},
}



@inproceedings{chagovets_reconstructive_2017,
	title = {Reconstructive {Phase} {Transition} in {YMnO}$_{\textrm{3}}$ –{BiFeO}$_{\textrm{3}}$ {Solid} {Solutions}},
	url = {https://elibrary.ru/item.asp?id=30471067},
	abstract = {The structures of the (1–x)YMnO 3 –xBiFeO 3 (0.05 ≤ x ≤ 0.25) solid solutions have been studied by means of the X-ray diffraction method. It was established that in the compounds of the (1–x)YMnO 3 –xBiFeO 3 system the P6 3 cm, the Pbam and Pnma phases are observed at room temperature after annealing at T 1 = 950 °C. The results revealed that in the compounds of the (1–x)YMnO 3 –xBiFeO 3 system the P6 3 cm and Pnma phases take place at room temperature after annealing at T 2 = 1100 °C. The symmetry of the phases, the unit cell parameters, the positional atomic parameters have been determined.},
	language = {en},
	urldate = {2023-11-11},
	author = {Chagovets, S. V. and Nazarenko, A. V. and Kozarenko, S. S. and Rudskaya, A. G. and Kupriyanov, M. F.},
	year = {2017},
	keywords = {(1-X)bifeo 3 -Xymno 3, Multiferroic, Phase Transition, X-Ray Diffraction, ⛔ No DOI found},
}



@article{stryukov_lattice_2017,
	title = {Lattice dynamics and structural distortions in the multiferroic ({Ba},{Sr}){TiO}$_{\textrm{3}}$/({Bi},{Nd}){FeO}$_{\textrm{3}}$ heterostructures},
	volume = {636},
	issn = {0040-6090},
	url = {https://www.sciencedirect.com/science/article/pii/S0040609017304443},
	doi = {10.1016/j.tsf.2017.06.009},
	abstract = {We report the synthesis, the structure and phonon spectra studies of epitaxial double-layer heterostructures consisting of Bi0.98Nd0.02FeO3 and Ba0.8Sr0.2TiO3 layers deposited on (100) MgO substrates. The results of x-ray diffraction and the polarization characteristics of Raman spectra suggest a monoclinic symmetry of the systems at room temperature. The observed spectra demonstrate the non-monotonous dependence on the layer thickness that apparently can be related with specificity of the light propagation in the layered thin-film systems.},
	urldate = {2023-11-11},
	journal = {Thin Solid Films},
	author = {Stryukov, D. V. and Razumnaya, A. G. and Golovko, Yu I. and Anokhin, A. S. and Lukyanchuk, I. A. and Shirokov, V. B. and Mukhortov, V. M.},
	month = aug,
	year = {2017},
	keywords = {X-ray diffraction, Raman spectroscopy, Bismuth ferrite, Heterostructures, Lattice distortions, Lattice dynamics, Sputtering},
	pages = {220--224},
	file = {ScienceDirect Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\TD9K6CTD\\S0040609017304443.html:text/html},
}



@article{trotsenko_invar_2017,
	title = {Invar effect accompanying charge order in {La}$_{\textrm{0.25}}${Ca}$_{\textrm{0.75}}${MnO}$_{\textrm{3}}$},
	volume = {72},
	issn = {1293-2558},
	url = {https://www.sciencedirect.com/science/article/pii/S1293255817305381},
	doi = {10.1016/j.solidstatesciences.2017.08.020},
	abstract = {To determine the role of the Jahn-Teller effect in the orbital and charge ordering of mixed crystals of the strongly correlated La1-xCaxMnO3 system, we have used the diffraction of synchrotron radiation and the subsequent Rietveld analysis of diffraction patterns in order to obtain structural data for La0.25Ca0.75MnO3 compound in the temperature range from 90 to 325 K with a step of ∼2 K. For the first time for this compound, an Invar effect was observed below the charge-order temperature. In the entire temperature range, atomic displacements were analyzed and correlations between charge ordering and deformational modes were made, on the basis of which the secondary role of the Jahn-Teller effect in observed structure distortions was established. A hypothesis of a spin crossover in the vicinity of the charge-ordering temperature is proposed that describes adequately both the obtained structural data and the results of measurements of the macroscopic magnetic and elastic properties of the studied compound as well as related materials with charge ordering.},
	urldate = {2023-11-11},
	journal = {Solid State Sciences},
	author = {Trotsenko, V. G. and Mikheykin, A. S. and Shirokov, V. B. and Razumnaya, A. G. and El Marssi, M. and Gorshunov, B. P. and Bush, A. A. and Torgashev, V. I.},
	month = oct,
	year = {2017},
	keywords = {Charge ordering, Correlated electron systems, Invar effect, Spin crossover},
	pages = {144--149},
}



@article{mikheykin_fast_2017,
	title = {Fast proton conduction in {Cs}$_{\textrm{3}}$({HSO}$_{\textrm{4}}$)$_{\textrm{2}}$({H}$_{\textrm{2}}${PO}$_{\textrm{4}}$) and {Cs}$_{\textrm{4}}$({HSO}$_{\textrm{4}}$)$_{\textrm{3}}$({H}$_{\textrm{2}}${PO}$_{\textrm{4}}$)},
	volume = {305},
	issn = {0167-2738},
	url = {https://www.sciencedirect.com/science/article/pii/S0167273816307147},
	doi = {10.1016/j.ssi.2017.04.017},
	abstract = {X-ray powder diffraction studies were performed on Cs3(HSO4)2(H2PO4) and Cs4(HSO4)3(H2PO4) in the range 340–440K. For the both compounds a first order phase transition from the monoclinic C2/c phase to the mixture of cubic Pm-3m and tetragonal I41/amd superprotonic phases takes place at 408–414 and 412–414K respectively; the ratio between cubic and tetragonal depends on material and temperature. The tetragonal phase transforms to the cubic modification on heating and this transition is reversible.},
	urldate = {2023-11-11},
	journal = {Solid State Ionics},
	author = {Mikheykin, A. S. and Chernyshov, D. Yu. and Makarova, I. P. and Grebenev, V. V. and Komornikov, V. A. and Selezneva, E. V.},
	month = jul,
	year = {2017},
	keywords = {Solid solutions, Phase transition, Superprotonics, XRPD},
	pages = {30--35},
	file = {ScienceDirect Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\ZKIPJH5U\\S0167273816307147.html:text/html},
}



@article{kuriganova_electrochemically_2017,
	title = {Electrochemically synthesized {Pt}/{TiO}$_{\textrm{2}}$-{C} catalysts for direct methanol fuel cell applications},
	volume = {27},
	issn = {0959-9436},
	url = {https://www.sciencedirect.com/science/article/pii/S0959943617300214},
	doi = {10.1016/j.mencom.2017.01.021},
	abstract = {The Pt/TiO2-C catalysts with different TiO2 loadings have been prepared by electrochemical oxidation/dispersion, and their good catalytic activity in CO stripping and methanol electrooxidation reactions has been shown.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Mendeleev Communications},
	author = {Kuriganova, Alexandra B. and Leontyev, Igor N. and Alexandrin, Alexander S. and Maslova, Olga A. and Rakhmatullin, Aydar I. and Smirnova, Nina V.},
	month = jan,
	year = {2017},
	pages = {67--69},
}



@inproceedings{kozakov_crystal_2017,
	address = {Cham},
	series = {Springer {Proceedings} in {Physics}},
	title = {Crystal {Structure}, {Phase} and {Elemental} {Composition} and {Chemical} {Bonding} in {Bi}$_{\textrm{1−{X}}}${A}$_{\textrm{{X}}}${FeO}$_{\textrm{3±{Y}}}$ {Systems} ({A} = {Sr}, {Ca}; 0 ≤{X} ≤ 1) from {X}-ray {Diffraction}, {Mössbauer}, and {X}-ray {Photoelectron} {Spectra}},
	isbn = {978-3-319-56062-5},
	doi = {10.1007/978-3-319-56062-5_13},
	abstract = {An integrated study of samples of Bi1−xAxFeO3±y(A = Sr, Ca) systems for 0 ≤ x ≤ 1 (step 0.1) is performed using X-ray diffractionX-ray diffraction (XRD)(XRD), Mössbauer spectroscopy (MS), and X-ray photoelectron spectroscopyX-ray photoelectron spectroscopy (XPS)(XPS). Considerable deviations of actual elemental compositions from nominal ones in the samples of both systems are discovered. Both Fe3+ and Fe4+ ions are found to be present in the samples of the Bi1−xSrxFeO3±ysystem with x {\textgreater} 0. No Fe4+ ions are discovered upon substitution of Bi3+ by Ca2+ in Bi1−xCaxFeO3±y, neither by Mössbauer spectroscopy, nor by XPS. Charge compensation in Bi1−xCaxFeO3±ytakes place mostly via creation of oxygen vacancies.},
	language = {en},
	booktitle = {Advanced {Materials}},
	publisher = {Springer International Publishing},
	author = {Kozakov, A. T. and Kochur, A. G. and Torgashev, V. I. and Kubrin, S. P. and Trotsenko, V. G. and Bush, A. A. and Nikolskii, A. V.},
	editor = {Parinov, Ivan A. and Chang, Shun-Hsyung and Jani, Muaffaq A.},
	year = {2017},
	keywords = {Actual Elemental Composition, concentrationsConcentration, Mössbauer Spectroscopy, Octahedral Oxygen Environment, xCa xFeO},
	pages = {145--153},
}



@inproceedings{shirokov_acoustic_2016,
	title = {Acoustic properties of {BST0}$_{\textrm{8}}$ films tunable by bias electric field},
	url = {https://ieeexplore.ieee.org/document/7819084?reload=true},
	doi = {10.1109/Dynamics.2016.7819084},
	abstract = {The effect of a bias electric field on the material coefficients of Ba0.8Sr0.2O3 (BST08) thin films was studied. The material constants are derived from piezoelectric effect equations by the linearization of nonlinear phenomenological state equations. The numerical results are obtained for the case of BST08 film with a misfit strain value equal to −4×10−3 located on a cubic substrate for the (001) cut plane in the electric field up to 5×107V/m applied along [100] direction in the film plane. The electromechanical coupling coefficient k11 reaches a maximum under applied electric field.},
	urldate = {2023-11-11},
	booktitle = {2016 {Dynamics} of {Systems}, {Mechanisms} and {Machines} ({Dynamics})},
	author = {Shirokov, V. B and Kalinchuck, V. V. and Timoshenko, P. E. and Shirokov, V. B. and Timoshenko, P. E. and Yuzyuk, Yu. I.},
	month = nov,
	year = {2016},
	pages = {1--4},
}



@article{__2017-5,
	title = {Эффект поля в структуре металл - сегнетоэлектрик - полупроводник с использованием многослойного сегнетоэлектрика},
	volume = {13},
	issn = {2500-0640},
	url = {https://elibrary.ru/item.asp?id=28843943},
	doi = {10.23885/2500-0640-2017-13-1-18-24},
	abstract = {Одной из важнейших концепций использования сегнетоэлектрических гетероструктур в микроэлектронике является энергонезависимая память (FeRAM), где в качестве подзатворного диэлектрика в полевом транзисторе используется сегнетоэлектрическая пленка. Вторым важным применением сегнетоэлектрических пленок является их использование при создании принципиально новых микроэлектромеханических устройств (МЕМС). Реализация МЕМС с использованием сегнетоэлектрических наноразмерных пленок в качестве активного элемента по своим параметрам в десятки раз будет превосходить существующие аналоги. В последние годы вопросам стабильности поляризованного состояния и динамики переключения поляризации придается большое значение. В данной работе впервые приведены результаты по исследованию эффекта поля в структуре металл - сегнетоэлектрик - полупроводник, где в качестве сегнетоэлектрика использованы многослойные сегнетоэлектрические слои. Использование многослойных сегнетоэлектрических гетероструктур приводит к самосогласованию поверхностных состояний на границах полупроводник - сегнетоэлектрик и сегнетоэлектрик - сегнетоэлектрик с переключаемой под действием внешнего поля спонтанной поляризацией. Это позволяет создать устойчивое поляризованное состояние с незначительной ее релаксацией.},
	language = {ru},
	number = {1},
	urldate = {2023-11-11},
	journal = {Наука Юга России},
	author = {Стрюков, Д. В. and Мухортов, В. М. and Бирюков, С. В. and Головко, Ю. И.},
	year = {2017},
	keywords = {Двумерные Напряжения, Двухслойные Сегнетоэлектрики, Сегнетоэлектрическая Пленка, Структура, Эффект Поля},
	pages = {18--24},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\A5UM2STP\\Стрюков и др. - 2017 - Эффект Поля В Структуре Металл - Сегнетоэлектрик -.pdf:application/pdf},
}



@article{__2017-6,
	title = {Экспериментальное и теоретическое исследование оптических антенн на основе наностержней {ZnO} покрытых тонкой пленкой серебра},
	issn = {0033-8494},
	url = {https://www.libnauka.ru/item.php?doi=10.7868/S0033849417110055},
	doi = {10.7868/S0033849417110055},
	language = {ru},
	number = {12},
	urldate = {2023-11-11},
	journal = {Радиотехника и электроника},
	author = {Кайдашев, Е. М. and Лерер, А.М. and Головачева, Е. В. and Кайдашев, В. Е. and Лянгузов, Н.В. and Цветянский, Е. А.},
	year = {2017},
	pages = {1173--1181},
}



@article{__2017-7,
	title = {Структура, динамика решетки и диэлектрические характеристики пленок {Sr}$_{\textrm{0.5}}${Ba}$_{\textrm{0.5}}${Nb}$_{\textrm{2}}${O}$_{\textrm{6}}$},
	volume = {59},
	issn = {0367-3294},
	url = {https://journals.ioffe.ru/articles/44376},
	doi = {10.21883/FTT.2017.05.44376.382},
	abstract = {Методом высокочастотного напыления в атмосфере кислорода получены пленки твердого раствора Sr
              0.5
              Ba
              0.5
              Nb
              2
              O
              6
              на подложке (111)Pt/(001)Si. Изучены их деполяризованные спектры комбинационного рассеяния света, структура и диэлектрические характеристики в широком диапазоне температур. Установлено, что пленки однофазны, обладают структурой тетрагональной вольфрамовой бронзы, имеют ярко выраженную аксиальную текстуру с осью 001, направленной перпендикулярно поверхности подложки. Показано, что в интервале температур 300-425 K в материале пленки происходит размытый фазовый переход в состояние сегнетоэлектрика-релаксора. Обсуждаются возможные причины выявленных закономерностей. Работа выполнена в рамках реализации государственного задания на 2016 г N 007-01114-16 ПР (проект N 0256-2014-0002) и гранта РФФИ N 16-32-60095 мол{\textbackslash}\_а{\textbackslash}\_дк. DOI: 10.21883/FTT.2017.05.44376.382},
	language = {ru},
	number = {5},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Павленко, А.В. and Захарченко, И.Н. and Анохин, А.С. and Куприна, Ю.А. and Киселева, Л.И and Юзюк, Ю.И.},
	year = {2017},
	pages = {888},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\BGRS77V9\\Павленко и др. - 2017 - Структура, динамика решетки и диэлектрические хара.pdf:application/pdf},
}



@article{__2017-8,
	title = {Получение, структура и диэлектрические свойства керамики и тонких поликристаллических пленок {PbMg}$_{\textrm{1/3}}${Nb}$_{\textrm{2/3}}${O}$_{\textrm{3}}$ на подложке {Si}(001)},
	volume = {13},
	issn = {2500-0640},
	url = {https://elibrary.ru/item.asp?id=29946411},
	doi = {10.23885/2500-0640-2017-13-3-27-33},
	abstract = {Методом газоразрядного RF-напыления в атмосфере чистого кислорода осуществлено напыление пленок сегнетоэлектрика-релаксора PbMg1/3Nb2/3O3 (PMN) на подложки (001)Si (p-тип). PMN-пленки являются поликристаллическими с параметрами ячейки, близкими к объемному материалу PMN. Следов примесных фаз в обоих объектах не выявлено. Количественный анализ характеристического рентгеновского спектра образцов показал, что соотношение катионного состава по Pb и Nb в пленке соответствует составу распыляемой мишени. Проведены измерения температурно-частотных зависимостей относительной диэлектрической проницаемости (ε/ε0) и тангенса угла диэлектрических потерь (tg δ) керамики PMN. При комнатной температуре керамике свойственны высокие значения ε/ε0 ≈ 5500 и низкие tg δ ≈ 0,02, при этом дисперсия ε/ε0 в исследуемом диапазоне f отсутствовала, а температура Бёрнса составила ≈300 °С. При электронно-микроскопическом исследовании поверхности и скола гетероструктуры PMN/Si установлено, что пленка однофазная, поликристаллическая с характерным размером кристаллитов 50... 70 нм, при этом следов присутствия переходного слоя оксида кремния на границе раздела пленка - подложка не выявлено. Проведены исследования вольт-фарадных характеристик гетероструктуры PMN/Si. Обсуждаются причины выявленных аномалий.},
	language = {ru},
	number = {3},
	urldate = {2023-11-11},
	journal = {Наука Юга России},
	author = {Павленко, А. В. and Лянгузов, Н. В. and Новиковский, Н. В. and Смотраков, В. Г. and Ковтун, А. П.},
	year = {2017},
	keywords = {Диэлектрическая Проницаемость, Магнониобат Свинца, Релаксор, Тонкие Пленки},
	pages = {27--33},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\K4J6BNEW\\Павленко и др. - 2017 - ПОЛУЧЕНИЕ, СТРУКТУРА И ДИЭЛЕКТРИЧЕСКИЕ СВОЙСТВА КЕ.pdf:application/pdf},
}



@inproceedings{__2017-9,
	title = {Особенности фазового перехода в сегнетоэлектрической сверхрешетке {BaTiO}$_{\textrm{3}}$/{SrTiO}$_{\textrm{3}}$},
	url = {https://elibrary.ru/item.asp?id=29647718},
	language = {ru},
	urldate = {2023-11-11},
	publisher = {Российский государственный педагогический университет им. А. И. Герцена},
	author = {Разумная, А. Г. and Горьковая, Е. Д. and Тихонов, Ю. А.},
	year = {2017},
	keywords = {⛔ No DOI found},
}



@inproceedings{__2017-10,
	title = {Оптические Свойства Тонких Пленок {BSn50}},
	url = {https://elibrary.ru/item.asp?id=29401602},
	language = {ru},
	urldate = {2023-11-11},
	publisher = {Российский государственный педагогический университет им. А. И. Герцена},
	author = {Широков, В. Б. and Павленко, А. В. and Михейкин, А. С. and Изюмский, К. С. and Ревинский, Ю. В.},
	year = {2017},
	keywords = {⛔ No DOI found},
}



@inproceedings{__2017-11,
	title = {Многослойные структуры мультиферроик-сегнетоэлектрик: КРС исследования},
	shorttitle = {Многослойные Структуры Мультиферроик-Сегнетоэлектрик},
	url = {https://elibrary.ru/item.asp?id=29647696},
	language = {ru},
	urldate = {2023-11-11},
	publisher = {Российский государственный педагогический университет им. А. И. Герцена},
	author = {Анохин, А. С. and Разумная, А. Г. and Головко, Ю. И. and Мухортов, В. М.},
	year = {2017},
	keywords = {⛔ No DOI found},
}



@inproceedings{__2017-12,
	title = {Магнитодиэлектрические свойства керамики {LSMO}/{GeO}$_{\textrm{2}}$},
	url = {https://elibrary.ru/item.asp?id=29647737},
	language = {ru},
	urldate = {2023-11-11},
	publisher = {Российский государственный педагогический университет им. А. И. Герцена},
	author = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Богатин, А. С. and Яценко, В. К. and Пруцакова, Н. В. and Чебанова, Е. В.},
	year = {2017},
	keywords = {⛔ No DOI found},
}



@article{__2017-13,
	title = {Динамика решетки в пленках ниобата бария-стронция \textit{Т }= 300-700 К},
	volume = {13},
	issn = {2500-0640},
	url = {https://elibrary.ru/item.asp?id=29760083},
	doi = {10.23885/2500-0640-2017-13-2-21-28},
	abstract = {Методом газоразрядного RF-напыления в атмосфере чистого кислорода осуществлено напыление пленки твердого раствора сегнетоэлектрика-релаксора Ba0,5Sr0,5Nb2O6 (BSN-50) на предварительно подготовленную подложку (111)Pt/(001)Si. Пленке BSN-50 свойственна аксиальная текстура, основные элементы (Ba, Sr, Nb) по ее толщине распределены равномерно, а количественный анализ характеристического рентгеновского спектра показал, что соотношение катионного состава соответствует составу BSN-50. При исследовании температурных зависимостей относительной диэлектрической проницаемости (ε′/ε0) и остаточной поляризации (PR) гетероструктуры Al/BSN-50/Pt/Si установлено, что фазовый переход из сегнетоэлектрической в параэлектрическую фазу достаточно сильно размыт (ширина максимума ε′/ε0(Тm) на полувысоте ΔT = 263 K) и происходит при температуре {\textasciitilde}427 К, намного превышающей температуру максимума диэлектрической проницаемости Tm = 334 K...

Методом газоразрядного RF-напыления в атмосфере чистого кислорода осуществлено напыление пленки твердого раствора сегнетоэлектрика-релаксора Ba0,5Sr0,5Nb2O6 (BSN-50) на предварительно подготовленную подложку (111)Pt/(001)Si. Пленке BSN-50 свойственна аксиальная текстура, основные элементы (Ba, Sr, Nb) по ее толщине распределены равномерно, а количественный анализ характеристического рентгеновского спектра показал, что соотношение катионного состава соответствует составу BSN-50. При исследовании температурных зависимостей относительной диэлектрической проницаемости (ε′/ε0) и остаточной поляризации (PR) гетероструктуры Al/BSN-50/Pt/Si установлено, что фазовый переход из сегнетоэлектрической в параэлектрическую фазу достаточно сильно размыт (ширина максимума ε′/ε0(Тm) на полувысоте ΔT = 263 K) и происходит при температуре {\textasciitilde}427 К, намного превышающей температуру максимума диэлектрической проницаемости Tm = 334 K. В диапазоне температур 300-700 K методом спектроскопии комбинационного рассеяния света изучена динамика решетки пленки BSN-50. Наибольший вклад в интенсивность спектра пленки BSN вносят три широкие полосы в районе 230 cm-1, 630 cm-1 и 850 cm-1, каждая из которых состоит из набора линий (всего 13 мод). Температурная зависимость частоты и полуширины полосы 630 cm-1 в спектре комбинационного рассеяния пленки BSN показывают четкую аномалию при сегнетоэлектрическом фазовом переходе.},
	language = {ru},
	number = {2},
	urldate = {2023-11-11},
	journal = {Наука Юга России},
	author = {Анохин, А. С. and Лянгузов, Н. В. and Павленко, А. В.},
	year = {2017},
	keywords = {Диэлектрическая Проницаемость, Пленки, Спектроскопия Крс},
	pages = {21--28},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\TM7MF7DI\\Анохин и др. - 2017 - ДИНАМИКА РЕШЕТКИ В ПЛЕНКАХ НИОБАТА БАРИЯ - СТРОНЦИ.pdf:application/pdf},
}



@article{baudry_dynamics_2015,
	title = {Dynamics of field-induced polarization reversal in thin strained perovskite ferroelectric films with \textit{с}-oriented polarization},
	volume = {91},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.91.144110},
	doi = {10.1103/PhysRevB.91.144110},
	abstract = {The field-induced polarization reversal in the c-oriented ferroelectric phase of strained perovskite film has been studied. We show that in addition to the conventional longitudinal switching mechanism, when the c-oriented polarization vector changes its modulus, the longitudinal-transversal and transversal mechanisms when the perpendicular component of polarization is dynamically admixed are possible. The latter process can occur either via the straight-abrupt or initially continues polarization turnover scenario. We specified the obtained results for the case of PbTiO3 and BaTiO3 ferroelectrics and propose the experimental methods for their investigation.},
	number = {14},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Baudry, Laurent and Luk'yanchuk, Igor A. and Razumnaya, Anna},
	month = apr,
	year = {2015},
	note = {Publisher: American Physical Society},
	pages = {144110},
	file = {Отправленная версия:C\:\\Users\\aleks\\Zotero\\storage\\TC6IA8BZ\\Baudry и др. - 2015 - Dynamics of field-induced polarization reversal in.pdf:application/pdf},
}



@article{__2017-14,
	title = {Вынужденный пироэффект в планарном поле},
	volume = {59},
	issn = {0367-3294},
	url = {https://journals.ioffe.ru/articles/44377},
	doi = {10.21883/FTT.2017.05.44377.397},
	abstract = {Исследованы действие вынужденной деформации и влияние планарного электрического поля на основное состояние сегнетоэлектрических тонких пленок Ba0.7Sr0.3O3, осажденных на (001)-ориентированные кубические подложки. Для значений вынужденной деформации, соответствующих различным основным состояниям, построена зависимость пироэлектрического коэффициента от величины электрического поля Ex в плоскости пленки. В областях, где пленка может работать в режиме диэлектрического болометра, наблюдается значение поля, при котором пирокоэффициент достигает экстремального значения. Существует значение вынужденной деформации, при котором пироэффект проявляется наиболее ярко. Работа выполнена за счет средств Российского научного фонда (грант N 14-12-00258). DOI: 10.21883/FTT.2017.05.44377.397},
	language = {ru},
	number = {5},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Широков, В.Б. and Разумная, А.Г. and Юзюк, Ю.И.},
	year = {2017},
	pages = {892},
	file = {Полный текст:C\:\\Users\\aleks\\Zotero\\storage\\WFDZMDZ3\\Широков и др. - 2017 - Вынужденный пироэффект в планарном поле.pdf:application/pdf},
}



@article{talanov_theory_2016,
	title = {Theory of the formation of {P}$_{\textrm{4{\textless}sub{\textgreater}1}}$32{\textless}/sub{\textgreater}({P}$_{\textrm{4{\textless}sub{\textgreater}3}}$32{\textless}/sub{\textgreater})-phase spinels},
	volume = {61},
	issn = {1562-689X},
	url = {https://doi.org/10.1134/S1063774516020280},
	doi = {10.1134/S1063774516020280},
	abstract = {A group-theoretical, thermodynamic, and structural study of the formation of P4132(P4332) spinel modification has been performed. In particular, the occurrence of unique hyper-kagome atomic order is analyzed. The critical order parameter inducing a phase transition is established. It is shown that the calculated structure of the low-symmetry P4132(P4332) phase is formed as a result of displacements of atoms of all types and due to the cation and anion ordering. The problem of the occurrence of unique hyper-kagome atomic order in the structures of P4132(P4332) spinel modifications is considered theoretically. It is proven within the Landau theory of phase transitions that the P4132(P4332) phase can be formed from the high-symmetry Fd3m phase with an ideal spinel structure only as a result of first-order phase transition. Therefore, the formation of hyper-kagome sublattice in the P4132(P4332) phase is accompanied by a significant transformation of the spinel structure.},
	language = {en},
	number = {2},
	urldate = {2023-11-11},
	journal = {Crystallography Reports},
	author = {Talanov, V. M. and Talanov, M. V. and Shirokov, V. B.},
	month = mar,
	year = {2016},
	keywords = {Crystallography Report, Ible Representation, Multicritical Point, Spinel Structure, Unusual Physical Property},
	pages = {159--169},
}



@article{makarova_structure_2016,
	title = {Structure of {Cs}$_{\textrm{4}}$({HSO}$_{\textrm{4}}$)$_{\textrm{3}}$({H}$_{\textrm{2}}${PO}$_{\textrm{4}}$) single crystals},
	volume = {61},
	issn = {1562-689X},
	url = {https://doi.org/10.1134/S1063774516010119},
	doi = {10.1134/S1063774516010119},
	abstract = {Single crystals of Cs4(HSO4)3(H2PO4) are synthesized and studied for the first time. The new compound is found in the course of studies of the phase diagram of the CsHSO4–CsH2PO4–H2O triple system. Data on the atomic crystal structure of single-crystalline and powder specimens, as well as on structural phase transitions, are obtained.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Crystallography Reports},
	author = {Makarova, I. P. and Grebenev, V. V. and Vasil’ev, I. I. and Dmitricheva, E. V. and Komornikov, V. A. and Dolbinina, V. V. and Mikheikin, A. S.},
	month = jan,
	year = {2016},
	keywords = {Crystallography Report, High Protonic Conductivity, Potassium Atom, Structural Phase Transition, Thermal Vibration},
	pages = {18--23},
}



@article{shirokov_physical_2016-1,
	title = {Physical properties of {Ba}$_{\textrm{0.8}}${Sr}$_{\textrm{0.2}}${TiO}$_{\textrm{3}}$ thin films},
	volume = {58},
	issn = {1090-6460},
	url = {https://doi.org/10.1134/S1063783416100346},
	doi = {10.1134/S1063783416100346},
	abstract = {The behavior of material constants in ferroelectric Ba0.8Sr0.2TiO3 thin films is studied depending on the misfit strain at room temperature in the context of nonlinear thermodynamic potential of the phenomenological theory. Some constants are found to undergo drastic changes with the alternating strain at the interfaces. The gathered results allow one to evaluate the material constants for a specific film and to outline the direction in searching the ways to synthesize films with the needed properties.},
	language = {en},
	number = {10},
	urldate = {2023-11-11},
	journal = {Physics of the Solid State},
	author = {Shirokov, V. B. and Kalinchuk, V. V. and Shakhovoi, R. A. and Yuzyuk, Yu. I.},
	month = oct,
	year = {2016},
	pages = {2035--2039},
}



@article{razumnaya_phase_2016,
	title = {Phase transition in ferroelectric {BaTiO}$_{\textrm{3}}$/{SrTiO}$_{\textrm{3}}$ superlattice: {Raman} spectroscopy studies},
	volume = {501},
	issn = {0015-0193},
	shorttitle = {Phase transition in ferroelectric {BaTiO3}/{SrTiO3} superlattice},
	url = {https://doi.org/10.1080/00150193.2016.1199201},
	doi = {10.1080/00150193.2016.1199201},
	abstract = {BaTiO3/SrTiO3 superlattice has been grown on (001)MgO substrate by pulsed laser deposition. The unit cell parameters of BaTiO3 and SrTiO3 layers and modulation period have been determined using X-ray diffraction. It was found that BaTiO3 and SrTiO3 layers revealed the pseudo-tetragonal distortion with out-of-plane and in-plane polarization, respectively. Electrostatic interaction of the alternating layers leads to the polarization rotations and to the symmetry lowering of the superlattice to orthorhombic or monoclinic with partial depolarization of the Raman spectra. It was found that the phase transition to the paraelectric phase occurs at ∼480 K.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Ferroelectrics},
	author = {Razumnaya, A. G. and Yuzyuk, Yu. I. and Zakharchenko, I. N. and Tikhonov, Yu. A. and Ortega, N. and Kumar, A. and Katiyar, R. S. and El Marssi, M. and Lukyanchuk, I. A.},
	month = sep,
	year = {2016},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/00150193.2016.1199201},
	keywords = {Raman spectroscopy, soft mode, superlattices},
	pages = {61--69},
}



@article{makarova_mmhnxo4m_2016,
	title = {M$_{\textrm{m}}${H}$_{\textrm{n}}$({XO}$_{\textrm{4}}$)$_{\textrm{(m + n)/2}}$ crystals: structure, phase transitions, hydrogen bonds, conductivity. {II}. {Structure} and properties of {Cs}$_{\textrm{3}}$({HSO}$_{\textrm{4}}$)$_{\textrm{2}}$({H}$_{\textrm{2}}${PO}$_{\textrm{4}}$) and {Cs}$_{\textrm{4}}$({HSO}$_{\textrm{4}}$)$_{\textrm{3}}$({H}$_{\textrm{2}}${PO}$_{\textrm{4}}$) single crystals},
	volume = {72},
	copyright = {Copyright (c) 2016 International Union of Crystallography},
	issn = {2052-5206},
	shorttitle = {{MmHn}({XO4})(m + n)/2 crystals},
	url = {http://scripts.iucr.org/cgi-bin/paper?bp5085},
	doi = {10.1107/S2052520615023069},
	abstract = {Cs3(HSO4)2(H2PO4) and Cs4(HSO4)3(H2PO4) single crystals were obtained for the first time based on a systematic study of the phase diagram of the CsHSO4–CsH2PO4–H2O ternary system. To reveal the structural conditionality for anomalies in physical properties, including dielectric and optical properties, diffraction studies of the crystal structure of Cs3(HSO4)2(H2PO4) and Cs4(HSO4)3(H2PO4) were performed, and their common structural features and differences were analyzed.},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Acta Crystallographica Section B: Structural Science, Crystal Engineering and Materials},
	author = {Makarova, I. and Grebenev, V. and Dmitricheva, E. and Vasiliev, I. and Komornikov, V. and Dolbinina, V. and Mikheykin, A.},
	month = feb,
	year = {2016},
	note = {Number: 1
Publisher: International Union of Crystallography},
	pages = {133--141},
}



@article{andreeva_domain_2016,
	title = {Domain structures and correlated out-of-plane and in-plane polarization reorientations in {Pb}({Zr}$_{\textrm{0.96}}${Ti}$_{\textrm{0.04}}$){O}$_{\textrm{3}}$ single crystal via piezoresponse force microscopy},
	volume = {6},
	issn = {2158-3226},
	url = {https://doi.org/10.1063/1.4962991},
	doi = {10.1063/1.4962991},
	abstract = {Pb(Zr1-xTix)O3 single crystal with a low titanium content (x = 4\%) was studied by the piezoresponse force microscopy (PFM) and X-ray diffraction (XRD). The XRD studies showed that the crystal faces are orthogonal to the principal cubic axes and confirmed the existence of an intermediate phase between the high-temperature paraelectric (PE) phase and the low-temperature antiferroelectric (AFE) one. A significant temperature hysteresis of phase transitions was observed by the XRD: On heating, the AFE state transforms into the intermediate one at about 373 K and the PE phase appears at 508 K, whereas on cooling the intermediate phase forms at 503 K and persists down to at least 313 K. The PFM investigation was focused on the intermediate phase and involved measurements of both out-of-plane and in-plane electromechanical responses of the (001)-oriented crystal face. The PFM images revealed the presence of polarization patterns switchable by an applied electric field, which confirms the ferroelectric character of the intermediate phase. Importantly, two types of regular domain structures were found, which differ by the spatial orientation of domain walls. The reconstruction of polarization configurations in the observed domain structures showed that one of them is a purely ferroelectric 180° structure with domain walls orthogonal to the crystal surface and parallel to one of the ⟨111⟩ pseudocubic directions. Another one is a ferroelectric-ferroelastic domain structure with the 71° walls parallel to the \{101\} or \{011\} crystallographic planes. Remarkably, this domain structure shows correlated out-of-plane and in-plane polarization reorientations after the poling with the aid of the microscope tip.},
	number = {9},
	urldate = {2023-11-11},
	journal = {AIP Advances},
	author = {Andreeva, N. V. and Pertsev, N. A. and Andronikova, D. A. and Filimonov, A. V. and Leontiev, N. G. and Leontyev, I. N. and Vakhrushev, S. B.},
	month = sep,
	year = {2016},
	pages = {095211},
	file = {Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\QV2ANVMG\\Andreeva и др. - 2016 - Domain structures and correlated out-of-plane and .pdf:application/pdf},
}



@article{googlev_determining_2016,
	title = {Determining the valence state of manganese ions in complex oxides {La}$_{\textrm{1–x}}${Ca}$_{\textrm{x}}${MnO}$_{\textrm{3}}$ (x = 0.5, 0.7, 0.85, and 0.9) based on {Mn2p} and {Mn3s} {X}-ray photoelectron spectra},
	volume = {80},
	issn = {1934-9432},
	url = {https://doi.org/10.3103/S1062873816060125},
	doi = {10.3103/S1062873816060125},
	abstract = {The valence state of manganese ions in complex oxides La1–xCaxMnO3 (x = 0.5, 0.7, 0.85, and 0.9) is studied on the basis of Mn2p and Mn3s X-ray photoelectron spectra. It is shown that manganese ions have the valence of Mn3+ and Mn4+ in the studied compounds. The relative Mn3+/Mn4+ content is determined.},
	language = {en},
	number = {6},
	urldate = {2023-11-11},
	journal = {Bulletin of the Russian Academy of Sciences: Physics},
	author = {Googlev, K. A. and Kozakov, A. T. and Kochur, A. G. and Nikolskii, A. V. and Torgashev, V. I. and Zvolenskaya, A. A.},
	month = jun,
	year = {2016},
	pages = {638--640},
}



@article{bronwald_composition_2016,
	title = {Composition dependence of the diffuse scattering in cubic {PbZr}$_{\textrm{1-x}}${Ti}$_{\textrm{x}}${O}$_{\textrm{3}}$},
	volume = {503},
	issn = {0015-0193},
	url = {https://doi.org/10.1080/00150193.2016.1217723},
	doi = {10.1080/00150193.2016.1217723},
	abstract = {The results of the experimental study of the diffuse scattering in ferroelectric solid solutions PbZr1-xTixO3 are reported. We have used X-ray diffraction to characterize the diffuse scattering in six single-crystals with . The comparison of diffuse intensity maps in almost pure lead zirconate and PbZr1-xTixO3 compounds with significant titanium doping shows that increasing lead titanate concentration gradually scales down the shape anisotropy of the scattering, but some details of the diffuse scattering that are not observed in pure PbTiO3 still remain.},
	number = {1},
	urldate = {2023-11-11},
	journal = {Ferroelectrics},
	author = {Bronwald, Iurii and Andronikova, Daria and Burkovsky, Roman and Chernyshev, Dmitry and Leontiev, N. G. and Leontiev, I. N. and Ye, Zuo-Guang and Vakhrushev, Sergey},
	month = oct,
	year = {2016},
	note = {Publisher: Taylor \& Francis
\_eprint: https://doi.org/10.1080/00150193.2016.1217723},
	keywords = {diffuse scattering, Lead zirconat-titanate, morphotropic phase boundary, PZT},
	pages = {45--51},
}



@article{kozakov_bi1-xcaxfeo3-_2016,
	title = {Bi$_{\textrm{1-x}}${Ca}$_{\textrm{x}}${FeO}$_{\textrm{3-δ}}$ (0 ≤ x ≤ 1) ceramics: {Crystal} structure, phase and elemental composition, and chemical bonding from {X}-ray diffraction, {Raman} scattering, {Mössbauer}, and {X}-ray photoelectron spectra},
	volume = {664},
	issn = {0925-8388},
	shorttitle = {Bi1-{xCaxFeO3}-δ (0 ≤ x ≤ 1) ceramics},
	url = {https://www.sciencedirect.com/science/article/pii/S0925838815320314},
	doi = {10.1016/j.jallcom.2015.12.241},
	abstract = {An integrated study of samples of Bi1−хCaхFeO3-δ (BCFO) system for 0 ≤ x ≤ 1 (step 0.1) is performed using X-ray diffraction (XRD), Raman scattering, Mössbauer spectroscopy, and X-ray photoelectron spectroscopy (XPS). Measured elemental compositions of samples were found to deviate substantially from nominal ones. X-ray structure analysis discovered a continuous series of solid solutions with perovskite structure (or its derivatives) on the interval of nominal Ca content 0 ≤ x ≤ 0.9. However, the analysis of the data from all the methods used, limits the region of single phase samples (in presence of insignificant amount of foreign ones) to nominal Ca content interval 0.1 {\textless} x {\textless} 0.4. No Fe4+ ions are discovered upon substitution of Bi3+ by Ca2+, neither by Mössbauer spectroscopy, nor by XPS. Charge compensation in Bi1−хCaхFeO3-δ takes place mostly via creation of oxygen vacancies. Charge transfer satellites position in Ca2p XPS is shown to be sensitive to a number of oxygen ions in the immediate environment of Ca.},
	urldate = {2023-11-11},
	journal = {Journal of Alloys and Compounds},
	author = {Kozakov, A. T. and Kochur, A. G. and Torgashev, V. I. and Googlev, K. A. and Kubrin, S. P. and Trotsenko, V. G. and Bush, A. A. and Nikolskii, A. V.},
	month = apr,
	year = {2016},
	keywords = {XPS, Mössbauer spectroscopy, Elemental composition, Vacancies, XRD, BiCaFeO, BiFeO, CaFeO, Phase analysis, Raman scattering},
	pages = {392--405},
}



@article{kadyrov_bandlike_2016,
	title = {Bandlike electrical transport in {Pr}$_{\textrm{1-x}}${Ca}$_{\textrm{x}}${MnO}$_{\textrm{3}}$ manganites},
	volume = {93},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.93.184303},
	doi = {10.1103/PhysRevB.93.184303},
	abstract = {The conductivity and dielectric permittivity spectra of polycrystalline manganites Pr1−xCaxMnO3 with x=0.3, 0.4, and 0.5 have been measured in a broad frequency range (5–3000cm−1) down to low temperatures. From the dispersion analysis the existence of a Drude component can be established that is associated with small polarons coherently moving within a band several meV wide. The temperature-dependent conductivity shows an activated behavior with an activation energy of approximately 165 meV above 170 K and 4.8 meV below 120 K. The change in the activation energy is assigned to the onset of magnetic order at 120 K. In all three samples an absorption band is discovered at 40–60cm−1 that is associated with the transition between Stark-split Pr3+ electron states which gain optical activity due to coupling to acoustical phonons.},
	number = {18},
	urldate = {2023-11-11},
	journal = {Physical Review B},
	author = {Kadyrov, L. S. and Zhang, T. and Zhukova, E. S. and Anzin, V. B. and Trotsenko, V. G. and Torgashev, V. I. and Dressel, M. and Gorshunov, B. P.},
	month = may,
	year = {2016},
	note = {Publisher: American Physical Society},
	pages = {184303},
}



@article{__2016-2,
	title = {Эффекты изменения стехиометрии {LaMnO}$_{\textrm{3}}$},
	volume = {80},
	issn = {0367-6765},
	url = {https://elibrary.ru/item.asp?id=26160197},
	doi = {10.7868/S0367676516060284},
	abstract = {Установлено, что в результате синтеза LaMnO3 из разных прекурсоров, приготовленных методом твердофазной реакции и методами совместного осаждения и сорбции, в зависимости от температур синтеза образуются перовскитовые фазы с разными отклонениями от стехиометрии, что приводит к существованию при комнатной температуре фаз разной симметрии: орторомбической (твердофазный синтез) и ромбоэдрической (влажные методы синтеза).},
	language = {ru},
	number = {6},
	urldate = {2023-11-11},
	journal = {Известия Российской Академии Наук. Серия Физическая},
	author = {Рудская, А. Г. and Чаговец, С. В. and Ананьева, Е. В. and Куприянов, М. Ф.},
	year = {2016},
	pages = {807},
}



@article{__2016-3,
	title = {Электрические свойства и структура новых слоистых оксидов 26,5 ( , , )},
	url = {http://ivdon.ru/ru/magazine/archive/n4y2016/3820},
	abstract = {Сетевой научный журнал «Инженерный вестник Дона»},
	language = {ru},
	urldate = {2023-11-11},
	author = {Чупахина, Т. И. and Мельникова, Н. В. and Гырдасова, О. И. and Никитина, Ю. А. and Гавриляченко, В. Г. and Кабиров, Ю. В. and Пруцакова, Н. В. and Чебанова, Е. В. and Русакова, Е. Б.},
	month = oct,
	year = {2016},
	keywords = {⛔ No DOI found},
	file = {Snapshot:C\:\\Users\\aleks\\Zotero\\storage\\2RRFFXDG\\3820.html:text/html},
}



@article{__2016-4,
	title = {Особенности низкочастотной колебательной динамики и низкотемпературная теплоемкость двустенных углеродных нанотрубок},
	volume = {58},
	url = {http://journals.ioffe.ru/articles/43055},
	abstract = {Построена континуальная модель низкочастотной динамики двустенной углеродной нанотрубки. В рамках предложенного подхода рассмотрено образование низкочастотной части фононного спектра двустенной нанотрубки из фононных спектров образующих ее одностенных нанотрубок. Рассмотрено влияние окружения на фононный спектр одиночной двустенной углеродной нанотрубки. Предложен комбинированный способ оценки коэффициентов ван-дер-ваальсова взаимодействия между стенками нанотрубки на основе спектроскопических данных и известных величин упругих модулей графита. Также рассчитана низкотемпературная удельная теплоемкость двустенных углеродных нанотрубок, которая в области применимости модели (T{\textless}35 K) оказывается значительно меньше, чем сумма удельных теплоемкостей двух образующих ее индивидуальных одностенных нанотрубок. Работа выполнена при поддержке Российского научного фонда (грант N 15-12-10004).},
	language = {ru},
	number = {5},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Авраменко, М. В. and Рошаль, С. Б.},
	month = apr,
	year = {2016},
	pages = {979--986},
	file = {Физика твердого тела:C\:\\Users\\aleks\\Zotero\\storage\\7ERGJUQT\\43055.html:text/html},
}



@article{__2015,
	title = {Рентгеноэлектронное и мессбауэровское исследования валентного состояния ионов переходных металлов в керамиках {Co}$_{\textrm{1-x}}${Fe}$_{\textrm{x}}${Cr}$_{\textrm{2}}${O4} (x=0.1,0.2, 0.5)},
	volume = {58},
	url = {http://journals.ioffe.ru/articles/42621},
	abstract = {Валентное состояние ионов переходных металлов в системе Сo1-xFexCr2O4 (x = 0.1, 0.2, 0.5) изучено с помощью рентгеновской фотоэлектронной и мессбауэровской спектроскопии. Показано присутствие в этой системе ионов Fe2+ и Fe3+. Относительные содержания Fe3+/Fe2+ определены путем подгонки экспериментальных Fe2p-спектров суперпозицией теоретических спектров Fe2+ и Fe3+, а также методом мессбауэровской спектроскопии. Работа выполнена при частичной поддержке Минобрнауки РФ проект 1880 и в рамках проектной части государственного задания Департамента науки и технологий Минобрнауки России N 3.1137.2014К, а также соглашения N 14.607.21.0110 от 27.11.2014 г., уникальный идентификатор соглашения RFMEFI60714X0110.},
	language = {ru},
	number = {1},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Кочур, А. Г. and Гуглев, К. А. and Козаков, А. Т. and Кубрин, С. П. and Никольский, А. В. and Торгашев, В. И.},
	month = dec,
	year = {2015},
	pages = {108--113},
	file = {Физика твердого тела:C\:\\Users\\aleks\\Zotero\\storage\\39KQTSIS\\42621.html:text/html},
}



@article{__2016-5,
	title = {Положительное магнитосопротивление композитов {La}$_{\textrm{0.7}}${Sr}$_{\textrm{0.3}}${MnO}$_{\textrm{3}}$/{C} при комнатной температуре},
	volume = {58},
	url = {http://journals.ioffe.ru/articles/43238},
	abstract = {Синтезированы двухфазные композиты xLa0.7Sr0.3MnO3/(100-x)C (x=5-85 mass/\%). Изучены их магниторезистивные свойства в магнитных полях от 0 до 15 kOe. При комнатной температуре значения положительного изотропного магнитосопротивления для образцов с x=50-60 mass\% достигают 15\%. Работа выполнена при финансовой поддержке РФФИ (проект N 14-03-00103).},
	language = {ru},
	number = {7},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Богатин, А. С. and Лянгузов, Н. В. and Гавриляченко, Т. В.},
	month = jun,
	year = {2016},
	pages = {1263--1265},
}



@article{__2016-6,
	title = {Отрицательная магниторезистивность композитной керамики (1-x){La}$_{\textrm{0.7}}${Sr}$_{\textrm{0.3}}${MnO}$_{\textrm{3}}$/x({GeO}$_{\textrm{2}}$, {Li}$_{\textrm{4}}${P}$_{\textrm{2}}${O}$_{\textrm{7}}$)},
	volume = {42},
	url = {http://journals.ioffe.ru/articles/43008},
	abstract = {Синтезированы керамические композиты (1-x)La0.7Sr0.3MnO3/x(GeO2) и (1-x)La0.7Sr0.3MnO3/x(Li4P2 O7), где x=0.1-0.3, отличающиеся высокими значениями отрицательной изотропной магниторезистивности (MR) при комнатной температуре. В композите, где в качестве барьерной компоненты с массовой долей 20\% использован GeO2, MR=15\% в магнитном поле 18 kOe, а в композите с Li4P2O7 при тех же условиях MR=16\%.},
	language = {ru},
	number = {6},
	urldate = {2023-11-11},
	journal = {Письма в ЖТФ},
	author = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Богатин, А. С. and Лянгузов, Н. В. and Гавриляченко, Т. В. and Медведев, Б. С.},
	month = feb,
	year = {2016},
	pages = {1--5},
	file = {Письма в журнал технической физики:C\:\\Users\\aleks\\Zotero\\storage\\4JRHC3G5\\43008.html:text/html},
}



@article{__2016-7,
	title = {Одношаговый синтез магниторезистивных композитных материалов {La}$_{\textrm{0.7}}${Sr}$_{\textrm{0.3}}${MnO}$_{\textrm{3}}$/{GeO}$_{\textrm{2}}$},
	url = {https://fundamental-research.ru/ru/article/view?id=40689},
	language = {ru},
	number = {9},
	urldate = {2023-11-11},
	journal = {Технические науки},
	author = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Пруцакова, Н. В. and Гуда, А. А. and Попов, Ю. В. and Чебанова, Е. В.},
	month = sep,
	year = {2016},
	pages = {26--30},
	file = {ОДНОШАГОВЫЙ СИНТЕЗ МАГНИТОРЕЗИСТИВНЫХ КОМПОЗИТНЫХ МАТЕРИАЛОВ LA0.7SR0.3MNO3/GEO2 - Фундаментальные исследования (научный журнал):C\:\\Users\\aleks\\Zotero\\storage\\T72K4G94\\view.html:text/html},
}



@article{__2015-1,
	title = {Влияние механизмов роста на деформацию элементарной ячейки и переключение поляризации в гетероструктурах титаната бария-стронция на оксиде магния},
	volume = {86},
	url = {http://journals.ioffe.ru/articles/42648},
	abstract = {Исследованы влияние механизмов роста на деформацию ячейки и связанное с этим изменение свойств монокристаллических пленок Ba0.8Sr0.2TiO3, выращенных на подложках MgO по механизмам роста Франка-Ван дер Мерве и Вольмера-Вебера. Показано, что деформация ячейки существенно зависит от толщины пленки и в значительной мере определяется механизмами роста. Установлено, что в рамках одной пары пленка-подложка можно варьировать напряжения в пленке от двумерно-растягивающих до сжимающих за счет изменения механизмов роста и толщины пленки.},
	language = {ru},
	number = {1},
	urldate = {2023-11-11},
	journal = {Журнал технической физики},
	author = {Мухортов, В. М. and Головко, Ю. И. and Бирюков, С. В. and Анохин, А. С. and Юзюк, Ю. И.},
	month = dec,
	year = {2015},
	pages = {93--98},
	file = {Журнал технической физики:C\:\\Users\\aleks\\Zotero\\storage\\RVFMF3E9\\42648.html:text/html},
}



@article{kochur_valence_2015,
	title = {Valence state of transition metal ions in {Co}$_{\textrm{1−x}}${Fe}$_{\textrm{x}}${Cr}$_{\textrm{2}}${O}$_{\textrm{4}}$ (x=0.1, 0.2, 0.5) ceramics from {X}-ray photoelectron and {Mössbauer} spectroscopy data},
	volume = {636},
	issn = {0925-8388},
	url = {https://www.sciencedirect.com/science/article/pii/S0925838815005903},
	doi = {10.1016/j.jallcom.2015.02.150},
	abstract = {Ceramics with nominal composition Co1−xFexCr2O4 (x=0.1, 0.2, 0.5) are synthesized via a solid state reaction method. Crystal structure of samples is studied with X-ray diffraction. Actual elemental composition is determined using X-ray microanalysis and X-ray photoelectron spectroscopy (XPS). Samples’ morphology is studied with scanning electron microscopy. Valence state of the Co, Fe and Cr ions is determined from 2p X-ray photoelectron spectra and Mössbauer spectra. XPS are assigned based on calculations with allowance for the multiplet splitting, crystal field, and the charge-transfer effects. Cobalt ions are found to be bivalent in tetrahedral coordination; chromium ions are trivalent in octahedral coordination. Fe ions are mostly in trivalent states, although Fe2+ ions are also present in significant amounts. Fe2+ ions are in tetrahedral coordination while Fe3+ ions occupy both tetrahedral and octahedral sites. Bulk and near-surface elemental compositions of the ceramic grains are noticeably different. Relative Fe3+/Fe2+ contents are the same in the volume and at the surface of the samples; relative number of Fe3+ ions increases upon the increase of x. A model of partly inverse spinel structure is suggested where the atoms of iron substitute both Co and Cr atoms.},
	urldate = {2023-11-11},
	journal = {Journal of Alloys and Compounds},
	author = {Kochur, A. G. and Kozakov, A. T. and Googlev, K. A. and Kubrin, S. P. and Nikolskii, A. V. and Torgashev, V. I. and Bush, A. A. and Shkuratov, V. Ya. and Shevtsova, S. I.},
	month = jul,
	year = {2015},
	keywords = {X-ray diffraction, XPS, CoFeCrO ceramics, Ions valence state, Mössbauer spectroscopy, X-ray microanalysis},
	pages = {241--248},
}



@article{kozakov_valence_2015,
	title = {Valence state of manganese and iron ions in {La}$_{\textrm{1−x}}${A}$_{\textrm{x}}${MnO}$_{\textrm{3}}$ ({A} = {Ca}, {Sr}) and {Bi}$_{\textrm{1−x}}${Sr}$_{\textrm{x}}${FeO}$_{\textrm{3}}$ systems from {Mn2p}, {Mn3s}, {Fe2p} and {Fe3s} {X}-ray photoelectron spectra. {Effect} of delocalization on {Fe3s} spectra splitting},
	volume = {647},
	issn = {0925-8388},
	url = {https://www.sciencedirect.com/science/article/pii/S0925838815302772},
	doi = {10.1016/j.jallcom.2015.06.161},
	abstract = {La1−xCaxMnO3 (x = 0.5, 0.7, 0.85, 0.95) ceramic samples are synthesized by solid state reaction method. Mn3s and Mn2p X-ray photoelectron spectra (XPS) of La1−xCaxMnO3, and Fe3s-spectra of Bi1−xSrxFeO3 (0 ≤ x ≤ 1) are measured at room temperature. Both Mn3+ and Mn4+ ions are discovered in La1−xCaxMnO3 similarly to the case of Fe3+ and Fe4+ found earlier in Bi1−xSrxFeO3 ceramics. Relative Mn3+/Mn4+ contents are determined by fitting measured Mn2p spectra with combinations of Mn2p spectra of compounds containing tri- and quadrivalent Mn ions. Relative portion of Mn4+ is shown to increase with the increase of x. Fe3s spectrum splitting in Bi1−xSrxFeO3 increases with x in contrast to the Mn3s-spectrum splitting in La1−xCaxMnO3 and La1−xSrxMnO3. Anomalous behavior of Fe3s splitting is explained in the frame of the model of partly itinerant 3d-electrons by strong effect of 3d electron delocalization on electron correlation interaction in final state of 3s photoabsorption.},
	urldate = {2023-11-11},
	journal = {Journal of Alloys and Compounds},
	author = {Kozakov, A. T. and Kochur, A. G. and Googlev, K. A. and Nikolskii, A. V. and Torgashev, V. I. and Trotsenko, V. G. and Bush, A. A.},
	month = oct,
	year = {2015},
	keywords = {XPS, BiSrFeO, Delocalization, Electron correlation, Fe3s, Itinerant 3d electrons, LaAMnO (A = Ca,Sr), Mn2p, Mn3s},
	pages = {947--955},
}



@article{mikheykin_cooperative_2015,
	title = {The cooperative {Jahn}–{Teller} effect and anti-isostructural phases in {Ni}$_{\textrm{1−x}}${Co}$_{\textrm{x}}${Cr}$_{\textrm{2}}${O}$_{\textrm{4}}$ solid solutions: {Synchrotron} {X}-ray diffraction study},
	volume = {86},
	issn = {0022-3697},
	shorttitle = {The cooperative {Jahn}–{Teller} effect and anti-isostructural phases in {Ni1}−{xCoxCr2O4} solid solutions},
	url = {https://www.sciencedirect.com/science/article/pii/S0022369715001651},
	doi = {10.1016/j.jpcs.2015.06.015},
	abstract = {A low-temperature high-resolution powder diffraction study has been carried out on a system of Ni1−xCoxCr2O4 solid solutions with x≤0.1 down to 5K. The tetragonal phase (I41/amd) with c/a{\textless}1 was experimentally observed in Ni0.9Co0.1Cr2O4 below ∼64K. The new phase is anti-isostructural to the well-known tetragonal phase of NiCr2O4. A unified phenomenological model has been applied to structural phase transitions in Ni1−xCoxCr2O4 solid solutions. It shows that the appearing of such a phase is justified from a structural point of view. Analysis of atomic displacements confirms predictions of the symmetry-based model-free consideration.},
	urldate = {2023-11-11},
	journal = {Journal of Physics and Chemistry of Solids},
	author = {Mikheykin, A. S. and Torgashev, V. I. and Yuzyuk, Yu. I. and Bush, A. A. and Talanov, V. M. and Cervellino, A. and Dmitriev, V. P.},
	month = nov,
	year = {2015},
	keywords = {A. Ceramics, C. X-ray diffraction, D. Crystal field, D. Crystal structure, D. Phase transitions},
	pages = {42--48},
}



@article{kadyrov_terahertz-infrared_2015,
	series = {Special {Issue} on {Electronic} {Crystals} ({ECRYS}-2014)},
	title = {Terahertz-infrared spectroscopy of overdoped manganites {La}$_{\textrm{1−x}}${Ca}$_{\textrm{x}}${MnO}$_{\textrm{3}}$},
	volume = {460},
	issn = {0921-4526},
	url = {https://www.sciencedirect.com/science/article/pii/S0921452614009041},
	doi = {10.1016/j.physb.2014.11.070},
	abstract = {Terahertz and infrared spectra of dielectric permittivity and optical conductivity of overdoped manganites La1−xCaxMnO3 (0.5≤x≤1) have been measured at frequencies ν from 4cm−1 to 700cm−1 and at temperatures T from 5K to 300K. The samples were prepared in the form of bulk polycrystals (ceramics) and epitaxial films (free-standing and on MgO substrates). Strongly asymmetric absorption bands have been found in the compounds which are in charge-ordered state (0.5{\textless}x{\textless}0.85) and have commensurate calcium doping. The bands are located close to the position of lowest energy van Hove singularity of the folded Brillouin zone. The bands are associated with a boson peak, i.e., with the excess of lattice acoustical vibrational states over the standard Debye contribution ({\textasciitilde}ν2). In addition, Raman scattering measurements on ceramic samples have been conducted, which confirmed our assignment of the bands’ origin. We firmly identify contribution to the low energy spectra due to quasi-free charge carriers. In the paramagnetic phase all samples show a Drude-like response corresponding to the band type of charge transport. At low temperatures, for the range of dopings 0.5≤x{\textless}0.85, the conductivity spectra show signatures of variable-range hopping mechanisms of transport.},
	urldate = {2023-11-11},
	journal = {Physica B: Condensed Matter},
	author = {Kadyrov, Lenar S. and Zhukova, Elena S. and Torgashev, Victor I. and Gorshunov, Boris P. and Prokhorov, Anatoly S. and Motovilova, Elizaveta A. and Fischgrabe, Florian and Moshnyaga, Vasily and Zhang, Tao and Kremer, Reinhard and Pracht, Uwe and Zapf, Sina and Pokorný, Jan and Untereiner, Gabriele and Kamba, Stanislav and Dressel, Martin},
	month = mar,
	year = {2015},
	keywords = {Raman spectroscopy, Manganites, Terahertz spectroscopy},
	pages = {199--201},
}



@article{shirokov_phenomenological_2015,
	title = {Phenomenological theory of phase transitions in epitaxial {Ba}$_{\textrm{x}}${Sr}$_{\textrm{1−x}}${TiO}$_{\textrm{3}}$ thin films on (111)-oriented cubic substrates},
	volume = {118},
	issn = {0021-8979},
	url = {https://doi.org/10.1063/1.4926788},
	doi = {10.1063/1.4926788},
	abstract = {A phenomenological thermodynamic theory of BaxSr1−xTiO3 (BST-x) thin films epitaxially grown on (111)-oriented cubic substrates is developed using the Landau-Devonshire approach. The group-theoretical analysis of the low-symmetry phases was performed taking into account two order parameters: the polarization related to ionic shifts in polar zone-center F1u mode and the out-of-phase rotation of TiO6 octahedra corresponding to the R25 zone-boundary mode in the parent cubic phase Pm3¯m. The eight-order thermodynamic potential for BST-x solid solutions was developed and analyzed. We constructed the “concentration-misfit strain” phase diagram for BST-x thin films at room temperature and found that polar rhombohedral R3m phase with the polarization normal to the substrate is stable for x \&gt; 0.72 and negative misfit strains, while ferroelectric monoclinic C2 and Cm phases with in-plane polarization are stable for much smaller x and positive or slightly negative misfit strains. We constructed the “temperature-misfit strain” phase diagrams for several concentrations (x = 1, 0.8, 0.6, 0.4, and 0.2). Systematic changes of the phase transition lines between the paraelectric and ferroelectric phases are discussed. The phase diagrams are useful for practical applications in thin-film engineering.},
	number = {2},
	urldate = {2023-11-11},
	journal = {Journal of Applied Physics},
	author = {Shirokov, V. B. and Shakhovoy, R. A. and Razumnaya, A. G. and Yuzyuk, Yu. I.},
	month = jul,
	year = {2015},
	pages = {024101},
}



@article{rudskaya_situ_2015,
	title = {In {Situ} {Studies} of {LaMnO}$_{\textrm{3}}$ {Phases} {Formation} {When} used of {Different} {Precursors}},
	url = {https://www.semanticscholar.org/paper/In-Situ-Studies-of-LaMnO-3-Phases-Formation-When-of-Rudskaya-Kofanova/3b5d3dfeb83398cd0265cf3d59a70448d257bdf0},
	abstract = {LaMnO3 specimens were synthesized with using of different precursors on X-ray diffractometer (method in situ). It was established that the cubic nanoand microcrystalline perovskite phases starts to form in the temperature range 400 – 600 °C. Synthesized LaMnO3 specimens at room temperature have stoichiometric and nonstoichiometric perovskite-type phases of different symmetry: Pnma (solid state synthesis) and R 3 c (wet methods of precursors’ preparation – sorption, co-precipitation and sol-gel)},
	urldate = {2023-11-11},
	journal = {International Journal of Advanced Research in Chemical Science},
	author = {Rudskaya, A. and Kofanova, N. B. and Kupriyanov, M.},
	year = {2015},
	file = {Full Text PDF:C\:\\Users\\aleks\\Zotero\\storage\\FT2R3G3W\\Rudskaya и др. - 2015 - In Situ Studies of LaMnO 3 Phases Formation When u.pdf:application/pdf},
}



@article{kozakov_fine_2015,
	title = {Fine structure of the {X}-ray photoelectron {Ni} 2$_{\textrm{p}}$ spectrum in {Ni}$_{\textrm{1–x}}${Co}$_{\textrm{x}}${Cr}$_{\textrm{2}}${O}$_{\textrm{4}}$ compounds},
	volume = {79},
	issn = {1934-9432},
	url = {https://doi.org/10.3103/S106287381511012X},
	doi = {10.3103/S106287381511012X},
	abstract = {An interpretation of the components of the fine structure of X-ray photoelectron Ni \$\$\{2\_\{\{p\_\{3/1,1/2\}\}\}\}\$\$spectra of Ni1–xCoxCr2O4 solid solutions (x = 0.8, 0.5, 0.3, 0.02, 0.01, 0.005, 0.0) is given. It is shown that the A and B components of the fine structure in Ni \$\$\{2\_\{\{p\_\{3/2\}\}\}\}\$\$spectra originate from the Ni2+ ions located in the octahedral and tetrahedral environments, respectively. The fraction of Ni2+ ions that occupy octahedral positions in ceramics of different composition is determined.},
	language = {en},
	number = {11},
	urldate = {2023-11-11},
	journal = {Bulletin of the Russian Academy of Sciences: Physics},
	author = {Kozakov, A. T. and Kochur, A. G. and Googlev, K. A. and Nikolskii, A. V. and Torgashev, V. I. and Shevcova, S. I.},
	month = nov,
	year = {2015},
	keywords = {Cr2O4 Solid Solution, Divalent Nickel, Hedral Position, Octahedral Crystal Field, Octahedral Position},
	pages = {1371--1375},
}



@article{tikhonov_emergence_2015,
	title = {Emergence of the sub-{THz} central peak at phase transitions in artificial {BaTiO}$_{\textrm{3}}$/({Ba},{Sr}){TiO}$_{\textrm{3}}$ superlattices},
	volume = {9},
	copyright = {© 2015 WILEY-VCH Verlag GmbH \& Co. KGaA, Weinheim},
	issn = {1862-6270},
	url = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssr.201409505},
	doi = {10.1002/pssr.201409505},
	abstract = {A prominent central peak in the sub-THz frequency range was observed in the Raman spectra of BaTiO3/(Ba,Sr)TiO3 (BT/BST) superlattice grown on (001)MgO substrate. Both soft and central mode show an anomaly around 200 K and 280 K, which can be correlated with orthorhombic to monoclinic phase transition of BST and BT, respectively. The observed temperature dependence of the central mode enabled us to explain rather broad temperature dependence of the dielectric permittivity previously observed in BT/BST superlattices. (© 2015 WILEY-VCH Verlag GmbH \&Co. KGaA, Weinheim)},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {physica status solidi (RRL) – Rapid Research Letters},
	author = {Tikhonov, Yu. A. and Razumnaya, A. G. and Torgashev, V. I. and Zakharchenko, I. N. and Yuzyuk, Yu. I. and El Marssi, M. and Ortega, N. and Kumar, A. and Katiyar, R. S.},
	year = {2015},
	note = {\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssr.201409505},
	keywords = {Raman spectroscopy, ferroelectrics, BaTiO3, phase transitions, soft mode, superlattices},
	pages = {68--71},
}



@article{doronkin_electrochemically_2016,
	title = {Electrochemically {Synthesized} {Pt}/{Al}$_{\textrm{2}}${O}$_{\textrm{3}}$ {Oxidation} {Catalysts}},
	volume = {146},
	issn = {1572-879X},
	url = {https://doi.org/10.1007/s10562-015-1651-z},
	doi = {10.1007/s10562-015-1651-z},
	abstract = {Pt/γ–Al2O3 catalysts made by fast and simple electrochemical dispersion method were characterized using X-ray absorption spectroscopy, CO chemisorption, transmission electron microscopy and X-ray diffraction, and compared with an impregnated catalyst with respect to oxidation of CO and NO. A combination of techniques revealed average particle sizes of 3–4 nm for 0.81–3.8 wt\% Pt/γ–Al2O3 catalysts. Electrochemically prepared materials demonstrated catalytic activity comparable to that of conventional impregnated catalyst and reasonable stability.},
	language = {en},
	number = {2},
	urldate = {2023-11-11},
	journal = {Catalysis Letters},
	author = {Doronkin, Dmitry E. and Kuriganova, Aleksandra B. and Leontyev, Igor N. and Baier, Sina and Lichtenberg, Henning and Smirnova, Nina V. and Grunwaldt, Jan-Dierk},
	month = feb,
	year = {2016},
	keywords = {DOC, Electrochemical dispersion, Oxidation, Platinum},
	pages = {452--463},
}



@article{anokhin_direct_2015,
	title = {Direct transition from the rhombohedral ferroelectric to the paraelectric phase in a ({Ba},{Sr}){TiO}$_{\textrm{3}}$ thin film on a (111){MgO} substrate},
	volume = {112},
	issn = {0295-5075},
	url = {https://dx.doi.org/10.1209/0295-5075/112/47001},
	doi = {10.1209/0295-5075/112/47001},
	abstract = {A heteroepitaxial (200 nm thick) (BST) thin film was deposited on a (111)MgO substrate using rf sputtering. X-ray diffraction examinations confirmed epitaxial growth and rhombohedral symmetry of the film ( and ) at room temperature. Polarized Raman spectra of the film were studied in the temperature range from 100 to 420 K. In contrast to a BST thin film grown on (001)MgO, the observed linear temperature dependence of the squared soft mode frequency suggests the displacive character of the ferroelectric-paraelectric phase transition in a BST thin film on (111)MgO.},
	language = {en},
	number = {4},
	urldate = {2023-11-11},
	journal = {Europhysics Letters},
	author = {Anokhin, A. S. and Yuzyuk, Yu I. and Lyanguzov, N. V. and Razumnaya, A. G. and Stryukov, D. V. and Bunina, O. A. and Golovko, Yu I. and Shirokov, V. B. and Mukhortov, V. M. and Marssi, M. El},
	month = nov,
	year = {2015},
	note = {Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica},
	pages = {47001},
}



@article{shirokov_control_2015,
	title = {Control of acoustic properties of a {BaTiO}$_{\textrm{3}}$ thin film by a planar electric field},
	volume = {111},
	issn = {0295-5075},
	url = {https://dx.doi.org/10.1209/0295-5075/111/16002},
	doi = {10.1209/0295-5075/111/16002},
	abstract = {An influence of a planar electric field on material coefficients of a barium titanate film has been studied. Electric-field dependences of dielectric constants, elastic and piezoelectric moduli were built for the (001)-oriented film on a cubic substrate with a misfit strain value equal to . It was revealed that an electromechanical coupling coefficient, k11, has a maximum at some value of the electric field, which depends on the clamping stress. The misfit strain dependence of the maximum value of the k11 coefficient was studied at strains below (c-phase).},
	language = {en},
	number = {1},
	urldate = {2023-11-11},
	journal = {Europhysics Letters},
	author = {Shirokov, Vladimir and Kalinchuk, Valery and Shakhovoy, Roman and Yuzyuk, Yury},
	month = jul,
	year = {2015},
	note = {Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica},
	pages = {16002},
}



@article{razumnaya_coexistence_2015,
	series = {Proceedings of the 16th {International} {Conference} on the {Physics} of {Light}–{Matter} {Coupling} in {Nanostructures}, {PLMCN} 2015 ({Medellín}, {Colombia}), 3-8 {February}, 2015},
	title = {Coexistence of the soft mode and sub-{THz} central peak in ferroelectric {BaTiO}$_{\textrm{3}}$/({Ba},{Sr}){TiO}$_{\textrm{3}}$ superlattices},
	volume = {87},
	issn = {0749-6036},
	url = {https://www.sciencedirect.com/science/article/pii/S0749603615301117},
	doi = {10.1016/j.spmi.2015.07.038},
	abstract = {Near- and sub-Terahertz dynamics of soft and Debye-type central modes was studied by the polarized Raman spectroscopy in ferroelectric BaTiO3/Ba0.3Sr0.7TiO3 (BT/BST) superlattice in the temperature range of 80–400K where system undergoes the series of phase transitions: paraelectric-tetragonal–monoclinic in BT layers and paraelectric-orthorhombic-monoclinic in BST layers. It was shown that temperature evolution of these modes can be described within the model of coexisted damped harmonic oscillator and Debye relaxator. The occurrence of the pronounced central mode can explain the recently observed relaxor-like dielectric anomaly in such superlattice.},
	urldate = {2023-11-11},
	journal = {Superlattices and Microstructures},
	author = {Razumnaya, A. G. and Tikhonov, Yu. A. and Yuzyuk, Yu. I. and Zakharchenko, I. N. and Torgashev, V. I. and Ortega, N. and Kumar, A. and Katiyar, R. S. and El Marssi, M. and Lukyanchuk, I. A.},
	month = nov,
	year = {2015},
	keywords = {Ferroelectrics, Raman spectroscopy, Debye relaxator, Phase transitions, Soft mode, Superlattice},
	pages = {19--24},
}



@article{__2015-2,
	title = {Фазовые переходы в двух- и трехкомпонентных сверхрешетках перовскитов},
	volume = {57},
	url = {http://journals.ioffe.ru/articles/41506},
	abstract = {Исследовано температурное поведение поляризационных спектров комбинационного рассеяния света двухслойной BaTiO3/Ba0.5Sr0.5TiO3 и трехслойной BaTiO3/Ba0.5Sr0.5TiO3/SrTiO3 сверхрешеток, полученных методом импульсного лазерного напыления на подложках (001)MgO. Установлено, что в трехслойной сверхрешетке частота мягкой моды E(TO) при комнатной температуре значительно выше (94 cm-1), чем в двухслойной (70 cm-1), что свидетельствует об увеличении двумерных напряжений в эпитаксиальных слоях трехслойной сверхрешетки. Анализ температурной зависимости интегральной интенсивности мягкой моды E(TO) позволяет предполагать, что в сверхрешетке BaTiO3/Ba0.5Sr0.5TiO3 переход из сегнетоэлектрической в параэлектрическую фазу происходит при {\textasciitilde}540 K, а в сверхрешетке BaTiO3/Ba0.5Sr0.5TiO3/SrTiO3 температура фазового перехода повышается до {\textasciitilde} 610 K из-за деформаций эпитаксиальных слоев. Работа выполнена за счет гранта Российского научного фонда (проект N 14-12-00258).},
	language = {ru},
	number = {3},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Тихонов, Ю. А. and Разумная, А. Г. and Маслова, О. А. and Захарченко, И. Н. and Юзюк, Ю. И. and Ortega, N. and Kumar, A. and Katiyar, R. S.},
	month = feb,
	year = {2015},
	pages = {475--480},
}



@article{__2015-3,
	title = {Зависимость свойств эпитаксиальных тонких пленок титаната бария-стронция при изменении толщины},
	volume = {57},
	url = {Зависимость свойств эпитаксиальных тонких пленок титаната бария-стронция при изменении толщины},
	abstract = {Проведены исследования гетероэпитаксиальных тонких пленок BaxSr1-xTiO3 различной толщины в параэлектрической фазе при температуре 600oC. Параметры решетки пленки показывают нелинейную зависимость от толщины. С уменьшением толщины происходит увеличение вынужденной деформации и увеличивается объем элементарной ячейки. Поведение вынужденной деформации при изменении толщины хорошо описывается в модели двойного электрического слоя, образовавшегося в процессе синтеза пленки на границе с подложкой. Работа выполнена при поддержке РФФИ (гранты N 13-02-00251а, 13-02-12085-ОФИ\_М и 13-01-90619 Арм\_а).},
	language = {ru},
	number = {8},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Широков, В. Б. and Головко, Ю. И. and Мухортов, В. М. and Юзюк, Ю. И. and Janolin, P. E. and Dkhil, B.},
	month = jul,
	year = {2015},
	pages = {1503--1508},
}



@article{__2015-4,
	title = {Структуры капсидов сферических вирусов как квазикристаллические укладки},
	volume = {57},
	url = {http://journals.ioffe.ru/articles/41613},
	abstract = {Рассматрены вирусные сферические оболочки с икосаэдрической симметрией как квазикристаллические укладки. Аналогично известной теории квазиэквивалентности Каспара и Клуга данный подход также минимизирует количество конформаций, необходимых белковой молекуле для образования связей с соседями в оболочке, но основан на отличных геометрических принципах. Предполагается, что центры белковых молекул находятся в вершинах плиток с одинаковыми ребрами, а количество разных сортов плиток минимально. Получены идеализированные координаты симметрийно-неэквивалентных позиций протеинов в шести различных типах капсидов. Подход описывает единообразно как структуры, удовлетворяющие хорошо известной геометрической модели Каспара и Клуга, так и противоречащие ей. Работа выполнена при поддержке РФФИ (грант N 13-02-12085офи\_м). В.Л. благодарит Labex NUMEV за финансовую поддержку.},
	language = {ru},
	number = {4},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Коневцова, О. В. and Лорман, В. Л. and Рошаль, С. Б.},
	month = mar,
	year = {2015},
	pages = {790--795},
}



@article{__2015-5,
	title = {Материальные константы тонких пленок титаната бария},
	volume = {57},
	url = {http://journals.ioffe.ru/articles/42109},
	abstract = {Нелинейные свойства титаната бария приводят к изменению материальных постоянных линейных уравнений пьезоэффекта для тонких пленок. На основе потенциала Ландау феноменологической теории исследовано поведение материальных постоянных монокристаллических тонких пленок титаната бария при комнатной температуре в зависимости от величины вынужденной деформации. Большинство материальных постоянных при изменении деформации испытывают аномалии на границах фаз. Внутри r-фазы некоторые упругие и электроупругие постоянные достигают экстремума. Полученные результаты позволяют определить направление поиска для получения пленок с необходимыми свойствами. Работа выполнена при финансовой поддержке Российского научного фонда, грант N 14-19-01676.},
	language = {ru},
	number = {8},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Широков, В. Б. and Калинчук, В. В. and Шаховой, Р. А. and Юзюк, Ю. И.},
	month = jul,
	year = {2015},
	pages = {1509--1514},
}



@article{__2015-6,
	title = {Критическое рассеяние синхротронного излучения в цирконате-титанате свинца с малой концентрацией титана},
	volume = {57},
	url = {http://journals.ioffe.ru/articles/42491},
	abstract = {Методом рассеяния синхротронного излучения исследовано диффузное рассеяние в монокристалле цирконата-титаната свинца с концентрацией титана 0.7 at.\%. Измерения проводились как в окрестности центра зоны Бриллюэна, так и в M-точке. В параэлектрической фазе вблизи центра зоны Бриллюэна выявлено сильно анизотропное диффузное рассеяние, анизотропия диффузного рассеяния сходна с наблюдаемой ранее в чистом цирконате свинца. Температурная зависимость этого диффузного рассеяния имеет критический вид с температурой Tc{\textasciitilde} 480 K. Диффузное рассеяние в окрестности M-точки слабо зависит от температуры, причем эта зависимость имеет различный характер в M-точках с различными индексами. Д.А. Андроникова благодарит за финансовую поддержку Правительство РФ (грант N 14.Б25.31.0025), С.Б. Вахрушев и Ю.А. Бронвальд благодарят РФФИ за финансовую поддержу в рамках научного проекта N 14-02-01208.},
	language = {ru},
	number = {12},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Андроникова, Д. А. and Босак, А. А. and Бронвальд, Ю. А. and Бурковский, Р. Г. and Вахрушев, С. Б. and Леонтьев, Н. Г. and Леонтьев, И. Н. and Таганцев, А. К. and Филимонов, А. В. and Чернышов, Д. Ю.},
	month = nov,
	year = {2015},
	pages = {2368--2373},
	file = {Физика твердого тела:C\:\\Users\\aleks\\Zotero\\storage\\AKG5ZVNI\\42491.html:text/html},
}



@article{__2015-7,
	title = {Сегнетоэлектрическая сверхрешетка на основе твердых растворов титаната бария-стронция},
	volume = {57},
	url = {http://journals.ioffe.ru/articles/42408},
	abstract = {Сверхрешетка состава Ba0.8Sr0.2TiO3/Ba0.4Sr0.6TiO3 выращена методом высокочастотного катодного распыления на подложке (001)MgO. С помощью рентгеновской дифракции определены параметры элементарных ячеек слоев сверхрешетки по нормали к подложке, период модуляции и ориентационные соотношения между пленкой и подложкой. На основе температурной зависимости поляризованных спектров комбинационного рассеяния света обнаружено, что наблюдается ужесточение мягкой моды E(TO) от 79 до 97 cm-1 в интервале температур 80-350 K. Характерных признаков последовательности фазовых переходов, которые имеют место в объемных образцах твердых растворов титаната бария-стронция аналогичных составов, не обнаружено, а переход из сегнетоэлектрической в параэлектрическую фазу в сверхрешетке происходит при температуре {\textasciitilde}350 K. Работа выполнена за счет средств Российского научного фонда (проект N 14-12-00258).},
	language = {ru},
	number = {11},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Разумная, А. Г. and Головко, Ю. И. and Лянгузов, Н. В. and Юзюк, Ю. И. and Широков, В. Б. and Мухортов, В. М. and El Marssi, M.},
	month = oct,
	year = {2015},
	pages = {2181--2185},
}



@article{__2014-7,
	title = {Магниторезистивность стеклокомпозитов {La}$_{\textrm{0.7}}${Sr}$_{\textrm{0.3}}${MnO}$_{\textrm{3}}$/ {Sb}$_{\textrm{2}}${O}$_{\textrm{3}}$ при комнатной температуре},
	volume = {57},
	url = {http://journals.ioffe.ru/articles/41214},
	abstract = {Синтезированы керамические композиты La0.7Sr0.3MnO3/Sb2O3 с различными массовыми соотношениями компонентов. Исследованы их магниторезистивные свойства в слабых магнитных полях. Значения отрицательной изотропной магниторезистивности при комнатной температуре для композитов 90\% La0.7Sr0.3MnO3/10\%Sb2O3 составляют -1.2\% при 0.25 kOe и -14\% при 20 kOe. Рост магниторезистивности при увеличении поля имеет черты релаксационного процесса. Работа выполнена при финансовой поддержке проекта РФФИ N 14-03-00103.},
	language = {ru},
	number = {1},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Чупахина, Т. И. and Гавриляченко, Т. В.},
	month = dec,
	year = {2014},
	pages = {16--18},
}



@inproceedings{torgashev_broadband_2015,
	title = {Broadband spectroscopy of {H}$_{\textrm{2}}${O} molecule confined in nano-cages of crystal lattice: {Low}-energy dynamics and incipient ferroelectric behavior},
	shorttitle = {Broadband spectroscopy of {H2O} molecule confined in nano-cages of crystal lattice},
	url = {https://ieeexplore.ieee.org/document/7327553?arnumber=7327553},
	doi = {10.1109/IRMMW-THz.2015.7327553},
	abstract = {Broadband (1 Hz to 100 THz) dielectric response of water-containing beryl crystals was measured at temperatures from 300 K down to 0.3 K. The low-energy dynamics of H2O molecules confined within nano-cages of the crystalline lattice was studied. We observe a THz-range soft mode indicating an incipient ferroelectric behavior due to interacting dipole moments of confined water molecules.},
	urldate = {2023-11-11},
	booktitle = {2015 40th {International} {Conference} on {Infrared}, {Millimeter}, and {Terahertz} waves ({IRMMW}-{THz})},
	author = {Torgashev, Victor I. and Gorshunov, Boris P. and Zhukova, Elena S. and Savinov, Maxim and Kadlec, Christelle and Kadlec, Filip and Skoromets, Volodymyr and Prokleška, J. and Thomas, Victor G. and Fursenko, Dmitry A. and Pestrjakov, Efim V. and Uskov, Vladimir V. and Shakurov, Gil'man S. and Kremer, Reinhard K. and Kadyrov, Lenar S. and Belyanchikov, Mikhail A. and Prokhorov, Anatoliy S. and Gorelik, Vladimir S. and Dressel, Martin},
	month = aug,
	year = {2015},
	note = {ISSN: 2162-2035},
	pages = {1--2},
}



@article{__2015-8,
	title = {Влияние процессов самоорганизации, дефектов, примесей, а также автокаталитических процессов на параметры пленок и наностержней {ZnO}},
	volume = {49},
	url = {https://journals.ioffe.ru/articles/42455},
	abstract = {Исследовано влияние параметров нанесения пленок ZnO на различные материалы подложек при использовании магнетронного распыления на переменном токе в газовой смеси аргона и кислорода. Наблюдалось явление самоорганизации, приводящее к неизменности морфологии поверхности пленок ZnO при варьировании материалов подложки и параметров нанесения. Параметры спектров макро- и микрофотолюминесценции исследованных пленок ZnO незначительно отличались от параметров спектров фотолюминесценции объемных кристаллов ZnO, полученных методом гидротермального роста. Наличие интенсивного излучения с малой величиной FWHM в разных областях спектра дает возможность рассматривать пленки ZnO, полученные магнетронным распылением, легированные РЗИ, как перспективный материал при создании оптоэлектронных приборов, работающих в широком спектральном диапазоне. Возможность реализации магнитного упорядочения при легировании РЗИ существенно расширяет функциональные возможности пленок ZnO. Параметры спектров фотолюминесценции наностержней ZnO определяются геометрическими параметрами, концентрацией и типом введенных примесей.},
	language = {ru},
	number = {11},
	urldate = {2023-11-11},
	journal = {Физика и техника полупроводников},
	author = {Мездрогина, М. М. and Еременко, М. В. and Петров, В. Н. and Теруков, Е. И. and Левицкий, В. С. and Кайдашев, Е. М. and Лянгузов, Н. В.},
	month = oct,
	year = {2015},
	pages = {1521--1530},
	file = {Физика и техника полупроводников:C\:\\Users\\aleks\\Zotero\\storage\\5XEFAQZX\\42455.html:text/html},
}



@article{__2014-8,
	title = {Особенности оптических фононов в спектрах комбинационного рассеяния массива вертикальных микростержней {ZnO} на кремнии},
	volume = {56},
	url = {http://journals.ioffe.ru/articles/26806},
	abstract = {Исследованы поляризованные спектры комбинационного рассеяния массива вертикальных микростержней оксида цинка, синтезированного карботермическим методом на подложке Si (001). Длина стержней составляет 9±0.5 mum, а диаметр - 210±50 nm. Рентгенографические исследования подтвердили взаимную кристаллографическую ориентацию [001]ZnO{\textbar}{\textbar}[001]Si в направлении нормали к плоскости подложки. В спектрах комбинационного рассеяния света стержней наблюдаются запрещенные правилами отбора для монокристалла в геометрии x(yz)x-моды A1(TO) и Ehigh2 и в геометрии x(zz)x-мода E1(LO). Обнаружены квазимоды Q(TO) и Q(LO), спектральное положение которых смещается при изменении угла падения возбуждающего излучения. Путем сравнения спектрального сдвига квазимод с экспериментальными данными для монокристалла произведена оценка интервала углов распространения возбуждающего излучения в массиве стержней, составляющего {\textasciitilde}25o при фиксированном угле падения. Работа выполнялась при финансовой поддержке Министерства образования и науки, тема N 2.5896 "Развитие методов получения и исследование свойств полупроводниковых наноструктур для создания элементов устройств нанофотоники".},
	language = {ru},
	number = {3},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Лянгузов, Н. В. and Анохин, А. С. and Левшов, Д. И. and Кайдашев, Е. М. and Юзюк, Ю. И. and Захарченко, И. Н. and Бунина, О. А.},
	month = feb,
	year = {2014},
	pages = {542--548},
}



@article{__2014-9,
	title = {Влияние редкоземельных ионов на диэлектрический отклик в стиллвеллитовых стеклах},
	volume = {56},
	url = {http://journals.ioffe.ru/articles/26789},
	abstract = {Проведено сравнение экспериментально полученных спектров функции диэлектрического отклика стекол состава LnBGeO5 (Ln = La, Pr, Tb, Er, Sm) в терагерцевом и инфракрасном диапазонах. Выделены полосы поглощения и установлены их вклады в диэлектрическую проницаемость, определены контуры бозонного пика и зависимость диэлектрических потерь от типа редкоземельного иона. Работа выполнена при поддержке Министерства образования и науки РФ (грант N 11.G34.31.0027) и РФФИ (грант N 11-02-00810-а).},
	language = {ru},
	number = {3},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Командин, Г. А. and Торгашев, В. И. and Сигаев, В. Н. and Савинков, В. И. and Лотарев, С. В. and Породинков, О. Е. and Спектор, И. Е.},
	month = feb,
	year = {2014},
	pages = {435--441},
}



@article{__2014-10,
	title = {Особенности ян-теллеровского перехода в твердых растворах {Ni}$_{\textrm{1-x}}${Co}$_{\textrm{x}}${Cr}$_{\textrm{2}}${O}$_{\textrm{4}}$},
	volume = {56},
	url = {http://journals.ioffe.ru/articles/26843},
	abstract = {Методами синхротронной порошковой рентгеновской дифракции исследована структура твердых растворов Ni1-xCоxCr2O4 в температурном интервале 90-350 K для составов с x=0; 0.005; 0.01; 0.015; 0.02; 0.1; 0.5; 0.8 и проведено уточнение их структур с помощью полнопрофильного анализа Ритвельда. На основе полученных данных построена T-x-фазовая диаграмма для твердых растворов в исследованном диапазоне температур и концентраций. Обнаруженные структурные фазовые переходы объяснены с точки зрения теории кристаллического поля и кооперативного эффекта Яна-Теллера. Оценена величина искажений полиэдров, являющихся причиной структурного фазового перехода. Обсуждается применимость феноменологической теории Ландау и возможность использования в качестве параметра порядка величины спонтанных деформаций},
	language = {ru},
	number = {4},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Михейкин, А. С. and Чернышов, Д. Ю. and Буш, А. А. and Прохоров, А. С. and Юзюк, Ю. И. and Дмитриев, В. П.},
	month = mar,
	year = {2014},
	pages = {754--760},
}



@article{__2014-11,
	title = {Фононные и магнонные возбуждения в спектрах комбинационного рассеяния света эпитаксиальной пленки феррита висмута},
	volume = {56},
	url = {http://journals.ioffe.ru/articles/41133},
	abstract = {Эпитаксиальная пленка феррита висмута BiFeO3 на монокристаллической подложке (001)MgO получена методом импульсного лазерного напыления с использованием буферных слоев SrTiO3 и SrRuO3. При комнатной температуре поляризационные характеристики спектров комбинационного рассеяния света исследованной пленки BiFeO3 предполагают моноклинную симметрию. Проведены высокотемпературные (295-1100 K) исследования спектров комбинационного рассеяния света в области частот 20{\textless}nu{\textless}1600 cm-1. Особое внимание уделено высокочастотной области, где наблюдаются полоса 610 cm-1, соответствующая максимуму плотности состояний магнонной ветви на границе зоны Бриллюэна, и интенсивная полоса в спектрах второго порядка с максимумом {\textasciitilde}1250 cm-1, соответствующая плотности состояний двухмагнонных возбуждений. Установлено, что при повышении температуры интенсивность полосы {\textasciitilde}1250 cm-1 линейно понижается и выше 650 K она отсутствует. Экстраполяция температурной зависимости интегральной интенсивности полосы 1250 cm-1 позволяет предполагать, что в данной пленке антиферромагнитный фазовый переход происходит при температуре {\textasciitilde}670 K.},
	language = {ru},
	number = {12},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Кхабири, Г. and Анохин, А. С. and Разумная, А. Г. and Юзюк, Ю. И. and Gueye, I. and Carcan, B. and Bouyanfif, H. and Wolfman, J. and Autret-Lambert, C. and El Marssi, M.},
	month = nov,
	year = {2014},
	pages = {2420--2425},
}



@article{__2014-12,
	title = {Исследование сверхрешеток {BaTiO}$_{\textrm{3}}$/({Ba}$_{\textrm{0.5}}$,{Sr}$_{\textrm{0.5}}$){TiO}$_{\textrm{3}}$/ {SrTiO}$_{\textrm{3}}$ методами рентгеновской дифракции и комбинационного рассеяния света},
	volume = {56},
	url = {http://journals.ioffe.ru/articles/26811},
	abstract = {Методами рентгеновской дифрактометрии определены структурные характеристики сверхрешетки BaTiO3/(Ba0.5,Sr0.5)TiO3/SrTiO3 на подложке (001) MgO. Получены период модуляции, параметры элементарных ячеек слоев, составляющих сверхрешетку, оценены величины областей когерентного рассеяния и средние микродеформации в направлении, перпендикулярном поверхности. Проведено сравнение с характеристиками двухслойной сверхрешетки BaTiO3/(Ba0.5,Sr0.5)TiO3. В спектрах комбинационного рассеяния света обнаружено существенное смещение мягкой E(TO)-моды в трехслойной сверхрешетке по сравнению с ее положением в двухслойной. Обнаруженные эффекты связываются с существенным увеличением температуры перехода трехслойной сверхрешетки в параэлектрическую фазу.},
	language = {ru},
	number = {3},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Тихонов, Ю. А. and Захарченко, И. Н. and Маслова, О. А. and Юзюк, Ю. И. and Ortega, N. and Kumar, A. and Katiyar, R. S.},
	month = feb,
	year = {2014},
	pages = {573--576},
}



@article{__2014-13,
	title = {Температурная эволюция спектров диэлектрического отклика стиллвеллитоподобных стекол в терагерцевом и инфракрасном диапазонах},
	volume = {56},
	url = {http://journals.ioffe.ru/articles/26909},
	abstract = {Измерены спектры пропускания и отражения стекла PrBGeO5 в терагерцевом и инфракрасном диапазонах. При низких температурах зарегистрированы рост диэлектрической проницаемости и появление узких линий резонансного типа в терагерцевом диапазоне. Рассчитаны спектры комплексной диэлектрической проницаемости по формулам Френеля и Крамерса-Кронига.},
	language = {ru},
	number = {6},
	urldate = {2023-11-11},
	journal = {Физика твердого тела},
	author = {Командин, Г. А. and Породинков, О. Е. and Гончаров, Ю. Г. and Спектор, И. Е. and Исхакова, Л. Д. and Сигаев, В. Н. and Лотарев, С. В. and Торгашев, В. И.},
	month = may,
	year = {2014},
	pages = {1152--1157},
}



@article{chalin_landau_2023,
	title = {Landau theory and self-assembly of spherical nanoclusters and nanoparticles with octahedral symmetry},
	volume = {107},
	issn = {2469-9950},
	url = {https://link.aps.org/doi/10.1103/PhysRevB.107.024102},
	doi = {10.1103/PhysRevB.107.024102},
	number = {2},
	journal = {Physical Review B},
	author = {Chalin, D. V. and Rochal, S. B.},
	month = jan,
	year = {2023},
	keywords = {Q1},
	pages = {024102},
}



@article{konevtsova_integration_2023,
	title = {Integration of {Cypoviruses} into polyhedrin matrix},
	volume = {5},
	issn = {2516-0230},
	url = {http://xlink.rsc.org/?DOI=D3NA00393K},
	doi = {10.1039/D3NA00393K},
	abstract = {Based on symmetry arguments we predict the architecture of the Cypovirus superstructure and propose an electrostatic mechanism for its disassembly in alkaline environment.},
	number = {16},
	journal = {Nanoscale Advances},
	author = {Konevtsova, Olga V. and Golushko, Ivan Yu. and Podgornik, Rudolf and Rochal, Sergei B.},
	year = {2023},
	keywords = {Q1},
	pages = {4140--4148},
}



@article{roshal_topological_2023,
	title = {Topological properties and shape of proliferative and nonproliferative cell monolayers},
	volume = {108},
	issn = {2470-0045},
	url = {https://link.aps.org/doi/10.1103/PhysRevE.108.024404},
	doi = {10.1103/PhysRevE.108.024404},
	number = {2},
	journal = {Physical Review E},
	author = {Roshal, Daria S. and Azzag, Karim and Fedorenko, Kirill K. and Rochal, Sergei B. and Baghdiguian, Stephen},
	month = aug,
	year = {2023},
	keywords = {Q1},
	pages = {024404},
}



@article{rochal_close_2023,
	title = {Close packings of identical proteins in small spherical capsids and similar proteinaceous shells},
	volume = {19},
	issn = {1744-683X},
	url = {http://xlink.rsc.org/?DOI=D3SM01106B},
	doi = {10.1039/D3SM01106B},
	abstract = {Analyzing anisotropy of protein shapes, we reveal energy and symmetry reasons controlling capsid structures, including their handedness and interprotein bonds.},
	number = {44},
	journal = {Soft Matter},
	author = {Rochal, Sergei B. and Konevtsova, Olga V. and Golushko, Ivan Yu. and Podgornik, Rudolf},
	year = {2023},
	keywords = {Q1},
	pages = {8649--8658},
}



@article{shirokov_thermodynamic_2023,
	title = {Thermodynamic analysis of electro-optic coefficients of ferroelectrics},
	volume = {133},
	issn = {0021-8979},
	url = {https://pubs.aip.org/jap/article/133/6/063103/2871932/Thermodynamic-analysis-of-electro-optic},
	doi = {10.1063/5.0137409},
	abstract = {The electro-optic coefficients of ferroelectric materials were obtained by Landau thermodynamic theory. It is proved that if the permittivity tensor is diagonal, then some ratios of the electro-optical coefficients are equal to the ratios of its diagonal components. The dependence of electro-optic coefficients on the external electric field for single-crystal barium titanate was studied and discussed. It is shown that electro-optic coefficients are rather high for barium titanate due to a non-linear response of dielectric susceptibility to electric field strength.},
	number = {6},
	journal = {Journal of Applied Physics},
	author = {Shirokov, V. B. and Timoshenko, P. E. and Kalinchuk, V. V.},
	month = feb,
	year = {2023},
	keywords = {Q2},
}



@article{shirokov_role_2023,
	title = {The role of elastic stress during thermomigration of liquid zones based on aluminum in silicon},
	volume = {85},
	issn = {18149146},
	url = {http://ppp.mech.unn.ru/index.php/ppp/article/view/774},
	doi = {10.32326/1814-9146-2023-85-3-426-436},
	abstract = {The method of thermomigration of liquid zones based on aluminum makes it possible to create complex structures of closed channels with boundaries formed from p-n junctions in single-crystal silicon wafers. The channels are characterized by the uniformity of their properties, and the pn junctions are characterized by their sharpness. Such structures are used in high-current electronics, photovoltaics, and microelectromechanical converters. Volumetric deformation inside and outside the channel due to alloying of silicon with aluminum leads to the formation of mechanical stresses. The equilibrium shape of the channels formed at high temperatures is determined by the minimum elastic energy and depends on the material parameters and geometry of the structure. Within the framework of the linear theory of elasticity, the behavior of elastic energy during the formation of the structure of thermomigration channels at high temperatures doped with aluminum in a single-crystalline (001) cut disk was studied. The simulation was performed using the finite element method in the COMSOL Multiphysics mathematical package. The study was carried out for practically important structures in which the direction of the edges is oriented along the diagonal of the square. Only such structures do not have breaks during the process of thermomigration. Based on the calculation results, it was revealed that the minimum elastic energy corresponds to structures with different crystalline orientations inside the channel and outside it – in the main silicon matrix. The direction of the crystalline axes inside the channel, corresponding to the minimum elastic energy, is rotated by 45 degrees in the plane of the disk relative to the direction of the axes of the main matrix of the silicon crystal. In addition, calculations showed that with such a turn, the shape of the channels changes. The minimum elastic energy corresponds not to vertical structures, but to inclined ones. The angle of inclination of the pyramids depends on the width of the channels and the distance between them.},
	number = {3},
	journal = {Problems of Strength and Plasticity},
	author = {Shirokov, V.B. and Seredin, B.M. and Timoshenko, P.E. and Kalinchuk, V.V. and Popov, V.P.},
	year = {2023},
	keywords = {Q4},
	pages = {426--436},
}



@article{shirokov__2023,
	title = {Генерация поверхностных акустических волн сегнетоэлектрической пленкой {BST} при действии одноосной нагрузки},
	issn = {2226-1869},
	url = {https://ered.pstu.ru/index.php/mechanics/article/view/3765},
	doi = {10.15593/perm.mech/2023.1.16},
	abstract = {The electro-mechanical properties of a ferroelectric film of barium strontium titanate (BST) film located on a silicon substrate depend on applied external strain. A significant dependence is observed for concentrations close to values, where a phase transition for the ferroelectric film occurs. A model of single-crystal BST film near the phase transition under uniaxial strain is studied by the thermodynamic theory of phase transitions. The material properties of the film obtained by the model are used for numerical study of the excitation of Rayleigh' acoustic waves on the surface of the film-substrate heterostructure. Shifting the extrema of S-parameters, characterizing the efficiency of excitation of surface acoustic waves, is shown under the applied strain. The change of S-parameters for the first three resonances determined principally by the geometry of the interdigital electrodes is presented. The largest shift of resonant frequency is observed in a case of the second resonance that corresponds to Sezava wave.},
	number = {1},
	journal = {PNRPU Mechanics Bulletin},
	author = {Shirokov, V. B. and Timoshenko, P. E. and Kalinchuk, V. V.},
	month = dec,
	year = {2023},
	keywords = {Q3},
	pages = {173--178},
}



@article{talanov_magnetic_2023,
	title = {Magnetic phase diagrams of the pyrochlore-based magnets: {Landau} theory},
	volume = {575},
	issn = {03048853},
	url = {https://linkinghub.elsevier.com/retrieve/pii/S0304885323003669},
	doi = {10.1016/j.jmmm.2023.170717},
	journal = {Journal of Magnetism and Magnetic Materials},
	author = {Talanov, M.V. and Shirokov, V.B. and Pimenov, M.S. and Talanov, V.M.},
	month = jun,
	year = {2023},
	keywords = {Q2},
	pages = {170717},
}



@article{talanov_symmetry-based_2023,
	title = {Symmetry-based prediction of the type-{II} multiferroics with pyrochlore structure},
	volume = {14},
	issn = {22208054},
	url = {http://nanojournal.ifmo.ru/en/articles-2/volume14/14-2/physics/paper09/},
	doi = {10.17586/2220-8054-2023-14-2-208-215},
	number = {2},
	journal = {Nanosystems: Physics, Chemistry, Mathematics},
	author = {Talanov, V.M. and Talanov, M.V. and Shirokov, V.B.},
	month = apr,
	year = {2023},
	keywords = {Q3},
	pages = {208--215},
}



@article{talanov_spin-induced_2023,
	title = {Spin-induced ferroelastics with pyrochlore lattices},
	volume = {612},
	issn = {0015-0193},
	url = {https://www.tandfonline.com/doi/full/10.1080/00150193.2023.2211291},
	doi = {10.1080/00150193.2023.2211291},
	number = {1},
	journal = {Ferroelectrics},
	author = {Talanov, M. V. and Shirokov, V. B. and Talanov, V. M.},
	month = aug,
	year = {2023},
	keywords = {Q4},
	pages = {1--9},
}



@article{talanov_spin_2023,
	title = {Spin order on the pyrochlore lattice: {Magnetic} crystallography, {Landau} thermodynamics and emergent phenomena},
	volume = {259},
	issn = {13596454},
	url = {https://linkinghub.elsevier.com/retrieve/pii/S1359645423005177},
	doi = {10.1016/j.actamat.2023.119187},
	journal = {Acta Materialia},
	author = {Talanov, Mikhail V. and Shirokov, Vladimir B. and Talanov, Valeriy M.},
	month = oct,
	year = {2023},
	keywords = {Q1},
	pages = {119187},
}



@inproceedings{__2023,
	title = {Мультипорядок, термодинамика и кристаллохимия тетрагональной фазы {MgTi}$_{\textrm{2}}${O}$_{\textrm{4}}$},
	isbn = {978-5-901688-53-3},
	url = {http://www.niic.nsc.ru/phocadownload/Conferences/2023/TiM-2023/2023 Tezisy Termodinamika.pdf#page=122},
	doi = {10.26902/THERM_2023_101},
	booktitle = {Термодинамика и материаловедение. Тезисы докладов {XV} Симпозиума с международным участием},
	publisher = {NIIC SB RAS},
	author = {Таланов, В.М. and Таланов, М.В. and Авакян, Л. А. and Широков, В. Б.},
	year = {2023},
	pages = {121},
}



@inproceedings{__2023-1,
	title = {Поверхностные эффекты в наноразмерных сегнетоэлектрических гетероструктурах},
	booktitle = {{XIII} Всероссийский съезд по теоретической и прикладной механике. Санкт-Петербург, 21-25 августа},
	author = {Калинчук, В.В. and Тимошенко, П.Е. and Широков, В.Б.},
	year = {2023},
	pages = {Т.4, С.670--672},
}



@inproceedings{__2023-2,
	title = {О перспективных для систем мониторинга слоистых структурах с сегнетоэлектрическим поверхностным слоем},
	doi = {10.18720/SPBPU/2/id23-630},
	booktitle = {{XIII} Всероссийский съезд по теоретической и прикладной механике. Санкт- Петербург, 21-25 августа},
	author = {Тимошенко, П.Е. and Широков, В.Б. and Калинчук, В.В.},
	year = {2023},
	pages = {Т.4, С.741--743},
}



@article{talanov_multiorder_2023,
	title = {Multiorder and the {Structural} {Mechanism} of the {LiRh}$_{\textrm{2}}${O}$_{\textrm{4}}$ {Tetragonal} {Phase} {Formation}},
	volume = {87},
	issn = {1062-8738},
	url = {https://link.springer.com/10.3103/S1062873823703136},
	doi = {10.3103/S1062873823703136},
	number = {9},
	journal = {Bulletin of the Russian Academy of Sciences: Physics},
	author = {Talanov, M. V. and Shirokov, V. B. and Talanov, V. M. and Aulov, M. S.},
	month = sep,
	year = {2023},
	keywords = {Q3},
	pages = {1263--1269},
}



@article{__2023-3,
	title = {Определение электрооптических коэффициентов титаната бария},
	volume = {510},
	doi = {10.31857/S2686740023030148},
	journal = {Доклады Российской Академии Наук. Физика, Технические науки},
	author = {Широков, В. Б. and Тимошенко, П. Е. and Калинчук, В. В.},
	year = {2023},
	pages = {38--43},
}



@article{kaydashev_photothermal_2023,
	title = {Photothermal Effect and Phase Transition in {VO}$_{\textrm{2}}$ Enhanced by {Plasmonic} {Particles}},
	volume = {16},
	issn = {1996-1944},
	url = {https://www.mdpi.com/1996-1944/16/7/2579},
	doi = {10.3390/ma16072579},
	abstract = {Phase change metasurfaces based on VO2, which are pre-heated with electric current and optically addressed by projected structured light hologram, are considered to become a new paradigm in programmed THz/middle IR flat optics. Macroscopic quasi-homogeneous arrays of Au nanoparticles show large near IR absorption and a significant photothermal effect capable of boosting a light-triggered switching of VO2 and are to be carefully examined. We propose a new approach to simultaneously probe the altered temperature and electric conductivity of a hybrid Au particle-VO2 film composite by monitoring a phase shift and attenuating a surface acoustic wave in a YX128° cut LiNbO3 substrate. The method shows a temperature resolution of 0.1 °C comparable with the best existing techniques for studying nanoobjects and surfaces. The laser-induced photothermal effects were characterized in a macroscopic array of Au nanostars (AuNSts) with different surface coverage. In a monolayer of 10 nm Au, coupled plasmonic nanoparticles were deposited on the LiNbO3 substrate. An optically triggered insulator-metal transition assisted by photothermal effect in AuNSts/VO2/TiO2/LiNbO3 composites was studied at varied light power. We believe that the proposed SAW-based method is of significant importance for the characterization and optimization of radiation absorbing or/and electrically heated elements of metasurfaces and other devices for lab-on-chip and optical communication/processor technology.},
	number = {7},
	journal = {Materials},
	author = {Kaydashev, Vladimir and Khlebtsov, Boris and Kutepov, Maxim and Nikolskiy, Anatoliy and Kozakov, Alexey and Konstantinov, Alexey and Mikheykin, Alexey and Karapetyan, Gevork and Kaidashev, Evgeni},
	month = mar,
	year = {2023},
	keywords = {Q2},
	pages = {2579},
}



@article{alekseenko_integrated_2023,
	title = {The integrated approach to studying the microstructure of de-alloyed {PtCu}/{C} electrocatalysts for {PEMFCs}},
	volume = {631},
	issn = {01694332},
	url = {https://linkinghub.elsevier.com/retrieve/pii/S0169433223012175},
	doi = {10.1016/j.apsusc.2023.157539},
	journal = {Applied Surface Science},
	author = {Alekseenko, A.A. and Pavlets, A.S. and Mikheykin, A.S. and Belenov, S.V. and Guterman, E.V.},
	month = sep,
	year = {2023},
	keywords = {Q1},
	pages = {157539},
}



@article{konstantinov_lattice_2023,
	title = {Lattice dynamics and phase transitions peculiarities of {Ba}$_{\textrm{x}}${Sr}$_{\textrm{1-x}}${TiO}$_{\textrm{3}}$ solid solutions with high {Sr} content},
	volume = {654},
	issn = {09214526},
	url = {https://linkinghub.elsevier.com/retrieve/pii/S0921452623000765},
	doi = {10.1016/j.physb.2023.414709},
	journal = {Physica B: Condensed Matter},
	author = {Konstantinov, A.S. and Linnik, E.D. and Razumnaya, A.G. and Mikheykin, A.S.},
	month = apr,
	year = {2023},
	keywords = {Q2},
	pages = {414709},
}



@article{angadi_high-performance_2023,
	title = {High-performance {LPG} sensing behaviour of {CoCr}$_{\textrm{2-x}}${Ce}$_{\textrm{x}}${O}$_{\textrm{4}}$ (x = 0 to 0.02) for sensor applications},
	volume = {34},
	issn = {0957-4522},
	url = {https://link.springer.com/10.1007/s10854-022-09725-1},
	doi = {10.1007/s10854-022-09725-1},
	number = {4},
	journal = {Journal of Materials Science: Materials in Electronics},
	author = {Angadi, V. Jagadeesha and Pasha, Apsar and Al-Dossari, M. and EL-Gawaad, N. S. Abd and Abdulvakhidov, Kamaludin and Lyanguzov, Nikolay and Khadke, Uday Kumar},
	month = feb,
	year = {2023},
	keywords = {Q2},
	pages = {318},
}



@article{andryushin_evolution_2023,
	title = {Evolution of the macroresponses during the transition from two-to six-component systems of the solid solutions with fundamentally different properties},
	volume = {49},
	issn = {02728842},
	url = {https://linkinghub.elsevier.com/retrieve/pii/S0272884223019983},
	doi = {10.1016/j.ceramint.2023.07.074},
	number = {19},
	journal = {Ceramics International},
	author = {Andryushin, K.P. and Mazuritsky, M.I. and Galatova, A.O. and Il'ina, M.V. and Soboleva, O.I. and Nagaenko, A.V. and Shilkina, L.A. and Dudkina, S.I. and Andryushina, I.N. and Rudskaya, A.G. and Khasbulatov, S.V. and Sadykov, Kh.A. and Reznichenko, L.A.},
	month = oct,
	year = {2023},
	keywords = {Q1},
	pages = {31265--31275},
}



@inproceedings{lebedinskaya_parameters_2023,
	title = {Parameters structure calculation of nonstoichiometric {Pb}({Mg}$_{\textrm{1-y}}${Nb}$_{\textrm{y}}$){O}$_{\textrm{3-z}}$ solid solutions},
	url = {http://aip.scitation.org/doi/abs/10.1063/5.0115358},
	doi = {10.1063/5.0115358},
	author = {Lebedinskaya, Alla and Rudskaya, Angela},
	year = {2023},
	pages = {040003},
}



@article{konstantin_multifunctional_2023,
	title = {Multifunctional {Materials} {Based} on the {Solid} {Solutions} of the ({Na}, {K}, {Cd}$_{\textrm{0.5}}$){NbO}$_{\textrm{3}}$3 ({KNN}-{Cd}) {System} {Modified} with {Rare} {Earth} {Elements}: {Crystal} {Structure}, {Microstructure}, and {Macroresponses}},
	volume = {6},
	issn = {2571-6131},
	url = {https://www.mdpi.com/2571-6131/6/1/21},
	doi = {10.3390/ceramics6010021},
	abstract = {Ceramic samples of polycomponent solid solutions (SSs) Na0.90K0.05Cd0.05NbO3 (Cd-modified KNN) and [(Na0.90K0.05Cd0.05)0.95REE0.05]NbO3, where REE = La, Pr, Tb, Dy, Ho, were obtained by the uniaxial hot pressing (UHP) method. The crystal lattice structures, morphological features of the microstructure, and dielectric and thermophysical properties of these ceramics have been investigated. For the first time, their strength characteristics (Young's modulus) and the critical stress intensity factor of the mode I Kic have been estimated. Photoluminescent properties have been compared in SSs [(Na0.90K0.05Cd0.05)0.95REE0.05]NbO3 in the visible wavelength range.},
	number = {1},
	journal = {Ceramics},
	author = {Konstantin, Andryushin and Palatnikov, Mikhail and Shilkina, Lidiya and Nagaenko, Alexandr and Shcherbina, Olga and Smirnov, Maxim and Sidorov, Nikolay and Kubrin, Stanislav and Rudskaya, Anzhela and Rudskiy, Daniil and Reznichenko, Larisa},
	month = feb,
	year = {2023},
	keywords = {Q2},
	pages = {342--363},
}



@article{sidorenko_radio-absorbing_2023,
	title = {Radio-absorbing properties of (1- x ){BiFeO}$_{\textrm{3-x}}${LaMnO}$_{\textrm{3}}$ (0.1 ≤ x ≤ 0.9) solid solutions},
	volume = {606},
	issn = {0015-0193},
	url = {https://www.tandfonline.com/doi/full/10.1080/00150193.2023.2189843},
	doi = {10.1080/00150193.2023.2189843},
	number = {1},
	journal = {Ferroelectrics},
	author = {Sidorenko, E. N. and Rudskaya, A. G. and Babenko, A. A. and Natkhin, I. I. and Galatova, A. O. and Rudsky, D. I.},
	month = apr,
	year = {2023},
	keywords = {Q4},
	pages = {50--60},
}



@incollection{sidorenko_investigation_2023,
	title = {Investigation of the {Microwave} {Properties} of the {Transparent} {Piezoceramics} {PLZT}},
	url = {https://link.springer.com/10.1007/978-3-031-21572-8_16},
	author = {Sidorenko, E. N. and Rudskaya, A. G. and Natkhin, I. I. and Rudsky, D. I. and Shpanko, S. P.},
	year = {2023},
	doi = {10.1007/978-3-031-21572-8_16},
	pages = {189--196},
}
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April 2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0272884222043309\"\n     onclick=\"log_download('molodtsova-gorshenkov-kolesnikov-leontyev-kaichev-zhigunov-faddeev-kuriganova-etal-fabricationofnanointextrm2otextrm3phasejunctionbypulsealternatingcurrentsynthesisforenhancedphotoelectrochemicalperformanceunravellingtheroleofsyntheticconditions-2023', 'https://linkinghub.elsevier.com/retrieve/pii/S0272884222043309', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Fabrication of nano-In$_{\\textrm{2}}$O$_{\\textrm{3}}$ phase junction by pulse alternating current synthesis for enhanced photoelectrochemical performance: Unravelling the role of synthetic conditions [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.ceramint.2022.11.293\"\n     onclick=\"log_download('molodtsova-gorshenkov-kolesnikov-leontyev-kaichev-zhigunov-faddeev-kuriganova-etal-fabricationofnanointextrm2otextrm3phasejunctionbypulsealternatingcurrentsynthesisforenhancedphotoelectrochemicalperformanceunravellingtheroleofsyntheticconditions-2023', 'http://doi.org/10.1016/j.ceramint.2022.11.293', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/molodtsova-gorshenkov-kolesnikov-leontyev-kaichev-zhigunov-faddeev-kuriganova-etal-fabricationofnanointextrm2otextrm3phasejunctionbypulsealternatingcurrentsynthesisforenhancedphotoelectrochemicalperformanceunravellingtheroleofsyntheticconditions-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>2 downloads</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('molodtsova-gorshenkov-kolesnikov-leontyev-kaichev-zhigunov-faddeev-kuriganova-etal-fabricationofnanointextrm2otextrm3phasejunctionbypulsealternatingcurrentsynthesisforenhancedphotoelectrochemicalperformanceunravellingtheroleofsyntheticconditions-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{molodtsova_fabrication_2023,\n\ttitle = {Fabrication of nano-{In}$_{\\textrm{2}}${O}$_{\\textrm{3}}$ phase junction by pulse alternating current synthesis for enhanced photoelectrochemical performance: {Unravelling} the role of synthetic conditions},\n\tvolume = {49},\n\tissn = {02728842},\n\tshorttitle = {Fabrication of nano-{In2O3} phase junction by pulse alternating current synthesis for enhanced photoelectrochemical performance},\n\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0272884222043309},\n\tdoi = {10.1016/j.ceramint.2022.11.293},\n\tlanguage = {en},\n\tnumber = {7},\n\turldate = {2023-11-11},\n\tjournal = {Ceramics International},\n\tauthor = {Molodtsova, Tatyana and Gorshenkov, Mikhail and Kolesnikov, Evgeny and Leontyev, Igor and Kaichev, Vasily and Zhigunov, Denis and Faddeev, Nikita and Kuriganova, Alexandra and Smirnova, Nina},\n\tmonth = apr,\n\tyear = {2023},\n\tkeywords = {Q1},\n\tpages = {10986--10992},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"konevtsova-golushko-podgornik-rochal-hiddensymmetryoftheflavivirusproteinshellandphcontrolledreconstructionoftheviralsurface-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://xlink.rsc.org/?DOI=D2BM01562E\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'konevtsova-golushko-podgornik-rochal-hiddensymmetryoftheflavivirusproteinshellandphcontrolledreconstructionoftheviralsurface-2023', 'http://xlink.rsc.org/?DOI=D2BM01562E', event);\">\n    Hidden symmetry of the flavivirus protein shell and pH-controlled reconstruction of the viral surface.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Konevtsova, O. V.; Golushko, I. Y.; Podgornik, R.;  and Rochal, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Biomaterials Science</i>, 11(1): 225–234.  2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://xlink.rsc.org/?DOI=D2BM01562E\"\n     onclick=\"log_download('konevtsova-golushko-podgornik-rochal-hiddensymmetryoftheflavivirusproteinshellandphcontrolledreconstructionoftheviralsurface-2023', 'http://xlink.rsc.org/?DOI=D2BM01562E', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Hidden symmetry of the flavivirus protein shell and pH-controlled reconstruction of the viral surface [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1039/D2BM01562E\"\n     onclick=\"log_download('konevtsova-golushko-podgornik-rochal-hiddensymmetryoftheflavivirusproteinshellandphcontrolledreconstructionoftheviralsurface-2023', 'http://doi.org/10.1039/D2BM01562E', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/konevtsova-golushko-podgornik-rochal-hiddensymmetryoftheflavivirusproteinshellandphcontrolledreconstructionoftheviralsurface-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('konevtsova-golushko-podgornik-rochal-hiddensymmetryoftheflavivirusproteinshellandphcontrolledreconstructionoftheviralsurface-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{konevtsova_hidden_2023,\n\ttitle = {Hidden symmetry of the flavivirus protein shell and {pH}-controlled reconstruction of the viral surface},\n\tvolume = {11},\n\tissn = {2047-4830, 2047-4849},\n\turl = {http://xlink.rsc.org/?DOI=D2BM01562E},\n\tdoi = {10.1039/D2BM01562E},\n\tabstract = {A pH-induced change in the charge distribution of proteins leads to a structural transformation of the outer flavivirus shell, which violates the hidden symmetry of the mutual arrangement of proteins located on opposite sides of the lipid membrane.\n          , \n            Using recent Zika virus structural data we reveal a hidden symmetry of protein order in immature and mature flavivirus shells, violating the Caspar–Klug paradigmatic model of capsid structures. We show that proteins of the outer immature shell layer exhibit trihexagonal tiling, while proteins from inner and outer layers conjointly form a double-shelled close-packed structure, based on a common triangular spherical lattice. Within the proposed structural model, we furthermore rationalize the structural organization of misassembled non-infectious subviral particles that have no inner capsid. We consider a pH-controlled structural reconstruction of the outer shell from the trimeric to the dimeric state, and demonstrate that this transition, occurring during the virus maturation, can be induced by changes in protein charges at lower pH, leading to a decrease in the electrostatic interaction free energy. This transition could also be assisted by electrostatic attraction of shell proteins to the interposed lipid membrane substrate separating the shells.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Biomaterials Science},\n\tauthor = {Konevtsova, Olga V. and Golushko, Ivan Yu. and Podgornik, Rudolf and Rochal, Sergei B.},\n\tyear = {2023},\n\tkeywords = {Q1},\n\tpages = {225--234},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A pH-induced change in the charge distribution of proteins leads to a structural transformation of the outer flavivirus shell, which violates the hidden symmetry of the mutual arrangement of proteins located on opposite sides of the lipid membrane. , Using recent Zika virus structural data we reveal a hidden symmetry of protein order in immature and mature flavivirus shells, violating the Caspar–Klug paradigmatic model of capsid structures. We show that proteins of the outer immature shell layer exhibit trihexagonal tiling, while proteins from inner and outer layers conjointly form a double-shelled close-packed structure, based on a common triangular spherical lattice. Within the proposed structural model, we furthermore rationalize the structural organization of misassembled non-infectious subviral particles that have no inner capsid. We consider a pH-controlled structural reconstruction of the outer shell from the trimeric to the dimeric state, and demonstrate that this transition, occurring during the virus maturation, can be induced by changes in protein charges at lower pH, leading to a decrease in the electrostatic interaction free energy. This transition could also be assisted by electrostatic attraction of shell proteins to the interposed lipid membrane substrate separating the shells.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"chalin-rochal-landautheoryandselfassemblyofsphericalnanoclustersandnanoparticleswithoctahedralsymmetry-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.107.024102\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'chalin-rochal-landautheoryandselfassemblyofsphericalnanoclustersandnanoparticleswithoctahedralsymmetry-2023', 'https://link.aps.org/doi/10.1103/PhysRevB.107.024102', event);\">\n    Landau theory and self-assembly of spherical nanoclusters and nanoparticles with octahedral symmetry.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Chalin, D. V.;  and Rochal, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 107(2): 024102. January 2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.107.024102\"\n     onclick=\"log_download('chalin-rochal-landautheoryandselfassemblyofsphericalnanoclustersandnanoparticleswithoctahedralsymmetry-2023', 'https://link.aps.org/doi/10.1103/PhysRevB.107.024102', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Landau theory and self-assembly of spherical nanoclusters and nanoparticles with octahedral symmetry [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.107.024102\"\n     onclick=\"log_download('chalin-rochal-landautheoryandselfassemblyofsphericalnanoclustersandnanoparticleswithoctahedralsymmetry-2023', 'http://doi.org/10.1103/PhysRevB.107.024102', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/chalin-rochal-landautheoryandselfassemblyofsphericalnanoclustersandnanoparticleswithoctahedralsymmetry-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('chalin-rochal-landautheoryandselfassemblyofsphericalnanoclustersandnanoparticleswithoctahedralsymmetry-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{chalin_landau_2023,\n\ttitle = {Landau theory and self-assembly of spherical nanoclusters and nanoparticles with octahedral symmetry},\n\tvolume = {107},\n\tissn = {2469-9950},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.107.024102},\n\tdoi = {10.1103/PhysRevB.107.024102},\n\tnumber = {2},\n\tjournal = {Physical Review B},\n\tauthor = {Chalin, D. V. and Rochal, S. B.},\n\tmonth = jan,\n\tyear = {2023},\n\tkeywords = {Q1},\n\tpages = {024102},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"konevtsova-golushko-podgornik-rochal-integrationofcypovirusesintopolyhedrinmatrix-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://xlink.rsc.org/?DOI=D3NA00393K\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'konevtsova-golushko-podgornik-rochal-integrationofcypovirusesintopolyhedrinmatrix-2023', 'http://xlink.rsc.org/?DOI=D3NA00393K', event);\">\n    Integration of Cypoviruses into polyhedrin matrix.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Konevtsova, O. V.; Golushko, I. Y.; Podgornik, R.;  and Rochal, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Nanoscale Advances</i>, 5(16): 4140–4148.  2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://xlink.rsc.org/?DOI=D3NA00393K\"\n     onclick=\"log_download('konevtsova-golushko-podgornik-rochal-integrationofcypovirusesintopolyhedrinmatrix-2023', 'http://xlink.rsc.org/?DOI=D3NA00393K', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Integration of Cypoviruses into polyhedrin matrix [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1039/D3NA00393K\"\n     onclick=\"log_download('konevtsova-golushko-podgornik-rochal-integrationofcypovirusesintopolyhedrinmatrix-2023', 'http://doi.org/10.1039/D3NA00393K', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/konevtsova-golushko-podgornik-rochal-integrationofcypovirusesintopolyhedrinmatrix-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('konevtsova-golushko-podgornik-rochal-integrationofcypovirusesintopolyhedrinmatrix-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{konevtsova_integration_2023,\n\ttitle = {Integration of {Cypoviruses} into polyhedrin matrix},\n\tvolume = {5},\n\tissn = {2516-0230},\n\turl = {http://xlink.rsc.org/?DOI=D3NA00393K},\n\tdoi = {10.1039/D3NA00393K},\n\tabstract = {Based on symmetry arguments we predict the architecture of the Cypovirus superstructure and propose an electrostatic mechanism for its disassembly in alkaline environment.},\n\tnumber = {16},\n\tjournal = {Nanoscale Advances},\n\tauthor = {Konevtsova, Olga V. and Golushko, Ivan Yu. and Podgornik, Rudolf and Rochal, Sergei B.},\n\tyear = {2023},\n\tkeywords = {Q1},\n\tpages = {4140--4148},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Based on symmetry arguments we predict the architecture of the Cypovirus superstructure and propose an electrostatic mechanism for its disassembly in alkaline environment.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"roshal-azzag-fedorenko-rochal-baghdiguian-topologicalpropertiesandshapeofproliferativeandnonproliferativecellmonolayers-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevE.108.024404\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'roshal-azzag-fedorenko-rochal-baghdiguian-topologicalpropertiesandshapeofproliferativeandnonproliferativecellmonolayers-2023', 'https://link.aps.org/doi/10.1103/PhysRevE.108.024404', event);\">\n    Topological properties and shape of proliferative and nonproliferative cell monolayers.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Roshal, D. S.; Azzag, K.; Fedorenko, K. K.; Rochal, S. B.;  and Baghdiguian, S.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review E</i>, 108(2): 024404. August 2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevE.108.024404\"\n     onclick=\"log_download('roshal-azzag-fedorenko-rochal-baghdiguian-topologicalpropertiesandshapeofproliferativeandnonproliferativecellmonolayers-2023', 'https://link.aps.org/doi/10.1103/PhysRevE.108.024404', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Topological properties and shape of proliferative and nonproliferative cell monolayers [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevE.108.024404\"\n     onclick=\"log_download('roshal-azzag-fedorenko-rochal-baghdiguian-topologicalpropertiesandshapeofproliferativeandnonproliferativecellmonolayers-2023', 'http://doi.org/10.1103/PhysRevE.108.024404', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/roshal-azzag-fedorenko-rochal-baghdiguian-topologicalpropertiesandshapeofproliferativeandnonproliferativecellmonolayers-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>1 download</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('roshal-azzag-fedorenko-rochal-baghdiguian-topologicalpropertiesandshapeofproliferativeandnonproliferativecellmonolayers-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{roshal_topological_2023,\n\ttitle = {Topological properties and shape of proliferative and nonproliferative cell monolayers},\n\tvolume = {108},\n\tissn = {2470-0045},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevE.108.024404},\n\tdoi = {10.1103/PhysRevE.108.024404},\n\tnumber = {2},\n\tjournal = {Physical Review E},\n\tauthor = {Roshal, Daria S. and Azzag, Karim and Fedorenko, Kirill K. and Rochal, Sergei B. and Baghdiguian, Stephen},\n\tmonth = aug,\n\tyear = {2023},\n\tkeywords = {Q1},\n\tpages = {024404},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"rochal-konevtsova-golushko-podgornik-closepackingsofidenticalproteinsinsmallsphericalcapsidsandsimilarproteinaceousshells-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://xlink.rsc.org/?DOI=D3SM01106B\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'rochal-konevtsova-golushko-podgornik-closepackingsofidenticalproteinsinsmallsphericalcapsidsandsimilarproteinaceousshells-2023', 'http://xlink.rsc.org/?DOI=D3SM01106B', event);\">\n    Close packings of identical proteins in small spherical capsids and similar proteinaceous shells.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Rochal, S. B.; Konevtsova, O. V.; Golushko, I. Y.;  and Podgornik, R.\n</span>\n\n  \n\n</span>\n\n  <i>Soft Matter</i>, 19(44): 8649–8658.  2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://xlink.rsc.org/?DOI=D3SM01106B\"\n     onclick=\"log_download('rochal-konevtsova-golushko-podgornik-closepackingsofidenticalproteinsinsmallsphericalcapsidsandsimilarproteinaceousshells-2023', 'http://xlink.rsc.org/?DOI=D3SM01106B', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Close packings of identical proteins in small spherical capsids and similar proteinaceous shells [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1039/D3SM01106B\"\n     onclick=\"log_download('rochal-konevtsova-golushko-podgornik-closepackingsofidenticalproteinsinsmallsphericalcapsidsandsimilarproteinaceousshells-2023', 'http://doi.org/10.1039/D3SM01106B', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/rochal-konevtsova-golushko-podgornik-closepackingsofidenticalproteinsinsmallsphericalcapsidsandsimilarproteinaceousshells-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('rochal-konevtsova-golushko-podgornik-closepackingsofidenticalproteinsinsmallsphericalcapsidsandsimilarproteinaceousshells-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{rochal_close_2023,\n\ttitle = {Close packings of identical proteins in small spherical capsids and similar proteinaceous shells},\n\tvolume = {19},\n\tissn = {1744-683X},\n\turl = {http://xlink.rsc.org/?DOI=D3SM01106B},\n\tdoi = {10.1039/D3SM01106B},\n\tabstract = {Analyzing anisotropy of protein shapes, we reveal energy and symmetry reasons controlling capsid structures, including their handedness and interprotein bonds.},\n\tnumber = {44},\n\tjournal = {Soft Matter},\n\tauthor = {Rochal, Sergei B. and Konevtsova, Olga V. and Golushko, Ivan Yu. and Podgornik, Rudolf},\n\tyear = {2023},\n\tkeywords = {Q1},\n\tpages = {8649--8658},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Analyzing anisotropy of protein shapes, we reveal energy and symmetry reasons controlling capsid structures, including their handedness and interprotein bonds.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-timoshenko-kalinchuk-thermodynamicanalysisofelectroopticcoefficientsofferroelectrics-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://pubs.aip.org/jap/article/133/6/063103/2871932/Thermodynamic-analysis-of-electro-optic\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-timoshenko-kalinchuk-thermodynamicanalysisofelectroopticcoefficientsofferroelectrics-2023', 'https://pubs.aip.org/jap/article/133/6/063103/2871932/Thermodynamic-analysis-of-electro-optic', event);\">\n    Thermodynamic analysis of electro-optic coefficients of ferroelectrics.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.; Timoshenko, P. E.;  and Kalinchuk, V. V.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Applied Physics</i>, 133(6). February 2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://pubs.aip.org/jap/article/133/6/063103/2871932/Thermodynamic-analysis-of-electro-optic\"\n     onclick=\"log_download('shirokov-timoshenko-kalinchuk-thermodynamicanalysisofelectroopticcoefficientsofferroelectrics-2023', 'https://pubs.aip.org/jap/article/133/6/063103/2871932/Thermodynamic-analysis-of-electro-optic', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Thermodynamic analysis of electro-optic coefficients of ferroelectrics [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/5.0137409\"\n     onclick=\"log_download('shirokov-timoshenko-kalinchuk-thermodynamicanalysisofelectroopticcoefficientsofferroelectrics-2023', 'http://doi.org/10.1063/5.0137409', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-timoshenko-kalinchuk-thermodynamicanalysisofelectroopticcoefficientsofferroelectrics-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-timoshenko-kalinchuk-thermodynamicanalysisofelectroopticcoefficientsofferroelectrics-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_thermodynamic_2023,\n\ttitle = {Thermodynamic analysis of electro-optic coefficients of ferroelectrics},\n\tvolume = {133},\n\tissn = {0021-8979},\n\turl = {https://pubs.aip.org/jap/article/133/6/063103/2871932/Thermodynamic-analysis-of-electro-optic},\n\tdoi = {10.1063/5.0137409},\n\tabstract = {The electro-optic coefficients of ferroelectric materials were obtained by Landau thermodynamic theory. It is proved that if the permittivity tensor is diagonal, then some ratios of the electro-optical coefficients are equal to the ratios of its diagonal components. The dependence of electro-optic coefficients on the external electric field for single-crystal barium titanate was studied and discussed. It is shown that electro-optic coefficients are rather high for barium titanate due to a non-linear response of dielectric susceptibility to electric field strength.},\n\tnumber = {6},\n\tjournal = {Journal of Applied Physics},\n\tauthor = {Shirokov, V. B. and Timoshenko, P. E. and Kalinchuk, V. V.},\n\tmonth = feb,\n\tyear = {2023},\n\tkeywords = {Q2},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The electro-optic coefficients of ferroelectric materials were obtained by Landau thermodynamic theory. It is proved that if the permittivity tensor is diagonal, then some ratios of the electro-optical coefficients are equal to the ratios of its diagonal components. The dependence of electro-optic coefficients on the external electric field for single-crystal barium titanate was studied and discussed. It is shown that electro-optic coefficients are rather high for barium titanate due to a non-linear response of dielectric susceptibility to electric field strength.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-seredin-timoshenko-kalinchuk-popov-theroleofelasticstressduringthermomigrationofliquidzonesbasedonaluminuminsilicon-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://ppp.mech.unn.ru/index.php/ppp/article/view/774\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-seredin-timoshenko-kalinchuk-popov-theroleofelasticstressduringthermomigrationofliquidzonesbasedonaluminuminsilicon-2023', 'http://ppp.mech.unn.ru/index.php/ppp/article/view/774', event);\">\n    The role of elastic stress during thermomigration of liquid zones based on aluminum in silicon.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V.; Seredin, B.; Timoshenko, P.; Kalinchuk, V.;  and Popov, V.\n</span>\n\n  \n\n</span>\n\n  <i>Problems of Strength and Plasticity</i>, 85(3): 426–436.  2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://ppp.mech.unn.ru/index.php/ppp/article/view/774\"\n     onclick=\"log_download('shirokov-seredin-timoshenko-kalinchuk-popov-theroleofelasticstressduringthermomigrationofliquidzonesbasedonaluminuminsilicon-2023', 'http://ppp.mech.unn.ru/index.php/ppp/article/view/774', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"The role of elastic stress during thermomigration of liquid zones based on aluminum in silicon [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.32326/1814-9146-2023-85-3-426-436\"\n     onclick=\"log_download('shirokov-seredin-timoshenko-kalinchuk-popov-theroleofelasticstressduringthermomigrationofliquidzonesbasedonaluminuminsilicon-2023', 'http://doi.org/10.32326/1814-9146-2023-85-3-426-436', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-seredin-timoshenko-kalinchuk-popov-theroleofelasticstressduringthermomigrationofliquidzonesbasedonaluminuminsilicon-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-seredin-timoshenko-kalinchuk-popov-theroleofelasticstressduringthermomigrationofliquidzonesbasedonaluminuminsilicon-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_role_2023,\n\ttitle = {The role of elastic stress during thermomigration of liquid zones based on aluminum in silicon},\n\tvolume = {85},\n\tissn = {18149146},\n\turl = {http://ppp.mech.unn.ru/index.php/ppp/article/view/774},\n\tdoi = {10.32326/1814-9146-2023-85-3-426-436},\n\tabstract = {The method of thermomigration of liquid zones based on aluminum makes it possible to create complex structures of closed channels with boundaries formed from p-n junctions in single-crystal silicon wafers. The channels are characterized by the uniformity of their properties, and the pn junctions are characterized by their sharpness. Such structures are used in high-current electronics, photovoltaics, and microelectromechanical converters. Volumetric deformation inside and outside the channel due to alloying of silicon with aluminum leads to the formation of mechanical stresses. The equilibrium shape of the channels formed at high temperatures is determined by the minimum elastic energy and depends on the material parameters and geometry of the structure. Within the framework of the linear theory of elasticity, the behavior of elastic energy during the formation of the structure of thermomigration channels at high temperatures doped with aluminum in a single-crystalline (001) cut disk was studied. The simulation was performed using the finite element method in the COMSOL Multiphysics mathematical package. The study was carried out for practically important structures in which the direction of the edges is oriented along the diagonal of the square. Only such structures do not have breaks during the process of thermomigration. Based on the calculation results, it was revealed that the minimum elastic energy corresponds to structures with different crystalline orientations inside the channel and outside it – in the main silicon matrix. The direction of the crystalline axes inside the channel, corresponding to the minimum elastic energy, is rotated by 45 degrees in the plane of the disk relative to the direction of the axes of the main matrix of the silicon crystal. In addition, calculations showed that with such a turn, the shape of the channels changes. The minimum elastic energy corresponds not to vertical structures, but to inclined ones. The angle of inclination of the pyramids depends on the width of the channels and the distance between them.},\n\tnumber = {3},\n\tjournal = {Problems of Strength and Plasticity},\n\tauthor = {Shirokov, V.B. and Seredin, B.M. and Timoshenko, P.E. and Kalinchuk, V.V. and Popov, V.P.},\n\tyear = {2023},\n\tkeywords = {Q4},\n\tpages = {426--436},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The method of thermomigration of liquid zones based on aluminum makes it possible to create complex structures of closed channels with boundaries formed from p-n junctions in single-crystal silicon wafers. The channels are characterized by the uniformity of their properties, and the pn junctions are characterized by their sharpness. Such structures are used in high-current electronics, photovoltaics, and microelectromechanical converters. Volumetric deformation inside and outside the channel due to alloying of silicon with aluminum leads to the formation of mechanical stresses. The equilibrium shape of the channels formed at high temperatures is determined by the minimum elastic energy and depends on the material parameters and geometry of the structure. Within the framework of the linear theory of elasticity, the behavior of elastic energy during the formation of the structure of thermomigration channels at high temperatures doped with aluminum in a single-crystalline (001) cut disk was studied. The simulation was performed using the finite element method in the COMSOL Multiphysics mathematical package. The study was carried out for practically important structures in which the direction of the edges is oriented along the diagonal of the square. Only such structures do not have breaks during the process of thermomigration. Based on the calculation results, it was revealed that the minimum elastic energy corresponds to structures with different crystalline orientations inside the channel and outside it – in the main silicon matrix. The direction of the crystalline axes inside the channel, corresponding to the minimum elastic energy, is rotated by 45 degrees in the plane of the disk relative to the direction of the axes of the main matrix of the silicon crystal. In addition, calculations showed that with such a turn, the shape of the channels changes. The minimum elastic energy corresponds not to vertical structures, but to inclined ones. The angle of inclination of the pyramids depends on the width of the channels and the distance between them.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-timoshenko-kalinchuk-bst-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://ered.pstu.ru/index.php/mechanics/article/view/3765\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-timoshenko-kalinchuk-bst-2023', 'https://ered.pstu.ru/index.php/mechanics/article/view/3765', event);\">\n    Генерация поверхностных акустических волн сегнетоэлектрической пленкой BST при действии одноосной нагрузки.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.; Timoshenko, P. E.;  and Kalinchuk, V. V.\n</span>\n\n  \n\n</span>\n\n  <i>PNRPU Mechanics Bulletin</i>, (1): 173–178. December 2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://ered.pstu.ru/index.php/mechanics/article/view/3765\"\n     onclick=\"log_download('shirokov-timoshenko-kalinchuk-bst-2023', 'https://ered.pstu.ru/index.php/mechanics/article/view/3765', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Генерация поверхностных акустических волн сегнетоэлектрической пленкой BST при действии одноосной нагрузки [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.15593/perm.mech/2023.1.16\"\n     onclick=\"log_download('shirokov-timoshenko-kalinchuk-bst-2023', 'http://doi.org/10.15593/perm.mech/2023.1.16', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-timoshenko-kalinchuk-bst-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-timoshenko-kalinchuk-bst-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov__2023,\n\ttitle = {Генерация поверхностных акустических волн сегнетоэлектрической пленкой {BST} при действии одноосной нагрузки},\n\tissn = {2226-1869},\n\turl = {https://ered.pstu.ru/index.php/mechanics/article/view/3765},\n\tdoi = {10.15593/perm.mech/2023.1.16},\n\tabstract = {The electro-mechanical properties of a ferroelectric film of barium strontium titanate (BST) film located on a silicon substrate depend on applied external strain. A significant dependence is observed for concentrations close to values, where a phase transition for the ferroelectric film occurs. A model of single-crystal BST film near the phase transition under uniaxial strain is studied by the thermodynamic theory of phase transitions. The material properties of the film obtained by the model are used for numerical study of the excitation of Rayleigh&#x27; acoustic waves on the surface of the film-substrate heterostructure. Shifting the extrema of S-parameters, characterizing the efficiency of excitation of surface acoustic waves, is shown under the applied strain. The change of S-parameters for the first three resonances determined principally by the geometry of the interdigital electrodes is presented. The largest shift of resonant frequency is observed in a case of the second resonance that corresponds to Sezava wave.},\n\tnumber = {1},\n\tjournal = {PNRPU Mechanics Bulletin},\n\tauthor = {Shirokov, V. B. and Timoshenko, P. E. and Kalinchuk, V. V.},\n\tmonth = dec,\n\tyear = {2023},\n\tkeywords = {Q3},\n\tpages = {173--178},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The electro-mechanical properties of a ferroelectric film of barium strontium titanate (BST) film located on a silicon substrate depend on applied external strain. A significant dependence is observed for concentrations close to values, where a phase transition for the ferroelectric film occurs. A model of single-crystal BST film near the phase transition under uniaxial strain is studied by the thermodynamic theory of phase transitions. The material properties of the film obtained by the model are used for numerical study of the excitation of Rayleigh' acoustic waves on the surface of the film-substrate heterostructure. Shifting the extrema of S-parameters, characterizing the efficiency of excitation of surface acoustic waves, is shown under the applied strain. The change of S-parameters for the first three resonances determined principally by the geometry of the interdigital electrodes is presented. The largest shift of resonant frequency is observed in a case of the second resonance that corresponds to Sezava wave.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"talanov-shirokov-pimenov-talanov-magneticphasediagramsofthepyrochlorebasedmagnetslandautheory-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0304885323003669\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'talanov-shirokov-pimenov-talanov-magneticphasediagramsofthepyrochlorebasedmagnetslandautheory-2023', 'https://linkinghub.elsevier.com/retrieve/pii/S0304885323003669', event);\">\n    Magnetic phase diagrams of the pyrochlore-based magnets: Landau theory.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Talanov, M.; Shirokov, V.; Pimenov, M.;  and Talanov, V.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Magnetism and Magnetic Materials</i>, 575: 170717. June 2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0304885323003669\"\n     onclick=\"log_download('talanov-shirokov-pimenov-talanov-magneticphasediagramsofthepyrochlorebasedmagnetslandautheory-2023', 'https://linkinghub.elsevier.com/retrieve/pii/S0304885323003669', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Magnetic phase diagrams of the pyrochlore-based magnets: Landau theory [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.jmmm.2023.170717\"\n     onclick=\"log_download('talanov-shirokov-pimenov-talanov-magneticphasediagramsofthepyrochlorebasedmagnetslandautheory-2023', 'http://doi.org/10.1016/j.jmmm.2023.170717', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/talanov-shirokov-pimenov-talanov-magneticphasediagramsofthepyrochlorebasedmagnetslandautheory-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('talanov-shirokov-pimenov-talanov-magneticphasediagramsofthepyrochlorebasedmagnetslandautheory-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{talanov_magnetic_2023,\n\ttitle = {Magnetic phase diagrams of the pyrochlore-based magnets: {Landau} theory},\n\tvolume = {575},\n\tissn = {03048853},\n\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0304885323003669},\n\tdoi = {10.1016/j.jmmm.2023.170717},\n\tjournal = {Journal of Magnetism and Magnetic Materials},\n\tauthor = {Talanov, M.V. and Shirokov, V.B. and Pimenov, M.S. and Talanov, V.M.},\n\tmonth = jun,\n\tyear = {2023},\n\tkeywords = {Q2},\n\tpages = {170717},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"talanov-talanov-shirokov-symmetrybasedpredictionofthetypeiimultiferroicswithpyrochlorestructure-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://nanojournal.ifmo.ru/en/articles-2/volume14/14-2/physics/paper09/\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'talanov-talanov-shirokov-symmetrybasedpredictionofthetypeiimultiferroicswithpyrochlorestructure-2023', 'http://nanojournal.ifmo.ru/en/articles-2/volume14/14-2/physics/paper09/', event);\">\n    Symmetry-based prediction of the type-II multiferroics with pyrochlore structure.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Talanov, V.; Talanov, M.;  and Shirokov, V.\n</span>\n\n  \n\n</span>\n\n  <i>Nanosystems: Physics, Chemistry, Mathematics</i>, 14(2): 208–215. April 2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://nanojournal.ifmo.ru/en/articles-2/volume14/14-2/physics/paper09/\"\n     onclick=\"log_download('talanov-talanov-shirokov-symmetrybasedpredictionofthetypeiimultiferroicswithpyrochlorestructure-2023', 'http://nanojournal.ifmo.ru/en/articles-2/volume14/14-2/physics/paper09/', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Symmetry-based prediction of the type-II multiferroics with pyrochlore structure [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.17586/2220-8054-2023-14-2-208-215\"\n     onclick=\"log_download('talanov-talanov-shirokov-symmetrybasedpredictionofthetypeiimultiferroicswithpyrochlorestructure-2023', 'http://doi.org/10.17586/2220-8054-2023-14-2-208-215', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/talanov-talanov-shirokov-symmetrybasedpredictionofthetypeiimultiferroicswithpyrochlorestructure-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('talanov-talanov-shirokov-symmetrybasedpredictionofthetypeiimultiferroicswithpyrochlorestructure-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{talanov_symmetry-based_2023,\n\ttitle = {Symmetry-based prediction of the type-{II} multiferroics with pyrochlore structure},\n\tvolume = {14},\n\tissn = {22208054},\n\turl = {http://nanojournal.ifmo.ru/en/articles-2/volume14/14-2/physics/paper09/},\n\tdoi = {10.17586/2220-8054-2023-14-2-208-215},\n\tnumber = {2},\n\tjournal = {Nanosystems: Physics, Chemistry, Mathematics},\n\tauthor = {Talanov, V.M. and Talanov, M.V. and Shirokov, V.B.},\n\tmonth = apr,\n\tyear = {2023},\n\tkeywords = {Q3},\n\tpages = {208--215},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"talanov-shirokov-talanov-spininducedferroelasticswithpyrochlorelattices-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.tandfonline.com/doi/full/10.1080/00150193.2023.2211291\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'talanov-shirokov-talanov-spininducedferroelasticswithpyrochlorelattices-2023', 'https://www.tandfonline.com/doi/full/10.1080/00150193.2023.2211291', event);\">\n    Spin-induced ferroelastics with pyrochlore lattices.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Talanov, M. V.; Shirokov, V. B.;  and Talanov, V. M.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 612(1): 1–9. August 2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.tandfonline.com/doi/full/10.1080/00150193.2023.2211291\"\n     onclick=\"log_download('talanov-shirokov-talanov-spininducedferroelasticswithpyrochlorelattices-2023', 'https://www.tandfonline.com/doi/full/10.1080/00150193.2023.2211291', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Spin-induced ferroelastics with pyrochlore lattices [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150193.2023.2211291\"\n     onclick=\"log_download('talanov-shirokov-talanov-spininducedferroelasticswithpyrochlorelattices-2023', 'http://doi.org/10.1080/00150193.2023.2211291', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/talanov-shirokov-talanov-spininducedferroelasticswithpyrochlorelattices-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('talanov-shirokov-talanov-spininducedferroelasticswithpyrochlorelattices-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{talanov_spin-induced_2023,\n\ttitle = {Spin-induced ferroelastics with pyrochlore lattices},\n\tvolume = {612},\n\tissn = {0015-0193},\n\turl = {https://www.tandfonline.com/doi/full/10.1080/00150193.2023.2211291},\n\tdoi = {10.1080/00150193.2023.2211291},\n\tnumber = {1},\n\tjournal = {Ferroelectrics},\n\tauthor = {Talanov, M. V. and Shirokov, V. B. and Talanov, V. M.},\n\tmonth = aug,\n\tyear = {2023},\n\tkeywords = {Q4},\n\tpages = {1--9},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"talanov-shirokov-talanov-spinorderonthepyrochlorelatticemagneticcrystallographylandauthermodynamicsandemergentphenomena-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S1359645423005177\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'talanov-shirokov-talanov-spinorderonthepyrochlorelatticemagneticcrystallographylandauthermodynamicsandemergentphenomena-2023', 'https://linkinghub.elsevier.com/retrieve/pii/S1359645423005177', event);\">\n    Spin order on the pyrochlore lattice: Magnetic crystallography, Landau thermodynamics and emergent phenomena.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Talanov, M. V.; Shirokov, V. B.;  and Talanov, V. M.\n</span>\n\n  \n\n</span>\n\n  <i>Acta Materialia</i>, 259: 119187. October 2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S1359645423005177\"\n     onclick=\"log_download('talanov-shirokov-talanov-spinorderonthepyrochlorelatticemagneticcrystallographylandauthermodynamicsandemergentphenomena-2023', 'https://linkinghub.elsevier.com/retrieve/pii/S1359645423005177', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Spin order on the pyrochlore lattice: Magnetic crystallography, Landau thermodynamics and emergent phenomena [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.actamat.2023.119187\"\n     onclick=\"log_download('talanov-shirokov-talanov-spinorderonthepyrochlorelatticemagneticcrystallographylandauthermodynamicsandemergentphenomena-2023', 'http://doi.org/10.1016/j.actamat.2023.119187', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/talanov-shirokov-talanov-spinorderonthepyrochlorelatticemagneticcrystallographylandauthermodynamicsandemergentphenomena-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('talanov-shirokov-talanov-spinorderonthepyrochlorelatticemagneticcrystallographylandauthermodynamicsandemergentphenomena-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{talanov_spin_2023,\n\ttitle = {Spin order on the pyrochlore lattice: {Magnetic} crystallography, {Landau} thermodynamics and emergent phenomena},\n\tvolume = {259},\n\tissn = {13596454},\n\turl = {https://linkinghub.elsevier.com/retrieve/pii/S1359645423005177},\n\tdoi = {10.1016/j.actamat.2023.119187},\n\tjournal = {Acta Materialia},\n\tauthor = {Talanov, Mikhail V. and Shirokov, Vladimir B. and Talanov, Valeriy M.},\n\tmonth = oct,\n\tyear = {2023},\n\tkeywords = {Q1},\n\tpages = {119187},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----mgtitextrm2otextrm4-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://www.niic.nsc.ru/phocadownload/Conferences/2023/TiM-2023/2023 Tezisy Termodinamika.pdf#page=122\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----mgtitextrm2otextrm4-2023', 'http://www.niic.nsc.ru/phocadownload/Conferences/2023/TiM-2023/2023 Tezisy Termodinamika.pdf#page=122', event);\">\n    Мультипорядок, термодинамика и кристаллохимия тетрагональной фазы MgTi$_{\\textrm{2}}$O$_{\\textrm{4}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Таланов, В.; Таланов, М.; Авакян, Л. А.;  and Широков, В. Б.\n</span>\n\n  \n\n</span>\n\n  In <i>Термодинамика и материаловедение. Тезисы докладов XV Симпозиума с международным участием</i>, pages 121,  2023. NIIC SB RAS\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://www.niic.nsc.ru/phocadownload/Conferences/2023/TiM-2023/2023 Tezisy Termodinamika.pdf#page=122\"\n     onclick=\"log_download('----mgtitextrm2otextrm4-2023', 'http://www.niic.nsc.ru/phocadownload/Conferences/2023/TiM-2023/2023 Tezisy Termodinamika.pdf#page=122', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Мультипорядок, термодинамика и кристаллохимия тетрагональной фазы MgTi$_{\\textrm{2}}$O$_{\\textrm{4}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.26902/THERM_2023_101\"\n     onclick=\"log_download('----mgtitextrm2otextrm4-2023', 'http://doi.org/10.26902/THERM_2023_101', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----mgtitextrm2otextrm4-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----mgtitextrm2otextrm4-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{__2023,\n\ttitle = {Мультипорядок, термодинамика и кристаллохимия тетрагональной фазы {MgTi}$_{\\textrm{2}}${O}$_{\\textrm{4}}$},\n\tisbn = {978-5-901688-53-3},\n\turl = {http://www.niic.nsc.ru/phocadownload/Conferences/2023/TiM-2023/2023 Tezisy Termodinamika.pdf#page=122},\n\tdoi = {10.26902/THERM_2023_101},\n\tbooktitle = {Термодинамика и материаловедение. Тезисы докладов {XV} Симпозиума с международным участием},\n\tpublisher = {NIIC SB RAS},\n\tauthor = {Таланов, В.М. and Таланов, М.В. and Авакян, Л. А. and Широков, В. Б.},\n\tyear = {2023},\n\tpages = {121},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  Поверхностные эффекты в наноразмерных сегнетоэлектрических гетероструктурах.\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Калинчук, В.; Тимошенко, П.;  and Широков, В.\n</span>\n\n  \n\n</span>\n\n  In <i>XIII Всероссийский съезд по теоретической и прикладной механике. Санкт-Петербург, 21-25 августа</i>, pages Т.4, С.670–672,  2023. \n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{__2023-1,\n\ttitle = {Поверхностные эффекты в наноразмерных сегнетоэлектрических гетероструктурах},\n\tbooktitle = {{XIII} Всероссийский съезд по теоретической и прикладной механике. Санкт-Петербург, 21-25 августа},\n\tauthor = {Калинчук, В.В. and Тимошенко, П.Е. and Широков, В.Б.},\n\tyear = {2023},\n\tpages = {Т.4, С.670--672},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  О перспективных для систем мониторинга слоистых структурах с сегнетоэлектрическим поверхностным слоем.\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Тимошенко, П.; Широков, В.;  and Калинчук, В.\n</span>\n\n  \n\n</span>\n\n  In <i>XIII Всероссийский съезд по теоретической и прикладной механике. Санкт- Петербург, 21-25 августа</i>, pages Т.4, С.741–743,  2023. \n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n\n  \n  <a href=\"http://doi.org/10.18720/SPBPU/2/id23-630\"\n     onclick=\"log_download('----2023', 'http://doi.org/10.18720/SPBPU/2/id23-630', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{__2023-2,\n\ttitle = {О перспективных для систем мониторинга слоистых структурах с сегнетоэлектрическим поверхностным слоем},\n\tdoi = {10.18720/SPBPU/2/id23-630},\n\tbooktitle = {{XIII} Всероссийский съезд по теоретической и прикладной механике. Санкт- Петербург, 21-25 августа},\n\tauthor = {Тимошенко, П.Е. and Широков, В.Б. and Калинчук, В.В.},\n\tyear = {2023},\n\tpages = {Т.4, С.741--743},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"talanov-shirokov-talanov-aulov-multiorderandthestructuralmechanismofthelirhtextrm2otextrm4tetragonalphaseformation-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.springer.com/10.3103/S1062873823703136\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'talanov-shirokov-talanov-aulov-multiorderandthestructuralmechanismofthelirhtextrm2otextrm4tetragonalphaseformation-2023', 'https://link.springer.com/10.3103/S1062873823703136', event);\">\n    Multiorder and the Structural Mechanism of the LiRh$_{\\textrm{2}}$O$_{\\textrm{4}}$ Tetragonal Phase Formation.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Talanov, M. V.; Shirokov, V. B.; Talanov, V. M.;  and Aulov, M. S.\n</span>\n\n  \n\n</span>\n\n  <i>Bulletin of the Russian Academy of Sciences: Physics</i>, 87(9): 1263–1269. September 2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.springer.com/10.3103/S1062873823703136\"\n     onclick=\"log_download('talanov-shirokov-talanov-aulov-multiorderandthestructuralmechanismofthelirhtextrm2otextrm4tetragonalphaseformation-2023', 'https://link.springer.com/10.3103/S1062873823703136', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Multiorder and the Structural Mechanism of the LiRh$_{\\textrm{2}}$O$_{\\textrm{4}}$ Tetragonal Phase Formation [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3103/S1062873823703136\"\n     onclick=\"log_download('talanov-shirokov-talanov-aulov-multiorderandthestructuralmechanismofthelirhtextrm2otextrm4tetragonalphaseformation-2023', 'http://doi.org/10.3103/S1062873823703136', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/talanov-shirokov-talanov-aulov-multiorderandthestructuralmechanismofthelirhtextrm2otextrm4tetragonalphaseformation-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('talanov-shirokov-talanov-aulov-multiorderandthestructuralmechanismofthelirhtextrm2otextrm4tetragonalphaseformation-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{talanov_multiorder_2023,\n\ttitle = {Multiorder and the {Structural} {Mechanism} of the {LiRh}$_{\\textrm{2}}${O}$_{\\textrm{4}}$ {Tetragonal} {Phase} {Formation}},\n\tvolume = {87},\n\tissn = {1062-8738},\n\turl = {https://link.springer.com/10.3103/S1062873823703136},\n\tdoi = {10.3103/S1062873823703136},\n\tnumber = {9},\n\tjournal = {Bulletin of the Russian Academy of Sciences: Physics},\n\tauthor = {Talanov, M. V. and Shirokov, V. B. and Talanov, V. M. and Aulov, M. S.},\n\tmonth = sep,\n\tyear = {2023},\n\tkeywords = {Q3},\n\tpages = {1263--1269},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  Определение электрооптических коэффициентов титаната бария.\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Широков, В. Б.; Тимошенко, П. Е.;  and Калинчук, В. В.\n</span>\n\n  \n\n</span>\n\n  <i>Доклады Российской Академии Наук. Физика, Технические науки</i>, 510: 38–43.  2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n\n  \n  <a href=\"http://doi.org/10.31857/S2686740023030148\"\n     onclick=\"log_download('----2023', 'http://doi.org/10.31857/S2686740023030148', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2023-3,\n\ttitle = {Определение электрооптических коэффициентов титаната бария},\n\tvolume = {510},\n\tdoi = {10.31857/S2686740023030148},\n\tjournal = {Доклады Российской Академии Наук. Физика, Технические науки},\n\tauthor = {Широков, В. Б. and Тимошенко, П. Е. and Калинчук, В. В.},\n\tyear = {2023},\n\tpages = {38--43},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kaydashev-khlebtsov-kutepov-nikolskiy-kozakov-konstantinov-mikheykin-karapetyan-etal-photothermaleffectandphasetransitioninvotextrm2enhancedbyplasmonicparticles-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.mdpi.com/1996-1944/16/7/2579\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kaydashev-khlebtsov-kutepov-nikolskiy-kozakov-konstantinov-mikheykin-karapetyan-etal-photothermaleffectandphasetransitioninvotextrm2enhancedbyplasmonicparticles-2023', 'https://www.mdpi.com/1996-1944/16/7/2579', event);\">\n    Photothermal Effect and Phase Transition in VO$_{\\textrm{2}}$ Enhanced by Plasmonic Particles.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kaydashev, V.; Khlebtsov, B.; Kutepov, M.; Nikolskiy, A.; Kozakov, A.; Konstantinov, A.; Mikheykin, A.; Karapetyan, G.;  and Kaidashev, E.\n</span>\n\n  \n\n</span>\n\n  <i>Materials</i>, 16(7): 2579. March 2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.mdpi.com/1996-1944/16/7/2579\"\n     onclick=\"log_download('kaydashev-khlebtsov-kutepov-nikolskiy-kozakov-konstantinov-mikheykin-karapetyan-etal-photothermaleffectandphasetransitioninvotextrm2enhancedbyplasmonicparticles-2023', 'https://www.mdpi.com/1996-1944/16/7/2579', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Photothermal Effect and Phase Transition in VO$_{\\textrm{2}}$ Enhanced by Plasmonic Particles [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3390/ma16072579\"\n     onclick=\"log_download('kaydashev-khlebtsov-kutepov-nikolskiy-kozakov-konstantinov-mikheykin-karapetyan-etal-photothermaleffectandphasetransitioninvotextrm2enhancedbyplasmonicparticles-2023', 'http://doi.org/10.3390/ma16072579', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kaydashev-khlebtsov-kutepov-nikolskiy-kozakov-konstantinov-mikheykin-karapetyan-etal-photothermaleffectandphasetransitioninvotextrm2enhancedbyplasmonicparticles-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kaydashev-khlebtsov-kutepov-nikolskiy-kozakov-konstantinov-mikheykin-karapetyan-etal-photothermaleffectandphasetransitioninvotextrm2enhancedbyplasmonicparticles-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kaydashev_photothermal_2023,\n\ttitle = {Photothermal Effect and Phase Transition in {VO}$_{\\textrm{2}}$ Enhanced by {Plasmonic} {Particles}},\n\tvolume = {16},\n\tissn = {1996-1944},\n\turl = {https://www.mdpi.com/1996-1944/16/7/2579},\n\tdoi = {10.3390/ma16072579},\n\tabstract = {Phase change metasurfaces based on VO2, which are pre-heated with electric current and optically addressed by projected structured light hologram, are considered to become a new paradigm in programmed THz/middle IR flat optics. Macroscopic quasi-homogeneous arrays of Au nanoparticles show large near IR absorption and a significant photothermal effect capable of boosting a light-triggered switching of VO2 and are to be carefully examined. We propose a new approach to simultaneously probe the altered temperature and electric conductivity of a hybrid Au particle-VO2 film composite by monitoring a phase shift and attenuating a surface acoustic wave in a YX128° cut LiNbO3 substrate. The method shows a temperature resolution of 0.1 °C comparable with the best existing techniques for studying nanoobjects and surfaces. The laser-induced photothermal effects were characterized in a macroscopic array of Au nanostars (AuNSts) with different surface coverage. In a monolayer of 10 nm Au, coupled plasmonic nanoparticles were deposited on the LiNbO3 substrate. An optically triggered insulator-metal transition assisted by photothermal effect in AuNSts/VO2/TiO2/LiNbO3 composites was studied at varied light power. We believe that the proposed SAW-based method is of significant importance for the characterization and optimization of radiation absorbing or/and electrically heated elements of metasurfaces and other devices for lab-on-chip and optical communication/processor technology.},\n\tnumber = {7},\n\tjournal = {Materials},\n\tauthor = {Kaydashev, Vladimir and Khlebtsov, Boris and Kutepov, Maxim and Nikolskiy, Anatoliy and Kozakov, Alexey and Konstantinov, Alexey and Mikheykin, Alexey and Karapetyan, Gevork and Kaidashev, Evgeni},\n\tmonth = mar,\n\tyear = {2023},\n\tkeywords = {Q2},\n\tpages = {2579},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Phase change metasurfaces based on VO2, which are pre-heated with electric current and optically addressed by projected structured light hologram, are considered to become a new paradigm in programmed THz/middle IR flat optics. Macroscopic quasi-homogeneous arrays of Au nanoparticles show large near IR absorption and a significant photothermal effect capable of boosting a light-triggered switching of VO2 and are to be carefully examined. We propose a new approach to simultaneously probe the altered temperature and electric conductivity of a hybrid Au particle-VO2 film composite by monitoring a phase shift and attenuating a surface acoustic wave in a YX128° cut LiNbO3 substrate. The method shows a temperature resolution of 0.1 °C comparable with the best existing techniques for studying nanoobjects and surfaces. The laser-induced photothermal effects were characterized in a macroscopic array of Au nanostars (AuNSts) with different surface coverage. In a monolayer of 10 nm Au, coupled plasmonic nanoparticles were deposited on the LiNbO3 substrate. An optically triggered insulator-metal transition assisted by photothermal effect in AuNSts/VO2/TiO2/LiNbO3 composites was studied at varied light power. We believe that the proposed SAW-based method is of significant importance for the characterization and optimization of radiation absorbing or/and electrically heated elements of metasurfaces and other devices for lab-on-chip and optical communication/processor technology.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"alekseenko-pavlets-mikheykin-belenov-guterman-theintegratedapproachtostudyingthemicrostructureofdealloyedptcucelectrocatalystsforpemfcs-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0169433223012175\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'alekseenko-pavlets-mikheykin-belenov-guterman-theintegratedapproachtostudyingthemicrostructureofdealloyedptcucelectrocatalystsforpemfcs-2023', 'https://linkinghub.elsevier.com/retrieve/pii/S0169433223012175', event);\">\n    The integrated approach to studying the microstructure of de-alloyed PtCu/C electrocatalysts for PEMFCs.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Alekseenko, A.; Pavlets, A.; Mikheykin, A.; Belenov, S.;  and Guterman, E.\n</span>\n\n  \n\n</span>\n\n  <i>Applied Surface Science</i>, 631: 157539. September 2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0169433223012175\"\n     onclick=\"log_download('alekseenko-pavlets-mikheykin-belenov-guterman-theintegratedapproachtostudyingthemicrostructureofdealloyedptcucelectrocatalystsforpemfcs-2023', 'https://linkinghub.elsevier.com/retrieve/pii/S0169433223012175', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"The integrated approach to studying the microstructure of de-alloyed PtCu/C electrocatalysts for PEMFCs [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.apsusc.2023.157539\"\n     onclick=\"log_download('alekseenko-pavlets-mikheykin-belenov-guterman-theintegratedapproachtostudyingthemicrostructureofdealloyedptcucelectrocatalystsforpemfcs-2023', 'http://doi.org/10.1016/j.apsusc.2023.157539', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/alekseenko-pavlets-mikheykin-belenov-guterman-theintegratedapproachtostudyingthemicrostructureofdealloyedptcucelectrocatalystsforpemfcs-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('alekseenko-pavlets-mikheykin-belenov-guterman-theintegratedapproachtostudyingthemicrostructureofdealloyedptcucelectrocatalystsforpemfcs-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{alekseenko_integrated_2023,\n\ttitle = {The integrated approach to studying the microstructure of de-alloyed {PtCu}/{C} electrocatalysts for {PEMFCs}},\n\tvolume = {631},\n\tissn = {01694332},\n\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0169433223012175},\n\tdoi = {10.1016/j.apsusc.2023.157539},\n\tjournal = {Applied Surface Science},\n\tauthor = {Alekseenko, A.A. and Pavlets, A.S. and Mikheykin, A.S. and Belenov, S.V. and Guterman, E.V.},\n\tmonth = sep,\n\tyear = {2023},\n\tkeywords = {Q1},\n\tpages = {157539},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"konstantinov-linnik-razumnaya-mikheykin-latticedynamicsandphasetransitionspeculiaritiesofbatextrmxsrtextrm1xtiotextrm3solidsolutionswithhighsrcontent-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0921452623000765\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'konstantinov-linnik-razumnaya-mikheykin-latticedynamicsandphasetransitionspeculiaritiesofbatextrmxsrtextrm1xtiotextrm3solidsolutionswithhighsrcontent-2023', 'https://linkinghub.elsevier.com/retrieve/pii/S0921452623000765', event);\">\n    Lattice dynamics and phase transitions peculiarities of Ba$_{\\textrm{x}}$Sr$_{\\textrm{1-x}}$TiO$_{\\textrm{3}}$ solid solutions with high Sr content.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Konstantinov, A.; Linnik, E.; Razumnaya, A.;  and Mikheykin, A.\n</span>\n\n  \n\n</span>\n\n  <i>Physica B: Condensed Matter</i>, 654: 414709. April 2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0921452623000765\"\n     onclick=\"log_download('konstantinov-linnik-razumnaya-mikheykin-latticedynamicsandphasetransitionspeculiaritiesofbatextrmxsrtextrm1xtiotextrm3solidsolutionswithhighsrcontent-2023', 'https://linkinghub.elsevier.com/retrieve/pii/S0921452623000765', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Lattice dynamics and phase transitions peculiarities of Ba$_{\\textrm{x}}$Sr$_{\\textrm{1-x}}$TiO$_{\\textrm{3}}$ solid solutions with high Sr content [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.physb.2023.414709\"\n     onclick=\"log_download('konstantinov-linnik-razumnaya-mikheykin-latticedynamicsandphasetransitionspeculiaritiesofbatextrmxsrtextrm1xtiotextrm3solidsolutionswithhighsrcontent-2023', 'http://doi.org/10.1016/j.physb.2023.414709', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/konstantinov-linnik-razumnaya-mikheykin-latticedynamicsandphasetransitionspeculiaritiesofbatextrmxsrtextrm1xtiotextrm3solidsolutionswithhighsrcontent-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('konstantinov-linnik-razumnaya-mikheykin-latticedynamicsandphasetransitionspeculiaritiesofbatextrmxsrtextrm1xtiotextrm3solidsolutionswithhighsrcontent-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{konstantinov_lattice_2023,\n\ttitle = {Lattice dynamics and phase transitions peculiarities of {Ba}$_{\\textrm{x}}${Sr}$_{\\textrm{1-x}}${TiO}$_{\\textrm{3}}$ solid solutions with high {Sr} content},\n\tvolume = {654},\n\tissn = {09214526},\n\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0921452623000765},\n\tdoi = {10.1016/j.physb.2023.414709},\n\tjournal = {Physica B: Condensed Matter},\n\tauthor = {Konstantinov, A.S. and Linnik, E.D. and Razumnaya, A.G. and Mikheykin, A.S.},\n\tmonth = apr,\n\tyear = {2023},\n\tkeywords = {Q2},\n\tpages = {414709},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"angadi-pasha-aldossari-elgawaad-abdulvakhidov-lyanguzov-khadke-highperformancelpgsensingbehaviourofcocrtextrm2xcetextrmxotextrm4x0to002forsensorapplications-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.springer.com/10.1007/s10854-022-09725-1\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'angadi-pasha-aldossari-elgawaad-abdulvakhidov-lyanguzov-khadke-highperformancelpgsensingbehaviourofcocrtextrm2xcetextrmxotextrm4x0to002forsensorapplications-2023', 'https://link.springer.com/10.1007/s10854-022-09725-1', event);\">\n    High-performance LPG sensing behaviour of CoCr$_{\\textrm{2-x}}$Ce$_{\\textrm{x}}$O$_{\\textrm{4}}$ (x = 0 to 0.02) for sensor applications.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Angadi, V. J.; Pasha, A.; Al-Dossari, M.; EL-Gawaad, N. S. A.; Abdulvakhidov, K.; Lyanguzov, N.;  and Khadke, U. K.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Materials Science: Materials in Electronics</i>, 34(4): 318. February 2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.springer.com/10.1007/s10854-022-09725-1\"\n     onclick=\"log_download('angadi-pasha-aldossari-elgawaad-abdulvakhidov-lyanguzov-khadke-highperformancelpgsensingbehaviourofcocrtextrm2xcetextrmxotextrm4x0to002forsensorapplications-2023', 'https://link.springer.com/10.1007/s10854-022-09725-1', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"High-performance LPG sensing behaviour of CoCr$_{\\textrm{2-x}}$Ce$_{\\textrm{x}}$O$_{\\textrm{4}}$ (x = 0 to 0.02) for sensor applications [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1007/s10854-022-09725-1\"\n     onclick=\"log_download('angadi-pasha-aldossari-elgawaad-abdulvakhidov-lyanguzov-khadke-highperformancelpgsensingbehaviourofcocrtextrm2xcetextrmxotextrm4x0to002forsensorapplications-2023', 'http://doi.org/10.1007/s10854-022-09725-1', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/angadi-pasha-aldossari-elgawaad-abdulvakhidov-lyanguzov-khadke-highperformancelpgsensingbehaviourofcocrtextrm2xcetextrmxotextrm4x0to002forsensorapplications-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('angadi-pasha-aldossari-elgawaad-abdulvakhidov-lyanguzov-khadke-highperformancelpgsensingbehaviourofcocrtextrm2xcetextrmxotextrm4x0to002forsensorapplications-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{angadi_high-performance_2023,\n\ttitle = {High-performance {LPG} sensing behaviour of {CoCr}$_{\\textrm{2-x}}${Ce}$_{\\textrm{x}}${O}$_{\\textrm{4}}$ (x = 0 to 0.02) for sensor applications},\n\tvolume = {34},\n\tissn = {0957-4522},\n\turl = {https://link.springer.com/10.1007/s10854-022-09725-1},\n\tdoi = {10.1007/s10854-022-09725-1},\n\tnumber = {4},\n\tjournal = {Journal of Materials Science: Materials in Electronics},\n\tauthor = {Angadi, V. Jagadeesha and Pasha, Apsar and Al-Dossari, M. and EL-Gawaad, N. S. Abd and Abdulvakhidov, Kamaludin and Lyanguzov, Nikolay and Khadke, Uday Kumar},\n\tmonth = feb,\n\tyear = {2023},\n\tkeywords = {Q2},\n\tpages = {318},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"andryushin-mazuritsky-galatova-ilina-soboleva-nagaenko-shilkina-dudkina-etal-evolutionofthemacroresponsesduringthetransitionfromtwotosixcomponentsystemsofthesolidsolutionswithfundamentallydifferentproperties-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0272884223019983\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'andryushin-mazuritsky-galatova-ilina-soboleva-nagaenko-shilkina-dudkina-etal-evolutionofthemacroresponsesduringthetransitionfromtwotosixcomponentsystemsofthesolidsolutionswithfundamentallydifferentproperties-2023', 'https://linkinghub.elsevier.com/retrieve/pii/S0272884223019983', event);\">\n    Evolution of the macroresponses during the transition from two-to six-component systems of the solid solutions with fundamentally different properties.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Andryushin, K.; Mazuritsky, M.; Galatova, A.; Il'ina, M.; Soboleva, O.; Nagaenko, A.; Shilkina, L.; Dudkina, S.; Andryushina, I.; Rudskaya, A.; Khasbulatov, S.; Sadykov, K.;  and Reznichenko, L.\n</span>\n\n  \n\n</span>\n\n  <i>Ceramics International</i>, 49(19): 31265–31275. October 2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0272884223019983\"\n     onclick=\"log_download('andryushin-mazuritsky-galatova-ilina-soboleva-nagaenko-shilkina-dudkina-etal-evolutionofthemacroresponsesduringthetransitionfromtwotosixcomponentsystemsofthesolidsolutionswithfundamentallydifferentproperties-2023', 'https://linkinghub.elsevier.com/retrieve/pii/S0272884223019983', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Evolution of the macroresponses during the transition from two-to six-component systems of the solid solutions with fundamentally different properties [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.ceramint.2023.07.074\"\n     onclick=\"log_download('andryushin-mazuritsky-galatova-ilina-soboleva-nagaenko-shilkina-dudkina-etal-evolutionofthemacroresponsesduringthetransitionfromtwotosixcomponentsystemsofthesolidsolutionswithfundamentallydifferentproperties-2023', 'http://doi.org/10.1016/j.ceramint.2023.07.074', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/andryushin-mazuritsky-galatova-ilina-soboleva-nagaenko-shilkina-dudkina-etal-evolutionofthemacroresponsesduringthetransitionfromtwotosixcomponentsystemsofthesolidsolutionswithfundamentallydifferentproperties-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('andryushin-mazuritsky-galatova-ilina-soboleva-nagaenko-shilkina-dudkina-etal-evolutionofthemacroresponsesduringthetransitionfromtwotosixcomponentsystemsofthesolidsolutionswithfundamentallydifferentproperties-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{andryushin_evolution_2023,\n\ttitle = {Evolution of the macroresponses during the transition from two-to six-component systems of the solid solutions with fundamentally different properties},\n\tvolume = {49},\n\tissn = {02728842},\n\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0272884223019983},\n\tdoi = {10.1016/j.ceramint.2023.07.074},\n\tnumber = {19},\n\tjournal = {Ceramics International},\n\tauthor = {Andryushin, K.P. and Mazuritsky, M.I. and Galatova, A.O. and Il&#x27;ina, M.V. and Soboleva, O.I. and Nagaenko, A.V. and Shilkina, L.A. and Dudkina, S.I. and Andryushina, I.N. and Rudskaya, A.G. and Khasbulatov, S.V. and Sadykov, Kh.A. and Reznichenko, L.A.},\n\tmonth = oct,\n\tyear = {2023},\n\tkeywords = {Q1},\n\tpages = {31265--31275},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"lebedinskaya-rudskaya-parametersstructurecalculationofnonstoichiometricpbmgtextrm1ynbtextrmyotextrm3zsolidsolutions-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://aip.scitation.org/doi/abs/10.1063/5.0115358\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'lebedinskaya-rudskaya-parametersstructurecalculationofnonstoichiometricpbmgtextrm1ynbtextrmyotextrm3zsolidsolutions-2023', 'http://aip.scitation.org/doi/abs/10.1063/5.0115358', event);\">\n    Parameters structure calculation of nonstoichiometric Pb(Mg$_{\\textrm{1-y}}$Nb$_{\\textrm{y}}$)O$_{\\textrm{3-z}}$ solid solutions.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Lebedinskaya, A.;  and Rudskaya, A.\n</span>\n\n  \n\n</span>\n\n  In pages 040003,  2023. \n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://aip.scitation.org/doi/abs/10.1063/5.0115358\"\n     onclick=\"log_download('lebedinskaya-rudskaya-parametersstructurecalculationofnonstoichiometricpbmgtextrm1ynbtextrmyotextrm3zsolidsolutions-2023', 'http://aip.scitation.org/doi/abs/10.1063/5.0115358', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Parameters structure calculation of nonstoichiometric Pb(Mg$_{\\textrm{1-y}}$Nb$_{\\textrm{y}}$)O$_{\\textrm{3-z}}$ solid solutions [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/5.0115358\"\n     onclick=\"log_download('lebedinskaya-rudskaya-parametersstructurecalculationofnonstoichiometricpbmgtextrm1ynbtextrmyotextrm3zsolidsolutions-2023', 'http://doi.org/10.1063/5.0115358', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/lebedinskaya-rudskaya-parametersstructurecalculationofnonstoichiometricpbmgtextrm1ynbtextrmyotextrm3zsolidsolutions-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('lebedinskaya-rudskaya-parametersstructurecalculationofnonstoichiometricpbmgtextrm1ynbtextrmyotextrm3zsolidsolutions-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{lebedinskaya_parameters_2023,\n\ttitle = {Parameters structure calculation of nonstoichiometric {Pb}({Mg}$_{\\textrm{1-y}}${Nb}$_{\\textrm{y}}$){O}$_{\\textrm{3-z}}$ solid solutions},\n\turl = {http://aip.scitation.org/doi/abs/10.1063/5.0115358},\n\tdoi = {10.1063/5.0115358},\n\tauthor = {Lebedinskaya, Alla and Rudskaya, Angela},\n\tyear = {2023},\n\tpages = {040003},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"konstantin-palatnikov-shilkina-nagaenko-shcherbina-smirnov-sidorov-kubrin-etal-multifunctionalmaterialsbasedonthesolidsolutionsofthenakcdtextrm05nbotextrm33knncdsystemmodifiedwithrareearthelementscrystalstructuremicrostructureandmacroresponses-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.mdpi.com/2571-6131/6/1/21\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'konstantin-palatnikov-shilkina-nagaenko-shcherbina-smirnov-sidorov-kubrin-etal-multifunctionalmaterialsbasedonthesolidsolutionsofthenakcdtextrm05nbotextrm33knncdsystemmodifiedwithrareearthelementscrystalstructuremicrostructureandmacroresponses-2023', 'https://www.mdpi.com/2571-6131/6/1/21', event);\">\n    Multifunctional Materials Based on the Solid Solutions of the (Na, K, Cd$_{\\textrm{0.5}}$)NbO$_{\\textrm{3}}$3 (KNN-Cd) System Modified with Rare Earth Elements: Crystal Structure, Microstructure, and Macroresponses.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Konstantin, A.; Palatnikov, M.; Shilkina, L.; Nagaenko, A.; Shcherbina, O.; Smirnov, M.; Sidorov, N.; Kubrin, S.; Rudskaya, A.; Rudskiy, D.;  and Reznichenko, L.\n</span>\n\n  \n\n</span>\n\n  <i>Ceramics</i>, 6(1): 342–363. February 2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.mdpi.com/2571-6131/6/1/21\"\n     onclick=\"log_download('konstantin-palatnikov-shilkina-nagaenko-shcherbina-smirnov-sidorov-kubrin-etal-multifunctionalmaterialsbasedonthesolidsolutionsofthenakcdtextrm05nbotextrm33knncdsystemmodifiedwithrareearthelementscrystalstructuremicrostructureandmacroresponses-2023', 'https://www.mdpi.com/2571-6131/6/1/21', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Multifunctional Materials Based on the Solid Solutions of the (Na, K, Cd$_{\\textrm{0.5}}$)NbO$_{\\textrm{3}}$3 (KNN-Cd) System Modified with Rare Earth Elements: Crystal Structure, Microstructure, and Macroresponses [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3390/ceramics6010021\"\n     onclick=\"log_download('konstantin-palatnikov-shilkina-nagaenko-shcherbina-smirnov-sidorov-kubrin-etal-multifunctionalmaterialsbasedonthesolidsolutionsofthenakcdtextrm05nbotextrm33knncdsystemmodifiedwithrareearthelementscrystalstructuremicrostructureandmacroresponses-2023', 'http://doi.org/10.3390/ceramics6010021', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/konstantin-palatnikov-shilkina-nagaenko-shcherbina-smirnov-sidorov-kubrin-etal-multifunctionalmaterialsbasedonthesolidsolutionsofthenakcdtextrm05nbotextrm33knncdsystemmodifiedwithrareearthelementscrystalstructuremicrostructureandmacroresponses-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('konstantin-palatnikov-shilkina-nagaenko-shcherbina-smirnov-sidorov-kubrin-etal-multifunctionalmaterialsbasedonthesolidsolutionsofthenakcdtextrm05nbotextrm33knncdsystemmodifiedwithrareearthelementscrystalstructuremicrostructureandmacroresponses-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{konstantin_multifunctional_2023,\n\ttitle = {Multifunctional {Materials} {Based} on the {Solid} {Solutions} of the ({Na}, {K}, {Cd}$_{\\textrm{0.5}}$){NbO}$_{\\textrm{3}}$3 ({KNN}-{Cd}) {System} {Modified} with {Rare} {Earth} {Elements}: {Crystal} {Structure}, {Microstructure}, and {Macroresponses}},\n\tvolume = {6},\n\tissn = {2571-6131},\n\turl = {https://www.mdpi.com/2571-6131/6/1/21},\n\tdoi = {10.3390/ceramics6010021},\n\tabstract = {Ceramic samples of polycomponent solid solutions (SSs) Na0.90K0.05Cd0.05NbO3 (Cd-modified KNN) and [(Na0.90K0.05Cd0.05)0.95REE0.05]NbO3, where REE = La, Pr, Tb, Dy, Ho, were obtained by the uniaxial hot pressing (UHP) method. The crystal lattice structures, morphological features of the microstructure, and dielectric and thermophysical properties of these ceramics have been investigated. For the first time, their strength characteristics (Young&#x27;s modulus) and the critical stress intensity factor of the mode I Kic have been estimated. Photoluminescent properties have been compared in SSs [(Na0.90K0.05Cd0.05)0.95REE0.05]NbO3 in the visible wavelength range.},\n\tnumber = {1},\n\tjournal = {Ceramics},\n\tauthor = {Konstantin, Andryushin and Palatnikov, Mikhail and Shilkina, Lidiya and Nagaenko, Alexandr and Shcherbina, Olga and Smirnov, Maxim and Sidorov, Nikolay and Kubrin, Stanislav and Rudskaya, Anzhela and Rudskiy, Daniil and Reznichenko, Larisa},\n\tmonth = feb,\n\tyear = {2023},\n\tkeywords = {Q2},\n\tpages = {342--363},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Ceramic samples of polycomponent solid solutions (SSs) Na0.90K0.05Cd0.05NbO3 (Cd-modified KNN) and [(Na0.90K0.05Cd0.05)0.95REE0.05]NbO3, where REE = La, Pr, Tb, Dy, Ho, were obtained by the uniaxial hot pressing (UHP) method. The crystal lattice structures, morphological features of the microstructure, and dielectric and thermophysical properties of these ceramics have been investigated. For the first time, their strength characteristics (Young's modulus) and the critical stress intensity factor of the mode I Kic have been estimated. Photoluminescent properties have been compared in SSs [(Na0.90K0.05Cd0.05)0.95REE0.05]NbO3 in the visible wavelength range.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"sidorenko-rudskaya-babenko-natkhin-galatova-rudsky-radioabsorbingpropertiesof1xbifeotextrm3xlamnotextrm301x09solidsolutions-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.tandfonline.com/doi/full/10.1080/00150193.2023.2189843\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'sidorenko-rudskaya-babenko-natkhin-galatova-rudsky-radioabsorbingpropertiesof1xbifeotextrm3xlamnotextrm301x09solidsolutions-2023', 'https://www.tandfonline.com/doi/full/10.1080/00150193.2023.2189843', event);\">\n    Radio-absorbing properties of (1- x )BiFeO$_{\\textrm{3-x}}$LaMnO$_{\\textrm{3}}$ (0.1 ≤ x ≤ 0.9) solid solutions.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Sidorenko, E. N.; Rudskaya, A. G.; Babenko, A. A.; Natkhin, I. I.; Galatova, A. O.;  and Rudsky, D. I.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 606(1): 50–60. April 2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.tandfonline.com/doi/full/10.1080/00150193.2023.2189843\"\n     onclick=\"log_download('sidorenko-rudskaya-babenko-natkhin-galatova-rudsky-radioabsorbingpropertiesof1xbifeotextrm3xlamnotextrm301x09solidsolutions-2023', 'https://www.tandfonline.com/doi/full/10.1080/00150193.2023.2189843', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Radio-absorbing properties of (1- x )BiFeO$_{\\textrm{3-x}}$LaMnO$_{\\textrm{3}}$ (0.1 ≤ x ≤ 0.9) solid solutions [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150193.2023.2189843\"\n     onclick=\"log_download('sidorenko-rudskaya-babenko-natkhin-galatova-rudsky-radioabsorbingpropertiesof1xbifeotextrm3xlamnotextrm301x09solidsolutions-2023', 'http://doi.org/10.1080/00150193.2023.2189843', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/sidorenko-rudskaya-babenko-natkhin-galatova-rudsky-radioabsorbingpropertiesof1xbifeotextrm3xlamnotextrm301x09solidsolutions-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('sidorenko-rudskaya-babenko-natkhin-galatova-rudsky-radioabsorbingpropertiesof1xbifeotextrm3xlamnotextrm301x09solidsolutions-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{sidorenko_radio-absorbing_2023,\n\ttitle = {Radio-absorbing properties of (1- x ){BiFeO}$_{\\textrm{3-x}}${LaMnO}$_{\\textrm{3}}$ (0.1 ≤ x ≤ 0.9) solid solutions},\n\tvolume = {606},\n\tissn = {0015-0193},\n\turl = {https://www.tandfonline.com/doi/full/10.1080/00150193.2023.2189843},\n\tdoi = {10.1080/00150193.2023.2189843},\n\tnumber = {1},\n\tjournal = {Ferroelectrics},\n\tauthor = {Sidorenko, E. N. and Rudskaya, A. G. and Babenko, A. A. and Natkhin, I. I. and Galatova, A. O. and Rudsky, D. I.},\n\tmonth = apr,\n\tyear = {2023},\n\tkeywords = {Q4},\n\tpages = {50--60},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"sidorenko-rudskaya-natkhin-rudsky-shpanko-investigationofthemicrowavepropertiesofthetransparentpiezoceramicsplzt-2023\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.springer.com/10.1007/978-3-031-21572-8_16\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'sidorenko-rudskaya-natkhin-rudsky-shpanko-investigationofthemicrowavepropertiesofthetransparentpiezoceramicsplzt-2023', 'https://link.springer.com/10.1007/978-3-031-21572-8_16', event);\">\n    Investigation of the Microwave Properties of the Transparent Piezoceramics PLZT.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Sidorenko, E. N.; Rudskaya, A. G.; Natkhin, I. I.; Rudsky, D. I.;  and Shpanko, S. P.\n</span>\n\n  \n\n</span>\n\n  In pages 189–196.  2023.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.springer.com/10.1007/978-3-031-21572-8_16\"\n     onclick=\"log_download('sidorenko-rudskaya-natkhin-rudsky-shpanko-investigationofthemicrowavepropertiesofthetransparentpiezoceramicsplzt-2023', 'https://link.springer.com/10.1007/978-3-031-21572-8_16', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Investigation of the Microwave Properties of the Transparent Piezoceramics PLZT [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1007/978-3-031-21572-8_16\"\n     onclick=\"log_download('sidorenko-rudskaya-natkhin-rudsky-shpanko-investigationofthemicrowavepropertiesofthetransparentpiezoceramicsplzt-2023', 'http://doi.org/10.1007/978-3-031-21572-8_16', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/sidorenko-rudskaya-natkhin-rudsky-shpanko-investigationofthemicrowavepropertiesofthetransparentpiezoceramicsplzt-2023\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('sidorenko-rudskaya-natkhin-rudsky-shpanko-investigationofthemicrowavepropertiesofthetransparentpiezoceramicsplzt-2023')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@incollection{sidorenko_investigation_2023,\n\ttitle = {Investigation of the {Microwave} {Properties} of the {Transparent} {Piezoceramics} {PLZT}},\n\turl = {https://link.springer.com/10.1007/978-3-031-21572-8_16},\n\tauthor = {Sidorenko, E. N. and Rudskaya, A. G. and Natkhin, I. I. and Rudsky, D. I. and Shpanko, S. P.},\n\tyear = {2023},\n\tdoi = {10.1007/978-3-031-21572-8_16},\n\tpages = {189--196},\n}\n</pre>\n</div>\n\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2022\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2022')\"\n      onkeypress=\"toggleGroup('group_2022')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2022</span>\n      <span class=\"bibbase_group_count\">\n        \n        (21)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"kuriganova-kubanova-leontyev-molodtsova-smirnova-pulseelectrolysistechniqueforpreparationofbimetaltincontainingelectrocatalyticmaterials-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.mdpi.com/2073-4344/12/11/1444\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kuriganova-kubanova-leontyev-molodtsova-smirnova-pulseelectrolysistechniqueforpreparationofbimetaltincontainingelectrocatalyticmaterials-2022', 'https://www.mdpi.com/2073-4344/12/11/1444', event);\">\n    Pulse Electrolysis Technique for Preparation of Bimetal Tin-Containing Electrocatalytic Materials.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kuriganova, A.; Kubanova, M.; Leontyev, I.; Molodtsova, T.;  and Smirnova, N.\n</span>\n\n  \n\n</span>\n\n  <i>Catalysts</i>, 12(11): 1444. November 2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.mdpi.com/2073-4344/12/11/1444\"\n     onclick=\"log_download('kuriganova-kubanova-leontyev-molodtsova-smirnova-pulseelectrolysistechniqueforpreparationofbimetaltincontainingelectrocatalyticmaterials-2022', 'https://www.mdpi.com/2073-4344/12/11/1444', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Pulse Electrolysis Technique for Preparation of Bimetal Tin-Containing Electrocatalytic Materials [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3390/catal12111444\"\n     onclick=\"log_download('kuriganova-kubanova-leontyev-molodtsova-smirnova-pulseelectrolysistechniqueforpreparationofbimetaltincontainingelectrocatalyticmaterials-2022', 'http://doi.org/10.3390/catal12111444', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kuriganova-kubanova-leontyev-molodtsova-smirnova-pulseelectrolysistechniqueforpreparationofbimetaltincontainingelectrocatalyticmaterials-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kuriganova-kubanova-leontyev-molodtsova-smirnova-pulseelectrolysistechniqueforpreparationofbimetaltincontainingelectrocatalyticmaterials-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kuriganova_pulse_2022,\n\ttitle = {Pulse {Electrolysis} {Technique} for {Preparation} of {Bimetal} {Tin}-{Containing} {Electrocatalytic} {Materials}},\n\tvolume = {12},\n\tissn = {2073-4344},\n\turl = {https://www.mdpi.com/2073-4344/12/11/1444},\n\tdoi = {10.3390/catal12111444},\n\tabstract = {Platinum–tin-containing materials are the most popular catalysts for processes occurring in fuel cells with direct ethanol oxidation. Pulse electrolysis based on the electrochemical dispersion of platinum electrodes under the influence of alternating pulse current in an alkaline electrolyte made it possible to introduce the tin component into the catalyst in the form of a dopant, an alloy with platinum, and in the form of an oxide phase and evaluate the effect of the form in which tin is present in the catalyst on its microstructural and electrocatalytic characteristics. The introduction of tin into the catalyst generally increases the rate of ethanol electrooxidation; however, with the most prominent effect observed when tin is present in form of an oxide.},\n\tlanguage = {en},\n\tnumber = {11},\n\turldate = {2023-11-11},\n\tjournal = {Catalysts},\n\tauthor = {Kuriganova, Alexandra and Kubanova, Marina and Leontyev, Igor and Molodtsova, Tatiana and Smirnova, Nina},\n\tmonth = nov,\n\tyear = {2022},\n\tpages = {1444},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\BTS2JHFX\\\\Kuriganova и др. - 2022 - Pulse Electrolysis Technique for Preparation of Bi.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Platinum–tin-containing materials are the most popular catalysts for processes occurring in fuel cells with direct ethanol oxidation. Pulse electrolysis based on the electrochemical dispersion of platinum electrodes under the influence of alternating pulse current in an alkaline electrolyte made it possible to introduce the tin component into the catalyst in the form of a dopant, an alloy with platinum, and in the form of an oxide phase and evaluate the effect of the form in which tin is present in the catalyst on its microstructural and electrocatalytic characteristics. The introduction of tin into the catalyst generally increases the rate of ethanol electrooxidation; however, with the most prominent effect observed when tin is present in form of an oxide.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"gerasimova-belenov-lyanguzov-pankov-tolstunov-pavlets-roleofthepotentialrangeduringstresstestingofplatinumcontainingelectrocatalystsatelevatedtemperature-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.mdpi.com/2073-4344/12/10/1179\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'gerasimova-belenov-lyanguzov-pankov-tolstunov-pavlets-roleofthepotentialrangeduringstresstestingofplatinumcontainingelectrocatalystsatelevatedtemperature-2022', 'https://www.mdpi.com/2073-4344/12/10/1179', event);\">\n    Role of the Potential Range during Stress Testing of Platinum-Containing Electrocatalysts at Elevated Temperature.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Gerasimova, I.; Belenov, S.; Lyanguzov, N.; Pankov, I.; Tolstunov, M.;  and Pavlets, A.\n</span>\n\n  \n\n</span>\n\n  <i>Catalysts</i>, 12(10): 1179. October 2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.mdpi.com/2073-4344/12/10/1179\"\n     onclick=\"log_download('gerasimova-belenov-lyanguzov-pankov-tolstunov-pavlets-roleofthepotentialrangeduringstresstestingofplatinumcontainingelectrocatalystsatelevatedtemperature-2022', 'https://www.mdpi.com/2073-4344/12/10/1179', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Role of the Potential Range during Stress Testing of Platinum-Containing Electrocatalysts at Elevated Temperature [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3390/catal12101179\"\n     onclick=\"log_download('gerasimova-belenov-lyanguzov-pankov-tolstunov-pavlets-roleofthepotentialrangeduringstresstestingofplatinumcontainingelectrocatalystsatelevatedtemperature-2022', 'http://doi.org/10.3390/catal12101179', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/gerasimova-belenov-lyanguzov-pankov-tolstunov-pavlets-roleofthepotentialrangeduringstresstestingofplatinumcontainingelectrocatalystsatelevatedtemperature-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('gerasimova-belenov-lyanguzov-pankov-tolstunov-pavlets-roleofthepotentialrangeduringstresstestingofplatinumcontainingelectrocatalystsatelevatedtemperature-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{gerasimova_role_2022,\n\ttitle = {Role of the {Potential} {Range} during {Stress} {Testing} of {Platinum}-{Containing} {Electrocatalysts} at {Elevated} {Temperature}},\n\tvolume = {12},\n\tissn = {2073-4344},\n\turl = {https://www.mdpi.com/2073-4344/12/10/1179},\n\tdoi = {10.3390/catal12101179},\n\tabstract = {The durability of low temperature proton exchange membrane fuel cell (PEMFC) catalysts crucially affects their lifetime. The choice of carbon support is important in terms of increasing the stability of catalysts. In this research, Pt/C samples were obtained using the polyol synthesis method on two types of carbon supports: the standard support, Vulcan XC-72, and carbon support with a high degree of graphitization, ECS-002402. One method for assessing structural characteristics is through transmission electron microscopy (TEM), according to which materials G1 and G2 showed an average nanoparticle size of 3.7 and 4.2 nm, respectively. On all catalysts, the oxygen reduction reaction proceeded according to the four electron mechanism. Durability was assessed by changes in ESA and activity in the ORR after 1000 cycles, with changes in the upper potential values: 0.7; 1.0; 1.2; and 1.4 V. After accelerated stress testing, the G1 material showed the greatest residual activity at a potential of 1.4 V (165 A/g (Pt). Based on the results of comparing various ADT protocols, the optimal mode of 0.4 and 1.4 V was chosen, and should be used for further studies comparing the durability of Pt/C catalysts.},\n\tlanguage = {en},\n\tnumber = {10},\n\turldate = {2023-11-11},\n\tjournal = {Catalysts},\n\tauthor = {Gerasimova, Irina and Belenov, Sergey and Lyanguzov, Nikolai and Pankov, Ilya and Tolstunov, Mikhail and Pavlets, Angelina},\n\tmonth = oct,\n\tyear = {2022},\n\tpages = {1179},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\IERK75HA\\\\Gerasimova и др. - 2022 - Role of the Potential Range during Stress Testing .pdf:application/pdf;Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\G3CGGG63\\\\Gerasimova и др. - 2022 - Role of the Potential Range during Stress Testing .pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The durability of low temperature proton exchange membrane fuel cell (PEMFC) catalysts crucially affects their lifetime. The choice of carbon support is important in terms of increasing the stability of catalysts. In this research, Pt/C samples were obtained using the polyol synthesis method on two types of carbon supports: the standard support, Vulcan XC-72, and carbon support with a high degree of graphitization, ECS-002402. One method for assessing structural characteristics is through transmission electron microscopy (TEM), according to which materials G1 and G2 showed an average nanoparticle size of 3.7 and 4.2 nm, respectively. On all catalysts, the oxygen reduction reaction proceeded according to the four electron mechanism. Durability was assessed by changes in ESA and activity in the ORR after 1000 cycles, with changes in the upper potential values: 0.7; 1.0; 1.2; and 1.4 V. After accelerated stress testing, the G1 material showed the greatest residual activity at a potential of 1.4 V (165 A/g (Pt). Based on the results of comparing various ADT protocols, the optimal mode of 0.4 and 1.4 V was chosen, and should be used for further studies comparing the durability of Pt/C catalysts.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"andryushin-dudkina-sahoo-shilkina-alyoshin-triger-andryushina-verbenko-etal-theinfluenceoftheelementalcompositioncrystalstructureandgrainstructureoftheferropiezoceramicsofvariousdegreesoftheferrohardnessonthestabilityofthepolarizedstate-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.mdpi.com/1996-1944/15/6/2118\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'andryushin-dudkina-sahoo-shilkina-alyoshin-triger-andryushina-verbenko-etal-theinfluenceoftheelementalcompositioncrystalstructureandgrainstructureoftheferropiezoceramicsofvariousdegreesoftheferrohardnessonthestabilityofthepolarizedstate-2022', 'https://www.mdpi.com/1996-1944/15/6/2118', event);\">\n    The Influence of the Elemental Composition, Crystal Structure, and Grain Structure of the Ferro-Piezoceramics of Various Degrees of the Ferro-Hardness on the Stability of the Polarized State.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Andryushin, K.; Dudkina, S.; Sahoo, S.; Shilkina, L.; Alyoshin, V.; Triger, E.; Andryushina, I.; Verbenko, I.; Rudskiy, D.; Rudskaya, A.;  and Reznichenko, L.\n</span>\n\n  \n\n</span>\n\n  <i>Materials</i>, 15(6): 2118. March 2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.mdpi.com/1996-1944/15/6/2118\"\n     onclick=\"log_download('andryushin-dudkina-sahoo-shilkina-alyoshin-triger-andryushina-verbenko-etal-theinfluenceoftheelementalcompositioncrystalstructureandgrainstructureoftheferropiezoceramicsofvariousdegreesoftheferrohardnessonthestabilityofthepolarizedstate-2022', 'https://www.mdpi.com/1996-1944/15/6/2118', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"The Influence of the Elemental Composition, Crystal Structure, and Grain Structure of the Ferro-Piezoceramics of Various Degrees of the Ferro-Hardness on the Stability of the Polarized State [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3390/ma15062118\"\n     onclick=\"log_download('andryushin-dudkina-sahoo-shilkina-alyoshin-triger-andryushina-verbenko-etal-theinfluenceoftheelementalcompositioncrystalstructureandgrainstructureoftheferropiezoceramicsofvariousdegreesoftheferrohardnessonthestabilityofthepolarizedstate-2022', 'http://doi.org/10.3390/ma15062118', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/andryushin-dudkina-sahoo-shilkina-alyoshin-triger-andryushina-verbenko-etal-theinfluenceoftheelementalcompositioncrystalstructureandgrainstructureoftheferropiezoceramicsofvariousdegreesoftheferrohardnessonthestabilityofthepolarizedstate-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('andryushin-dudkina-sahoo-shilkina-alyoshin-triger-andryushina-verbenko-etal-theinfluenceoftheelementalcompositioncrystalstructureandgrainstructureoftheferropiezoceramicsofvariousdegreesoftheferrohardnessonthestabilityofthepolarizedstate-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{andryushin_influence_2022,\n\ttitle = {The {Influence} of the {Elemental} {Composition}, {Crystal} {Structure}, and {Grain} {Structure} of the {Ferro}-{Piezoceramics} of {Various} {Degrees} of the {Ferro}-{Hardness} on the {Stability} of the {Polarized} {State}},\n\tvolume = {15},\n\tissn = {1996-1944},\n\turl = {https://www.mdpi.com/1996-1944/15/6/2118},\n\tdoi = {10.3390/ma15062118},\n\tabstract = {Ferro-piezoceramic materials (FPCM) with different degrees of ferrohardness were fabricated by double solid-phase synthesis followed by the sintering technique using hot pressing method. The X-ray studies carried out in a wide temperature range showed that with increasing temperature, each of the studied FPCM undergoes a series of phase transformations, accompanied by a change in the symmetry of the unit cell. In this case, near the phase transition to the nonpolar cubic phase, in each of the FPCM, the formation of a fuzzy symmetry region is observed, which is characterized by weak distortions and temperature–time instability of the crystal structure. The study of the piezoelectric modulus d33 in the quasi-static regime as a function of temperature made it possible to reveal the different nature of its behavior in materials of various degrees of ferrohardness. It was shown that the conservation of the state in ferrosoft materials above the Curie temperature is associated with the relaxation nature of the change in their properties, the existence of a region of fuzzy symmetry (noncubic phase) in them above the Curie temperature, and increased inertia of the system. The expediency of taking into account the presented results in the development of electromechanical converters based on FPCM of various degrees of ferrohardness, operated under temperature effects, including cyclic ones, was shown.},\n\tlanguage = {en},\n\tnumber = {6},\n\turldate = {2023-11-11},\n\tjournal = {Materials},\n\tauthor = {Andryushin, Konstantin and Dudkina, Svetlana and Sahoo, Sushrisangita and Shilkina, Lidiya and Alyoshin, Vladimir and Triger, Ekaterina and Andryushina, Inna and Verbenko, Iliya and Rudskiy, Daniil and Rudskaya, Angela and Reznichenko, Larisa},\n\tmonth = mar,\n\tyear = {2022},\n\tpages = {2118},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\G8H4F7ND\\\\Andryushin и др. - 2022 - The Influence of the Elemental Composition, Crysta.pdf:application/pdf;Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\J7PHWKJD\\\\Andryushin и др. - 2022 - The Influence of the Elemental Composition, Crysta.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Ferro-piezoceramic materials (FPCM) with different degrees of ferrohardness were fabricated by double solid-phase synthesis followed by the sintering technique using hot pressing method. The X-ray studies carried out in a wide temperature range showed that with increasing temperature, each of the studied FPCM undergoes a series of phase transformations, accompanied by a change in the symmetry of the unit cell. In this case, near the phase transition to the nonpolar cubic phase, in each of the FPCM, the formation of a fuzzy symmetry region is observed, which is characterized by weak distortions and temperature–time instability of the crystal structure. The study of the piezoelectric modulus d33 in the quasi-static regime as a function of temperature made it possible to reveal the different nature of its behavior in materials of various degrees of ferrohardness. It was shown that the conservation of the state in ferrosoft materials above the Curie temperature is associated with the relaxation nature of the change in their properties, the existence of a region of fuzzy symmetry (noncubic phase) in them above the Curie temperature, and increased inertia of the system. The expediency of taking into account the presented results in the development of electromechanical converters based on FPCM of various degrees of ferrohardness, operated under temperature effects, including cyclic ones, was shown.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"konevtsova-roshal-rochal-moirpatternsandcarbonnanotubesorting-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://iopscience.iop.org/article/10.1088/2399-1984/ac4a27\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'konevtsova-roshal-rochal-moirpatternsandcarbonnanotubesorting-2022', 'https://iopscience.iop.org/article/10.1088/2399-1984/ac4a27', event);\">\n    Moiré patterns and carbon nanotube sorting.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Konevtsova, O. V; Roshal, D. S;  and Rochal, S. B\n</span>\n\n  \n\n</span>\n\n  <i>Nano Futures</i>, 6(1): 015005. March 2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://iopscience.iop.org/article/10.1088/2399-1984/ac4a27\"\n     onclick=\"log_download('konevtsova-roshal-rochal-moirpatternsandcarbonnanotubesorting-2022', 'https://iopscience.iop.org/article/10.1088/2399-1984/ac4a27', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Moiré patterns and carbon nanotube sorting [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/2399-1984/ac4a27\"\n     onclick=\"log_download('konevtsova-roshal-rochal-moirpatternsandcarbonnanotubesorting-2022', 'http://doi.org/10.1088/2399-1984/ac4a27', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/konevtsova-roshal-rochal-moirpatternsandcarbonnanotubesorting-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('konevtsova-roshal-rochal-moirpatternsandcarbonnanotubesorting-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{konevtsova_moire_2022,\n\ttitle = {Moiré patterns and carbon nanotube sorting},\n\tvolume = {6},\n\tissn = {2399-1984},\n\turl = {https://iopscience.iop.org/article/10.1088/2399-1984/ac4a27},\n\tdoi = {10.1088/2399-1984/ac4a27},\n\tabstract = {Abstract\n            Moiré patterns (MPs), arising from the superposition of two lattices with close periods, are tightly related to the physicochemical properties of bilayer nanostructures. Here, we develop the theory of complex MPs emerging in twisted bilayer graphene and planar nets of double-walled nanotubes at significant relative twist and/or deformation of layers. The proposed theory clarifies the physicochemical regularities arising at sorting of single-walled carbon nanotubes (SWCNTs) by organic molecules, which self-assemble in regular coatings on both the tubes and planar graphene. We introduce and consider an outer tubular virtual lattice that is a parent structure for the deposited coating and due to this fact, its existence is crucial for the coating formation. As we show, such outer lattices exist only for successfully sorted SWCNTs and the superposition between the outer lattice and SWCNT forms a specific long-period MP. We explain known experimental results of SWCNT sorting by molecules of flavin group, poly(9,9-dioctylfluorene-2,7-diyl), and poly [(m-phenylenevinylene)-alt-(p-phenylenevinylene)]. Also, our approach points out other organic molecules and polymers suitable for effective carbon nanotube sorting.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Nano Futures},\n\tauthor = {Konevtsova, Olga V and Roshal, Daria S and Rochal, Sergei B},\n\tmonth = mar,\n\tyear = {2022},\n\tpages = {015005},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Abstract Moiré patterns (MPs), arising from the superposition of two lattices with close periods, are tightly related to the physicochemical properties of bilayer nanostructures. Here, we develop the theory of complex MPs emerging in twisted bilayer graphene and planar nets of double-walled nanotubes at significant relative twist and/or deformation of layers. The proposed theory clarifies the physicochemical regularities arising at sorting of single-walled carbon nanotubes (SWCNTs) by organic molecules, which self-assemble in regular coatings on both the tubes and planar graphene. We introduce and consider an outer tubular virtual lattice that is a parent structure for the deposited coating and due to this fact, its existence is crucial for the coating formation. As we show, such outer lattices exist only for successfully sorted SWCNTs and the superposition between the outer lattice and SWCNT forms a specific long-period MP. We explain known experimental results of SWCNT sorting by molecules of flavin group, poly(9,9-dioctylfluorene-2,7-diyl), and poly [(m-phenylenevinylene)-alt-(p-phenylenevinylene)]. Also, our approach points out other organic molecules and polymers suitable for effective carbon nanotube sorting.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"chalin-levshov-myasnikova-rochal-tightbindingapproximationforbilayergrapheneandnanotubestructuresfromcommensurabilitytoincommensurabilitybetweenthelayers-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.105.045402\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'chalin-levshov-myasnikova-rochal-tightbindingapproximationforbilayergrapheneandnanotubestructuresfromcommensurabilitytoincommensurabilitybetweenthelayers-2022', 'https://link.aps.org/doi/10.1103/PhysRevB.105.045402', event);\">\n    Tight-binding approximation for bilayer graphene and nanotube structures: From commensurability to incommensurability between the layers.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Chalin, D. V.; Levshov, D. I.; Myasnikova, A. E.;  and Rochal, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 105(4): 045402. January 2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.105.045402\"\n     onclick=\"log_download('chalin-levshov-myasnikova-rochal-tightbindingapproximationforbilayergrapheneandnanotubestructuresfromcommensurabilitytoincommensurabilitybetweenthelayers-2022', 'https://link.aps.org/doi/10.1103/PhysRevB.105.045402', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Tight-binding approximation for bilayer graphene and nanotube structures: From commensurability to incommensurability between the layers [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.105.045402\"\n     onclick=\"log_download('chalin-levshov-myasnikova-rochal-tightbindingapproximationforbilayergrapheneandnanotubestructuresfromcommensurabilitytoincommensurabilitybetweenthelayers-2022', 'http://doi.org/10.1103/PhysRevB.105.045402', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/chalin-levshov-myasnikova-rochal-tightbindingapproximationforbilayergrapheneandnanotubestructuresfromcommensurabilitytoincommensurabilitybetweenthelayers-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('chalin-levshov-myasnikova-rochal-tightbindingapproximationforbilayergrapheneandnanotubestructuresfromcommensurabilitytoincommensurabilitybetweenthelayers-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{chalin_tight-binding_2022,\n\ttitle = {Tight-binding approximation for bilayer graphene and nanotube structures: {From} commensurability to incommensurability between the layers},\n\tvolume = {105},\n\tissn = {2469-9950, 2469-9969},\n\tshorttitle = {Tight-binding approximation for bilayer graphene and nanotube structures},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.105.045402},\n\tdoi = {10.1103/PhysRevB.105.045402},\n\tlanguage = {en},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Chalin, D. V. and Levshov, D. I. and Myasnikova, A. E. and Rochal, S. B.},\n\tmonth = jan,\n\tyear = {2022},\n\tpages = {045402},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\MDNW4VT5\\\\Chalin и др. - 2022 - Tight-binding approximation for bilayer graphene a.pdf:application/pdf;Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\VM6EQJBB\\\\Chalin и др. - 2022 - Tight-binding approximation for bilayer graphene a.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-timoshenko-kalinchuk-efficiencyofgenerationofsurfaceacousticwavesinbariumstrontiumtitanatethinfilms-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://ieeexplore.ieee.org/document/9744607/\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-timoshenko-kalinchuk-efficiencyofgenerationofsurfaceacousticwavesinbariumstrontiumtitanatethinfilms-2022', 'https://ieeexplore.ieee.org/document/9744607/', event);\">\n    Efficiency of Generation of Surface Acoustic Waves in Barium Strontium Titanate Thin Films.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.; Timoshenko, P. E.;  and Kalinchuk, V. V.\n</span>\n\n  \n\n</span>\n\n  <i>IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control</i>, 69(5): 1815–1820. May 2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://ieeexplore.ieee.org/document/9744607/\"\n     onclick=\"log_download('shirokov-timoshenko-kalinchuk-efficiencyofgenerationofsurfaceacousticwavesinbariumstrontiumtitanatethinfilms-2022', 'https://ieeexplore.ieee.org/document/9744607/', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Efficiency of Generation of Surface Acoustic Waves in Barium Strontium Titanate Thin Films [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1109/TUFFC.2022.3163610\"\n     onclick=\"log_download('shirokov-timoshenko-kalinchuk-efficiencyofgenerationofsurfaceacousticwavesinbariumstrontiumtitanatethinfilms-2022', 'http://doi.org/10.1109/TUFFC.2022.3163610', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-timoshenko-kalinchuk-efficiencyofgenerationofsurfaceacousticwavesinbariumstrontiumtitanatethinfilms-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-timoshenko-kalinchuk-efficiencyofgenerationofsurfaceacousticwavesinbariumstrontiumtitanatethinfilms-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_efficiency_2022,\n\ttitle = {Efficiency of {Generation} of {Surface} {Acoustic} {Waves} in {Barium} {Strontium} {Titanate} {Thin} {Films}},\n\tvolume = {69},\n\tissn = {0885-3010, 1525-8955},\n\turl = {https://ieeexplore.ieee.org/document/9744607/},\n\tdoi = {10.1109/TUFFC.2022.3163610},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control},\n\tauthor = {Shirokov, Vladimir B. and Timoshenko, Pavel E. and Kalinchuk, Valery V.},\n\tmonth = may,\n\tyear = {2022},\n\tpages = {1815--1820},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"roshal-martin-fedorenko-golushko-molle-baghdiguian-rochal-randomnatureofepithelialcancercellmonolayers-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://royalsocietypublishing.org/doi/10.1098/rsif.2022.0026\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'roshal-martin-fedorenko-golushko-molle-baghdiguian-rochal-randomnatureofepithelialcancercellmonolayers-2022', 'https://royalsocietypublishing.org/doi/10.1098/rsif.2022.0026', event);\">\n    Random nature of epithelial cancer cell monolayers.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Roshal, D. S.; Martin, M.; Fedorenko, K.; Golushko, I.; Molle, V.; Baghdiguian, S.;  and Rochal, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of The Royal Society Interface</i>, 19(190): 20220026. May 2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://royalsocietypublishing.org/doi/10.1098/rsif.2022.0026\"\n     onclick=\"log_download('roshal-martin-fedorenko-golushko-molle-baghdiguian-rochal-randomnatureofepithelialcancercellmonolayers-2022', 'https://royalsocietypublishing.org/doi/10.1098/rsif.2022.0026', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Random nature of epithelial cancer cell monolayers [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1098/rsif.2022.0026\"\n     onclick=\"log_download('roshal-martin-fedorenko-golushko-molle-baghdiguian-rochal-randomnatureofepithelialcancercellmonolayers-2022', 'http://doi.org/10.1098/rsif.2022.0026', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/roshal-martin-fedorenko-golushko-molle-baghdiguian-rochal-randomnatureofepithelialcancercellmonolayers-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>1 download</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('roshal-martin-fedorenko-golushko-molle-baghdiguian-rochal-randomnatureofepithelialcancercellmonolayers-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{roshal_random_2022,\n\ttitle = {Random nature of epithelial cancer cell monolayers},\n\tvolume = {19},\n\tissn = {1742-5662},\n\turl = {https://royalsocietypublishing.org/doi/10.1098/rsif.2022.0026},\n\tdoi = {10.1098/rsif.2022.0026},\n\tabstract = {Although the polygonal shape of epithelial cells has been drawing the attention of scientists for several centuries, only a decade and a half ago it was demonstrated that distributions of polygon types (DOPTs) are similar in proliferative epithelia of many different plant and animal species. In this study, we show that hyper-proliferation of cancer cells disrupts this universal paradigm and results in randomly organized epithelial structures. Examining non-synchronized and synchronized HeLa cervix cells, we suppose that the spread of cell sizes is the main parameter controlling the DOPT in the cancer cell monolayers. To test this hypothesis, we develop a theory of morphologically similar random polygonal packings. By analysing differences between tumoural and normal epithelial cell monolayers, we conclude that the latter have more ordered structures because of their lower proliferation rates and, consequently, more effective relaxation of mechanical stress associated with cell division and growth. To explain the structural features of normal proliferative epithelium, we take into account the spread of cell sizes in the monolayer. The proposed theory also rationalizes some highly ordered unconventional post-mitotic epithelia.},\n\tlanguage = {en},\n\tnumber = {190},\n\turldate = {2023-11-11},\n\tjournal = {Journal of The Royal Society Interface},\n\tauthor = {Roshal, Daria S. and Martin, Marianne and Fedorenko, Kirill and Golushko, Ivan and Molle, Virginie and Baghdiguian, Stephen and Rochal, Sergei B.},\n\tmonth = may,\n\tyear = {2022},\n\tpages = {20220026},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\9ZQ6KFAD\\\\Roshal и др. - 2022 - Random nature of epithelial cancer cell monolayers.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Although the polygonal shape of epithelial cells has been drawing the attention of scientists for several centuries, only a decade and a half ago it was demonstrated that distributions of polygon types (DOPTs) are similar in proliferative epithelia of many different plant and animal species. In this study, we show that hyper-proliferation of cancer cells disrupts this universal paradigm and results in randomly organized epithelial structures. Examining non-synchronized and synchronized HeLa cervix cells, we suppose that the spread of cell sizes is the main parameter controlling the DOPT in the cancer cell monolayers. To test this hypothesis, we develop a theory of morphologically similar random polygonal packings. By analysing differences between tumoural and normal epithelial cell monolayers, we conclude that the latter have more ordered structures because of their lower proliferation rates and, consequently, more effective relaxation of mechanical stress associated with cell division and growth. To explain the structural features of normal proliferative epithelium, we take into account the spread of cell sizes in the monolayer. The proposed theory also rationalizes some highly ordered unconventional post-mitotic epithelia.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"andryushin-shilkina-khasbulatov-nagaenko-dudkina-andryushina-sadykov-verbenko-etal-theeffectsofthemodificationofthebstsystemsolidsolutionswithrareearthelements-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0272884221030534\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'andryushin-shilkina-khasbulatov-nagaenko-dudkina-andryushina-sadykov-verbenko-etal-theeffectsofthemodificationofthebstsystemsolidsolutionswithrareearthelements-2022', 'https://linkinghub.elsevier.com/retrieve/pii/S0272884221030534', event);\">\n    The effects of the modification of the BST-system solid solutions with rare earth elements.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Andryushin, K.; Shilkina, L.; Khasbulatov, S.; Nagaenko, A.; Dudkina, S.; Andryushina, I.; Sadykov, K.; Verbenko, I.; Rudskaya, A.;  and Reznichenko, L.\n</span>\n\n  \n\n</span>\n\n  <i>Ceramics International</i>, 48(2): 1642–1658. January 2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0272884221030534\"\n     onclick=\"log_download('andryushin-shilkina-khasbulatov-nagaenko-dudkina-andryushina-sadykov-verbenko-etal-theeffectsofthemodificationofthebstsystemsolidsolutionswithrareearthelements-2022', 'https://linkinghub.elsevier.com/retrieve/pii/S0272884221030534', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"The effects of the modification of the BST-system solid solutions with rare earth elements [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.ceramint.2021.09.243\"\n     onclick=\"log_download('andryushin-shilkina-khasbulatov-nagaenko-dudkina-andryushina-sadykov-verbenko-etal-theeffectsofthemodificationofthebstsystemsolidsolutionswithrareearthelements-2022', 'http://doi.org/10.1016/j.ceramint.2021.09.243', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/andryushin-shilkina-khasbulatov-nagaenko-dudkina-andryushina-sadykov-verbenko-etal-theeffectsofthemodificationofthebstsystemsolidsolutionswithrareearthelements-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('andryushin-shilkina-khasbulatov-nagaenko-dudkina-andryushina-sadykov-verbenko-etal-theeffectsofthemodificationofthebstsystemsolidsolutionswithrareearthelements-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{andryushin_effects_2022,\n\ttitle = {The effects of the modification of the {BST}-system solid solutions with rare earth elements},\n\tvolume = {48},\n\tissn = {02728842},\n\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0272884221030534},\n\tdoi = {10.1016/j.ceramint.2021.09.243},\n\tlanguage = {en},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Ceramics International},\n\tauthor = {Andryushin, K.P. and Shilkina, L.A. and Khasbulatov, S.V. and Nagaenko, A.V. and Dudkina, S.I. and Andryushina, I.N. and Sadykov, KhA. and Verbenko, I.A. and Rudskaya, A.G. and Reznichenko, L.A.},\n\tmonth = jan,\n\tyear = {2022},\n\tpages = {1642--1658},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"lukyanchuk-razumnaya-sen-tikhonov-vinokur-theferroelectricfieldeffecttransistorwithnegativecapacitance-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.nature.com/articles/s41524-022-00738-2\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'lukyanchuk-razumnaya-sen-tikhonov-vinokur-theferroelectricfieldeffecttransistorwithnegativecapacitance-2022', 'https://www.nature.com/articles/s41524-022-00738-2', event);\">\n    The ferroelectric field-effect transistor with negative capacitance.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Luk’yanchuk, I.; Razumnaya, A.; Sené, A.; Tikhonov, Y.;  and Vinokur, V. M.\n</span>\n\n  \n\n</span>\n\n  <i>npj Computational Materials</i>, 8(1): 52. March 2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.nature.com/articles/s41524-022-00738-2\"\n     onclick=\"log_download('lukyanchuk-razumnaya-sen-tikhonov-vinokur-theferroelectricfieldeffecttransistorwithnegativecapacitance-2022', 'https://www.nature.com/articles/s41524-022-00738-2', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"The ferroelectric field-effect transistor with negative capacitance [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1038/s41524-022-00738-2\"\n     onclick=\"log_download('lukyanchuk-razumnaya-sen-tikhonov-vinokur-theferroelectricfieldeffecttransistorwithnegativecapacitance-2022', 'http://doi.org/10.1038/s41524-022-00738-2', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/lukyanchuk-razumnaya-sen-tikhonov-vinokur-theferroelectricfieldeffecttransistorwithnegativecapacitance-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('lukyanchuk-razumnaya-sen-tikhonov-vinokur-theferroelectricfieldeffecttransistorwithnegativecapacitance-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{lukyanchuk_ferroelectric_2022,\n\ttitle = {The ferroelectric field-effect transistor with negative capacitance},\n\tvolume = {8},\n\tissn = {2057-3960},\n\turl = {https://www.nature.com/articles/s41524-022-00738-2},\n\tdoi = {10.1038/s41524-022-00738-2},\n\tabstract = {Abstract\n            Integrating ferroelectric negative capacitance (NC) into the field-effect transistor (FET) promises to break fundamental limits of power dissipation known as Boltzmann tyranny. However, realizing the stable static negative capacitance in the non-transient non-hysteretic regime remains a daunting task. The problem stems from the lack of understanding of how the fundamental origin of the NC due to the emergence of the domain state can be put in use for implementing the NC FET. Here we put forth an ingenious design for the ferroelectric domain-based field-effect transistor with the stable reversible static negative capacitance. Using dielectric coating of the ferroelectric capacitor enables the tunability of the negative capacitance improving tremendously the performance of the field-effect transistors.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {npj Computational Materials},\n\tauthor = {Luk’yanchuk, I. and Razumnaya, A. and Sené, A. and Tikhonov, Y. and Vinokur, V. M.},\n\tmonth = mar,\n\tyear = {2022},\n\tpages = {52},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\RNZJZAMQ\\\\Luk’yanchuk и др. - 2022 - The ferroelectric field-effect transistor with neg.pdf:application/pdf;Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\NWIGDCZ5\\\\Luk’yanchuk и др. - 2022 - The ferroelectric field-effect transistor with neg.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Abstract Integrating ferroelectric negative capacitance (NC) into the field-effect transistor (FET) promises to break fundamental limits of power dissipation known as Boltzmann tyranny. However, realizing the stable static negative capacitance in the non-transient non-hysteretic regime remains a daunting task. The problem stems from the lack of understanding of how the fundamental origin of the NC due to the emergence of the domain state can be put in use for implementing the NC FET. Here we put forth an ingenious design for the ferroelectric domain-based field-effect transistor with the stable reversible static negative capacitance. Using dielectric coating of the ferroelectric capacitor enables the tunability of the negative capacitance improving tremendously the performance of the field-effect transistors.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"nikolaev-kazmina-lyanguzov-abdulvakhidov-kaidashev-synthesisofznonanorodsforpiezoelectricresonatorsandsensors-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.worldscientific.com/doi/abs/10.1142/S2010135X21600201\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'nikolaev-kazmina-lyanguzov-abdulvakhidov-kaidashev-synthesisofznonanorodsforpiezoelectricresonatorsandsensors-2022', 'https://www.worldscientific.com/doi/abs/10.1142/S2010135X21600201', event);\">\n    Synthesis of ZnO nanorods for piezoelectric resonators and sensors.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Nikolaev, A. L.; Kazmina, M. A.; Lyanguzov, N. V.; Abdulvakhidov, K. G.;  and Kaidashev, E. M.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Advanced Dielectrics</i>, 12(01): 2160020. February 2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.worldscientific.com/doi/abs/10.1142/S2010135X21600201\"\n     onclick=\"log_download('nikolaev-kazmina-lyanguzov-abdulvakhidov-kaidashev-synthesisofznonanorodsforpiezoelectricresonatorsandsensors-2022', 'https://www.worldscientific.com/doi/abs/10.1142/S2010135X21600201', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Synthesis of ZnO nanorods for piezoelectric resonators and sensors [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1142/S2010135X21600201\"\n     onclick=\"log_download('nikolaev-kazmina-lyanguzov-abdulvakhidov-kaidashev-synthesisofznonanorodsforpiezoelectricresonatorsandsensors-2022', 'http://doi.org/10.1142/S2010135X21600201', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/nikolaev-kazmina-lyanguzov-abdulvakhidov-kaidashev-synthesisofznonanorodsforpiezoelectricresonatorsandsensors-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('nikolaev-kazmina-lyanguzov-abdulvakhidov-kaidashev-synthesisofznonanorodsforpiezoelectricresonatorsandsensors-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{nikolaev_synthesis_2022,\n\ttitle = {Synthesis of {ZnO} nanorods for piezoelectric resonators and sensors},\n\tvolume = {12},\n\tissn = {2010-135X, 2010-1368},\n\turl = {https://www.worldscientific.com/doi/abs/10.1142/S2010135X21600201},\n\tdoi = {10.1142/S2010135X21600201},\n\tabstract = {Efficiency of the piezoelectric chemisensors may be considerably enhanced by use of zinc oxide nanorods as sensing elements. ZnO nanorod arrays being good piezoelectric materials possess large surface area, which provides extra benefits for chemisorption and photodetection. Highly oriented nanorod arrays are typically prepared onto highly crystalline substrates, whereas the nanorods growth onto metal contacts meets significant technological difficulties. In this paper, we report on carbothermal, electrochemical, and hydrothermal techniques of ZnO nanorod arrays synthesis on metal contacts. The optical and structural properties of the obtained nanorods were studied using scanning electron microscopy, X-ray diffraction (XRD), Raman spectroscopy, and luminescence spectroscopy. A reliable technique was developed for obtaining ohmic contact with the grown nanorods. I–U curves of prepared contact were studied. Carbothermal synthesis made it possible to obtain the most crystallinely perfect, homogeneous, and dense arrays of nanorods and control the concentration of point defects by changing the synthesis parameters over a wide range. The electrochemical synthesis demonstrated excellent results for synthesis of ZnO nanorods on the surface of resonator electrodes.},\n\tlanguage = {en},\n\tnumber = {01},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Advanced Dielectrics},\n\tauthor = {Nikolaev, A. L. and Kazmina, M. A. and Lyanguzov, N. V. and Abdulvakhidov, K. G. and Kaidashev, E. M.},\n\tmonth = feb,\n\tyear = {2022},\n\tpages = {2160020},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Efficiency of the piezoelectric chemisensors may be considerably enhanced by use of zinc oxide nanorods as sensing elements. ZnO nanorod arrays being good piezoelectric materials possess large surface area, which provides extra benefits for chemisorption and photodetection. Highly oriented nanorod arrays are typically prepared onto highly crystalline substrates, whereas the nanorods growth onto metal contacts meets significant technological difficulties. In this paper, we report on carbothermal, electrochemical, and hydrothermal techniques of ZnO nanorod arrays synthesis on metal contacts. The optical and structural properties of the obtained nanorods were studied using scanning electron microscopy, X-ray diffraction (XRD), Raman spectroscopy, and luminescence spectroscopy. A reliable technique was developed for obtaining ohmic contact with the grown nanorods. I–U curves of prepared contact were studied. Carbothermal synthesis made it possible to obtain the most crystallinely perfect, homogeneous, and dense arrays of nanorods and control the concentration of point defects by changing the synthesis parameters over a wide range. The electrochemical synthesis demonstrated excellent results for synthesis of ZnO nanorods on the surface of resonator electrodes.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"merselmiz-hanani-prah-mezzane-hajji-abkhar-spreitzer-vengust-etal-designofleadfreebcztbasedceramicswithenhancedpiezoelectricenergyharvestingperformances-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://xlink.rsc.org/?DOI=D1CP04723J\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'merselmiz-hanani-prah-mezzane-hajji-abkhar-spreitzer-vengust-etal-designofleadfreebcztbasedceramicswithenhancedpiezoelectricenergyharvestingperformances-2022', 'http://xlink.rsc.org/?DOI=D1CP04723J', event);\">\n    Design of lead-free BCZT-based ceramics with enhanced piezoelectric energy harvesting performances.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Merselmiz, S.; Hanani, Z.; Prah, U.; Mezzane, D.; Hajji, L.; Abkhar, Z.; Spreitzer, M.; Vengust, D.; Uršič, H.; Fabijan, D.; Razumnaya, A. G.; Shapovalova, O.; Luk'yanchuk, I. A.;  and Kutnjak, Z.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Chemistry Chemical Physics</i>, 24(10): 6026–6036.  2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://xlink.rsc.org/?DOI=D1CP04723J\"\n     onclick=\"log_download('merselmiz-hanani-prah-mezzane-hajji-abkhar-spreitzer-vengust-etal-designofleadfreebcztbasedceramicswithenhancedpiezoelectricenergyharvestingperformances-2022', 'http://xlink.rsc.org/?DOI=D1CP04723J', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Design of lead-free BCZT-based ceramics with enhanced piezoelectric energy harvesting performances [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1039/D1CP04723J\"\n     onclick=\"log_download('merselmiz-hanani-prah-mezzane-hajji-abkhar-spreitzer-vengust-etal-designofleadfreebcztbasedceramicswithenhancedpiezoelectricenergyharvestingperformances-2022', 'http://doi.org/10.1039/D1CP04723J', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/merselmiz-hanani-prah-mezzane-hajji-abkhar-spreitzer-vengust-etal-designofleadfreebcztbasedceramicswithenhancedpiezoelectricenergyharvestingperformances-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('merselmiz-hanani-prah-mezzane-hajji-abkhar-spreitzer-vengust-etal-designofleadfreebcztbasedceramicswithenhancedpiezoelectricenergyharvestingperformances-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{merselmiz_design_2022,\n\ttitle = {Design of lead-free {BCZT}-based ceramics with enhanced piezoelectric energy harvesting performances},\n\tvolume = {24},\n\tissn = {1463-9076, 1463-9084},\n\turl = {http://xlink.rsc.org/?DOI=D1CP04723J},\n\tdoi = {10.1039/D1CP04723J},\n\tabstract = {The benefits of the multiphase convergence strategy to design ferroelectric ceramics for piezoelectric energy harvesting applications over a broad temperature range.\n          , \n            \n              The design of lead-free ceramics for piezoelectric energy harvesting applications has become a hot topic. Among these materials, Ba\n              0.85\n              Ca\n              0.15\n              Zr\n              0.10\n              Ti\n              0.90\n              O\n              3\n              (BCZT) and BaTi\n              0.89\n              Sn\n              0.11\n              O\n              3\n              (BTSn) are considered as potential candidates due to their enhanced piezoelectric properties. Here, the structural, electrical, piezoelectric and piezoelectric energy harvesting properties of the (1 −\n              x\n              )Ba\n              0.85\n              Ca\n              0.15\n              Zr\n              0.10\n              Ti\n              0.90\n              O\n              3\n              −\n              x\n              BaTi\n              0.89\n              Sn\n              0.11\n              O\n              3\n              (\n              x\n              BTSn,\n              x\n              = 0.2, 0.4 and 0.6) system are investigated. A systematic study of the structural properties of the\n              x\n              BTSn samples was carried out using X-ray diffraction, Raman spectroscopy, and dielectric measurements. The addition of BTSn allows a successive phase transition, which broadens the application temperature range. The enhanced piezoelectric energy harvesting properties were found in the 0.2BTSn ceramic, where the large-signal and small-signal piezoelectric coefficients, piezoelectric voltage and the piezoelectric figure of merit reached 245 pm V\n              −1\n              , 228 pC N\n              −1\n              , 16.2 mV m N\n              −1\n              and 3.7 pm\n              2\n              N\n              −1\n              , respectively. Consequently, the combination of BCZT and BTSn could provide suitable lead-free materials with enhanced piezoelectric energy harvesting performances.},\n\tlanguage = {en},\n\tnumber = {10},\n\turldate = {2023-11-11},\n\tjournal = {Physical Chemistry Chemical Physics},\n\tauthor = {Merselmiz, Soukaina and Hanani, Zouhair and Prah, Uroš and Mezzane, Daoud and Hajji, Lahoucine and Abkhar, Zahra and Spreitzer, Matjaž and Vengust, Damjan and Uršič, Hana and Fabijan, David and Razumnaya, Anna G. and Shapovalova, Olesia and Luk&#x27;yanchuk, Igor A. and Kutnjak, Zdravko},\n\tyear = {2022},\n\tpages = {6026--6036},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The benefits of the multiphase convergence strategy to design ferroelectric ceramics for piezoelectric energy harvesting applications over a broad temperature range. , The design of lead-free ceramics for piezoelectric energy harvesting applications has become a hot topic. Among these materials, Ba 0.85 Ca 0.15 Zr 0.10 Ti 0.90 O 3 (BCZT) and BaTi 0.89 Sn 0.11 O 3 (BTSn) are considered as potential candidates due to their enhanced piezoelectric properties. Here, the structural, electrical, piezoelectric and piezoelectric energy harvesting properties of the (1 − x )Ba 0.85 Ca 0.15 Zr 0.10 Ti 0.90 O 3 − x BaTi 0.89 Sn 0.11 O 3 ( x BTSn, x = 0.2, 0.4 and 0.6) system are investigated. A systematic study of the structural properties of the x BTSn samples was carried out using X-ray diffraction, Raman spectroscopy, and dielectric measurements. The addition of BTSn allows a successive phase transition, which broadens the application temperature range. The enhanced piezoelectric energy harvesting properties were found in the 0.2BTSn ceramic, where the large-signal and small-signal piezoelectric coefficients, piezoelectric voltage and the piezoelectric figure of merit reached 245 pm V −1 , 228 pC N −1 , 16.2 mV m N −1 and 3.7 pm 2 N −1 , respectively. Consequently, the combination of BCZT and BTSn could provide suitable lead-free materials with enhanced piezoelectric energy harvesting performances.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kuriganova-leontyev-avramenko-faddeev-smirnova-graphenestructurespreparedviapulsealternatingcurrenttechnique-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0959943622001249\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kuriganova-leontyev-avramenko-faddeev-smirnova-graphenestructurespreparedviapulsealternatingcurrenttechnique-2022', 'https://linkinghub.elsevier.com/retrieve/pii/S0959943622001249', event);\">\n    Graphene structures prepared via pulse alternating current technique.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kuriganova, A. B.; Leontyev, I. N.; Avramenko, M. V.; Faddeev, N. A.;  and Smirnova, N. V.\n</span>\n\n  \n\n</span>\n\n  <i>Mendeleev Communications</i>, 32(3): 308–310. May 2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0959943622001249\"\n     onclick=\"log_download('kuriganova-leontyev-avramenko-faddeev-smirnova-graphenestructurespreparedviapulsealternatingcurrenttechnique-2022', 'https://linkinghub.elsevier.com/retrieve/pii/S0959943622001249', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Graphene structures prepared via pulse alternating current technique [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.mencom.2022.05.005\"\n     onclick=\"log_download('kuriganova-leontyev-avramenko-faddeev-smirnova-graphenestructurespreparedviapulsealternatingcurrenttechnique-2022', 'http://doi.org/10.1016/j.mencom.2022.05.005', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kuriganova-leontyev-avramenko-faddeev-smirnova-graphenestructurespreparedviapulsealternatingcurrenttechnique-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kuriganova-leontyev-avramenko-faddeev-smirnova-graphenestructurespreparedviapulsealternatingcurrenttechnique-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kuriganova_graphene_2022,\n\ttitle = {Graphene structures prepared via pulse alternating current technique},\n\tvolume = {32},\n\tissn = {09599436},\n\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0959943622001249},\n\tdoi = {10.1016/j.mencom.2022.05.005},\n\tlanguage = {en},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Mendeleev Communications},\n\tauthor = {Kuriganova, Alexandra B. and Leontyev, Igor N. and Avramenko, Marina V. and Faddeev, Nikita A. and Smirnova, Nina V.},\n\tmonth = may,\n\tyear = {2022},\n\tpages = {308--310},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"timoshenko-lerer-rochal-terahertzfrequencyselectivesurfacesusingheterostructuresbasedontwodimensionaldiffractiongratingofsinglewalledcarbonnanotubes-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.tandfonline.com/doi/full/10.1080/19475411.2022.2148307\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'timoshenko-lerer-rochal-terahertzfrequencyselectivesurfacesusingheterostructuresbasedontwodimensionaldiffractiongratingofsinglewalledcarbonnanotubes-2022', 'https://www.tandfonline.com/doi/full/10.1080/19475411.2022.2148307', event);\">\n    Terahertz frequency selective surfaces using heterostructures based on two-dimensional diffraction grating of single-walled carbon nanotubes.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Timoshenko, P. E.; Lerer, A.;  and Rochal, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>International Journal of Smart and Nano Materials</i>, 14(1): 21–35. December 2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.tandfonline.com/doi/full/10.1080/19475411.2022.2148307\"\n     onclick=\"log_download('timoshenko-lerer-rochal-terahertzfrequencyselectivesurfacesusingheterostructuresbasedontwodimensionaldiffractiongratingofsinglewalledcarbonnanotubes-2022', 'https://www.tandfonline.com/doi/full/10.1080/19475411.2022.2148307', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Terahertz frequency selective surfaces using heterostructures based on two-dimensional diffraction grating of single-walled carbon nanotubes [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/19475411.2022.2148307\"\n     onclick=\"log_download('timoshenko-lerer-rochal-terahertzfrequencyselectivesurfacesusingheterostructuresbasedontwodimensionaldiffractiongratingofsinglewalledcarbonnanotubes-2022', 'http://doi.org/10.1080/19475411.2022.2148307', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/timoshenko-lerer-rochal-terahertzfrequencyselectivesurfacesusingheterostructuresbasedontwodimensionaldiffractiongratingofsinglewalledcarbonnanotubes-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('timoshenko-lerer-rochal-terahertzfrequencyselectivesurfacesusingheterostructuresbasedontwodimensionaldiffractiongratingofsinglewalledcarbonnanotubes-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{timoshenko_terahertz_2022,\n\ttitle = {Terahertz frequency selective surfaces using heterostructures based on two-dimensional diffraction grating of single-walled carbon nanotubes},\n\tvolume = {14},\n\tissn = {1947-5411, 1947-542X},\n\turl = {https://www.tandfonline.com/doi/full/10.1080/19475411.2022.2148307},\n\tdoi = {10.1080/19475411.2022.2148307},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {International Journal of Smart and Nano Materials},\n\tauthor = {Timoshenko, Pavel Evgenjevich and Lerer, Alexander and Rochal, Sergei Bernardovich},\n\tmonth = dec,\n\tyear = {2022},\n\tkeywords = {Q1},\n\tpages = {21--35},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\4F954CZU\\\\Timoshenko и др. - 2023 - Terahertz frequency selective surfaces using heter.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"tikhonov-maguire-mccluskey-mcconville-kumar-lu-meier-razumnaya-etal-polarizationtopologyatthenominallychargeddomainwallsinuniaxialferroelectrics-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/10.1002/adma.202203028\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'tikhonov-maguire-mccluskey-mcconville-kumar-lu-meier-razumnaya-etal-polarizationtopologyatthenominallychargeddomainwallsinuniaxialferroelectrics-2022', 'https://onlinelibrary.wiley.com/doi/10.1002/adma.202203028', event);\">\n    Polarization Topology at the Nominally Charged Domain Walls in Uniaxial Ferroelectrics.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Tikhonov, Y.; Maguire, J. R.; McCluskey, C. J.; McConville, J. P. V.; Kumar, A.; Lu, H.; Meier, D.; Razumnaya, A.; Gregg, J. M.; Gruverman, A.; Vinokur, V. M.;  and Luk'yanchuk, I.\n</span>\n\n  \n\n</span>\n\n  <i>Advanced Materials</i>, 34(45): 2203028. November 2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/10.1002/adma.202203028\"\n     onclick=\"log_download('tikhonov-maguire-mccluskey-mcconville-kumar-lu-meier-razumnaya-etal-polarizationtopologyatthenominallychargeddomainwallsinuniaxialferroelectrics-2022', 'https://onlinelibrary.wiley.com/doi/10.1002/adma.202203028', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Polarization Topology at the Nominally Charged Domain Walls in Uniaxial Ferroelectrics [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1002/adma.202203028\"\n     onclick=\"log_download('tikhonov-maguire-mccluskey-mcconville-kumar-lu-meier-razumnaya-etal-polarizationtopologyatthenominallychargeddomainwallsinuniaxialferroelectrics-2022', 'http://doi.org/10.1002/adma.202203028', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/tikhonov-maguire-mccluskey-mcconville-kumar-lu-meier-razumnaya-etal-polarizationtopologyatthenominallychargeddomainwallsinuniaxialferroelectrics-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('tikhonov-maguire-mccluskey-mcconville-kumar-lu-meier-razumnaya-etal-polarizationtopologyatthenominallychargeddomainwallsinuniaxialferroelectrics-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{tikhonov_polarization_2022,\n\ttitle = {Polarization {Topology} at the {Nominally} {Charged} {Domain} {Walls} in {Uniaxial} {Ferroelectrics}},\n\tvolume = {34},\n\tissn = {0935-9648, 1521-4095},\n\turl = {https://onlinelibrary.wiley.com/doi/10.1002/adma.202203028},\n\tdoi = {10.1002/adma.202203028},\n\tabstract = {Abstract\n            \n              Ferroelectric domain walls provide a fertile environment for novel materials physics. If a polarization discontinuity arises, it can drive a redistribution of electronic carriers and changes in band structure, which often result in emergent 2D conductivity. If such a discontinuity is not tolerated, then its amelioration usually involves the formation of complex topological patterns, such as flux‐closure domains, dipolar vortices, skyrmions, merons, or Hopfions. The degrees of freedom required for the development of such patterns, in which dipolar rotation is a hallmark, are readily found in multiaxial ferroelectrics. In uniaxial ferroelectrics, where only two opposite polar orientations are possible, it has been assumed that discontinuities are unavoidable when antiparallel components of polarization meet. This perception has been borne out by the appearance of charged conducting domain walls in systems such as hexagonal manganites and lithium niobate. Here, experimental and theoretical investigations on lead germanate (Pb\n              5\n              Ge\n              3\n              O\n              11\n              ) reveal that polar discontinuities can be obviated at head‐to‐head and tail‐to‐tail domain walls by mutual domain bifurcation along two different axes, creating a characteristic saddle‐point domain wall morphology and associated novel dipolar topology, removing the need for screening charge accumulation and associated conductivity enhancement.},\n\tlanguage = {en},\n\tnumber = {45},\n\turldate = {2023-11-11},\n\tjournal = {Advanced Materials},\n\tauthor = {Tikhonov, Yurii and Maguire, Jesi R. and McCluskey, Conor J. and McConville, James P. V. and Kumar, Amit and Lu, Haidong and Meier, Dennis and Razumnaya, Anna and Gregg, John Martin and Gruverman, Alexei and Vinokur, Valerii M. and Luk&#x27;yanchuk, Igor},\n\tmonth = nov,\n\tyear = {2022},\n\tpages = {2203028},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\2JEF82TV\\\\Tikhonov и др. - 2022 - Polarization Topology at the Nominally Charged Dom.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Abstract Ferroelectric domain walls provide a fertile environment for novel materials physics. If a polarization discontinuity arises, it can drive a redistribution of electronic carriers and changes in band structure, which often result in emergent 2D conductivity. If such a discontinuity is not tolerated, then its amelioration usually involves the formation of complex topological patterns, such as flux‐closure domains, dipolar vortices, skyrmions, merons, or Hopfions. The degrees of freedom required for the development of such patterns, in which dipolar rotation is a hallmark, are readily found in multiaxial ferroelectrics. In uniaxial ferroelectrics, where only two opposite polar orientations are possible, it has been assumed that discontinuities are unavoidable when antiparallel components of polarization meet. This perception has been borne out by the appearance of charged conducting domain walls in systems such as hexagonal manganites and lithium niobate. Here, experimental and theoretical investigations on lead germanate (Pb 5 Ge 3 O 11 ) reveal that polar discontinuities can be obviated at head‐to‐head and tail‐to‐tail domain walls by mutual domain bifurcation along two different axes, creating a characteristic saddle‐point domain wall morphology and associated novel dipolar topology, removing the need for screening charge accumulation and associated conductivity enhancement.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"pavlenko-dirino-boron-kondovych-sen-tikhonov-razumnaya-vinokur-etal-phasediagramofastrainedferroelectricnanowire-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.mdpi.com/2073-4352/12/4/453\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'pavlenko-dirino-boron-kondovych-sen-tikhonov-razumnaya-vinokur-etal-phasediagramofastrainedferroelectricnanowire-2022', 'https://www.mdpi.com/2073-4352/12/4/453', event);\">\n    Phase Diagram of a Strained Ferroelectric Nanowire.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Pavlenko, M. A.; Di Rino, F.; Boron, L.; Kondovych, S.; Sené, A.; Tikhonov, Y. A.; Razumnaya, A. G.; Vinokur, V. M.; Sepliarsky, M.;  and Lukyanchuk, I. A.\n</span>\n\n  \n\n</span>\n\n  <i>Crystals</i>, 12(4): 453. March 2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.mdpi.com/2073-4352/12/4/453\"\n     onclick=\"log_download('pavlenko-dirino-boron-kondovych-sen-tikhonov-razumnaya-vinokur-etal-phasediagramofastrainedferroelectricnanowire-2022', 'https://www.mdpi.com/2073-4352/12/4/453', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Phase Diagram of a Strained Ferroelectric Nanowire [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3390/cryst12040453\"\n     onclick=\"log_download('pavlenko-dirino-boron-kondovych-sen-tikhonov-razumnaya-vinokur-etal-phasediagramofastrainedferroelectricnanowire-2022', 'http://doi.org/10.3390/cryst12040453', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/pavlenko-dirino-boron-kondovych-sen-tikhonov-razumnaya-vinokur-etal-phasediagramofastrainedferroelectricnanowire-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('pavlenko-dirino-boron-kondovych-sen-tikhonov-razumnaya-vinokur-etal-phasediagramofastrainedferroelectricnanowire-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{pavlenko_phase_2022,\n\ttitle = {Phase {Diagram} of a {Strained} {Ferroelectric} {Nanowire}},\n\tvolume = {12},\n\tissn = {2073-4352},\n\turl = {https://www.mdpi.com/2073-4352/12/4/453},\n\tdoi = {10.3390/cryst12040453},\n\tabstract = {Ferroelectric materials manifest unique dielectric, ferroelastic, and piezoelectric properties. A targeted design of ferroelectrics at the nanoscale is not only of fundamental appeal but holds the highest potential for applications. Compared to two-dimensional nanostructures such as thin films and superlattices, one-dimensional ferroelectric nanowires are investigated to a much lesser extent. Here, we reveal a variety of the topological polarization states, particularly the vortex and helical chiral phases, in loaded ferroelectric nanowires, which enable us to complete the strain–temperature phase diagram of the one-dimensional ferroelectrics. These phases are of prime importance for optoelectronics and quantum communication technologies.},\n\tlanguage = {en},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Crystals},\n\tauthor = {Pavlenko, Maksim A. and Di Rino, Franco and Boron, Leo and Kondovych, Svitlana and Sené, Anaïs and Tikhonov, Yuri A. and Razumnaya, Anna G. and Vinokur, Valerii M. and Sepliarsky, Marcelo and Lukyanchuk, Igor A.},\n\tmonth = mar,\n\tyear = {2022},\n\tpages = {453},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\9V22JHFK\\\\Pavlenko и др. - 2022 - Phase Diagram of a Strained Ferroelectric Nanowire.pdf:application/pdf;Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\NDRVUCFW\\\\Pavlenko и др. - 2022 - Phase Diagram of a Strained Ferroelectric Nanowire.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Ferroelectric materials manifest unique dielectric, ferroelastic, and piezoelectric properties. A targeted design of ferroelectrics at the nanoscale is not only of fundamental appeal but holds the highest potential for applications. Compared to two-dimensional nanostructures such as thin films and superlattices, one-dimensional ferroelectric nanowires are investigated to a much lesser extent. Here, we reveal a variety of the topological polarization states, particularly the vortex and helical chiral phases, in loaded ferroelectric nanowires, which enable us to complete the strain–temperature phase diagram of the one-dimensional ferroelectrics. These phases are of prime importance for optoelectronics and quantum communication technologies.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"rochal-konevtsova-roshal-boi-golushko-podgornik-packingandtrimertodimerproteinreconstructioninicosahedralviralshellswithasingletypeofsymmetricalstructuralunit-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://xlink.rsc.org/?DOI=D2NA00461E\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'rochal-konevtsova-roshal-boi-golushko-podgornik-packingandtrimertodimerproteinreconstructioninicosahedralviralshellswithasingletypeofsymmetricalstructuralunit-2022', 'http://xlink.rsc.org/?DOI=D2NA00461E', event);\">\n    Packing and trimer-to-dimer protein reconstruction in icosahedral viral shells with a single type of symmetrical structural unit.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Rochal, S. B.; Konevtsova, O. V.; Roshal, D. S.; Božič, A.; Golushko, I. Y.;  and Podgornik, R.\n</span>\n\n  \n\n</span>\n\n  <i>Nanoscale Advances</i>, 4(21): 4677–4688.  2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://xlink.rsc.org/?DOI=D2NA00461E\"\n     onclick=\"log_download('rochal-konevtsova-roshal-boi-golushko-podgornik-packingandtrimertodimerproteinreconstructioninicosahedralviralshellswithasingletypeofsymmetricalstructuralunit-2022', 'http://xlink.rsc.org/?DOI=D2NA00461E', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Packing and trimer-to-dimer protein reconstruction in icosahedral viral shells with a single type of symmetrical structural unit [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1039/D2NA00461E\"\n     onclick=\"log_download('rochal-konevtsova-roshal-boi-golushko-podgornik-packingandtrimertodimerproteinreconstructioninicosahedralviralshellswithasingletypeofsymmetricalstructuralunit-2022', 'http://doi.org/10.1039/D2NA00461E', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/rochal-konevtsova-roshal-boi-golushko-podgornik-packingandtrimertodimerproteinreconstructioninicosahedralviralshellswithasingletypeofsymmetricalstructuralunit-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('rochal-konevtsova-roshal-boi-golushko-podgornik-packingandtrimertodimerproteinreconstructioninicosahedralviralshellswithasingletypeofsymmetricalstructuralunit-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{rochal_packing_2022,\n\ttitle = {Packing and trimer-to-dimer protein reconstruction in icosahedral viral shells with a single type of symmetrical structural unit},\n\tvolume = {4},\n\tissn = {2516-0230},\n\turl = {http://xlink.rsc.org/?DOI=D2NA00461E},\n\tdoi = {10.1039/D2NA00461E},\n\tabstract = {Modelling morphological transformation in\n              Flavivirus\n              proteinaceous shells at maturation. Locally periodic arrangement of pr peptides makes the dimeric state energetically more favorable at a low pH level.\n            \n          , \n            \n              Understanding the principles of protein packing and the mechanisms driving morphological transformations in virus shells (capsids) during their maturation can be pivotal for the development of new antiviral strategies. Here, we study how these principles and mechanisms manifest themselves in icosahedral viral capsids assembled from identical symmetric structural units (capsomeres). To rationalize such shells, we model capsomers as symmetrical groups of identical particles interacting with a short-range potential typical of the classic Tammes problem. The capsomere particles are assumed to retain their relative positions on the vertices of planar polygons placed on the spherical shell and to interact only with the particles from other capsomeres. Minimization of the interaction energy enforces equal distances between the nearest particles belonging to neighboring capsomeres and minimizes the number of different local environments. Thus, our model implements the Caspar and Klug quasi-equivalence principle and leads to packings strikingly similar to real capsids. We then study a reconstruction of protein trimers into dimers in a\n              Flavivirus\n              shell during its maturation, connecting the relevant structural changes with the modifications of the electrostatic charges of proteins, wrought by the oxidative switch in the bathing solution that is essential for the process. We highlight the key role of pr peptides in the shell reconstruction and show that the highly ordered arrangement of these subunits in the dimeric state is energetically favored at a low pH level. We also discuss the electrostatic mechanisms controlling the release of pr peptides in the last irreversible step of the maturation process.},\n\tlanguage = {en},\n\tnumber = {21},\n\turldate = {2023-11-11},\n\tjournal = {Nanoscale Advances},\n\tauthor = {Rochal, Sergei B. and Konevtsova, Olga V. and Roshal, Daria S. and Božič, Anže and Golushko, Ivan Yu. and Podgornik, Rudolf},\n\tyear = {2022},\n\tpages = {4677--4688},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\DB8I4DZC\\\\Rochal и др. - 2022 - Packing and trimer-to-dimer protein reconstruction.pdf:application/pdf;Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\7PKD38HX\\\\Rochal и др. - 2022 - Packing and trimer-to-dimer protein reconstruction.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Modelling morphological transformation in Flavivirus proteinaceous shells at maturation. Locally periodic arrangement of pr peptides makes the dimeric state energetically more favorable at a low pH level. , Understanding the principles of protein packing and the mechanisms driving morphological transformations in virus shells (capsids) during their maturation can be pivotal for the development of new antiviral strategies. Here, we study how these principles and mechanisms manifest themselves in icosahedral viral capsids assembled from identical symmetric structural units (capsomeres). To rationalize such shells, we model capsomers as symmetrical groups of identical particles interacting with a short-range potential typical of the classic Tammes problem. The capsomere particles are assumed to retain their relative positions on the vertices of planar polygons placed on the spherical shell and to interact only with the particles from other capsomeres. Minimization of the interaction energy enforces equal distances between the nearest particles belonging to neighboring capsomeres and minimizes the number of different local environments. Thus, our model implements the Caspar and Klug quasi-equivalence principle and leads to packings strikingly similar to real capsids. We then study a reconstruction of protein trimers into dimers in a Flavivirus shell during its maturation, connecting the relevant structural changes with the modifications of the electrostatic charges of proteins, wrought by the oxidative switch in the bathing solution that is essential for the process. We highlight the key role of pr peptides in the shell reconstruction and show that the highly ordered arrangement of these subunits in the dimeric state is energetically favored at a low pH level. We also discuss the electrostatic mechanisms controlling the release of pr peptides in the last irreversible step of the maturation process.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-razumnaya-mikheykin-thermodynamictheoryofpbtextrmxsrtextrm1xtiotextrm3solidsolutions-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0022369721004613\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-razumnaya-mikheykin-thermodynamictheoryofpbtextrmxsrtextrm1xtiotextrm3solidsolutions-2022', 'https://linkinghub.elsevier.com/retrieve/pii/S0022369721004613', event);\">\n    Thermodynamic theory of Pb$_{\\textrm{x}}$Sr$_{\\textrm{1-x}}$TiO$_{\\textrm{3}}$ solid solutions.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V.; Razumnaya, A.;  and Mikheykin, A.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics and Chemistry of Solids</i>, 161: 110395. February 2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0022369721004613\"\n     onclick=\"log_download('shirokov-razumnaya-mikheykin-thermodynamictheoryofpbtextrmxsrtextrm1xtiotextrm3solidsolutions-2022', 'https://linkinghub.elsevier.com/retrieve/pii/S0022369721004613', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Thermodynamic theory of Pb$_{\\textrm{x}}$Sr$_{\\textrm{1-x}}$TiO$_{\\textrm{3}}$ solid solutions [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.jpcs.2021.110395\"\n     onclick=\"log_download('shirokov-razumnaya-mikheykin-thermodynamictheoryofpbtextrmxsrtextrm1xtiotextrm3solidsolutions-2022', 'http://doi.org/10.1016/j.jpcs.2021.110395', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-razumnaya-mikheykin-thermodynamictheoryofpbtextrmxsrtextrm1xtiotextrm3solidsolutions-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-razumnaya-mikheykin-thermodynamictheoryofpbtextrmxsrtextrm1xtiotextrm3solidsolutions-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_thermodynamic_2022,\n\ttitle = {Thermodynamic theory of {Pb}$_{\\textrm{x}}${Sr}$_{\\textrm{1-x}}${TiO}$_{\\textrm{3}}$ solid solutions},\n\tvolume = {161},\n\tissn = {00223697},\n\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0022369721004613},\n\tdoi = {10.1016/j.jpcs.2021.110395},\n\tlanguage = {en},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics and Chemistry of Solids},\n\tauthor = {Shirokov, V.B. and Razumnaya, A.G. and Mikheykin, A.S.},\n\tmonth = feb,\n\tyear = {2022},\n\tpages = {110395},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"abdulvakhidov-li-abdulvakhidov-soldatov-nazarenko-kulbuzhev-mardasova-lyanguzov-etal-studyofthestructuralphasestateandphysicalpropertiesof1xcofetextrm2otextrm4xpbtiotextrm3compositions-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.springer.com/10.1007/s00339-022-05442-y\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'abdulvakhidov-li-abdulvakhidov-soldatov-nazarenko-kulbuzhev-mardasova-lyanguzov-etal-studyofthestructuralphasestateandphysicalpropertiesof1xcofetextrm2otextrm4xpbtiotextrm3compositions-2022', 'https://link.springer.com/10.1007/s00339-022-05442-y', event);\">\n    Study of the structural-phase state and physical properties of (1 − x)(CoFe$_{\\textrm{2}}$O$_{\\textrm{4}}$) − x(PbTiO$_{\\textrm{3}}$) compositions.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Abdulvakhidov, B.; Li, Z.; Abdulvakhidov, K.; Soldatov, A.; Nazarenko, A.; Kulbuzhev, B.; Mardasova, I.; Lyanguzov, N.; Sitalo, E.; Sadykov, S.; Sirota, M.; Dmitrenko, I.;  and Manukyan, A.\n</span>\n\n  \n\n</span>\n\n  <i>Applied Physics A</i>, 128(4): 293. April 2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.springer.com/10.1007/s00339-022-05442-y\"\n     onclick=\"log_download('abdulvakhidov-li-abdulvakhidov-soldatov-nazarenko-kulbuzhev-mardasova-lyanguzov-etal-studyofthestructuralphasestateandphysicalpropertiesof1xcofetextrm2otextrm4xpbtiotextrm3compositions-2022', 'https://link.springer.com/10.1007/s00339-022-05442-y', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Study of the structural-phase state and physical properties of (1 − x)(CoFe$_{\\textrm{2}}$O$_{\\textrm{4}}$) − x(PbTiO$_{\\textrm{3}}$) compositions [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1007/s00339-022-05442-y\"\n     onclick=\"log_download('abdulvakhidov-li-abdulvakhidov-soldatov-nazarenko-kulbuzhev-mardasova-lyanguzov-etal-studyofthestructuralphasestateandphysicalpropertiesof1xcofetextrm2otextrm4xpbtiotextrm3compositions-2022', 'http://doi.org/10.1007/s00339-022-05442-y', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/abdulvakhidov-li-abdulvakhidov-soldatov-nazarenko-kulbuzhev-mardasova-lyanguzov-etal-studyofthestructuralphasestateandphysicalpropertiesof1xcofetextrm2otextrm4xpbtiotextrm3compositions-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('abdulvakhidov-li-abdulvakhidov-soldatov-nazarenko-kulbuzhev-mardasova-lyanguzov-etal-studyofthestructuralphasestateandphysicalpropertiesof1xcofetextrm2otextrm4xpbtiotextrm3compositions-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{abdulvakhidov_study_2022,\n\ttitle = {Study of the structural-phase state and physical properties of (1 − x)({CoFe}$_{\\textrm{2}}${O}$_{\\textrm{4}}$) − x({PbTiO}$_{\\textrm{3}}$) compositions},\n\tvolume = {128},\n\tissn = {0947-8396, 1432-0630},\n\turl = {https://link.springer.com/10.1007/s00339-022-05442-y},\n\tdoi = {10.1007/s00339-022-05442-y},\n\tlanguage = {en},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Applied Physics A},\n\tauthor = {Abdulvakhidov, Bashir and Li, Zhengyou and Abdulvakhidov, Kamaludin and Soldatov, Alexander and Nazarenko, Alexander and Kulbuzhev, Bashir and Mardasova, Irina and Lyanguzov, Nikolay and Sitalo, Evgeniy and Sadykov, Sadyk and Sirota, Marina and Dmitrenko, Ivan and Manukyan, Aram},\n\tmonth = apr,\n\tyear = {2022},\n\tpages = {293},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"zahid-hadouch-amjoud-mezzane-goun-hoummada-alimoussa-razumnaya-etal-enhancednearambienttemperatureenergystorageandelectrocaloriceffectintheleadfreebatitextrm089sntextrm011otextrm3ceramicsynthesizedbysolgelmethod-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.springer.com/10.1007/s10854-022-08233-6\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'zahid-hadouch-amjoud-mezzane-goun-hoummada-alimoussa-razumnaya-etal-enhancednearambienttemperatureenergystorageandelectrocaloriceffectintheleadfreebatitextrm089sntextrm011otextrm3ceramicsynthesizedbysolgelmethod-2022', 'https://link.springer.com/10.1007/s10854-022-08233-6', event);\">\n    Enhanced near-ambient temperature energy storage and electrocaloric effect in the lead-free BaTi$_{\\textrm{0.89}}$Sn$_{\\textrm{0.11}}$O$_{\\textrm{3}}$ ceramic synthesized by sol–gel method.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Zahid, M.; Hadouch, Y.; Amjoud, M.; Mezzane, D.; Gouné, M.; Hoummada, K.; Alimoussa, A.; Razumnaya, A. G.; Rožič, B.;  and Kutnjak, Z.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Materials Science: Materials in Electronics</i>, 33(16): 12900–12911. June 2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.springer.com/10.1007/s10854-022-08233-6\"\n     onclick=\"log_download('zahid-hadouch-amjoud-mezzane-goun-hoummada-alimoussa-razumnaya-etal-enhancednearambienttemperatureenergystorageandelectrocaloriceffectintheleadfreebatitextrm089sntextrm011otextrm3ceramicsynthesizedbysolgelmethod-2022', 'https://link.springer.com/10.1007/s10854-022-08233-6', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Enhanced near-ambient temperature energy storage and electrocaloric effect in the lead-free BaTi$_{\\textrm{0.89}}$Sn$_{\\textrm{0.11}}$O$_{\\textrm{3}}$ ceramic synthesized by sol–gel method [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1007/s10854-022-08233-6\"\n     onclick=\"log_download('zahid-hadouch-amjoud-mezzane-goun-hoummada-alimoussa-razumnaya-etal-enhancednearambienttemperatureenergystorageandelectrocaloriceffectintheleadfreebatitextrm089sntextrm011otextrm3ceramicsynthesizedbysolgelmethod-2022', 'http://doi.org/10.1007/s10854-022-08233-6', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/zahid-hadouch-amjoud-mezzane-goun-hoummada-alimoussa-razumnaya-etal-enhancednearambienttemperatureenergystorageandelectrocaloriceffectintheleadfreebatitextrm089sntextrm011otextrm3ceramicsynthesizedbysolgelmethod-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('zahid-hadouch-amjoud-mezzane-goun-hoummada-alimoussa-razumnaya-etal-enhancednearambienttemperatureenergystorageandelectrocaloriceffectintheleadfreebatitextrm089sntextrm011otextrm3ceramicsynthesizedbysolgelmethod-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{zahid_enhanced_2022,\n\ttitle = {Enhanced near-ambient temperature energy storage and electrocaloric effect in the lead-free {BaTi}$_{\\textrm{0.89}}${Sn}$_{\\textrm{0.11}}${O}$_{\\textrm{3}}$ ceramic synthesized by sol–gel method},\n\tvolume = {33},\n\tissn = {0957-4522, 1573-482X},\n\turl = {https://link.springer.com/10.1007/s10854-022-08233-6},\n\tdoi = {10.1007/s10854-022-08233-6},\n\tlanguage = {en},\n\tnumber = {16},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Materials Science: Materials in Electronics},\n\tauthor = {Zahid, Marwa and Hadouch, Youness and Amjoud, M’barek and Mezzane, Daoud and Gouné, Mohamed and Hoummada, Khalid and Alimoussa, Abdelhadi and Razumnaya, Anna G. and Rožič, Brigita and Kutnjak, Zdravko},\n\tmonth = jun,\n\tyear = {2022},\n\tpages = {12900--12911},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\JXG9ZCDZ\\\\Zahid и др. - 2022 - Enhanced near-ambient temperature energy storage a.pdf:application/pdf;Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\GCABVF4P\\\\Zahid и др. - 2022 - Enhanced near-ambient temperature energy storage a.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"zaitouni-hajji-mezzane-choukri-razumnaya-gagou-hoummada-alimoussa-etal-enhancedelectrocaloricandenergystoragepropertiesofenvironmentfriendlyferroelectricbatextrm09srtextrm01titextrm1xsntextrmxotextrm3ceramics-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S2352492822002227\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'zaitouni-hajji-mezzane-choukri-razumnaya-gagou-hoummada-alimoussa-etal-enhancedelectrocaloricandenergystoragepropertiesofenvironmentfriendlyferroelectricbatextrm09srtextrm01titextrm1xsntextrmxotextrm3ceramics-2022', 'https://linkinghub.elsevier.com/retrieve/pii/S2352492822002227', event);\">\n    Enhanced electrocaloric and energy-storage properties of environment-friendly ferroelectric Ba$_{\\textrm{0.9}}$Sr$_{\\textrm{0.1}}$Ti$_{\\textrm{1−x}}$Sn$_{\\textrm{x}}$O$_{\\textrm{3}}$ ceramics.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Zaitouni, H.; Hajji, L.; Mezzane, D.; Choukri, E.; Razumnaya, A.; Gagou, Y.; Hoummada, K.; Alimoussa, A.; Rožič, B.; Črešnar, D.; El Marssi, M.;  and Kutnjak, Z.\n</span>\n\n  \n\n</span>\n\n  <i>Materials Today Communications</i>, 31: 103351. June 2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S2352492822002227\"\n     onclick=\"log_download('zaitouni-hajji-mezzane-choukri-razumnaya-gagou-hoummada-alimoussa-etal-enhancedelectrocaloricandenergystoragepropertiesofenvironmentfriendlyferroelectricbatextrm09srtextrm01titextrm1xsntextrmxotextrm3ceramics-2022', 'https://linkinghub.elsevier.com/retrieve/pii/S2352492822002227', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Enhanced electrocaloric and energy-storage properties of environment-friendly ferroelectric Ba$_{\\textrm{0.9}}$Sr$_{\\textrm{0.1}}$Ti$_{\\textrm{1−x}}$Sn$_{\\textrm{x}}$O$_{\\textrm{3}}$ ceramics [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.mtcomm.2022.103351\"\n     onclick=\"log_download('zaitouni-hajji-mezzane-choukri-razumnaya-gagou-hoummada-alimoussa-etal-enhancedelectrocaloricandenergystoragepropertiesofenvironmentfriendlyferroelectricbatextrm09srtextrm01titextrm1xsntextrmxotextrm3ceramics-2022', 'http://doi.org/10.1016/j.mtcomm.2022.103351', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/zaitouni-hajji-mezzane-choukri-razumnaya-gagou-hoummada-alimoussa-etal-enhancedelectrocaloricandenergystoragepropertiesofenvironmentfriendlyferroelectricbatextrm09srtextrm01titextrm1xsntextrmxotextrm3ceramics-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('zaitouni-hajji-mezzane-choukri-razumnaya-gagou-hoummada-alimoussa-etal-enhancedelectrocaloricandenergystoragepropertiesofenvironmentfriendlyferroelectricbatextrm09srtextrm01titextrm1xsntextrmxotextrm3ceramics-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{zaitouni_enhanced_2022,\n\ttitle = {Enhanced electrocaloric and energy-storage properties of environment-friendly ferroelectric {Ba}$_{\\textrm{0.9}}${Sr}$_{\\textrm{0.1}}${Ti}$_{\\textrm{1−x}}${Sn}$_{\\textrm{x}}${O}$_{\\textrm{3}}$ ceramics},\n\tvolume = {31},\n\tissn = {23524928},\n\turl = {https://linkinghub.elsevier.com/retrieve/pii/S2352492822002227},\n\tdoi = {10.1016/j.mtcomm.2022.103351},\n\tlanguage = {en},\n\turldate = {2023-11-11},\n\tjournal = {Materials Today Communications},\n\tauthor = {Zaitouni, H. and Hajji, L. and Mezzane, D. and Choukri, E. and Razumnaya, A.G. and Gagou, Y. and Hoummada, K. and Alimoussa, A. and Rožič, B. and Črešnar, D. and El Marssi, M. and Kutnjak, Z.},\n\tmonth = jun,\n\tyear = {2022},\n\tpages = {103351},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\24PCRTWA\\\\Zaitouni и др. - 2022 - Enhanced electrocaloric and energy-storage propert.pdf:application/pdf;Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\C3NG5P6W\\\\Zaitouni и др. - 2022 - Enhanced electrocaloric and energy-storage propert.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"hadouch-benmoumen-mezzourh-mezzane-amjoud-asbani-razumnaya-gagou-etal-electrocaloriceffectandhighenergystorageefficiencyinleadfreebatextrm095catextrm005titextrm089sntextrm011otextrm3ceramicelaboratedbysolgelmethod-2022\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.springer.com/10.1007/s10854-021-07411-2\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'hadouch-benmoumen-mezzourh-mezzane-amjoud-asbani-razumnaya-gagou-etal-electrocaloriceffectandhighenergystorageefficiencyinleadfreebatextrm095catextrm005titextrm089sntextrm011otextrm3ceramicelaboratedbysolgelmethod-2022', 'https://link.springer.com/10.1007/s10854-021-07411-2', event);\">\n    Electrocaloric effect and high energy storage efficiency in lead-free Ba$_{\\textrm{0.95}}$Ca$_{\\textrm{0.05}}$Ti$_{\\textrm{0.89}}$Sn$_{\\textrm{0.11}}$O$_{\\textrm{3}}$ ceramic elaborated by sol–gel method.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Hadouch, Y.; Ben Moumen, S.; Mezzourh, H.; Mezzane, D.; Amjoud, M.; Asbani, B.; Razumnaya, A. G.; Gagou, Y.; Rožič, B.; Kutnjak, Z.;  and El Marssi, M.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Materials Science: Materials in Electronics</i>, 33(4): 2067–2079. February 2022.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.springer.com/10.1007/s10854-021-07411-2\"\n     onclick=\"log_download('hadouch-benmoumen-mezzourh-mezzane-amjoud-asbani-razumnaya-gagou-etal-electrocaloriceffectandhighenergystorageefficiencyinleadfreebatextrm095catextrm005titextrm089sntextrm011otextrm3ceramicelaboratedbysolgelmethod-2022', 'https://link.springer.com/10.1007/s10854-021-07411-2', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Electrocaloric effect and high energy storage efficiency in lead-free Ba$_{\\textrm{0.95}}$Ca$_{\\textrm{0.05}}$Ti$_{\\textrm{0.89}}$Sn$_{\\textrm{0.11}}$O$_{\\textrm{3}}$ ceramic elaborated by sol–gel method [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1007/s10854-021-07411-2\"\n     onclick=\"log_download('hadouch-benmoumen-mezzourh-mezzane-amjoud-asbani-razumnaya-gagou-etal-electrocaloriceffectandhighenergystorageefficiencyinleadfreebatextrm095catextrm005titextrm089sntextrm011otextrm3ceramicelaboratedbysolgelmethod-2022', 'http://doi.org/10.1007/s10854-021-07411-2', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/hadouch-benmoumen-mezzourh-mezzane-amjoud-asbani-razumnaya-gagou-etal-electrocaloriceffectandhighenergystorageefficiencyinleadfreebatextrm095catextrm005titextrm089sntextrm011otextrm3ceramicelaboratedbysolgelmethod-2022\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('hadouch-benmoumen-mezzourh-mezzane-amjoud-asbani-razumnaya-gagou-etal-electrocaloriceffectandhighenergystorageefficiencyinleadfreebatextrm095catextrm005titextrm089sntextrm011otextrm3ceramicelaboratedbysolgelmethod-2022')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{hadouch_electrocaloric_2022,\n\ttitle = {Electrocaloric effect and high energy storage efficiency in lead-free {Ba}$_{\\textrm{0.95}}${Ca}$_{\\textrm{0.05}}${Ti}$_{\\textrm{0.89}}${Sn}$_{\\textrm{0.11}}${O}$_{\\textrm{3}}$ ceramic elaborated by sol–gel method},\n\tvolume = {33},\n\tissn = {0957-4522, 1573-482X},\n\turl = {https://link.springer.com/10.1007/s10854-021-07411-2},\n\tdoi = {10.1007/s10854-021-07411-2},\n\tlanguage = {en},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Materials Science: Materials in Electronics},\n\tauthor = {Hadouch, Youness and Ben Moumen, Said and Mezzourh, Hanane and Mezzane, Daoud and Amjoud, M’barek and Asbani, Bouchra and Razumnaya, Anna G. and Gagou, Yaovi and Rožič, Brigita and Kutnjak, Zdravko and El Marssi, Mimoun},\n\tmonth = feb,\n\tyear = {2022},\n\tpages = {2067--2079},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\3DEEINNF\\\\Hadouch и др. - 2022 - Electrocaloric effect and high energy storage effi.pdf:application/pdf;Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\ECS5QNNK\\\\Hadouch и др. - 2022 - Electrocaloric effect and high energy storage effi.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2021\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2021')\"\n      onkeypress=\"toggleGroup('group_2021')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2021</span>\n      <span class=\"bibbase_group_count\">\n        \n        (19)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"vakhrushev-leontyev-bosak-udovenko-petroukhno-temperatureevolutionofinelasticsynchrotronradiationscatteringinpbzrtextrm0985titextrm0015otextrm3inthevicinityofmpoint-2021\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://ieeexplore.ieee.org/document/9614882/\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'vakhrushev-leontyev-bosak-udovenko-petroukhno-temperatureevolutionofinelasticsynchrotronradiationscatteringinpbzrtextrm0985titextrm0015otextrm3inthevicinityofmpoint-2021', 'https://ieeexplore.ieee.org/document/9614882/', event);\">\n    Temperature Evolution of Inelastic Synchrotron Radiation Scattering in PbZr $_{\\textrm{0.985}}$Ti$_{\\textrm{0.015}}$O$_{\\textrm{3}}$ in the Vicinity of M-Point.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Vakhrushev, S. B.; Leontyev, I. N.; Bosak, A.; Udovenko, S. A.;  and Petroukhno, K. A.\n</span>\n\n  \n\n</span>\n\n  In <i>2021 International Conference on Electrical Engineering and Photonics (EExPolytech)</i>, pages 143–145, St. Petersburg, Russian Federation, October 2021. IEEE\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://ieeexplore.ieee.org/document/9614882/\"\n     onclick=\"log_download('vakhrushev-leontyev-bosak-udovenko-petroukhno-temperatureevolutionofinelasticsynchrotronradiationscatteringinpbzrtextrm0985titextrm0015otextrm3inthevicinityofmpoint-2021', 'https://ieeexplore.ieee.org/document/9614882/', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Temperature Evolution of Inelastic Synchrotron Radiation Scattering in PbZr $_{\\textrm{0.985}}$Ti$_{\\textrm{0.015}}$O$_{\\textrm{3}}$ in the Vicinity of M-Point [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1109/EExPolytech53083.2021.9614882\"\n     onclick=\"log_download('vakhrushev-leontyev-bosak-udovenko-petroukhno-temperatureevolutionofinelasticsynchrotronradiationscatteringinpbzrtextrm0985titextrm0015otextrm3inthevicinityofmpoint-2021', 'http://doi.org/10.1109/EExPolytech53083.2021.9614882', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/vakhrushev-leontyev-bosak-udovenko-petroukhno-temperatureevolutionofinelasticsynchrotronradiationscatteringinpbzrtextrm0985titextrm0015otextrm3inthevicinityofmpoint-2021\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('vakhrushev-leontyev-bosak-udovenko-petroukhno-temperatureevolutionofinelasticsynchrotronradiationscatteringinpbzrtextrm0985titextrm0015otextrm3inthevicinityofmpoint-2021')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{vakhrushev_temperature_2021,\n\taddress = {St. Petersburg, Russian Federation},\n\ttitle = {Temperature {Evolution} of {Inelastic} {Synchrotron} {Radiation} {Scattering} in {PbZr} $_{\\textrm{0.985}}${Ti}$_{\\textrm{0.015}}${O}$_{\\textrm{3}}$ in the {Vicinity} of {M}-{Point}},\n\tisbn = {978-1-66544-972-4},\n\turl = {https://ieeexplore.ieee.org/document/9614882/},\n\tdoi = {10.1109/EExPolytech53083.2021.9614882},\n\turldate = {2023-11-10},\n\tbooktitle = {2021 {International} {Conference} on {Electrical} {Engineering} and {Photonics} ({EExPolytech})},\n\tpublisher = {IEEE},\n\tauthor = {Vakhrushev, Sergey B. and Leontyev, Igor N. and Bosak, Alexey and Udovenko, Stanislav A. and Petroukhno, Konstantin A.},\n\tmonth = oct,\n\tyear = {2021},\n\tpages = {143--145},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"redina-avramenko-lyanguzov-characteristicsofcarbonnanotubessynthesizedfrommethaneandacetyleneinthepresenceofafecltextrm3catalyst-2021\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://link.springer.com/10.1134/S106378422103021X\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'redina-avramenko-lyanguzov-characteristicsofcarbonnanotubessynthesizedfrommethaneandacetyleneinthepresenceofafecltextrm3catalyst-2021', 'http://link.springer.com/10.1134/S106378422103021X', event);\">\n    Characteristics of Carbon Nanotubes Synthesized from Methane and Acetylene in the Presence of a FeCl$_{\\textrm{3}}$ Catalyst.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Redina, A. G.; Avramenko, M. V.;  and Lyanguzov, N. V.\n</span>\n\n  \n\n</span>\n\n  <i>Technical Physics</i>, 66(3): 445–452. March 2021.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://link.springer.com/10.1134/S106378422103021X\"\n     onclick=\"log_download('redina-avramenko-lyanguzov-characteristicsofcarbonnanotubessynthesizedfrommethaneandacetyleneinthepresenceofafecltextrm3catalyst-2021', 'http://link.springer.com/10.1134/S106378422103021X', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Characteristics of Carbon Nanotubes Synthesized from Methane and Acetylene in the Presence of a FeCl$_{\\textrm{3}}$ Catalyst [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S106378422103021X\"\n     onclick=\"log_download('redina-avramenko-lyanguzov-characteristicsofcarbonnanotubessynthesizedfrommethaneandacetyleneinthepresenceofafecltextrm3catalyst-2021', 'http://doi.org/10.1134/S106378422103021X', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/redina-avramenko-lyanguzov-characteristicsofcarbonnanotubessynthesizedfrommethaneandacetyleneinthepresenceofafecltextrm3catalyst-2021\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('redina-avramenko-lyanguzov-characteristicsofcarbonnanotubessynthesizedfrommethaneandacetyleneinthepresenceofafecltextrm3catalyst-2021')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{redina_characteristics_2021,\n\ttitle = {Characteristics of {Carbon} {Nanotubes} {Synthesized} from {Methane} and {Acetylene} in the {Presence} of a {FeCl}$_{\\textrm{3}}$ {Catalyst}},\n\tvolume = {66},\n\tissn = {1063-7842, 1090-6525},\n\turl = {http://link.springer.com/10.1134/S106378422103021X},\n\tdoi = {10.1134/S106378422103021X},\n\tlanguage = {en},\n\tnumber = {3},\n\turldate = {2023-11-10},\n\tjournal = {Technical Physics},\n\tauthor = {Redina, A. G. and Avramenko, M. V. and Lyanguzov, N. V.},\n\tmonth = mar,\n\tyear = {2021},\n\tpages = {445--452},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"linnik-lukyanchuk-mikheykin-ragulya-gorshunov-alyabyeva-zhukov-mezzane-etal-crystalstructureandthespectralresponseofthebadopedsrtiotextrm3incipientferroelectrics-2021\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/10.1002/pssb.202100010\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'linnik-lukyanchuk-mikheykin-ragulya-gorshunov-alyabyeva-zhukov-mezzane-etal-crystalstructureandthespectralresponseofthebadopedsrtiotextrm3incipientferroelectrics-2021', 'https://onlinelibrary.wiley.com/doi/10.1002/pssb.202100010', event);\">\n    Crystal Structure and the Spectral Response of the Ba‐Doped SrTiO$_{\\textrm{3}}$ Incipient Ferroelectrics.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Linnik, E. D.; Lukyanchuk, I. A.; Mikheykin, A. S.; Ragulya, A. V.; Gorshunov, B. P.; Alyabyeva, L. N.; Zhukov, S. S.; Mezzane, D.;  and Razumnaya, A. G.\n</span>\n\n  \n\n</span>\n\n  <i>physica status solidi (b)</i>, 258(7): 2100010. July 2021.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/10.1002/pssb.202100010\"\n     onclick=\"log_download('linnik-lukyanchuk-mikheykin-ragulya-gorshunov-alyabyeva-zhukov-mezzane-etal-crystalstructureandthespectralresponseofthebadopedsrtiotextrm3incipientferroelectrics-2021', 'https://onlinelibrary.wiley.com/doi/10.1002/pssb.202100010', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Crystal Structure and the Spectral Response of the Ba‐Doped SrTiO$_{\\textrm{3}}$ Incipient Ferroelectrics [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1002/pssb.202100010\"\n     onclick=\"log_download('linnik-lukyanchuk-mikheykin-ragulya-gorshunov-alyabyeva-zhukov-mezzane-etal-crystalstructureandthespectralresponseofthebadopedsrtiotextrm3incipientferroelectrics-2021', 'http://doi.org/10.1002/pssb.202100010', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/linnik-lukyanchuk-mikheykin-ragulya-gorshunov-alyabyeva-zhukov-mezzane-etal-crystalstructureandthespectralresponseofthebadopedsrtiotextrm3incipientferroelectrics-2021\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('linnik-lukyanchuk-mikheykin-ragulya-gorshunov-alyabyeva-zhukov-mezzane-etal-crystalstructureandthespectralresponseofthebadopedsrtiotextrm3incipientferroelectrics-2021')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{linnik_crystal_2021,\n\ttitle = {Crystal {Structure} and the {Spectral} {Response} of the {Ba}‐{Doped} {SrTiO}$_{\\textrm{3}}$ {Incipient} {Ferroelectrics}},\n\tvolume = {258},\n\tissn = {0370-1972, 1521-3951},\n\turl = {https://onlinelibrary.wiley.com/doi/10.1002/pssb.202100010},\n\tdoi = {10.1002/pssb.202100010},\n\tabstract = {The crystal structure and lattice dynamics of quantum paraelectric Ba\n                \n                  x\n                \n                Sr\n                \n                  1−\n                  x\n                \n                TiO\n                3\n                (\n                x\n                 = 0, 0.01, 0.02) solid solutions are studied using X‐ray diffraction (XRD), Raman and terahertz‐infrared (THz‐IR) spectroscopies in a temperature range of 4–300 K. XRD and Raman spectroscopy reveal the cubic‐to‐tetragonal nonpolar structural phase transition at about 100 K. At the same time, Raman spectra manifest the presence of polar modes, TO\n                2\n                and TO\n                4\n                , normally prohibited in paraelectric phase. Emergence of these modes indicates the appearance of the polar nanoregions in a broad temperature range. The modes become more intensive at low temperatures, and temperature dependence of their intensities on cooling reveals the kink‐like change of the slope from flat to steep, indicating on activation of polar nanoregions. The transmission THz‐IR spectra show that squared frequency of the polar TO\n                1\n                soft mode, responsible for ferroelectric transition, follows Cochran&#x27;s behavior at high temperatures. However, at low temperatures, it doesn&#x27;t vanish at extrapolated Curie temperature but saturates, demonstrating the plateau feature below 20 K. This behavior, coherent with known saturation of the dielectric constant, indicates that transition to ferroelectric phase in Ba\n                \n                  x\n                \n                Sr\n                \n                  1−\n                  x\n                \n                TiO\n                3\n                is suppressed by quantum fluctuations and the system stays in quantum paraelectric state at very low temperatures.},\n\tlanguage = {en},\n\tnumber = {7},\n\turldate = {2023-11-10},\n\tjournal = {physica status solidi (b)},\n\tauthor = {Linnik, Ekaterina D. and Lukyanchuk, Igor A. and Mikheykin, Alexey S. and Ragulya, Andrey V. and Gorshunov, Boris P. and Alyabyeva, Liudmila N. and Zhukov, Sergey S. and Mezzane, Daoud and Razumnaya, Anna G.},\n\tmonth = jul,\n\tyear = {2021},\n\tpages = {2100010},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The crystal structure and lattice dynamics of quantum paraelectric Ba x Sr 1− x TiO 3 ( x  = 0, 0.01, 0.02) solid solutions are studied using X‐ray diffraction (XRD), Raman and terahertz‐infrared (THz‐IR) spectroscopies in a temperature range of 4–300 K. XRD and Raman spectroscopy reveal the cubic‐to‐tetragonal nonpolar structural phase transition at about 100 K. At the same time, Raman spectra manifest the presence of polar modes, TO 2 and TO 4 , normally prohibited in paraelectric phase. Emergence of these modes indicates the appearance of the polar nanoregions in a broad temperature range. The modes become more intensive at low temperatures, and temperature dependence of their intensities on cooling reveals the kink‐like change of the slope from flat to steep, indicating on activation of polar nanoregions. The transmission THz‐IR spectra show that squared frequency of the polar TO 1 soft mode, responsible for ferroelectric transition, follows Cochran's behavior at high temperatures. However, at low temperatures, it doesn't vanish at extrapolated Curie temperature but saturates, demonstrating the plateau feature below 20 K. This behavior, coherent with known saturation of the dielectric constant, indicates that transition to ferroelectric phase in Ba x Sr 1− x TiO 3 is suppressed by quantum fluctuations and the system stays in quantum paraelectric state at very low temperatures.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-razumnaya-mikheykin-ferromagnetoelectricphasesofhexaferritesagrouptheoreticalanalysis-2021\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://scripts.iucr.org/cgi-bin/paper?S2052520621007125\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-razumnaya-mikheykin-ferromagnetoelectricphasesofhexaferritesagrouptheoreticalanalysis-2021', 'https://scripts.iucr.org/cgi-bin/paper?S2052520621007125', event);\">\n    Ferromagnetoelectric phases of hexaferrites: a group-theoretical analysis.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.; Razumnaya, A. G.;  and Mikheykin, A. S.\n</span>\n\n  \n\n</span>\n\n  <i>Acta Crystallographica Section B Structural Science, Crystal Engineering and Materials</i>, 77(5): 740–748. October 2021.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://scripts.iucr.org/cgi-bin/paper?S2052520621007125\"\n     onclick=\"log_download('shirokov-razumnaya-mikheykin-ferromagnetoelectricphasesofhexaferritesagrouptheoreticalanalysis-2021', 'https://scripts.iucr.org/cgi-bin/paper?S2052520621007125', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Ferromagnetoelectric phases of hexaferrites: a group-theoretical analysis [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1107/S2052520621007125\"\n     onclick=\"log_download('shirokov-razumnaya-mikheykin-ferromagnetoelectricphasesofhexaferritesagrouptheoreticalanalysis-2021', 'http://doi.org/10.1107/S2052520621007125', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-razumnaya-mikheykin-ferromagnetoelectricphasesofhexaferritesagrouptheoreticalanalysis-2021\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-razumnaya-mikheykin-ferromagnetoelectricphasesofhexaferritesagrouptheoreticalanalysis-2021')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_ferromagnetoelectric_2021,\n\ttitle = {Ferromagnetoelectric phases of hexaferrites: a group-theoretical analysis},\n\tvolume = {77},\n\tissn = {2052-5206},\n\tshorttitle = {Ferromagnetoelectric phases of hexaferrites},\n\turl = {https://scripts.iucr.org/cgi-bin/paper?S2052520621007125},\n\tdoi = {10.1107/S2052520621007125},\n\tabstract = {A symmetry-guided approach for designing and tailoring magnetoelectric and multiferroic hexaferrites is proposed. A group-theoretical study of the magnetoferroelectric structures of a hexagonal ferrite was carried out. The results were applied to M-, W- and Z-type hexaferrites. It is shown that the magnetic structure cannot be collinear in the main magnetic phase, with the direction of the magnetic moment along the hexagonal axis. Magnetic sublattices are shown in which cation substitution should lead to the formation of a multiferroic state. A thermodynamic model of a hexagonal ferroelectric ferrimagnet was constructed, in which isostructural phase transitions were observed.},\n\tnumber = {5},\n\turldate = {2023-11-10},\n\tjournal = {Acta Crystallographica Section B Structural Science, Crystal Engineering and Materials},\n\tauthor = {Shirokov, Vladimir Borisovich and Razumnaya, Anna Grigoryevna and Mikheykin, Alexey Sergeevich},\n\tmonth = oct,\n\tyear = {2021},\n\tpages = {740--748},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A symmetry-guided approach for designing and tailoring magnetoelectric and multiferroic hexaferrites is proposed. A group-theoretical study of the magnetoferroelectric structures of a hexagonal ferrite was carried out. The results were applied to M-, W- and Z-type hexaferrites. It is shown that the magnetic structure cannot be collinear in the main magnetic phase, with the direction of the magnetic moment along the hexagonal axis. Magnetic sublattices are shown in which cation substitution should lead to the formation of a multiferroic state. A thermodynamic model of a hexagonal ferroelectric ferrimagnet was constructed, in which isostructural phase transitions were observed.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"chalin-bureau-parmeggiani-rochal-kissa-golushko-modelingandliveimagingofmechanicalinstabilitiesinthezebrafishaortaduringhematopoiesis-2021\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.nature.com/articles/s41598-021-88667-w\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'chalin-bureau-parmeggiani-rochal-kissa-golushko-modelingandliveimagingofmechanicalinstabilitiesinthezebrafishaortaduringhematopoiesis-2021', 'https://www.nature.com/articles/s41598-021-88667-w', event);\">\n    Modeling and live imaging of mechanical instabilities in the zebrafish aorta during hematopoiesis.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Chalin, D.; Bureau, C.; Parmeggiani, A.; Rochal, S.; Kissa, K.;  and Golushko, I.\n</span>\n\n  \n\n</span>\n\n  <i>Scientific Reports</i>, 11(1): 9316. April 2021.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.nature.com/articles/s41598-021-88667-w\"\n     onclick=\"log_download('chalin-bureau-parmeggiani-rochal-kissa-golushko-modelingandliveimagingofmechanicalinstabilitiesinthezebrafishaortaduringhematopoiesis-2021', 'https://www.nature.com/articles/s41598-021-88667-w', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Modeling and live imaging of mechanical instabilities in the zebrafish aorta during hematopoiesis [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1038/s41598-021-88667-w\"\n     onclick=\"log_download('chalin-bureau-parmeggiani-rochal-kissa-golushko-modelingandliveimagingofmechanicalinstabilitiesinthezebrafishaortaduringhematopoiesis-2021', 'http://doi.org/10.1038/s41598-021-88667-w', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/chalin-bureau-parmeggiani-rochal-kissa-golushko-modelingandliveimagingofmechanicalinstabilitiesinthezebrafishaortaduringhematopoiesis-2021\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('chalin-bureau-parmeggiani-rochal-kissa-golushko-modelingandliveimagingofmechanicalinstabilitiesinthezebrafishaortaduringhematopoiesis-2021')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{chalin_modeling_2021,\n\ttitle = {Modeling and live imaging of mechanical instabilities in the zebrafish aorta during hematopoiesis},\n\tvolume = {11},\n\tissn = {2045-2322},\n\turl = {https://www.nature.com/articles/s41598-021-88667-w},\n\tdoi = {10.1038/s41598-021-88667-w},\n\tabstract = {Abstract\n            All blood cells originate from hematopoietic stem/progenitor cells (HSPCs). HSPCs are formed from endothelial cells (ECs) of the dorsal aorta (DA), via endothelial-to-hematopoietic transition (EHT). The zebrafish is a primary model organism to study the process in vivo. While the role of mechanical stress in controlling gene expression promoting cell differentiation is actively investigated, mechanisms driving shape changes of the DA and individual ECs remain poorly understood. We address this problem by developing a new DA micromechanical model and applying it to experimental data on zebrafish morphogenesis. The model considers the DA as an isotropic tubular membrane subjected to hydrostatic blood pressure and axial stress. The DA evolution is described as a movement in the dimensionless controlling parameters space: normalized hydrostatic pressure and axial stress. We argue that HSPC production is accompanied by two mechanical instabilities arising in the system due to the plane stress in the DA walls and show how a complex interplay between mechanical forces in the system drives the emerging morphological changes.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-10},\n\tjournal = {Scientific Reports},\n\tauthor = {Chalin, Dmitrii and Bureau, Charlotte and Parmeggiani, Andrea and Rochal, Sergei and Kissa, Karima and Golushko, Ivan},\n\tmonth = apr,\n\tyear = {2021},\n\tpages = {9316},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\PXM8A3B8\\\\Chalin и др. - 2021 - Modeling and live imaging of mechanical instabilit.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Abstract All blood cells originate from hematopoietic stem/progenitor cells (HSPCs). HSPCs are formed from endothelial cells (ECs) of the dorsal aorta (DA), via endothelial-to-hematopoietic transition (EHT). The zebrafish is a primary model organism to study the process in vivo. While the role of mechanical stress in controlling gene expression promoting cell differentiation is actively investigated, mechanisms driving shape changes of the DA and individual ECs remain poorly understood. We address this problem by developing a new DA micromechanical model and applying it to experimental data on zebrafish morphogenesis. The model considers the DA as an isotropic tubular membrane subjected to hydrostatic blood pressure and axial stress. The DA evolution is described as a movement in the dimensionless controlling parameters space: normalized hydrostatic pressure and axial stress. We argue that HSPC production is accompanied by two mechanical instabilities arising in the system due to the plane stress in the DA walls and show how a complex interplay between mechanical forces in the system drives the emerging morphological changes.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"moysa-nagaenko-shilkina-andryushin-andryushina-reznichenko-rudskiy-rudskaya-theinfluenceoftheinternalstructureonthepolarizationpropertiesofthesolidsolutionsofthethreecomponentsystemofthesodiumpotassiumcadmiumniobates-2021\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.tandfonline.com/doi/full/10.1080/00150193.2021.1888228\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'moysa-nagaenko-shilkina-andryushin-andryushina-reznichenko-rudskiy-rudskaya-theinfluenceoftheinternalstructureonthepolarizationpropertiesofthesolidsolutionsofthethreecomponentsystemofthesodiumpotassiumcadmiumniobates-2021', 'https://www.tandfonline.com/doi/full/10.1080/00150193.2021.1888228', event);\">\n    The influence of the internal structure on the polarization properties of the solid solutions of the three-component system of the sodium – potassium – cadmium niobates.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Moysa, M. O.; Nagaenko, A. V.; Shilkina, L. A.; Andryushin, K. P.; Andryushina, I. N.; Reznichenko, L. A.; Rudskiy, D. I.;  and Rudskaya, A. G.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 575(1): 64–74. April 2021.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.tandfonline.com/doi/full/10.1080/00150193.2021.1888228\"\n     onclick=\"log_download('moysa-nagaenko-shilkina-andryushin-andryushina-reznichenko-rudskiy-rudskaya-theinfluenceoftheinternalstructureonthepolarizationpropertiesofthesolidsolutionsofthethreecomponentsystemofthesodiumpotassiumcadmiumniobates-2021', 'https://www.tandfonline.com/doi/full/10.1080/00150193.2021.1888228', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"The influence of the internal structure on the polarization properties of the solid solutions of the three-component system of the sodium – potassium – cadmium niobates [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150193.2021.1888228\"\n     onclick=\"log_download('moysa-nagaenko-shilkina-andryushin-andryushina-reznichenko-rudskiy-rudskaya-theinfluenceoftheinternalstructureonthepolarizationpropertiesofthesolidsolutionsofthethreecomponentsystemofthesodiumpotassiumcadmiumniobates-2021', 'http://doi.org/10.1080/00150193.2021.1888228', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/moysa-nagaenko-shilkina-andryushin-andryushina-reznichenko-rudskiy-rudskaya-theinfluenceoftheinternalstructureonthepolarizationpropertiesofthesolidsolutionsofthethreecomponentsystemofthesodiumpotassiumcadmiumniobates-2021\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('moysa-nagaenko-shilkina-andryushin-andryushina-reznichenko-rudskiy-rudskaya-theinfluenceoftheinternalstructureonthepolarizationpropertiesofthesolidsolutionsofthethreecomponentsystemofthesodiumpotassiumcadmiumniobates-2021')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{moysa_influence_2021,\n\ttitle = {The influence of the internal structure on the polarization properties of the solid solutions of the three-component system of the sodium – potassium – cadmium niobates},\n\tvolume = {575},\n\tissn = {0015-0193, 1563-5112},\n\turl = {https://www.tandfonline.com/doi/full/10.1080/00150193.2021.1888228},\n\tdoi = {10.1080/00150193.2021.1888228},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-10},\n\tjournal = {Ferroelectrics},\n\tauthor = {Moysa, M. O. and Nagaenko, A. V. and Shilkina, L. A. and Andryushin, K. P. and Andryushina, I. N. and Reznichenko, L. A. and Rudskiy, D. I. and Rudskaya, A. G.},\n\tmonth = apr,\n\tyear = {2021},\n\tpages = {64--74},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"vakhrushev-andronikova-bronwald-koroleva-chernyshov-filimonov-udovenko-rudskoy-etal-electricfieldcontrolofantiferroelectricdomainpattern-2021\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.103.214108\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'vakhrushev-andronikova-bronwald-koroleva-chernyshov-filimonov-udovenko-rudskoy-etal-electricfieldcontrolofantiferroelectricdomainpattern-2021', 'https://link.aps.org/doi/10.1103/PhysRevB.103.214108', event);\">\n    Electric field control of antiferroelectric domain pattern.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Vakhrushev, S. B.; Andronikova, D.; Bronwald, I.; Koroleva, E. Y.; Chernyshov, D.; Filimonov, A. V.; Udovenko, S. A.; Rudskoy, A. I.; Ishikawa, D.; Baron, A. Q. R.; Bosak, A.; Leontiev, I. N.;  and Tagantsev, A. K.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 103(21): 214108. June 2021.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.103.214108\"\n     onclick=\"log_download('vakhrushev-andronikova-bronwald-koroleva-chernyshov-filimonov-udovenko-rudskoy-etal-electricfieldcontrolofantiferroelectricdomainpattern-2021', 'https://link.aps.org/doi/10.1103/PhysRevB.103.214108', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Electric field control of antiferroelectric domain pattern [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.103.214108\"\n     onclick=\"log_download('vakhrushev-andronikova-bronwald-koroleva-chernyshov-filimonov-udovenko-rudskoy-etal-electricfieldcontrolofantiferroelectricdomainpattern-2021', 'http://doi.org/10.1103/PhysRevB.103.214108', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/vakhrushev-andronikova-bronwald-koroleva-chernyshov-filimonov-udovenko-rudskoy-etal-electricfieldcontrolofantiferroelectricdomainpattern-2021\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('vakhrushev-andronikova-bronwald-koroleva-chernyshov-filimonov-udovenko-rudskoy-etal-electricfieldcontrolofantiferroelectricdomainpattern-2021')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{vakhrushev_electric_2021,\n\ttitle = {Electric field control of antiferroelectric domain pattern},\n\tvolume = {103},\n\tissn = {2469-9950, 2469-9969},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.103.214108},\n\tdoi = {10.1103/PhysRevB.103.214108},\n\tlanguage = {en},\n\tnumber = {21},\n\turldate = {2023-11-10},\n\tjournal = {Physical Review B},\n\tauthor = {Vakhrushev, S. B. and Andronikova, D. and Bronwald, Iu. and Koroleva, E. Yu. and Chernyshov, D. and Filimonov, A. V. and Udovenko, S. A. and Rudskoy, A. I. and Ishikawa, D. and Baron, A. Q. R. and Bosak, A. and Leontiev, I. N. and Tagantsev, Alexander K.},\n\tmonth = jun,\n\tyear = {2021},\n\tpages = {214108},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"lukyanchuk-vinokur-dynamicsofpolarizationvorticesrevealedinaferroelectricmaterial-2021\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.nature.com/articles/d41586-021-00887-2\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'lukyanchuk-vinokur-dynamicsofpolarizationvorticesrevealedinaferroelectricmaterial-2021', 'https://www.nature.com/articles/d41586-021-00887-2', event);\">\n    Dynamics of polarization vortices revealed in a ferroelectric material.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Luk’yanchuk, I.;  and Vinokur, V. M.\n</span>\n\n  \n\n</span>\n\n  <i>Nature</i>, 592(7854): 359–360. April 2021.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.nature.com/articles/d41586-021-00887-2\"\n     onclick=\"log_download('lukyanchuk-vinokur-dynamicsofpolarizationvorticesrevealedinaferroelectricmaterial-2021', 'https://www.nature.com/articles/d41586-021-00887-2', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Dynamics of polarization vortices revealed in a ferroelectric material [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1038/d41586-021-00887-2\"\n     onclick=\"log_download('lukyanchuk-vinokur-dynamicsofpolarizationvorticesrevealedinaferroelectricmaterial-2021', 'http://doi.org/10.1038/d41586-021-00887-2', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/lukyanchuk-vinokur-dynamicsofpolarizationvorticesrevealedinaferroelectricmaterial-2021\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('lukyanchuk-vinokur-dynamicsofpolarizationvorticesrevealedinaferroelectricmaterial-2021')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{lukyanchuk_dynamics_2021,\n\ttitle = {Dynamics of polarization vortices revealed in a ferroelectric material},\n\tvolume = {592},\n\tissn = {0028-0836, 1476-4687},\n\turl = {https://www.nature.com/articles/d41586-021-00887-2},\n\tdoi = {10.1038/d41586-021-00887-2},\n\tlanguage = {en},\n\tnumber = {7854},\n\turldate = {2023-11-10},\n\tjournal = {Nature},\n\tauthor = {Luk’yanchuk, Igor and Vinokur, Valerii M.},\n\tmonth = apr,\n\tyear = {2021},\n\tpages = {359--360},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kondovych-gruverman-lukyanchuk-tipinduceddomainprotrusioninferroelectricfilmswithinplanepolarization-2021\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://pubs.aip.org/jap/article/129/5/054103/1080347/Tip-induced-domain-protrusion-in-ferroelectric\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kondovych-gruverman-lukyanchuk-tipinduceddomainprotrusioninferroelectricfilmswithinplanepolarization-2021', 'https://pubs.aip.org/jap/article/129/5/054103/1080347/Tip-induced-domain-protrusion-in-ferroelectric', event);\">\n    Tip-induced domain protrusion in ferroelectric films with in-plane polarization.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kondovych, S.; Gruverman, A.;  and Luk’yanchuk, I.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Applied Physics</i>, 129(5): 054103. February 2021.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://pubs.aip.org/jap/article/129/5/054103/1080347/Tip-induced-domain-protrusion-in-ferroelectric\"\n     onclick=\"log_download('kondovych-gruverman-lukyanchuk-tipinduceddomainprotrusioninferroelectricfilmswithinplanepolarization-2021', 'https://pubs.aip.org/jap/article/129/5/054103/1080347/Tip-induced-domain-protrusion-in-ferroelectric', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Tip-induced domain protrusion in ferroelectric films with in-plane polarization [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/5.0035950\"\n     onclick=\"log_download('kondovych-gruverman-lukyanchuk-tipinduceddomainprotrusioninferroelectricfilmswithinplanepolarization-2021', 'http://doi.org/10.1063/5.0035950', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kondovych-gruverman-lukyanchuk-tipinduceddomainprotrusioninferroelectricfilmswithinplanepolarization-2021\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kondovych-gruverman-lukyanchuk-tipinduceddomainprotrusioninferroelectricfilmswithinplanepolarization-2021')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kondovych_tip-induced_2021,\n\ttitle = {Tip-induced domain protrusion in ferroelectric films with in-plane polarization},\n\tvolume = {129},\n\tissn = {0021-8979, 1089-7550},\n\turl = {https://pubs.aip.org/jap/article/129/5/054103/1080347/Tip-induced-domain-protrusion-in-ferroelectric},\n\tdoi = {10.1063/5.0035950},\n\tabstract = {Charge manipulation and fabrication of stable domain patterns in ferroelectric materials by scanning probe microscopy open up broad avenues for the development of tunable electronics. Harnessing the polarization energy and electrostatic forces with specific geometry of the system enables producing the nanoscale domains by-design. Along with that, domain engineering requires mastery of underlying physical mechanisms that govern the domain formation. Here, we present a theoretical description of the domain formation by a scanning probe microscopy tip in a ferroelectric film with strong in-plane anisotropy of polarization. We demonstrate that local charge injection produces wedge-shaped domains that propagate along the anisotropy axis, whereas the tip-written lines of charge generate a comb-like domain structure. The results of our calculations agree with earlier experimental observations and allow for the optimization of the targeted domain structures.},\n\tlanguage = {en},\n\tnumber = {5},\n\turldate = {2023-11-10},\n\tjournal = {Journal of Applied Physics},\n\tauthor = {Kondovych, S. and Gruverman, A. and Luk’yanchuk, I.},\n\tmonth = feb,\n\tyear = {2021},\n\tpages = {054103},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\2AIGWX9B\\\\Kondovych и др. - 2021 - Tip-induced domain protrusion in ferroelectric fil.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Charge manipulation and fabrication of stable domain patterns in ferroelectric materials by scanning probe microscopy open up broad avenues for the development of tunable electronics. Harnessing the polarization energy and electrostatic forces with specific geometry of the system enables producing the nanoscale domains by-design. Along with that, domain engineering requires mastery of underlying physical mechanisms that govern the domain formation. Here, we present a theoretical description of the domain formation by a scanning probe microscopy tip in a ferroelectric film with strong in-plane anisotropy of polarization. We demonstrate that local charge injection produces wedge-shaped domains that propagate along the anisotropy axis, whereas the tip-written lines of charge generate a comb-like domain structure. The results of our calculations agree with earlier experimental observations and allow for the optimization of the targeted domain structures.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"andryushin-sakhnenko-turik-shilkina-pavelko-dudkina-rudskaya-rudskiy-etal-reasonsforthehighelectricalconductivityofbismuthferriteandwaystominimizeit-2021\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.mdpi.com/2076-3417/11/3/1025\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'andryushin-sakhnenko-turik-shilkina-pavelko-dudkina-rudskaya-rudskiy-etal-reasonsforthehighelectricalconductivityofbismuthferriteandwaystominimizeit-2021', 'https://www.mdpi.com/2076-3417/11/3/1025', event);\">\n    Reasons for the High Electrical Conductivity of Bismuth Ferrite and Ways to Minimize It.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Andryushin, K.; Sakhnenko, V.; Turik, A.; Shilkina, L.; Pavelko, A.; Dudkina, S.; Rudskaya, A.; Rudskiy, D.; Verbenko, I.; Hasbulatov, S.; Reznichenko, L.; Parinov, I.; Chang, S.;  and Wang, H.\n</span>\n\n  \n\n</span>\n\n  <i>Applied Sciences</i>, 11(3): 1025. January 2021.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.mdpi.com/2076-3417/11/3/1025\"\n     onclick=\"log_download('andryushin-sakhnenko-turik-shilkina-pavelko-dudkina-rudskaya-rudskiy-etal-reasonsforthehighelectricalconductivityofbismuthferriteandwaystominimizeit-2021', 'https://www.mdpi.com/2076-3417/11/3/1025', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Reasons for the High Electrical Conductivity of Bismuth Ferrite and Ways to Minimize It [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3390/app11031025\"\n     onclick=\"log_download('andryushin-sakhnenko-turik-shilkina-pavelko-dudkina-rudskaya-rudskiy-etal-reasonsforthehighelectricalconductivityofbismuthferriteandwaystominimizeit-2021', 'http://doi.org/10.3390/app11031025', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/andryushin-sakhnenko-turik-shilkina-pavelko-dudkina-rudskaya-rudskiy-etal-reasonsforthehighelectricalconductivityofbismuthferriteandwaystominimizeit-2021\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('andryushin-sakhnenko-turik-shilkina-pavelko-dudkina-rudskaya-rudskiy-etal-reasonsforthehighelectricalconductivityofbismuthferriteandwaystominimizeit-2021')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{andryushin_reasons_2021,\n\ttitle = {Reasons for the {High} {Electrical} {Conductivity} of {Bismuth} {Ferrite} and {Ways} to {Minimize} {It}},\n\tvolume = {11},\n\tissn = {2076-3417},\n\turl = {https://www.mdpi.com/2076-3417/11/3/1025},\n\tdoi = {10.3390/app11031025},\n\tabstract = {The reasons for the high electrical conductivity of bismuth ferrite due to its natural composite structure, structural non-stoichiometry, redox processes, and the boundary position in the perovskite family have been considered. It has been shown that it is possible to significantly (2–3 orders of magnitude) reduce the conductivity of BiFeO3 by introducing large-sized ions of rare-earth elements (REE: La, Pr, Nd, Sm, Eu, Gd with 0.94 ≤ R¯ ≤ 1.04 Å) in amounts of up to 10 mol \\%. An interpretation of the observed effects has been given. A consideration about the appropriateness of taking into account the presented results when developing devices using materials of the BiFeO3/REE type has been expressed.},\n\tlanguage = {en},\n\tnumber = {3},\n\turldate = {2023-11-10},\n\tjournal = {Applied Sciences},\n\tauthor = {Andryushin, Konstantin and Sakhnenko, Vladimir and Turik, Anatoliy and Shilkina, Lidiya and Pavelko, Alexey and Dudkina, Svetlana and Rudskaya, Angela and Rudskiy, Daniil and Verbenko, Iliya and Hasbulatov, Sidek and Reznichenko, Larisa and Parinov, Ivan and Chang, Shun-Hsyung and Wang, Hung-Yu},\n\tmonth = jan,\n\tyear = {2021},\n\tpages = {1025},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\6GVK6IPC\\\\Andryushin и др. - 2021 - Reasons for the High Electrical Conductivity of Bi.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The reasons for the high electrical conductivity of bismuth ferrite due to its natural composite structure, structural non-stoichiometry, redox processes, and the boundary position in the perovskite family have been considered. It has been shown that it is possible to significantly (2–3 orders of magnitude) reduce the conductivity of BiFeO3 by introducing large-sized ions of rare-earth elements (REE: La, Pr, Nd, Sm, Eu, Gd with 0.94 ≤ R¯ ≤ 1.04 Å) in amounts of up to 10 mol %. An interpretation of the observed effects has been given. A consideration about the appropriateness of taking into account the presented results when developing devices using materials of the BiFeO3/REE type has been expressed.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"chernysheva-pudova-popov-smirnova-maslova-allix-rakhmatullin-leontyev-etal-nonisothermaldecompositionasefficientandsimplesynthesismethodofniocnanoparticlesforasymmetricsupercapacitors-2021\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.mdpi.com/2079-4991/11/1/187\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'chernysheva-pudova-popov-smirnova-maslova-allix-rakhmatullin-leontyev-etal-nonisothermaldecompositionasefficientandsimplesynthesismethodofniocnanoparticlesforasymmetricsupercapacitors-2021', 'https://www.mdpi.com/2079-4991/11/1/187', event);\">\n    Non-Isothermal Decomposition as Efficient and Simple Synthesis Method of NiO/C Nanoparticles for Asymmetric Supercapacitors.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Chernysheva, D.; Pudova, L.; Popov, Y.; Smirnova, N.; Maslova, O.; Allix, M.; Rakhmatullin, A.; Leontyev, N.; Nikolaev, A.;  and Leontyev, I.\n</span>\n\n  \n\n</span>\n\n  <i>Nanomaterials</i>, 11(1): 187. January 2021.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.mdpi.com/2079-4991/11/1/187\"\n     onclick=\"log_download('chernysheva-pudova-popov-smirnova-maslova-allix-rakhmatullin-leontyev-etal-nonisothermaldecompositionasefficientandsimplesynthesismethodofniocnanoparticlesforasymmetricsupercapacitors-2021', 'https://www.mdpi.com/2079-4991/11/1/187', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Non-Isothermal Decomposition as Efficient and Simple Synthesis Method of NiO/C Nanoparticles for Asymmetric Supercapacitors [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3390/nano11010187\"\n     onclick=\"log_download('chernysheva-pudova-popov-smirnova-maslova-allix-rakhmatullin-leontyev-etal-nonisothermaldecompositionasefficientandsimplesynthesismethodofniocnanoparticlesforasymmetricsupercapacitors-2021', 'http://doi.org/10.3390/nano11010187', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/chernysheva-pudova-popov-smirnova-maslova-allix-rakhmatullin-leontyev-etal-nonisothermaldecompositionasefficientandsimplesynthesismethodofniocnanoparticlesforasymmetricsupercapacitors-2021\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('chernysheva-pudova-popov-smirnova-maslova-allix-rakhmatullin-leontyev-etal-nonisothermaldecompositionasefficientandsimplesynthesismethodofniocnanoparticlesforasymmetricsupercapacitors-2021')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{chernysheva_non-isothermal_2021,\n\ttitle = {Non-{Isothermal} {Decomposition} as {Efficient} and {Simple} {Synthesis} {Method} of {NiO}/{C} {Nanoparticles} for {Asymmetric} {Supercapacitors}},\n\tvolume = {11},\n\tissn = {2079-4991},\n\turl = {https://www.mdpi.com/2079-4991/11/1/187},\n\tdoi = {10.3390/nano11010187},\n\tabstract = {A series of NiO/C nanocomposites with NiO concentrations ranging from 10 to 90 wt\\% was synthesized using a simple and efficient two-step method based on non-isothermal decomposition of Nickel(II) bis(acetylacetonate). X-ray diffraction (XRD) measurements of these NiO/C nanocomposites demonstrate the presence of β-NiO. NiO/C nanocomposites are composed of spherical particles distributed over the carbon support surface. The average diameter of nickel oxide spheres increases with the NiO content and are estimated as 36, 50 and 205 nm for nanocomposites with 10, 50 and 80 wt\\% NiO concentrations, respectively. In turn, each NiO sphere contains several nickel oxide nanoparticles, whose average sizes are 7–8 nm. According to the tests performed using a three-electrode cell, specific capacitance (SC) of NiO/C nanocomposites increases from 200 to 400 F/g as the NiO content achieves a maximum of 60 wt\\% concentration, after which the SC decreases. The study of the NiO/C composite showing the highest SC in three- and two-electrode cells reveals that its SC remains almost unchanged while increasing the current density, and the sample demonstrates excellent cycling stability properties. Finally, NiO/C (60\\% NiO) composites are shown to be promising materials for charging quartz clocks with a power rating of 1.5 V (30 min).},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-10},\n\tjournal = {Nanomaterials},\n\tauthor = {Chernysheva, Daria and Pudova, Ludmila and Popov, Yuri and Smirnova, Nina and Maslova, Olga and Allix, Mathieu and Rakhmatullin, Aydar and Leontyev, Nikolay and Nikolaev, Andrey and Leontyev, Igor},\n\tmonth = jan,\n\tyear = {2021},\n\tpages = {187},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\A9ZZXP6R\\\\Chernysheva и др. - 2021 - Non-Isothermal Decomposition as Efficient and Simp.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A series of NiO/C nanocomposites with NiO concentrations ranging from 10 to 90 wt% was synthesized using a simple and efficient two-step method based on non-isothermal decomposition of Nickel(II) bis(acetylacetonate). X-ray diffraction (XRD) measurements of these NiO/C nanocomposites demonstrate the presence of β-NiO. NiO/C nanocomposites are composed of spherical particles distributed over the carbon support surface. The average diameter of nickel oxide spheres increases with the NiO content and are estimated as 36, 50 and 205 nm for nanocomposites with 10, 50 and 80 wt% NiO concentrations, respectively. In turn, each NiO sphere contains several nickel oxide nanoparticles, whose average sizes are 7–8 nm. According to the tests performed using a three-electrode cell, specific capacitance (SC) of NiO/C nanocomposites increases from 200 to 400 F/g as the NiO content achieves a maximum of 60 wt% concentration, after which the SC decreases. The study of the NiO/C composite showing the highest SC in three- and two-electrode cells reveals that its SC remains almost unchanged while increasing the current density, and the sample demonstrates excellent cycling stability properties. Finally, NiO/C (60% NiO) composites are shown to be promising materials for charging quartz clocks with a power rating of 1.5 V (30 min).\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"nikolaev-kamencev-lyanguzov-aizikovich-pulsedlaserdepositionofaunanoparticlesonznonanostructures-2021\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://iopscience.iop.org/article/10.1088/1757-899X/1029/1/012064\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'nikolaev-kamencev-lyanguzov-aizikovich-pulsedlaserdepositionofaunanoparticlesonznonanostructures-2021', 'https://iopscience.iop.org/article/10.1088/1757-899X/1029/1/012064', event);\">\n    Pulsed laser deposition of Au nanoparticles on ZnO nanostructures.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Nikolaev, A L; Kamencev, A S; Lyanguzov, N V;  and Aizikovich, S M\n</span>\n\n  \n\n</span>\n\n  <i>IOP Conference Series: Materials Science and Engineering</i>, 1029(1): 012064. January 2021.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://iopscience.iop.org/article/10.1088/1757-899X/1029/1/012064\"\n     onclick=\"log_download('nikolaev-kamencev-lyanguzov-aizikovich-pulsedlaserdepositionofaunanoparticlesonznonanostructures-2021', 'https://iopscience.iop.org/article/10.1088/1757-899X/1029/1/012064', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Pulsed laser deposition of Au nanoparticles on ZnO nanostructures [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/1757-899X/1029/1/012064\"\n     onclick=\"log_download('nikolaev-kamencev-lyanguzov-aizikovich-pulsedlaserdepositionofaunanoparticlesonznonanostructures-2021', 'http://doi.org/10.1088/1757-899X/1029/1/012064', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/nikolaev-kamencev-lyanguzov-aizikovich-pulsedlaserdepositionofaunanoparticlesonznonanostructures-2021\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('nikolaev-kamencev-lyanguzov-aizikovich-pulsedlaserdepositionofaunanoparticlesonznonanostructures-2021')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{nikolaev_pulsed_2021,\n\ttitle = {Pulsed laser deposition of {Au} nanoparticles on {ZnO} nanostructures},\n\tvolume = {1029},\n\tissn = {1757-8981, 1757-899X},\n\turl = {https://iopscience.iop.org/article/10.1088/1757-899X/1029/1/012064},\n\tdoi = {10.1088/1757-899X/1029/1/012064},\n\tabstract = {Abstract\n            Au nanoparticles and ultrathin gold films were obtained on the surface of thin (100 nm) ZnO films on Si (001) by pulsed laser deposition (PLD) at high argon pressure by sputtering a pure gold target with a CL3100 pulsed excimer laser (λ = 248 nm) at room temperature. The dependence of the size and distribution of nanoparticles on the argon pressure in the vacuum chamber (PAr), the power density of laser radiation (j), and the number of laser pulses (N) was investigated. Also, to obtain nanostructures, axial and non-axial deposition was used, where the substrate was located perpendicular and parallel to the plasma torch, respectively. Stable modes of obtaining gold nanoparticles with high uniformity and average size from 4 to 10 nm were demonstrated. The modes of stable and reproducible deposition of ultrathin Au films (23-42 nm) and percolation structures (18-20 nm) were also demonstrated. Thus, PLD is a reliable and flexible tool for obtaining nanoparticles and ultrathin Au films the average size and thickness of which can be predictably controlled by varying the deposition parameters. This technique is well suited for coating with gold nanoparticles the surface of nanostructured materials based on chemically active substances that are particularly sensitive to surface cleanliness, which cannot be coated by standard methods.},\n\tnumber = {1},\n\turldate = {2023-11-10},\n\tjournal = {IOP Conference Series: Materials Science and Engineering},\n\tauthor = {Nikolaev, A L and Kamencev, A S and Lyanguzov, N V and Aizikovich, S M},\n\tmonth = jan,\n\tyear = {2021},\n\tpages = {012064},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\N97WGD4I\\\\Nikolaev и др. - 2021 - Pulsed laser deposition of Au nanoparticles on ZnO.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Abstract Au nanoparticles and ultrathin gold films were obtained on the surface of thin (100 nm) ZnO films on Si (001) by pulsed laser deposition (PLD) at high argon pressure by sputtering a pure gold target with a CL3100 pulsed excimer laser (λ = 248 nm) at room temperature. The dependence of the size and distribution of nanoparticles on the argon pressure in the vacuum chamber (PAr), the power density of laser radiation (j), and the number of laser pulses (N) was investigated. Also, to obtain nanostructures, axial and non-axial deposition was used, where the substrate was located perpendicular and parallel to the plasma torch, respectively. Stable modes of obtaining gold nanoparticles with high uniformity and average size from 4 to 10 nm were demonstrated. The modes of stable and reproducible deposition of ultrathin Au films (23-42 nm) and percolation structures (18-20 nm) were also demonstrated. Thus, PLD is a reliable and flexible tool for obtaining nanoparticles and ultrathin Au films the average size and thickness of which can be predictably controlled by varying the deposition parameters. This technique is well suited for coating with gold nanoparticles the surface of nanostructured materials based on chemically active substances that are particularly sensitive to surface cleanliness, which cannot be coated by standard methods.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"alyabyeva-prokhorov-vinnik-anzin-ahmed-mikheykin-bednyakov-kadlec-etal-leadsubstitutedbariumhexaferritefortunableterahertzoptoelectronics-2021\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.nature.com/articles/s41427-021-00331-x\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'alyabyeva-prokhorov-vinnik-anzin-ahmed-mikheykin-bednyakov-kadlec-etal-leadsubstitutedbariumhexaferritefortunableterahertzoptoelectronics-2021', 'https://www.nature.com/articles/s41427-021-00331-x', event);\">\n    Lead-substituted barium hexaferrite for tunable terahertz optoelectronics.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Alyabyeva, L. N.; Prokhorov, A. S.; Vinnik, D. A.; Anzin, V. B.; Ahmed, A. G.; Mikheykin, A.; Bednyakov, P.; Kadlec, C.; Kadlec, F.; De Prado, E.; Prokleška, J.; Proschek, P.; Kamba, S.; Pronin, A. V.; Dressel, M.; Abalmasov, V. A.; Dremov, V. V.; Schmid, S.; Savinov, M.; Lunkenheimer, P.;  and Gorshunov, B. P.\n</span>\n\n  \n\n</span>\n\n  <i>NPG Asia Materials</i>, 13(1): 63. December 2021.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.nature.com/articles/s41427-021-00331-x\"\n     onclick=\"log_download('alyabyeva-prokhorov-vinnik-anzin-ahmed-mikheykin-bednyakov-kadlec-etal-leadsubstitutedbariumhexaferritefortunableterahertzoptoelectronics-2021', 'https://www.nature.com/articles/s41427-021-00331-x', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Lead-substituted barium hexaferrite for tunable terahertz optoelectronics [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1038/s41427-021-00331-x\"\n     onclick=\"log_download('alyabyeva-prokhorov-vinnik-anzin-ahmed-mikheykin-bednyakov-kadlec-etal-leadsubstitutedbariumhexaferritefortunableterahertzoptoelectronics-2021', 'http://doi.org/10.1038/s41427-021-00331-x', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/alyabyeva-prokhorov-vinnik-anzin-ahmed-mikheykin-bednyakov-kadlec-etal-leadsubstitutedbariumhexaferritefortunableterahertzoptoelectronics-2021\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('alyabyeva-prokhorov-vinnik-anzin-ahmed-mikheykin-bednyakov-kadlec-etal-leadsubstitutedbariumhexaferritefortunableterahertzoptoelectronics-2021')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{alyabyeva_lead-substituted_2021,\n\ttitle = {Lead-substituted barium hexaferrite for tunable terahertz optoelectronics},\n\tvolume = {13},\n\tissn = {1884-4049, 1884-4057},\n\turl = {https://www.nature.com/articles/s41427-021-00331-x},\n\tdoi = {10.1038/s41427-021-00331-x},\n\tabstract = {Abstract\n            \n              Due to their outstanding dielectric and magnetic properties, hexaferrites are attracting ever-increasing attention for developing electronic components of next-generation communication systems. The complex crystal structure of hexaferrites and the critical dependences of their electric and magnetic properties on external factors, such as magnetic/electric fields, pressure, and doping, open ample opportunities for targeted tuning of these properties when designing specific devices. Here we explored the electromagnetic properties of lead-substituted barium hexaferrite, Ba\n              \n                1−\n                x\n              \n              Pb\n              \n                x\n              \n              Fe\n              12\n              O\n              19\n              , a compound featuring an extremely rich set of physical phenomena that are inherent in the dielectric and magnetic subsystems and can have a significant effect on its electromagnetic response at terahertz frequencies. We performed the first detailed measurements of the temperature-dependent (5–300 K) dielectric response of single-crystalline Ba\n              \n                1−\n                x\n              \n              Pb\n              \n                x\n              \n              Fe\n              12\n              O\n              19\n              in an extremely broad spectral range of 1 Hz–240 THz. We fully analyzed numerous phenomena with a corresponding wide distribution of specific energies that can affect the terahertz properties of the material. The most important fundamental finding is the observation of a ferroelectric-like terahertz excitation with an unusual temperature behavior of its frequency and strength. We suggest microscopic models that explain the origin of the excitation and its nonstandard temperature evolution. Several narrower terahertz excitations are associated with electronic transitions between the fine-structure components of the Fe\n              2+\n              ground state. The discovered radio-frequency relaxations are attributed to the response of magnetic domains. Gigahertz resonances are presumably of magnetoelectric origin. The obtained data on diverse electromagnetic properties of Ba\n              \n                1−\n                x\n              \n              Pb\n              \n                x\n              \n              Fe\n              12\n              O\n              19\n              compounds provide information that makes the entire class of hexaferrites attractive for manufacturing electronic devices for the terahertz range.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-10},\n\tjournal = {NPG Asia Materials},\n\tauthor = {Alyabyeva, L. N. and Prokhorov, A. S. and Vinnik, D. A. and Anzin, V. B. and Ahmed, A. G. and Mikheykin, A. and Bednyakov, P. and Kadlec, C. and Kadlec, F. and De Prado, E. and Prokleška, J. and Proschek, P. and Kamba, S. and Pronin, A. V. and Dressel, M. and Abalmasov, V. A. and Dremov, V. V. and Schmid, S. and Savinov, M. and Lunkenheimer, P. and Gorshunov, B. P.},\n\tmonth = dec,\n\tyear = {2021},\n\tpages = {63},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\3G3UAQ2R\\\\Alyabyeva и др. - 2021 - Lead-substituted barium hexaferrite for tunable te.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Abstract Due to their outstanding dielectric and magnetic properties, hexaferrites are attracting ever-increasing attention for developing electronic components of next-generation communication systems. The complex crystal structure of hexaferrites and the critical dependences of their electric and magnetic properties on external factors, such as magnetic/electric fields, pressure, and doping, open ample opportunities for targeted tuning of these properties when designing specific devices. Here we explored the electromagnetic properties of lead-substituted barium hexaferrite, Ba 1− x Pb x Fe 12 O 19 , a compound featuring an extremely rich set of physical phenomena that are inherent in the dielectric and magnetic subsystems and can have a significant effect on its electromagnetic response at terahertz frequencies. We performed the first detailed measurements of the temperature-dependent (5–300 K) dielectric response of single-crystalline Ba 1− x Pb x Fe 12 O 19 in an extremely broad spectral range of 1 Hz–240 THz. We fully analyzed numerous phenomena with a corresponding wide distribution of specific energies that can affect the terahertz properties of the material. The most important fundamental finding is the observation of a ferroelectric-like terahertz excitation with an unusual temperature behavior of its frequency and strength. We suggest microscopic models that explain the origin of the excitation and its nonstandard temperature evolution. Several narrower terahertz excitations are associated with electronic transitions between the fine-structure components of the Fe 2+ ground state. The discovered radio-frequency relaxations are attributed to the response of magnetic domains. Gigahertz resonances are presumably of magnetoelectric origin. The obtained data on diverse electromagnetic properties of Ba 1− x Pb x Fe 12 O 19 compounds provide information that makes the entire class of hexaferrites attractive for manufacturing electronic devices for the terahertz range.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"chernysheva-leontyev-avramenko-lyanguzov-grebenyuk-smirnova-onestepsimultaneouselectrochemicalsynthesisofniomultilayergraphenenanocompositeasanelectrodematerialforhighperformancesupercapacitors-2021\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0959943621000596\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'chernysheva-leontyev-avramenko-lyanguzov-grebenyuk-smirnova-onestepsimultaneouselectrochemicalsynthesisofniomultilayergraphenenanocompositeasanelectrodematerialforhighperformancesupercapacitors-2021', 'https://linkinghub.elsevier.com/retrieve/pii/S0959943621000596', event);\">\n    One step simultaneous electrochemical synthesis of NiO/multilayer graphene nanocomposite as an electrode material for high performance supercapacitors.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Chernysheva, D. V.; Leontyev, I. N.; Avramenko, M. V.; Lyanguzov, N. V.; Grebenyuk, T. I.;  and Smirnova, N. V.\n</span>\n\n  \n\n</span>\n\n  <i>Mendeleev Communications</i>, 31(2): 160–162. March 2021.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0959943621000596\"\n     onclick=\"log_download('chernysheva-leontyev-avramenko-lyanguzov-grebenyuk-smirnova-onestepsimultaneouselectrochemicalsynthesisofniomultilayergraphenenanocompositeasanelectrodematerialforhighperformancesupercapacitors-2021', 'https://linkinghub.elsevier.com/retrieve/pii/S0959943621000596', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"One step simultaneous electrochemical synthesis of NiO/multilayer graphene nanocomposite as an electrode material for high performance supercapacitors [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.mencom.2021.03.005\"\n     onclick=\"log_download('chernysheva-leontyev-avramenko-lyanguzov-grebenyuk-smirnova-onestepsimultaneouselectrochemicalsynthesisofniomultilayergraphenenanocompositeasanelectrodematerialforhighperformancesupercapacitors-2021', 'http://doi.org/10.1016/j.mencom.2021.03.005', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/chernysheva-leontyev-avramenko-lyanguzov-grebenyuk-smirnova-onestepsimultaneouselectrochemicalsynthesisofniomultilayergraphenenanocompositeasanelectrodematerialforhighperformancesupercapacitors-2021\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('chernysheva-leontyev-avramenko-lyanguzov-grebenyuk-smirnova-onestepsimultaneouselectrochemicalsynthesisofniomultilayergraphenenanocompositeasanelectrodematerialforhighperformancesupercapacitors-2021')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{chernysheva_one_2021,\n\ttitle = {One step simultaneous electrochemical synthesis of {NiO}/multilayer graphene nanocomposite as an electrode material for high performance supercapacitors},\n\tvolume = {31},\n\tissn = {09599436},\n\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0959943621000596},\n\tdoi = {10.1016/j.mencom.2021.03.005},\n\tlanguage = {en},\n\tnumber = {2},\n\turldate = {2023-11-10},\n\tjournal = {Mendeleev Communications},\n\tauthor = {Chernysheva, Daria V. and Leontyev, Igor N. and Avramenko, Marina V. and Lyanguzov, Nikolay V. and Grebenyuk, Tatyana I. and Smirnova, Nina V.},\n\tmonth = mar,\n\tyear = {2021},\n\tpages = {160--162},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"nagaenko-andryushina-andryushin-shilkina-rudskaya-reznichenko-theinfluenceofthermodynamicbackgroundonthephasepicturemacroresponsesandtheeffectsofthetemporaryagingofleadtitaniumdopedwithalkalineearthmetaloxides-2021\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0272884220331928\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'nagaenko-andryushina-andryushin-shilkina-rudskaya-reznichenko-theinfluenceofthermodynamicbackgroundonthephasepicturemacroresponsesandtheeffectsofthetemporaryagingofleadtitaniumdopedwithalkalineearthmetaloxides-2021', 'https://linkinghub.elsevier.com/retrieve/pii/S0272884220331928', event);\">\n    The influence of thermodynamic background on the phase picture, macroresponses and the effects of the temporary aging of lead titanium doped with alkaline earth metal oxides.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Nagaenko, A.; Andryushina, I.; Andryushin, K.; Shilkina, L.; Rudskaya, A.;  and Reznichenko, L.\n</span>\n\n  \n\n</span>\n\n  <i>Ceramics International</i>, 47(4): 5639–5647. February 2021.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0272884220331928\"\n     onclick=\"log_download('nagaenko-andryushina-andryushin-shilkina-rudskaya-reznichenko-theinfluenceofthermodynamicbackgroundonthephasepicturemacroresponsesandtheeffectsofthetemporaryagingofleadtitaniumdopedwithalkalineearthmetaloxides-2021', 'https://linkinghub.elsevier.com/retrieve/pii/S0272884220331928', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"The influence of thermodynamic background on the phase picture, macroresponses and the effects of the temporary aging of lead titanium doped with alkaline earth metal oxides [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.ceramint.2020.10.149\"\n     onclick=\"log_download('nagaenko-andryushina-andryushin-shilkina-rudskaya-reznichenko-theinfluenceofthermodynamicbackgroundonthephasepicturemacroresponsesandtheeffectsofthetemporaryagingofleadtitaniumdopedwithalkalineearthmetaloxides-2021', 'http://doi.org/10.1016/j.ceramint.2020.10.149', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/nagaenko-andryushina-andryushin-shilkina-rudskaya-reznichenko-theinfluenceofthermodynamicbackgroundonthephasepicturemacroresponsesandtheeffectsofthetemporaryagingofleadtitaniumdopedwithalkalineearthmetaloxides-2021\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('nagaenko-andryushina-andryushin-shilkina-rudskaya-reznichenko-theinfluenceofthermodynamicbackgroundonthephasepicturemacroresponsesandtheeffectsofthetemporaryagingofleadtitaniumdopedwithalkalineearthmetaloxides-2021')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{nagaenko_influence_2021,\n\ttitle = {The influence of thermodynamic background on the phase picture, macroresponses and the effects of the temporary aging of lead titanium doped with alkaline earth metal oxides},\n\tvolume = {47},\n\tissn = {02728842},\n\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0272884220331928},\n\tdoi = {10.1016/j.ceramint.2020.10.149},\n\tlanguage = {en},\n\tnumber = {4},\n\turldate = {2023-11-10},\n\tjournal = {Ceramics International},\n\tauthor = {Nagaenko, A.V. and Andryushina, I.N. and Andryushin, K.P. and Shilkina, L.A. and Rudskaya, A.G. and Reznichenko, L.A.},\n\tmonth = feb,\n\tyear = {2021},\n\tpages = {5639--5647},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"merselmiz-hanani-mezzane-razumnaya-amjoud-hajji-terenchuk-roi-etal-thermalstabilityoftheenhancedpiezoelectricenergystorageandelectrocaloricpropertiesofaleadfreebcztceramic-2021\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://xlink.rsc.org/?DOI=D0RA09707A\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'merselmiz-hanani-mezzane-razumnaya-amjoud-hajji-terenchuk-roi-etal-thermalstabilityoftheenhancedpiezoelectricenergystorageandelectrocaloricpropertiesofaleadfreebcztceramic-2021', 'http://xlink.rsc.org/?DOI=D0RA09707A', event);\">\n    Thermal-stability of the enhanced piezoelectric, energy storage and electrocaloric properties of a lead-free BCZT ceramic.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Merselmiz, S.; Hanani, Z.; Mezzane, D.; Razumnaya, A. G.; Amjoud, M.; Hajji, L.; Terenchuk, S.; Rožič, B.; Luk'yanchuk, I. A.;  and Kutnjak, Z.\n</span>\n\n  \n\n</span>\n\n  <i>RSC Advances</i>, 11(16): 9459–9468.  2021.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://xlink.rsc.org/?DOI=D0RA09707A\"\n     onclick=\"log_download('merselmiz-hanani-mezzane-razumnaya-amjoud-hajji-terenchuk-roi-etal-thermalstabilityoftheenhancedpiezoelectricenergystorageandelectrocaloricpropertiesofaleadfreebcztceramic-2021', 'http://xlink.rsc.org/?DOI=D0RA09707A', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Thermal-stability of the enhanced piezoelectric, energy storage and electrocaloric properties of a lead-free BCZT ceramic [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1039/D0RA09707A\"\n     onclick=\"log_download('merselmiz-hanani-mezzane-razumnaya-amjoud-hajji-terenchuk-roi-etal-thermalstabilityoftheenhancedpiezoelectricenergystorageandelectrocaloricpropertiesofaleadfreebcztceramic-2021', 'http://doi.org/10.1039/D0RA09707A', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/merselmiz-hanani-mezzane-razumnaya-amjoud-hajji-terenchuk-roi-etal-thermalstabilityoftheenhancedpiezoelectricenergystorageandelectrocaloricpropertiesofaleadfreebcztceramic-2021\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('merselmiz-hanani-mezzane-razumnaya-amjoud-hajji-terenchuk-roi-etal-thermalstabilityoftheenhancedpiezoelectricenergystorageandelectrocaloricpropertiesofaleadfreebcztceramic-2021')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{merselmiz_thermal-stability_2021,\n\ttitle = {Thermal-stability of the enhanced piezoelectric, energy storage and electrocaloric properties of a lead-free {BCZT} ceramic},\n\tvolume = {11},\n\tissn = {2046-2069},\n\turl = {http://xlink.rsc.org/?DOI=D0RA09707A},\n\tdoi = {10.1039/D0RA09707A},\n\tabstract = {High-thermal stability of the recovered energy density and significant electrocaloric temperature change over a broad temperature span in a lead-free BCZT ceramic.\n          , \n            \n              The lead-free Ba\n              0.85\n              Ca\n              0.15\n              Zr\n              0.10\n              Ti\n              0.90\n              O\n              3\n              (BCZT) relaxor ferroelectric ceramic has aroused much attention due to its enhanced piezoelectric, energy storage and electrocaloric properties. In this study, the BCZT ceramic was elaborated by the solid-state reaction route, and the temperature-dependence of the structural, electrical, piezoelectric, energy storage and electrocaloric properties was investigated. X-ray diffraction analysis revealed a pure perovskite phase, and the temperature-dependence of Raman spectroscopy, dielectric and ferroelectric measurements revealed the phase transitions in the BCZT ceramic. At room temperature, the strain and the large-signal piezoelectric coefficient\n              \n              reached a maximum of 0.062\\% and 234 pm V\n              −1\n              , respectively. Furthermore, enhanced recovered energy density (\n              W\n              rec\n              = 62 mJ cm\n              −3\n              ) and high-energy storage efficiency (\n              η\n              ) of 72.9\\% at 130 °C were found. The BCZT ceramic demonstrated excellent thermal stability of the energy storage variation (ESV), less than ±5.5\\% in the temperature range of 30–100 °C compared to other lead-free ceramics. The electrocaloric response in the BCZT ceramic was explored\n              via\n              the indirect approach by using the Maxwell relation. Significant electrocaloric temperature change (Δ\n              T\n              ) of 0.57 K over a broad temperature span (\n              T\n              span\n              = 70 °C) and enhanced coefficient of performance (COP = 11) were obtained under 25 kV cm\n              −1\n              . The obtained results make the BCZT ceramic a suitable eco-friendly material for energy storage and solid-state electrocaloric cooling devices.},\n\tlanguage = {en},\n\tnumber = {16},\n\turldate = {2023-11-10},\n\tjournal = {RSC Advances},\n\tauthor = {Merselmiz, Soukaina and Hanani, Zouhair and Mezzane, Daoud and Razumnaya, Anna G. and Amjoud, M&#x27;barek and Hajji, Lahoucine and Terenchuk, Svitlana and Rožič, Brigita and Luk&#x27;yanchuk, Igor A. and Kutnjak, Zdravko},\n\tyear = {2021},\n\tpages = {9459--9468},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\AUJR9SKH\\\\Merselmiz и др. - 2021 - Thermal-stability of the enhanced piezoelectric, e.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  High-thermal stability of the recovered energy density and significant electrocaloric temperature change over a broad temperature span in a lead-free BCZT ceramic. , The lead-free Ba 0.85 Ca 0.15 Zr 0.10 Ti 0.90 O 3 (BCZT) relaxor ferroelectric ceramic has aroused much attention due to its enhanced piezoelectric, energy storage and electrocaloric properties. In this study, the BCZT ceramic was elaborated by the solid-state reaction route, and the temperature-dependence of the structural, electrical, piezoelectric, energy storage and electrocaloric properties was investigated. X-ray diffraction analysis revealed a pure perovskite phase, and the temperature-dependence of Raman spectroscopy, dielectric and ferroelectric measurements revealed the phase transitions in the BCZT ceramic. At room temperature, the strain and the large-signal piezoelectric coefficient reached a maximum of 0.062% and 234 pm V −1 , respectively. Furthermore, enhanced recovered energy density ( W rec = 62 mJ cm −3 ) and high-energy storage efficiency ( η ) of 72.9% at 130 °C were found. The BCZT ceramic demonstrated excellent thermal stability of the energy storage variation (ESV), less than ±5.5% in the temperature range of 30–100 °C compared to other lead-free ceramics. The electrocaloric response in the BCZT ceramic was explored via the indirect approach by using the Maxwell relation. Significant electrocaloric temperature change (Δ T ) of 0.57 K over a broad temperature span ( T span = 70 °C) and enhanced coefficient of performance (COP = 11) were obtained under 25 kV cm −1 . The obtained results make the BCZT ceramic a suitable eco-friendly material for energy storage and solid-state electrocaloric cooling devices.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"mikheykin-shirokov-marssi-mezzane-lyanguzov-pavlenko-stryukov-razumnaya-twinboundaryengineeringandthicknesseffectonstrontiumbariumniobatethinfilmsonmgosubstrate-2021\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0925838821029984\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'mikheykin-shirokov-marssi-mezzane-lyanguzov-pavlenko-stryukov-razumnaya-twinboundaryengineeringandthicknesseffectonstrontiumbariumniobatethinfilmsonmgosubstrate-2021', 'https://linkinghub.elsevier.com/retrieve/pii/S0925838821029984', event);\">\n    Twin-boundary engineering and thickness effect on strontium-barium niobate thin films on MgO substrate.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Mikheykin, A.; Shirokov, V.; Marssi, M. E.; Mezzane, D.; Lyanguzov, N.; Pavlenko, A.; Stryukov, D.;  and Razumnaya, A.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Alloys and Compounds</i>, 888: 161589. December 2021.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0925838821029984\"\n     onclick=\"log_download('mikheykin-shirokov-marssi-mezzane-lyanguzov-pavlenko-stryukov-razumnaya-twinboundaryengineeringandthicknesseffectonstrontiumbariumniobatethinfilmsonmgosubstrate-2021', 'https://linkinghub.elsevier.com/retrieve/pii/S0925838821029984', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Twin-boundary engineering and thickness effect on strontium-barium niobate thin films on MgO substrate [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.jallcom.2021.161589\"\n     onclick=\"log_download('mikheykin-shirokov-marssi-mezzane-lyanguzov-pavlenko-stryukov-razumnaya-twinboundaryengineeringandthicknesseffectonstrontiumbariumniobatethinfilmsonmgosubstrate-2021', 'http://doi.org/10.1016/j.jallcom.2021.161589', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/mikheykin-shirokov-marssi-mezzane-lyanguzov-pavlenko-stryukov-razumnaya-twinboundaryengineeringandthicknesseffectonstrontiumbariumniobatethinfilmsonmgosubstrate-2021\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('mikheykin-shirokov-marssi-mezzane-lyanguzov-pavlenko-stryukov-razumnaya-twinboundaryengineeringandthicknesseffectonstrontiumbariumniobatethinfilmsonmgosubstrate-2021')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{mikheykin_twin-boundary_2021,\n\ttitle = {Twin-boundary engineering and thickness effect on strontium-barium niobate thin films on {MgO} substrate},\n\tvolume = {888},\n\tissn = {09258388},\n\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0925838821029984},\n\tdoi = {10.1016/j.jallcom.2021.161589},\n\tlanguage = {en},\n\turldate = {2023-11-10},\n\tjournal = {Journal of Alloys and Compounds},\n\tauthor = {Mikheykin, A.S. and Shirokov, V.B. and Marssi, M. El and Mezzane, D. and Lyanguzov, N.V. and Pavlenko, A.V. and Stryukov, D.V. and Razumnaya, A.G.},\n\tmonth = dec,\n\tyear = {2021},\n\tpages = {161589},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"ulyankina-molodtsova-gorshenkov-leontyev-zhigunov-konstantinova-lastovina-tolasz-etal-photocatalyticdegradationofciprofloxacininwateratnanoznopreparedbypulsealternatingcurrentelectrochemicalsynthesis-2021\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S2214714420306863\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'ulyankina-molodtsova-gorshenkov-leontyev-zhigunov-konstantinova-lastovina-tolasz-etal-photocatalyticdegradationofciprofloxacininwateratnanoznopreparedbypulsealternatingcurrentelectrochemicalsynthesis-2021', 'https://linkinghub.elsevier.com/retrieve/pii/S2214714420306863', event);\">\n    Photocatalytic degradation of ciprofloxacin in water at nano-ZnO prepared by pulse alternating current electrochemical synthesis.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Ulyankina, A.; Molodtsova, T.; Gorshenkov, M.; Leontyev, I.; Zhigunov, D.; Konstantinova, E.; Lastovina, T.; Tolasz, J.; Henych, J.; Licciardello, N.; Cuniberti, G.;  and Smirnova, N.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Water Process Engineering</i>, 40: 101809. April 2021.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S2214714420306863\"\n     onclick=\"log_download('ulyankina-molodtsova-gorshenkov-leontyev-zhigunov-konstantinova-lastovina-tolasz-etal-photocatalyticdegradationofciprofloxacininwateratnanoznopreparedbypulsealternatingcurrentelectrochemicalsynthesis-2021', 'https://linkinghub.elsevier.com/retrieve/pii/S2214714420306863', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Photocatalytic degradation of ciprofloxacin in water at nano-ZnO prepared by pulse alternating current electrochemical synthesis [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.jwpe.2020.101809\"\n     onclick=\"log_download('ulyankina-molodtsova-gorshenkov-leontyev-zhigunov-konstantinova-lastovina-tolasz-etal-photocatalyticdegradationofciprofloxacininwateratnanoznopreparedbypulsealternatingcurrentelectrochemicalsynthesis-2021', 'http://doi.org/10.1016/j.jwpe.2020.101809', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/ulyankina-molodtsova-gorshenkov-leontyev-zhigunov-konstantinova-lastovina-tolasz-etal-photocatalyticdegradationofciprofloxacininwateratnanoznopreparedbypulsealternatingcurrentelectrochemicalsynthesis-2021\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('ulyankina-molodtsova-gorshenkov-leontyev-zhigunov-konstantinova-lastovina-tolasz-etal-photocatalyticdegradationofciprofloxacininwateratnanoznopreparedbypulsealternatingcurrentelectrochemicalsynthesis-2021')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{ulyankina_photocatalytic_2021,\n\ttitle = {Photocatalytic degradation of ciprofloxacin in water at nano-{ZnO} prepared by pulse alternating current electrochemical synthesis},\n\tvolume = {40},\n\tissn = {22147144},\n\turl = {https://linkinghub.elsevier.com/retrieve/pii/S2214714420306863},\n\tdoi = {10.1016/j.jwpe.2020.101809},\n\tlanguage = {en},\n\turldate = {2023-11-10},\n\tjournal = {Journal of Water Process Engineering},\n\tauthor = {Ulyankina, Anna and Molodtsova, Tatiana and Gorshenkov, Mikhail and Leontyev, Igor and Zhigunov, Denis and Konstantinova, Elizaveta and Lastovina, Tatiana and Tolasz, Jakub and Henych, Jiří and Licciardello, Nadia and Cuniberti, Gianaurelio and Smirnova, Nina},\n\tmonth = apr,\n\tyear = {2021},\n\tpages = {101809},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"linnik-mikheykin-rubi-shirokov-mezzane-kondovych-lukyanchuk-razumnaya-ramanresponseofquantumcriticalferroelectricpbdopedsrtiotextrm3-2021\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.mdpi.com/2073-4352/11/12/1469\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'linnik-mikheykin-rubi-shirokov-mezzane-kondovych-lukyanchuk-razumnaya-ramanresponseofquantumcriticalferroelectricpbdopedsrtiotextrm3-2021', 'https://www.mdpi.com/2073-4352/11/12/1469', event);\">\n    Raman Response of Quantum Critical Ferroelectric Pb-Doped SrTiO$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Linnik, E. D.; Mikheykin, A. S.; Rubi, D.; Shirokov, V. B.; Mezzane, D.; Kondovych, S. V.; Lukyanchuk, I. A.;  and Razumnaya, A. G.\n</span>\n\n  \n\n</span>\n\n  <i>Crystals</i>, 11(12): 1469. November 2021.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.mdpi.com/2073-4352/11/12/1469\"\n     onclick=\"log_download('linnik-mikheykin-rubi-shirokov-mezzane-kondovych-lukyanchuk-razumnaya-ramanresponseofquantumcriticalferroelectricpbdopedsrtiotextrm3-2021', 'https://www.mdpi.com/2073-4352/11/12/1469', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Raman Response of Quantum Critical Ferroelectric Pb-Doped SrTiO$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3390/cryst11121469\"\n     onclick=\"log_download('linnik-mikheykin-rubi-shirokov-mezzane-kondovych-lukyanchuk-razumnaya-ramanresponseofquantumcriticalferroelectricpbdopedsrtiotextrm3-2021', 'http://doi.org/10.3390/cryst11121469', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/linnik-mikheykin-rubi-shirokov-mezzane-kondovych-lukyanchuk-razumnaya-ramanresponseofquantumcriticalferroelectricpbdopedsrtiotextrm3-2021\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('linnik-mikheykin-rubi-shirokov-mezzane-kondovych-lukyanchuk-razumnaya-ramanresponseofquantumcriticalferroelectricpbdopedsrtiotextrm3-2021')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{linnik_raman_2021,\n\ttitle = {Raman {Response} of {Quantum} {Critical} {Ferroelectric} {Pb}-{Doped} {SrTiO}$_{\\textrm{3}}$},\n\tvolume = {11},\n\tissn = {2073-4352},\n\turl = {https://www.mdpi.com/2073-4352/11/12/1469},\n\tdoi = {10.3390/cryst11121469},\n\tabstract = {A quantum paraelectric SrTiO3 is a material situated in close proximity to a quantum critical point (QCP) of ferroelectric transition in which the critical temperature to the ferroelectric state is suppressed down to 0 K. However, the understanding of the behavior of the phase transition in the vicinity of this point remains challenging. Using the concentration x of Pb in solid solution Sr1−xPbxTiO3 (PSTx) as a tuning parameter and applying the combination of Raman and dielectric spectroscopy methods, we approach the QCP in PSTx and study the interplay of classical and quantum phenomena in the region of criticality. We obtain the critical temperature of PSTx and the evolution of the temperature-dependent dynamical properties of the system as a function of x to reveal the mechanism of the transition. We show that the ferroelectric transition occurs gradually through the emergence of the polar nanoregions inside the non-polar tetragonal phase with their further expansion on cooling. We also study the ferroelastic cubic-to-tetragonal structural transition, occurring at higher temperatures, and show that its properties are almost concentration-independent and not affected by the quantum criticality.},\n\tlanguage = {en},\n\tnumber = {12},\n\turldate = {2023-11-10},\n\tjournal = {Crystals},\n\tauthor = {Linnik, Ekaterina D. and Mikheykin, Alexey S. and Rubi, Diego and Shirokov, Vladimir B. and Mezzane, Daoud and Kondovych, Svitlana V. and Lukyanchuk, Igor A. and Razumnaya, Anna G.},\n\tmonth = nov,\n\tyear = {2021},\n\tpages = {1469},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\DT8BPF4T\\\\Linnik и др. - 2021 - Raman Response of Quantum Critical Ferroelectric P.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A quantum paraelectric SrTiO3 is a material situated in close proximity to a quantum critical point (QCP) of ferroelectric transition in which the critical temperature to the ferroelectric state is suppressed down to 0 K. However, the understanding of the behavior of the phase transition in the vicinity of this point remains challenging. Using the concentration x of Pb in solid solution Sr1−xPbxTiO3 (PSTx) as a tuning parameter and applying the combination of Raman and dielectric spectroscopy methods, we approach the QCP in PSTx and study the interplay of classical and quantum phenomena in the region of criticality. We obtain the critical temperature of PSTx and the evolution of the temperature-dependent dynamical properties of the system as a function of x to reveal the mechanism of the transition. We show that the ferroelectric transition occurs gradually through the emergence of the polar nanoregions inside the non-polar tetragonal phase with their further expansion on cooling. We also study the ferroelastic cubic-to-tetragonal structural transition, occurring at higher temperatures, and show that its properties are almost concentration-independent and not affected by the quantum criticality.\n</div>\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2020\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2020')\"\n      onkeypress=\"toggleGroup('group_2020')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2020</span>\n      <span class=\"bibbase_group_count\">\n        \n        (25)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"ahlskog-hokkanen-levshov-svensson-volodin-vanhaesendonck-individualarcdischargesynthesizedmultiwalledcarbonnanotubesprobedwithmultiplemeasurementtechniques-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://pubs.aip.org/jvb/article/38/4/042804/592550/Individual-arc-discharge-synthesized-multiwalled\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'ahlskog-hokkanen-levshov-svensson-volodin-vanhaesendonck-individualarcdischargesynthesizedmultiwalledcarbonnanotubesprobedwithmultiplemeasurementtechniques-2020', 'https://pubs.aip.org/jvb/article/38/4/042804/592550/Individual-arc-discharge-synthesized-multiwalled', event);\">\n    Individual arc-discharge synthesized multiwalled carbon nanotubes probed with multiple measurement techniques.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Ahlskog, M.; Hokkanen, M. J.; Levshov, D.; Svensson, K.; Volodin, A.;  and Van Haesendonck, C.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Vacuum Science & Technology B, Nanotechnology and Microelectronics: Materials, Processing, Measurement, and Phenomena</i>, 38(4): 042804. July 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://pubs.aip.org/jvb/article/38/4/042804/592550/Individual-arc-discharge-synthesized-multiwalled\"\n     onclick=\"log_download('ahlskog-hokkanen-levshov-svensson-volodin-vanhaesendonck-individualarcdischargesynthesizedmultiwalledcarbonnanotubesprobedwithmultiplemeasurementtechniques-2020', 'https://pubs.aip.org/jvb/article/38/4/042804/592550/Individual-arc-discharge-synthesized-multiwalled', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Individual arc-discharge synthesized multiwalled carbon nanotubes probed with multiple measurement techniques [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1116/6.0000187\"\n     onclick=\"log_download('ahlskog-hokkanen-levshov-svensson-volodin-vanhaesendonck-individualarcdischargesynthesizedmultiwalledcarbonnanotubesprobedwithmultiplemeasurementtechniques-2020', 'http://doi.org/10.1116/6.0000187', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/ahlskog-hokkanen-levshov-svensson-volodin-vanhaesendonck-individualarcdischargesynthesizedmultiwalledcarbonnanotubesprobedwithmultiplemeasurementtechniques-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('ahlskog-hokkanen-levshov-svensson-volodin-vanhaesendonck-individualarcdischargesynthesizedmultiwalledcarbonnanotubesprobedwithmultiplemeasurementtechniques-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{ahlskog_individual_2020,\n\ttitle = {Individual arc-discharge synthesized multiwalled carbon nanotubes probed with multiple measurement techniques},\n\tvolume = {38},\n\tissn = {2166-2746, 2166-2754},\n\turl = {https://pubs.aip.org/jvb/article/38/4/042804/592550/Individual-arc-discharge-synthesized-multiwalled},\n\tdoi = {10.1116/6.0000187},\n\tabstract = {Arc-discharge synthesized multiwalled carbon nanotubes (AD-MWNT), or related MWNTs, exhibit a good quality compared to the more common type of MWNT synthesized by catalytic chemical vapor deposition methods. Yet experimental measurements on these are rather few and typically have not correlated data from different measurement techniques. Here, the authors report Raman spectroscopy, scanning probe microscopy, conductivity measurements, and force microscopy on single AD-MWNTs. The results demonstrate the high quality of AD-MWNTs and are compatible with the view of them as the best approximation of MWNTs as an assembly of defect-free concentric individual single-walled carbon nanotubes. The authors also demonstrate conductance measurements over a step on the surface of an AD-MWNT, which is due to an abruptly broken outer layer(s), whereby the interlayer resistance is measured.},\n\tlanguage = {en},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Vacuum Science \\&amp; Technology B, Nanotechnology and Microelectronics: Materials, Processing, Measurement, and Phenomena},\n\tauthor = {Ahlskog, Markus and Hokkanen, Matti J. and Levshov, Dmitry and Svensson, Krister and Volodin, Alexander and Van Haesendonck, Chris},\n\tmonth = jul,\n\tyear = {2020},\n\tpages = {042804},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\76DFFX6C\\\\Ahlskog и др. - 2020 - Individual arc-discharge synthesized multiwalled c.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Arc-discharge synthesized multiwalled carbon nanotubes (AD-MWNT), or related MWNTs, exhibit a good quality compared to the more common type of MWNT synthesized by catalytic chemical vapor deposition methods. Yet experimental measurements on these are rather few and typically have not correlated data from different measurement techniques. Here, the authors report Raman spectroscopy, scanning probe microscopy, conductivity measurements, and force microscopy on single AD-MWNTs. The results demonstrate the high quality of AD-MWNTs and are compatible with the view of them as the best approximation of MWNTs as an assembly of defect-free concentric individual single-walled carbon nanotubes. The authors also demonstrate conductance measurements over a step on the surface of an AD-MWNT, which is due to an abruptly broken outer layer(s), whereby the interlayer resistance is measured.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"chalin-rochal-bandstructureandintertubeopticaltransitionsindoublewalledcarbonnanotubes-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.102.115426\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'chalin-rochal-bandstructureandintertubeopticaltransitionsindoublewalledcarbonnanotubes-2020', 'https://link.aps.org/doi/10.1103/PhysRevB.102.115426', event);\">\n    Band structure and inter-tube optical transitions in double-walled carbon nanotubes.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Chalin, D. V.;  and Rochal, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 102(11): 115426. September 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.102.115426\"\n     onclick=\"log_download('chalin-rochal-bandstructureandintertubeopticaltransitionsindoublewalledcarbonnanotubes-2020', 'https://link.aps.org/doi/10.1103/PhysRevB.102.115426', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Band structure and inter-tube optical transitions in double-walled carbon nanotubes [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.102.115426\"\n     onclick=\"log_download('chalin-rochal-bandstructureandintertubeopticaltransitionsindoublewalledcarbonnanotubes-2020', 'http://doi.org/10.1103/PhysRevB.102.115426', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/chalin-rochal-bandstructureandintertubeopticaltransitionsindoublewalledcarbonnanotubes-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('chalin-rochal-bandstructureandintertubeopticaltransitionsindoublewalledcarbonnanotubes-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{chalin_band_2020,\n\ttitle = {Band structure and inter-tube optical transitions in double-walled carbon nanotubes},\n\tvolume = {102},\n\tissn = {2469-9950, 2469-9969},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.102.115426},\n\tdoi = {10.1103/PhysRevB.102.115426},\n\tlanguage = {en},\n\tnumber = {11},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Chalin, D. V. and Rochal, S. B.},\n\tmonth = sep,\n\tyear = {2020},\n\tpages = {115426},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\2XJKU38W\\\\Chalin и Rochal - 2020 - Band structure and inter-tube optical transitions .pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"sadyrin-swain-mitrin-rzhepakovsky-nikolaev-irkha-yogina-lyanguzov-etal-characterizationofenamelanddentineaboutawhitespotlesionmechanicalpropertiesmineraldensitymicrostructureandmolecularcomposition-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.mdpi.com/2079-4991/10/9/1889\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'sadyrin-swain-mitrin-rzhepakovsky-nikolaev-irkha-yogina-lyanguzov-etal-characterizationofenamelanddentineaboutawhitespotlesionmechanicalpropertiesmineraldensitymicrostructureandmolecularcomposition-2020', 'https://www.mdpi.com/2079-4991/10/9/1889', event);\">\n    Characterization of Enamel and Dentine about a White Spot Lesion: Mechanical Properties, Mineral Density, Microstructure and Molecular Composition.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Sadyrin, E.; Swain, M.; Mitrin, B.; Rzhepakovsky, I.; Nikolaev, A.; Irkha, V.; Yogina, D.; Lyanguzov, N.; Maksyukov, S.;  and Aizikovich, S.\n</span>\n\n  \n\n</span>\n\n  <i>Nanomaterials</i>, 10(9): 1889. September 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.mdpi.com/2079-4991/10/9/1889\"\n     onclick=\"log_download('sadyrin-swain-mitrin-rzhepakovsky-nikolaev-irkha-yogina-lyanguzov-etal-characterizationofenamelanddentineaboutawhitespotlesionmechanicalpropertiesmineraldensitymicrostructureandmolecularcomposition-2020', 'https://www.mdpi.com/2079-4991/10/9/1889', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Characterization of Enamel and Dentine about a White Spot Lesion: Mechanical Properties, Mineral Density, Microstructure and Molecular Composition [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3390/nano10091889\"\n     onclick=\"log_download('sadyrin-swain-mitrin-rzhepakovsky-nikolaev-irkha-yogina-lyanguzov-etal-characterizationofenamelanddentineaboutawhitespotlesionmechanicalpropertiesmineraldensitymicrostructureandmolecularcomposition-2020', 'http://doi.org/10.3390/nano10091889', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/sadyrin-swain-mitrin-rzhepakovsky-nikolaev-irkha-yogina-lyanguzov-etal-characterizationofenamelanddentineaboutawhitespotlesionmechanicalpropertiesmineraldensitymicrostructureandmolecularcomposition-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('sadyrin-swain-mitrin-rzhepakovsky-nikolaev-irkha-yogina-lyanguzov-etal-characterizationofenamelanddentineaboutawhitespotlesionmechanicalpropertiesmineraldensitymicrostructureandmolecularcomposition-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{sadyrin_characterization_2020,\n\ttitle = {Characterization of {Enamel} and {Dentine} about a {White} {Spot} {Lesion}: {Mechanical} {Properties}, {Mineral} {Density}, {Microstructure} and {Molecular} {Composition}},\n\tvolume = {10},\n\tissn = {2079-4991},\n\tshorttitle = {Characterization of {Enamel} and {Dentine} about a {White} {Spot} {Lesion}},\n\turl = {https://www.mdpi.com/2079-4991/10/9/1889},\n\tdoi = {10.3390/nano10091889},\n\tabstract = {The study focuses on in vitro tracing of some fundamental changes that emerge in teeth at the initial stage of caries development using multiple approaches. The research was conducted on a mostly sound maxillary molar tooth but with a clearly visible natural proximal white spot lesion (WSL). Values of mineral density, reduced Young’s modulus, indentation hardness and creep as well as the molecular composition and surface microstructure of the WSL and bordering dentine area were studied. The results obtained were compared to those of sound enamel and dentine on the same tooth. A decrease of mechanical properties and mineral density both for the WSL and bordering dentine was detected in comparison to the sound counterparts, as well as increase of creep for the enamel WSL. Differences in molecular composition and surface microstructure (including the indenter impressions) were found and described. WSL induces a serious change in the state of not only the visually affected enamel but also surrounding visually intact enamel and dentine in its vicinity. The results provide the basis for future studies of efficacy of minimal invasive treatments of caries.},\n\tlanguage = {en},\n\tnumber = {9},\n\turldate = {2023-11-11},\n\tjournal = {Nanomaterials},\n\tauthor = {Sadyrin, Evgeniy and Swain, Michael and Mitrin, Boris and Rzhepakovsky, Igor and Nikolaev, Andrey and Irkha, Vladimir and Yogina, Diana and Lyanguzov, Nikolay and Maksyukov, Stanislav and Aizikovich, Sergei},\n\tmonth = sep,\n\tyear = {2020},\n\tpages = {1889},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\95JZJ5NP\\\\Sadyrin и др. - 2020 - Characterization of Enamel and Dentine about a Whi.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The study focuses on in vitro tracing of some fundamental changes that emerge in teeth at the initial stage of caries development using multiple approaches. The research was conducted on a mostly sound maxillary molar tooth but with a clearly visible natural proximal white spot lesion (WSL). Values of mineral density, reduced Young’s modulus, indentation hardness and creep as well as the molecular composition and surface microstructure of the WSL and bordering dentine area were studied. The results obtained were compared to those of sound enamel and dentine on the same tooth. A decrease of mechanical properties and mineral density both for the WSL and bordering dentine was detected in comparison to the sound counterparts, as well as increase of creep for the enamel WSL. Differences in molecular composition and surface microstructure (including the indenter impressions) were found and described. WSL induces a serious change in the state of not only the visually affected enamel but also surrounding visually intact enamel and dentine in its vicinity. The results provide the basis for future studies of efficacy of minimal invasive treatments of caries.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kuriganova-faddeev-gorshenkov-kuznetsov-leontyev-smirnova-acomparisonofbottomupandtopdownapproachestothesynthesisofptcelectrocatalysts-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.mdpi.com/2227-9717/8/8/947\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kuriganova-faddeev-gorshenkov-kuznetsov-leontyev-smirnova-acomparisonofbottomupandtopdownapproachestothesynthesisofptcelectrocatalysts-2020', 'https://www.mdpi.com/2227-9717/8/8/947', event);\">\n    A Comparison of “Bottom-Up” and “Top-Down” Approaches to the Synthesis of Pt/C Electrocatalysts.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kuriganova, A.; Faddeev, N.; Gorshenkov, M.; Kuznetsov, D.; Leontyev, I.;  and Smirnova, N.\n</span>\n\n  \n\n</span>\n\n  <i>Processes</i>, 8(8): 947. August 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.mdpi.com/2227-9717/8/8/947\"\n     onclick=\"log_download('kuriganova-faddeev-gorshenkov-kuznetsov-leontyev-smirnova-acomparisonofbottomupandtopdownapproachestothesynthesisofptcelectrocatalysts-2020', 'https://www.mdpi.com/2227-9717/8/8/947', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"A Comparison of “Bottom-Up” and “Top-Down” Approaches to the Synthesis of Pt/C Electrocatalysts [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3390/pr8080947\"\n     onclick=\"log_download('kuriganova-faddeev-gorshenkov-kuznetsov-leontyev-smirnova-acomparisonofbottomupandtopdownapproachestothesynthesisofptcelectrocatalysts-2020', 'http://doi.org/10.3390/pr8080947', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kuriganova-faddeev-gorshenkov-kuznetsov-leontyev-smirnova-acomparisonofbottomupandtopdownapproachestothesynthesisofptcelectrocatalysts-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kuriganova-faddeev-gorshenkov-kuznetsov-leontyev-smirnova-acomparisonofbottomupandtopdownapproachestothesynthesisofptcelectrocatalysts-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kuriganova_comparison_2020,\n\ttitle = {A {Comparison} of “{Bottom}-{Up}” and “{Top}-{Down}” {Approaches} to the {Synthesis} of {Pt}/{C} {Electrocatalysts}},\n\tvolume = {8},\n\tissn = {2227-9717},\n\turl = {https://www.mdpi.com/2227-9717/8/8/947},\n\tdoi = {10.3390/pr8080947},\n\tabstract = {Three 40 wt \\% Pt/C electrocatalysts prepared using two different approaches—the polyol process and electrochemical dispersion of platinum under pulse alternating current—and a commercial Pt/C catalyst (Johnson Matthey prod.) were examined via X-ray diffraction (XRD) and transmission electron microscopy (TEM). The stability characteristics of the Pt/C catalysts were studied via long-term cycling, revealing that, for all cycling modes, the best stability was achieved for the Pt/C catalyst with the largest platinum nanoparticle sizes, which was synthesized via electrochemical dispersion of platinum under pulse alternating current. Our results show that the mass and specific electrocatalytic activities of Pt/C catalysts toward ethanol electrooxidation are determined by the value of the electrochemically active Pt surface area in the catalysts.},\n\tlanguage = {en},\n\tnumber = {8},\n\turldate = {2023-11-11},\n\tjournal = {Processes},\n\tauthor = {Kuriganova, Alexandra and Faddeev, Nikita and Gorshenkov, Mikhail and Kuznetsov, Dmitri and Leontyev, Igor and Smirnova, Nina},\n\tmonth = aug,\n\tyear = {2020},\n\tpages = {947},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\86DZKUPG\\\\Kuriganova и др. - 2020 - A Comparison of “Bottom-Up” and “Top-Down” Approac.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Three 40 wt % Pt/C electrocatalysts prepared using two different approaches—the polyol process and electrochemical dispersion of platinum under pulse alternating current—and a commercial Pt/C catalyst (Johnson Matthey prod.) were examined via X-ray diffraction (XRD) and transmission electron microscopy (TEM). The stability characteristics of the Pt/C catalysts were studied via long-term cycling, revealing that, for all cycling modes, the best stability was achieved for the Pt/C catalyst with the largest platinum nanoparticle sizes, which was synthesized via electrochemical dispersion of platinum under pulse alternating current. Our results show that the mass and specific electrocatalytic activities of Pt/C catalysts toward ethanol electrooxidation are determined by the value of the electrochemically active Pt surface area in the catalysts.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kuriganova-chernysheva-faddeev-leontyev-smirnova-dobrovolskii-pacsynthesisandcomparisonofcatalystsfordirectethanolfuelcells-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.mdpi.com/2227-9717/8/6/712\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kuriganova-chernysheva-faddeev-leontyev-smirnova-dobrovolskii-pacsynthesisandcomparisonofcatalystsfordirectethanolfuelcells-2020', 'https://www.mdpi.com/2227-9717/8/6/712', event);\">\n    PAC Synthesis and Comparison of Catalysts for Direct Ethanol Fuel Cells.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kuriganova, A.; Chernysheva, D.; Faddeev, N.; Leontyev, I.; Smirnova, N.;  and Dobrovolskii, Y.\n</span>\n\n  \n\n</span>\n\n  <i>Processes</i>, 8(6): 712. June 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.mdpi.com/2227-9717/8/6/712\"\n     onclick=\"log_download('kuriganova-chernysheva-faddeev-leontyev-smirnova-dobrovolskii-pacsynthesisandcomparisonofcatalystsfordirectethanolfuelcells-2020', 'https://www.mdpi.com/2227-9717/8/6/712', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"PAC Synthesis and Comparison of Catalysts for Direct Ethanol Fuel Cells [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3390/pr8060712\"\n     onclick=\"log_download('kuriganova-chernysheva-faddeev-leontyev-smirnova-dobrovolskii-pacsynthesisandcomparisonofcatalystsfordirectethanolfuelcells-2020', 'http://doi.org/10.3390/pr8060712', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kuriganova-chernysheva-faddeev-leontyev-smirnova-dobrovolskii-pacsynthesisandcomparisonofcatalystsfordirectethanolfuelcells-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kuriganova-chernysheva-faddeev-leontyev-smirnova-dobrovolskii-pacsynthesisandcomparisonofcatalystsfordirectethanolfuelcells-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kuriganova_pac_2020,\n\ttitle = {{PAC} {Synthesis} and {Comparison} of {Catalysts} for {Direct} {Ethanol} {Fuel} {Cells}},\n\tvolume = {8},\n\tissn = {2227-9717},\n\turl = {https://www.mdpi.com/2227-9717/8/6/712},\n\tdoi = {10.3390/pr8060712},\n\tabstract = {Pt/C, PtMOn/C (M = Ni, Sn, Ti, and PtX/C (X = Rh, Ir) catalyst systems were prepared by using the pulse alternating current (PAC) technique. Physical and electrochemical parameters of samples were carried out by x-ray powder diffraction (XRD), transmission electron microscopy (TEM), and CO stripping. The catalytic activity of the synthesized samples for the ethanol electrooxidation reaction (EOR) was investigated. The XRD patterns of the samples showed the presence of diffraction peaks characteristic for Pt, NiO, SnO2, TiO2, Rh, and Ir. The TEM images indicate that the Pt, Rh, and PtIr (alloys) particles had a uniform distribution over the carbon surface in the Pt/C, PtRh/C, PtIr/C, and PtMOn/C (M = Ni, Sn, Ti) catalysts. The electrochemically active surface area of catalysts was determined by the CO-stripping method. The addition of a second element to Pt or the use of hybrid supported catalysts can evidently improve the EOR activity. A remarkable positive affecting shift of the onset potential for the EOR was observed as follows: PtSnO2/C {\\textgreater} PtTiO2/C ≈ PtIr/C ≈ PtNiO/C {\\textgreater} PtRh/C ≈ Pt/C. The addition of SnO2 to Pt/C catalyst led to the decrease of the onset potential and to significantly facilitate the EOR. The long-term cyclic stability of the synthesized catalysts was investigated. Thereby, the PtSnO2/C catalyst prepared by the PAC technique can be considered as a promising anode catalyst for direct ethanol fuel cells.},\n\tlanguage = {en},\n\tnumber = {6},\n\turldate = {2023-11-11},\n\tjournal = {Processes},\n\tauthor = {Kuriganova, Alexandra and Chernysheva, Daria and Faddeev, Nikita and Leontyev, Igor and Smirnova, Nina and Dobrovolskii, Yury},\n\tmonth = jun,\n\tyear = {2020},\n\tpages = {712},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\JUTMKRJV\\\\Kuriganova и др. - 2020 - PAC Synthesis and Comparison of Catalysts for Dire.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Pt/C, PtMOn/C (M = Ni, Sn, Ti, and PtX/C (X = Rh, Ir) catalyst systems were prepared by using the pulse alternating current (PAC) technique. Physical and electrochemical parameters of samples were carried out by x-ray powder diffraction (XRD), transmission electron microscopy (TEM), and CO stripping. The catalytic activity of the synthesized samples for the ethanol electrooxidation reaction (EOR) was investigated. The XRD patterns of the samples showed the presence of diffraction peaks characteristic for Pt, NiO, SnO2, TiO2, Rh, and Ir. The TEM images indicate that the Pt, Rh, and PtIr (alloys) particles had a uniform distribution over the carbon surface in the Pt/C, PtRh/C, PtIr/C, and PtMOn/C (M = Ni, Sn, Ti) catalysts. The electrochemically active surface area of catalysts was determined by the CO-stripping method. The addition of a second element to Pt or the use of hybrid supported catalysts can evidently improve the EOR activity. A remarkable positive affecting shift of the onset potential for the EOR was observed as follows: PtSnO2/C \\textgreater PtTiO2/C ≈ PtIr/C ≈ PtNiO/C \\textgreater PtRh/C ≈ Pt/C. The addition of SnO2 to Pt/C catalyst led to the decrease of the onset potential and to significantly facilitate the EOR. The long-term cyclic stability of the synthesized catalysts was investigated. Thereby, the PtSnO2/C catalyst prepared by the PAC technique can be considered as a promising anode catalyst for direct ethanol fuel cells.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"roshal-azzag-legoff-rochal-baghdiguian-crystallikeorderanddefectsinmetazoanepitheliawithsphericalgeometry-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.nature.com/articles/s41598-020-64598-w\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'roshal-azzag-legoff-rochal-baghdiguian-crystallikeorderanddefectsinmetazoanepitheliawithsphericalgeometry-2020', 'https://www.nature.com/articles/s41598-020-64598-w', event);\">\n    Crystal-like order and defects in metazoan epithelia with spherical geometry.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Roshal, D. S.; Azzag, K.; Le Goff, E.; Rochal, S. B.;  and Baghdiguian, S.\n</span>\n\n  \n\n</span>\n\n  <i>Scientific Reports</i>, 10(1): 7652. May 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.nature.com/articles/s41598-020-64598-w\"\n     onclick=\"log_download('roshal-azzag-legoff-rochal-baghdiguian-crystallikeorderanddefectsinmetazoanepitheliawithsphericalgeometry-2020', 'https://www.nature.com/articles/s41598-020-64598-w', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Crystal-like order and defects in metazoan epithelia with spherical geometry [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1038/s41598-020-64598-w\"\n     onclick=\"log_download('roshal-azzag-legoff-rochal-baghdiguian-crystallikeorderanddefectsinmetazoanepitheliawithsphericalgeometry-2020', 'http://doi.org/10.1038/s41598-020-64598-w', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/roshal-azzag-legoff-rochal-baghdiguian-crystallikeorderanddefectsinmetazoanepitheliawithsphericalgeometry-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('roshal-azzag-legoff-rochal-baghdiguian-crystallikeorderanddefectsinmetazoanepitheliawithsphericalgeometry-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{roshal_crystal-like_2020,\n\ttitle = {Crystal-like order and defects in metazoan epithelia with spherical geometry},\n\tvolume = {10},\n\tissn = {2045-2322},\n\turl = {https://www.nature.com/articles/s41598-020-64598-w},\n\tdoi = {10.1038/s41598-020-64598-w},\n\tabstract = {Abstract\n            Since Robert Hooke studied cork cell patterns in 1665, scientists have been puzzled by why cells form such ordered structures. The laws underlying this type of organization are universal, and we study them comparing the living and non-living two-dimensional systems self-organizing at the spherical surface. Such-type physical systems often possess trigonal order with specific elongated defects, scars and pleats, where the 5-valence and 7-valence vertices alternate. In spite of the fact that the same physical and topological rules are involved in the structural organization of biological systems, such topological defects were never reported in epithelia. We have discovered them in the follicular spherical epithelium of ascidians that are emerging models in developmental biology. Surprisingly, the considered defects appear in the epithelium even when the number of cells in it is significantly less than the previously known threshold value. We explain this result by differences in the cell sizes and check our hypothesis considering the self-assembly of different random size particles on the spherical surface. Scars, pleats and other complex defects found in ascidian samples can play an unexpected and decisive role in the permanent renewal and reorganization of epithelia, which forms or lines many tissues and organs in metazoans.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Scientific Reports},\n\tauthor = {Roshal, Daria S. and Azzag, Karim and Le Goff, Emilie and Rochal, Sergei B. and Baghdiguian, Stephen},\n\tmonth = may,\n\tyear = {2020},\n\tpages = {7652},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\JI45G85W\\\\Roshal и др. - 2020 - Crystal-like order and defects in metazoan epithel.pdf:application/pdf;Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\J7BDDRP3\\\\Roshal и др. - 2020 - Crystal-like order and defects in metazoan epithel.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Abstract Since Robert Hooke studied cork cell patterns in 1665, scientists have been puzzled by why cells form such ordered structures. The laws underlying this type of organization are universal, and we study them comparing the living and non-living two-dimensional systems self-organizing at the spherical surface. Such-type physical systems often possess trigonal order with specific elongated defects, scars and pleats, where the 5-valence and 7-valence vertices alternate. In spite of the fact that the same physical and topological rules are involved in the structural organization of biological systems, such topological defects were never reported in epithelia. We have discovered them in the follicular spherical epithelium of ascidians that are emerging models in developmental biology. Surprisingly, the considered defects appear in the epithelium even when the number of cells in it is significantly less than the previously known threshold value. We explain this result by differences in the cell sizes and check our hypothesis considering the self-assembly of different random size particles on the spherical surface. Scars, pleats and other complex defects found in ascidian samples can play an unexpected and decisive role in the permanent renewal and reorganization of epithelia, which forms or lines many tissues and organs in metazoans.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kaydashev-timoshenko-kutepov-karapetyan-kirtaev-kaidashev-surfaceacousticwavesbasedmethodtostudyphotothermalresponseofplasmonicnanoobjectsandmetasurfaces-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.spiedigitallibrary.org/conference-proceedings-of-spie/11457/2559972/Surface-acoustic-waves-based-method-to-study-photothermal-response-of/10.1117/12.2559972.full\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kaydashev-timoshenko-kutepov-karapetyan-kirtaev-kaidashev-surfaceacousticwavesbasedmethodtostudyphotothermalresponseofplasmonicnanoobjectsandmetasurfaces-2020', 'https://www.spiedigitallibrary.org/conference-proceedings-of-spie/11457/2559972/Surface-acoustic-waves-based-method-to-study-photothermal-response-of/10.1117/12.2559972.full', event);\">\n    Surface acoustic waves based method to study photothermal response of plasmonic nano-objects and metasurfaces.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kaydashev, V. E.; Timoshenko, P.; Kutepov, M.; Karapetyan, G.; Kirtaev, R.;  and Kaidashev, E.\n</span>\n\n  \n\n</span>\n\n  In Tuchin, V. V.;  and Genina, E. A., editor(s), <i>Saratov Fall Meeting 2019: Optical and Nano-Technologies for Biology and Medicine</i>, pages 13, Saratov, Russian Federation, April 2020. SPIE\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.spiedigitallibrary.org/conference-proceedings-of-spie/11457/2559972/Surface-acoustic-waves-based-method-to-study-photothermal-response-of/10.1117/12.2559972.full\"\n     onclick=\"log_download('kaydashev-timoshenko-kutepov-karapetyan-kirtaev-kaidashev-surfaceacousticwavesbasedmethodtostudyphotothermalresponseofplasmonicnanoobjectsandmetasurfaces-2020', 'https://www.spiedigitallibrary.org/conference-proceedings-of-spie/11457/2559972/Surface-acoustic-waves-based-method-to-study-photothermal-response-of/10.1117/12.2559972.full', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Surface acoustic waves based method to study photothermal response of plasmonic nano-objects and metasurfaces [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1117/12.2559972\"\n     onclick=\"log_download('kaydashev-timoshenko-kutepov-karapetyan-kirtaev-kaidashev-surfaceacousticwavesbasedmethodtostudyphotothermalresponseofplasmonicnanoobjectsandmetasurfaces-2020', 'http://doi.org/10.1117/12.2559972', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kaydashev-timoshenko-kutepov-karapetyan-kirtaev-kaidashev-surfaceacousticwavesbasedmethodtostudyphotothermalresponseofplasmonicnanoobjectsandmetasurfaces-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kaydashev-timoshenko-kutepov-karapetyan-kirtaev-kaidashev-surfaceacousticwavesbasedmethodtostudyphotothermalresponseofplasmonicnanoobjectsandmetasurfaces-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{kaydashev_surface_2020,\n\taddress = {Saratov, Russian Federation},\n\ttitle = {Surface acoustic waves based method to study photothermal response of plasmonic nano-objects and metasurfaces},\n\tisbn = {978-1-5106-3718-4 978-1-5106-3719-1},\n\turl = {https://www.spiedigitallibrary.org/conference-proceedings-of-spie/11457/2559972/Surface-acoustic-waves-based-method-to-study-photothermal-response-of/10.1117/12.2559972.full},\n\tdoi = {10.1117/12.2559972},\n\turldate = {2023-11-11},\n\tbooktitle = {Saratov {Fall} {Meeting} 2019: {Optical} and {Nano}-{Technologies} for {Biology} and {Medicine}},\n\tpublisher = {SPIE},\n\tauthor = {Kaydashev, Vladimir E. and Timoshenko, Pavel and Kutepov, Maxim and Karapetyan, Gevork and Kirtaev, Roman and Kaidashev, Evgeni},\n\teditor = {Tuchin, Valery V. and Genina, Elina A.},\n\tmonth = apr,\n\tyear = {2020},\n\tpages = {13},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"tikhonov-kondovych-mangeri-pavlenko-baudry-sen-galda-nakhmanson-etal-controllableskyrmionchiralityinferroelectrics-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.nature.com/articles/s41598-020-65291-8\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'tikhonov-kondovych-mangeri-pavlenko-baudry-sen-galda-nakhmanson-etal-controllableskyrmionchiralityinferroelectrics-2020', 'https://www.nature.com/articles/s41598-020-65291-8', event);\">\n    Controllable skyrmion chirality in ferroelectrics.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Tikhonov, Y.; Kondovych, S.; Mangeri, J.; Pavlenko, M.; Baudry, L.; Sené, A.; Galda, A.; Nakhmanson, S.; Heinonen, O.; Razumnaya, A.; Luk’yanchuk, I.;  and Vinokur, V. M.\n</span>\n\n  \n\n</span>\n\n  <i>Scientific Reports</i>, 10(1): 8657. May 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.nature.com/articles/s41598-020-65291-8\"\n     onclick=\"log_download('tikhonov-kondovych-mangeri-pavlenko-baudry-sen-galda-nakhmanson-etal-controllableskyrmionchiralityinferroelectrics-2020', 'https://www.nature.com/articles/s41598-020-65291-8', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Controllable skyrmion chirality in ferroelectrics [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1038/s41598-020-65291-8\"\n     onclick=\"log_download('tikhonov-kondovych-mangeri-pavlenko-baudry-sen-galda-nakhmanson-etal-controllableskyrmionchiralityinferroelectrics-2020', 'http://doi.org/10.1038/s41598-020-65291-8', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/tikhonov-kondovych-mangeri-pavlenko-baudry-sen-galda-nakhmanson-etal-controllableskyrmionchiralityinferroelectrics-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('tikhonov-kondovych-mangeri-pavlenko-baudry-sen-galda-nakhmanson-etal-controllableskyrmionchiralityinferroelectrics-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{tikhonov_controllable_2020,\n\ttitle = {Controllable skyrmion chirality in ferroelectrics},\n\tvolume = {10},\n\tissn = {2045-2322},\n\turl = {https://www.nature.com/articles/s41598-020-65291-8},\n\tdoi = {10.1038/s41598-020-65291-8},\n\tabstract = {Abstract\n            Chirality, an intrinsic handedness, is one of the most intriguing fundamental phenomena in nature. Materials composed of chiral molecules find broad applications in areas ranging from nonlinear optics and spintronics to biology and pharmaceuticals. However, chirality is usually an invariable inherent property of a given material that cannot be easily changed at will. Here, we demonstrate that ferroelectric nanodots support skyrmions the chirality of which can be controlled and switched. We devise protocols for realizing control and efficient manipulations of the different types of skyrmions. Our findings open the route for controlled chirality with potential applications in ferroelectric-based information technologies.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Scientific Reports},\n\tauthor = {Tikhonov, Yu. and Kondovych, S. and Mangeri, J. and Pavlenko, M. and Baudry, L. and Sené, A. and Galda, A. and Nakhmanson, S. and Heinonen, O. and Razumnaya, A. and Luk’yanchuk, I. and Vinokur, V. M.},\n\tmonth = may,\n\tyear = {2020},\n\tpages = {8657},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\AXZJJ5II\\\\Tikhonov и др. - 2020 - Controllable skyrmion chirality in ferroelectrics.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Abstract Chirality, an intrinsic handedness, is one of the most intriguing fundamental phenomena in nature. Materials composed of chiral molecules find broad applications in areas ranging from nonlinear optics and spintronics to biology and pharmaceuticals. However, chirality is usually an invariable inherent property of a given material that cannot be easily changed at will. Here, we demonstrate that ferroelectric nanodots support skyrmions the chirality of which can be controlled and switched. We devise protocols for realizing control and efficient manipulations of the different types of skyrmions. Our findings open the route for controlled chirality with potential applications in ferroelectric-based information technologies.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"lukyanchuk-tikhonov-razumnaya-vinokur-hopfionsemergeinferroelectrics-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.nature.com/articles/s41467-020-16258-w\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'lukyanchuk-tikhonov-razumnaya-vinokur-hopfionsemergeinferroelectrics-2020', 'https://www.nature.com/articles/s41467-020-16258-w', event);\">\n    Hopfions emerge in ferroelectrics.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Luk’yanchuk, I.; Tikhonov, Y.; Razumnaya, A.;  and Vinokur, V. M.\n</span>\n\n  \n\n</span>\n\n  <i>Nature Communications</i>, 11(1): 2433. May 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.nature.com/articles/s41467-020-16258-w\"\n     onclick=\"log_download('lukyanchuk-tikhonov-razumnaya-vinokur-hopfionsemergeinferroelectrics-2020', 'https://www.nature.com/articles/s41467-020-16258-w', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Hopfions emerge in ferroelectrics [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1038/s41467-020-16258-w\"\n     onclick=\"log_download('lukyanchuk-tikhonov-razumnaya-vinokur-hopfionsemergeinferroelectrics-2020', 'http://doi.org/10.1038/s41467-020-16258-w', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/lukyanchuk-tikhonov-razumnaya-vinokur-hopfionsemergeinferroelectrics-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('lukyanchuk-tikhonov-razumnaya-vinokur-hopfionsemergeinferroelectrics-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{lukyanchuk_hopfions_2020,\n\ttitle = {Hopfions emerge in ferroelectrics},\n\tvolume = {11},\n\tissn = {2041-1723},\n\turl = {https://www.nature.com/articles/s41467-020-16258-w},\n\tdoi = {10.1038/s41467-020-16258-w},\n\tabstract = {Abstract\n            Paradigmatic knotted solitons, Hopfions, that are characterized by topological Hopf invariant, attract an intense attention in the diverse areas of physics ranging from high-energy physics, cosmology and astrophysics to biology, magneto- and hydrodynamics and condensed matter physics. Yet, while being of broad interest, they remain elusive and under-explored. Here we demonstrate that Hopfions emerge as a basic configuration of polarization field in confined ferroelectric nanoparticles. Our findings establish that Hopfions are of fundamental importance for the electromagnetic behavior of the nanocomposits and can result in advanced functionalities of these materials.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Nature Communications},\n\tauthor = {Luk’yanchuk, I. and Tikhonov, Y. and Razumnaya, A. and Vinokur, V. M.},\n\tmonth = may,\n\tyear = {2020},\n\tpages = {2433},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\B5GV9UWB\\\\Luk’yanchuk и др. - 2020 - Hopfions emerge in ferroelectrics.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Abstract Paradigmatic knotted solitons, Hopfions, that are characterized by topological Hopf invariant, attract an intense attention in the diverse areas of physics ranging from high-energy physics, cosmology and astrophysics to biology, magneto- and hydrodynamics and condensed matter physics. Yet, while being of broad interest, they remain elusive and under-explored. Here we demonstrate that Hopfions emerge as a basic configuration of polarization field in confined ferroelectric nanoparticles. Our findings establish that Hopfions are of fundamental importance for the electromagnetic behavior of the nanocomposits and can result in advanced functionalities of these materials.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"anokhin-razumnaya-pavlenko-latticedynamicsofthestrontiumferrotungstateinthetemperaturerange300700k-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://link.springer.com/10.1134/S1063783420120033\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'anokhin-razumnaya-pavlenko-latticedynamicsofthestrontiumferrotungstateinthetemperaturerange300700k-2020', 'http://link.springer.com/10.1134/S1063783420120033', event);\">\n    Lattice Dynamics of the Strontium Ferrotungstate in the Temperature Range 300–700 K.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Anokhin, A. S.; Razumnaya, A. G.;  and Pavlenko, A. V.\n</span>\n\n  \n\n</span>\n\n  <i>Physics of the Solid State</i>, 62(12): 2434–2438. December 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://link.springer.com/10.1134/S1063783420120033\"\n     onclick=\"log_download('anokhin-razumnaya-pavlenko-latticedynamicsofthestrontiumferrotungstateinthetemperaturerange300700k-2020', 'http://link.springer.com/10.1134/S1063783420120033', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Lattice Dynamics of the Strontium Ferrotungstate in the Temperature Range 300–700 K [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1063783420120033\"\n     onclick=\"log_download('anokhin-razumnaya-pavlenko-latticedynamicsofthestrontiumferrotungstateinthetemperaturerange300700k-2020', 'http://doi.org/10.1134/S1063783420120033', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/anokhin-razumnaya-pavlenko-latticedynamicsofthestrontiumferrotungstateinthetemperaturerange300700k-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('anokhin-razumnaya-pavlenko-latticedynamicsofthestrontiumferrotungstateinthetemperaturerange300700k-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{anokhin_lattice_2020,\n\ttitle = {Lattice {Dynamics} of the {Strontium} {Ferrotungstate} in the {Temperature} {Range} 300–700 {K}},\n\tvolume = {62},\n\tissn = {1063-7834, 1090-6460},\n\turl = {http://link.springer.com/10.1134/S1063783420120033},\n\tdoi = {10.1134/S1063783420120033},\n\tlanguage = {en},\n\tnumber = {12},\n\turldate = {2023-11-11},\n\tjournal = {Physics of the Solid State},\n\tauthor = {Anokhin, A. S. and Razumnaya, A. G. and Pavlenko, A. V.},\n\tmonth = dec,\n\tyear = {2020},\n\tpages = {2434--2438},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kuriganova-leontyev-ulyankina-smirnova-electrochemicaldispersiontechniqueforthepreparationofsndopedptparticlesandtheiruseaselectrocatalysts-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0959943620302625\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kuriganova-leontyev-ulyankina-smirnova-electrochemicaldispersiontechniqueforthepreparationofsndopedptparticlesandtheiruseaselectrocatalysts-2020', 'https://linkinghub.elsevier.com/retrieve/pii/S0959943620302625', event);\">\n    Electrochemical dispersion technique for the preparation of Sn-doped Pt particles and their use as electrocatalysts.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kuriganova, A. B.; Leontyev, I. N.; Ulyankina, A. A.;  and Smirnova, N. V.\n</span>\n\n  \n\n</span>\n\n  <i>Mendeleev Communications</i>, 30(5): 663–665. September 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0959943620302625\"\n     onclick=\"log_download('kuriganova-leontyev-ulyankina-smirnova-electrochemicaldispersiontechniqueforthepreparationofsndopedptparticlesandtheiruseaselectrocatalysts-2020', 'https://linkinghub.elsevier.com/retrieve/pii/S0959943620302625', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Electrochemical dispersion technique for the preparation of Sn-doped Pt particles and their use as electrocatalysts [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.mencom.2020.09.037\"\n     onclick=\"log_download('kuriganova-leontyev-ulyankina-smirnova-electrochemicaldispersiontechniqueforthepreparationofsndopedptparticlesandtheiruseaselectrocatalysts-2020', 'http://doi.org/10.1016/j.mencom.2020.09.037', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kuriganova-leontyev-ulyankina-smirnova-electrochemicaldispersiontechniqueforthepreparationofsndopedptparticlesandtheiruseaselectrocatalysts-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kuriganova-leontyev-ulyankina-smirnova-electrochemicaldispersiontechniqueforthepreparationofsndopedptparticlesandtheiruseaselectrocatalysts-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kuriganova_electrochemical_2020,\n\ttitle = {Electrochemical dispersion technique for the preparation of {Sn}-doped {Pt} particles and their use as electrocatalysts},\n\tvolume = {30},\n\tissn = {09599436},\n\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0959943620302625},\n\tdoi = {10.1016/j.mencom.2020.09.037},\n\tlanguage = {en},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Mendeleev Communications},\n\tauthor = {Kuriganova, Alexandra B. and Leontyev, Igor N. and Ulyankina, Anna A. and Smirnova, Nina V.},\n\tmonth = sep,\n\tyear = {2020},\n\tpages = {663--665},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"payod-grassano-santos-levshov-pulci-saroka-2n4ruleandanatlasofbulkopticalresonancesofzigzaggraphenenanoribbons-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.nature.com/articles/s41467-019-13728-8\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'payod-grassano-santos-levshov-pulci-saroka-2n4ruleandanatlasofbulkopticalresonancesofzigzaggraphenenanoribbons-2020', 'https://www.nature.com/articles/s41467-019-13728-8', event);\">\n    2N+4-rule and an atlas of bulk optical resonances of zigzag graphene nanoribbons.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Payod, R. B.; Grassano, D.; Santos, G. N. C.; Levshov, D. I.; Pulci, O.;  and Saroka, V. A.\n</span>\n\n  \n\n</span>\n\n  <i>Nature Communications</i>, 11(1): 82. January 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.nature.com/articles/s41467-019-13728-8\"\n     onclick=\"log_download('payod-grassano-santos-levshov-pulci-saroka-2n4ruleandanatlasofbulkopticalresonancesofzigzaggraphenenanoribbons-2020', 'https://www.nature.com/articles/s41467-019-13728-8', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"2N+4-rule and an atlas of bulk optical resonances of zigzag graphene nanoribbons [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1038/s41467-019-13728-8\"\n     onclick=\"log_download('payod-grassano-santos-levshov-pulci-saroka-2n4ruleandanatlasofbulkopticalresonancesofzigzaggraphenenanoribbons-2020', 'http://doi.org/10.1038/s41467-019-13728-8', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/payod-grassano-santos-levshov-pulci-saroka-2n4ruleandanatlasofbulkopticalresonancesofzigzaggraphenenanoribbons-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('payod-grassano-santos-levshov-pulci-saroka-2n4ruleandanatlasofbulkopticalresonancesofzigzaggraphenenanoribbons-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{payod_2n4-rule_2020,\n\ttitle = {{2N}+4-rule and an atlas of bulk optical resonances of zigzag graphene nanoribbons},\n\tvolume = {11},\n\tissn = {2041-1723},\n\turl = {https://www.nature.com/articles/s41467-019-13728-8},\n\tdoi = {10.1038/s41467-019-13728-8},\n\tabstract = {Abstract\n            \n              Development of on-chip integrated carbon-based optoelectronic nanocircuits requires fast and non-invasive structural characterization of their building blocks. Recent advances in synthesis of single wall carbon nanotubes and graphene nanoribbons allow for their use as atomically precise building blocks. However, while cataloged experimental data are available for the structural characterization of carbon nanotubes, such an atlas is absent for graphene nanoribbons. Here we theoretically investigate the optical absorption resonances of armchair carbon nanotubes and zigzag graphene nanoribbons continuously spanning the tube (ribbon) transverse sizes from 0.5(0.4) nm to 8.1(12.8) nm. We show that the linear mapping is guaranteed between the tube and ribbon bulk resonance when the number of atoms in the tube unit cell is\n              \n                \n                  \\$\\$2N+4\\$\\$\n                  \n                    2\n                    N\n                    +\n                    4\n                  \n                \n              \n              , where\n              \n                \n                  \\$\\$N\\$\\$\n                  \n                    N\n                  \n                \n              \n              is the number of atoms in the ribbon unit cell. Thus, an atlas of carbon nanotubes optical transitions can be mapped to an atlas of zigzag graphene nanoribbons.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-10},\n\tjournal = {Nature Communications},\n\tauthor = {Payod, Renebeth B. and Grassano, Davide and Santos, Gil Nonato C. and Levshov, Dmitry I. and Pulci, Olivia and Saroka, Vasil A.},\n\tmonth = jan,\n\tyear = {2020},\n\tpages = {82},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\GVJGZB4S\\\\Payod и др. - 2020 - 2N+4-rule and an atlas of bulk optical resonances .pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Abstract Development of on-chip integrated carbon-based optoelectronic nanocircuits requires fast and non-invasive structural characterization of their building blocks. Recent advances in synthesis of single wall carbon nanotubes and graphene nanoribbons allow for their use as atomically precise building blocks. However, while cataloged experimental data are available for the structural characterization of carbon nanotubes, such an atlas is absent for graphene nanoribbons. Here we theoretically investigate the optical absorption resonances of armchair carbon nanotubes and zigzag graphene nanoribbons continuously spanning the tube (ribbon) transverse sizes from 0.5(0.4) nm to 8.1(12.8) nm. We show that the linear mapping is guaranteed between the tube and ribbon bulk resonance when the number of atoms in the tube unit cell is $$2N+4$$ 2 N + 4 , where $$N$$ N is the number of atoms in the ribbon unit cell. Thus, an atlas of carbon nanotubes optical transitions can be mapped to an atlas of zigzag graphene nanoribbons.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-timoshenko-pankin-razumnaya-tunableelectromechanicalpropertiesofabariumstrontiumtitanateferroelectricfilmunderauniaxialstress-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://ieeexplore.ieee.org/document/9146729/\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-timoshenko-pankin-razumnaya-tunableelectromechanicalpropertiesofabariumstrontiumtitanateferroelectricfilmunderauniaxialstress-2020', 'https://ieeexplore.ieee.org/document/9146729/', event);\">\n    Tunable Electromechanical Properties of a Barium Strontium Titanate Ferroelectric Film Under a Uniaxial Stress.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.; Timoshenko, P. E.; Pan'kin, A. V.;  and Razumnaya, A. G.\n</span>\n\n  \n\n</span>\n\n  <i>IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control</i>, 67(12): 2704–2709. December 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://ieeexplore.ieee.org/document/9146729/\"\n     onclick=\"log_download('shirokov-timoshenko-pankin-razumnaya-tunableelectromechanicalpropertiesofabariumstrontiumtitanateferroelectricfilmunderauniaxialstress-2020', 'https://ieeexplore.ieee.org/document/9146729/', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Tunable Electromechanical Properties of a Barium Strontium Titanate Ferroelectric Film Under a Uniaxial Stress [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1109/TUFFC.2020.3011591\"\n     onclick=\"log_download('shirokov-timoshenko-pankin-razumnaya-tunableelectromechanicalpropertiesofabariumstrontiumtitanateferroelectricfilmunderauniaxialstress-2020', 'http://doi.org/10.1109/TUFFC.2020.3011591', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-timoshenko-pankin-razumnaya-tunableelectromechanicalpropertiesofabariumstrontiumtitanateferroelectricfilmunderauniaxialstress-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-timoshenko-pankin-razumnaya-tunableelectromechanicalpropertiesofabariumstrontiumtitanateferroelectricfilmunderauniaxialstress-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_tunable_2020,\n\ttitle = {Tunable {Electromechanical} {Properties} of a {Barium} {Strontium} {Titanate} {Ferroelectric} {Film} {Under} a {Uniaxial} {Stress}},\n\tvolume = {67},\n\tissn = {0885-3010, 1525-8955},\n\turl = {https://ieeexplore.ieee.org/document/9146729/},\n\tdoi = {10.1109/TUFFC.2020.3011591},\n\tnumber = {12},\n\turldate = {2023-11-11},\n\tjournal = {IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control},\n\tauthor = {Shirokov, Vladimir Borisovich and Timoshenko, Pavel Evgenjevich and Pan&#x27;kin, Artyom Vital&#x27;yevich and Razumnaya, Anna Grigoryevna},\n\tmonth = dec,\n\tyear = {2020},\n\tpages = {2704--2709},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"hanani-mezzane-amjoud-gagou-hoummada-perrin-razumnaya-kutnjak-etal-structuraldielectricandferroelectricpropertiesofleadfreebcztceramicselaboratedbylowtemperaturehydrothermalprocessing-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.springer.com/10.1007/s10854-020-03555-9\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'hanani-mezzane-amjoud-gagou-hoummada-perrin-razumnaya-kutnjak-etal-structuraldielectricandferroelectricpropertiesofleadfreebcztceramicselaboratedbylowtemperaturehydrothermalprocessing-2020', 'https://link.springer.com/10.1007/s10854-020-03555-9', event);\">\n    Structural, dielectric, and ferroelectric properties of lead-free BCZT ceramics elaborated by low-temperature hydrothermal processing.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Hanani, Z.; Mezzane, D.; Amjoud, M.; Gagou, Y.; Hoummada, K.; Perrin, C.; Razumnaya, A. G.; Kutnjak, Z.; Bouzina, A.; Marssi, M. E.; Gouné, M.;  and Rožič, B.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Materials Science: Materials in Electronics</i>, 31(13): 10096–10104. July 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.springer.com/10.1007/s10854-020-03555-9\"\n     onclick=\"log_download('hanani-mezzane-amjoud-gagou-hoummada-perrin-razumnaya-kutnjak-etal-structuraldielectricandferroelectricpropertiesofleadfreebcztceramicselaboratedbylowtemperaturehydrothermalprocessing-2020', 'https://link.springer.com/10.1007/s10854-020-03555-9', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Structural, dielectric, and ferroelectric properties of lead-free BCZT ceramics elaborated by low-temperature hydrothermal processing [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1007/s10854-020-03555-9\"\n     onclick=\"log_download('hanani-mezzane-amjoud-gagou-hoummada-perrin-razumnaya-kutnjak-etal-structuraldielectricandferroelectricpropertiesofleadfreebcztceramicselaboratedbylowtemperaturehydrothermalprocessing-2020', 'http://doi.org/10.1007/s10854-020-03555-9', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/hanani-mezzane-amjoud-gagou-hoummada-perrin-razumnaya-kutnjak-etal-structuraldielectricandferroelectricpropertiesofleadfreebcztceramicselaboratedbylowtemperaturehydrothermalprocessing-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('hanani-mezzane-amjoud-gagou-hoummada-perrin-razumnaya-kutnjak-etal-structuraldielectricandferroelectricpropertiesofleadfreebcztceramicselaboratedbylowtemperaturehydrothermalprocessing-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{hanani_structural_2020,\n\ttitle = {Structural, dielectric, and ferroelectric properties of lead-free {BCZT} ceramics elaborated by low-temperature hydrothermal processing},\n\tvolume = {31},\n\tissn = {0957-4522, 1573-482X},\n\turl = {https://link.springer.com/10.1007/s10854-020-03555-9},\n\tdoi = {10.1007/s10854-020-03555-9},\n\tlanguage = {en},\n\tnumber = {13},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Materials Science: Materials in Electronics},\n\tauthor = {Hanani, Zouhair and Mezzane, Daoud and Amjoud, M’barek and Gagou, Yaovi and Hoummada, Khalid and Perrin, Carine and Razumnaya, Anna G. and Kutnjak, Zdravko and Bouzina, Adnane and Marssi, Mimoun El and Gouné, Mohamed and Rožič, Brigita},\n\tmonth = jul,\n\tyear = {2020},\n\tpages = {10096--10104},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\ZEME2MZQ\\\\Hanani и др. - 2020 - Structural, dielectric, and ferroelectric properti.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"hanani-merselmiz-danine-stein-mezzane-amjoud-lahcini-gagou-etal-enhanceddielectricandelectrocaloricpropertiesinleadfreerodlikebcztceramics-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://link.springer.com/10.1007/s40145-020-0361-1\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'hanani-merselmiz-danine-stein-mezzane-amjoud-lahcini-gagou-etal-enhanceddielectricandelectrocaloricpropertiesinleadfreerodlikebcztceramics-2020', 'http://link.springer.com/10.1007/s40145-020-0361-1', event);\">\n    Enhanced dielectric and electrocaloric properties in lead-free rod-like BCZT ceramics.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Hanani, Z.; Merselmiz, S.; Danine, A.; Stein, N.; Mezzane, D.; Amjoud, M.; Lahcini, M.; Gagou, Y.; Spreitzer, M.; Vengust, D.; Kutnjak, Z.; El Marssi, M.; Luk’yanchuk, I. A.;  and Gouné, M.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Advanced Ceramics</i>, 9(2): 210–219. April 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://link.springer.com/10.1007/s40145-020-0361-1\"\n     onclick=\"log_download('hanani-merselmiz-danine-stein-mezzane-amjoud-lahcini-gagou-etal-enhanceddielectricandelectrocaloricpropertiesinleadfreerodlikebcztceramics-2020', 'http://link.springer.com/10.1007/s40145-020-0361-1', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Enhanced dielectric and electrocaloric properties in lead-free rod-like BCZT ceramics [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1007/s40145-020-0361-1\"\n     onclick=\"log_download('hanani-merselmiz-danine-stein-mezzane-amjoud-lahcini-gagou-etal-enhanceddielectricandelectrocaloricpropertiesinleadfreerodlikebcztceramics-2020', 'http://doi.org/10.1007/s40145-020-0361-1', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/hanani-merselmiz-danine-stein-mezzane-amjoud-lahcini-gagou-etal-enhanceddielectricandelectrocaloricpropertiesinleadfreerodlikebcztceramics-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('hanani-merselmiz-danine-stein-mezzane-amjoud-lahcini-gagou-etal-enhanceddielectricandelectrocaloricpropertiesinleadfreerodlikebcztceramics-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{hanani_enhanced_2020,\n\ttitle = {Enhanced dielectric and electrocaloric properties in lead-free rod-like {BCZT} ceramics},\n\tvolume = {9},\n\tissn = {2226-4108, 2227-8508},\n\turl = {http://link.springer.com/10.1007/s40145-020-0361-1},\n\tdoi = {10.1007/s40145-020-0361-1},\n\tabstract = {Abstract\n            \n              Ba\n              0.85\n              Ca\n              0.15\n              Zr\n              0.10\n              Ti\n              0.90\n              O\n              3\n              (BCZT) lead-free ceramics demonstrated excellent dielectric, ferroelectric, and piezoelectric properties at the morphotropic phase boundary (MPB). So far, to study the effect of morphological changes on dielectric and ferroelectric properties in lead-free BCZT ceramics, researchers have mostly focused on the influence of spherical grain shape change. In this study, BCZT ceramics with rod-like grains and aspect ratio of about 10 were synthesized by surfactant-assisted solvothermal route. X-ray diffraction (XRD) and selected area electron diffraction (SAED) performed at room temperature confirm the crystallization of pure perovskite with tetragonal symmetry. Scanning electron microscopy (SEM) image showed that BCZT ceramics have kept the 1D rod-like grains with an average aspect ratio of about 4. Rod-like BCZT ceramics exhibit enhanced dielectric ferroelectric (ɛ\n              r\n              = 11,906, tanδ = 0.014,\n              P\n              r\n              = 6.01 μgC/cm\n              2\n              , and\n              E\n              c\n              = 2.46 kV/cm), and electrocaloric properties (Δ\n              T\n              = 0.492 K and gZ = 0.289 (K·mm)/kV at 17 kV/cm) with respect to spherical BCZT ceramics. Therefore, rod-like BCZT lead-free ceramics have good potential to be used in solid-state refrigeration technology.},\n\tlanguage = {en},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Advanced Ceramics},\n\tauthor = {Hanani, Zouhair and Merselmiz, Soukaina and Danine, Abdelaadim and Stein, Nicolas and Mezzane, Daoud and Amjoud, M’barek and Lahcini, Mohammed and Gagou, Yaovi and Spreitzer, Matjaz and Vengust, Damjan and Kutnjak, Zdravko and El Marssi, Mimoun and Luk’yanchuk, Igor A. and Gouné, Mohamed},\n\tmonth = apr,\n\tyear = {2020},\n\tpages = {210--219},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\PIFXGEQ5\\\\Hanani и др. - 2020 - Enhanced dielectric and electrocaloric properties .pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Abstract Ba 0.85 Ca 0.15 Zr 0.10 Ti 0.90 O 3 (BCZT) lead-free ceramics demonstrated excellent dielectric, ferroelectric, and piezoelectric properties at the morphotropic phase boundary (MPB). So far, to study the effect of morphological changes on dielectric and ferroelectric properties in lead-free BCZT ceramics, researchers have mostly focused on the influence of spherical grain shape change. In this study, BCZT ceramics with rod-like grains and aspect ratio of about 10 were synthesized by surfactant-assisted solvothermal route. X-ray diffraction (XRD) and selected area electron diffraction (SAED) performed at room temperature confirm the crystallization of pure perovskite with tetragonal symmetry. Scanning electron microscopy (SEM) image showed that BCZT ceramics have kept the 1D rod-like grains with an average aspect ratio of about 4. Rod-like BCZT ceramics exhibit enhanced dielectric ferroelectric (ɛ r = 11,906, tanδ = 0.014, P r = 6.01 μgC/cm 2 , and E c = 2.46 kV/cm), and electrocaloric properties (Δ T = 0.492 K and gZ = 0.289 (K·mm)/kV at 17 kV/cm) with respect to spherical BCZT ceramics. Therefore, rod-like BCZT lead-free ceramics have good potential to be used in solid-state refrigeration technology.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"alyabyeva-yegiyan-torgashev-prokhorov-vinnik-gudkova-zherebtsov-dressel-etal-terahertzinfraredspectroscopyofti4dopedmtypebariumhexaferrite-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0925838819346444\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'alyabyeva-yegiyan-torgashev-prokhorov-vinnik-gudkova-zherebtsov-dressel-etal-terahertzinfraredspectroscopyofti4dopedmtypebariumhexaferrite-2020', 'https://linkinghub.elsevier.com/retrieve/pii/S0925838819346444', event);\">\n    Terahertz-infrared spectroscopy of Ti4+-doped M-type barium hexaferrite.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Alyabyeva, L.; Yegiyan, S.; Torgashev, V.; Prokhorov, A. S.; Vinnik, D.; Gudkova, S.; Zherebtsov, D.; Dressel, M.;  and Gorshunov, B.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Alloys and Compounds</i>, 820: 153398. April 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0925838819346444\"\n     onclick=\"log_download('alyabyeva-yegiyan-torgashev-prokhorov-vinnik-gudkova-zherebtsov-dressel-etal-terahertzinfraredspectroscopyofti4dopedmtypebariumhexaferrite-2020', 'https://linkinghub.elsevier.com/retrieve/pii/S0925838819346444', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Terahertz-infrared spectroscopy of Ti4+-doped M-type barium hexaferrite [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.jallcom.2019.153398\"\n     onclick=\"log_download('alyabyeva-yegiyan-torgashev-prokhorov-vinnik-gudkova-zherebtsov-dressel-etal-terahertzinfraredspectroscopyofti4dopedmtypebariumhexaferrite-2020', 'http://doi.org/10.1016/j.jallcom.2019.153398', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/alyabyeva-yegiyan-torgashev-prokhorov-vinnik-gudkova-zherebtsov-dressel-etal-terahertzinfraredspectroscopyofti4dopedmtypebariumhexaferrite-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('alyabyeva-yegiyan-torgashev-prokhorov-vinnik-gudkova-zherebtsov-dressel-etal-terahertzinfraredspectroscopyofti4dopedmtypebariumhexaferrite-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{alyabyeva_terahertz-infrared_2020,\n\ttitle = {Terahertz-infrared spectroscopy of {Ti4}+-doped {M}-type barium hexaferrite},\n\tvolume = {820},\n\tissn = {09258388},\n\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0925838819346444},\n\tdoi = {10.1016/j.jallcom.2019.153398},\n\tlanguage = {en},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Alloys and Compounds},\n\tauthor = {Alyabyeva, Liudmila and Yegiyan, Samvel and Torgashev, Victor and Prokhorov, Anatoly S. and Vinnik, Denis and Gudkova, Svetlana and Zherebtsov, Dmitry and Dressel, Martin and Gorshunov, Boris},\n\tmonth = apr,\n\tyear = {2020},\n\tpages = {153398},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"hanani-merselmiz-mezzane-amjoud-bradeko-roi-lahcini-elmarssi-etal-thermallystablehighenergystorageperformancesandlargeelectrocaloriceffectoverabroadtemperaturespaninleadfreebcztceramic-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://xlink.rsc.org/?DOI=D0RA06116F\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'hanani-merselmiz-mezzane-amjoud-bradeko-roi-lahcini-elmarssi-etal-thermallystablehighenergystorageperformancesandlargeelectrocaloriceffectoverabroadtemperaturespaninleadfreebcztceramic-2020', 'http://xlink.rsc.org/?DOI=D0RA06116F', event);\">\n    Thermally-stable high energy storage performances and large electrocaloric effect over a broad temperature span in lead-free BCZT ceramic.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Hanani, Z.; Merselmiz, S.; Mezzane, D.; Amjoud, M.; Bradeško, A.; Rožič, B.; Lahcini, M.; El Marssi, M.; Ragulya, A. V.; Luk'yanchuk, I. A.; Kutnjak, Z.;  and Gouné, M.\n</span>\n\n  \n\n</span>\n\n  <i>RSC Advances</i>, 10(51): 30746–30755.  2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://xlink.rsc.org/?DOI=D0RA06116F\"\n     onclick=\"log_download('hanani-merselmiz-mezzane-amjoud-bradeko-roi-lahcini-elmarssi-etal-thermallystablehighenergystorageperformancesandlargeelectrocaloriceffectoverabroadtemperaturespaninleadfreebcztceramic-2020', 'http://xlink.rsc.org/?DOI=D0RA06116F', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Thermally-stable high energy storage performances and large electrocaloric effect over a broad temperature span in lead-free BCZT ceramic [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1039/D0RA06116F\"\n     onclick=\"log_download('hanani-merselmiz-mezzane-amjoud-bradeko-roi-lahcini-elmarssi-etal-thermallystablehighenergystorageperformancesandlargeelectrocaloriceffectoverabroadtemperaturespaninleadfreebcztceramic-2020', 'http://doi.org/10.1039/D0RA06116F', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/hanani-merselmiz-mezzane-amjoud-bradeko-roi-lahcini-elmarssi-etal-thermallystablehighenergystorageperformancesandlargeelectrocaloriceffectoverabroadtemperaturespaninleadfreebcztceramic-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('hanani-merselmiz-mezzane-amjoud-bradeko-roi-lahcini-elmarssi-etal-thermallystablehighenergystorageperformancesandlargeelectrocaloriceffectoverabroadtemperaturespaninleadfreebcztceramic-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{hanani_thermally-stable_2020,\n\ttitle = {Thermally-stable high energy storage performances and large electrocaloric effect over a broad temperature span in lead-free {BCZT} ceramic},\n\tvolume = {10},\n\tissn = {2046-2069},\n\turl = {http://xlink.rsc.org/?DOI=D0RA06116F},\n\tdoi = {10.1039/D0RA06116F},\n\tabstract = {Thermally-stable recovered energy density and significant electrocaloric temperature change over a broad temperature span in BCZT ceramic elaborated by low-temperature hydrothermal processing.\n          , \n            \n              Ba\n              0.85\n              Ca\n              0.15\n              Zr\n              0.10\n              Ti\n              0.90\n              O\n              3\n              (BCZT) relaxor ferroelectric ceramics exhibit enhanced energy storage and electrocaloric performances due to their excellent dielectric and ferroelectric properties. In this study, the temperature-dependence of the structural and dielectric properties, as well as the field and temperature-dependence of the energy storage and the electrocaloric properties in BCZT ceramics elaborated at low-temperature hydrothermal processing are investigated. X-ray diffraction and Raman spectroscopy results confirmed the ferroelectric–paraelectric phase transition in the BCZT ceramic. At room temperature and 1 kHz, the dielectric constant and dielectric loss reached 5000 and 0.029, respectively. The BCZT ceramic showed a large recovered energy density (\n              W\n              rec\n              ) of 414.1 mJ cm\n              −3\n              at 380 K, with an energy efficiency of 78.6\\%, and high thermal-stability of\n              W\n              rec\n              of 3.9\\% in the temperature range of 340–400 K. The electrocaloric effect in BCZT was explored\n              via\n              an indirect approach following the Maxwell relation at 60 kV cm\n              −1\n              . The significant electrocaloric temperature change of 1.479 K at 367 K, a broad temperature span of 87 K, an enhanced refrigerant capacity of 140.33 J kg\n              −1\n              , and a high coefficient of performance of 6.12 obtained at 60 kV cm\n              −1\n              make BCZT ceramics potentially useful coolant materials in the development of future eco-friendly solid-state refrigeration technology.},\n\tlanguage = {en},\n\tnumber = {51},\n\turldate = {2023-11-11},\n\tjournal = {RSC Advances},\n\tauthor = {Hanani, Zouhair and Merselmiz, Soukaina and Mezzane, Daoud and Amjoud, M&#x27;barek and Bradeško, Andraž and Rožič, Brigita and Lahcini, Mohammed and El Marssi, Mimoun and Ragulya, Andrey V. and Luk&#x27;yanchuk, Igor A. and Kutnjak, Zdravko and Gouné, Mohamed},\n\tyear = {2020},\n\tpages = {30746--30755},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\3987HKNB\\\\Hanani и др. - 2020 - Thermally-stable high energy storage performances .pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Thermally-stable recovered energy density and significant electrocaloric temperature change over a broad temperature span in BCZT ceramic elaborated by low-temperature hydrothermal processing. , Ba 0.85 Ca 0.15 Zr 0.10 Ti 0.90 O 3 (BCZT) relaxor ferroelectric ceramics exhibit enhanced energy storage and electrocaloric performances due to their excellent dielectric and ferroelectric properties. In this study, the temperature-dependence of the structural and dielectric properties, as well as the field and temperature-dependence of the energy storage and the electrocaloric properties in BCZT ceramics elaborated at low-temperature hydrothermal processing are investigated. X-ray diffraction and Raman spectroscopy results confirmed the ferroelectric–paraelectric phase transition in the BCZT ceramic. At room temperature and 1 kHz, the dielectric constant and dielectric loss reached 5000 and 0.029, respectively. The BCZT ceramic showed a large recovered energy density ( W rec ) of 414.1 mJ cm −3 at 380 K, with an energy efficiency of 78.6%, and high thermal-stability of W rec of 3.9% in the temperature range of 340–400 K. The electrocaloric effect in BCZT was explored via an indirect approach following the Maxwell relation at 60 kV cm −1 . The significant electrocaloric temperature change of 1.479 K at 367 K, a broad temperature span of 87 K, an enhanced refrigerant capacity of 140.33 J kg −1 , and a high coefficient of performance of 6.12 obtained at 60 kV cm −1 make BCZT ceramics potentially useful coolant materials in the development of future eco-friendly solid-state refrigeration technology.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"timoshenko-shirokov-kalinchuk-finiteelementmodelingofsawfiltersbasedonthinfilmsofbariumstrontiumtitanate-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/doi_resolution.asp?doi=10%2E31429%2Fvestnik%2D17%2D4%2D48%2D56\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'timoshenko-shirokov-kalinchuk-finiteelementmodelingofsawfiltersbasedonthinfilmsofbariumstrontiumtitanate-2020', 'https://elibrary.ru/doi_resolution.asp?doi=10%2E31429%2Fvestnik%2D17%2D4%2D48%2D56', event);\">\n    Finite-element Modeling of SAW-filters Based on Thin Films of Barium Strontium Titanate.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Timoshenko, P.; Shirokov, V.;  and Kalinchuk, V.\n</span>\n\n  \n\n</span>\n\n  <i>Ecological Bulletin of Research Centers of the Black Sea Economic Cooperation</i>, 17(4): 48–56.  2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/doi_resolution.asp?doi=10%2E31429%2Fvestnik%2D17%2D4%2D48%2D56\"\n     onclick=\"log_download('timoshenko-shirokov-kalinchuk-finiteelementmodelingofsawfiltersbasedonthinfilmsofbariumstrontiumtitanate-2020', 'https://elibrary.ru/doi_resolution.asp?doi=10%2E31429%2Fvestnik%2D17%2D4%2D48%2D56', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Finite-element Modeling of SAW-filters Based on Thin Films of Barium Strontium Titanate [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.31429/vestnik-17-4-48-56\"\n     onclick=\"log_download('timoshenko-shirokov-kalinchuk-finiteelementmodelingofsawfiltersbasedonthinfilmsofbariumstrontiumtitanate-2020', 'http://doi.org/10.31429/vestnik-17-4-48-56', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/timoshenko-shirokov-kalinchuk-finiteelementmodelingofsawfiltersbasedonthinfilmsofbariumstrontiumtitanate-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('timoshenko-shirokov-kalinchuk-finiteelementmodelingofsawfiltersbasedonthinfilmsofbariumstrontiumtitanate-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{timoshenko_finite-element_2020,\n\ttitle = {Finite-element {Modeling} of {SAW}-filters {Based} on {Thin} {Films} of {Barium} {Strontium} {Titanate}},\n\tvolume = {17},\n\tissn = {1729-5459},\n\turl = {https://elibrary.ru/doi_resolution.asp?doi=10%2E31429%2Fvestnik%2D17%2D4%2D48%2D56},\n\tdoi = {10.31429/vestnik-17-4-48-56},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Ecological Bulletin of Research Centers of the Black Sea Economic Cooperation},\n\tauthor = {Timoshenko, P.E. and Shirokov, V.B. and Kalinchuk, V.V.},\n\tyear = {2020},\n\tpages = {48--56},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"konevtsova-roshal-podgornik-rochal-irreversibleandreversiblemorphologicalchangesintheii6capsidandsimilarviralshellssymmetryandmicromechanics-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://xlink.rsc.org/?DOI=D0SM01338B\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'konevtsova-roshal-podgornik-rochal-irreversibleandreversiblemorphologicalchangesintheii6capsidandsimilarviralshellssymmetryandmicromechanics-2020', 'http://xlink.rsc.org/?DOI=D0SM01338B', event);\">\n    Irreversible and reversible morphological changes in the <i>ϕ</i> 6 capsid and similar viral shells: symmetry and micromechanics.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Konevtsova, O. V.; Roshal, D. S.; Podgornik, R.;  and Rochal, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Soft Matter</i>, 16(40): 9383–9392.  2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://xlink.rsc.org/?DOI=D0SM01338B\"\n     onclick=\"log_download('konevtsova-roshal-podgornik-rochal-irreversibleandreversiblemorphologicalchangesintheii6capsidandsimilarviralshellssymmetryandmicromechanics-2020', 'http://xlink.rsc.org/?DOI=D0SM01338B', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Irreversible and reversible morphological changes in the &lt;i&gt;ϕ&lt;/i&gt; 6 capsid and similar viral shells: symmetry and micromechanics [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1039/D0SM01338B\"\n     onclick=\"log_download('konevtsova-roshal-podgornik-rochal-irreversibleandreversiblemorphologicalchangesintheii6capsidandsimilarviralshellssymmetryandmicromechanics-2020', 'http://doi.org/10.1039/D0SM01338B', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/konevtsova-roshal-podgornik-rochal-irreversibleandreversiblemorphologicalchangesintheii6capsidandsimilarviralshellssymmetryandmicromechanics-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('konevtsova-roshal-podgornik-rochal-irreversibleandreversiblemorphologicalchangesintheii6capsidandsimilarviralshellssymmetryandmicromechanics-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{konevtsova_irreversible_2020,\n\ttitle = {Irreversible and reversible morphological changes in the \\textit{ϕ} 6 capsid and similar viral shells: symmetry and micromechanics},\n\tvolume = {16},\n\tissn = {1744-683X, 1744-6848},\n\tshorttitle = {Irreversible and reversible morphological changes in the \\textit{ϕ} 6 capsid and similar viral shells},\n\turl = {http://xlink.rsc.org/?DOI=D0SM01338B},\n\tdoi = {10.1039/D0SM01338B},\n\tabstract = {We propose a new micromechanical model perfectly describing the capsid shapes and morphological transformations that occur between the states of the dodecahedral\n              ϕ\n              6 capsid and similar viral shells due to the sequential packaging of RNA segments.\n            \n          , \n            \n              Understanding the physicochemical processes occurring in viruses during their maturation is of fundamental importance since only mature viruses can infect host cells. Here we consider the irreversible and reversible morphological changes that occur with the dodecahedral\n              ϕ\n              6 procapsid during the sequential packaging of 3 RNA segments forming the viral genome. It is shown that the dodecahedral shape of all the four observed capsid states is perfectly reproduced by a sphere radially deformed by only two irreducible spherical harmonics with icosahedral symmetry and wave numbers\n              l\n              = 6 and\n              l\n              = 10. The rotation of proteins around the 3-fold axes at the Procapsid → Intermediate 1 irreversible transformation is in fact also well described with the shear field containing only two irreducible harmonics with the same two wave numbers. The high stability of the Intermediate 1 state is discussed and the shapes of the Intermediate 2 state and Capsid (reversibly transforming back to the Intermediate 1 state) are shown to be mainly due to the isotropic pressure that the encapsidated RNA segments exert on the shell walls. The hidden symmetry of the capsid and the physicochemical features of the\n              in vitro\n              genome extraction from the viral shell are also elucidated.},\n\tlanguage = {en},\n\tnumber = {40},\n\turldate = {2023-11-11},\n\tjournal = {Soft Matter},\n\tauthor = {Konevtsova, Olga V. and Roshal, Daria S. and Podgornik, Rudolf and Rochal, Sergei B.},\n\tyear = {2020},\n\tpages = {9383--9392},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We propose a new micromechanical model perfectly describing the capsid shapes and morphological transformations that occur between the states of the dodecahedral ϕ 6 capsid and similar viral shells due to the sequential packaging of RNA segments. , Understanding the physicochemical processes occurring in viruses during their maturation is of fundamental importance since only mature viruses can infect host cells. Here we consider the irreversible and reversible morphological changes that occur with the dodecahedral ϕ 6 procapsid during the sequential packaging of 3 RNA segments forming the viral genome. It is shown that the dodecahedral shape of all the four observed capsid states is perfectly reproduced by a sphere radially deformed by only two irreducible spherical harmonics with icosahedral symmetry and wave numbers l = 6 and l = 10. The rotation of proteins around the 3-fold axes at the Procapsid → Intermediate 1 irreversible transformation is in fact also well described with the shear field containing only two irreducible harmonics with the same two wave numbers. The high stability of the Intermediate 1 state is discussed and the shapes of the Intermediate 2 state and Capsid (reversibly transforming back to the Intermediate 1 state) are shown to be mainly due to the isotropic pressure that the encapsidated RNA segments exert on the shell walls. The hidden symmetry of the capsid and the physicochemical features of the in vitro genome extraction from the viral shell are also elucidated.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"konevtsova-roshal-dmitriev-rochal-carbonnanotubesortingduetocommensuratemolecularwrapping-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://xlink.rsc.org/?DOI=D0NR03236K\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'konevtsova-roshal-dmitriev-rochal-carbonnanotubesortingduetocommensuratemolecularwrapping-2020', 'http://xlink.rsc.org/?DOI=D0NR03236K', event);\">\n    Carbon nanotube sorting due to commensurate molecular wrapping.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Konevtsova, O. V.; Roshal, D. S.; Dmitriev, V. P.;  and Rochal, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Nanoscale</i>, 12(29): 15725–15735.  2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://xlink.rsc.org/?DOI=D0NR03236K\"\n     onclick=\"log_download('konevtsova-roshal-dmitriev-rochal-carbonnanotubesortingduetocommensuratemolecularwrapping-2020', 'http://xlink.rsc.org/?DOI=D0NR03236K', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Carbon nanotube sorting due to commensurate molecular wrapping [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1039/D0NR03236K\"\n     onclick=\"log_download('konevtsova-roshal-dmitriev-rochal-carbonnanotubesortingduetocommensuratemolecularwrapping-2020', 'http://doi.org/10.1039/D0NR03236K', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/konevtsova-roshal-dmitriev-rochal-carbonnanotubesortingduetocommensuratemolecularwrapping-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('konevtsova-roshal-dmitriev-rochal-carbonnanotubesortingduetocommensuratemolecularwrapping-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{konevtsova_carbon_2020,\n\ttitle = {Carbon nanotube sorting due to commensurate molecular wrapping},\n\tvolume = {12},\n\tissn = {2040-3364, 2040-3372},\n\turl = {http://xlink.rsc.org/?DOI=D0NR03236K},\n\tdoi = {10.1039/D0NR03236K},\n\tabstract = {Commensurate wrapping of carbon nanotubes ensures their selection by flavin group molecules.\n          , \n            Single-walled carbon nanotubes (SWCNTs) can be sorted by their structural parameters using organic molecules and polymers: some of which, demonstrating a profound affinity only for specific nanotubes, form dense coatings on them. Here, analyzing well-known examples of flavin group molecules and those of 2,4-dichlorophenoxyacetic acid, we show for the first time that successful formation of the considered coatings depends on the ability of molecules to wrap around the SWCNT in a commensurate way. Commensurability provides a decrease in the free energy of the resulting bilayer system and makes the coating much more stable. Concurrently, it strongly relates the nanotube chiral vector with the geometric characteristics of the adhering molecules, which leads to revealed selection rules. If they are not satisfied, the deposition of molecules does not occur or is insignificant. The proposed theory unambiguously explains known experimental results on the formation of spiral wrappings of SWCNTs by flavin group molecules and points out other organic molecules and polymers suitable for effective CNT sorting.},\n\tlanguage = {en},\n\tnumber = {29},\n\turldate = {2023-11-11},\n\tjournal = {Nanoscale},\n\tauthor = {Konevtsova, Olga V. and Roshal, Daria S. and Dmitriev, Vladimir P. and Rochal, Sergei B.},\n\tyear = {2020},\n\tpages = {15725--15735},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Commensurate wrapping of carbon nanotubes ensures their selection by flavin group molecules. , Single-walled carbon nanotubes (SWCNTs) can be sorted by their structural parameters using organic molecules and polymers: some of which, demonstrating a profound affinity only for specific nanotubes, form dense coatings on them. Here, analyzing well-known examples of flavin group molecules and those of 2,4-dichlorophenoxyacetic acid, we show for the first time that successful formation of the considered coatings depends on the ability of molecules to wrap around the SWCNT in a commensurate way. Commensurability provides a decrease in the free energy of the resulting bilayer system and makes the coating much more stable. Concurrently, it strongly relates the nanotube chiral vector with the geometric characteristics of the adhering molecules, which leads to revealed selection rules. If they are not satisfied, the deposition of molecules does not occur or is insignificant. The proposed theory unambiguously explains known experimental results on the formation of spiral wrappings of SWCNTs by flavin group molecules and points out other organic molecules and polymers suitable for effective CNT sorting.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"poullet-golushko-lorman-travnickova-bureau-chalin-rochal-parmeggiani-etal-mechanicalinstabilitiesofaortadrivebloodstemcellproductionalivestudy-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1007/s00018-019-03372-2\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'poullet-golushko-lorman-travnickova-bureau-chalin-rochal-parmeggiani-etal-mechanicalinstabilitiesofaortadrivebloodstemcellproductionalivestudy-2020', 'https://doi.org/10.1007/s00018-019-03372-2', event);\">\n    Mechanical instabilities of aorta drive blood stem cell production: a live study.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Poullet, N.; Golushko, I.; Lorman, V.; Travnickova, J.; Bureau, C.; Chalin, D.; Rochal, S.; Parmeggiani, A.;  and Kissa, K.\n</span>\n\n  \n\n</span>\n\n  <i>Cellular and Molecular Life Sciences</i>, 77(17): 3453–3464. September 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1007/s00018-019-03372-2\"\n     onclick=\"log_download('poullet-golushko-lorman-travnickova-bureau-chalin-rochal-parmeggiani-etal-mechanicalinstabilitiesofaortadrivebloodstemcellproductionalivestudy-2020', 'https://doi.org/10.1007/s00018-019-03372-2', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Mechanical instabilities of aorta drive blood stem cell production: a live study [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1007/s00018-019-03372-2\"\n     onclick=\"log_download('poullet-golushko-lorman-travnickova-bureau-chalin-rochal-parmeggiani-etal-mechanicalinstabilitiesofaortadrivebloodstemcellproductionalivestudy-2020', 'http://doi.org/10.1007/s00018-019-03372-2', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/poullet-golushko-lorman-travnickova-bureau-chalin-rochal-parmeggiani-etal-mechanicalinstabilitiesofaortadrivebloodstemcellproductionalivestudy-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('poullet-golushko-lorman-travnickova-bureau-chalin-rochal-parmeggiani-etal-mechanicalinstabilitiesofaortadrivebloodstemcellproductionalivestudy-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{poullet_mechanical_2020,\n\ttitle = {Mechanical instabilities of aorta drive blood stem cell production: a live study},\n\tvolume = {77},\n\tissn = {1420-9071},\n\tshorttitle = {Mechanical instabilities of aorta drive blood stem cell production},\n\turl = {https://doi.org/10.1007/s00018-019-03372-2},\n\tdoi = {10.1007/s00018-019-03372-2},\n\tabstract = {During embryogenesis of all vertebrates, haematopoietic stem/progenitor cells (HSPCs) extrude from the aorta by a complex process named endothelial-to-haematopoietic transition (EHT). HSPCs will then colonize haematopoietic organs allowing haematopoiesis throughout adult life. The mechanism underlying EHT including the role of each aortic endothelial cell (EC) within the global aorta dynamics remains unknown. In the present study, we show for the first time that EHT involves the remodelling of individual cells within a collective migration of ECs which is tightly orchestrated, resulting in HSPCs extrusion in the sub-aortic space without compromising aorta integrity. By performing a cross-disciplinary study which combines high-resolution 4D imaging and theoretical analysis based on the concepts of classical mechanics, we propose that this complex developmental process is dependent on mechanical instabilities of the aorta preparing and facilitating the extrusion of HSPCs.},\n\tlanguage = {en},\n\tnumber = {17},\n\turldate = {2023-11-11},\n\tjournal = {Cellular and Molecular Life Sciences},\n\tauthor = {Poullet, Nausicaa and Golushko, Ivan and Lorman, Vladimir and Travnickova, Jana and Bureau, Charlotte and Chalin, Dmitrii and Rochal, Sergei and Parmeggiani, Andrea and Kissa, Karima},\n\tmonth = sep,\n\tyear = {2020},\n\tkeywords = {4D microscopy, Endothelial-to-haematopoietic transition, Haematopoiesis, Modeling, Zebrafish},\n\tpages = {3453--3464},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\8C4TEQZS\\\\Poullet и др. - 2020 - Mechanical instabilities of aorta drive blood stem.pdf:application/pdf;Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\6C7BISAS\\\\Poullet и др. - 2020 - Mechanical instabilities of aorta drive blood stem.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  During embryogenesis of all vertebrates, haematopoietic stem/progenitor cells (HSPCs) extrude from the aorta by a complex process named endothelial-to-haematopoietic transition (EHT). HSPCs will then colonize haematopoietic organs allowing haematopoiesis throughout adult life. The mechanism underlying EHT including the role of each aortic endothelial cell (EC) within the global aorta dynamics remains unknown. In the present study, we show for the first time that EHT involves the remodelling of individual cells within a collective migration of ECs which is tightly orchestrated, resulting in HSPCs extrusion in the sub-aortic space without compromising aorta integrity. By performing a cross-disciplinary study which combines high-resolution 4D imaging and theoretical analysis based on the concepts of classical mechanics, we propose that this complex developmental process is dependent on mechanical instabilities of the aorta preparing and facilitating the extrusion of HSPCs.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"weber-lebedinskaya-rudsky-kabirov-rudskaya-kupriyanov-structuralfeaturesoftheatextrm2tisitextrm2otextrm8iaibaandpbcompounds-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.worldscientific.com/doi/abs/10.1142/S2010135X20500228\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'weber-lebedinskaya-rudsky-kabirov-rudskaya-kupriyanov-structuralfeaturesoftheatextrm2tisitextrm2otextrm8iaibaandpbcompounds-2020', 'https://www.worldscientific.com/doi/abs/10.1142/S2010135X20500228', event);\">\n    Structural features of the A$_{\\textrm{2}}$TiSi$_{\\textrm{2}}$O$_{\\textrm{8}}$ ( <i>A</i> -Ba and Pb) compounds.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Weber, S.; Lebedinskaya, A.; Rudsky, D.; Kabirov, Y.; Rudskaya, A.;  and Kupriyanov, M.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Advanced Dielectrics</i>, 10(05): 2050022. October 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.worldscientific.com/doi/abs/10.1142/S2010135X20500228\"\n     onclick=\"log_download('weber-lebedinskaya-rudsky-kabirov-rudskaya-kupriyanov-structuralfeaturesoftheatextrm2tisitextrm2otextrm8iaibaandpbcompounds-2020', 'https://www.worldscientific.com/doi/abs/10.1142/S2010135X20500228', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Structural features of the A$_{\\textrm{2}}$TiSi$_{\\textrm{2}}$O$_{\\textrm{8}}$ ( &lt;i&gt;A&lt;/i&gt; -Ba and Pb) compounds [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1142/S2010135X20500228\"\n     onclick=\"log_download('weber-lebedinskaya-rudsky-kabirov-rudskaya-kupriyanov-structuralfeaturesoftheatextrm2tisitextrm2otextrm8iaibaandpbcompounds-2020', 'http://doi.org/10.1142/S2010135X20500228', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/weber-lebedinskaya-rudsky-kabirov-rudskaya-kupriyanov-structuralfeaturesoftheatextrm2tisitextrm2otextrm8iaibaandpbcompounds-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('weber-lebedinskaya-rudsky-kabirov-rudskaya-kupriyanov-structuralfeaturesoftheatextrm2tisitextrm2otextrm8iaibaandpbcompounds-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{weber_structural_2020,\n\ttitle = {Structural features of the {A}$_{\\textrm{2}}${TiSi}$_{\\textrm{2}}${O}$_{\\textrm{8}}$ ( \\textit{{A}} -{Ba} and {Pb}) compounds},\n\tvolume = {10},\n\tissn = {2010-135X, 2010-1368},\n\turl = {https://www.worldscientific.com/doi/abs/10.1142/S2010135X20500228},\n\tdoi = {10.1142/S2010135X20500228},\n\tabstract = {X-ray diffraction studies of synthesized Ba\n              2\n              TiSi\n              2\n              O\n              8\n              have shown that this compound has a fresnoite structure and is characterized by a polar phase [Formula: see text]4bm at room temperature. The synthesis of Pb\n              2\n              TiSi\n              2\n              O\n              8\n              in the fresnoite phase under the selected synthesis conditions has led to the formation of a perovskite tetragonal phase [Formula: see text]4mm corresponding to PbTiO\n              3\n              .},\n\tlanguage = {en},\n\tnumber = {05},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Advanced Dielectrics},\n\tauthor = {Weber, Svetlana and Lebedinskaya, Alla and Rudsky, Daniil and Kabirov, Yuri and Rudskaya, Anzhela and Kupriyanov, Michael},\n\tmonth = oct,\n\tyear = {2020},\n\tpages = {2050022},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\CQ956RAJ\\\\Weber и др. - 2020 - Structural features of the A2TiSi2O8 ( A -B.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  X-ray diffraction studies of synthesized Ba 2 TiSi 2 O 8 have shown that this compound has a fresnoite structure and is characterized by a polar phase [Formula: see text]4bm at room temperature. The synthesis of Pb 2 TiSi 2 O 8 in the fresnoite phase under the selected synthesis conditions has led to the formation of a perovskite tetragonal phase [Formula: see text]4mm corresponding to PbTiO 3 .\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-razumnaya-softmodesbehaviorinbilayerbasrtiotextrm3basrtiotextrm3heterostructures-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.tandfonline.com/doi/full/10.1080/00150193.2020.1791593\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-razumnaya-softmodesbehaviorinbilayerbasrtiotextrm3basrtiotextrm3heterostructures-2020', 'https://www.tandfonline.com/doi/full/10.1080/00150193.2020.1791593', event);\">\n    Soft modes behavior in bilayer (Ba,Sr)TiO$_{\\textrm{3}}$ /(Ba,Sr)TiO$_{\\textrm{3}}$ heterostructures.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.;  and Razumnaya, A. G.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 567(1): 102–112. October 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.tandfonline.com/doi/full/10.1080/00150193.2020.1791593\"\n     onclick=\"log_download('shirokov-razumnaya-softmodesbehaviorinbilayerbasrtiotextrm3basrtiotextrm3heterostructures-2020', 'https://www.tandfonline.com/doi/full/10.1080/00150193.2020.1791593', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Soft modes behavior in bilayer (Ba,Sr)TiO$_{\\textrm{3}}$ /(Ba,Sr)TiO$_{\\textrm{3}}$ heterostructures [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150193.2020.1791593\"\n     onclick=\"log_download('shirokov-razumnaya-softmodesbehaviorinbilayerbasrtiotextrm3basrtiotextrm3heterostructures-2020', 'http://doi.org/10.1080/00150193.2020.1791593', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-razumnaya-softmodesbehaviorinbilayerbasrtiotextrm3basrtiotextrm3heterostructures-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-razumnaya-softmodesbehaviorinbilayerbasrtiotextrm3basrtiotextrm3heterostructures-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_soft_2020,\n\ttitle = {Soft modes behavior in bilayer ({Ba},{Sr}){TiO}$_{\\textrm{3}}$ /({Ba},{Sr}){TiO}$_{\\textrm{3}}$ heterostructures},\n\tvolume = {567},\n\tissn = {0015-0193, 1563-5112},\n\turl = {https://www.tandfonline.com/doi/full/10.1080/00150193.2020.1791593},\n\tdoi = {10.1080/00150193.2020.1791593},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Ferroelectrics},\n\tauthor = {Shirokov, V. B. and Razumnaya, A. G.},\n\tmonth = oct,\n\tyear = {2020},\n\tpages = {102--112},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"merselmiz-hanani-mezzane-spreitzer-bradeko-fabijan-vengust-amjoud-etal-highenergystorageefficiencyandlargeelectrocaloriceffectinleadfreebatitextrm089sntextrm011otextrm3ceramic-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S027288422031823X\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'merselmiz-hanani-mezzane-spreitzer-bradeko-fabijan-vengust-amjoud-etal-highenergystorageefficiencyandlargeelectrocaloriceffectinleadfreebatitextrm089sntextrm011otextrm3ceramic-2020', 'https://linkinghub.elsevier.com/retrieve/pii/S027288422031823X', event);\">\n    High energy storage efficiency and large electrocaloric effect in lead-free BaTi$_{\\textrm{0.89}}$Sn$_{\\textrm{0.11}}$O$_{\\textrm{3}}$ ceramic.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Merselmiz, S.; Hanani, Z.; Mezzane, D.; Spreitzer, M.; Bradeško, A.; Fabijan, D.; Vengust, D.; Amjoud, M.; Hajji, L.; Abkhar, Z.; Razumnaya, A. G.; Rožič, B.; Luk'yanchuk, I. A.;  and Kutnjak, Z.\n</span>\n\n  \n\n</span>\n\n  <i>Ceramics International</i>, 46(15): 23867–23876. October 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S027288422031823X\"\n     onclick=\"log_download('merselmiz-hanani-mezzane-spreitzer-bradeko-fabijan-vengust-amjoud-etal-highenergystorageefficiencyandlargeelectrocaloriceffectinleadfreebatitextrm089sntextrm011otextrm3ceramic-2020', 'https://linkinghub.elsevier.com/retrieve/pii/S027288422031823X', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"High energy storage efficiency and large electrocaloric effect in lead-free BaTi$_{\\textrm{0.89}}$Sn$_{\\textrm{0.11}}$O$_{\\textrm{3}}$ ceramic [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.ceramint.2020.06.163\"\n     onclick=\"log_download('merselmiz-hanani-mezzane-spreitzer-bradeko-fabijan-vengust-amjoud-etal-highenergystorageefficiencyandlargeelectrocaloriceffectinleadfreebatitextrm089sntextrm011otextrm3ceramic-2020', 'http://doi.org/10.1016/j.ceramint.2020.06.163', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/merselmiz-hanani-mezzane-spreitzer-bradeko-fabijan-vengust-amjoud-etal-highenergystorageefficiencyandlargeelectrocaloriceffectinleadfreebatitextrm089sntextrm011otextrm3ceramic-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('merselmiz-hanani-mezzane-spreitzer-bradeko-fabijan-vengust-amjoud-etal-highenergystorageefficiencyandlargeelectrocaloriceffectinleadfreebatitextrm089sntextrm011otextrm3ceramic-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{merselmiz_high_2020,\n\ttitle = {High energy storage efficiency and large electrocaloric effect in lead-free {BaTi}$_{\\textrm{0.89}}${Sn}$_{\\textrm{0.11}}${O}$_{\\textrm{3}}$ ceramic},\n\tvolume = {46},\n\tissn = {02728842},\n\turl = {https://linkinghub.elsevier.com/retrieve/pii/S027288422031823X},\n\tdoi = {10.1016/j.ceramint.2020.06.163},\n\tlanguage = {en},\n\tnumber = {15},\n\turldate = {2023-11-11},\n\tjournal = {Ceramics International},\n\tauthor = {Merselmiz, Soukaina and Hanani, Zouhair and Mezzane, Daoud and Spreitzer, Matjaž and Bradeško, Andraž and Fabijan, David and Vengust, Damjan and Amjoud, M’Barek and Hajji, Lahoucine and Abkhar, Zahra and Razumnaya, Anna G. and Rožič, Brigita and Luk&#x27;yanchuk, Igor A. and Kutnjak, Zdravko},\n\tmonth = oct,\n\tyear = {2020},\n\tpages = {23867--23876},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\K8VED7CU\\\\Merselmiz и др. - 2020 - High energy storage efficiency and large electroca.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"razumnaya-mikheykin-stryukov-anokhin-pavlenko-shirokov-kaliteevski-mezzane-etal-builtinelectricfieldinducespolarizationrotationinbilayerbifeotextrm3basrtiotextrm3thinfilms-2020\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0925838819334103\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'razumnaya-mikheykin-stryukov-anokhin-pavlenko-shirokov-kaliteevski-mezzane-etal-builtinelectricfieldinducespolarizationrotationinbilayerbifeotextrm3basrtiotextrm3thinfilms-2020', 'https://linkinghub.elsevier.com/retrieve/pii/S0925838819334103', event);\">\n    Built-in electric field induces polarization rotation in bilayer BiFeO$_{\\textrm{3}}$/(Ba,Sr)TiO$_{\\textrm{3}}$ thin films.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Razumnaya, A.; Mikheykin, A.; Stryukov, D.; Anokhin, A.; Pavlenko, A.; Shirokov, V.; Kaliteevski, M.; Mezzane, D.;  and Lukyanchuk, I.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Alloys and Compounds</i>, 812: 152164. January 2020.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/S0925838819334103\"\n     onclick=\"log_download('razumnaya-mikheykin-stryukov-anokhin-pavlenko-shirokov-kaliteevski-mezzane-etal-builtinelectricfieldinducespolarizationrotationinbilayerbifeotextrm3basrtiotextrm3thinfilms-2020', 'https://linkinghub.elsevier.com/retrieve/pii/S0925838819334103', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Built-in electric field induces polarization rotation in bilayer BiFeO$_{\\textrm{3}}$/(Ba,Sr)TiO$_{\\textrm{3}}$ thin films [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.jallcom.2019.152164\"\n     onclick=\"log_download('razumnaya-mikheykin-stryukov-anokhin-pavlenko-shirokov-kaliteevski-mezzane-etal-builtinelectricfieldinducespolarizationrotationinbilayerbifeotextrm3basrtiotextrm3thinfilms-2020', 'http://doi.org/10.1016/j.jallcom.2019.152164', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/razumnaya-mikheykin-stryukov-anokhin-pavlenko-shirokov-kaliteevski-mezzane-etal-builtinelectricfieldinducespolarizationrotationinbilayerbifeotextrm3basrtiotextrm3thinfilms-2020\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('razumnaya-mikheykin-stryukov-anokhin-pavlenko-shirokov-kaliteevski-mezzane-etal-builtinelectricfieldinducespolarizationrotationinbilayerbifeotextrm3basrtiotextrm3thinfilms-2020')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{razumnaya_built-electric_2020,\n\ttitle = {Built-in electric field induces polarization rotation in bilayer {BiFeO}$_{\\textrm{3}}$/({Ba},{Sr}){TiO}$_{\\textrm{3}}$ thin films},\n\tvolume = {812},\n\tissn = {09258388},\n\turl = {https://linkinghub.elsevier.com/retrieve/pii/S0925838819334103},\n\tdoi = {10.1016/j.jallcom.2019.152164},\n\tlanguage = {en},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Alloys and Compounds},\n\tauthor = {Razumnaya, A.G. and Mikheykin, A.S. and Stryukov, D.V. and Anokhin, A.S. and Pavlenko, A.V. and Shirokov, V.B. and Kaliteevski, M.A. and Mezzane, D. and Lukyanchuk, I.},\n\tmonth = jan,\n\tyear = {2020},\n\tpages = {152164},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\5XSCX5X3\\\\Razumnaya и др. - 2020 - Built-in electric field induces polarization rotat.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2019\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2019')\"\n      onkeypress=\"toggleGroup('group_2019')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2019</span>\n      <span class=\"bibbase_group_count\">\n        \n        (34)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"konevtsova-roshal-boi-podgornik-rochal-hiddensymmetryoftheanomalousbluetongueviruscapsidanditsroleintheinfectionprocess-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://pubs.rsc.org/en/content/articlelanding/2019/sm/c9sm01335k\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'konevtsova-roshal-boi-podgornik-rochal-hiddensymmetryoftheanomalousbluetongueviruscapsidanditsroleintheinfectionprocess-2019', 'https://pubs.rsc.org/en/content/articlelanding/2019/sm/c9sm01335k', event);\">\n    Hidden symmetry of the anomalous bluetongue virus capsid and its role in the infection process.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Konevtsova, O. V.; Roshal, D. S.; Božič, A. L.; Podgornik, R.;  and Rochal, S.\n</span>\n\n  \n\n</span>\n\n  <i>Soft Matter</i>, 15(38): 7663–7671. October 2019.\n  <span class=\"note\">Publisher: The Royal Society of Chemistry</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://pubs.rsc.org/en/content/articlelanding/2019/sm/c9sm01335k\"\n     onclick=\"log_download('konevtsova-roshal-boi-podgornik-rochal-hiddensymmetryoftheanomalousbluetongueviruscapsidanditsroleintheinfectionprocess-2019', 'https://pubs.rsc.org/en/content/articlelanding/2019/sm/c9sm01335k', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Hidden symmetry of the anomalous bluetongue virus capsid and its role in the infection process [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1039/C9SM01335K\"\n     onclick=\"log_download('konevtsova-roshal-boi-podgornik-rochal-hiddensymmetryoftheanomalousbluetongueviruscapsidanditsroleintheinfectionprocess-2019', 'http://doi.org/10.1039/C9SM01335K', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/konevtsova-roshal-boi-podgornik-rochal-hiddensymmetryoftheanomalousbluetongueviruscapsidanditsroleintheinfectionprocess-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('konevtsova-roshal-boi-podgornik-rochal-hiddensymmetryoftheanomalousbluetongueviruscapsidanditsroleintheinfectionprocess-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{konevtsova_hidden_2019,\n\ttitle = {Hidden symmetry of the anomalous bluetongue virus capsid and its role in the infection process},\n\tvolume = {15},\n\tissn = {1744-6848},\n\turl = {https://pubs.rsc.org/en/content/articlelanding/2019/sm/c9sm01335k},\n\tdoi = {10.1039/C9SM01335K},\n\tabstract = {Clear understanding of the principles that control the arrangement of proteins and their self-assembly into viral shells is very important for the development of antiviral strategies. Here we consider the structural peculiarities and hidden symmetry of the anomalous bluetongue virus (BTV) capsid. Each of its three concentric shells violates the paradigmatic geometrical model of Caspar and Klug, which is otherwise well suited to describe most of the known icosahedral viral shells. As we show, three icosahedral spherical lattices, which are commensurate with each other and possess locally hexagonal (primitive or honeycomb) order, underlie the proteinaceous shells of the BTV capsid. This interpretation of the multishelled envelope allows us to discuss the so-called “symmetry mismatch” between its layers. We also analyze the structural stability of the considered spherical lattices on the basis of the classical theory of spherical packing and relate the proximity of the outer spherical lattice to destabilization with the fact that during infection of the cell VP2 trimers are detached from the surface of the BTV capsid. An electrostatic mechanism that can assist in this detachment is discussed in detail.},\n\tlanguage = {en},\n\tnumber = {38},\n\turldate = {2023-11-11},\n\tjournal = {Soft Matter},\n\tauthor = {Konevtsova, Olga V. and Roshal, Daria S. and Božič, Anže Lošdorfer and Podgornik, Rudolf and Rochal, Sergey},\n\tmonth = oct,\n\tyear = {2019},\n\tnote = {Publisher: The Royal Society of Chemistry},\n\tpages = {7663--7671},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Clear understanding of the principles that control the arrangement of proteins and their self-assembly into viral shells is very important for the development of antiviral strategies. Here we consider the structural peculiarities and hidden symmetry of the anomalous bluetongue virus (BTV) capsid. Each of its three concentric shells violates the paradigmatic geometrical model of Caspar and Klug, which is otherwise well suited to describe most of the known icosahedral viral shells. As we show, three icosahedral spherical lattices, which are commensurate with each other and possess locally hexagonal (primitive or honeycomb) order, underlie the proteinaceous shells of the BTV capsid. This interpretation of the multishelled envelope allows us to discuss the so-called “symmetry mismatch” between its layers. We also analyze the structural stability of the considered spherical lattices on the basis of the classical theory of spherical packing and relate the proximity of the outer spherical lattice to destabilization with the fact that during infection of the cell VP2 trimers are detached from the surface of the BTV capsid. An electrostatic mechanism that can assist in this detachment is discussed in detail.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"belyanchikov-savinov-bednyakov-bedran-thomas-torgashev-prokhorov-loidl-etal-hertztoterahertzdielectricresponseofnanoconfinedwatermolecules-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://ieeexplore.ieee.org/document/8873987\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'belyanchikov-savinov-bednyakov-bedran-thomas-torgashev-prokhorov-loidl-etal-hertztoterahertzdielectricresponseofnanoconfinedwatermolecules-2019', 'https://ieeexplore.ieee.org/document/8873987', event);\">\n    Hertz-to-terahertz dielectric response of nanoconfined water molecules.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Belyanchikov, M.; Savinov, M.; Bednyakov, P.; Bedran, Z.; Thomas, V.; Torgashev, V.; Prokhorov, A.; Loidl, A.; Lunkenheimer, P.; Zhukova, E.; Uykur, E.; Dressel, M.;  and Gorshunov, B.\n</span>\n\n  \n\n</span>\n\n  In <i>2019 44th International Conference on Infrared, Millimeter, and Terahertz Waves (IRMMW-THz)</i>, pages 1–3, September 2019. \n  <span class=\"note\">ISSN: 2162-2035</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://ieeexplore.ieee.org/document/8873987\"\n     onclick=\"log_download('belyanchikov-savinov-bednyakov-bedran-thomas-torgashev-prokhorov-loidl-etal-hertztoterahertzdielectricresponseofnanoconfinedwatermolecules-2019', 'https://ieeexplore.ieee.org/document/8873987', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Hertz-to-terahertz dielectric response of nanoconfined water molecules [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1109/IRMMW-THz.2019.8873987\"\n     onclick=\"log_download('belyanchikov-savinov-bednyakov-bedran-thomas-torgashev-prokhorov-loidl-etal-hertztoterahertzdielectricresponseofnanoconfinedwatermolecules-2019', 'http://doi.org/10.1109/IRMMW-THz.2019.8873987', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/belyanchikov-savinov-bednyakov-bedran-thomas-torgashev-prokhorov-loidl-etal-hertztoterahertzdielectricresponseofnanoconfinedwatermolecules-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('belyanchikov-savinov-bednyakov-bedran-thomas-torgashev-prokhorov-loidl-etal-hertztoterahertzdielectricresponseofnanoconfinedwatermolecules-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{belyanchikov_hertz--terahertz_2019,\n\ttitle = {Hertz-to-terahertz dielectric response of nanoconfined water molecules},\n\turl = {https://ieeexplore.ieee.org/document/8873987},\n\tdoi = {10.1109/IRMMW-THz.2019.8873987},\n\tabstract = {Broad-band dielectric spectroscopy, heat capacity measurements and molecular dynamic simulations are applied to study excitations of interacting electric dipoles spatially arranged in a network with an inter-dipole distance of 5-10 Å. The dipoles with magnitude of 1.85 Debye are represented by single H2O molecules located in voids (0.5 nm size) formed by ions of the crystal lattice of cordierite. We discover emergence of nontrivial disordered paraelectric phase of dipolar system with signs of phase transition below 3 K.},\n\turldate = {2023-11-11},\n\tbooktitle = {2019 44th {International} {Conference} on {Infrared}, {Millimeter}, and {Terahertz} {Waves} ({IRMMW}-{THz})},\n\tauthor = {Belyanchikov, M. and Savinov, M. and Bednyakov, P. and Bedran, Z. and Thomas, V. and Torgashev, V. and Prokhorov, A. and Loidl, A. and Lunkenheimer, P. and Zhukova, E. and Uykur, E. and Dressel, M. and Gorshunov, B.},\n\tmonth = sep,\n\tyear = {2019},\n\tnote = {ISSN: 2162-2035},\n\tpages = {1--3},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\DNQPGUUM\\\\Belyanchikov и др. - 2019 - Hertz-to-terahertz dielectric response of nanoconf.pdf:application/pdf;IEEE Xplore Abstract Record:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\RR6G2M8H\\\\8873987.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Broad-band dielectric spectroscopy, heat capacity measurements and molecular dynamic simulations are applied to study excitations of interacting electric dipoles spatially arranged in a network with an inter-dipole distance of 5-10 Å. The dipoles with magnitude of 1.85 Debye are represented by single H2O molecules located in voids (0.5 nm size) formed by ions of the crystal lattice of cordierite. We discover emergence of nontrivial disordered paraelectric phase of dipolar system with signs of phase transition below 3 K.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"andronikova-bronwald-leontyev-leontyev-chernyshov-filimonov-vakhrushev-structuralpeculiaritiesoftheintermediatephaseinzrrichleadzirconatetitanate-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1063783419100056\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'andronikova-bronwald-leontyev-leontyev-chernyshov-filimonov-vakhrushev-structuralpeculiaritiesoftheintermediatephaseinzrrichleadzirconatetitanate-2019', 'https://doi.org/10.1134/S1063783419100056', event);\">\n    Structural Peculiarities of the Intermediate Phase in Zr-Rich Lead Zirconate Titanate.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Andronikova, D. A.; Bronwald, I. A.; Leontyev, N. G.; Leontyev, I. N.; Chernyshov, D. Y.; Filimonov, A. V.;  and Vakhrushev, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Physics of the Solid State</i>, 61(10): 1772–1778. October 2019.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1063783419100056\"\n     onclick=\"log_download('andronikova-bronwald-leontyev-leontyev-chernyshov-filimonov-vakhrushev-structuralpeculiaritiesoftheintermediatephaseinzrrichleadzirconatetitanate-2019', 'https://doi.org/10.1134/S1063783419100056', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Structural Peculiarities of the Intermediate Phase in Zr-Rich Lead Zirconate Titanate [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1063783419100056\"\n     onclick=\"log_download('andronikova-bronwald-leontyev-leontyev-chernyshov-filimonov-vakhrushev-structuralpeculiaritiesoftheintermediatephaseinzrrichleadzirconatetitanate-2019', 'http://doi.org/10.1134/S1063783419100056', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/andronikova-bronwald-leontyev-leontyev-chernyshov-filimonov-vakhrushev-structuralpeculiaritiesoftheintermediatephaseinzrrichleadzirconatetitanate-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('andronikova-bronwald-leontyev-leontyev-chernyshov-filimonov-vakhrushev-structuralpeculiaritiesoftheintermediatephaseinzrrichleadzirconatetitanate-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{andronikova_structural_2019,\n\ttitle = {Structural {Peculiarities} of the {Intermediate} {Phase} in {Zr}-{Rich} {Lead} {Zirconate} {Titanate}},\n\tvolume = {61},\n\tissn = {1090-6460},\n\turl = {https://doi.org/10.1134/S1063783419100056},\n\tdoi = {10.1134/S1063783419100056},\n\tabstract = {This paper presents the results of X-ray diffraction studies on a single crystal of lead zirconate titanate PbZr0.993Ti0.007O3 in the region of existence of an intermediate ferroelectric phase. In addition to the known superstructure reflections of the M type qM = \\$\\${\\textbackslash}left{\\textbackslash}\\{ \\{{\\textbackslash}frac\\{1\\}\\{2\\},{\\textbackslash}frac\\{1\\}\\{2\\},0\\} {\\textbackslash}right{\\textbackslash}\\}\\$\\$and the first-order satellite reflections qM + \\{δ, δ, δ\\}, unknown second-order satellites have been observed near qM and near the Bragg reflections. Structural model of regular system of antiphase domains is used for diffraction calculation. The model is shown to describe the first- and second-orders satellite reflections in the vicinity of qM, but it cannot explain the appearance of satellites around the main Bragg peaks. A possible origin of the system of the superstructures observed in the intermediate phase is discussed.},\n\tlanguage = {en},\n\tnumber = {10},\n\turldate = {2023-11-11},\n\tjournal = {Physics of the Solid State},\n\tauthor = {Andronikova, D. A. and Bronwald, I. A. and Leontyev, N. G. and Leontyev, I. N. and Chernyshov, D. Yu. and Filimonov, A. V. and Vakhrushev, S. B.},\n\tmonth = oct,\n\tyear = {2019},\n\tkeywords = {ferroelectrics, phase transitions, and crystal structure, perovskite structure, X-ray scattering},\n\tpages = {1772--1778},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  This paper presents the results of X-ray diffraction studies on a single crystal of lead zirconate titanate PbZr0.993Ti0.007O3 in the region of existence of an intermediate ferroelectric phase. In addition to the known superstructure reflections of the M type qM = $$\\left\\\\ \\\\frac\\1\\\\2\\,\\frac\\1\\\\2\\,0\\ \\right\\\\$$and the first-order satellite reflections qM + \\δ, δ, δ\\, unknown second-order satellites have been observed near qM and near the Bragg reflections. Structural model of regular system of antiphase domains is used for diffraction calculation. The model is shown to describe the first- and second-orders satellite reflections in the vicinity of qM, but it cannot explain the appearance of satellites around the main Bragg peaks. A possible origin of the system of the superstructures observed in the intermediate phase is discussed.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"rochal-levshov-avramenko-arenal-cao-nguyen-sauvajol-paillet-chiralitymanifestationinelasticcouplingbetweenthelayersofdoublewalledcarbonnanotubes-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://pubs.rsc.org/en/content/articlelanding/2019/nr/c9nr03853a\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'rochal-levshov-avramenko-arenal-cao-nguyen-sauvajol-paillet-chiralitymanifestationinelasticcouplingbetweenthelayersofdoublewalledcarbonnanotubes-2019', 'https://pubs.rsc.org/en/content/articlelanding/2019/nr/c9nr03853a', event);\">\n    Chirality manifestation in elastic coupling between the layers of double-walled carbon nanotubes.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Rochal, S.; Levshov, D.; Avramenko, M.; Arenal, R.; Cao, T. T.; Nguyen, V. C.; Sauvajol, J.;  and Paillet, M.\n</span>\n\n  \n\n</span>\n\n  <i>Nanoscale</i>, 11(34): 16092–16102. August 2019.\n  <span class=\"note\">Publisher: The Royal Society of Chemistry</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://pubs.rsc.org/en/content/articlelanding/2019/nr/c9nr03853a\"\n     onclick=\"log_download('rochal-levshov-avramenko-arenal-cao-nguyen-sauvajol-paillet-chiralitymanifestationinelasticcouplingbetweenthelayersofdoublewalledcarbonnanotubes-2019', 'https://pubs.rsc.org/en/content/articlelanding/2019/nr/c9nr03853a', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Chirality manifestation in elastic coupling between the layers of double-walled carbon nanotubes [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1039/C9NR03853A\"\n     onclick=\"log_download('rochal-levshov-avramenko-arenal-cao-nguyen-sauvajol-paillet-chiralitymanifestationinelasticcouplingbetweenthelayersofdoublewalledcarbonnanotubes-2019', 'http://doi.org/10.1039/C9NR03853A', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/rochal-levshov-avramenko-arenal-cao-nguyen-sauvajol-paillet-chiralitymanifestationinelasticcouplingbetweenthelayersofdoublewalledcarbonnanotubes-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('rochal-levshov-avramenko-arenal-cao-nguyen-sauvajol-paillet-chiralitymanifestationinelasticcouplingbetweenthelayersofdoublewalledcarbonnanotubes-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{rochal_chirality_2019,\n\ttitle = {Chirality manifestation in elastic coupling between the layers of double-walled carbon nanotubes},\n\tvolume = {11},\n\tissn = {2040-3372},\n\turl = {https://pubs.rsc.org/en/content/articlelanding/2019/nr/c9nr03853a},\n\tdoi = {10.1039/C9NR03853A},\n\tabstract = {The search for new relatively easy physicochemical methods for the structural identification of carbon nanotubes represents a key challenge. Here, analyzing the experimental data on double-walled carbon nanotubes (DWCNTs) obtained by us and taken from the literature, we have expressed the magnitude of elastic coupling between two tubular walls forming a DWCNT as a simple function dependent not only on DWCNT diameters but also on the difference between the chirality angles of the constituent nanotubes. To get this quite unexpected result, which allows us to relate more precisely the structural parameters of a DWCNT with frequencies of its radial breathing-like modes (RBLM), we have developed a new model for the RBLM dynamics that takes into account a possible deposition of water molecules from ambient air onto the DWCNT surface. The model constructed allows us to predict the higher prevalence of DWCNTs comprising two walls with identical handedness. The application of the results obtained for the identification of DWCNTs is also considered.},\n\tlanguage = {en},\n\tnumber = {34},\n\turldate = {2023-11-11},\n\tjournal = {Nanoscale},\n\tauthor = {Rochal, Sergei and Levshov, Dmitry and Avramenko, Marina and Arenal, Raul and Cao, Thi Thanh and Nguyen, Van Chuc and Sauvajol, Jean-Louis and Paillet, Matthieu},\n\tmonth = aug,\n\tyear = {2019},\n\tnote = {Publisher: The Royal Society of Chemistry},\n\tpages = {16092--16102},\n\tfile = {Supplementary Information PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\EJHII2SI\\\\Rochal и др. - 2019 - Chirality manifestation in elastic coupling betwee.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The search for new relatively easy physicochemical methods for the structural identification of carbon nanotubes represents a key challenge. Here, analyzing the experimental data on double-walled carbon nanotubes (DWCNTs) obtained by us and taken from the literature, we have expressed the magnitude of elastic coupling between two tubular walls forming a DWCNT as a simple function dependent not only on DWCNT diameters but also on the difference between the chirality angles of the constituent nanotubes. To get this quite unexpected result, which allows us to relate more precisely the structural parameters of a DWCNT with frequencies of its radial breathing-like modes (RBLM), we have developed a new model for the RBLM dynamics that takes into account a possible deposition of water molecules from ambient air onto the DWCNT surface. The model constructed allows us to predict the higher prevalence of DWCNTs comprising two walls with identical handedness. The application of the results obtained for the identification of DWCNTs is also considered.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"levi-kalinchuk-shirokov-somedynamicfeaturesofferroelectricthinfilms-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/1260/9/092004\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'levi-kalinchuk-shirokov-somedynamicfeaturesofferroelectricthinfilms-2019', 'https://dx.doi.org/10.1088/1742-6596/1260/9/092004', event);\">\n    Some dynamic features of ferroelectric thin films.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Levi, M. O.; Kalinchuk, V. V.;  and Shirokov, V. B.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics: Conference Series</i>, 1260(9): 092004. August 2019.\n  <span class=\"note\">Publisher: IOP Publishing</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/1260/9/092004\"\n     onclick=\"log_download('levi-kalinchuk-shirokov-somedynamicfeaturesofferroelectricthinfilms-2019', 'https://dx.doi.org/10.1088/1742-6596/1260/9/092004', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Some dynamic features of ferroelectric thin films [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/1742-6596/1260/9/092004\"\n     onclick=\"log_download('levi-kalinchuk-shirokov-somedynamicfeaturesofferroelectricthinfilms-2019', 'http://doi.org/10.1088/1742-6596/1260/9/092004', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/levi-kalinchuk-shirokov-somedynamicfeaturesofferroelectricthinfilms-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('levi-kalinchuk-shirokov-somedynamicfeaturesofferroelectricthinfilms-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{levi_dynamic_2019,\n\ttitle = {Some dynamic features of ferroelectric thin films},\n\tvolume = {1260},\n\tissn = {1742-6596},\n\turl = {https://dx.doi.org/10.1088/1742-6596/1260/9/092004},\n\tdoi = {10.1088/1742-6596/1260/9/092004},\n\tabstract = {The dynamic problem of the surface acoustic wave propagation in a thin-film structure is investigated. The propagation of plane waves in the film-substrate structure is considered. Thin film is made of barium titanate oxide, and solid substrate is made of magnesium oxide. Ferroelectric film is subjected to misfit strain because of the deposition. Assumed that the solid substrate retains its properties due to the large difference in the hardness of the materials. Built Green function, obtained phase velocities and electromechanical coupling coefficients in the C-phase of BaTiO3. The present investigation is of practical interest for developing high-frequencies smart ferroelectric devices for engineering applications.},\n\tlanguage = {en},\n\tnumber = {9},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics: Conference Series},\n\tauthor = {Levi, M. O. and Kalinchuk, V. V. and Shirokov, V. B.},\n\tmonth = aug,\n\tyear = {2019},\n\tnote = {Publisher: IOP Publishing},\n\tpages = {092004},\n\tfile = {IOP Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\7XMUB7ZU\\\\Levi и др. - 2019 - Some dynamic features of ferroelectric thin films.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The dynamic problem of the surface acoustic wave propagation in a thin-film structure is investigated. The propagation of plane waves in the film-substrate structure is considered. Thin film is made of barium titanate oxide, and solid substrate is made of magnesium oxide. Ferroelectric film is subjected to misfit strain because of the deposition. Assumed that the solid substrate retains its properties due to the large difference in the hardness of the materials. Built Green function, obtained phase velocities and electromechanical coupling coefficients in the C-phase of BaTiO3. The present investigation is of practical interest for developing high-frequencies smart ferroelectric devices for engineering applications.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"chalin-avramenko-parmeggiani-rochal-lowfrequencyphonondynamicsandrelatedthermalpropertiesofaxiallystressedsinglewalledcarbonnanotubes-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/1361-648X/ab285c\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'chalin-avramenko-parmeggiani-rochal-lowfrequencyphonondynamicsandrelatedthermalpropertiesofaxiallystressedsinglewalledcarbonnanotubes-2019', 'https://dx.doi.org/10.1088/1361-648X/ab285c', event);\">\n    Low-frequency phonon dynamics and related thermal properties of axially stressed single-walled carbon nanotubes.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Chalin, D.; Avramenko, M.; Parmeggiani, A.;  and Rochal, S.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics: Condensed Matter</i>, 31(42): 425302. July 2019.\n  <span class=\"note\">Publisher: IOP Publishing</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/1361-648X/ab285c\"\n     onclick=\"log_download('chalin-avramenko-parmeggiani-rochal-lowfrequencyphonondynamicsandrelatedthermalpropertiesofaxiallystressedsinglewalledcarbonnanotubes-2019', 'https://dx.doi.org/10.1088/1361-648X/ab285c', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Low-frequency phonon dynamics and related thermal properties of axially stressed single-walled carbon nanotubes [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/1361-648X/ab285c\"\n     onclick=\"log_download('chalin-avramenko-parmeggiani-rochal-lowfrequencyphonondynamicsandrelatedthermalpropertiesofaxiallystressedsinglewalledcarbonnanotubes-2019', 'http://doi.org/10.1088/1361-648X/ab285c', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/chalin-avramenko-parmeggiani-rochal-lowfrequencyphonondynamicsandrelatedthermalpropertiesofaxiallystressedsinglewalledcarbonnanotubes-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('chalin-avramenko-parmeggiani-rochal-lowfrequencyphonondynamicsandrelatedthermalpropertiesofaxiallystressedsinglewalledcarbonnanotubes-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{chalin_low-frequency_2019,\n\ttitle = {Low-frequency phonon dynamics and related thermal properties of axially stressed single-walled carbon nanotubes},\n\tvolume = {31},\n\tissn = {0953-8984},\n\turl = {https://dx.doi.org/10.1088/1361-648X/ab285c},\n\tdoi = {10.1088/1361-648X/ab285c},\n\tabstract = {Synthesis temperatures of composite materials are usually far less than the ones of their use, thus carbon nanotubes (CNTs) embedded into a polymer matrix undergo significant axial stress. We develop a continuous theory, which describes the dynamics of stressed single-walled (SW-) CNTs and predicts their low-frequency phonon spectra. The changes in dispersion laws of SWCNT low-frequency phonon modes due to the axial stress of different signs are discussed. Then, the results obtained are used to analyze low-temperature (T {\\textless} 70 K) heat capacity and thermal conductivity of individual nanotubes. We demonstrate that compressive stress leads to increase in heat capacity CV of an individual SWCNT, while tensile stress causes CV to decrease. In the latter case at T → 0 heat capacity diminishes according to a linear law T instead of a power one T1/2. Nevertheless, according to our results, axial stress hardly affects low-temperature thermal conductance of SWCNTs. Influence of investigated effects on the corresponding macroscopic properties of CNT-based composite materials are also discussed.},\n\tlanguage = {en},\n\tnumber = {42},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics: Condensed Matter},\n\tauthor = {Chalin, Dmitrii and Avramenko, Marina and Parmeggiani, Andrea and Rochal, Sergei},\n\tmonth = jul,\n\tyear = {2019},\n\tnote = {Publisher: IOP Publishing},\n\tpages = {425302},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Synthesis temperatures of composite materials are usually far less than the ones of their use, thus carbon nanotubes (CNTs) embedded into a polymer matrix undergo significant axial stress. We develop a continuous theory, which describes the dynamics of stressed single-walled (SW-) CNTs and predicts their low-frequency phonon spectra. The changes in dispersion laws of SWCNT low-frequency phonon modes due to the axial stress of different signs are discussed. Then, the results obtained are used to analyze low-temperature (T \\textless 70 K) heat capacity and thermal conductivity of individual nanotubes. We demonstrate that compressive stress leads to increase in heat capacity CV of an individual SWCNT, while tensile stress causes CV to decrease. In the latter case at T → 0 heat capacity diminishes according to a linear law T instead of a power one T1/2. Nevertheless, according to our results, axial stress hardly affects low-temperature thermal conductance of SWCNTs. Influence of investigated effects on the corresponding macroscopic properties of CNT-based composite materials are also discussed.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"alyabyeva-torgashev-zhukova-vinnik-prokhorov-gudkova-gngora-ivek-etal-influenceofchemicalsubstitutiononbroadbanddielectricresponseofbariumleadmtypehexaferrite-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/1367-2630/ab2476\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'alyabyeva-torgashev-zhukova-vinnik-prokhorov-gudkova-gngora-ivek-etal-influenceofchemicalsubstitutiononbroadbanddielectricresponseofbariumleadmtypehexaferrite-2019', 'https://dx.doi.org/10.1088/1367-2630/ab2476', event);\">\n    Influence of chemical substitution on broadband dielectric response of barium-lead M-type hexaferrite.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Alyabyeva, L. N.; Torgashev, V. I.; Zhukova, E. S.; Vinnik, D. A.; Prokhorov, A. S.; Gudkova, S. A.; Góngora, D. R.; Ivek, T.; Tomić, S.; Novosel, N.; Starešinić, D.; Dominko, D.; Jagličić, Z.; Dressel, M.; Zherebtsov, D. A.;  and Gorshunov, B. P.\n</span>\n\n  \n\n</span>\n\n  <i>New Journal of Physics</i>, 21(6): 063016. June 2019.\n  <span class=\"note\">Publisher: IOP Publishing</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/1367-2630/ab2476\"\n     onclick=\"log_download('alyabyeva-torgashev-zhukova-vinnik-prokhorov-gudkova-gngora-ivek-etal-influenceofchemicalsubstitutiononbroadbanddielectricresponseofbariumleadmtypehexaferrite-2019', 'https://dx.doi.org/10.1088/1367-2630/ab2476', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Influence of chemical substitution on broadband dielectric response of barium-lead M-type hexaferrite [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/1367-2630/ab2476\"\n     onclick=\"log_download('alyabyeva-torgashev-zhukova-vinnik-prokhorov-gudkova-gngora-ivek-etal-influenceofchemicalsubstitutiononbroadbanddielectricresponseofbariumleadmtypehexaferrite-2019', 'http://doi.org/10.1088/1367-2630/ab2476', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/alyabyeva-torgashev-zhukova-vinnik-prokhorov-gudkova-gngora-ivek-etal-influenceofchemicalsubstitutiononbroadbanddielectricresponseofbariumleadmtypehexaferrite-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('alyabyeva-torgashev-zhukova-vinnik-prokhorov-gudkova-gngora-ivek-etal-influenceofchemicalsubstitutiononbroadbanddielectricresponseofbariumleadmtypehexaferrite-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{alyabyeva_influence_2019,\n\ttitle = {Influence of chemical substitution on broadband dielectric response of barium-lead {M}-type hexaferrite},\n\tvolume = {21},\n\tissn = {1367-2630},\n\turl = {https://dx.doi.org/10.1088/1367-2630/ab2476},\n\tdoi = {10.1088/1367-2630/ab2476},\n\tabstract = {We report on the electrodynamic properties of the single crystalline lead-substituted M-type barium hexaferrite, Ba0.3Pb0.7Fe12O19, performed in the broad frequency range including radio-frequency, terahertz and sub-terahertz bands, which are particularly important for the development of microelectronic devices. We demonstrate how changing on a molecular level the chemical characteristics (composition, intermolecular interaction, spin-orbital interaction) of lead-substituted M-type hexaferrite influences its radio-frequency and terahertz electrodynamic response. Our results indicate a critical temperature range, 50 K {\\textless} T {\\textless} 70 K, where significant changes of the electrodynamic response occur that are interpreted as freezing of dynamical oscillations of bi-pyramidal Fe(2b) ions. In the range 5–300 K, the heat capacity shows no sign of any phase transition and is solely determined by electron and phonon contributions. An anomalous electrodynamic response is detected at 1–2 THz that features a rich set of absorption resonances which are associated with electronic transitions within the fine-structured Fe2+ ground state and are visualized in the spectra due to magnetostriction and electron–phonon interaction. We show that lead substitution of barium in barium hexaferrite, BaFe12O19, leads to the emergence of a pronounced dielectric and magnetic relaxational dynamics at radio-frequencies and that both dynamics have the same characteristic relaxation times, thus evidencing the bi-relaxor-like nature of Ba0.3Pb0.7Fe12O19. We associate the origin of the relaxations as connected with the motion of magnetic domain walls. In order to unveil crucial influence of chemical substitution on electrodynamic characteristics of the compound, we analyze our results on substituted compound in comparison with the data available for pristine barium (BaFe12O19) and pristine lead (PbFe12O19) hexaferrites. The obtained spectroscopic data on the dielectric properties of Ba0.3Pb0.7Fe12O19 provide insight into fundamental phenomena responsible for the absorption mechanisms of the compound and demonstrates that chemical ionic substitution is an effective tool to tune the dielectric properties of the whole family of hexaferrites.},\n\tlanguage = {en},\n\tnumber = {6},\n\turldate = {2023-11-11},\n\tjournal = {New Journal of Physics},\n\tauthor = {Alyabyeva, Liudmila N. and Torgashev, Victor I. and Zhukova, Elena S. and Vinnik, Denis A. and Prokhorov, Anatoliy S. and Gudkova, Svetlana A. and Góngora, David Rivas and Ivek, Tomislav and Tomić, Silvia and Novosel, Nikolina and Starešinić, Damir and Dominko, Damir and Jagličić, Zvonko and Dressel, Martin and Zherebtsov, Dmitry A. and Gorshunov, Boris P.},\n\tmonth = jun,\n\tyear = {2019},\n\tnote = {Publisher: IOP Publishing},\n\tpages = {063016},\n\tfile = {IOP Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\4XWDRV9S\\\\Alyabyeva и др. - 2019 - Influence of chemical substitution on broadband di.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We report on the electrodynamic properties of the single crystalline lead-substituted M-type barium hexaferrite, Ba0.3Pb0.7Fe12O19, performed in the broad frequency range including radio-frequency, terahertz and sub-terahertz bands, which are particularly important for the development of microelectronic devices. We demonstrate how changing on a molecular level the chemical characteristics (composition, intermolecular interaction, spin-orbital interaction) of lead-substituted M-type hexaferrite influences its radio-frequency and terahertz electrodynamic response. Our results indicate a critical temperature range, 50 K \\textless T \\textless 70 K, where significant changes of the electrodynamic response occur that are interpreted as freezing of dynamical oscillations of bi-pyramidal Fe(2b) ions. In the range 5–300 K, the heat capacity shows no sign of any phase transition and is solely determined by electron and phonon contributions. An anomalous electrodynamic response is detected at 1–2 THz that features a rich set of absorption resonances which are associated with electronic transitions within the fine-structured Fe2+ ground state and are visualized in the spectra due to magnetostriction and electron–phonon interaction. We show that lead substitution of barium in barium hexaferrite, BaFe12O19, leads to the emergence of a pronounced dielectric and magnetic relaxational dynamics at radio-frequencies and that both dynamics have the same characteristic relaxation times, thus evidencing the bi-relaxor-like nature of Ba0.3Pb0.7Fe12O19. We associate the origin of the relaxations as connected with the motion of magnetic domain walls. In order to unveil crucial influence of chemical substitution on electrodynamic characteristics of the compound, we analyze our results on substituted compound in comparison with the data available for pristine barium (BaFe12O19) and pristine lead (PbFe12O19) hexaferrites. The obtained spectroscopic data on the dielectric properties of Ba0.3Pb0.7Fe12O19 provide insight into fundamental phenomena responsible for the absorption mechanisms of the compound and demonstrates that chemical ionic substitution is an effective tool to tune the dielectric properties of the whole family of hexaferrites.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"talanov-talanov-shirokov-grouptheoreticalclassificationofaristotypesofcationandanionordersinperovskites-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1063774519030258\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'talanov-talanov-shirokov-grouptheoreticalclassificationofaristotypesofcationandanionordersinperovskites-2019', 'https://doi.org/10.1134/S1063774519030258', event);\">\n    Group-Theoretical Classification of Aristotypes of Cation and Anion Orders in Perovskites.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Talanov, M. V.; Talanov, V. M.;  and Shirokov, V. B.\n</span>\n\n  \n\n</span>\n\n  <i>Crystallography Reports</i>, 64(3): 386–391. May 2019.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1063774519030258\"\n     onclick=\"log_download('talanov-talanov-shirokov-grouptheoreticalclassificationofaristotypesofcationandanionordersinperovskites-2019', 'https://doi.org/10.1134/S1063774519030258', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Group-Theoretical Classification of Aristotypes of Cation and Anion Orders in Perovskites [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1063774519030258\"\n     onclick=\"log_download('talanov-talanov-shirokov-grouptheoreticalclassificationofaristotypesofcationandanionordersinperovskites-2019', 'http://doi.org/10.1134/S1063774519030258', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/talanov-talanov-shirokov-grouptheoreticalclassificationofaristotypesofcationandanionordersinperovskites-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('talanov-talanov-shirokov-grouptheoreticalclassificationofaristotypesofcationandanionordersinperovskites-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{talanov_group-theoretical_2019,\n\ttitle = {Group-{Theoretical} {Classification} of {Aristotypes} of {Cation} and {Anion} {Orders} in {Perovskites}},\n\tvolume = {64},\n\tissn = {1562-689X},\n\turl = {https://doi.org/10.1134/S1063774519030258},\n\tdoi = {10.1134/S1063774519030258},\n\tabstract = {A group-theoretical classification of cation and anion orders of crystals with a perovskite structure is presented. Aristotypes are idealized structures (phases), from which the low-symmetry ordered modifications of perovskites are formed as a result of rotations and deformation of octahedra, as well as the cooperative Jahn–Teller effect and other physical phenomena. Seven aristotype classes have been distinguished, which are characterized by the atomic ordering in each of Wyckoff positions and simultaneous atomic ordering in several positions. The critical and secondary (improper) order parameters, describing the formation of ordered structures, are determined. The classification proposed makes it possible to systematize a variety of known phases, establish genetic structural links between low-symmetry ordered structures, and design new materials.},\n\tlanguage = {en},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Crystallography Reports},\n\tauthor = {Talanov, M. V. and Talanov, V. M. and Shirokov, V. B.},\n\tmonth = may,\n\tyear = {2019},\n\tpages = {386--391},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A group-theoretical classification of cation and anion orders of crystals with a perovskite structure is presented. Aristotypes are idealized structures (phases), from which the low-symmetry ordered modifications of perovskites are formed as a result of rotations and deformation of octahedra, as well as the cooperative Jahn–Teller effect and other physical phenomena. Seven aristotype classes have been distinguished, which are characterized by the atomic ordering in each of Wyckoff positions and simultaneous atomic ordering in several positions. The critical and secondary (improper) order parameters, describing the formation of ordered structures, are determined. The classification proposed makes it possible to systematize a variety of known phases, establish genetic structural links between low-symmetry ordered structures, and design new materials.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"lukyanchuk-zaitseva-levashenko-kvassay-kondovych-tikhonov-baudry-razumnaya-ferroelectricmultiplevaluedlogicunits-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/00150193.2019.1592436\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'lukyanchuk-zaitseva-levashenko-kvassay-kondovych-tikhonov-baudry-razumnaya-ferroelectricmultiplevaluedlogicunits-2019', 'https://doi.org/10.1080/00150193.2019.1592436', event);\">\n    Ferroelectric multiple-valued logic units.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Lukyanchuk, I.; Zaitseva, E.; Levashenko, V.; Kvassay, M.; Kondovych, S.; Tikhonov, Y.; Baudry, L.;  and Razumnaya, A.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 543(1): 213–221. April 2019.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2019.1592436</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/00150193.2019.1592436\"\n     onclick=\"log_download('lukyanchuk-zaitseva-levashenko-kvassay-kondovych-tikhonov-baudry-razumnaya-ferroelectricmultiplevaluedlogicunits-2019', 'https://doi.org/10.1080/00150193.2019.1592436', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Ferroelectric multiple-valued logic units [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150193.2019.1592436\"\n     onclick=\"log_download('lukyanchuk-zaitseva-levashenko-kvassay-kondovych-tikhonov-baudry-razumnaya-ferroelectricmultiplevaluedlogicunits-2019', 'http://doi.org/10.1080/00150193.2019.1592436', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/lukyanchuk-zaitseva-levashenko-kvassay-kondovych-tikhonov-baudry-razumnaya-ferroelectricmultiplevaluedlogicunits-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('lukyanchuk-zaitseva-levashenko-kvassay-kondovych-tikhonov-baudry-razumnaya-ferroelectricmultiplevaluedlogicunits-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{lukyanchuk_ferroelectric_2019,\n\ttitle = {Ferroelectric multiple-valued logic units},\n\tvolume = {543},\n\tissn = {0015-0193},\n\turl = {https://doi.org/10.1080/00150193.2019.1592436},\n\tdoi = {10.1080/00150193.2019.1592436},\n\tabstract = {Employing many-valued logic (MVL) data processing allows to dramatically increase the performance of computing circuits. Here we propose to employ ferroelectrics for the material implementation of MVL units basing on their ability to pin the polarization as a sequence of multi-stable states. Two conceptual ideas are considered. As the first system, we suggest using the strained ferroelectric films that can host the polarization states, allowing the effective field-induced multilevel switching between them. As the second one, we propose to employ the ferroelectric nano-samples that confine the topologically protected polarization textures, which may be used as MVL structural elements. We demonstrate that these systems are suitable for engineering of the 3-, 4- and even 5-level logic units and consider the circuit design for such elements.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Ferroelectrics},\n\tauthor = {Lukyanchuk, Igor and Zaitseva, Elena and Levashenko, Vitaly and Kvassay, Miroslav and Kondovych, Svitlana and Tikhonov, Yuri and Baudry, Laurent and Razumnaya, Anna},\n\tmonth = apr,\n\tyear = {2019},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/00150193.2019.1592436},\n\tkeywords = {Ferroelectrics, switching, domain, hysteresis, multiple-valued logic, skyrmion, topological structures, vortex},\n\tpages = {213--221},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\VXZHNBRF\\\\Lukyanchuk и др. - 2019 - Ferroelectric multiple-valued logic units.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Employing many-valued logic (MVL) data processing allows to dramatically increase the performance of computing circuits. Here we propose to employ ferroelectrics for the material implementation of MVL units basing on their ability to pin the polarization as a sequence of multi-stable states. Two conceptual ideas are considered. As the first system, we suggest using the strained ferroelectric films that can host the polarization states, allowing the effective field-induced multilevel switching between them. As the second one, we propose to employ the ferroelectric nano-samples that confine the topologically protected polarization textures, which may be used as MVL structural elements. We demonstrate that these systems are suitable for engineering of the 3-, 4- and even 5-level logic units and consider the circuit design for such elements.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"gorkovaya-tikhonov-torgashev-mikheykin-lukyanchuk-mezzane-ortega-kumar-etal-propertiesofthelowfrequencyphononspectraofferroelectricbariumtitanatebasedheterostructures-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/00150193.2019.1592446\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'gorkovaya-tikhonov-torgashev-mikheykin-lukyanchuk-mezzane-ortega-kumar-etal-propertiesofthelowfrequencyphononspectraofferroelectricbariumtitanatebasedheterostructures-2019', 'https://doi.org/10.1080/00150193.2019.1592446', event);\">\n    Properties of the low-frequency phonon spectra of ferroelectric barium titanate-based heterostructures.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Gor’kovaya, E. D.; Tikhonov, Y. A.; Torgashev, V. I.; Mikheykin, A. S.; Lukyanchuk, I. A.; Mezzane, D.; Ortega, N.; Kumar, A.; Katiyar, R. S.;  and Razumnaya, A. G.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 543(1): 36–47. April 2019.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2019.1592446</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/00150193.2019.1592446\"\n     onclick=\"log_download('gorkovaya-tikhonov-torgashev-mikheykin-lukyanchuk-mezzane-ortega-kumar-etal-propertiesofthelowfrequencyphononspectraofferroelectricbariumtitanatebasedheterostructures-2019', 'https://doi.org/10.1080/00150193.2019.1592446', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Properties of the low-frequency phonon spectra of ferroelectric barium titanate-based heterostructures [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150193.2019.1592446\"\n     onclick=\"log_download('gorkovaya-tikhonov-torgashev-mikheykin-lukyanchuk-mezzane-ortega-kumar-etal-propertiesofthelowfrequencyphononspectraofferroelectricbariumtitanatebasedheterostructures-2019', 'http://doi.org/10.1080/00150193.2019.1592446', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/gorkovaya-tikhonov-torgashev-mikheykin-lukyanchuk-mezzane-ortega-kumar-etal-propertiesofthelowfrequencyphononspectraofferroelectricbariumtitanatebasedheterostructures-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('gorkovaya-tikhonov-torgashev-mikheykin-lukyanchuk-mezzane-ortega-kumar-etal-propertiesofthelowfrequencyphononspectraofferroelectricbariumtitanatebasedheterostructures-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{gorkovaya_properties_2019,\n\ttitle = {Properties of the low-frequency phonon spectra of ferroelectric barium titanate-based heterostructures},\n\tvolume = {543},\n\tissn = {0015-0193},\n\turl = {https://doi.org/10.1080/00150193.2019.1592446},\n\tdoi = {10.1080/00150193.2019.1592446},\n\tabstract = {Polarized Raman spectra of the epitaxial Ba0.5Sr0.5TiO3 film, bi-color BaTiO3/Ba0.5Sr0.5TiO3 superlattice and tri-color BaTiO3/Ba0.5Sr0.5TiO3/SrTiO3 superlattice were studied in a broad temperature range of 80–700 K. Based on the temperature dependence of the polar modes we determined the phase transitions temperatures in the studied heterostructures. In the sub-THz frequency range of the Y(XZ)Y¯spectra, we revealed the coexistence of the Debye-type central peak and soft mode in bi-color BaTiO3/Ba0.5Sr0.5TiO3 superlattice.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Ferroelectrics},\n\tauthor = {Gor’kovaya, E. D. and Tikhonov, Yu. A. and Torgashev, V. I. and Mikheykin, A. S. and Lukyanchuk, I. A. and Mezzane, D. and Ortega, N. and Kumar, A. and Katiyar, R. S. and Razumnaya, A. G.},\n\tmonth = apr,\n\tyear = {2019},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/00150193.2019.1592446},\n\tkeywords = {Raman spectroscopy, soft mode, central peak, superlattice, thin film},\n\tpages = {36--47},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\PCXC4STE\\\\Gor’kovaya и др. - 2019 - Properties of the low-frequency phonon spectra of .pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Polarized Raman spectra of the epitaxial Ba0.5Sr0.5TiO3 film, bi-color BaTiO3/Ba0.5Sr0.5TiO3 superlattice and tri-color BaTiO3/Ba0.5Sr0.5TiO3/SrTiO3 superlattice were studied in a broad temperature range of 80–700 K. Based on the temperature dependence of the polar modes we determined the phase transitions temperatures in the studied heterostructures. In the sub-THz frequency range of the Y(XZ)Y¯spectra, we revealed the coexistence of the Debye-type central peak and soft mode in bi-color BaTiO3/Ba0.5Sr0.5TiO3 superlattice.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"roshal-konevtsova-lodorferboi-podgornik-rochal-phinducedmorphologicalchangesofproteinaceousviralshells-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.nature.com/articles/s41598-019-41799-6\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'roshal-konevtsova-lodorferboi-podgornik-rochal-phinducedmorphologicalchangesofproteinaceousviralshells-2019', 'https://www.nature.com/articles/s41598-019-41799-6', event);\">\n    pH-induced morphological changes of proteinaceous viral shells.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Roshal, D.; Konevtsova, O.; Lošdorfer Božič, A.; Podgornik, R.;  and Rochal, S.\n</span>\n\n  \n\n</span>\n\n  <i>Scientific Reports</i>, 9(1): 5341. March 2019.\n  <span class=\"note\">Number: 1 Publisher: Nature Publishing Group</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.nature.com/articles/s41598-019-41799-6\"\n     onclick=\"log_download('roshal-konevtsova-lodorferboi-podgornik-rochal-phinducedmorphologicalchangesofproteinaceousviralshells-2019', 'https://www.nature.com/articles/s41598-019-41799-6', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"pH-induced morphological changes of proteinaceous viral shells [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1038/s41598-019-41799-6\"\n     onclick=\"log_download('roshal-konevtsova-lodorferboi-podgornik-rochal-phinducedmorphologicalchangesofproteinaceousviralshells-2019', 'http://doi.org/10.1038/s41598-019-41799-6', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/roshal-konevtsova-lodorferboi-podgornik-rochal-phinducedmorphologicalchangesofproteinaceousviralshells-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('roshal-konevtsova-lodorferboi-podgornik-rochal-phinducedmorphologicalchangesofproteinaceousviralshells-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{roshal_ph-induced_2019,\n\ttitle = {{pH}-induced morphological changes of proteinaceous viral shells},\n\tvolume = {9},\n\tcopyright = {2019 The Author(s)},\n\tissn = {2045-2322},\n\turl = {https://www.nature.com/articles/s41598-019-41799-6},\n\tdoi = {10.1038/s41598-019-41799-6},\n\tabstract = {Changes in environmental pH can induce morphological changes in empty proteinaceous shells of bacteriophages in vitro that are very similar to changes occurring in viral capsids in vivo after encapsidation of DNA. These changes in capsid shape and size cannot be explained with a simple elastic model alone. We propose a new theoretical framework that combines the elasticity of thin icosahedral shells with the pH dependence of capsid charge distribution. Minimization of the sum of elastic and electrostatic free energies leads to equilibrium shapes of viral shells that depend on a single elastic parameter and the detailed configuration of the imbedded protein charges. Based on the in vitro shell reconstructions of bacteriophage HK97 we elucidate the details of how the reversible transition between Prohead II and Expansion Intermediate II states of the HK97 procapsid is induced by pH changes, as well as some other features of the bacteriophage maturation.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Scientific Reports},\n\tauthor = {Roshal, D. and Konevtsova, O. and Lošdorfer Božič, A. and Podgornik, R. and Rochal, S.},\n\tmonth = mar,\n\tyear = {2019},\n\tnote = {Number: 1\nPublisher: Nature Publishing Group},\n\tkeywords = {Biological physics, Molecular self-assembly},\n\tpages = {5341},\n\tfile = {Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\MGU2DMMM\\\\Roshal и др. - 2019 - pH-induced morphological changes of proteinaceous .pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Changes in environmental pH can induce morphological changes in empty proteinaceous shells of bacteriophages in vitro that are very similar to changes occurring in viral capsids in vivo after encapsidation of DNA. These changes in capsid shape and size cannot be explained with a simple elastic model alone. We propose a new theoretical framework that combines the elasticity of thin icosahedral shells with the pH dependence of capsid charge distribution. Minimization of the sum of elastic and electrostatic free energies leads to equilibrium shapes of viral shells that depend on a single elastic parameter and the detailed configuration of the imbedded protein charges. Based on the in vitro shell reconstructions of bacteriophage HK97 we elucidate the details of how the reversible transition between Prohead II and Expansion Intermediate II states of the HK97 procapsid is induced by pH changes, as well as some other features of the bacteriophage maturation.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"lerer-golovacheva-ivanova-makhno-timoshenko-absorbingtwodimensionallyperiodicstructuresonnewplasmonicmaterials-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1007/s11141-019-09938-1\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'lerer-golovacheva-ivanova-makhno-timoshenko-absorbingtwodimensionallyperiodicstructuresonnewplasmonicmaterials-2019', 'https://doi.org/10.1007/s11141-019-09938-1', event);\">\n    Absorbing Two-Dimensionally Periodic Structures on New Plasmonic Materials.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Lerer, A. M.; Golovacheva, E. V.; Ivanova, I. N.; Makhno, V. V.;  and Timoshenko, P. E.\n</span>\n\n  \n\n</span>\n\n  <i>Radiophysics and Quantum Electronics</i>, 61(11): 801–805. April 2019.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1007/s11141-019-09938-1\"\n     onclick=\"log_download('lerer-golovacheva-ivanova-makhno-timoshenko-absorbingtwodimensionallyperiodicstructuresonnewplasmonicmaterials-2019', 'https://doi.org/10.1007/s11141-019-09938-1', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Absorbing Two-Dimensionally Periodic Structures on New Plasmonic Materials [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1007/s11141-019-09938-1\"\n     onclick=\"log_download('lerer-golovacheva-ivanova-makhno-timoshenko-absorbingtwodimensionallyperiodicstructuresonnewplasmonicmaterials-2019', 'http://doi.org/10.1007/s11141-019-09938-1', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/lerer-golovacheva-ivanova-makhno-timoshenko-absorbingtwodimensionallyperiodicstructuresonnewplasmonicmaterials-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('lerer-golovacheva-ivanova-makhno-timoshenko-absorbingtwodimensionallyperiodicstructuresonnewplasmonicmaterials-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{lerer_absorbing_2019,\n\ttitle = {Absorbing {Two}-{Dimensionally} {Periodic} {Structures} on {New} {Plasmonic} {Materials}},\n\tvolume = {61},\n\tissn = {1573-9120},\n\turl = {https://doi.org/10.1007/s11141-019-09938-1},\n\tdoi = {10.1007/s11141-019-09938-1},\n\tabstract = {We study theoretically two-dimensionally periodic gratings of plasmonic strips on substrates which contain dielectric and plasmonic layers. The developed electrodynamic model is based on solving the vector integro-differential equation of diffraction by three-dimensional dielectric bodies by the Galerkin method. It is shown that at the resonant frequencies of the surface plasmon polariton, these structures absorb almost 100\\% of the energy of the incident radiation in a wide wavelength range. The use of nonmetal plasmonic materials makes it possible to create a wideband absorber of infrared waves.},\n\tlanguage = {en},\n\tnumber = {11},\n\turldate = {2023-11-11},\n\tjournal = {Radiophysics and Quantum Electronics},\n\tauthor = {Lerer, A. M. and Golovacheva, E. V. and Ivanova, I. N. and Makhno, V. V. and Timoshenko, P. E.},\n\tmonth = apr,\n\tyear = {2019},\n\tpages = {801--805},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We study theoretically two-dimensionally periodic gratings of plasmonic strips on substrates which contain dielectric and plasmonic layers. The developed electrodynamic model is based on solving the vector integro-differential equation of diffraction by three-dimensional dielectric bodies by the Galerkin method. It is shown that at the resonant frequencies of the surface plasmon polariton, these structures absorb almost 100% of the energy of the incident radiation in a wide wavelength range. The use of nonmetal plasmonic materials makes it possible to create a wideband absorber of infrared waves.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"faddeev-kuriganova-leontev-smirnova-electrocatalyticpropertiesofrhcandptrhccatalystsfabricatedbythemethodofelectrochemicaldispersion-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1023193519030066\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'faddeev-kuriganova-leontev-smirnova-electrocatalyticpropertiesofrhcandptrhccatalystsfabricatedbythemethodofelectrochemicaldispersion-2019', 'https://doi.org/10.1134/S1023193519030066', event);\">\n    Electrocatalytic Properties of Rh/C and Pt-Rh/C Catalysts Fabricated by the Method of Electrochemical Dispersion.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Faddeev, N. A.; Kuriganova, A. B.; Leont′ev, I. N.;  and Smirnova, N. V.\n</span>\n\n  \n\n</span>\n\n  <i>Russian Journal of Electrochemistry</i>, 55(4): 346–350. April 2019.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1023193519030066\"\n     onclick=\"log_download('faddeev-kuriganova-leontev-smirnova-electrocatalyticpropertiesofrhcandptrhccatalystsfabricatedbythemethodofelectrochemicaldispersion-2019', 'https://doi.org/10.1134/S1023193519030066', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Electrocatalytic Properties of Rh/C and Pt-Rh/C Catalysts Fabricated by the Method of Electrochemical Dispersion [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1023193519030066\"\n     onclick=\"log_download('faddeev-kuriganova-leontev-smirnova-electrocatalyticpropertiesofrhcandptrhccatalystsfabricatedbythemethodofelectrochemicaldispersion-2019', 'http://doi.org/10.1134/S1023193519030066', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/faddeev-kuriganova-leontev-smirnova-electrocatalyticpropertiesofrhcandptrhccatalystsfabricatedbythemethodofelectrochemicaldispersion-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('faddeev-kuriganova-leontev-smirnova-electrocatalyticpropertiesofrhcandptrhccatalystsfabricatedbythemethodofelectrochemicaldispersion-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{faddeev_electrocatalytic_2019,\n\ttitle = {Electrocatalytic {Properties} of {Rh}/{C} and {Pt}-{Rh}/{C} {Catalysts} {Fabricated} by the {Method} of {Electrochemical} {Dispersion}},\n\tvolume = {55},\n\tissn = {1608-3342},\n\turl = {https://doi.org/10.1134/S1023193519030066},\n\tdoi = {10.1134/S1023193519030066},\n\tabstract = {The Pt/C, Rh/C, and Pt-Rh/C catalytic systems with uniform distribution of metal phase over the surface of carbon support and an average size of Pt and Rh nanoparticles of 7.3 and 6.5 nm, respectively, are fabricated by the method of electrochemical dispersion of metals in the aqueous electrolytes containing Na+. It is shown that the double-layer potential E = 300 mV (RHE) is the optimal potential of CO adsorption for determining the electrochemically active surface area of Pt/C, Rh/C, and Pt-Rh/C catalysts by the method of oxidative desorption of CO. The introduction of Rh into the Pt/C catalyst enables us to increase the specific activity and reduce the potential of the onset of methanol oxidation.},\n\tlanguage = {en},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Russian Journal of Electrochemistry},\n\tauthor = {Faddeev, N. A. and Kuriganova, A. B. and Leont′ev, I. N. and Smirnova, N. V.},\n\tmonth = apr,\n\tyear = {2019},\n\tkeywords = {electrochemical dispersion, fuel cell, electrocatalysis, platinum, rhodium},\n\tpages = {346--350},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The Pt/C, Rh/C, and Pt-Rh/C catalytic systems with uniform distribution of metal phase over the surface of carbon support and an average size of Pt and Rh nanoparticles of 7.3 and 6.5 nm, respectively, are fabricated by the method of electrochemical dispersion of metals in the aqueous electrolytes containing Na+. It is shown that the double-layer potential E = 300 mV (RHE) is the optimal potential of CO adsorption for determining the electrochemically active surface area of Pt/C, Rh/C, and Pt-Rh/C catalysts by the method of oxidative desorption of CO. The introduction of Rh into the Pt/C catalyst enables us to increase the specific activity and reduce the potential of the onset of methanol oxidation.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"southernfederaluniversity-leontiev-panich-southernfederaluniversity-smotrakov-southernfederaluniversity-fesenko-southernfederaluniversity-highpressurecontainerfortheresearchofphasetransitionsofferroelectricsundervariablehydrostaticpressureelectricfieldstrengthandtemperature-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://red.jfop.ru/jfop-1901-022029\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'southernfederaluniversity-leontiev-panich-southernfederaluniversity-smotrakov-southernfederaluniversity-fesenko-southernfederaluniversity-highpressurecontainerfortheresearchofphasetransitionsofferroelectricsundervariablehydrostaticpressureelectricfieldstrengthandtemperature-2019', 'http://red.jfop.ru/jfop-1901-022029', event);\">\n    High-pressure container for the research of phase transitions of ferroelectrics under variable hydrostatic pressure, electric field strength and temperature.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Southern Federal University; Leontiev, I.; Panich, A.; Southern Federal University; Smotrakov, V.; Southern Federal University; Fesenko, O.;  and Southern Federal University\n</span>\n\n  \n\n</span>\n\n  <i>Физические основы приборостроения</i>, 8(1): 22–29. March 2019.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://red.jfop.ru/jfop-1901-022029\"\n     onclick=\"log_download('southernfederaluniversity-leontiev-panich-southernfederaluniversity-smotrakov-southernfederaluniversity-fesenko-southernfederaluniversity-highpressurecontainerfortheresearchofphasetransitionsofferroelectricsundervariablehydrostaticpressureelectricfieldstrengthandtemperature-2019', 'http://red.jfop.ru/jfop-1901-022029', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"High-pressure container for the research of phase transitions of ferroelectrics under variable hydrostatic pressure, electric field strength and temperature [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.25210/jfop-1901-022029\"\n     onclick=\"log_download('southernfederaluniversity-leontiev-panich-southernfederaluniversity-smotrakov-southernfederaluniversity-fesenko-southernfederaluniversity-highpressurecontainerfortheresearchofphasetransitionsofferroelectricsundervariablehydrostaticpressureelectricfieldstrengthandtemperature-2019', 'http://doi.org/10.25210/jfop-1901-022029', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/southernfederaluniversity-leontiev-panich-southernfederaluniversity-smotrakov-southernfederaluniversity-fesenko-southernfederaluniversity-highpressurecontainerfortheresearchofphasetransitionsofferroelectricsundervariablehydrostaticpressureelectricfieldstrengthandtemperature-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('southernfederaluniversity-leontiev-panich-southernfederaluniversity-smotrakov-southernfederaluniversity-fesenko-southernfederaluniversity-highpressurecontainerfortheresearchofphasetransitionsofferroelectricsundervariablehydrostaticpressureelectricfieldstrengthandtemperature-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{southern_federal_university_high-pressure_2019,\n\ttitle = {High-pressure container for the research of phase transitions of ferroelectrics under variable hydrostatic pressure, electric field strength and temperature},\n\tvolume = {8},\n\tissn = {22254293},\n\turl = {http://red.jfop.ru/jfop-1901-022029},\n\tdoi = {10.25210/jfop-1901-022029},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Физические основы приборостроения},\n\tauthor = {{Southern Federal University} and Leontiev, I.N. and Panich, A.E. and {Southern Federal University} and Smotrakov, V.G. and {Southern Federal University} and Fesenko, O.E. and {Southern Federal University}},\n\tmonth = mar,\n\tyear = {2019},\n\tpages = {22--29},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"hanani-mezzane-amjoud-fourcade-razumnaya-lukyanchuk-goun-enhancementofdielectricpropertiesofleadfreebcztferroelectricceramicsbygrainsizeengineering-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0749603617323121\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'hanani-mezzane-amjoud-fourcade-razumnaya-lukyanchuk-goun-enhancementofdielectricpropertiesofleadfreebcztferroelectricceramicsbygrainsizeengineering-2019', 'https://www.sciencedirect.com/science/article/pii/S0749603617323121', event);\">\n    Enhancement of dielectric properties of lead-free BCZT ferroelectric ceramics by grain size engineering.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Hanani, Z.; Mezzane, D.; Amjoud, M.; Fourcade, S.; Razumnaya, A. G.; Luk'yanchuk, I. A.;  and Gouné, M.\n</span>\n\n  \n\n</span>\n\n  <i>Superlattices and Microstructures</i>, 127: 109–117. March 2019.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0749603617323121\"\n     onclick=\"log_download('hanani-mezzane-amjoud-fourcade-razumnaya-lukyanchuk-goun-enhancementofdielectricpropertiesofleadfreebcztferroelectricceramicsbygrainsizeengineering-2019', 'https://www.sciencedirect.com/science/article/pii/S0749603617323121', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Enhancement of dielectric properties of lead-free BCZT ferroelectric ceramics by grain size engineering [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.spmi.2018.03.004\"\n     onclick=\"log_download('hanani-mezzane-amjoud-fourcade-razumnaya-lukyanchuk-goun-enhancementofdielectricpropertiesofleadfreebcztferroelectricceramicsbygrainsizeengineering-2019', 'http://doi.org/10.1016/j.spmi.2018.03.004', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/hanani-mezzane-amjoud-fourcade-razumnaya-lukyanchuk-goun-enhancementofdielectricpropertiesofleadfreebcztferroelectricceramicsbygrainsizeengineering-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('hanani-mezzane-amjoud-fourcade-razumnaya-lukyanchuk-goun-enhancementofdielectricpropertiesofleadfreebcztferroelectricceramicsbygrainsizeengineering-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{hanani_enhancement_2019,\n\tseries = {Materials {Science} for {Green} {Energy} {Ifran} {City}},\n\ttitle = {Enhancement of dielectric properties of lead-free {BCZT} ferroelectric ceramics by grain size engineering},\n\tvolume = {127},\n\tissn = {0749-6036},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0749603617323121},\n\tdoi = {10.1016/j.spmi.2018.03.004},\n\tabstract = {Lead-free Ba0.85Ca0.15Ti0.9Zr0.1O3 (BCZT) ceramics had attracted much attention for the fabrication of microelectronic devices by virtue of their excellent dielectric, ferroelectric and piezoelectric properties. To understand the effects of both mean grain size and grain size distribution on the dielectric properties of lead-free Ba0.85Ca0.15Ti0.9Zr0.1O3 (BCZT) ferroelectric relaxors, an original method was proposed. It is based on the surfactant-assisted solvothermal processing coupled with low-temperature conventional sintering at 1250 °C. In this way, three highly dense BCZT with different mean grain size and dissimilar grain size distribution were designed. A significant increase of dielectric properties was obtained by a control of grain size and densification process. The dielectric constants measured were ranged from 5370 to 9646 and the dielectric loss was enhanced by 70\\%. Surprisingly, it was evidenced that there is unequivocal link between mean grain size with dielectric properties. Indeed, it was found that the presence of high density of refined grains leads to an improvement of dielectric properties due to an enhancement of densification. This work may provide a new strategy to design ferroelectric materials with enhanced properties.},\n\turldate = {2023-11-11},\n\tjournal = {Superlattices and Microstructures},\n\tauthor = {Hanani, Z. and Mezzane, D. and Amjoud, M. and Fourcade, S. and Razumnaya, A. G. and Luk&#x27;yanchuk, I. A. and Gouné, M.},\n\tmonth = mar,\n\tyear = {2019},\n\tkeywords = {BCZT, Dielectric, Ferroelectric, Lead-free, Microstructure, Relaxor},\n\tpages = {109--117},\n\tfile = {Принятая версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\ZTGFIZUV\\\\Hanani и др. - 2019 - Enhancement of dielectric properties of lead-free .pdf:application/pdf;ScienceDirect Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\AEC2RSBJ\\\\S0749603617323121.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Lead-free Ba0.85Ca0.15Ti0.9Zr0.1O3 (BCZT) ceramics had attracted much attention for the fabrication of microelectronic devices by virtue of their excellent dielectric, ferroelectric and piezoelectric properties. To understand the effects of both mean grain size and grain size distribution on the dielectric properties of lead-free Ba0.85Ca0.15Ti0.9Zr0.1O3 (BCZT) ferroelectric relaxors, an original method was proposed. It is based on the surfactant-assisted solvothermal processing coupled with low-temperature conventional sintering at 1250 °C. In this way, three highly dense BCZT with different mean grain size and dissimilar grain size distribution were designed. A significant increase of dielectric properties was obtained by a control of grain size and densification process. The dielectric constants measured were ranged from 5370 to 9646 and the dielectric loss was enhanced by 70%. Surprisingly, it was evidenced that there is unequivocal link between mean grain size with dielectric properties. Indeed, it was found that the presence of high density of refined grains leads to an improvement of dielectric properties due to an enhancement of densification. This work may provide a new strategy to design ferroelectric materials with enhanced properties.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"lukyanchuk-tikhonov-sen-razumnaya-vinokur-harnessingferroelectricdomainsfornegativecapacitance-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.nature.com/articles/s42005-019-0121-0\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'lukyanchuk-tikhonov-sen-razumnaya-vinokur-harnessingferroelectricdomainsfornegativecapacitance-2019', 'https://www.nature.com/articles/s42005-019-0121-0', event);\">\n    Harnessing ferroelectric domains for negative capacitance.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Luk’yanchuk, I.; Tikhonov, Y.; Sené, A.; Razumnaya, A.;  and Vinokur, V. M.\n</span>\n\n  \n\n</span>\n\n  <i>Communications Physics</i>, 2(1): 1–6. February 2019.\n  <span class=\"note\">Number: 1 Publisher: Nature Publishing Group</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.nature.com/articles/s42005-019-0121-0\"\n     onclick=\"log_download('lukyanchuk-tikhonov-sen-razumnaya-vinokur-harnessingferroelectricdomainsfornegativecapacitance-2019', 'https://www.nature.com/articles/s42005-019-0121-0', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Harnessing ferroelectric domains for negative capacitance [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1038/s42005-019-0121-0\"\n     onclick=\"log_download('lukyanchuk-tikhonov-sen-razumnaya-vinokur-harnessingferroelectricdomainsfornegativecapacitance-2019', 'http://doi.org/10.1038/s42005-019-0121-0', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/lukyanchuk-tikhonov-sen-razumnaya-vinokur-harnessingferroelectricdomainsfornegativecapacitance-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('lukyanchuk-tikhonov-sen-razumnaya-vinokur-harnessingferroelectricdomainsfornegativecapacitance-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{lukyanchuk_harnessing_2019,\n\ttitle = {Harnessing ferroelectric domains for negative capacitance},\n\tvolume = {2},\n\tcopyright = {2019 The Author(s)},\n\tissn = {2399-3650},\n\turl = {https://www.nature.com/articles/s42005-019-0121-0},\n\tdoi = {10.1038/s42005-019-0121-0},\n\tabstract = {A pressing quest for overcoming Boltzmann tyranny in low-power nanoscale electronics ignited an extensive search for the devices possessing the negative circuit constants. The emergent concept of the ferroelectric-based negative capacitance triggered then the explosive activity in the field. However, most of the research addressed transient negative capacitance, leaving the basic question of the existence of the steady-state negative capacitance unresolved. Here, we show that the ferroelectric nanodot capacitor hosts a stable two-domain state realizing the static reversible negative capacitance device thus opening routes for the extensive use of the negative capacitance in domain wall-based nanoelectronics.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Communications Physics},\n\tauthor = {Luk’yanchuk, I. and Tikhonov, Y. and Sené, A. and Razumnaya, A. and Vinokur, V. M.},\n\tmonth = feb,\n\tyear = {2019},\n\tnote = {Number: 1\nPublisher: Nature Publishing Group},\n\tkeywords = {Ferroelectrics and multiferroics, interfaces and thin films, Surfaces},\n\tpages = {1--6},\n\tfile = {Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\T4E6X2XN\\\\Luk’yanchuk и др. - 2019 - Harnessing ferroelectric domains for negative capa.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A pressing quest for overcoming Boltzmann tyranny in low-power nanoscale electronics ignited an extensive search for the devices possessing the negative circuit constants. The emergent concept of the ferroelectric-based negative capacitance triggered then the explosive activity in the field. However, most of the research addressed transient negative capacitance, leaving the basic question of the existence of the steady-state negative capacitance unresolved. Here, we show that the ferroelectric nanodot capacitor hosts a stable two-domain state realizing the static reversible negative capacitance device thus opening routes for the extensive use of the negative capacitance in domain wall-based nanoelectronics.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kocharian-gyulasaryan-estiphanos-avramenko-nelms-bernal-sharoyan-manukyan-ferromagnetismandgiantparamagnetismofcoppernanoparticlesincarbonmatrix-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://ieeexplore.ieee.org/document/8476555\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kocharian-gyulasaryan-estiphanos-avramenko-nelms-bernal-sharoyan-manukyan-ferromagnetismandgiantparamagnetismofcoppernanoparticlesincarbonmatrix-2019', 'https://ieeexplore.ieee.org/document/8476555', event);\">\n    Ferromagnetism and Giant Paramagnetism of Copper Nanoparticles in Carbon Matrix.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kocharian, A.; Gyulasaryan, H.; Estiphanos, M.; Avramenko, M.; Nelms, K.; Bernal, O.; Sharoyan, E.;  and Manukyan, A.\n</span>\n\n  \n\n</span>\n\n  <i>IEEE Transactions on Magnetics</i>, 55(2): 1–4. February 2019.\n  <span class=\"note\">Conference Name: IEEE Transactions on Magnetics</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://ieeexplore.ieee.org/document/8476555\"\n     onclick=\"log_download('kocharian-gyulasaryan-estiphanos-avramenko-nelms-bernal-sharoyan-manukyan-ferromagnetismandgiantparamagnetismofcoppernanoparticlesincarbonmatrix-2019', 'https://ieeexplore.ieee.org/document/8476555', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Ferromagnetism and Giant Paramagnetism of Copper Nanoparticles in Carbon Matrix [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1109/TMAG.2018.2862413\"\n     onclick=\"log_download('kocharian-gyulasaryan-estiphanos-avramenko-nelms-bernal-sharoyan-manukyan-ferromagnetismandgiantparamagnetismofcoppernanoparticlesincarbonmatrix-2019', 'http://doi.org/10.1109/TMAG.2018.2862413', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kocharian-gyulasaryan-estiphanos-avramenko-nelms-bernal-sharoyan-manukyan-ferromagnetismandgiantparamagnetismofcoppernanoparticlesincarbonmatrix-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kocharian-gyulasaryan-estiphanos-avramenko-nelms-bernal-sharoyan-manukyan-ferromagnetismandgiantparamagnetismofcoppernanoparticlesincarbonmatrix-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kocharian_ferromagnetism_2019,\n\ttitle = {Ferromagnetism and {Giant} {Paramagnetism} of {Copper} {Nanoparticles} in {Carbon} {Matrix}},\n\tvolume = {55},\n\tissn = {1941-0069},\n\turl = {https://ieeexplore.ieee.org/document/8476555},\n\tdoi = {10.1109/TMAG.2018.2862413},\n\tabstract = {Systematic X-ray diffraction, transmission electron microscopy (TEM), Raman and magnetic measurements were performed to study the structural and magnetic properties of copper nanoparticles (NPs) in carbon matrix. The weight concentration of Cu in carbon matrix is 8 wt\\%. The carbon-coated core-shell structures with bimodal size distribution with 4 and 300 nm average sizes of NPs are confirmed by scanning electron microscopy and TEM. Our results on magnetization carried out by vibrational magnetometer for copper NPs provide a strong evidence for coexistence of ferromagnetism and giant paramagnetism in wide range of temperature and magnetic field. The magnetic susceptibility at T = 10 K shows high value of giant paramagnetism with χ = 5×10-5 emu/gCuOe while ferromagnetic behavior with hysteresis is preserved up to the room temperature.},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {IEEE Transactions on Magnetics},\n\tauthor = {Kocharian, Armen and Gyulasaryan, Harutyun and Estiphanos, Medhanie and Avramenko, Marina and Nelms, Katherine and Bernal, Oscar and Sharoyan, Eduard and Manukyan, Aram},\n\tmonth = feb,\n\tyear = {2019},\n\tnote = {Conference Name: IEEE Transactions on Magnetics},\n\tpages = {1--4},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\DCWF2WPV\\\\Kocharian и др. - 2019 - Ferromagnetism and Giant Paramagnetism of Copper N.pdf:application/pdf;IEEE Xplore Abstract Record:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\CA3E5JSV\\\\8476555.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Systematic X-ray diffraction, transmission electron microscopy (TEM), Raman and magnetic measurements were performed to study the structural and magnetic properties of copper nanoparticles (NPs) in carbon matrix. The weight concentration of Cu in carbon matrix is 8 wt%. The carbon-coated core-shell structures with bimodal size distribution with 4 and 300 nm average sizes of NPs are confirmed by scanning electron microscopy and TEM. Our results on magnetization carried out by vibrational magnetometer for copper NPs provide a strong evidence for coexistence of ferromagnetism and giant paramagnetism in wide range of temperature and magnetic field. The magnetic susceptibility at T = 10 K shows high value of giant paramagnetism with χ = 5×10-5 emu/gCuOe while ferromagnetic behavior with hysteresis is preserved up to the room temperature.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"andronikova-bronwald-leontiev-leontiev-chernyshov-filimonov-vakhrushev-incommensurateinstabilityanddiffusescatteringatbrillouinzoneboundaryinzrrichleadzirconatetitanate-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/00150193.2019.1569987\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'andronikova-bronwald-leontiev-leontiev-chernyshov-filimonov-vakhrushev-incommensurateinstabilityanddiffusescatteringatbrillouinzoneboundaryinzrrichleadzirconatetitanate-2019', 'https://doi.org/10.1080/00150193.2019.1569987', event);\">\n    Incommensurate instability and diffuse scattering at Brillouin zone boundary in Zr-rich lead zirconate titanate.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Andronikova, D. A.; Bronwald, I. A.; Leontiev, I. N.; Leontiev, N. G.; Chernyshov, D. Y.; Filimonov, A. V.;  and Vakhrushev, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 538(1): 65–73. January 2019.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2019.1569987</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/00150193.2019.1569987\"\n     onclick=\"log_download('andronikova-bronwald-leontiev-leontiev-chernyshov-filimonov-vakhrushev-incommensurateinstabilityanddiffusescatteringatbrillouinzoneboundaryinzrrichleadzirconatetitanate-2019', 'https://doi.org/10.1080/00150193.2019.1569987', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Incommensurate instability and diffuse scattering at Brillouin zone boundary in Zr-rich lead zirconate titanate [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150193.2019.1569987\"\n     onclick=\"log_download('andronikova-bronwald-leontiev-leontiev-chernyshov-filimonov-vakhrushev-incommensurateinstabilityanddiffusescatteringatbrillouinzoneboundaryinzrrichleadzirconatetitanate-2019', 'http://doi.org/10.1080/00150193.2019.1569987', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/andronikova-bronwald-leontiev-leontiev-chernyshov-filimonov-vakhrushev-incommensurateinstabilityanddiffusescatteringatbrillouinzoneboundaryinzrrichleadzirconatetitanate-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('andronikova-bronwald-leontiev-leontiev-chernyshov-filimonov-vakhrushev-incommensurateinstabilityanddiffusescatteringatbrillouinzoneboundaryinzrrichleadzirconatetitanate-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{andronikova_incommensurate_2019,\n\ttitle = {Incommensurate instability and diffuse scattering at {Brillouin} zone boundary in {Zr}-rich lead zirconate titanate},\n\tvolume = {538},\n\tissn = {0015-0193},\n\turl = {https://doi.org/10.1080/00150193.2019.1569987},\n\tdoi = {10.1080/00150193.2019.1569987},\n\tabstract = {Detailed study of the X-ray diffuse scattering in the paraelectric phase of the PbZr0.985Ti0.015O3 was carried out. We concentrated on the analysis of the scattering peculiarities in the vicinities of M- and R- points of the Brillouin zone. We have observed a critical increase of the diffuse scattering at the position Q ≈ (0.47 + h 0.53 + k l) slightly aside of M point on cooling to the intermediate phase. We attribute observed critical scattering to a mixed mode containing both oxygen octahedral tilts and antiparallel cationic displacements. Tentative conclusion is made describing earlier reported complicated set of the satellite peaks around M-point as the result of the soft-mode driven incommensurate phase transition.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Ferroelectrics},\n\tauthor = {Andronikova, D. A. and Bronwald, Iu. A. and Leontiev, I. N. and Leontiev, N. G. and Chernyshov, D. Yu. and Filimonov, A. V. and Vakhrushev, S. B.},\n\tmonth = jan,\n\tyear = {2019},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/00150193.2019.1569987},\n\tkeywords = {phase transitions, diffuse scattering, Ferroelectricity},\n\tpages = {65--73},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Detailed study of the X-ray diffuse scattering in the paraelectric phase of the PbZr0.985Ti0.015O3 was carried out. We concentrated on the analysis of the scattering peculiarities in the vicinities of M- and R- points of the Brillouin zone. We have observed a critical increase of the diffuse scattering at the position Q ≈ (0.47 + h 0.53 + k l) slightly aside of M point on cooling to the intermediate phase. We attribute observed critical scattering to a mixed mode containing both oxygen octahedral tilts and antiparallel cationic displacements. Tentative conclusion is made describing earlier reported complicated set of the satellite peaks around M-point as the result of the soft-mode driven incommensurate phase transition.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kuriganova-faddeev-leontyev-allix-rakhmatullin-smirnova-newelectrochemicalapproachforthesynthesisofpdpdocelectrocatalystandapplicationtoformicacidelectrooxidation-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201901628\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kuriganova-faddeev-leontyev-allix-rakhmatullin-smirnova-newelectrochemicalapproachforthesynthesisofpdpdocelectrocatalystandapplicationtoformicacidelectrooxidation-2019', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201901628', event);\">\n    New Electrochemical Approach for the Synthesis of Pd-PdO/C Electrocatalyst and Application to Formic Acid Electrooxidation.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kuriganova, A. B.; Faddeev, N. A.; Leontyev, I. N.; Allix, M.; Rakhmatullin, A.;  and Smirnova, N. V.\n</span>\n\n  \n\n</span>\n\n  <i>ChemistrySelect</i>, 4(29): 8390–8393.  2019.\n  <span class=\"note\">_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/slct.201901628</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201901628\"\n     onclick=\"log_download('kuriganova-faddeev-leontyev-allix-rakhmatullin-smirnova-newelectrochemicalapproachforthesynthesisofpdpdocelectrocatalystandapplicationtoformicacidelectrooxidation-2019', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201901628', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"New Electrochemical Approach for the Synthesis of Pd-PdO/C Electrocatalyst and Application to Formic Acid Electrooxidation [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1002/slct.201901628\"\n     onclick=\"log_download('kuriganova-faddeev-leontyev-allix-rakhmatullin-smirnova-newelectrochemicalapproachforthesynthesisofpdpdocelectrocatalystandapplicationtoformicacidelectrooxidation-2019', 'http://doi.org/10.1002/slct.201901628', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kuriganova-faddeev-leontyev-allix-rakhmatullin-smirnova-newelectrochemicalapproachforthesynthesisofpdpdocelectrocatalystandapplicationtoformicacidelectrooxidation-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kuriganova-faddeev-leontyev-allix-rakhmatullin-smirnova-newelectrochemicalapproachforthesynthesisofpdpdocelectrocatalystandapplicationtoformicacidelectrooxidation-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kuriganova_new_2019,\n\ttitle = {New {Electrochemical} {Approach} for the {Synthesis} of {Pd}-{PdO}/{C} {Electrocatalyst} and {Application} to {Formic} {Acid} {Electrooxidation}},\n\tvolume = {4},\n\tcopyright = {© 2019 Wiley-VCH Verlag GmbH \\&amp; Co. KGaA, Weinheim},\n\tissn = {2365-6549},\n\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201901628},\n\tdoi = {10.1002/slct.201901628},\n\tabstract = {Pd-PdO/C catalyst for formic acid electrooxidation has been synthesized via electrochemical dispersion of Pd foil electrodes under pulse alternating current conditions in NaCl aqueous electrolyte. About 35 wt\\% of the as-prepared Pd-PdO/C specimen is PdO as revealed by X-ray diffraction. The microstructural characteristics and catalytic activity of the synthesized Pd/C catalyst have been compared with those of a Pt/C catalyst prepared under the same conditions. Pd nanoparticles of Pd-PdO/C catalyst exhibit smaller average dimensions and narrower particle size distribution – 7.4±0.5 nm and 1.9±0.5 respectively for Pd and PdO particles. The process of ethanol electrooxidation on the catalyst was characterized by high overvoltage (up to 800 mV). The overvoltage of the formic acid electrochemical oxidation on Pd/C is 590 mV less than on Pt/C.},\n\tlanguage = {en},\n\tnumber = {29},\n\turldate = {2023-11-11},\n\tjournal = {ChemistrySelect},\n\tauthor = {Kuriganova, Alexandra B. and Faddeev, Nikita A. and Leontyev, Igor N. and Allix, Mathieu and Rakhmatullin, Aydar and Smirnova, Nina V.},\n\tyear = {2019},\n\tnote = {\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/slct.201901628},\n\tkeywords = {alternating current, electrochemical dispersion, formic acid, fuel cell, Pd/C},\n\tpages = {8390--8393},\n\tfile = {Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\QME9WT8N\\\\slct.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Pd-PdO/C catalyst for formic acid electrooxidation has been synthesized via electrochemical dispersion of Pd foil electrodes under pulse alternating current conditions in NaCl aqueous electrolyte. About 35 wt% of the as-prepared Pd-PdO/C specimen is PdO as revealed by X-ray diffraction. The microstructural characteristics and catalytic activity of the synthesized Pd/C catalyst have been compared with those of a Pt/C catalyst prepared under the same conditions. Pd nanoparticles of Pd-PdO/C catalyst exhibit smaller average dimensions and narrower particle size distribution – 7.4±0.5 nm and 1.9±0.5 respectively for Pd and PdO particles. The process of ethanol electrooxidation on the catalyst was characterized by high overvoltage (up to 800 mV). The overvoltage of the formic acid electrochemical oxidation on Pd/C is 590 mV less than on Pt/C.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"pimonov-konevtsova-rochal-anomaloussmallviralshellsandsimplestpolyhedrawithicosahedralsymmetrytherhombictriacontahedroncase-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.iucr.org/a/issues/2019/01/00/eo5089/\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'pimonov-konevtsova-rochal-anomaloussmallviralshellsandsimplestpolyhedrawithicosahedralsymmetrytherhombictriacontahedroncase-2019', 'https://journals.iucr.org/a/issues/2019/01/00/eo5089/', event);\">\n    Anomalous small viral shells and simplest polyhedra with icosahedral symmetry: the rhombic triacontahedron case.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Pimonov, V. V.; Konevtsova, O. V.;  and Rochal, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Acta Crystallographica Section A: Foundations and Advances</i>, 75(1): 135–141. January 2019.\n  <span class=\"note\">Number: 1 Publisher: International Union of Crystallography</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.iucr.org/a/issues/2019/01/00/eo5089/\"\n     onclick=\"log_download('pimonov-konevtsova-rochal-anomaloussmallviralshellsandsimplestpolyhedrawithicosahedralsymmetrytherhombictriacontahedroncase-2019', 'https://journals.iucr.org/a/issues/2019/01/00/eo5089/', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Anomalous small viral shells and simplest polyhedra with icosahedral symmetry: the rhombic triacontahedron case [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1107/S2053273318015656\"\n     onclick=\"log_download('pimonov-konevtsova-rochal-anomaloussmallviralshellsandsimplestpolyhedrawithicosahedralsymmetrytherhombictriacontahedroncase-2019', 'http://doi.org/10.1107/S2053273318015656', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/pimonov-konevtsova-rochal-anomaloussmallviralshellsandsimplestpolyhedrawithicosahedralsymmetrytherhombictriacontahedroncase-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('pimonov-konevtsova-rochal-anomaloussmallviralshellsandsimplestpolyhedrawithicosahedralsymmetrytherhombictriacontahedroncase-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{pimonov_anomalous_2019,\n\ttitle = {Anomalous small viral shells and simplest polyhedra with icosahedral symmetry: the rhombic triacontahedron case},\n\tvolume = {75},\n\tcopyright = {Copyright (c) 2019 International Union of Crystallography},\n\tissn = {2053-2733},\n\tshorttitle = {Anomalous small viral shells and simplest polyhedra with icosahedral symmetry},\n\turl = {https://journals.iucr.org/a/issues/2019/01/00/eo5089/},\n\tdoi = {10.1107/S2053273318015656},\n\tabstract = {The symmetry of the capsomers forming a viral shell determines the polyhedron underlying the shell structure. If the capsid is self-assembled from dimers, this is the rhombic triacontahedron with 30 equivalent rhombic faces.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Acta Crystallographica Section A: Foundations and Advances},\n\tauthor = {Pimonov, V. V. and Konevtsova, O. V. and Rochal, S. B.},\n\tmonth = jan,\n\tyear = {2019},\n\tnote = {Number: 1\nPublisher: International Union of Crystallography},\n\tpages = {135--141},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The symmetry of the capsomers forming a viral shell determines the polyhedron underlying the shell structure. If the capsid is self-assembled from dimers, this is the rhombic triacontahedron with 30 equivalent rhombic faces.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/47244\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---2019', 'https://journals.ioffe.ru/articles/47244', event);\">\n    Тепловые флуктуации и резонансные свойства сканирующих зондов на основе углеродных нанотрубок.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Чалин, Д.;  and Авраменко, М.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 61(3): 514.  2019.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/47244\"\n     onclick=\"log_download('---2019', 'https://journals.ioffe.ru/articles/47244', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Тепловые флуктуации и резонансные свойства сканирующих зондов на основе углеродных нанотрубок [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.21883/FTT.2019.03.47244.237\"\n     onclick=\"log_download('---2019', 'http://doi.org/10.21883/FTT.2019.03.47244.237', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2019,\n\ttitle = {Тепловые флуктуации и резонансные свойства сканирующих зондов на основе углеродных нанотрубок},\n\tvolume = {61},\n\tissn = {0367-3294},\n\turl = {https://journals.ioffe.ru/articles/47244},\n\tdoi = {10.21883/FTT.2019.03.47244.237},\n\tabstract = {AbstractThe design of cantilevers and microelectromechanical systems based on carbon nanotubes necessitates a thorough study of their thermal fluctuations and resonance properties. This work aims at the simulation of thermal fluctuations and power spectral density for single-walled carbon nanotubes in the context of the continuous model of elastic cylindrical membranes with nonmacroscopic thicknesses. The conditions imposed on the geometry of this probe and providing its stable operation, as well as the high lateral resolution determined by only the radius of the nanotube independently on its thermal vibrations, are found, as well. The most intensive resonance modes, making the greatest contribution to the thermal fluctuations of carbon nanotubes, are established, and their frequencies are found analytically.\n          , \n            Проектирование кантилеверов и микроэлектромеханических систем с использованием углеродных нанотрубок неразрывно связано с изучением их тепловых флуктуаций и резонансных свойств. В настоящей работе для одностенных углеродных нанотрубок производится расчет тепловых флуктуаций и спектральной плотности интенсивности колебаний в рамках континуальной модели упругих цилиндрических мембран, не обладающих макроскопической толщиной. Найдены налагаемые на геометрию такого зонда условия, выполнение которых обеспечивает как стабильность его работы, так и высокое латеральное разрешение, определяющееся только радиусом нанотрубки и не зависящее от величины ее тепловых колебаний. Определены самые интенсивные резонансные моды, дающие наибольший вклад в тепловые флуктуации углеродных нанотрубок, а также получено аналитическое выражение для их частот.},\n\tlanguage = {ru},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Чалин, Д.В. and Авраменко, М.В.},\n\tyear = {2019},\n\tpages = {514},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\GE9CNIBE\\\\Чалин и Авраменко - 2019 - Тепловые флуктуации и резонансные свойства сканиру.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  AbstractThe design of cantilevers and microelectromechanical systems based on carbon nanotubes necessitates a thorough study of their thermal fluctuations and resonance properties. This work aims at the simulation of thermal fluctuations and power spectral density for single-walled carbon nanotubes in the context of the continuous model of elastic cylindrical membranes with nonmacroscopic thicknesses. The conditions imposed on the geometry of this probe and providing its stable operation, as well as the high lateral resolution determined by only the radius of the nanotube independently on its thermal vibrations, are found, as well. The most intensive resonance modes, making the greatest contribution to the thermal fluctuations of carbon nanotubes, are established, and their frequencies are found analytically. , Проектирование кантилеверов и микроэлектромеханических систем с использованием углеродных нанотрубок неразрывно связано с изучением их тепловых флуктуаций и резонансных свойств. В настоящей работе для одностенных углеродных нанотрубок производится расчет тепловых флуктуаций и спектральной плотности интенсивности колебаний в рамках континуальной модели упругих цилиндрических мембран, не обладающих макроскопической толщиной. Найдены налагаемые на геометрию такого зонда условия, выполнение которых обеспечивает как стабильность его работы, так и высокое латеральное разрешение, определяющееся только радиусом нанотрубки и не зависящее от величины ее тепловых колебаний. Определены самые интенсивные резонансные моды, дающие наибольший вклад в тепловые флуктуации углеродных нанотрубок, а также получено аналитическое выражение для их частот.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"--2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=39552125\"\n     onclick=\"return trackOutboundLink('publications', 'click', '--2019', 'https://elibrary.ru/item.asp?id=39552125', event);\">\n    Сферические упаковки в оболочках вирусов, эпителиальных монослоях и коллоидных кристаллах.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Рошаль, Д. С.\n</span>\n\n  \n\n</span>\n\n  In <i>Материалы XVI Международной конференции, посвященной 80-летию со дня рождения профессора Мишеля Деза</i>, pages 2, Тула,  2019. Тульский государственный педагогический университет им. Л.Н. Толстого\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=39552125\"\n     onclick=\"log_download('--2019', 'https://elibrary.ru/item.asp?id=39552125', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Сферические упаковки в оболочках вирусов, эпителиальных монослоях и коллоидных кристаллах [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/--2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>1 download</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('--2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{__2019-1,\n\taddress = {Тула},\n\ttitle = {Сферические упаковки в оболочках вирусов, эпителиальных монослоях и коллоидных кристаллах},\n\tshorttitle = {Алгебра, теория чисел и дискретная геометрия},\n\turl = {https://elibrary.ru/item.asp?id=39552125},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tbooktitle = {Материалы {XVI} Международной конференции,  посвященной 80-летию со дня рождения  профессора Мишеля Деза},\n\tpublisher = {Тульский государственный педагогический университет им. Л.Н. Толстого},\n\tauthor = {Рошаль, Д. С.},\n\tyear = {2019},\n\tpages = {2},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=39539483\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------2019', 'https://elibrary.ru/item.asp?id=39539483', event);\">\n    Оптические свойства фотонных кристаллов на основе наностержней оксида цинка, покрытых тонкой пленкой плазмонного материала.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Лерер, А. М.; Тимошенко, П. Е.; Головачева, Е. В.; Кайдашев, Е. М.;  and Турчин, А. С.\n</span>\n\n  \n\n</span>\n\n  <i>Электроника И Микроэлектроника Свч</i>, 1: 209–213.  2019.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=39539483\"\n     onclick=\"log_download('------2019', 'https://elibrary.ru/item.asp?id=39539483', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Оптические свойства фотонных кристаллов на основе наностержней оксида цинка, покрытых тонкой пленкой плазмонного материала [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2019-2,\n\ttitle = {Оптические свойства фотонных кристаллов на основе наностержней оксида цинка, покрытых тонкой пленкой плазмонного материала},\n\tvolume = {1},\n\turl = {https://elibrary.ru/item.asp?id=39539483},\n\tabstract = {В данной работе исследовались зависимости оптических свойств фотонных кристаллов, представляющих двумерно-периодическую решетку наностержней оксида цинка от геометрических параметров и типов их тонкопленочного покрытия плазмонными материалами (Au, Ag, Cu, AZO, GZO, AGZO и т. п.). В расчетах учтены свойства металлов и диэлектриков в оптическом диапазоне. Характеристики двухмерно-периодических структур, образованных бесконечно длинными слоистыми цилиндрами на основе ZnO, рассчитаны методом разделения переменных в цилиндрической системе координат. Проведено сравнение полученных численных данных с результатами конечноэлементного моделирования.},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tjournal = {Электроника И Микроэлектроника Свч},\n\tauthor = {Лерер, А. М. and Тимошенко, П. Е. and Головачева, Е. В. and Кайдашев, Е. М. and Турчин, А. С.},\n\tyear = {2019},\n\tkeywords = {Дифракция, Наностержни, Оксид Цинка, Оптические Наноантенны, Оптические Свойства, Плазмон-Поляритон, Плазмонный Резонанс, Фотонная Запрещенная Зона, Фотонный Кристалл, ⛔ No DOI found},\n\tpages = {209--213},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  В данной работе исследовались зависимости оптических свойств фотонных кристаллов, представляющих двумерно-периодическую решетку наностержней оксида цинка от геометрических параметров и типов их тонкопленочного покрытия плазмонными материалами (Au, Ag, Cu, AZO, GZO, AGZO и т. п.). В расчетах учтены свойства металлов и диэлектриков в оптическом диапазоне. Характеристики двухмерно-периодических структур, образованных бесконечно длинными слоистыми цилиндрами на основе ZnO, рассчитаны методом разделения переменных в цилиндрической системе координат. Проведено сравнение полученных численных данных с результатами конечноэлементного моделирования.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"ahmed-alyabyeva-torgashev-prokhorov-vinnik-dressel-gorshunov-effectofaluminiumsubstitutiononlowenergyelectrodynamicsofbariumleadmtypehexagonalferrites-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/1389/1/012044\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'ahmed-alyabyeva-torgashev-prokhorov-vinnik-dressel-gorshunov-effectofaluminiumsubstitutiononlowenergyelectrodynamicsofbariumleadmtypehexagonalferrites-2019', 'https://dx.doi.org/10.1088/1742-6596/1389/1/012044', event);\">\n    Effect of aluminium substitution on low energy electrodynamics of barium-lead M-type hexagonal ferrites.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Ahmed, A.; Alyabyeva, L.; Torgashev, V.; Prokhorov, A. S.; Vinnik, D.; Dressel, M.;  and Gorshunov, B.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics: Conference Series</i>, 1389(1): 012044. November 2019.\n  <span class=\"note\">Publisher: IOP Publishing</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/1389/1/012044\"\n     onclick=\"log_download('ahmed-alyabyeva-torgashev-prokhorov-vinnik-dressel-gorshunov-effectofaluminiumsubstitutiononlowenergyelectrodynamicsofbariumleadmtypehexagonalferrites-2019', 'https://dx.doi.org/10.1088/1742-6596/1389/1/012044', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Effect of aluminium substitution on low energy electrodynamics of barium-lead M-type hexagonal ferrites [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/1742-6596/1389/1/012044\"\n     onclick=\"log_download('ahmed-alyabyeva-torgashev-prokhorov-vinnik-dressel-gorshunov-effectofaluminiumsubstitutiononlowenergyelectrodynamicsofbariumleadmtypehexagonalferrites-2019', 'http://doi.org/10.1088/1742-6596/1389/1/012044', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/ahmed-alyabyeva-torgashev-prokhorov-vinnik-dressel-gorshunov-effectofaluminiumsubstitutiononlowenergyelectrodynamicsofbariumleadmtypehexagonalferrites-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('ahmed-alyabyeva-torgashev-prokhorov-vinnik-dressel-gorshunov-effectofaluminiumsubstitutiononlowenergyelectrodynamicsofbariumleadmtypehexagonalferrites-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{ahmed_effect_2019,\n\ttitle = {Effect of aluminium substitution on low energy electrodynamics of barium-lead {M}-type hexagonal ferrites},\n\tvolume = {1389},\n\tissn = {1742-6596},\n\turl = {https://dx.doi.org/10.1088/1742-6596/1389/1/012044},\n\tdoi = {10.1088/1742-6596/1389/1/012044},\n\tabstract = {We present the first detailed study of the terahertz-infrared dielectric response of single crystalline lead-substituted M-type barium hexaferrites doped with Al3+. The broadband spectra of complex dielectric permittivity ε*(v)=ε’(v)+iε&quot;(v) of Ba0.8Pb0.2AlxFe12-xO19 with concentrations of the dopant x(Al)=1.2, 3, 3.3 are obtained for two principle polarizations using Fourier-transform infrared spectroscopy and terahertz time-domain spectroscopy in the temperature range from 4 to 300 K and at frequencies from 10 cm−1 up to 8000 cm−1. We observe a rich set of excitations and assign them to the electronic transitions within the ground state 5E of the 4-fold coordinated divalent iron and to phonon resonances. Effect of Al3+ cation substitution on low energy (terahertz) dielectric response and infrared phonon spectra of barium-lead M-type hexaferrites is analysed and discussed.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics: Conference Series},\n\tauthor = {Ahmed, Asmaa and Alyabyeva, Liudmila and Torgashev, Victor and Prokhorov, Anatoly S. and Vinnik, Denis and Dressel, Martin and Gorshunov, Boris},\n\tmonth = nov,\n\tyear = {2019},\n\tnote = {Publisher: IOP Publishing},\n\tpages = {012044},\n\tfile = {IOP Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\F2HHUAX3\\\\Ahmed и др. - 2019 - Effect of aluminium substitution on low energy ele.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We present the first detailed study of the terahertz-infrared dielectric response of single crystalline lead-substituted M-type barium hexaferrites doped with Al3+. The broadband spectra of complex dielectric permittivity ε*(v)=ε’(v)+iε\"(v) of Ba0.8Pb0.2AlxFe12-xO19 with concentrations of the dopant x(Al)=1.2, 3, 3.3 are obtained for two principle polarizations using Fourier-transform infrared spectroscopy and terahertz time-domain spectroscopy in the temperature range from 4 to 300 K and at frequencies from 10 cm−1 up to 8000 cm−1. We observe a rich set of excitations and assign them to the electronic transitions within the ground state 5E of the 4-fold coordinated divalent iron and to phonon resonances. Effect of Al3+ cation substitution on low energy (terahertz) dielectric response and infrared phonon spectra of barium-lead M-type hexaferrites is analysed and discussed.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"mukhortov-golovko-anokhin-stryukov-biryukov-timoshenko-structurelatticedynamicspropertiesofbismuthtitanateheterostructures-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/1361-6463/ab4bf6\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'mukhortov-golovko-anokhin-stryukov-biryukov-timoshenko-structurelatticedynamicspropertiesofbismuthtitanateheterostructures-2019', 'https://dx.doi.org/10.1088/1361-6463/ab4bf6', event);\">\n    Structure, lattice dynamics, properties of bismuth titanate heterostructures.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Mukhortov, V. M.; Golovko, Y. I.; Anokhin, A. S.; Stryukov, D. V.; Biryukov, S. V.;  and Timoshenko, P. E.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics D: Applied Physics</i>, 53(3): 035304. November 2019.\n  <span class=\"note\">Publisher: IOP Publishing</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/1361-6463/ab4bf6\"\n     onclick=\"log_download('mukhortov-golovko-anokhin-stryukov-biryukov-timoshenko-structurelatticedynamicspropertiesofbismuthtitanateheterostructures-2019', 'https://dx.doi.org/10.1088/1361-6463/ab4bf6', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Structure, lattice dynamics, properties of bismuth titanate heterostructures [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/1361-6463/ab4bf6\"\n     onclick=\"log_download('mukhortov-golovko-anokhin-stryukov-biryukov-timoshenko-structurelatticedynamicspropertiesofbismuthtitanateheterostructures-2019', 'http://doi.org/10.1088/1361-6463/ab4bf6', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/mukhortov-golovko-anokhin-stryukov-biryukov-timoshenko-structurelatticedynamicspropertiesofbismuthtitanateheterostructures-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('mukhortov-golovko-anokhin-stryukov-biryukov-timoshenko-structurelatticedynamicspropertiesofbismuthtitanateheterostructures-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{mukhortov_structure_2019,\n\ttitle = {Structure, lattice dynamics, properties of bismuth titanate heterostructures},\n\tvolume = {53},\n\tissn = {0022-3727},\n\turl = {https://dx.doi.org/10.1088/1361-6463/ab4bf6},\n\tdoi = {10.1088/1361-6463/ab4bf6},\n\tabstract = {We investigated the epitaxial Bi4Ti3O12 (BTO) thin films with different thicknesses on a (0 0 1) MgO substrate with a Ba0.4Sr0.6TiO3 buffer layer (4 nm). The crystallographic axis [1 0 0] of Bi4Ti3O12 film is rotated on degrees relative to [1 0 0] MgO axis. When the thickness of Bi4Ti3O12 film is less than 40 nm, the unit cell of the film is compressed in the normal to the interface plane direction. In cases of large film thicknesses, the sign of strain changes and correspondingly the unit cell is stretched. Switched spontaneous polarization in the interface plane with 180° domain structure occurs at 10 nm film thickness and increases with a thickness up to 55 C cm−2. Changes in the Raman spectra of the Bi4Ti3O12 films indicates to increase of monoclinic distortion of the film unit cell in comparison with the bulk unit cell. The anisotropy of in-plane dielectric properties and the effect of internal strain on dielectric properties for the Bi4Ti3O12 films are confirmed by the study of the dielectric characteristics of the films.},\n\tlanguage = {en},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics D: Applied Physics},\n\tauthor = {Mukhortov, V. M. and Golovko, Yu I. and Anokhin, A. S. and Stryukov, D. V. and Biryukov, S. V. and Timoshenko, P. E.},\n\tmonth = nov,\n\tyear = {2019},\n\tnote = {Publisher: IOP Publishing},\n\tpages = {035304},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We investigated the epitaxial Bi4Ti3O12 (BTO) thin films with different thicknesses on a (0 0 1) MgO substrate with a Ba0.4Sr0.6TiO3 buffer layer (4 nm). The crystallographic axis [1 0 0] of Bi4Ti3O12 film is rotated on degrees relative to [1 0 0] MgO axis. When the thickness of Bi4Ti3O12 film is less than 40 nm, the unit cell of the film is compressed in the normal to the interface plane direction. In cases of large film thicknesses, the sign of strain changes and correspondingly the unit cell is stretched. Switched spontaneous polarization in the interface plane with 180° domain structure occurs at 10 nm film thickness and increases with a thickness up to 55 C cm−2. Changes in the Raman spectra of the Bi4Ti3O12 films indicates to increase of monoclinic distortion of the film unit cell in comparison with the bulk unit cell. The anisotropy of in-plane dielectric properties and the effect of internal strain on dielectric properties for the Bi4Ti3O12 films are confirmed by the study of the dielectric characteristics of the films.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"yegiyan-alyabyeva-torgashev-vinnik-gudkova-prokhorov-dressel-gorshunov-terahertzinfraredspectroscopyofsinglecrystallinemtypehexaferritebatitextrmxfetextrm12xotextrm19-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/1389/1/012038\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'yegiyan-alyabyeva-torgashev-vinnik-gudkova-prokhorov-dressel-gorshunov-terahertzinfraredspectroscopyofsinglecrystallinemtypehexaferritebatitextrmxfetextrm12xotextrm19-2019', 'https://dx.doi.org/10.1088/1742-6596/1389/1/012038', event);\">\n    Terahertz-infrared spectroscopy of single crystalline m-type hexaferrite BaTi$_{\\textrm{x}}$Fe$_{\\textrm{12-x}}$O$_{\\textrm{19}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Yegiyan, S. R.; Alyabyeva, L. N.; Torgashev, V. I.; Vinnik, D. A.; Gudkova, S. A.; Prokhorov, A. S.; Dressel, M.;  and Gorshunov, B. P.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics: Conference Series</i>, 1389(1): 012038. November 2019.\n  <span class=\"note\">Publisher: IOP Publishing</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/1389/1/012038\"\n     onclick=\"log_download('yegiyan-alyabyeva-torgashev-vinnik-gudkova-prokhorov-dressel-gorshunov-terahertzinfraredspectroscopyofsinglecrystallinemtypehexaferritebatitextrmxfetextrm12xotextrm19-2019', 'https://dx.doi.org/10.1088/1742-6596/1389/1/012038', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Terahertz-infrared spectroscopy of single crystalline m-type hexaferrite BaTi$_{\\textrm{x}}$Fe$_{\\textrm{12-x}}$O$_{\\textrm{19}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/1742-6596/1389/1/012038\"\n     onclick=\"log_download('yegiyan-alyabyeva-torgashev-vinnik-gudkova-prokhorov-dressel-gorshunov-terahertzinfraredspectroscopyofsinglecrystallinemtypehexaferritebatitextrmxfetextrm12xotextrm19-2019', 'http://doi.org/10.1088/1742-6596/1389/1/012038', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/yegiyan-alyabyeva-torgashev-vinnik-gudkova-prokhorov-dressel-gorshunov-terahertzinfraredspectroscopyofsinglecrystallinemtypehexaferritebatitextrmxfetextrm12xotextrm19-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('yegiyan-alyabyeva-torgashev-vinnik-gudkova-prokhorov-dressel-gorshunov-terahertzinfraredspectroscopyofsinglecrystallinemtypehexaferritebatitextrmxfetextrm12xotextrm19-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{yegiyan_terahertz-infrared_2019,\n\ttitle = {Terahertz-infrared spectroscopy of single crystalline m-type hexaferrite {BaTi}$_{\\textrm{x}}${Fe}$_{\\textrm{12-x}}${O}$_{\\textrm{19}}$},\n\tvolume = {1389},\n\tissn = {1742-6596},\n\turl = {https://dx.doi.org/10.1088/1742-6596/1389/1/012038},\n\tdoi = {10.1088/1742-6596/1389/1/012038},\n\tabstract = {We have studied polarization-dependent broad-band dielectric response of single-crystalline Ti-substituted barium hexaferrites BaTixFe12-xO19, x=0.64., 0.75, 1.1, in the frequency range from 10 to 8000 cm−1 and at temperatures from 5 to 300 K. In addition to a rich set of phonon resonances located at frequencies from 90 to 800 cm−1 we observed an unusual low-energy response (terahertz region, 10-100 cm−1) stemming from two different effects: relaxational process and second order spin-orbit coupling in Fe2+ ground state, that may set up new prospects for doped hexaferrites in terahertz technologies.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics: Conference Series},\n\tauthor = {Yegiyan, S. R. and Alyabyeva, L. N. and Torgashev, V. I. and Vinnik, D. A. and Gudkova, S. A. and Prokhorov, A. S. and Dressel, M. and Gorshunov, B. P.},\n\tmonth = nov,\n\tyear = {2019},\n\tnote = {Publisher: IOP Publishing},\n\tpages = {012038},\n\tfile = {IOP Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\UWP6ZQD3\\\\Yegiyan и др. - 2019 - Terahertz-infrared spectroscopy of single crystall.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We have studied polarization-dependent broad-band dielectric response of single-crystalline Ti-substituted barium hexaferrites BaTixFe12-xO19, x=0.64., 0.75, 1.1, in the frequency range from 10 to 8000 cm−1 and at temperatures from 5 to 300 K. In addition to a rich set of phonon resonances located at frequencies from 90 to 800 cm−1 we observed an unusual low-energy response (terahertz region, 10-100 cm−1) stemming from two different effects: relaxational process and second order spin-orbit coupling in Fe2+ ground state, that may set up new prospects for doped hexaferrites in terahertz technologies.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"boldyrev-pavlenko-shilkina-nazarenko-bokov-reznichenko-rudskaya-panchenko-structuremicrostructuredielectricandpiezoelectricpropertiesof1xybifeotextrm3xpbfetextrm05nbtextrm05otextrm3ypbtiotextrm3ceramics-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0272884219310296\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'boldyrev-pavlenko-shilkina-nazarenko-bokov-reznichenko-rudskaya-panchenko-structuremicrostructuredielectricandpiezoelectricpropertiesof1xybifeotextrm3xpbfetextrm05nbtextrm05otextrm3ypbtiotextrm3ceramics-2019', 'https://www.sciencedirect.com/science/article/pii/S0272884219310296', event);\">\n    Structure, microstructure, dielectric and piezoelectric properties of (1-x-y)BiFeO$_{\\textrm{3}}$-xPbFe$_{\\textrm{0.5}}$Nb$_{\\textrm{0.5}}$O$_{\\textrm{3}}$-yPbTiO$_{\\textrm{3}}$ ceramics.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Boldyrev, N. A.; Pavlenko, A. V.; Shilkina, L. A.; Nazarenko, A. V.; Bokov, A. A.; Reznichenko, L. A.; Rudskaya, A. G.;  and Panchenko, E. I.\n</span>\n\n  \n\n</span>\n\n  <i>Ceramics International</i>, 45(12): 14768–14774. August 2019.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0272884219310296\"\n     onclick=\"log_download('boldyrev-pavlenko-shilkina-nazarenko-bokov-reznichenko-rudskaya-panchenko-structuremicrostructuredielectricandpiezoelectricpropertiesof1xybifeotextrm3xpbfetextrm05nbtextrm05otextrm3ypbtiotextrm3ceramics-2019', 'https://www.sciencedirect.com/science/article/pii/S0272884219310296', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Structure, microstructure, dielectric and piezoelectric properties of (1-x-y)BiFeO$_{\\textrm{3}}$-xPbFe$_{\\textrm{0.5}}$Nb$_{\\textrm{0.5}}$O$_{\\textrm{3}}$-yPbTiO$_{\\textrm{3}}$ ceramics [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.ceramint.2019.04.204\"\n     onclick=\"log_download('boldyrev-pavlenko-shilkina-nazarenko-bokov-reznichenko-rudskaya-panchenko-structuremicrostructuredielectricandpiezoelectricpropertiesof1xybifeotextrm3xpbfetextrm05nbtextrm05otextrm3ypbtiotextrm3ceramics-2019', 'http://doi.org/10.1016/j.ceramint.2019.04.204', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/boldyrev-pavlenko-shilkina-nazarenko-bokov-reznichenko-rudskaya-panchenko-structuremicrostructuredielectricandpiezoelectricpropertiesof1xybifeotextrm3xpbfetextrm05nbtextrm05otextrm3ypbtiotextrm3ceramics-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('boldyrev-pavlenko-shilkina-nazarenko-bokov-reznichenko-rudskaya-panchenko-structuremicrostructuredielectricandpiezoelectricpropertiesof1xybifeotextrm3xpbfetextrm05nbtextrm05otextrm3ypbtiotextrm3ceramics-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{boldyrev_structure_2019,\n\ttitle = {Structure, microstructure, dielectric and piezoelectric properties of (1-x-y){BiFeO}$_{\\textrm{3}}$-{xPbFe}$_{\\textrm{0.5}}${Nb}$_{\\textrm{0.5}}${O}$_{\\textrm{3}}$-{yPbTiO}$_{\\textrm{3}}$ ceramics},\n\tvolume = {45},\n\tissn = {0272-8842},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0272884219310296},\n\tdoi = {10.1016/j.ceramint.2019.04.204},\n\tabstract = {Ceramics of seven quasi-binary concentration sections of the ternary solid solution system (1-x-y)BiFeO3-xPbFe0.5Nb0.5O3-yPbTiO3 were prepared by the conventional solid-phase reaction method in the range of 0.05 ≤ x ≤ 0.325; 0.05 ≤ y ≤ 0.325. By using x-ray diffraction technique, the phase diagram of the system was constructed which was shown to contain the regions of tetragonal and rhombohedral symmetry and the morphotropic phase boundary between them. Grain morphology, dielectric and piezoelectric properties of selected solid solutions were investigated. The highest piezoelectric coefficient d33 = 50 pC/N was obtained. Dielectric characteristics of ceramics revealed ferroelectric relaxor behavior and region of diffuse phase transition from the paraelectric to ferroelectric phase in the temperature range of 600–800 K.},\n\tnumber = {12},\n\turldate = {2023-11-11},\n\tjournal = {Ceramics International},\n\tauthor = {Boldyrev, N. A. and Pavlenko, A. V. and Shilkina, L. A. and Nazarenko, A. V. and Bokov, A. A. and Reznichenko, L. A. and Rudskaya, A. G. and Panchenko, E. I.},\n\tmonth = aug,\n\tyear = {2019},\n\tkeywords = {Dielectric properties, Perovskites multiferroics, Piezoelectric properties, Solid solutions},\n\tpages = {14768--14774},\n\tfile = {ScienceDirect Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\FR6CF252\\\\S0272884219310296.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Ceramics of seven quasi-binary concentration sections of the ternary solid solution system (1-x-y)BiFeO3-xPbFe0.5Nb0.5O3-yPbTiO3 were prepared by the conventional solid-phase reaction method in the range of 0.05 ≤ x ≤ 0.325; 0.05 ≤ y ≤ 0.325. By using x-ray diffraction technique, the phase diagram of the system was constructed which was shown to contain the regions of tetragonal and rhombohedral symmetry and the morphotropic phase boundary between them. Grain morphology, dielectric and piezoelectric properties of selected solid solutions were investigated. The highest piezoelectric coefficient d33 = 50 pC/N was obtained. Dielectric characteristics of ceramics revealed ferroelectric relaxor behavior and region of diffuse phase transition from the paraelectric to ferroelectric phase in the temperature range of 600–800 K.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kabirov-bogatin-sidorenko-belokobylsky-mikheikin-letovaltsev-bulanova-prutsakova-piezoresistanceandmagnetoresistanceofcompositesbasedonmanganitelatextrm07srtextrm03mnotextrm3-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://lettersonmaterials.com/en/Readers/Article.aspx?aid=15201\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kabirov-bogatin-sidorenko-belokobylsky-mikheikin-letovaltsev-bulanova-prutsakova-piezoresistanceandmagnetoresistanceofcompositesbasedonmanganitelatextrm07srtextrm03mnotextrm3-2019', 'https://lettersonmaterials.com/en/Readers/Article.aspx?aid=15201', event);\">\n    Piezoresistance and magnetoresistance of composites based on manganite La$_{\\textrm{0.7}}$Sr$_{\\textrm{0.3}}$MnO$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kabirov, Y. V.; Bogatin, A. S.; Sidorenko, E. N.; Belokobylsky, M. V.; Mikheikin, A. S.; Letovaltsev, A. O.; Bulanova, A. L.;  and Prutsakova, N. V.\n</span>\n\n  \n\n</span>\n\n  <i>Letters on Materials</i>, 9(2): 223–227. May 2019.\n  <span class=\"note\">Publisher: Letters on Materials</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://lettersonmaterials.com/en/Readers/Article.aspx?aid=15201\"\n     onclick=\"log_download('kabirov-bogatin-sidorenko-belokobylsky-mikheikin-letovaltsev-bulanova-prutsakova-piezoresistanceandmagnetoresistanceofcompositesbasedonmanganitelatextrm07srtextrm03mnotextrm3-2019', 'https://lettersonmaterials.com/en/Readers/Article.aspx?aid=15201', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Piezoresistance and magnetoresistance of composites based on manganite La$_{\\textrm{0.7}}$Sr$_{\\textrm{0.3}}$MnO$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.22226/2410-3535-2019-2-223-227\"\n     onclick=\"log_download('kabirov-bogatin-sidorenko-belokobylsky-mikheikin-letovaltsev-bulanova-prutsakova-piezoresistanceandmagnetoresistanceofcompositesbasedonmanganitelatextrm07srtextrm03mnotextrm3-2019', 'http://doi.org/10.22226/2410-3535-2019-2-223-227', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kabirov-bogatin-sidorenko-belokobylsky-mikheikin-letovaltsev-bulanova-prutsakova-piezoresistanceandmagnetoresistanceofcompositesbasedonmanganitelatextrm07srtextrm03mnotextrm3-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kabirov-bogatin-sidorenko-belokobylsky-mikheikin-letovaltsev-bulanova-prutsakova-piezoresistanceandmagnetoresistanceofcompositesbasedonmanganitelatextrm07srtextrm03mnotextrm3-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kabirov_piezoresistance_2019,\n\ttitle = {Piezoresistance and magnetoresistance of composites based on manganite {La}$_{\\textrm{0.7}}${Sr}$_{\\textrm{0.3}}${MnO}$_{\\textrm{3}}$},\n\tvolume = {9},\n\tissn = {2218-5046},\n\turl = {https://lettersonmaterials.com/en/Readers/Article.aspx?aid=15201},\n\tdoi = {10.22226/2410-3535-2019-2-223-227},\n\tabstract = {The development of new sensitive multifunctional materials, which simultaneously react both to mechanical pressure and a constant magnetic field, is one of challenges of the modern materials science. In order to create materials that can simultaneously possess extrinsic piezoresistance and magnetoresistance, polymer composites based on La0.7Sr0.3MnO3 (LSMO) and low density polyethylene (LDPE) of composition (100‑x)LSMO / xLDPE at x = 7, 8, 9, 12, 15, 17, 18, 22 mass percent have been synthesized in this work. The composites have been synthesized at 170°C and a pressure of 50 MPa in the presence of hydrocarbons. The phase composition of the obtained samples has been studied by X-ray diffraction and infrared spectroscopy. Electric, piezoresistance and magnetoresistance properties of the samples have been studied. It has been found out that with increasing concentration of polyethylene, the electrical resistance of the samples also increases. It has been established that the percolation threshold of the composites is about 13 wt.\\% of polyethylene. A maximum is observed in the dependence of the electrical resistance of the samples on the uniaxial pressure at a concentration of polyethylene near the percolation threshold at x =15 wt.\\%. Samples with concentration of x =15 wt.\\% of low density polyethylene show extrinsic piezoresistance of about 17 \\% in the pressure range 0 – 270 kPa. Significant hysteresis is observed when considering the dependence of piezoresistance on pressure for all samples. The pressure sensitivity for a sample of 85 \\%LSMO / 15 \\%LDPE reaches 8.40 mΩ / Pa. The maximum values of the negative isotropic tunnel magnetoresistance of the composites 88 \\%LSMO / 12 \\%LDPE have values of about 2 \\% in a 15 kOe magnetic field. We believe that the materials studied in the paper could be useful for designing multifunctional biosensors of mechanical pressure and constant magnetic field.},\n\tlanguage = {en},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Letters on Materials},\n\tauthor = {Kabirov, Y. V. and Bogatin, A. S. and Sidorenko, E. N. and Belokobylsky, M. V. and Mikheikin, A. S. and Letovaltsev, A. O. and Bulanova, A. L. and Prutsakova, N. V.},\n\tmonth = may,\n\tyear = {2019},\n\tnote = {Publisher: Letters on Materials},\n\tpages = {223--227},\n\tfile = {Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\KQGQ4KDV\\\\Kabirov и др. - 2019 - Piezoresistance and magnetoresistance of composite.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The development of new sensitive multifunctional materials, which simultaneously react both to mechanical pressure and a constant magnetic field, is one of challenges of the modern materials science. In order to create materials that can simultaneously possess extrinsic piezoresistance and magnetoresistance, polymer composites based on La0.7Sr0.3MnO3 (LSMO) and low density polyethylene (LDPE) of composition (100‑x)LSMO / xLDPE at x = 7, 8, 9, 12, 15, 17, 18, 22 mass percent have been synthesized in this work. The composites have been synthesized at 170°C and a pressure of 50 MPa in the presence of hydrocarbons. The phase composition of the obtained samples has been studied by X-ray diffraction and infrared spectroscopy. Electric, piezoresistance and magnetoresistance properties of the samples have been studied. It has been found out that with increasing concentration of polyethylene, the electrical resistance of the samples also increases. It has been established that the percolation threshold of the composites is about 13 wt.% of polyethylene. A maximum is observed in the dependence of the electrical resistance of the samples on the uniaxial pressure at a concentration of polyethylene near the percolation threshold at x =15 wt.%. Samples with concentration of x =15 wt.% of low density polyethylene show extrinsic piezoresistance of about 17 % in the pressure range 0 – 270 kPa. Significant hysteresis is observed when considering the dependence of piezoresistance on pressure for all samples. The pressure sensitivity for a sample of 85 %LSMO / 15 %LDPE reaches 8.40 mΩ / Pa. The maximum values of the negative isotropic tunnel magnetoresistance of the composites 88 %LSMO / 12 %LDPE have values of about 2 % in a 15 kOe magnetic field. We believe that the materials studied in the paper could be useful for designing multifunctional biosensors of mechanical pressure and constant magnetic field.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"hanani-mezzane-amjoud-razumnaya-fourcade-gagou-hoummada-elmarssi-etal-phasetransitionsenergystorageperformancesandelectrocaloriceffectoftheleadfreebatextrm085catextrm015zrtextrm010titextrm090otextrm3ceramicrelaxor-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1007/s10854-019-00946-5\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'hanani-mezzane-amjoud-razumnaya-fourcade-gagou-hoummada-elmarssi-etal-phasetransitionsenergystorageperformancesandelectrocaloriceffectoftheleadfreebatextrm085catextrm015zrtextrm010titextrm090otextrm3ceramicrelaxor-2019', 'https://doi.org/10.1007/s10854-019-00946-5', event);\">\n    Phase transitions, energy storage performances and electrocaloric effect of the lead-free Ba$_{\\textrm{0.85}}$Ca$_{\\textrm{0.15}}$Zr$_{\\textrm{0.10}}$Ti$_{\\textrm{0.90}}$O$_{\\textrm{3}}$ ceramic relaxor.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Hanani, Z.; Mezzane, D.; Amjoud, M.; Razumnaya, A. G.; Fourcade, S.; Gagou, Y.; Hoummada, K.; El Marssi, M.;  and Gouné, M.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Materials Science: Materials in Electronics</i>, 30(7): 6430–6438. April 2019.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1007/s10854-019-00946-5\"\n     onclick=\"log_download('hanani-mezzane-amjoud-razumnaya-fourcade-gagou-hoummada-elmarssi-etal-phasetransitionsenergystorageperformancesandelectrocaloriceffectoftheleadfreebatextrm085catextrm015zrtextrm010titextrm090otextrm3ceramicrelaxor-2019', 'https://doi.org/10.1007/s10854-019-00946-5', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Phase transitions, energy storage performances and electrocaloric effect of the lead-free Ba$_{\\textrm{0.85}}$Ca$_{\\textrm{0.15}}$Zr$_{\\textrm{0.10}}$Ti$_{\\textrm{0.90}}$O$_{\\textrm{3}}$ ceramic relaxor [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1007/s10854-019-00946-5\"\n     onclick=\"log_download('hanani-mezzane-amjoud-razumnaya-fourcade-gagou-hoummada-elmarssi-etal-phasetransitionsenergystorageperformancesandelectrocaloriceffectoftheleadfreebatextrm085catextrm015zrtextrm010titextrm090otextrm3ceramicrelaxor-2019', 'http://doi.org/10.1007/s10854-019-00946-5', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/hanani-mezzane-amjoud-razumnaya-fourcade-gagou-hoummada-elmarssi-etal-phasetransitionsenergystorageperformancesandelectrocaloriceffectoftheleadfreebatextrm085catextrm015zrtextrm010titextrm090otextrm3ceramicrelaxor-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('hanani-mezzane-amjoud-razumnaya-fourcade-gagou-hoummada-elmarssi-etal-phasetransitionsenergystorageperformancesandelectrocaloriceffectoftheleadfreebatextrm085catextrm015zrtextrm010titextrm090otextrm3ceramicrelaxor-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{hanani_phase_2019,\n\ttitle = {Phase transitions, energy storage performances and electrocaloric effect of the lead-free {Ba}$_{\\textrm{0.85}}${Ca}$_{\\textrm{0.15}}${Zr}$_{\\textrm{0.10}}${Ti}$_{\\textrm{0.90}}${O}$_{\\textrm{3}}$ ceramic relaxor},\n\tvolume = {30},\n\tissn = {1573-482X},\n\turl = {https://doi.org/10.1007/s10854-019-00946-5},\n\tdoi = {10.1007/s10854-019-00946-5},\n\tabstract = {Lead-free Ba0.85Ca0.15Zr0.10Ti0.90O3 (BCZT) ceramic exhibits excellent dielectric, ferroelectric and piezoelectric properties at the morphotropic phase boundary (MPB). Previously, we demonstrated that the use of the anionic surfactant sodium dodecyl sulfate (SDS, NaC12H25SO4) could enhance the dielectric properties of BCZT ceramic using surfactant-assisted solvothermal processing [1]. In the present study, structural, dielectric, ferroelectric properties, as well as electrocaloric effect and energy storage performances of this BCZT ceramic were thoroughly investigated. X-ray diffraction (XRD) measurements revealed the presence of single perovskite phase at room temperature with the coexistence of orthorhombic and tetragonal symmetries. In-situ Raman spectroscopy results confirmed the existence of all phase transitions from rhombohedral through orthorhombic and tetragonal to cubic symmetries when the temperature varies as reported in undoped-BaTiO3. Evolution of energy storage performances with temperature have been investigated. BCZT ceramic exhibits a high energy storage efficiency of {\\textasciitilde} 80\\% at 120 °C. In addition, the electrocaloric responsivity was found to be 0.164 × 10−6 K·m/V at 363 K.},\n\tlanguage = {en},\n\tnumber = {7},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Materials Science: Materials in Electronics},\n\tauthor = {Hanani, Zouhair and Mezzane, Daoud and Amjoud, M’barek and Razumnaya, Anna G. and Fourcade, Sébastien and Gagou, Yaovi and Hoummada, Khalid and El Marssi, Mimoun and Gouné, Mohamed},\n\tmonth = apr,\n\tyear = {2019},\n\tpages = {6430--6438},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\8NW2JEKW\\\\Hanani и др. - 2019 - Phase transitions, energy storage performances and.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Lead-free Ba0.85Ca0.15Zr0.10Ti0.90O3 (BCZT) ceramic exhibits excellent dielectric, ferroelectric and piezoelectric properties at the morphotropic phase boundary (MPB). Previously, we demonstrated that the use of the anionic surfactant sodium dodecyl sulfate (SDS, NaC12H25SO4) could enhance the dielectric properties of BCZT ceramic using surfactant-assisted solvothermal processing [1]. In the present study, structural, dielectric, ferroelectric properties, as well as electrocaloric effect and energy storage performances of this BCZT ceramic were thoroughly investigated. X-ray diffraction (XRD) measurements revealed the presence of single perovskite phase at room temperature with the coexistence of orthorhombic and tetragonal symmetries. In-situ Raman spectroscopy results confirmed the existence of all phase transitions from rhombohedral through orthorhombic and tetragonal to cubic symmetries when the temperature varies as reported in undoped-BaTiO3. Evolution of energy storage performances with temperature have been investigated. BCZT ceramic exhibits a high energy storage efficiency of ~ 80% at 120 °C. In addition, the electrocaloric responsivity was found to be 0.164 × 10−6 K·m/V at 363 K.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-talanov-phasetransitionsinbitextrm4titextrm3otextrm12-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.iucr.org/b/issues/2019/06/00/dq5041/\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-talanov-phasetransitionsinbitextrm4titextrm3otextrm12-2019', 'https://journals.iucr.org/b/issues/2019/06/00/dq5041/', event);\">\n    Phase transitions in Bi$_{\\textrm{4}}$Ti$_{\\textrm{3}}$O$_{\\textrm{12}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.;  and Talanov, M. V.\n</span>\n\n  \n\n</span>\n\n  <i>Acta Crystallographica Section B: Structural Science, Crystal Engineering and Materials</i>, 75(6): 978–986. December 2019.\n  <span class=\"note\">Number: 6 Publisher: International Union of Crystallography</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.iucr.org/b/issues/2019/06/00/dq5041/\"\n     onclick=\"log_download('shirokov-talanov-phasetransitionsinbitextrm4titextrm3otextrm12-2019', 'https://journals.iucr.org/b/issues/2019/06/00/dq5041/', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Phase transitions in Bi$_{\\textrm{4}}$Ti$_{\\textrm{3}}$O$_{\\textrm{12}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1107/S2052520619011843\"\n     onclick=\"log_download('shirokov-talanov-phasetransitionsinbitextrm4titextrm3otextrm12-2019', 'http://doi.org/10.1107/S2052520619011843', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-talanov-phasetransitionsinbitextrm4titextrm3otextrm12-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-talanov-phasetransitionsinbitextrm4titextrm3otextrm12-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_phase_2019,\n\ttitle = {Phase transitions in {Bi}$_{\\textrm{4}}${Ti}$_{\\textrm{3}}${O}$_{\\textrm{12}}$},\n\tvolume = {75},\n\tcopyright = {Copyright (c) 2019 International Union of Crystallography},\n\tissn = {2052-5206},\n\turl = {https://journals.iucr.org/b/issues/2019/06/00/dq5041/},\n\tdoi = {10.1107/S2052520619011843},\n\tabstract = {A Landau-type phase diagram describing the temperature phase transitions in the layered perovskite ferroelectric Bi4Ti3O12 is constructed.},\n\tlanguage = {en},\n\tnumber = {6},\n\turldate = {2023-11-11},\n\tjournal = {Acta Crystallographica Section B: Structural Science, Crystal Engineering and Materials},\n\tauthor = {Shirokov, V. B. and Talanov, M. V.},\n\tmonth = dec,\n\tyear = {2019},\n\tnote = {Number: 6\nPublisher: International Union of Crystallography},\n\tpages = {978--986},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A Landau-type phase diagram describing the temperature phase transitions in the layered perovskite ferroelectric Bi4Ti3O12 is constructed.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kuriganova-smirnova-leontyev-avramenko-investigationofstructuralmicrostructuralandelectrochemicalcharacteristicsofptsnotextrmxcelectrocatalystspreparedviaelectrochemicaldispersionoftinandplatinum-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://ctj-isuct.ru/article/view/1551\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kuriganova-smirnova-leontyev-avramenko-investigationofstructuralmicrostructuralandelectrochemicalcharacteristicsofptsnotextrmxcelectrocatalystspreparedviaelectrochemicaldispersionoftinandplatinum-2019', 'http://ctj-isuct.ru/article/view/1551', event);\">\n    INVESTIGATION OF STRUCTURAL, MICROSTRUCTURAL AND ELECTROCHEMICAL CHARACTERISTICS OF Pt/SnO$_{\\textrm{x}}$-C ELECTROCATALYSTS PREPARED VIA ELECTROCHEMICAL DISPERSION OF TIN AND PLATINUM.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kuriganova, A. B.; Smirnova, N. V.; Leontyev, I. N.;  and Avramenko, M. V.\n</span>\n\n  \n\n</span>\n\n  <i>ИЗВЕСТИЯ ВЫСШИХ УЧЕБНЫХ ЗАВЕДЕНИЙ. СЕРИЯ «ХИМИЯ И ХИМИЧЕСКАЯ ТЕХНОЛОГИЯ»</i>, 62(9): 53–59. August 2019.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://ctj-isuct.ru/article/view/1551\"\n     onclick=\"log_download('kuriganova-smirnova-leontyev-avramenko-investigationofstructuralmicrostructuralandelectrochemicalcharacteristicsofptsnotextrmxcelectrocatalystspreparedviaelectrochemicaldispersionoftinandplatinum-2019', 'http://ctj-isuct.ru/article/view/1551', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"INVESTIGATION OF STRUCTURAL, MICROSTRUCTURAL AND ELECTROCHEMICAL CHARACTERISTICS OF Pt/SnO$_{\\textrm{x}}$-C ELECTROCATALYSTS PREPARED VIA ELECTROCHEMICAL DISPERSION OF TIN AND PLATINUM [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.6060/ivkkt.20196209.5945\"\n     onclick=\"log_download('kuriganova-smirnova-leontyev-avramenko-investigationofstructuralmicrostructuralandelectrochemicalcharacteristicsofptsnotextrmxcelectrocatalystspreparedviaelectrochemicaldispersionoftinandplatinum-2019', 'http://doi.org/10.6060/ivkkt.20196209.5945', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kuriganova-smirnova-leontyev-avramenko-investigationofstructuralmicrostructuralandelectrochemicalcharacteristicsofptsnotextrmxcelectrocatalystspreparedviaelectrochemicaldispersionoftinandplatinum-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kuriganova-smirnova-leontyev-avramenko-investigationofstructuralmicrostructuralandelectrochemicalcharacteristicsofptsnotextrmxcelectrocatalystspreparedviaelectrochemicaldispersionoftinandplatinum-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kuriganova_investigation_2019,\n\ttitle = {{INVESTIGATION} {OF} {STRUCTURAL}, {MICROSTRUCTURAL} {AND} {ELECTROCHEMICAL} {CHARACTERISTICS} {OF} {Pt}/{SnO}$_{\\textrm{x}}$-{C} {ELECTROCATALYSTS} {PREPARED} {VIA} {ELECTROCHEMICAL} {DISPERSION} {OF} {TIN} {AND} {PLATINUM}},\n\tvolume = {62},\n\tissn = {2500-3070},\n\turl = {http://ctj-isuct.ru/article/view/1551},\n\tdoi = {10.6060/ivkkt.20196209.5945},\n\tabstract = {Аннотация\n\t\t\t\t\tПорошки оксидов олова (SnOx) с различной структурой и составом и Pt/SnOx-C электрокатализаторы для топливных элементов с прямым окислением этанола были получены путем электрохимического диспергирования оловянных и платиновых электродов под действием импульсного переменного тока с использованием электролитов с различными типами анионов (Cl- и F-). Полученные порошки оксидов олова, композиционные носители SnOx-C и катализаторы Pt/SnOx-C были исследованы различными методами: рентгеновская дифракция, рамановская спектроскопия, сканирующая и просвечивающая электронная микроскопия. Наночастицы SnO2 со средним размером 5 - 8 нм были синтезированы в Cl- -содержащем растворе. В свою очередь, было обнаружено, что во F- - содержащем электролите были получены наночастицы SnO с выраженной анизотропией формы и размером частиц. Полученные оксиды олова использовались в качестве предшественников в синтезе Pt/SnOx-C катализаторов (загрузка Pt 20\\%, D111 = 10,5-13,5 нм) также с применением технологии электрохимического диспергирования под действием импульсного переменного тока. Электрохимически активная площадь поверхности Pt/SnOx-C электрокатализаторов, определенная методом окислительной десорбции CO, составляла 13-15 м2г-1. Электрокаталитическую активность электрокатализаторов изучали для реакции электрохимического окисления этанола методами циклической вольтамперометрии с использованием вращающегося дискового электрода. Было обнаружено, что присутствие оксидов олова оказывает одинаковое влияние на реакции электрохимического окисления СО и этанола независимо от структурных особенностей их частиц.\n{\\textless}span style=&quot;opacity: 0;&quot;{\\textgreater} . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . {\\textless}/span{\\textgreater}},\n\tlanguage = {ru-RU},\n\tnumber = {9},\n\turldate = {2023-11-11},\n\tjournal = {ИЗВЕСТИЯ ВЫСШИХ УЧЕБНЫХ ЗАВЕДЕНИЙ. СЕРИЯ «ХИМИЯ И ХИМИЧЕСКАЯ ТЕХНОЛОГИЯ»},\n\tauthor = {Kuriganova, Alexandra B. and Smirnova, Nina V. and Leontyev, Igor N. and Avramenko, Marina V.},\n\tmonth = aug,\n\tyear = {2019},\n\tkeywords = {Pt/C, оксиды олова, топливный элемент, электроокисление этанола, электрохимическое диспергирование},\n\tpages = {53--59},\n\tfile = {Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\VKA94EMJ\\\\Kuriganova и др. - 2019 - INVESTIGATION OF STRUCTURAL, MICROSTRUCTURAL AND E.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Аннотация Порошки оксидов олова (SnOx) с различной структурой и составом и Pt/SnOx-C электрокатализаторы для топливных элементов с прямым окислением этанола были получены путем электрохимического диспергирования оловянных и платиновых электродов под действием импульсного переменного тока с использованием электролитов с различными типами анионов (Cl- и F-). Полученные порошки оксидов олова, композиционные носители SnOx-C и катализаторы Pt/SnOx-C были исследованы различными методами: рентгеновская дифракция, рамановская спектроскопия, сканирующая и просвечивающая электронная микроскопия. Наночастицы SnO2 со средним размером 5 - 8 нм были синтезированы в Cl- -содержащем растворе. В свою очередь, было обнаружено, что во F- - содержащем электролите были получены наночастицы SnO с выраженной анизотропией формы и размером частиц. Полученные оксиды олова использовались в качестве предшественников в синтезе Pt/SnOx-C катализаторов (загрузка Pt 20%, D111 = 10,5-13,5 нм) также с применением технологии электрохимического диспергирования под действием импульсного переменного тока. Электрохимически активная площадь поверхности Pt/SnOx-C электрокатализаторов, определенная методом окислительной десорбции CO, составляла 13-15 м2г-1. Электрокаталитическую активность электрокатализаторов изучали для реакции электрохимического окисления этанола методами циклической вольтамперометрии с использованием вращающегося дискового электрода. Было обнаружено, что присутствие оксидов олова оказывает одинаковое влияние на реакции электрохимического окисления СО и этанола независимо от структурных особенностей их частиц. \\textlessspan style=\"opacity: 0;\"\\textgreater . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . \\textless/span\\textgreater\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"ulyankina-avramenko-kusnetsov-firestein-zhigunov-smirnova-electrochemicalsynthesisoftiotextrm2underpulsealternatingcurrenteffectofthermaltreatmentonthephotocatalyticactivity-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201803367\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'ulyankina-avramenko-kusnetsov-firestein-zhigunov-smirnova-electrochemicalsynthesisoftiotextrm2underpulsealternatingcurrenteffectofthermaltreatmentonthephotocatalyticactivity-2019', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201803367', event);\">\n    Electrochemical Synthesis of TiO$_{\\textrm{2}}$ under Pulse Alternating Current: Effect of Thermal Treatment on the Photocatalytic Activity.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Ulyankina, A.; Avramenko, M.; Kusnetsov, D.; Firestein, K.; Zhigunov, D.;  and Smirnova, N.\n</span>\n\n  \n\n</span>\n\n  <i>ChemistrySelect</i>, 4(6): 2001–2007.  2019.\n  <span class=\"note\">_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/slct.201803367</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201803367\"\n     onclick=\"log_download('ulyankina-avramenko-kusnetsov-firestein-zhigunov-smirnova-electrochemicalsynthesisoftiotextrm2underpulsealternatingcurrenteffectofthermaltreatmentonthephotocatalyticactivity-2019', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201803367', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Electrochemical Synthesis of TiO$_{\\textrm{2}}$ under Pulse Alternating Current: Effect of Thermal Treatment on the Photocatalytic Activity [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1002/slct.201803367\"\n     onclick=\"log_download('ulyankina-avramenko-kusnetsov-firestein-zhigunov-smirnova-electrochemicalsynthesisoftiotextrm2underpulsealternatingcurrenteffectofthermaltreatmentonthephotocatalyticactivity-2019', 'http://doi.org/10.1002/slct.201803367', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/ulyankina-avramenko-kusnetsov-firestein-zhigunov-smirnova-electrochemicalsynthesisoftiotextrm2underpulsealternatingcurrenteffectofthermaltreatmentonthephotocatalyticactivity-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('ulyankina-avramenko-kusnetsov-firestein-zhigunov-smirnova-electrochemicalsynthesisoftiotextrm2underpulsealternatingcurrenteffectofthermaltreatmentonthephotocatalyticactivity-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{ulyankina_electrochemical_2019,\n\ttitle = {Electrochemical {Synthesis} of {TiO}$_{\\textrm{2}}$ under {Pulse} {Alternating} {Current}: {Effect} of {Thermal} {Treatment} on the {Photocatalytic} {Activity}},\n\tvolume = {4},\n\tcopyright = {© 2019 Wiley-VCH Verlag GmbH \\&amp; Co. KGaA, Weinheim},\n\tissn = {2365-6549},\n\tshorttitle = {Electrochemical {Synthesis} of {TiO2} under {Pulse} {Alternating} {Current}},\n\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201803367},\n\tdoi = {10.1002/slct.201803367},\n\tabstract = {The current work aimed to study the effect of thermal treatment on the structural, optical, and photocatalytic properties of TiO2 nanoparticles synthesized by a novel large-scale electrochemical method using pulse alternating current (PAC). The obtained titania was characterized via XRD, TEM, XPS, UV-Vis DRS, PL, Raman and FTIR spectroscopy. The as-prepared TiO2 was found to be poorly crystallized and partly amorphous. Following thermal annealing, the anatase structure is developed at temperatures of 400–600 °C. The photoreactivity of the TiO2 nanoparticles was evaluated for the degradation of methylene blue (MB) and rhodamin B (RhB) dyes under UVA irradiation. As shown, the adsorption properties and photocatalytic activity of the as-prepared TiO2 strongly depend on the chemical nature of the dye. The enhanced photocatalytic performance for the MB and RhB degradation was observed for the sample annealed at 400 °C, which coincides with a balance between the degree of crystallinity, specific surface area, optical properties and efficiency of electron-hole pair separation.},\n\tlanguage = {en},\n\tnumber = {6},\n\turldate = {2023-11-11},\n\tjournal = {ChemistrySelect},\n\tauthor = {Ulyankina, Anna and Avramenko, Marina and Kusnetsov, Denis and Firestein, Konstantin and Zhigunov, Denis and Smirnova, Nina},\n\tyear = {2019},\n\tnote = {\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/slct.201803367},\n\tkeywords = {crystallinity, dye, electrochemical synthesis, photocatalysis, titanium dioxide},\n\tpages = {2001--2007},\n\tfile = {Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\NQTKT7VJ\\\\slct.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The current work aimed to study the effect of thermal treatment on the structural, optical, and photocatalytic properties of TiO2 nanoparticles synthesized by a novel large-scale electrochemical method using pulse alternating current (PAC). The obtained titania was characterized via XRD, TEM, XPS, UV-Vis DRS, PL, Raman and FTIR spectroscopy. The as-prepared TiO2 was found to be poorly crystallized and partly amorphous. Following thermal annealing, the anatase structure is developed at temperatures of 400–600 °C. The photoreactivity of the TiO2 nanoparticles was evaluated for the degradation of methylene blue (MB) and rhodamin B (RhB) dyes under UVA irradiation. As shown, the adsorption properties and photocatalytic activity of the as-prepared TiO2 strongly depend on the chemical nature of the dye. The enhanced photocatalytic performance for the MB and RhB degradation was observed for the sample annealed at 400 °C, which coincides with a balance between the degree of crystallinity, specific surface area, optical properties and efficiency of electron-hole pair separation.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"--------etal--2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.libnauka.ru/item.php?doi=10.7868/S25000640190103\"\n     onclick=\"return trackOutboundLink('publications', 'click', '--------etal--2019', 'https://www.libnauka.ru/item.php?doi=10.7868/S25000640190103', event);\">\n    Температурная зависимость фононных и магнонных мод в гетероструктурах мультиферроик - сегнетоэлектрик.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Бабарикин, Д.; Разумная, А.; Стрюков, Д.; Анохин, А.; Михейкин, А.; Павленко, А.; Широков, В.; Зинченко, С.;  and Мухортов, В.\n</span>\n\n  \n\n</span>\n\n  <i>Science in the South of Russia</i>, (1): 21–30.  2019.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.libnauka.ru/item.php?doi=10.7868/S25000640190103\"\n     onclick=\"log_download('--------etal--2019', 'https://www.libnauka.ru/item.php?doi=10.7868/S25000640190103', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Температурная зависимость фононных и магнонных мод в гетероструктурах мультиферроик - сегнетоэлектрик [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.7868/S25000640190103\"\n     onclick=\"log_download('--------etal--2019', 'http://doi.org/10.7868/S25000640190103', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/--------etal--2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('--------etal--2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2019-3,\n\ttitle = {Температурная зависимость фононных и магнонных мод в гетероструктурах мультиферроик - сегнетоэлектрик},\n\tissn = {2500-0640},\n\turl = {https://www.libnauka.ru/item.php?doi=10.7868/S25000640190103},\n\tdoi = {10.7868/S25000640190103},\n\tabstract = {Пленки феррита висмута BiFeO выращены на монокристаллической подложке (001) MgO по блочному механизму роста методом высокочастотного катодного распыления с использованием в качестве буферного слоя сегнетоэлектрика BaSr \\_ TiO при варьировании состава x. Изучение гетероструктур методом рентгеновской дифракции показало, что пленки характеризуются псевдотетрагональной симметрией при комнатной температуре. Определено, что степень тетрагонального искажения слоев BaSr \\_ TiO возрастает с увеличением концентрации Ba, в то время как в слоях BiFeO она остается практически неизменной. Методом атомно-силовой микроскопии установлено, что пленки BiFeOвыросли по блочному механизму роста, причем блоки строго ориентированы относительно друг друга и кристаллографических осей подложки MgO. Высокотемпературные исследования спектров комбинационного рассеяния света в широком диапазоне температур 295-900 K и частот от 50 до 1600 смпоказали, что интенсивность полосы 1250 см, соответствующей плотности состояний двухмагнонных возбуждений, линейно понижается при повышении температуры. Анализ температурного поведения полосы 1250 см позволяет предполагать, что в изученных пленках BiFeO антиферромагнитный фазовый переход происходит в диапазоне температур 600-700 K. Использование сегнетоэлектрических буферных слоев BaSr \\_ TiO с разной степенью тетрагонального искажения позволяет управлять деформацией пленок BiFeO, возникающей в результате несоответствия параметров решеток в смежных слоях, и тем самым искусственно варьировать свойства данных структур.},\n\tlanguage = {ru},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Science in the South of Russia},\n\tauthor = {Бабарикин, Д.С. and Разумная, А.Г. and Стрюков, Д.В. and Анохин, А.С. and Михейкин, А.С. and Павленко, А.В. and Широков, В.Б. and Зинченко, С.П. and Мухортов, В.М.},\n\tyear = {2019},\n\tpages = {21--30},\n\tfile = {Бабарикин и др. - 2019 - Температурная зависимость фононных и магнонных мод.pdf:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\2GW49MUE\\\\Бабарикин и др. - 2019 - Температурная зависимость фононных и магнонных мод.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Пленки феррита висмута BiFeO выращены на монокристаллической подложке (001) MgO по блочному механизму роста методом высокочастотного катодного распыления с использованием в качестве буферного слоя сегнетоэлектрика BaSr _ TiO при варьировании состава x. Изучение гетероструктур методом рентгеновской дифракции показало, что пленки характеризуются псевдотетрагональной симметрией при комнатной температуре. Определено, что степень тетрагонального искажения слоев BaSr _ TiO возрастает с увеличением концентрации Ba, в то время как в слоях BiFeO она остается практически неизменной. Методом атомно-силовой микроскопии установлено, что пленки BiFeOвыросли по блочному механизму роста, причем блоки строго ориентированы относительно друг друга и кристаллографических осей подложки MgO. Высокотемпературные исследования спектров комбинационного рассеяния света в широком диапазоне температур 295-900 K и частот от 50 до 1600 смпоказали, что интенсивность полосы 1250 см, соответствующей плотности состояний двухмагнонных возбуждений, линейно понижается при повышении температуры. Анализ температурного поведения полосы 1250 см позволяет предполагать, что в изученных пленках BiFeO антиферромагнитный фазовый переход происходит в диапазоне температур 600-700 K. Использование сегнетоэлектрических буферных слоев BaSr _ TiO с разной степенью тетрагонального искажения позволяет управлять деформацией пленок BiFeO, возникающей в результате несоответствия параметров решеток в смежных слоях, и тем самым искусственно варьировать свойства данных структур.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"maslova-iltis-desgranges-ammar-genevois-debilbao-canizars-barannikova-etal-characterizationofanuotextrm2ceramicviaramanimagingandelectronbackscatteringdiffraction-2019\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S1044580318315651\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'maslova-iltis-desgranges-ammar-genevois-debilbao-canizars-barannikova-etal-characterizationofanuotextrm2ceramicviaramanimagingandelectronbackscatteringdiffraction-2019', 'https://www.sciencedirect.com/science/article/pii/S1044580318315651', event);\">\n    Characterization of an UO$_{\\textrm{2}}$ ceramic via Raman imaging and electron back-scattering diffraction.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Maslova, O. A.; Iltis, X.; Desgranges, L.; Ammar, M. R.; Genevois, C.; de Bilbao, E.; Canizarès, A.; Barannikova, S. A.; Leontyev, I. N.;  and Simon, P.\n</span>\n\n  \n\n</span>\n\n  <i>Materials Characterization</i>, 147: 280–285. January 2019.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S1044580318315651\"\n     onclick=\"log_download('maslova-iltis-desgranges-ammar-genevois-debilbao-canizars-barannikova-etal-characterizationofanuotextrm2ceramicviaramanimagingandelectronbackscatteringdiffraction-2019', 'https://www.sciencedirect.com/science/article/pii/S1044580318315651', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Characterization of an UO$_{\\textrm{2}}$ ceramic via Raman imaging and electron back-scattering diffraction [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.matchar.2018.11.006\"\n     onclick=\"log_download('maslova-iltis-desgranges-ammar-genevois-debilbao-canizars-barannikova-etal-characterizationofanuotextrm2ceramicviaramanimagingandelectronbackscatteringdiffraction-2019', 'http://doi.org/10.1016/j.matchar.2018.11.006', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/maslova-iltis-desgranges-ammar-genevois-debilbao-canizars-barannikova-etal-characterizationofanuotextrm2ceramicviaramanimagingandelectronbackscatteringdiffraction-2019\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('maslova-iltis-desgranges-ammar-genevois-debilbao-canizars-barannikova-etal-characterizationofanuotextrm2ceramicviaramanimagingandelectronbackscatteringdiffraction-2019')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{maslova_characterization_2019,\n\ttitle = {Characterization of an {UO}$_{\\textrm{2}}$ ceramic via {Raman} imaging and electron back-scattering diffraction},\n\tvolume = {147},\n\tissn = {1044-5803},\n\turl = {https://www.sciencedirect.com/science/article/pii/S1044580318315651},\n\tdoi = {10.1016/j.matchar.2018.11.006},\n\tabstract = {A surface state analysis of an UO2 ceramic is performed by combining Raman imaging and electron back-scattering diffraction. Special attention is paid to the behavior of the T2g band intensity versus the crystalline orientation. In order to clarify the origin of the T2g intensity variation in the appropriate Raman image, electron back-scattering diffraction (EBSD) measurements are carried out. EBSD data allow a theoretical estimation of the Raman T2g band intensities. Both maps have been compared in order to correlate them, and to distinguish regions where they are analogous, from those where some physical or chemical effects (stoichiometry, or strains) induce different behavior. More generally, this highlights the interest and the complementarity of combining Raman spectroscopy and EBSD for a better microstructure knowledge.},\n\turldate = {2023-11-11},\n\tjournal = {Materials Characterization},\n\tauthor = {Maslova, O. A. and Iltis, X. and Desgranges, L. and Ammar, M. R. and Genevois, C. and de Bilbao, E. and Canizarès, A. and Barannikova, S. A. and Leontyev, I. N. and Simon, P.},\n\tmonth = jan,\n\tyear = {2019},\n\tkeywords = {Crystalline orientation, Crystallographic indices, EBSD, Euler angles, Pole figures, Raman imaging, T band, UO},\n\tpages = {280--285},\n\tfile = {ScienceDirect Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\IZ29TZSV\\\\S1044580318315651.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A surface state analysis of an UO2 ceramic is performed by combining Raman imaging and electron back-scattering diffraction. Special attention is paid to the behavior of the T2g band intensity versus the crystalline orientation. In order to clarify the origin of the T2g intensity variation in the appropriate Raman image, electron back-scattering diffraction (EBSD) measurements are carried out. EBSD data allow a theoretical estimation of the Raman T2g band intensities. Both maps have been compared in order to correlate them, and to distinguish regions where they are analogous, from those where some physical or chemical effects (stoichiometry, or strains) induce different behavior. More generally, this highlights the interest and the complementarity of combining Raman spectroscopy and EBSD for a better microstructure knowledge.\n</div>\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2018\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2018')\"\n      onkeypress=\"toggleGroup('group_2018')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2018</span>\n      <span class=\"bibbase_group_count\">\n        \n        (27)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"chernysheva-vlaic-leontyev-pudova-ivanov-avramenko-allix-rakhmatullin-etal-synthesisofco3o4cooohviaelectrochemicaldispersionusingapulsealternatingcurrentmethodforlithiumionbatteriesandsupercapacitors-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S129325581830551X\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'chernysheva-vlaic-leontyev-pudova-ivanov-avramenko-allix-rakhmatullin-etal-synthesisofco3o4cooohviaelectrochemicaldispersionusingapulsealternatingcurrentmethodforlithiumionbatteriesandsupercapacitors-2018', 'https://www.sciencedirect.com/science/article/pii/S129325581830551X', event);\">\n    Synthesis of Co3O4/CoOOH via electrochemical dispersion using a pulse alternating current method for lithium-ion batteries and supercapacitors.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Chernysheva, D.; Vlaic, C.; Leontyev, I.; Pudova, L.; Ivanov, S.; Avramenko, M.; Allix, M.; Rakhmatullin, A.; Maslova, O.; Bund, A.;  and Smirnova, N.\n</span>\n\n  \n\n</span>\n\n  <i>Solid State Sciences</i>, 86: 53–59. December 2018.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S129325581830551X\"\n     onclick=\"log_download('chernysheva-vlaic-leontyev-pudova-ivanov-avramenko-allix-rakhmatullin-etal-synthesisofco3o4cooohviaelectrochemicaldispersionusingapulsealternatingcurrentmethodforlithiumionbatteriesandsupercapacitors-2018', 'https://www.sciencedirect.com/science/article/pii/S129325581830551X', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Synthesis of Co3O4/CoOOH via electrochemical dispersion using a pulse alternating current method for lithium-ion batteries and supercapacitors [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.solidstatesciences.2018.10.005\"\n     onclick=\"log_download('chernysheva-vlaic-leontyev-pudova-ivanov-avramenko-allix-rakhmatullin-etal-synthesisofco3o4cooohviaelectrochemicaldispersionusingapulsealternatingcurrentmethodforlithiumionbatteriesandsupercapacitors-2018', 'http://doi.org/10.1016/j.solidstatesciences.2018.10.005', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/chernysheva-vlaic-leontyev-pudova-ivanov-avramenko-allix-rakhmatullin-etal-synthesisofco3o4cooohviaelectrochemicaldispersionusingapulsealternatingcurrentmethodforlithiumionbatteriesandsupercapacitors-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('chernysheva-vlaic-leontyev-pudova-ivanov-avramenko-allix-rakhmatullin-etal-synthesisofco3o4cooohviaelectrochemicaldispersionusingapulsealternatingcurrentmethodforlithiumionbatteriesandsupercapacitors-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{chernysheva_synthesis_2018,\n\ttitle = {Synthesis of {Co3O4}/{CoOOH} via electrochemical dispersion using a pulse alternating current method for lithium-ion batteries and supercapacitors},\n\tvolume = {86},\n\tissn = {1293-2558},\n\turl = {https://www.sciencedirect.com/science/article/pii/S129325581830551X},\n\tdoi = {10.1016/j.solidstatesciences.2018.10.005},\n\tabstract = {We report a convenient, low-cost and ecofriendly approach for the fabrication of a Co3O4/CoOOH electrode material intended for lithium ion batteries (LIBs) and supercapacitors (SCs) using the electrochemical dispersion of the cobalt foil through the pulse alternating current (PAC) method. The synthesized material is a Co3O4/CoOOH composite (with about 10–15 wt\\% CoOOH) in the form of nanosheets with a length of approximately 200 nm and a thickness of 10–20 nm. It is found to exhibit high reversible discharge specific capacities and good cycling behavior while tested as the anode material in LIBs. Measuring the reversible capacitance at high (2C) and low (C/20) cycling rates gives the values of 610 mAh g−1 and 1030 mAh g−1, respectively. The specimen possesses excellent performance as the electrode for SCs with the retention of capacitance up to 98\\% at the current density increasing from 0.5 to 10 A g−1. After 1000 cycles at a current density of 10 A g−1 the electrode maintains about 90\\% of its initial capacitance which evidences the long cycle life. Hence, electrochemically prepared Co3O4/CoOOH seems to be a promising candidate for high-performance LIBs and SCs applications.},\n\turldate = {2023-11-11},\n\tjournal = {Solid State Sciences},\n\tauthor = {Chernysheva, Daria and Vlaic, Codruta and Leontyev, Igor and Pudova, Lyudmila and Ivanov, Svetlozar and Avramenko, Marina and Allix, Mathieu and Rakhmatullin, Aydar and Maslova, Olga and Bund, Andreas and Smirnova, Nina},\n\tmonth = dec,\n\tyear = {2018},\n\tpages = {53--59},\n\tfile = {ScienceDirect Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\9GU5I35X\\\\S129325581830551X.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We report a convenient, low-cost and ecofriendly approach for the fabrication of a Co3O4/CoOOH electrode material intended for lithium ion batteries (LIBs) and supercapacitors (SCs) using the electrochemical dispersion of the cobalt foil through the pulse alternating current (PAC) method. The synthesized material is a Co3O4/CoOOH composite (with about 10–15 wt% CoOOH) in the form of nanosheets with a length of approximately 200 nm and a thickness of 10–20 nm. It is found to exhibit high reversible discharge specific capacities and good cycling behavior while tested as the anode material in LIBs. Measuring the reversible capacitance at high (2C) and low (C/20) cycling rates gives the values of 610 mAh g−1 and 1030 mAh g−1, respectively. The specimen possesses excellent performance as the electrode for SCs with the retention of capacitance up to 98% at the current density increasing from 0.5 to 10 A g−1. After 1000 cycles at a current density of 10 A g−1 the electrode maintains about 90% of its initial capacitance which evidences the long cycle life. Hence, electrochemically prepared Co3O4/CoOOH seems to be a promising candidate for high-performance LIBs and SCs applications.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kulbakov-kuriganova-allix-rakhmatullin-smirnova-maslova-leontyev-nonisothermaldecompositionofplatinumacetylacetonateasacostefficientandsizecontrolledsynthesisofptcnanoparticles-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S1566736718303686\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kulbakov-kuriganova-allix-rakhmatullin-smirnova-maslova-leontyev-nonisothermaldecompositionofplatinumacetylacetonateasacostefficientandsizecontrolledsynthesisofptcnanoparticles-2018', 'https://www.sciencedirect.com/science/article/pii/S1566736718303686', event);\">\n    Non-isothermal decomposition of platinum acetylacetonate as a cost-efficient and Size-Controlled Synthesis of Pt/C nanoparticles.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kulbakov, A. A.; Kuriganova, A. B.; Allix, M.; Rakhmatullin, A.; Smirnova, N.; Maslova, O. A.;  and Leontyev, I. N.\n</span>\n\n  \n\n</span>\n\n  <i>Catalysis Communications</i>, 117: 14–18. December 2018.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S1566736718303686\"\n     onclick=\"log_download('kulbakov-kuriganova-allix-rakhmatullin-smirnova-maslova-leontyev-nonisothermaldecompositionofplatinumacetylacetonateasacostefficientandsizecontrolledsynthesisofptcnanoparticles-2018', 'https://www.sciencedirect.com/science/article/pii/S1566736718303686', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Non-isothermal decomposition of platinum acetylacetonate as a cost-efficient and Size-Controlled Synthesis of Pt/C nanoparticles [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.catcom.2018.08.022\"\n     onclick=\"log_download('kulbakov-kuriganova-allix-rakhmatullin-smirnova-maslova-leontyev-nonisothermaldecompositionofplatinumacetylacetonateasacostefficientandsizecontrolledsynthesisofptcnanoparticles-2018', 'http://doi.org/10.1016/j.catcom.2018.08.022', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kulbakov-kuriganova-allix-rakhmatullin-smirnova-maslova-leontyev-nonisothermaldecompositionofplatinumacetylacetonateasacostefficientandsizecontrolledsynthesisofptcnanoparticles-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kulbakov-kuriganova-allix-rakhmatullin-smirnova-maslova-leontyev-nonisothermaldecompositionofplatinumacetylacetonateasacostefficientandsizecontrolledsynthesisofptcnanoparticles-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kulbakov_non-isothermal_2018,\n\ttitle = {Non-isothermal decomposition of platinum acetylacetonate as a cost-efficient and {Size}-{Controlled} {Synthesis} of {Pt}/{C} nanoparticles},\n\tvolume = {117},\n\tissn = {1566-7367},\n\turl = {https://www.sciencedirect.com/science/article/pii/S1566736718303686},\n\tdoi = {10.1016/j.catcom.2018.08.022},\n\tabstract = {A simple two-stage synthesis of Pt/C nanoparticles based on the non-isothermal decomposition of platinum acetylacetonate is presented. It allows not only production of Pt nanoparticles, but also their sizes control during the synthesis. The heating rate is the key factor for tuning the average Pt nanoparticle size. The electrochemical surface area of produced nanoparticles enlarges with rising heating rate, which can enrich 103 m2/g. The growth dynamics of Pt/C nanoparticles is tracked via in-situ XRD. Furthermore, the electrocatalytic activity of Pt/C catalysts is studied as a function of platinum particle size in cases of ethanol electro-oxidation and oxygen reduction reactions.},\n\turldate = {2023-11-11},\n\tjournal = {Catalysis Communications},\n\tauthor = {Kulbakov, Anton A. and Kuriganova, Alexandra B. and Allix, Mathieu and Rakhmatullin, Aydar and Smirnova, NinaV. and Maslova, Olga A. and Leontyev, Igor N.},\n\tmonth = dec,\n\tyear = {2018},\n\tkeywords = {Pt/C, In-situ, Pt acetylacetonate, Size control, Thermal decomposition},\n\tpages = {14--18},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A simple two-stage synthesis of Pt/C nanoparticles based on the non-isothermal decomposition of platinum acetylacetonate is presented. It allows not only production of Pt nanoparticles, but also their sizes control during the synthesis. The heating rate is the key factor for tuning the average Pt nanoparticle size. The electrochemical surface area of produced nanoparticles enlarges with rising heating rate, which can enrich 103 m2/g. The growth dynamics of Pt/C nanoparticles is tracked via in-situ XRD. Furthermore, the electrocatalytic activity of Pt/C catalysts is studied as a function of platinum particle size in cases of ethanol electro-oxidation and oxygen reduction reactions.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"pryadchenko-belenov-shemet-srabionyan-avakyan-volochaev-mikheykin-bdoyan-etal-effectofthermaltreatmentontheatomicstructureandelectrochemicalcharacteristicsofbimetallicptcucoreshellnanoparticlesinptcucelectrocatalysts-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1021/acs.jpcc.8b03696\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'pryadchenko-belenov-shemet-srabionyan-avakyan-volochaev-mikheykin-bdoyan-etal-effectofthermaltreatmentontheatomicstructureandelectrochemicalcharacteristicsofbimetallicptcucoreshellnanoparticlesinptcucelectrocatalysts-2018', 'https://doi.org/10.1021/acs.jpcc.8b03696', event);\">\n    Effect of Thermal Treatment on the Atomic Structure and Electrochemical Characteristics of Bimetallic PtCu Core–Shell Nanoparticles in PtCu/C Electrocatalysts.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Pryadchenko, V. V.; Belenov, S. V.; Shemet, D. B.; Srabionyan, V. V.; Avakyan, L. A.; Volochaev, V. A.; Mikheykin, A. S.; Bdoyan, K. E.; Zizak, I.; Guterman, V. E.;  and Bugaev, L. A.\n</span>\n\n  \n\n</span>\n\n  <i>The Journal of Physical Chemistry C</i>, 122(30): 17199–17210. August 2018.\n  <span class=\"note\">Publisher: American Chemical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1021/acs.jpcc.8b03696\"\n     onclick=\"log_download('pryadchenko-belenov-shemet-srabionyan-avakyan-volochaev-mikheykin-bdoyan-etal-effectofthermaltreatmentontheatomicstructureandelectrochemicalcharacteristicsofbimetallicptcucoreshellnanoparticlesinptcucelectrocatalysts-2018', 'https://doi.org/10.1021/acs.jpcc.8b03696', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Effect of Thermal Treatment on the Atomic Structure and Electrochemical Characteristics of Bimetallic PtCu Core–Shell Nanoparticles in PtCu/C Electrocatalysts [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1021/acs.jpcc.8b03696\"\n     onclick=\"log_download('pryadchenko-belenov-shemet-srabionyan-avakyan-volochaev-mikheykin-bdoyan-etal-effectofthermaltreatmentontheatomicstructureandelectrochemicalcharacteristicsofbimetallicptcucoreshellnanoparticlesinptcucelectrocatalysts-2018', 'http://doi.org/10.1021/acs.jpcc.8b03696', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/pryadchenko-belenov-shemet-srabionyan-avakyan-volochaev-mikheykin-bdoyan-etal-effectofthermaltreatmentontheatomicstructureandelectrochemicalcharacteristicsofbimetallicptcucoreshellnanoparticlesinptcucelectrocatalysts-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('pryadchenko-belenov-shemet-srabionyan-avakyan-volochaev-mikheykin-bdoyan-etal-effectofthermaltreatmentontheatomicstructureandelectrochemicalcharacteristicsofbimetallicptcucoreshellnanoparticlesinptcucelectrocatalysts-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{pryadchenko_effect_2018,\n\ttitle = {Effect of {Thermal} {Treatment} on the {Atomic} {Structure} and {Electrochemical} {Characteristics} of {Bimetallic} {PtCu} {Core}–{Shell} {Nanoparticles} in {PtCu}/{C} {Electrocatalysts}},\n\tvolume = {122},\n\tissn = {1932-7447},\n\turl = {https://doi.org/10.1021/acs.jpcc.8b03696},\n\tdoi = {10.1021/acs.jpcc.8b03696},\n\tabstract = {Supported PtCu/C electrocatalysts containing core–shell bimetallic PtCu nanoparticles were synthesized by sequential chemical reduction of Cu2+ and Pt(IV) in a carbon suspension, prepared on the basis of ethylene glycol–water solvent, and then treated at different temperatures in the range from 250 to 350 °C. The structural characterization of “as-prepared” PtCu nanoparticles and of those obtained after the thermal treatments was performed by transmission electron microscopy, X-ray diffraction, and Pt L3- and Cu K-edge extended X-ray absorption fine structure spectroscopy. The atomic cluster models of PtCu nanoparticles before and after the thermal treatment, reflecting the character of the components’ distribution, were generated. The electrochemical performance of the obtained PtCu/C electrocatalysts in oxygen reduction reaction was studied by cycling and linear voltammetry.},\n\tnumber = {30},\n\turldate = {2023-11-11},\n\tjournal = {The Journal of Physical Chemistry C},\n\tauthor = {Pryadchenko, Vasiliy V. and Belenov, Sergey V. and Shemet, Darya B. and Srabionyan, Vasiliy V. and Avakyan, Leon A. and Volochaev, Vadim A. and Mikheykin, Alexey S. and Bdoyan, Karina E. and Zizak, Ivo and Guterman, Vladimir E. and Bugaev, Lusegen A.},\n\tmonth = aug,\n\tyear = {2018},\n\tnote = {Publisher: American Chemical Society},\n\tpages = {17199--17210},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Supported PtCu/C electrocatalysts containing core–shell bimetallic PtCu nanoparticles were synthesized by sequential chemical reduction of Cu2+ and Pt(IV) in a carbon suspension, prepared on the basis of ethylene glycol–water solvent, and then treated at different temperatures in the range from 250 to 350 °C. The structural characterization of “as-prepared” PtCu nanoparticles and of those obtained after the thermal treatments was performed by transmission electron microscopy, X-ray diffraction, and Pt L3- and Cu K-edge extended X-ray absorption fine structure spectroscopy. The atomic cluster models of PtCu nanoparticles before and after the thermal treatment, reflecting the character of the components’ distribution, were generated. The electrochemical performance of the obtained PtCu/C electrocatalysts in oxygen reduction reaction was studied by cycling and linear voltammetry.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kuriganova-leontev-smirnova-ptirccatalystssynthesizedbyelectrochemicaldispersionmethodforprotonexchangemembranefuelcells-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1023193518060113\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kuriganova-leontev-smirnova-ptirccatalystssynthesizedbyelectrochemicaldispersionmethodforprotonexchangemembranefuelcells-2018', 'https://doi.org/10.1134/S1023193518060113', event);\">\n    PtIr/C Catalysts Synthesized by Electrochemical Dispersion Method for Proton Exchange Membrane Fuel Cells.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kuriganova, A. B.; Leont’ev, I. N.;  and Smirnova, N. V.\n</span>\n\n  \n\n</span>\n\n  <i>Russian Journal of Electrochemistry</i>, 54(6): 561–565. June 2018.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1023193518060113\"\n     onclick=\"log_download('kuriganova-leontev-smirnova-ptirccatalystssynthesizedbyelectrochemicaldispersionmethodforprotonexchangemembranefuelcells-2018', 'https://doi.org/10.1134/S1023193518060113', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"PtIr/C Catalysts Synthesized by Electrochemical Dispersion Method for Proton Exchange Membrane Fuel Cells [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1023193518060113\"\n     onclick=\"log_download('kuriganova-leontev-smirnova-ptirccatalystssynthesizedbyelectrochemicaldispersionmethodforprotonexchangemembranefuelcells-2018', 'http://doi.org/10.1134/S1023193518060113', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kuriganova-leontev-smirnova-ptirccatalystssynthesizedbyelectrochemicaldispersionmethodforprotonexchangemembranefuelcells-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kuriganova-leontev-smirnova-ptirccatalystssynthesizedbyelectrochemicaldispersionmethodforprotonexchangemembranefuelcells-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kuriganova_ptirc_2018,\n\ttitle = {{PtIr}/{C} {Catalysts} {Synthesized} by {Electrochemical} {Dispersion} {Method} for {Proton} {Exchange} {Membrane} {Fuel} {Cells}},\n\tvolume = {54},\n\tissn = {1608-3342},\n\turl = {https://doi.org/10.1134/S1023193518060113},\n\tdoi = {10.1134/S1023193518060113},\n\tabstract = {PtIr/C electrocatalyst with the metal phase uniformly distributed over the carbon support surface and the average size of PtIr nanoparticles of 5.9 nm is synthesized by electrochemical dispersion of Pt90Ir10 alloy under the action of alternating pulse current. It is shown that the presence of iridium within the composition of a Pt/C catalyst lowers down the overpotential of CO oxidation and increases catalyst’s specific activity with respect to electrochemical oxidation of ethanol.},\n\tlanguage = {en},\n\tnumber = {6},\n\turldate = {2023-11-11},\n\tjournal = {Russian Journal of Electrochemistry},\n\tauthor = {Kuriganova, A. B. and Leont’ev, I. N. and Smirnova, N. V.},\n\tmonth = jun,\n\tyear = {2018},\n\tkeywords = {electrochemical dispersion, fuel cell, electrocatalysis, platinum, iridium},\n\tpages = {561--565},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  PtIr/C electrocatalyst with the metal phase uniformly distributed over the carbon support surface and the average size of PtIr nanoparticles of 5.9 nm is synthesized by electrochemical dispersion of Pt90Ir10 alloy under the action of alternating pulse current. It is shown that the presence of iridium within the composition of a Pt/C catalyst lowers down the overpotential of CO oxidation and increases catalyst’s specific activity with respect to electrochemical oxidation of ethanol.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"dmitriev-chernyshov-dyadkin-makarova-leontyev-andronikova-bronwald-burkovsky-etal-crystallographybasedonsynchrotronradiationexperimentsofrussianusersoftheesrfbm01diffractionbeamline-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1027451018030084\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'dmitriev-chernyshov-dyadkin-makarova-leontyev-andronikova-bronwald-burkovsky-etal-crystallographybasedonsynchrotronradiationexperimentsofrussianusersoftheesrfbm01diffractionbeamline-2018', 'https://doi.org/10.1134/S1027451018030084', event);\">\n    Crystallography Based on Synchrotron Radiation: Experiments of Russian Users of the ESRF BM01 Diffraction Beam Line.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Dmitriev, V. P.; Chernyshov, D. Y.; Dyadkin, V. A.; Makarova, I. P.; Leontyev, I. N.; Andronikova, D. A.; Bronwald, I.; Burkovsky, R. G.; Vakhrushev, S. B.; Filimonov, A. V.;  and Grigoriev, S. V.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Surface Investigation: X-ray, Synchrotron and Neutron Techniques</i>, 12(3): 395–407. May 2018.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1027451018030084\"\n     onclick=\"log_download('dmitriev-chernyshov-dyadkin-makarova-leontyev-andronikova-bronwald-burkovsky-etal-crystallographybasedonsynchrotronradiationexperimentsofrussianusersoftheesrfbm01diffractionbeamline-2018', 'https://doi.org/10.1134/S1027451018030084', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Crystallography Based on Synchrotron Radiation: Experiments of Russian Users of the ESRF BM01 Diffraction Beam Line [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1027451018030084\"\n     onclick=\"log_download('dmitriev-chernyshov-dyadkin-makarova-leontyev-andronikova-bronwald-burkovsky-etal-crystallographybasedonsynchrotronradiationexperimentsofrussianusersoftheesrfbm01diffractionbeamline-2018', 'http://doi.org/10.1134/S1027451018030084', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/dmitriev-chernyshov-dyadkin-makarova-leontyev-andronikova-bronwald-burkovsky-etal-crystallographybasedonsynchrotronradiationexperimentsofrussianusersoftheesrfbm01diffractionbeamline-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('dmitriev-chernyshov-dyadkin-makarova-leontyev-andronikova-bronwald-burkovsky-etal-crystallographybasedonsynchrotronradiationexperimentsofrussianusersoftheesrfbm01diffractionbeamline-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{dmitriev_crystallography_2018,\n\ttitle = {Crystallography {Based} on {Synchrotron} {Radiation}: {Experiments} of {Russian} {Users} of the {ESRF} {BM01} {Diffraction} {Beam} {Line}},\n\tvolume = {12},\n\tissn = {1819-7094},\n\tshorttitle = {Crystallography {Based} on {Synchrotron} {Radiation}},\n\turl = {https://doi.org/10.1134/S1027451018030084},\n\tdoi = {10.1134/S1027451018030084},\n\tabstract = {The review deals with studies carried out at the BM01 diffraction beam line of the European Synchrotron Radiation Facility. X-ray diffraction analysis of single-crystal proton conductors demonstrates the possibilities of a precise diffraction experiment in which phase transitions associated with the release of crystallization water and transformation of the network of hydrogen contacts are investigated. Scanning of reciprocal space with the help of a 2D detector enables us to determine the new phase symmetry in a thin-film multiferroic sample based on bismuth ferrite (the given phase is stable only under thin-film conditions). A combination of Bragg and diffusion scattering processes is employed to investigate the interdependence between the structure and dynamics of a crystal lattice and the physical properties of a relaxor material with a perovskite-like structure. The complementarity and synergy of neutron and synchrotron experiments are demonstrated using the combined study of materials from the manganese-silicide group, which has revealed a nontrivial relationship between magnetic and crystallographic chiralities in noncollinear magnets. Although the given review is limited to only a few experiments carried out by Russian scientists at the BM01 beam line, they still illustrate a variety of problems that can be solved using a modern diffraction station where the bending magnet of a third-generation synchrotron is employed as the synchrotron radiation source.},\n\tlanguage = {en},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Surface Investigation: X-ray, Synchrotron and Neutron Techniques},\n\tauthor = {Dmitriev, V. P. and Chernyshov, D. Yu. and Dyadkin, V. A. and Makarova, I. P. and Leontyev, I. N. and Andronikova, D. A. and Bronwald, I. and Burkovsky, R. G. and Vakhrushev, S. B. and Filimonov, A. V. and Grigoriev, S. V.},\n\tmonth = may,\n\tyear = {2018},\n\tkeywords = {crystallography, synchrotron X-ray diffraction, X-ray analysis},\n\tpages = {395--407},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The review deals with studies carried out at the BM01 diffraction beam line of the European Synchrotron Radiation Facility. X-ray diffraction analysis of single-crystal proton conductors demonstrates the possibilities of a precise diffraction experiment in which phase transitions associated with the release of crystallization water and transformation of the network of hydrogen contacts are investigated. Scanning of reciprocal space with the help of a 2D detector enables us to determine the new phase symmetry in a thin-film multiferroic sample based on bismuth ferrite (the given phase is stable only under thin-film conditions). A combination of Bragg and diffusion scattering processes is employed to investigate the interdependence between the structure and dynamics of a crystal lattice and the physical properties of a relaxor material with a perovskite-like structure. The complementarity and synergy of neutron and synchrotron experiments are demonstrated using the combined study of materials from the manganese-silicide group, which has revealed a nontrivial relationship between magnetic and crystallographic chiralities in noncollinear magnets. Although the given review is limited to only a few experiments carried out by Russian scientists at the BM01 beam line, they still illustrate a variety of problems that can be solved using a modern diffraction station where the bending magnet of a third-generation synchrotron is employed as the synchrotron radiation source.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-pavlenko-stryukov-revinskii-opticalpropertiesofbariumstrontiumniobatesbn61films-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1063783418050293\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-pavlenko-stryukov-revinskii-opticalpropertiesofbariumstrontiumniobatesbn61films-2018', 'https://doi.org/10.1134/S1063783418050293', event);\">\n    Optical Properties of Barium Strontium Niobate SBN61 Films.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.; Pavlenko, A. V.; Stryukov, D. V.;  and Revinskii, Y. V.\n</span>\n\n  \n\n</span>\n\n  <i>Physics of the Solid State</i>, 60(5): 1005–1010. May 2018.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1063783418050293\"\n     onclick=\"log_download('shirokov-pavlenko-stryukov-revinskii-opticalpropertiesofbariumstrontiumniobatesbn61films-2018', 'https://doi.org/10.1134/S1063783418050293', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Optical Properties of Barium Strontium Niobate SBN61 Films [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1063783418050293\"\n     onclick=\"log_download('shirokov-pavlenko-stryukov-revinskii-opticalpropertiesofbariumstrontiumniobatesbn61films-2018', 'http://doi.org/10.1134/S1063783418050293', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-pavlenko-stryukov-revinskii-opticalpropertiesofbariumstrontiumniobatesbn61films-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-pavlenko-stryukov-revinskii-opticalpropertiesofbariumstrontiumniobatesbn61films-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_optical_2018,\n\ttitle = {Optical {Properties} of {Barium} {Strontium} {Niobate} {SBN61} {Films}},\n\tvolume = {60},\n\tissn = {1090-6460},\n\turl = {https://doi.org/10.1134/S1063783418050293},\n\tdoi = {10.1134/S1063783418050293},\n\tabstract = {Heteroepitaxial Sr0.61Ba0.39Nb2O6 films have been formed on MgO(001) substrates by RF deposition in an oxygen atmosphere. The film orientation with respect to the substrate is investigated using X-ray diffraction. The permittivity dispersion parameters in the visible range are determined by measuring optical transmission spectra. The films are found to have a wider band gap and a smaller refractive index as compared with the single-crystal material.},\n\tlanguage = {en},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Physics of the Solid State},\n\tauthor = {Shirokov, V. B. and Pavlenko, A. V. and Stryukov, D. V. and Revinskii, Yu. V.},\n\tmonth = may,\n\tyear = {2018},\n\tpages = {1005--1010},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Heteroepitaxial Sr0.61Ba0.39Nb2O6 films have been formed on MgO(001) substrates by RF deposition in an oxygen atmosphere. The film orientation with respect to the substrate is investigated using X-ray diffraction. The permittivity dispersion parameters in the visible range are determined by measuring optical transmission spectra. The films are found to have a wider band gap and a smaller refractive index as compared with the single-crystal material.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kuriganova-leontyev-maslova-smirnova-electrochemicallysynthesizedptbasedcatalystswithdifferentcarbonsupportsforprotonexchangemembranefuelcellapplications-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0959943618301834\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kuriganova-leontyev-maslova-smirnova-electrochemicallysynthesizedptbasedcatalystswithdifferentcarbonsupportsforprotonexchangemembranefuelcellapplications-2018', 'https://www.sciencedirect.com/science/article/pii/S0959943618301834', event);\">\n    Electrochemically synthesized Pt-based catalysts with different carbon supports for proton exchange membrane fuel cell applications.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kuriganova, A. B.; Leontyev, I. N.; Maslova, O. A.;  and Smirnova, N. V.\n</span>\n\n  \n\n</span>\n\n  <i>Mendeleev Communications</i>, 28(4): 444–446. July 2018.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0959943618301834\"\n     onclick=\"log_download('kuriganova-leontyev-maslova-smirnova-electrochemicallysynthesizedptbasedcatalystswithdifferentcarbonsupportsforprotonexchangemembranefuelcellapplications-2018', 'https://www.sciencedirect.com/science/article/pii/S0959943618301834', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Electrochemically synthesized Pt-based catalysts with different carbon supports for proton exchange membrane fuel cell applications [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.mencom.2018.07.036\"\n     onclick=\"log_download('kuriganova-leontyev-maslova-smirnova-electrochemicallysynthesizedptbasedcatalystswithdifferentcarbonsupportsforprotonexchangemembranefuelcellapplications-2018', 'http://doi.org/10.1016/j.mencom.2018.07.036', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kuriganova-leontyev-maslova-smirnova-electrochemicallysynthesizedptbasedcatalystswithdifferentcarbonsupportsforprotonexchangemembranefuelcellapplications-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kuriganova-leontyev-maslova-smirnova-electrochemicallysynthesizedptbasedcatalystswithdifferentcarbonsupportsforprotonexchangemembranefuelcellapplications-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kuriganova_electrochemically_2018,\n\ttitle = {Electrochemically synthesized {Pt}-based catalysts with different carbon supports for proton exchange membrane fuel cell applications},\n\tvolume = {28},\n\tissn = {0959-9436},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0959943618301834},\n\tdoi = {10.1016/j.mencom.2018.07.036},\n\tabstract = {The Pt/C catalysts containing various types of carbon support were prepared via electrochemical oxidation/dispersion. Their different catalytic activity in CO-stripping and ethanol electrooxidation was revealed.},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Mendeleev Communications},\n\tauthor = {Kuriganova, Alexandra B. and Leontyev, Igor N. and Maslova, Olga A. and Smirnova, Nina V.},\n\tmonth = jul,\n\tyear = {2018},\n\tpages = {444--446},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The Pt/C catalysts containing various types of carbon support were prepared via electrochemical oxidation/dispersion. Their different catalytic activity in CO-stripping and ethanol electrooxidation was revealed.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-kalinchuk-timoshenko-electricfielddependentmechanicalandelectricalpropertiesofbariumstrontiumtitanatefilmsfortunabledeviceapplications-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0040609018302918\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-kalinchuk-timoshenko-electricfielddependentmechanicalandelectricalpropertiesofbariumstrontiumtitanatefilmsfortunabledeviceapplications-2018', 'https://www.sciencedirect.com/science/article/pii/S0040609018302918', event);\">\n    Electric-field-dependent mechanical and electrical properties of barium strontium titanate films for tunable device applications.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.; Kalinchuk, V. V.;  and Timoshenko, P. E.\n</span>\n\n  \n\n</span>\n\n  <i>Thin Solid Films</i>, 657: 8–15. July 2018.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0040609018302918\"\n     onclick=\"log_download('shirokov-kalinchuk-timoshenko-electricfielddependentmechanicalandelectricalpropertiesofbariumstrontiumtitanatefilmsfortunabledeviceapplications-2018', 'https://www.sciencedirect.com/science/article/pii/S0040609018302918', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Electric-field-dependent mechanical and electrical properties of barium strontium titanate films for tunable device applications [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.tsf.2018.04.029\"\n     onclick=\"log_download('shirokov-kalinchuk-timoshenko-electricfielddependentmechanicalandelectricalpropertiesofbariumstrontiumtitanatefilmsfortunabledeviceapplications-2018', 'http://doi.org/10.1016/j.tsf.2018.04.029', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-kalinchuk-timoshenko-electricfielddependentmechanicalandelectricalpropertiesofbariumstrontiumtitanatefilmsfortunabledeviceapplications-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-kalinchuk-timoshenko-electricfielddependentmechanicalandelectricalpropertiesofbariumstrontiumtitanatefilmsfortunabledeviceapplications-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_electric-field-dependent_2018,\n\ttitle = {Electric-field-dependent mechanical and electrical properties of barium strontium titanate films for tunable device applications},\n\tvolume = {657},\n\tissn = {0040-6090},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0040609018302918},\n\tdoi = {10.1016/j.tsf.2018.04.029},\n\tabstract = {Developing the novel electric field tunable, reconfigurable, adaptive and frequency-agile microwave devices with specific properties involves technological and scientific activities in the studying of material properties. Measurements of its properties could be a difficult and expensive issue, especially when it concerns thin-film ferroelectrics. Their electromechanical properties change significantly under applied DC bias field. The material coefficients of barium strontium titanate thin films are still unknown; therefore, it is expedient to carry out their calculations. In the present paper, the linear equations of piezoelectric effect have been written for thin barium strontium titanate films under DC bias electric field in paraelectric phase (induced piezoelectric effect) based on the grand potential of Landau theory of phase transitions. The dependence of material constants for thin films of Ba0.65Sr0.35TiO3 (BST65) on the applied planar field at different lattice misfit strains has been studied for this phase. All induced piezoelectric moduli show extreme behavior during field alteration. Elastic moduli show similar abnormal behavior. The alterations increase as misfit strain is approaching the critical value.},\n\turldate = {2023-11-11},\n\tjournal = {Thin Solid Films},\n\tauthor = {Shirokov, V. B. and Kalinchuk, V. V. and Timoshenko, P. E.},\n\tmonth = jul,\n\tyear = {2018},\n\tkeywords = {Phenomenological theory, Phase transitions, Barium strontium titanate, Ferroelectric thin film},\n\tpages = {8--15},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Developing the novel electric field tunable, reconfigurable, adaptive and frequency-agile microwave devices with specific properties involves technological and scientific activities in the studying of material properties. Measurements of its properties could be a difficult and expensive issue, especially when it concerns thin-film ferroelectrics. Their electromechanical properties change significantly under applied DC bias field. The material coefficients of barium strontium titanate thin films are still unknown; therefore, it is expedient to carry out their calculations. In the present paper, the linear equations of piezoelectric effect have been written for thin barium strontium titanate films under DC bias electric field in paraelectric phase (induced piezoelectric effect) based on the grand potential of Landau theory of phase transitions. The dependence of material constants for thin films of Ba0.65Sr0.35TiO3 (BST65) on the applied planar field at different lattice misfit strains has been studied for this phase. All induced piezoelectric moduli show extreme behavior during field alteration. Elastic moduli show similar abnormal behavior. The alterations increase as misfit strain is approaching the critical value.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kaydashev-zolotukhin-belanova-anokhin-zharinov-kaidashev-macroscopicmonolayerofplasmoncoupledgoldnanoparticlesonmirrorforfluorescenceenhancement-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.spiedigitallibrary.org/conference-proceedings-of-spie/10716/107161F/Macroscopic-monolayer-of-plasmon-coupled-gold-nanoparticles-on-mirror-for/10.1117/12.2315071.full\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kaydashev-zolotukhin-belanova-anokhin-zharinov-kaidashev-macroscopicmonolayerofplasmoncoupledgoldnanoparticlesonmirrorforfluorescenceenhancement-2018', 'https://www.spiedigitallibrary.org/conference-proceedings-of-spie/10716/107161F/Macroscopic-monolayer-of-plasmon-coupled-gold-nanoparticles-on-mirror-for/10.1117/12.2315071.full', event);\">\n    Macroscopic monolayer of plasmon coupled gold nanoparticles on mirror for fluorescence enhancement.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kaydashev, V. E.; Zolotukhin, P.; Belanova, A.; Anokhin, A. S.; Zharinov, V. S.;  and Kaidashev, E. M.\n</span>\n\n  \n\n</span>\n\n  In <i>Saratov Fall Meeting 2017: Optical Technologies in Biophysics and Medicine XIX</i>, volume 10716, pages 357–363, April 2018. SPIE\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.spiedigitallibrary.org/conference-proceedings-of-spie/10716/107161F/Macroscopic-monolayer-of-plasmon-coupled-gold-nanoparticles-on-mirror-for/10.1117/12.2315071.full\"\n     onclick=\"log_download('kaydashev-zolotukhin-belanova-anokhin-zharinov-kaidashev-macroscopicmonolayerofplasmoncoupledgoldnanoparticlesonmirrorforfluorescenceenhancement-2018', 'https://www.spiedigitallibrary.org/conference-proceedings-of-spie/10716/107161F/Macroscopic-monolayer-of-plasmon-coupled-gold-nanoparticles-on-mirror-for/10.1117/12.2315071.full', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Macroscopic monolayer of plasmon coupled gold nanoparticles on mirror for fluorescence enhancement [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1117/12.2315071\"\n     onclick=\"log_download('kaydashev-zolotukhin-belanova-anokhin-zharinov-kaidashev-macroscopicmonolayerofplasmoncoupledgoldnanoparticlesonmirrorforfluorescenceenhancement-2018', 'http://doi.org/10.1117/12.2315071', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kaydashev-zolotukhin-belanova-anokhin-zharinov-kaidashev-macroscopicmonolayerofplasmoncoupledgoldnanoparticlesonmirrorforfluorescenceenhancement-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kaydashev-zolotukhin-belanova-anokhin-zharinov-kaidashev-macroscopicmonolayerofplasmoncoupledgoldnanoparticlesonmirrorforfluorescenceenhancement-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{kaydashev_macroscopic_2018,\n\ttitle = {Macroscopic monolayer of plasmon coupled gold nanoparticles on mirror for fluorescence enhancement},\n\tvolume = {10716},\n\turl = {https://www.spiedigitallibrary.org/conference-proceedings-of-spie/10716/107161F/Macroscopic-monolayer-of-plasmon-coupled-gold-nanoparticles-on-mirror-for/10.1117/12.2315071.full},\n\tdoi = {10.1117/12.2315071},\n\tabstract = {We study an ability of a large quasi-homogeneous monolayer of Au plasmon coupled nanoparticles separated from continuous Au film by polymer spacer to enhance a fluorescence of adsorbed molecular species. A fluorescence response of Methylene Blue molecules is studied as a function of polymer film thickness. A change of plasmonic properties of a system, its ability to enhance a fluorescence and the possible heating of a structure upon light absorption are discussed.},\n\turldate = {2023-11-11},\n\tbooktitle = {Saratov {Fall} {Meeting} 2017: {Optical} {Technologies} in {Biophysics} and {Medicine} {XIX}},\n\tpublisher = {SPIE},\n\tauthor = {Kaydashev, V. E. and Zolotukhin, P. and Belanova, A. and Anokhin, A. S. and Zharinov, V. S. and Kaidashev, E. M.},\n\tmonth = apr,\n\tyear = {2018},\n\tpages = {357--363},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We study an ability of a large quasi-homogeneous monolayer of Au plasmon coupled nanoparticles separated from continuous Au film by polymer spacer to enhance a fluorescence of adsorbed molecular species. A fluorescence response of Methylene Blue molecules is studied as a function of polymer film thickness. A change of plasmonic properties of a system, its ability to enhance a fluorescence and the possible heating of a structure upon light absorption are discussed.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kaydashev-lyanguzov-anokhin-chernishov-kaidashev-sersofmethyleneblueinducedbyplasmoniccouplednanoparticlearrays-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.spiedigitallibrary.org/conference-proceedings-of-spie/10716/107161E/SERS-of-Methylene-Blue-induced-by-plasmonic-coupled-nanoparticle-arrays/10.1117/12.2315007.full\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kaydashev-lyanguzov-anokhin-chernishov-kaidashev-sersofmethyleneblueinducedbyplasmoniccouplednanoparticlearrays-2018', 'https://www.spiedigitallibrary.org/conference-proceedings-of-spie/10716/107161E/SERS-of-Methylene-Blue-induced-by-plasmonic-coupled-nanoparticle-arrays/10.1117/12.2315007.full', event);\">\n    SERS of Methylene Blue induced by plasmonic coupled nanoparticle arrays.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kaydashev, V. E.; Lyanguzov, N. V.; Anokhin, A. S.; Chernishov, A.;  and Kaidashev, E. M.\n</span>\n\n  \n\n</span>\n\n  In <i>Saratov Fall Meeting 2017: Optical Technologies in Biophysics and Medicine XIX</i>, volume 10716, pages 350–356, April 2018. SPIE\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.spiedigitallibrary.org/conference-proceedings-of-spie/10716/107161E/SERS-of-Methylene-Blue-induced-by-plasmonic-coupled-nanoparticle-arrays/10.1117/12.2315007.full\"\n     onclick=\"log_download('kaydashev-lyanguzov-anokhin-chernishov-kaidashev-sersofmethyleneblueinducedbyplasmoniccouplednanoparticlearrays-2018', 'https://www.spiedigitallibrary.org/conference-proceedings-of-spie/10716/107161E/SERS-of-Methylene-Blue-induced-by-plasmonic-coupled-nanoparticle-arrays/10.1117/12.2315007.full', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"SERS of Methylene Blue induced by plasmonic coupled nanoparticle arrays [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1117/12.2315007\"\n     onclick=\"log_download('kaydashev-lyanguzov-anokhin-chernishov-kaidashev-sersofmethyleneblueinducedbyplasmoniccouplednanoparticlearrays-2018', 'http://doi.org/10.1117/12.2315007', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kaydashev-lyanguzov-anokhin-chernishov-kaidashev-sersofmethyleneblueinducedbyplasmoniccouplednanoparticlearrays-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kaydashev-lyanguzov-anokhin-chernishov-kaidashev-sersofmethyleneblueinducedbyplasmoniccouplednanoparticlearrays-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{kaydashev_sers_2018,\n\ttitle = {{SERS} of {Methylene} {Blue} induced by plasmonic coupled nanoparticle arrays},\n\tvolume = {10716},\n\turl = {https://www.spiedigitallibrary.org/conference-proceedings-of-spie/10716/107161E/SERS-of-Methylene-Blue-induced-by-plasmonic-coupled-nanoparticle-arrays/10.1117/12.2315007.full},\n\tdoi = {10.1117/12.2315007},\n\tabstract = {We study the surface enhanced Raman scattering of Methylene Blue (MB) dye molecules induced by large quasihomogeneous arrays of plasmon coupled 5-8 nm Au nanoparticle separated by distances less than 10 nm. Also, the variation of the fluorescence enhancement/SERS properties for as-prepared coupled particles and agglomerated particles obtained upon heat treatment and percolation-like films is analyzed for two measurement protocols, i.e. when measured through the solution and for a monolayer of MB molecules chemisorbed on a surface.},\n\turldate = {2023-11-11},\n\tbooktitle = {Saratov {Fall} {Meeting} 2017: {Optical} {Technologies} in {Biophysics} and {Medicine} {XIX}},\n\tpublisher = {SPIE},\n\tauthor = {Kaydashev, V. E. and Lyanguzov, N. V. and Anokhin, A. S. and Chernishov, A. and Kaidashev, E. M.},\n\tmonth = apr,\n\tyear = {2018},\n\tpages = {350--356},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We study the surface enhanced Raman scattering of Methylene Blue (MB) dye molecules induced by large quasihomogeneous arrays of plasmon coupled 5-8 nm Au nanoparticle separated by distances less than 10 nm. Also, the variation of the fluorescence enhancement/SERS properties for as-prepared coupled particles and agglomerated particles obtained upon heat treatment and percolation-like films is analyzed for two measurement protocols, i.e. when measured through the solution and for a monolayer of MB molecules chemisorbed on a surface.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-kalinchuk-timoshenko-propertiesofthinfilmsofbariumstrontiumtitanatesolidsolutionsbyinducedpiezoelectriceffect-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1028335818040092\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-kalinchuk-timoshenko-propertiesofthinfilmsofbariumstrontiumtitanatesolidsolutionsbyinducedpiezoelectriceffect-2018', 'https://doi.org/10.1134/S1028335818040092', event);\">\n    Properties of Thin Films of Barium–Strontium Titanate Solid Solutions by Induced Piezoelectric Effect.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.; Kalinchuk, V. V.;  and Timoshenko, P. E.\n</span>\n\n  \n\n</span>\n\n  <i>Doklady Physics</i>, 63(4): 142–146. April 2018.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1028335818040092\"\n     onclick=\"log_download('shirokov-kalinchuk-timoshenko-propertiesofthinfilmsofbariumstrontiumtitanatesolidsolutionsbyinducedpiezoelectriceffect-2018', 'https://doi.org/10.1134/S1028335818040092', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Properties of Thin Films of Barium–Strontium Titanate Solid Solutions by Induced Piezoelectric Effect [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1028335818040092\"\n     onclick=\"log_download('shirokov-kalinchuk-timoshenko-propertiesofthinfilmsofbariumstrontiumtitanatesolidsolutionsbyinducedpiezoelectriceffect-2018', 'http://doi.org/10.1134/S1028335818040092', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-kalinchuk-timoshenko-propertiesofthinfilmsofbariumstrontiumtitanatesolidsolutionsbyinducedpiezoelectriceffect-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-kalinchuk-timoshenko-propertiesofthinfilmsofbariumstrontiumtitanatesolidsolutionsbyinducedpiezoelectriceffect-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_properties_2018,\n\ttitle = {Properties of {Thin} {Films} of {Barium}–{Strontium} {Titanate} {Solid} {Solutions} by {Induced} {Piezoelectric} {Effect}},\n\tvolume = {63},\n\tissn = {1562-6903},\n\turl = {https://doi.org/10.1134/S1028335818040092},\n\tdoi = {10.1134/S1028335818040092},\n\tabstract = {Piezoelectric effect equations have been derived by linearizing the nonlinear equations of state of a thin film existing in a paraelectric phase in the presence of an external electrical field (induced piezoelectric effect). The behavior of the piezoelectric and elastic constants of thin films of a solid barium–strontium titanate solution BST065 (x = 0.65) in a planar field at different misfit strain values has been studied numerically.},\n\tlanguage = {en},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Doklady Physics},\n\tauthor = {Shirokov, V. B. and Kalinchuk, V. V. and Timoshenko, P. E.},\n\tmonth = apr,\n\tyear = {2018},\n\tpages = {142--146},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Piezoelectric effect equations have been derived by linearizing the nonlinear equations of state of a thin film existing in a paraelectric phase in the presence of an external electrical field (induced piezoelectric effect). The behavior of the piezoelectric and elastic constants of thin films of a solid barium–strontium titanate solution BST065 (x = 0.65) in a planar field at different misfit strain values has been studied numerically.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"popov-levshov-sauvajol-paillet-computationalstudyoftheshiftofthegbandofdoublewalledcarbonnanotubesduetointerlayerinteractions-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.97.165417\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'popov-levshov-sauvajol-paillet-computationalstudyoftheshiftofthegbandofdoublewalledcarbonnanotubesduetointerlayerinteractions-2018', 'https://link.aps.org/doi/10.1103/PhysRevB.97.165417', event);\">\n    Computational study of the shift of the G band of double-walled carbon nanotubes due to interlayer interactions.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Popov, V. N.; Levshov, D. I.; Sauvajol, J.;  and Paillet, M.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 97(16): 165417. April 2018.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.97.165417\"\n     onclick=\"log_download('popov-levshov-sauvajol-paillet-computationalstudyoftheshiftofthegbandofdoublewalledcarbonnanotubesduetointerlayerinteractions-2018', 'https://link.aps.org/doi/10.1103/PhysRevB.97.165417', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Computational study of the shift of the G band of double-walled carbon nanotubes due to interlayer interactions [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.97.165417\"\n     onclick=\"log_download('popov-levshov-sauvajol-paillet-computationalstudyoftheshiftofthegbandofdoublewalledcarbonnanotubesduetointerlayerinteractions-2018', 'http://doi.org/10.1103/PhysRevB.97.165417', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/popov-levshov-sauvajol-paillet-computationalstudyoftheshiftofthegbandofdoublewalledcarbonnanotubesduetointerlayerinteractions-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('popov-levshov-sauvajol-paillet-computationalstudyoftheshiftofthegbandofdoublewalledcarbonnanotubesduetointerlayerinteractions-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{popov_computational_2018,\n\ttitle = {Computational study of the shift of the {G} band of double-walled carbon nanotubes due to interlayer interactions},\n\tvolume = {97},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.97.165417},\n\tdoi = {10.1103/PhysRevB.97.165417},\n\tabstract = {The interactions between the layers of double-walled carbon nanotubes induce a measurable shift of the G bands relative to the isolated layers. While experimental data on this shift in freestanding double-walled carbon nanotubes has been reported in the past several years, a comprehensive theoretical description of the observed shift is still lacking. The prediction of this shift is important for supporting the assignment of the measured double-walled nanotubes to particular nanotube types. Here, we report a computational study of the G-band shift as a function of the semiconducting inner layer radius and interlayer separation. We find that with increasing interlayer separation, the G band shift decreases, passes through zero and becomes negative, and further increases in absolute value for the wide range of considered inner layer radii. The theoretical predictions are shown to agree with the available experimental data within the experimental uncertainty.},\n\tnumber = {16},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Popov, Valentin N. and Levshov, Dmitry I. and Sauvajol, Jean-Louis and Paillet, Matthieu},\n\tmonth = apr,\n\tyear = {2018},\n\tnote = {Publisher: American Physical Society},\n\tpages = {165417},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\VT7RDBBS\\\\Popov и др. - 2018 - Computational study of the shift of the G band of .pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The interactions between the layers of double-walled carbon nanotubes induce a measurable shift of the G bands relative to the isolated layers. While experimental data on this shift in freestanding double-walled carbon nanotubes has been reported in the past several years, a comprehensive theoretical description of the observed shift is still lacking. The prediction of this shift is important for supporting the assignment of the measured double-walled nanotubes to particular nanotube types. Here, we report a computational study of the G-band shift as a function of the semiconducting inner layer radius and interlayer separation. We find that with increasing interlayer separation, the G band shift decreases, passes through zero and becomes negative, and further increases in absolute value for the wide range of considered inner layer radii. The theoretical predictions are shown to agree with the available experimental data within the experimental uncertainty.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"timoshenko-kalinchuk-shirokov-finiteelementanalysisofscatteringparametersofsurfaceacousticwavebandpassfilterformedonbariumtitanatethinfilm-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/19475411.2018.1447045\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'timoshenko-kalinchuk-shirokov-finiteelementanalysisofscatteringparametersofsurfaceacousticwavebandpassfilterformedonbariumtitanatethinfilm-2018', 'https://doi.org/10.1080/19475411.2018.1447045', event);\">\n    Finite-element analysis of scattering parameters of surface acoustic wave bandpass filter formed on barium titanate thin film.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Timoshenko, P. E.; Kalinchuk, V. V.;  and Shirokov, V. B.\n</span>\n\n  \n\n</span>\n\n  <i>International Journal of Smart and Nano Materials</i>, 9(2): 88–98. April 2018.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/19475411.2018.1447045</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/19475411.2018.1447045\"\n     onclick=\"log_download('timoshenko-kalinchuk-shirokov-finiteelementanalysisofscatteringparametersofsurfaceacousticwavebandpassfilterformedonbariumtitanatethinfilm-2018', 'https://doi.org/10.1080/19475411.2018.1447045', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Finite-element analysis of scattering parameters of surface acoustic wave bandpass filter formed on barium titanate thin film [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/19475411.2018.1447045\"\n     onclick=\"log_download('timoshenko-kalinchuk-shirokov-finiteelementanalysisofscatteringparametersofsurfaceacousticwavebandpassfilterformedonbariumtitanatethinfilm-2018', 'http://doi.org/10.1080/19475411.2018.1447045', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/timoshenko-kalinchuk-shirokov-finiteelementanalysisofscatteringparametersofsurfaceacousticwavebandpassfilterformedonbariumtitanatethinfilm-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('timoshenko-kalinchuk-shirokov-finiteelementanalysisofscatteringparametersofsurfaceacousticwavebandpassfilterformedonbariumtitanatethinfilm-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{timoshenko_finite-element_2018,\n\ttitle = {Finite-element analysis of scattering parameters of surface acoustic wave bandpass filter formed on barium titanate thin film},\n\tvolume = {9},\n\tissn = {1947-5411},\n\turl = {https://doi.org/10.1080/19475411.2018.1447045},\n\tdoi = {10.1080/19475411.2018.1447045},\n\tabstract = {The frequency dependence of scattering parameters of interdigital surface acoustic wave transducers placed on ferroelectric barium titanate (BaTiO3) epitaxial film in c-phase coated over magnesium oxide has been studied using the finite-element method (FEM) approach along with the perfectly matched layer (PML) technique. The interdigital transducer which has a comb-like structure with aluminum electrodes excites the mechanical wave. The distance between the fingers allows tuning the frequency properties of the wave propagation. The magnesium oxide is taken as the substrate. The two-dimensional model of two-port surface acoustic wave filter is created to calculate scattering parameters and to show how to design the fixture in COMSOLTM. Some practical computational challenges of finite element modeling of SAW devices in COMSOLTM are shown. The effect of lattice misfit strain on acoustic properties of heterostructures of BaTiO3 epitaxial film in c-phase at room temperature is discussed in present article for two low-frequency surface acoustic resonances.},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {International Journal of Smart and Nano Materials},\n\tauthor = {Timoshenko, Pavel E. and Kalinchuk, Valery V. and Shirokov, Vladimir B.},\n\tmonth = apr,\n\tyear = {2018},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/19475411.2018.1447045},\n\tkeywords = {thin films, ferroelectrics, COMSOL, finite element method (FEM), SAW filters},\n\tpages = {88--98},\n\tfile = {Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\AAZMSR86\\\\Timoshenko и др. - 2018 - Finite-element analysis of scattering parameters o.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The frequency dependence of scattering parameters of interdigital surface acoustic wave transducers placed on ferroelectric barium titanate (BaTiO3) epitaxial film in c-phase coated over magnesium oxide has been studied using the finite-element method (FEM) approach along with the perfectly matched layer (PML) technique. The interdigital transducer which has a comb-like structure with aluminum electrodes excites the mechanical wave. The distance between the fingers allows tuning the frequency properties of the wave propagation. The magnesium oxide is taken as the substrate. The two-dimensional model of two-port surface acoustic wave filter is created to calculate scattering parameters and to show how to design the fixture in COMSOLTM. Some practical computational challenges of finite element modeling of SAW devices in COMSOLTM are shown. The effect of lattice misfit strain on acoustic properties of heterostructures of BaTiO3 epitaxial film in c-phase at room temperature is discussed in present article for two low-frequency surface acoustic resonances.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"ulyankina-leontyev-avramenko-zhigunov-smirnova-largescalesynthesisofznonanostructuresbypulseelectrochemicalmethodandtheirphotocatalyticproperties-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S1369800117320528\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'ulyankina-leontyev-avramenko-zhigunov-smirnova-largescalesynthesisofznonanostructuresbypulseelectrochemicalmethodandtheirphotocatalyticproperties-2018', 'https://www.sciencedirect.com/science/article/pii/S1369800117320528', event);\">\n    Large-scale synthesis of ZnO nanostructures by pulse electrochemical method and their photocatalytic properties.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Ulyankina, A.; Leontyev, I.; Avramenko, M.; Zhigunov, D.;  and Smirnova, N.\n</span>\n\n  \n\n</span>\n\n  <i>Materials Science in Semiconductor Processing</i>, 76: 7–13. March 2018.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S1369800117320528\"\n     onclick=\"log_download('ulyankina-leontyev-avramenko-zhigunov-smirnova-largescalesynthesisofznonanostructuresbypulseelectrochemicalmethodandtheirphotocatalyticproperties-2018', 'https://www.sciencedirect.com/science/article/pii/S1369800117320528', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Large-scale synthesis of ZnO nanostructures by pulse electrochemical method and their photocatalytic properties [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.mssp.2017.12.011\"\n     onclick=\"log_download('ulyankina-leontyev-avramenko-zhigunov-smirnova-largescalesynthesisofznonanostructuresbypulseelectrochemicalmethodandtheirphotocatalyticproperties-2018', 'http://doi.org/10.1016/j.mssp.2017.12.011', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/ulyankina-leontyev-avramenko-zhigunov-smirnova-largescalesynthesisofznonanostructuresbypulseelectrochemicalmethodandtheirphotocatalyticproperties-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('ulyankina-leontyev-avramenko-zhigunov-smirnova-largescalesynthesisofznonanostructuresbypulseelectrochemicalmethodandtheirphotocatalyticproperties-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{ulyankina_large-scale_2018,\n\ttitle = {Large-scale synthesis of {ZnO} nanostructures by pulse electrochemical method and their photocatalytic properties},\n\tvolume = {76},\n\tissn = {1369-8001},\n\turl = {https://www.sciencedirect.com/science/article/pii/S1369800117320528},\n\tdoi = {10.1016/j.mssp.2017.12.011},\n\tabstract = {In this paper, we report a simple environment-friendly and large-scale approach to synthesis of highly crystalline zinc oxide nanostructures using pulse alternating current (PAC). The morphological results demonstrate flower-like architectures of nanoparticle-based and nanorod-based zinc oxide (ZnO-NPs and ZnO-NRs) obtained in KCl and NaCl as electrolytes. The photocatalytic activity of the obtained materials was performed in methylene blue dye degradation reaction under UV light irradiation. A high efficiency of {\\textasciitilde} 90\\% within 60min with excellent rate constant (k = 0.0386min−1) was observed in the presence of ZnO-NPs synthesized in 2M KCl which is attributed to the larger specific surface area (27m2g−1), total pore volume and more defective structure.},\n\turldate = {2023-11-11},\n\tjournal = {Materials Science in Semiconductor Processing},\n\tauthor = {Ulyankina, Anna and Leontyev, Igor and Avramenko, Marina and Zhigunov, Denis and Smirnova, Nina},\n\tmonth = mar,\n\tyear = {2018},\n\tkeywords = {Electrochemical synthesis, Nanocrystalline materials, Photocatalytic activity, Pulse alternating current, Semiconductors, ZnO},\n\tpages = {7--13},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  In this paper, we report a simple environment-friendly and large-scale approach to synthesis of highly crystalline zinc oxide nanostructures using pulse alternating current (PAC). The morphological results demonstrate flower-like architectures of nanoparticle-based and nanorod-based zinc oxide (ZnO-NPs and ZnO-NRs) obtained in KCl and NaCl as electrolytes. The photocatalytic activity of the obtained materials was performed in methylene blue dye degradation reaction under UV light irradiation. A high efficiency of ~ 90% within 60min with excellent rate constant (k = 0.0386min−1) was observed in the presence of ZnO-NPs synthesized in 2M KCl which is attributed to the larger specific surface area (27m2g−1), total pore volume and more defective structure.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"mikheykin-anokhin-torgashev-zhukova-gorshunov-prokhorov-bush-natureoflocalsymmetryviolationsofionsinthemagneticsubsystemofmagnetoplumbitecrystalaccordingtoramanscatteringspectroscopydata-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.3103/S1062873818030140\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'mikheykin-anokhin-torgashev-zhukova-gorshunov-prokhorov-bush-natureoflocalsymmetryviolationsofionsinthemagneticsubsystemofmagnetoplumbitecrystalaccordingtoramanscatteringspectroscopydata-2018', 'https://doi.org/10.3103/S1062873818030140', event);\">\n    Nature of Local Symmetry Violations of Ions in the Magnetic Subsystem of Magnetoplumbite Crystal, According to Raman Scattering Spectroscopy Data.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Mikheykin, A. S.; Anokhin, A. S.; Torgashev, V. I.; Zhukova, E. S.; Gorshunov, B. P.; Prokhorov, A. S.;  and Bush, A. A.\n</span>\n\n  \n\n</span>\n\n  <i>Bulletin of the Russian Academy of Sciences: Physics</i>, 82(3): 266–268. March 2018.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.3103/S1062873818030140\"\n     onclick=\"log_download('mikheykin-anokhin-torgashev-zhukova-gorshunov-prokhorov-bush-natureoflocalsymmetryviolationsofionsinthemagneticsubsystemofmagnetoplumbitecrystalaccordingtoramanscatteringspectroscopydata-2018', 'https://doi.org/10.3103/S1062873818030140', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Nature of Local Symmetry Violations of Ions in the Magnetic Subsystem of Magnetoplumbite Crystal, According to Raman Scattering Spectroscopy Data [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3103/S1062873818030140\"\n     onclick=\"log_download('mikheykin-anokhin-torgashev-zhukova-gorshunov-prokhorov-bush-natureoflocalsymmetryviolationsofionsinthemagneticsubsystemofmagnetoplumbitecrystalaccordingtoramanscatteringspectroscopydata-2018', 'http://doi.org/10.3103/S1062873818030140', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/mikheykin-anokhin-torgashev-zhukova-gorshunov-prokhorov-bush-natureoflocalsymmetryviolationsofionsinthemagneticsubsystemofmagnetoplumbitecrystalaccordingtoramanscatteringspectroscopydata-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('mikheykin-anokhin-torgashev-zhukova-gorshunov-prokhorov-bush-natureoflocalsymmetryviolationsofionsinthemagneticsubsystemofmagnetoplumbitecrystalaccordingtoramanscatteringspectroscopydata-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{mikheykin_nature_2018,\n\ttitle = {Nature of {Local} {Symmetry} {Violations} of {Ions} in the {Magnetic} {Subsystem} of {Magnetoplumbite} {Crystal}, {According} to {Raman} {Scattering} {Spectroscopy} {Data}},\n\tvolume = {82},\n\tissn = {1934-9432},\n\turl = {https://doi.org/10.3103/S1062873818030140},\n\tdoi = {10.3103/S1062873818030140},\n\tabstract = {The structure of an M-type lead hexaferrite (magnetoplumbite) crystal is studied via the diffraction of synchrotron radiation. The crystal model contains two iron ions positions with dynamic disorder. The dynamics of the crystal lattice in the temperature range of 80 to 775 K is studied by Raman scattering. Particular attention is given to the discussing the nature of the local disorder of iron ions in the trigonal bipyramidal environment of oxygen ions.},\n\tlanguage = {en},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Bulletin of the Russian Academy of Sciences: Physics},\n\tauthor = {Mikheykin, A. S. and Anokhin, A. S. and Torgashev, V. I. and Zhukova, E. S. and Gorshunov, B. P. and Prokhorov, A. S. and Bush, A. A.},\n\tmonth = mar,\n\tyear = {2018},\n\tpages = {266--268},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The structure of an M-type lead hexaferrite (magnetoplumbite) crystal is studied via the diffraction of synchrotron radiation. The crystal model contains two iron ions positions with dynamic disorder. The dynamics of the crystal lattice in the temperature range of 80 to 775 K is studied by Raman scattering. Particular attention is given to the discussing the nature of the local disorder of iron ions in the trigonal bipyramidal environment of oxygen ions.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-shakhovoy-pankin-kalinchuk-piezoelectriccoefficientsofthebariumstrontiumtitanatefilmona111orientedsubstrate-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/1757-899X/324/1/012006\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-shakhovoy-pankin-kalinchuk-piezoelectriccoefficientsofthebariumstrontiumtitanatefilmona111orientedsubstrate-2018', 'https://dx.doi.org/10.1088/1757-899X/324/1/012006', event);\">\n    Piezoelectric coefficients of the barium-strontium titanate film on a (111)-oriented substrate.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.; Shakhovoy, R. A.; Pan’kin, A. V.;  and Kalinchuk, V. V.\n</span>\n\n  \n\n</span>\n\n  <i>IOP Conference Series: Materials Science and Engineering</i>, 324(1): 012006. March 2018.\n  <span class=\"note\">Publisher: IOP Publishing</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/1757-899X/324/1/012006\"\n     onclick=\"log_download('shirokov-shakhovoy-pankin-kalinchuk-piezoelectriccoefficientsofthebariumstrontiumtitanatefilmona111orientedsubstrate-2018', 'https://dx.doi.org/10.1088/1757-899X/324/1/012006', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Piezoelectric coefficients of the barium-strontium titanate film on a (111)-oriented substrate [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/1757-899X/324/1/012006\"\n     onclick=\"log_download('shirokov-shakhovoy-pankin-kalinchuk-piezoelectriccoefficientsofthebariumstrontiumtitanatefilmona111orientedsubstrate-2018', 'http://doi.org/10.1088/1757-899X/324/1/012006', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-shakhovoy-pankin-kalinchuk-piezoelectriccoefficientsofthebariumstrontiumtitanatefilmona111orientedsubstrate-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-shakhovoy-pankin-kalinchuk-piezoelectriccoefficientsofthebariumstrontiumtitanatefilmona111orientedsubstrate-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_piezoelectric_2018,\n\ttitle = {Piezoelectric coefficients of the barium-strontium titanate film on a (111)-oriented substrate},\n\tvolume = {324},\n\tissn = {1757-899X},\n\turl = {https://dx.doi.org/10.1088/1757-899X/324/1/012006},\n\tdoi = {10.1088/1757-899X/324/1/012006},\n\tabstract = {Within the framework of the phenomenological theory of phase transitions, we consider properties of the Ba0.8Sr0.2TiO3 (BST80) film grown on a (111)-oriented cubic substrate. The film was revealed to exhibit three ferroelectric phases with different orientations of spontaneous polarization. It is shown that some piezoelectric moduli should demonstrate anomalous behavior near the phase boundaries.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {IOP Conference Series: Materials Science and Engineering},\n\tauthor = {Shirokov, V. B. and Shakhovoy, R. A. and Pan’kin, A. V. and Kalinchuk, V. V.},\n\tmonth = mar,\n\tyear = {2018},\n\tnote = {Publisher: IOP Publishing},\n\tpages = {012006},\n\tfile = {IOP Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\74MIZ5W7\\\\Shirokov и др. - 2018 - Piezoelectric coefficients of the barium-strontium.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Within the framework of the phenomenological theory of phase transitions, we consider properties of the Ba0.8Sr0.2TiO3 (BST80) film grown on a (111)-oriented cubic substrate. The film was revealed to exhibit three ferroelectric phases with different orientations of spontaneous polarization. It is shown that some piezoelectric moduli should demonstrate anomalous behavior near the phase boundaries.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"zhilin-karapetyan-kutepov-minasyan-yatsenko-kaidashev-growthandstudyofzincoxidenanorodsarraysonpiezoelectricsubstrates-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  Growth and Study of Zinc Oxide Nanorods Arrays on Piezoelectric Substrates.\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Zhilin, D. A.; Karapetyan, G. Y.; Kutepov, M. E.; Minasyan, T. A.; Yatsenko, V. I.;  and Kaidashev, E. M.\n</span>\n\n  \n\n</span>\n\n  In Parinov, I. A.; Chang, S.;  and Gupta, V. K., editor(s), <i>Advanced Materials</i>, of <i>Springer Proceedings in Physics</i>, pages 25–31, Cham,  2018. Springer International Publishing\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n\n  \n  <a href=\"http://doi.org/10.1007/978-3-319-78919-4_2\"\n     onclick=\"log_download('zhilin-karapetyan-kutepov-minasyan-yatsenko-kaidashev-growthandstudyofzincoxidenanorodsarraysonpiezoelectricsubstrates-2018', 'http://doi.org/10.1007/978-3-319-78919-4_2', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/zhilin-karapetyan-kutepov-minasyan-yatsenko-kaidashev-growthandstudyofzincoxidenanorodsarraysonpiezoelectricsubstrates-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('zhilin-karapetyan-kutepov-minasyan-yatsenko-kaidashev-growthandstudyofzincoxidenanorodsarraysonpiezoelectricsubstrates-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{zhilin_growth_2018,\n\taddress = {Cham},\n\tseries = {Springer {Proceedings} in {Physics}},\n\ttitle = {Growth and {Study} of {Zinc} {Oxide} {Nanorods} {Arrays} on {Piezoelectric} {Substrates}},\n\tisbn = {978-3-319-78919-4},\n\tdoi = {10.1007/978-3-319-78919-4_2},\n\tabstract = {Our studies have shown the possibility of using the thermal synthesisSynthesismethod from Zn vapors to obtain ZnO nanorodsZnO nanorods (ZnO NRs)arrays as a sensitive element for UV radiation SAW sensors. The piezoelectricPiezoelectricproperties of the LiNbO3 substrate typically degrade upon nanorods growth at elevated temperature. This limitation is solved by using additional annealing of prepared structureStructureat 550 °C in an oxygen atmosphere. The obtained ZnO NRs were investigated by scanning electron microscopy and photoluminescence.},\n\tlanguage = {en},\n\tbooktitle = {Advanced {Materials}},\n\tpublisher = {Springer International Publishing},\n\tauthor = {Zhilin, D. A. and Karapetyan, G. Y. and Kutepov, M. E. and Minasyan, T. A. and Yatsenko, V. I. and Kaidashev, E. M.},\n\teditor = {Parinov, Ivan A. and Chang, Shun-Hsyung and Gupta, Vijay K.},\n\tyear = {2018},\n\tkeywords = {Carbothermal Method, LiNbO3 Substrate, structureStructure, synthesisSynthesis, Zinc Oxide Nanorod Arrays},\n\tpages = {25--31},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Our studies have shown the possibility of using the thermal synthesisSynthesismethod from Zn vapors to obtain ZnO nanorodsZnO nanorods (ZnO NRs)arrays as a sensitive element for UV radiation SAW sensors. The piezoelectricPiezoelectricproperties of the LiNbO3 substrate typically degrade upon nanorods growth at elevated temperature. This limitation is solved by using additional annealing of prepared structureStructureat 550 °C in an oxygen atmosphere. The obtained ZnO NRs were investigated by scanning electron microscopy and photoluminescence.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kulbakov-allix-rakhmatullin-mikheykin-popov-smirnova-maslova-leontyev-insituinvestigationofnonisothermaldecompositionofptacetylacetonateasonestepsizecontrolledsynthesisofptnanoparticles-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssa.201800488\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kulbakov-allix-rakhmatullin-mikheykin-popov-smirnova-maslova-leontyev-insituinvestigationofnonisothermaldecompositionofptacetylacetonateasonestepsizecontrolledsynthesisofptnanoparticles-2018', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/pssa.201800488', event);\">\n    In Situ Investigation of Non-Isothermal Decomposition of Pt Acetylacetonate as One-Step Size-Controlled Synthesis of Pt Nanoparticles.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kulbakov, A. A.; Allix, M.; Rakhmatullin, A.; Mikheykin, A. S.; Popov, Y. V.; Smirnova, N. V.; Maslova, O.;  and Leontyev, I. N.\n</span>\n\n  \n\n</span>\n\n  <i>physica status solidi (a)</i>, 215(23): 1800488.  2018.\n  <span class=\"note\">_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssa.201800488</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssa.201800488\"\n     onclick=\"log_download('kulbakov-allix-rakhmatullin-mikheykin-popov-smirnova-maslova-leontyev-insituinvestigationofnonisothermaldecompositionofptacetylacetonateasonestepsizecontrolledsynthesisofptnanoparticles-2018', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/pssa.201800488', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"In Situ Investigation of Non-Isothermal Decomposition of Pt Acetylacetonate as One-Step Size-Controlled Synthesis of Pt Nanoparticles [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1002/pssa.201800488\"\n     onclick=\"log_download('kulbakov-allix-rakhmatullin-mikheykin-popov-smirnova-maslova-leontyev-insituinvestigationofnonisothermaldecompositionofptacetylacetonateasonestepsizecontrolledsynthesisofptnanoparticles-2018', 'http://doi.org/10.1002/pssa.201800488', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kulbakov-allix-rakhmatullin-mikheykin-popov-smirnova-maslova-leontyev-insituinvestigationofnonisothermaldecompositionofptacetylacetonateasonestepsizecontrolledsynthesisofptnanoparticles-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kulbakov-allix-rakhmatullin-mikheykin-popov-smirnova-maslova-leontyev-insituinvestigationofnonisothermaldecompositionofptacetylacetonateasonestepsizecontrolledsynthesisofptnanoparticles-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kulbakov_situ_2018,\n\ttitle = {In {Situ} {Investigation} of {Non}-{Isothermal} {Decomposition} of {Pt} {Acetylacetonate} as {One}-{Step} {Size}-{Controlled} {Synthesis} of {Pt} {Nanoparticles}},\n\tvolume = {215},\n\tcopyright = {© 2018 WILEY-VCH Verlag GmbH \\&amp; Co. KGaA, Weinheim},\n\tissn = {1862-6319},\n\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssa.201800488},\n\tdoi = {10.1002/pssa.201800488},\n\tabstract = {Interest in the development of state-of-the-art methods for synthesis of Pt nanoparticles is dictated by both unique properties of platinum itself and the wide range of platinum nanoparticles applications. Platinum acetylacetonate and platinum nanoparticles produced by the thermal decomposition of Pt(acac)2 are studied via in situ X-ray diffraction and Raman spectroscopy, thermal gravimetry, scanning (SEM), and transmission electronic microscopy (TEM). The experiments are made at heating rates of 1 and 5 K min−1. A comparative analysis of SEM, TEM, and XRD data highlights the formation of coarse Pt particles with sizes of ≈60–160 nm, which are composed of nanoparticles with dimensions of 1.9 and 4.1 nm for 1 K min−1- and 5 K min−1-heating rates, respectively. The desirable average size of nanoparticles upon their synthesis can thus be achieved by a simple tuning of the heating rate of acetylacetate thermal decomposition. The present results open up the possibility to use a trivial non-isothermal thermal decomposition method in the synthesis of both supported and unsupported nanoparticles of predetermined size for other chemical elements such as Pd, Ni, Co, etc. from their acetylacetonates.},\n\tlanguage = {en},\n\tnumber = {23},\n\turldate = {2023-11-11},\n\tjournal = {physica status solidi (a)},\n\tauthor = {Kulbakov, Anton A. and Allix, Mathieu and Rakhmatullin, Aydar and Mikheykin, Alexey S. and Popov, Yuri V. and Smirnova, Nina V. and Maslova, Olga and Leontyev, Igor N.},\n\tyear = {2018},\n\tnote = {\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssa.201800488},\n\tkeywords = {in situ characterizations, platinum acetylacetonate, Pt nanoparticles, thermal decomposition},\n\tpages = {1800488},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Interest in the development of state-of-the-art methods for synthesis of Pt nanoparticles is dictated by both unique properties of platinum itself and the wide range of platinum nanoparticles applications. Platinum acetylacetonate and platinum nanoparticles produced by the thermal decomposition of Pt(acac)2 are studied via in situ X-ray diffraction and Raman spectroscopy, thermal gravimetry, scanning (SEM), and transmission electronic microscopy (TEM). The experiments are made at heating rates of 1 and 5 K min−1. A comparative analysis of SEM, TEM, and XRD data highlights the formation of coarse Pt particles with sizes of ≈60–160 nm, which are composed of nanoparticles with dimensions of 1.9 and 4.1 nm for 1 K min−1- and 5 K min−1-heating rates, respectively. The desirable average size of nanoparticles upon their synthesis can thus be achieved by a simple tuning of the heating rate of acetylacetate thermal decomposition. The present results open up the possibility to use a trivial non-isothermal thermal decomposition method in the synthesis of both supported and unsupported nanoparticles of predetermined size for other chemical elements such as Pd, Ni, Co, etc. from their acetylacetonates.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"novikova-kuriganova-leontyev-gerasimova-maslova-rakhmatullin-smirnova-dobrovolsky-influenceofcarbonsupportoncatalyticlayerperformanceofprotonexchangemembranefuelcells-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1007/s12678-017-0416-4\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'novikova-kuriganova-leontyev-gerasimova-maslova-rakhmatullin-smirnova-dobrovolsky-influenceofcarbonsupportoncatalyticlayerperformanceofprotonexchangemembranefuelcells-2018', 'https://doi.org/10.1007/s12678-017-0416-4', event);\">\n    Influence of Carbon Support on Catalytic Layer Performance of Proton Exchange Membrane Fuel Cells.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Novikova, K.; Kuriganova, A.; Leontyev, I.; Gerasimova, E.; Maslova, O.; Rakhmatullin, A.; Smirnova, N.;  and Dobrovolsky, Y.\n</span>\n\n  \n\n</span>\n\n  <i>Electrocatalysis</i>, 9(1): 22–30. January 2018.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1007/s12678-017-0416-4\"\n     onclick=\"log_download('novikova-kuriganova-leontyev-gerasimova-maslova-rakhmatullin-smirnova-dobrovolsky-influenceofcarbonsupportoncatalyticlayerperformanceofprotonexchangemembranefuelcells-2018', 'https://doi.org/10.1007/s12678-017-0416-4', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Influence of Carbon Support on Catalytic Layer Performance of Proton Exchange Membrane Fuel Cells [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1007/s12678-017-0416-4\"\n     onclick=\"log_download('novikova-kuriganova-leontyev-gerasimova-maslova-rakhmatullin-smirnova-dobrovolsky-influenceofcarbonsupportoncatalyticlayerperformanceofprotonexchangemembranefuelcells-2018', 'http://doi.org/10.1007/s12678-017-0416-4', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/novikova-kuriganova-leontyev-gerasimova-maslova-rakhmatullin-smirnova-dobrovolsky-influenceofcarbonsupportoncatalyticlayerperformanceofprotonexchangemembranefuelcells-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('novikova-kuriganova-leontyev-gerasimova-maslova-rakhmatullin-smirnova-dobrovolsky-influenceofcarbonsupportoncatalyticlayerperformanceofprotonexchangemembranefuelcells-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{novikova_influence_2018,\n\ttitle = {Influence of {Carbon} {Support} on {Catalytic} {Layer} {Performance} of {Proton} {Exchange} {Membrane} {Fuel} {Cells}},\n\tvolume = {9},\n\tissn = {1868-5994},\n\turl = {https://doi.org/10.1007/s12678-017-0416-4},\n\tdoi = {10.1007/s12678-017-0416-4},\n\tabstract = {Pt-based catalysts supported onto various carbon nanotubes (CNTs) and carbon black Vulcan XC-72 have been studied in this work. The samples have been prepared via electrochemical dispersion technique. The carbon nanotubes exhibit the mesoporous morphology with the pore size of 5—30 nm, while Vulcan XC-72 support exhibits a microporous structure. The agglomeration of Pt particles (5—7 nm) is found to be more extended at the carbon nanotubes compared to the carbon black. The examination of the synthesized catalysts in a catalytic membrane electrode assembly layer reveals that CNTs favor a power density higher than in the carbon black support owing to a more suitable porous structure of the catalyst layer. Moreover, the maximum characteristics of membrane electrode assembly are obtained for few-walled carbon nanotubes with a broad carbon having size distribution.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Electrocatalysis},\n\tauthor = {Novikova, Ksenia and Kuriganova, Alexandra and Leontyev, Igor and Gerasimova, Ekaterina and Maslova, Olga and Rakhmatullin, Aydar and Smirnova, Nina and Dobrovolsky, Yuri},\n\tmonth = jan,\n\tyear = {2018},\n\tkeywords = {Carbon nanotubes, Carbon support, Catalytic layer structure, PEM fuel cell, Pt/C},\n\tpages = {22--30},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Pt-based catalysts supported onto various carbon nanotubes (CNTs) and carbon black Vulcan XC-72 have been studied in this work. The samples have been prepared via electrochemical dispersion technique. The carbon nanotubes exhibit the mesoporous morphology with the pore size of 5—30 nm, while Vulcan XC-72 support exhibits a microporous structure. The agglomeration of Pt particles (5—7 nm) is found to be more extended at the carbon nanotubes compared to the carbon black. The examination of the synthesized catalysts in a catalytic membrane electrode assembly layer reveals that CNTs favor a power density higher than in the carbon black support owing to a more suitable porous structure of the catalyst layer. Moreover, the maximum characteristics of membrane electrode assembly are obtained for few-walled carbon nanotubes with a broad carbon having size distribution.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"leontyev-kuriganova-allix-rakhmatullin-timoshenko-maslova-mikheykin-smirnova-ontheevaluationoftheaveragecrystallinesizeandsurfaceareaofplatinumcatalystnanoparticles-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201800240\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'leontyev-kuriganova-allix-rakhmatullin-timoshenko-maslova-mikheykin-smirnova-ontheevaluationoftheaveragecrystallinesizeandsurfaceareaofplatinumcatalystnanoparticles-2018', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201800240', event);\">\n    On the Evaluation of the Average Crystalline Size and Surface Area of Platinum Catalyst Nanoparticles.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Leontyev, I. N.; Kuriganova, A. B.; Allix, M.; Rakhmatullin, A.; Timoshenko, P. E.; Maslova, O. A.; Mikheykin, A. S.;  and Smirnova, N. V.\n</span>\n\n  \n\n</span>\n\n  <i>physica status solidi (b)</i>, 255(10): 1800240.  2018.\n  <span class=\"note\">_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201800240</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201800240\"\n     onclick=\"log_download('leontyev-kuriganova-allix-rakhmatullin-timoshenko-maslova-mikheykin-smirnova-ontheevaluationoftheaveragecrystallinesizeandsurfaceareaofplatinumcatalystnanoparticles-2018', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201800240', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"On the Evaluation of the Average Crystalline Size and Surface Area of Platinum Catalyst Nanoparticles [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1002/pssb.201800240\"\n     onclick=\"log_download('leontyev-kuriganova-allix-rakhmatullin-timoshenko-maslova-mikheykin-smirnova-ontheevaluationoftheaveragecrystallinesizeandsurfaceareaofplatinumcatalystnanoparticles-2018', 'http://doi.org/10.1002/pssb.201800240', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/leontyev-kuriganova-allix-rakhmatullin-timoshenko-maslova-mikheykin-smirnova-ontheevaluationoftheaveragecrystallinesizeandsurfaceareaofplatinumcatalystnanoparticles-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('leontyev-kuriganova-allix-rakhmatullin-timoshenko-maslova-mikheykin-smirnova-ontheevaluationoftheaveragecrystallinesizeandsurfaceareaofplatinumcatalystnanoparticles-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{leontyev_evaluation_2018,\n\ttitle = {On the {Evaluation} of the {Average} {Crystalline} {Size} and {Surface} {Area} of {Platinum} {Catalyst} {Nanoparticles}},\n\tvolume = {255},\n\tcopyright = {© 2018 WILEY-VCH Verlag GmbH \\&amp; Co. KGaA, Weinheim},\n\tissn = {1521-3951},\n\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201800240},\n\tdoi = {10.1002/pssb.201800240},\n\tabstract = {In the present work, the effect of grain size distribution on the diffraction profile shape is inspected via analysis of the mutual ratio of Lorentz and Gauss components in pseudo-Voigt function which is used for simulating X-ray profiles of nanoparticles. As established from the plotted dependences, the error in the average Pt nanoparticles size determination reaches 56\\% and the discrepancy between calculated Pt nanoparticle surface areas attains 60\\%. Furthermore, the determination error becomes greater with increasing the Lorentz contribution to pseudo-Voigt function, or, in fact, with enlarging particle size distribution. The empirically found electrochemical surface area of Pt/C electrocatalyst is compared with that evaluated from XRD data using the Scherrer formula and particle size distribution data analysis.},\n\tlanguage = {en},\n\tnumber = {10},\n\turldate = {2023-11-11},\n\tjournal = {physica status solidi (b)},\n\tauthor = {Leontyev, Igor N. and Kuriganova, Alexandra B. and Allix, Mathieu and Rakhmatullin, Aydar and Timoshenko, Pavel E. and Maslova, Olga A. and Mikheykin, Alexey S. and Smirnova, Nina V.},\n\tyear = {2018},\n\tnote = {\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201800240},\n\tkeywords = {X-ray diffraction, Pt/C, average nanoparticle size, catalysts, specific surface area},\n\tpages = {1800240},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  In the present work, the effect of grain size distribution on the diffraction profile shape is inspected via analysis of the mutual ratio of Lorentz and Gauss components in pseudo-Voigt function which is used for simulating X-ray profiles of nanoparticles. As established from the plotted dependences, the error in the average Pt nanoparticles size determination reaches 56% and the discrepancy between calculated Pt nanoparticle surface areas attains 60%. Furthermore, the determination error becomes greater with increasing the Lorentz contribution to pseudo-Voigt function, or, in fact, with enlarging particle size distribution. The empirically found electrochemical surface area of Pt/C electrocatalyst is compared with that evaluated from XRD data using the Scherrer formula and particle size distribution data analysis.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"rochal-roshal-myasnikova-lorman-commensurabilitybetweenproteinnanotubesincontractileejectionnanomachines-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://pubs.rsc.org/en/content/articlelanding/2018/nr/c7nr06940e\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'rochal-roshal-myasnikova-lorman-commensurabilitybetweenproteinnanotubesincontractileejectionnanomachines-2018', 'https://pubs.rsc.org/en/content/articlelanding/2018/nr/c7nr06940e', event);\">\n    Commensurability between protein nanotubes in contractile ejection nanomachines.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Rochal, S. B.; Roshal, D. S.; Myasnikova, A. E.;  and Lorman, V. L.\n</span>\n\n  \n\n</span>\n\n  <i>Nanoscale</i>, 10(2): 758–764. January 2018.\n  <span class=\"note\">Publisher: The Royal Society of Chemistry</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://pubs.rsc.org/en/content/articlelanding/2018/nr/c7nr06940e\"\n     onclick=\"log_download('rochal-roshal-myasnikova-lorman-commensurabilitybetweenproteinnanotubesincontractileejectionnanomachines-2018', 'https://pubs.rsc.org/en/content/articlelanding/2018/nr/c7nr06940e', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Commensurability between protein nanotubes in contractile ejection nanomachines [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1039/C7NR06940E\"\n     onclick=\"log_download('rochal-roshal-myasnikova-lorman-commensurabilitybetweenproteinnanotubesincontractileejectionnanomachines-2018', 'http://doi.org/10.1039/C7NR06940E', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/rochal-roshal-myasnikova-lorman-commensurabilitybetweenproteinnanotubesincontractileejectionnanomachines-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('rochal-roshal-myasnikova-lorman-commensurabilitybetweenproteinnanotubesincontractileejectionnanomachines-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{rochal_commensurability_2018,\n\ttitle = {Commensurability between protein nanotubes in contractile ejection nanomachines},\n\tvolume = {10},\n\tissn = {2040-3372},\n\turl = {https://pubs.rsc.org/en/content/articlelanding/2018/nr/c7nr06940e},\n\tdoi = {10.1039/C7NR06940E},\n\tabstract = {Contractile ejection nanomachines being sheath–tube assemblies create an opening in the cell membrane to translocate molecules or ions across it. Here, on the most structurally investigated examples of the bacteriophage T4 tail and pyocin R2, we show that the rearrangement of the sheath structure resulting in its contraction and twist occurs in such a way that the contracted sheath becomes commensurate with the inner tube. This fact dictates the previously unknown simple geometrical relationship between the nanotube symmetries. Using the Frank and van der Merwe classical theory of commensurability, we study an interaction between two protein nanotubes forming such nanomachines and obtain an expression for the corresponding energy, which depends on the tube structures and their mutual arrangement. The appearance of commensurability between the contracted sheath and the inner tube decreases both the interaction energy and the total energy of the system. It improves the nanomachine efficiency, since the energy gain obtained increases the torque of the inner tube piercing the cell membrane.},\n\tlanguage = {en},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Nanoscale},\n\tauthor = {Rochal, Sergey B. and Roshal, Daria S. and Myasnikova, Anna E. and Lorman, Vladimir L.},\n\tmonth = jan,\n\tyear = {2018},\n\tnote = {Publisher: The Royal Society of Chemistry},\n\tpages = {758--764},\n\tfile = {Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\J2A5BG4M\\\\Rochal и др. - 2018 - Commensurability between protein nanotubes in cont.pdf:application/pdf;Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\TABA9EAQ\\\\Rochal и др. - 2018 - Commensurability between protein nanotubes in cont.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Contractile ejection nanomachines being sheath–tube assemblies create an opening in the cell membrane to translocate molecules or ions across it. Here, on the most structurally investigated examples of the bacteriophage T4 tail and pyocin R2, we show that the rearrangement of the sheath structure resulting in its contraction and twist occurs in such a way that the contracted sheath becomes commensurate with the inner tube. This fact dictates the previously unknown simple geometrical relationship between the nanotube symmetries. Using the Frank and van der Merwe classical theory of commensurability, we study an interaction between two protein nanotubes forming such nanomachines and obtain an expression for the corresponding energy, which depends on the tube structures and their mutual arrangement. The appearance of commensurability between the contracted sheath and the inner tube decreases both the interaction energy and the total energy of the system. It improves the nanomachine efficiency, since the energy gain obtained increases the torque of the inner tube piercing the cell membrane.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"ulyankina-leontyev-maslova-allix-rakhmatullin-nevzorova-valeev-yalovega-etal-copperoxidesforenergystorageapplicationnovelpulsealternatingcurrentsynthesis-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S1369800117313975\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'ulyankina-leontyev-maslova-allix-rakhmatullin-nevzorova-valeev-yalovega-etal-copperoxidesforenergystorageapplicationnovelpulsealternatingcurrentsynthesis-2018', 'https://www.sciencedirect.com/science/article/pii/S1369800117313975', event);\">\n    Copper oxides for energy storage application: Novel pulse alternating current synthesis.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Ulyankina, A.; Leontyev, I.; Maslova, O.; Allix, M.; Rakhmatullin, A.; Nevzorova, N.; Valeev, R.; Yalovega, G.;  and Smirnova, N.\n</span>\n\n  \n\n</span>\n\n  <i>Materials Science in Semiconductor Processing</i>, 73: 111–116. January 2018.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S1369800117313975\"\n     onclick=\"log_download('ulyankina-leontyev-maslova-allix-rakhmatullin-nevzorova-valeev-yalovega-etal-copperoxidesforenergystorageapplicationnovelpulsealternatingcurrentsynthesis-2018', 'https://www.sciencedirect.com/science/article/pii/S1369800117313975', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Copper oxides for energy storage application: Novel pulse alternating current synthesis [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.mssp.2017.08.001\"\n     onclick=\"log_download('ulyankina-leontyev-maslova-allix-rakhmatullin-nevzorova-valeev-yalovega-etal-copperoxidesforenergystorageapplicationnovelpulsealternatingcurrentsynthesis-2018', 'http://doi.org/10.1016/j.mssp.2017.08.001', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/ulyankina-leontyev-maslova-allix-rakhmatullin-nevzorova-valeev-yalovega-etal-copperoxidesforenergystorageapplicationnovelpulsealternatingcurrentsynthesis-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('ulyankina-leontyev-maslova-allix-rakhmatullin-nevzorova-valeev-yalovega-etal-copperoxidesforenergystorageapplicationnovelpulsealternatingcurrentsynthesis-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{ulyankina_copper_2018,\n\tseries = {Semiconductor materials for green energy and environmental applications},\n\ttitle = {Copper oxides for energy storage application: {Novel} pulse alternating current synthesis},\n\tvolume = {73},\n\tissn = {1369-8001},\n\tshorttitle = {Copper oxides for energy storage application},\n\turl = {https://www.sciencedirect.com/science/article/pii/S1369800117313975},\n\tdoi = {10.1016/j.mssp.2017.08.001},\n\tabstract = {Copper oxide powders (CuOx) were reported to be electrochemically obtained under pulse alternating current by a facile and inexpensive one-pot method. The effect of the synthesis conditions on the copper electrode oxidation rate and product morphology and composition was studied. The CuOx products were characterized by X-ray powder diffraction (XRD), Raman spectroscopy, X-ray absorption near-edge structure (XANES) spectroscopy, energy dispersive spectroscopy (EDS), scanning electron microscopy (SEM) and transmission electron microscopy (TEM). Depending on the synthesis conditions, the powders reveal different morphologies and composition, such as Cu2O octahedra, Cu2O decorated with CuO or Cu2O-CuO bilayered composite. Cyclic voltammetry and charge-discharge measurements were used to study the electrochemical energy conversion properties of the materials. The results of the electrocatalytic study indicate that the powder with Cu2O-CuO bilayered polyhedra is suitable for use in methanol oxidation; and the powder with Cu2O octahedra has shown a good specific capacitance for supercapacitors.},\n\turldate = {2023-11-11},\n\tjournal = {Materials Science in Semiconductor Processing},\n\tauthor = {Ulyankina, A. and Leontyev, I. and Maslova, O. and Allix, M. and Rakhmatullin, A. and Nevzorova, N. and Valeev, R. and Yalovega, G. and Smirnova, N.},\n\tmonth = jan,\n\tyear = {2018},\n\tpages = {111--116},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Copper oxide powders (CuOx) were reported to be electrochemically obtained under pulse alternating current by a facile and inexpensive one-pot method. The effect of the synthesis conditions on the copper electrode oxidation rate and product morphology and composition was studied. The CuOx products were characterized by X-ray powder diffraction (XRD), Raman spectroscopy, X-ray absorption near-edge structure (XANES) spectroscopy, energy dispersive spectroscopy (EDS), scanning electron microscopy (SEM) and transmission electron microscopy (TEM). Depending on the synthesis conditions, the powders reveal different morphologies and composition, such as Cu2O octahedra, Cu2O decorated with CuO or Cu2O-CuO bilayered composite. Cyclic voltammetry and charge-discharge measurements were used to study the electrochemical energy conversion properties of the materials. The results of the electrocatalytic study indicate that the powder with Cu2O-CuO bilayered polyhedra is suitable for use in methanol oxidation; and the powder with Cu2O octahedra has shown a good specific capacitance for supercapacitors.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"talanov-shirokov-avakyan-talanov-borlakov-vanadiumclustersformationingeometricallyfrustratedspineloxidealvtextrm2otextrm4-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://scripts.iucr.org/cgi-bin/paper?dq5028\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'talanov-shirokov-avakyan-talanov-borlakov-vanadiumclustersformationingeometricallyfrustratedspineloxidealvtextrm2otextrm4-2018', 'http://scripts.iucr.org/cgi-bin/paper?dq5028', event);\">\n    Vanadium clusters formation in geometrically frustrated spinel oxide AlV$_{\\textrm{2}}$O$_{\\textrm{4}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Talanov, M. V.; Shirokov, V. B.; Avakyan, L. A.; Talanov, V. M.;  and Borlakov, K. S.\n</span>\n\n  \n\n</span>\n\n  <i>Acta Crystallographica Section B: Structural Science, Crystal Engineering and Materials</i>, 74(4): 337–353. August 2018.\n  <span class=\"note\">Number: 4 Publisher: International Union of Crystallography</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://scripts.iucr.org/cgi-bin/paper?dq5028\"\n     onclick=\"log_download('talanov-shirokov-avakyan-talanov-borlakov-vanadiumclustersformationingeometricallyfrustratedspineloxidealvtextrm2otextrm4-2018', 'http://scripts.iucr.org/cgi-bin/paper?dq5028', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Vanadium clusters formation in geometrically frustrated spinel oxide AlV$_{\\textrm{2}}$O$_{\\textrm{4}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1107/S2052520618007242\"\n     onclick=\"log_download('talanov-shirokov-avakyan-talanov-borlakov-vanadiumclustersformationingeometricallyfrustratedspineloxidealvtextrm2otextrm4-2018', 'http://doi.org/10.1107/S2052520618007242', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/talanov-shirokov-avakyan-talanov-borlakov-vanadiumclustersformationingeometricallyfrustratedspineloxidealvtextrm2otextrm4-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('talanov-shirokov-avakyan-talanov-borlakov-vanadiumclustersformationingeometricallyfrustratedspineloxidealvtextrm2otextrm4-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{talanov_vanadium_2018,\n\ttitle = {Vanadium clusters formation in geometrically frustrated spinel oxide {AlV}$_{\\textrm{2}}${O}$_{\\textrm{4}}$},\n\tvolume = {74},\n\tcopyright = {Copyright (c) 2018 International Union of Crystallography},\n\tissn = {2052-5206},\n\turl = {http://scripts.iucr.org/cgi-bin/paper?dq5028},\n\tdoi = {10.1107/S2052520618007242},\n\tabstract = {The spinel oxide AlV2O4 is a unique material, in which the formation of clusters is accompanied by atomic, charge and orbital ordering and a rhombohedral lattice distortion. In this work a theory of the structural phase transition in AlV2O4 is proposed. This theory is based on the study of the order-parameter symmetry, thermodynamics, electron density distribution, crystal chemistry and mechanisms of formation of the atomic and orbital structures of the rhombohedral phase. It is established that the critical order parameter is transformed according to irreducible representation k9(τ4) (in Kovalev notation) of the Fd {\\textbackslash}bar\\{3\\}m space group. Knowledge of the order-parameter symmetry allows us to show that the derived AlV2O4 rhombohedral structure is a result of displacements of all atom types and the ordering of Al atoms (1:1 order type in tetrahedral spinel sites), V atoms (1:1:6 order type in octahedral sites) and O atoms (1:1:3:3 order type), and the ordering of dxy, dxz and dyz orbitals. Application of the density functional theory showed that V atoms in the Kagomé sublattice formed separate trimers. Also, no sign of metallic bonding between separate vanadium trimers in the heptamer structure was found. The density functional theory study and the crystal chemical analysis of V—O bond lengths allowed us to assume the existence of dimers and trimers as main clusters in the structure of the AlV2O4 rhombohedral modification. The trimer model of the low-symmetry AlV2O4 structure is proposed. Within the Landau theory of phase transitions, typical diagrams of possible phase states are built. It is shown that phase states can be changed as a first-order phase transition close to the second order in the vicinity of tricritical points of the phase diagrams.},\n\tlanguage = {en},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Acta Crystallographica Section B: Structural Science, Crystal Engineering and Materials},\n\tauthor = {Talanov, M. V. and Shirokov, V. B. and Avakyan, L. A. and Talanov, V. M. and Borlakov, K. S.},\n\tmonth = aug,\n\tyear = {2018},\n\tnote = {Number: 4\nPublisher: International Union of Crystallography},\n\tpages = {337--353},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The spinel oxide AlV2O4 is a unique material, in which the formation of clusters is accompanied by atomic, charge and orbital ordering and a rhombohedral lattice distortion. In this work a theory of the structural phase transition in AlV2O4 is proposed. This theory is based on the study of the order-parameter symmetry, thermodynamics, electron density distribution, crystal chemistry and mechanisms of formation of the atomic and orbital structures of the rhombohedral phase. It is established that the critical order parameter is transformed according to irreducible representation k9(τ4) (in Kovalev notation) of the Fd \\bar\\3\\m space group. Knowledge of the order-parameter symmetry allows us to show that the derived AlV2O4 rhombohedral structure is a result of displacements of all atom types and the ordering of Al atoms (1:1 order type in tetrahedral spinel sites), V atoms (1:1:6 order type in octahedral sites) and O atoms (1:1:3:3 order type), and the ordering of dxy, dxz and dyz orbitals. Application of the density functional theory showed that V atoms in the Kagomé sublattice formed separate trimers. Also, no sign of metallic bonding between separate vanadium trimers in the heptamer structure was found. The density functional theory study and the crystal chemical analysis of V—O bond lengths allowed us to assume the existence of dimers and trimers as main clusters in the structure of the AlV2O4 rhombohedral modification. The trimer model of the low-symmetry AlV2O4 structure is proposed. Within the Landau theory of phase transitions, typical diagrams of possible phase states are built. It is shown that phase states can be changed as a first-order phase transition close to the second order in the vicinity of tricritical points of the phase diagrams.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kozakov-kochur-trotsenko-nikolskii-elmarssi-gorshunov-torgashev-valencestateofcationsinmanganitesprtextrm1xcatextrmxmnotextrm303x05fromxraydiffractionandxrayphotoelectronspectroscopy-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0925838818300021\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kozakov-kochur-trotsenko-nikolskii-elmarssi-gorshunov-torgashev-valencestateofcationsinmanganitesprtextrm1xcatextrmxmnotextrm303x05fromxraydiffractionandxrayphotoelectronspectroscopy-2018', 'https://www.sciencedirect.com/science/article/pii/S0925838818300021', event);\">\n    Valence state of cations in manganites Pr$_{\\textrm{1-x}}$Ca$_{\\textrm{x}}$MnO$_{\\textrm{3}}$ (0.3 ≤ x ≤ 0.5) from X-ray diffraction and X-ray photoelectron spectroscopy.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kozakov, A. T.; Kochur, A. G.; Trotsenko, V. G.; Nikolskii, A. V.; El Marssi, M.; Gorshunov, B. P.;  and Torgashev, V. I.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Alloys and Compounds</i>, 740: 132–142. April 2018.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0925838818300021\"\n     onclick=\"log_download('kozakov-kochur-trotsenko-nikolskii-elmarssi-gorshunov-torgashev-valencestateofcationsinmanganitesprtextrm1xcatextrmxmnotextrm303x05fromxraydiffractionandxrayphotoelectronspectroscopy-2018', 'https://www.sciencedirect.com/science/article/pii/S0925838818300021', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Valence state of cations in manganites Pr$_{\\textrm{1-x}}$Ca$_{\\textrm{x}}$MnO$_{\\textrm{3}}$ (0.3 ≤ x ≤ 0.5) from X-ray diffraction and X-ray photoelectron spectroscopy [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.jallcom.2018.01.002\"\n     onclick=\"log_download('kozakov-kochur-trotsenko-nikolskii-elmarssi-gorshunov-torgashev-valencestateofcationsinmanganitesprtextrm1xcatextrmxmnotextrm303x05fromxraydiffractionandxrayphotoelectronspectroscopy-2018', 'http://doi.org/10.1016/j.jallcom.2018.01.002', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kozakov-kochur-trotsenko-nikolskii-elmarssi-gorshunov-torgashev-valencestateofcationsinmanganitesprtextrm1xcatextrmxmnotextrm303x05fromxraydiffractionandxrayphotoelectronspectroscopy-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kozakov-kochur-trotsenko-nikolskii-elmarssi-gorshunov-torgashev-valencestateofcationsinmanganitesprtextrm1xcatextrmxmnotextrm303x05fromxraydiffractionandxrayphotoelectronspectroscopy-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kozakov_valence_2018,\n\ttitle = {Valence state of cations in manganites {Pr}$_{\\textrm{1-x}}${Ca}$_{\\textrm{x}}${MnO}$_{\\textrm{3}}$ (0.3 ≤ x ≤ 0.5) from {X}-ray diffraction and {X}-ray photoelectron spectroscopy},\n\tvolume = {740},\n\tissn = {0925-8388},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0925838818300021},\n\tdoi = {10.1016/j.jallcom.2018.01.002},\n\tabstract = {Polycrystalline Pr1-xCaxMnO3 (х = 0.3, 0.35, 04, 0.45, and 0.5) samples are synthesized by solid-state reaction method. Crystal structure of the samples is studied by X-ray diffraction method with Rietveld refinement. Diffraction patterns from all the samples are well indexed within the Pnma space group. It is shown that lattice parameters and unit cell volume decrease monotonically and O−Mn−O angles become closer to the ideal 180⁰ value upon the growth of x. Mn2p, Mn3s, Ca2p, Pr3d, Pr4d, and O1s X-ray photoelectron spectra are measured. Pr3d and Pr4d spectra are calculated in isolated ion approximation with approximate accounting for the charge transfer effect. Elemental compositions of samples are measured by the XPS method; they differ noticeably from the nominal ones. Charge compensation upon heterovalent Pr3+ → Ca2+ substitution is shown to realize via two mechanisms: creation of oxygen vacancies and formation of Mn4+ ions coexisting with Mn3+. Relative Mn4+/Mn3+ abundances are determined via decomposition of Mn2p and Mn3s XPS into contributions from the spectra of tri- and quadrivalent Mn ions. The amount of Mn4+ ions is shown to increase with Ca content x.},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Alloys and Compounds},\n\tauthor = {Kozakov, A. T. and Kochur, A. G. and Trotsenko, V. G. and Nikolskii, A. V. and El Marssi, M. and Gorshunov, B. P. and Torgashev, V. I.},\n\tmonth = apr,\n\tyear = {2018},\n\tkeywords = {XPS, Manganites, Cations valence state, Elemental composition, Mn/Mn content, PCaMnO (PCMO) ceramics, Vacancies, XRD},\n\tpages = {132--142},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Polycrystalline Pr1-xCaxMnO3 (х = 0.3, 0.35, 04, 0.45, and 0.5) samples are synthesized by solid-state reaction method. Crystal structure of the samples is studied by X-ray diffraction method with Rietveld refinement. Diffraction patterns from all the samples are well indexed within the Pnma space group. It is shown that lattice parameters and unit cell volume decrease monotonically and O−Mn−O angles become closer to the ideal 180⁰ value upon the growth of x. Mn2p, Mn3s, Ca2p, Pr3d, Pr4d, and O1s X-ray photoelectron spectra are measured. Pr3d and Pr4d spectra are calculated in isolated ion approximation with approximate accounting for the charge transfer effect. Elemental compositions of samples are measured by the XPS method; they differ noticeably from the nominal ones. Charge compensation upon heterovalent Pr3+ → Ca2+ substitution is shown to realize via two mechanisms: creation of oxygen vacancies and formation of Mn4+ ions coexisting with Mn3+. Relative Mn4+/Mn3+ abundances are determined via decomposition of Mn2p and Mn3s XPS into contributions from the spectra of tri- and quadrivalent Mn ions. The amount of Mn4+ ions is shown to increase with Ca content x.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"trotsenko-mikheykin-shirokov-razumnaya-bush-kadyrov-elmarssi-gorshunov-etal-temperaturebehavioroftherotationalorderparametersinalatextrm025catextrm075mnotextrm3solidsolution-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.3103/S1062873818030310\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'trotsenko-mikheykin-shirokov-razumnaya-bush-kadyrov-elmarssi-gorshunov-etal-temperaturebehavioroftherotationalorderparametersinalatextrm025catextrm075mnotextrm3solidsolution-2018', 'https://doi.org/10.3103/S1062873818030310', event);\">\n    Temperature Behavior of the Rotational Order Parameters in a La$_{\\textrm{0.25}}$Ca$_{\\textrm{0.75}}$MnO$_{\\textrm{3}}$ Solid Solution.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Trotsenko, V. G.; Mikheykin, A. S.; Shirokov, V. B.; Razumnaya, A. G.; Bush, A. A.; Kadyrov, L. S.; El Marssi, M.; Gorshunov, B. P.;  and Torgashev, V. I.\n</span>\n\n  \n\n</span>\n\n  <i>Bulletin of the Russian Academy of Sciences: Physics</i>, 82(3): 335–337. March 2018.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.3103/S1062873818030310\"\n     onclick=\"log_download('trotsenko-mikheykin-shirokov-razumnaya-bush-kadyrov-elmarssi-gorshunov-etal-temperaturebehavioroftherotationalorderparametersinalatextrm025catextrm075mnotextrm3solidsolution-2018', 'https://doi.org/10.3103/S1062873818030310', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Temperature Behavior of the Rotational Order Parameters in a La$_{\\textrm{0.25}}$Ca$_{\\textrm{0.75}}$MnO$_{\\textrm{3}}$ Solid Solution [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3103/S1062873818030310\"\n     onclick=\"log_download('trotsenko-mikheykin-shirokov-razumnaya-bush-kadyrov-elmarssi-gorshunov-etal-temperaturebehavioroftherotationalorderparametersinalatextrm025catextrm075mnotextrm3solidsolution-2018', 'http://doi.org/10.3103/S1062873818030310', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/trotsenko-mikheykin-shirokov-razumnaya-bush-kadyrov-elmarssi-gorshunov-etal-temperaturebehavioroftherotationalorderparametersinalatextrm025catextrm075mnotextrm3solidsolution-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('trotsenko-mikheykin-shirokov-razumnaya-bush-kadyrov-elmarssi-gorshunov-etal-temperaturebehavioroftherotationalorderparametersinalatextrm025catextrm075mnotextrm3solidsolution-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{trotsenko_temperature_2018,\n\ttitle = {Temperature {Behavior} of the {Rotational} {Order} {Parameters} in a {La}$_{\\textrm{0.25}}${Ca}$_{\\textrm{0.75}}${MnO}$_{\\textrm{3}}$ {Solid} {Solution}},\n\tvolume = {82},\n\tissn = {1934-9432},\n\turl = {https://doi.org/10.3103/S1062873818030310},\n\tdoi = {10.3103/S1062873818030310},\n\tabstract = {The behavior of the crystal structure of a La0.25Ca0.75MnO3 solid solution in the temperature range of 80–725 K is studied. It is established that rotational structural distortions predominate during the transition to a charge-ordered state},\n\tlanguage = {en},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Bulletin of the Russian Academy of Sciences: Physics},\n\tauthor = {Trotsenko, V. G. and Mikheykin, A. S. and Shirokov, V. B. and Razumnaya, A. G. and Bush, A. A. and Kadyrov, L. S. and El Marssi, M. and Gorshunov, B. P. and Torgashev, V. I.},\n\tmonth = mar,\n\tyear = {2018},\n\tpages = {335--337},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The behavior of the crystal structure of a La0.25Ca0.75MnO3 solid solution in the temperature range of 80–725 K is studied. It is established that rotational structural distortions predominate during the transition to a charge-ordered state\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kabirov-gavrilyachenko-bogatin-sitalo-yatsenko-effectofamagneticfieldonthepermittivityof80latextrm07srtextrm03mnotextrm320geotextrm2composite-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1063783418010110\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kabirov-gavrilyachenko-bogatin-sitalo-yatsenko-effectofamagneticfieldonthepermittivityof80latextrm07srtextrm03mnotextrm320geotextrm2composite-2018', 'https://doi.org/10.1134/S1063783418010110', event);\">\n    Effect of a magnetic field on the permittivity of 80%La$_{\\textrm{0.7}}$Sr$_{\\textrm{0.3}}$MnO$_{\\textrm{3}}$/20%GeO$_{\\textrm{2}}$ composite.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kabirov, Y. V.; Gavrilyachenko, V. G.; Bogatin, A. S.; Sitalo, E. I.;  and Yatsenko, V. K.\n</span>\n\n  \n\n</span>\n\n  <i>Physics of the Solid State</i>, 60(1): 60–63. January 2018.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1063783418010110\"\n     onclick=\"log_download('kabirov-gavrilyachenko-bogatin-sitalo-yatsenko-effectofamagneticfieldonthepermittivityof80latextrm07srtextrm03mnotextrm320geotextrm2composite-2018', 'https://doi.org/10.1134/S1063783418010110', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Effect of a magnetic field on the permittivity of 80%La$_{\\textrm{0.7}}$Sr$_{\\textrm{0.3}}$MnO$_{\\textrm{3}}$/20%GeO$_{\\textrm{2}}$ composite [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1063783418010110\"\n     onclick=\"log_download('kabirov-gavrilyachenko-bogatin-sitalo-yatsenko-effectofamagneticfieldonthepermittivityof80latextrm07srtextrm03mnotextrm320geotextrm2composite-2018', 'http://doi.org/10.1134/S1063783418010110', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kabirov-gavrilyachenko-bogatin-sitalo-yatsenko-effectofamagneticfieldonthepermittivityof80latextrm07srtextrm03mnotextrm320geotextrm2composite-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kabirov-gavrilyachenko-bogatin-sitalo-yatsenko-effectofamagneticfieldonthepermittivityof80latextrm07srtextrm03mnotextrm320geotextrm2composite-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kabirov_effect_2018,\n\ttitle = {Effect of a magnetic field on the permittivity of 80\\%{La}$_{\\textrm{0.7}}${Sr}$_{\\textrm{0.3}}${MnO}$_{\\textrm{3}}$/20\\%{GeO}$_{\\textrm{2}}$ composite},\n\tvolume = {60},\n\tissn = {1090-6460},\n\turl = {https://doi.org/10.1134/S1063783418010110},\n\tdoi = {10.1134/S1063783418010110},\n\tabstract = {The dielectric properties of a magnetoresistive conducting two-phase 80\\%La0.7Sr0.3MnO3/20\\%GeO2 (wt \\%) composite have been studied near the percolation threshold in magnetic fields from 0 to 15 kOe at frequencies of the measurement field from 5 kHz to 1 MHz. The samples have inductive impedances; i.e., their permittivities can be considered negative due to a high conductivity in this frequency range. The permittivity increases in magnitude in magnetic field, and the values of the magnetodielectric coefficient reach 23\\% at room temperature. The reasons for the effect of magnetic field on the dielectric permittivity of samples are discussed.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Physics of the Solid State},\n\tauthor = {Kabirov, Yu. V. and Gavrilyachenko, V. G. and Bogatin, A. S. and Sitalo, E. I. and Yatsenko, V. K.},\n\tmonth = jan,\n\tyear = {2018},\n\tpages = {60--63},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The dielectric properties of a magnetoresistive conducting two-phase 80%La0.7Sr0.3MnO3/20%GeO2 (wt %) composite have been studied near the percolation threshold in magnetic fields from 0 to 15 kOe at frequencies of the measurement field from 5 kHz to 1 MHz. The samples have inductive impedances; i.e., their permittivities can be considered negative due to a high conductivity in this frequency range. The permittivity increases in magnitude in magnetic field, and the values of the magnetodielectric coefficient reach 23% at room temperature. The reasons for the effect of magnetic field on the dielectric permittivity of samples are discussed.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"gorshunov-zhukova-komandin-torgashev-muratov-aleshchenko-demishev-shitsevalova-etal-collectiveinfraredexcitationinlubtextrm12cageglass-2018\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S0021364018020029\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'gorshunov-zhukova-komandin-torgashev-muratov-aleshchenko-demishev-shitsevalova-etal-collectiveinfraredexcitationinlubtextrm12cageglass-2018', 'https://doi.org/10.1134/S0021364018020029', event);\">\n    Collective Infrared Excitation in LuB$_{\\textrm{12}}$ Cage-Glass.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Gorshunov, B. P.; Zhukova, E. S.; Komandin, G. A.; Torgashev, V. I.; Muratov, A. V.; Aleshchenko, Y. A.; Demishev, S. V.; Shitsevalova, N. Y.; Filipov, V. B.;  and Sluchanko, N. E.\n</span>\n\n  \n\n</span>\n\n  <i>JETP Letters</i>, 107(2): 100–105. January 2018.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S0021364018020029\"\n     onclick=\"log_download('gorshunov-zhukova-komandin-torgashev-muratov-aleshchenko-demishev-shitsevalova-etal-collectiveinfraredexcitationinlubtextrm12cageglass-2018', 'https://doi.org/10.1134/S0021364018020029', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Collective Infrared Excitation in LuB$_{\\textrm{12}}$ Cage-Glass [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S0021364018020029\"\n     onclick=\"log_download('gorshunov-zhukova-komandin-torgashev-muratov-aleshchenko-demishev-shitsevalova-etal-collectiveinfraredexcitationinlubtextrm12cageglass-2018', 'http://doi.org/10.1134/S0021364018020029', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/gorshunov-zhukova-komandin-torgashev-muratov-aleshchenko-demishev-shitsevalova-etal-collectiveinfraredexcitationinlubtextrm12cageglass-2018\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('gorshunov-zhukova-komandin-torgashev-muratov-aleshchenko-demishev-shitsevalova-etal-collectiveinfraredexcitationinlubtextrm12cageglass-2018')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{gorshunov_collective_2018,\n\ttitle = {Collective {Infrared} {Excitation} in {LuB}$_{\\textrm{12}}$ {Cage}-{Glass}},\n\tvolume = {107},\n\tissn = {1090-6487},\n\turl = {https://doi.org/10.1134/S0021364018020029},\n\tdoi = {10.1134/S0021364018020029},\n\tabstract = {By measuring room temperature infrared (40–35000 cm–1) reflectivity of metallic LuB12 single crystals with different isotopic compositions (natB, 10B, 11B), we find that to model the spectrum we had to introduce, additionally to Drude free-carrier component, a broad excitation with unusually large dielectric contribution (Δε = 8000 ± 4000), which is characterized by a non-Lorentzian lineshape. It is suggested that the origin of the excitation is connected with cooperative dynamics of Jahn–Teller active B12 molecules producing quasilocal vibrations (rattling modes) of caged lutetium ions. The coupling of the Lu3+ rattling motions with the charge carriers of conduction band is proposed to be the reason of strongly damped character of the excitation.},\n\tlanguage = {en},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {JETP Letters},\n\tauthor = {Gorshunov, B. P. and Zhukova, E. S. and Komandin, G. A. and Torgashev, V. I. and Muratov, A. V. and Aleshchenko, Yu. A. and Demishev, S. V. and Shitsevalova, N. Yu. and Filipov, V. B. and Sluchanko, N. E.},\n\tmonth = jan,\n\tyear = {2018},\n\tpages = {100--105},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  By measuring room temperature infrared (40–35000 cm–1) reflectivity of metallic LuB12 single crystals with different isotopic compositions (natB, 10B, 11B), we find that to model the spectrum we had to introduce, additionally to Drude free-carrier component, a broad excitation with unusually large dielectric contribution (Δε = 8000 ± 4000), which is characterized by a non-Lorentzian lineshape. It is suggested that the origin of the excitation is connected with cooperative dynamics of Jahn–Teller active B12 molecules producing quasilocal vibrations (rattling modes) of caged lutetium ions. The coupling of the Lu3+ rattling motions with the charge carriers of conduction band is proposed to be the reason of strongly damped character of the excitation.\n</div>\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2017\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2017')\"\n      onkeypress=\"toggleGroup('group_2017')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2017</span>\n      <span class=\"bibbase_group_count\">\n        \n        (41)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"levshov-parret-tran-michel-cao-nguyen-arenal-popov-etal-photoluminescencefromanindividualdoublewalledcarbonnanotube-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.96.195410\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'levshov-parret-tran-michel-cao-nguyen-arenal-popov-etal-photoluminescencefromanindividualdoublewalledcarbonnanotube-2017', 'https://link.aps.org/doi/10.1103/PhysRevB.96.195410', event);\">\n    Photoluminescence from an individual double-walled carbon nanotube.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Levshov, D. I.; Parret, R.; Tran, H.; Michel, T.; Cao, T. T.; Nguyen, V. C.; Arenal, R.; Popov, V. N.; Rochal, S. B.; Sauvajol, J.; Zahab, A.;  and Paillet, M.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 96(19): 195410. November 2017.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.96.195410\"\n     onclick=\"log_download('levshov-parret-tran-michel-cao-nguyen-arenal-popov-etal-photoluminescencefromanindividualdoublewalledcarbonnanotube-2017', 'https://link.aps.org/doi/10.1103/PhysRevB.96.195410', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Photoluminescence from an individual double-walled carbon nanotube [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.96.195410\"\n     onclick=\"log_download('levshov-parret-tran-michel-cao-nguyen-arenal-popov-etal-photoluminescencefromanindividualdoublewalledcarbonnanotube-2017', 'http://doi.org/10.1103/PhysRevB.96.195410', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/levshov-parret-tran-michel-cao-nguyen-arenal-popov-etal-photoluminescencefromanindividualdoublewalledcarbonnanotube-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('levshov-parret-tran-michel-cao-nguyen-arenal-popov-etal-photoluminescencefromanindividualdoublewalledcarbonnanotube-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{levshov_photoluminescence_2017,\n\ttitle = {Photoluminescence from an individual double-walled carbon nanotube},\n\tvolume = {96},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.96.195410},\n\tdoi = {10.1103/PhysRevB.96.195410},\n\tabstract = {We report direct and unambiguous evidence of the existence of inner semiconducting tube (ISCT) photoluminescence (PL) from measurements performed on four individual freestanding index-identified double-walled carbon nanotubes (DWNTs). Based on thorough Rayleigh scattering, Raman scattering, and PL experiments, we are able to demonstrate that the ISCT PL is observed with a quantum yield estimated to be a few 10−6 independent of the semiconducting or metallic nature of the outer tube. This result is mainly attributed to ultrafast exciton transfer from the inner to outer tube. Furthermore, by carrying out PL excitation experiments on the (14,1)@(15,12) DWNT, we show that the ISCT PL can be detected through the optical excitation of the outer tube, indicating that the exciton transfer can also occur in the opposite way.},\n\tnumber = {19},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Levshov, Dmitry I. and Parret, Romain and Tran, Huy-Nam and Michel, Thierry and Cao, Thi Thanh and Nguyen, Van Chuc and Arenal, Raul and Popov, Valentin N. and Rochal, Sergei B. and Sauvajol, Jean-Louis and Zahab, Ahmed-Azmi and Paillet, Matthieu},\n\tmonth = nov,\n\tyear = {2017},\n\tnote = {Publisher: American Physical Society},\n\tpages = {195410},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\6UGH2Z3Z\\\\Levshov и др. - 2017 - Photoluminescence from an individual double-walled.pdf:application/pdf;APS Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\4XVAB652\\\\PhysRevB.96.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We report direct and unambiguous evidence of the existence of inner semiconducting tube (ISCT) photoluminescence (PL) from measurements performed on four individual freestanding index-identified double-walled carbon nanotubes (DWNTs). Based on thorough Rayleigh scattering, Raman scattering, and PL experiments, we are able to demonstrate that the ISCT PL is observed with a quantum yield estimated to be a few 10−6 independent of the semiconducting or metallic nature of the outer tube. This result is mainly attributed to ultrafast exciton transfer from the inner to outer tube. Furthermore, by carrying out PL excitation experiments on the (14,1)@(15,12) DWNT, we show that the ISCT PL can be detected through the optical excitation of the outer tube, indicating that the exciton transfer can also occur in the opposite way.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"motovilov-savinov-zhukova-pronin-gagkaeva-grinenko-sidoruk-voeikova-etal-observationofdielectricuniversalitiesinalbumincytochromecandshewanellaoneidensismr1extracellularmatrix-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.nature.com/articles/s41598-017-15693-y\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'motovilov-savinov-zhukova-pronin-gagkaeva-grinenko-sidoruk-voeikova-etal-observationofdielectricuniversalitiesinalbumincytochromecandshewanellaoneidensismr1extracellularmatrix-2017', 'https://www.nature.com/articles/s41598-017-15693-y', event);\">\n    Observation of dielectric universalities in albumin, cytochrome C and Shewanella oneidensis MR-1 extracellular matrix.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Motovilov, K. A.; Savinov, M.; Zhukova, E. S.; Pronin, A. A.; Gagkaeva, Z. V.; Grinenko, V.; Sidoruk, K. V.; Voeikova, T. A.; Barzilovich, P. Y.; Grebenko, A. K.; Lisovskii, S. V.; Torgashev, V. I.; Bednyakov, P.; Pokorný, J.; Dressel, M.;  and Gorshunov, B. P.\n</span>\n\n  \n\n</span>\n\n  <i>Scientific Reports</i>, 7(1): 15731. November 2017.\n  <span class=\"note\">Number: 1 Publisher: Nature Publishing Group</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.nature.com/articles/s41598-017-15693-y\"\n     onclick=\"log_download('motovilov-savinov-zhukova-pronin-gagkaeva-grinenko-sidoruk-voeikova-etal-observationofdielectricuniversalitiesinalbumincytochromecandshewanellaoneidensismr1extracellularmatrix-2017', 'https://www.nature.com/articles/s41598-017-15693-y', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Observation of dielectric universalities in albumin, cytochrome C and Shewanella oneidensis MR-1 extracellular matrix [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1038/s41598-017-15693-y\"\n     onclick=\"log_download('motovilov-savinov-zhukova-pronin-gagkaeva-grinenko-sidoruk-voeikova-etal-observationofdielectricuniversalitiesinalbumincytochromecandshewanellaoneidensismr1extracellularmatrix-2017', 'http://doi.org/10.1038/s41598-017-15693-y', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/motovilov-savinov-zhukova-pronin-gagkaeva-grinenko-sidoruk-voeikova-etal-observationofdielectricuniversalitiesinalbumincytochromecandshewanellaoneidensismr1extracellularmatrix-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('motovilov-savinov-zhukova-pronin-gagkaeva-grinenko-sidoruk-voeikova-etal-observationofdielectricuniversalitiesinalbumincytochromecandshewanellaoneidensismr1extracellularmatrix-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{motovilov_observation_2017,\n\ttitle = {Observation of dielectric universalities in albumin, cytochrome {C} and {Shewanella} oneidensis {MR}-1 extracellular matrix},\n\tvolume = {7},\n\tcopyright = {2017 The Author(s)},\n\tissn = {2045-2322},\n\turl = {https://www.nature.com/articles/s41598-017-15693-y},\n\tdoi = {10.1038/s41598-017-15693-y},\n\tabstract = {The electrodynamics of metals is well understood within the Drude conductivity model; properties of insulators and semiconductors are governed by a gap in the electronic states. But there is a great variety of disordered materials that do not fall in these categories and still respond to external field in an amazingly uniform manner. At radiofrequencies delocalized charges yield a frequency-independent conductivity σ1(ν) whose magnitude exponentially decreases while cooling. With increasing frequency, dispersionless conductivity starts to reveal a power-law dependence σ1(ν)∝νswith s {\\textless} 1 caused by hopping charge carriers. At low temperatures, such Universal Dielectric Response can cross over to another universal regime with nearly constant loss ε″∝σ1/ν = const. The powerful research potential based on such universalities is widely used in condensed matter physics. Here we study the broad-band (1–1012 Hz) dielectric response of Shewanella oneidensis MR-1 extracellular matrix, cytochrome C and serum albumin. Applying concepts of condensed matter physics, we identify transport mechanisms and a number of energy, time, frequency, spatial and temperature scales in these biological objects, which can provide us with deeper insight into the protein dynamics.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Scientific Reports},\n\tauthor = {Motovilov, K. A. and Savinov, M. and Zhukova, E. S. and Pronin, A. A. and Gagkaeva, Z. V. and Grinenko, V. and Sidoruk, K. V. and Voeikova, T. A. and Barzilovich, P. Yu and Grebenko, A. K. and Lisovskii, S. V. and Torgashev, V. I. and Bednyakov, P. and Pokorný, J. and Dressel, M. and Gorshunov, B. P.},\n\tmonth = nov,\n\tyear = {2017},\n\tnote = {Number: 1\nPublisher: Nature Publishing Group},\n\tkeywords = {Biomaterials – proteins, Polymers},\n\tpages = {15731},\n\tfile = {Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\4QFUHD76\\\\Motovilov и др. - 2017 - Observation of dielectric universalities in albumi.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The electrodynamics of metals is well understood within the Drude conductivity model; properties of insulators and semiconductors are governed by a gap in the electronic states. But there is a great variety of disordered materials that do not fall in these categories and still respond to external field in an amazingly uniform manner. At radiofrequencies delocalized charges yield a frequency-independent conductivity σ1(ν) whose magnitude exponentially decreases while cooling. With increasing frequency, dispersionless conductivity starts to reveal a power-law dependence σ1(ν)∝νswith s \\textless 1 caused by hopping charge carriers. At low temperatures, such Universal Dielectric Response can cross over to another universal regime with nearly constant loss ε″∝σ1/ν = const. The powerful research potential based on such universalities is widely used in condensed matter physics. Here we study the broad-band (1–1012 Hz) dielectric response of Shewanella oneidensis MR-1 extracellular matrix, cytochrome C and serum albumin. Applying concepts of condensed matter physics, we identify transport mechanisms and a number of energy, time, frequency, spatial and temperature scales in these biological objects, which can provide us with deeper insight into the protein dynamics.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"chalin-avramenko-rochal-simpletheoryoflowtemperaturethermalconductivityinsingleanddoublewalledcarbonnanotubes-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.96.155413\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'chalin-avramenko-rochal-simpletheoryoflowtemperaturethermalconductivityinsingleanddoublewalledcarbonnanotubes-2017', 'https://link.aps.org/doi/10.1103/PhysRevB.96.155413', event);\">\n    Simple theory of low-temperature thermal conductivity in single- and double-walled carbon nanotubes.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Chalin, D. V.; Avramenko, M. V.;  and Rochal, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 96(15): 155413. October 2017.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.96.155413\"\n     onclick=\"log_download('chalin-avramenko-rochal-simpletheoryoflowtemperaturethermalconductivityinsingleanddoublewalledcarbonnanotubes-2017', 'https://link.aps.org/doi/10.1103/PhysRevB.96.155413', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Simple theory of low-temperature thermal conductivity in single- and double-walled carbon nanotubes [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.96.155413\"\n     onclick=\"log_download('chalin-avramenko-rochal-simpletheoryoflowtemperaturethermalconductivityinsingleanddoublewalledcarbonnanotubes-2017', 'http://doi.org/10.1103/PhysRevB.96.155413', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/chalin-avramenko-rochal-simpletheoryoflowtemperaturethermalconductivityinsingleanddoublewalledcarbonnanotubes-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('chalin-avramenko-rochal-simpletheoryoflowtemperaturethermalconductivityinsingleanddoublewalledcarbonnanotubes-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{chalin_simple_2017,\n\ttitle = {Simple theory of low-temperature thermal conductivity in single- and double-walled carbon nanotubes},\n\tvolume = {96},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.96.155413},\n\tdoi = {10.1103/PhysRevB.96.155413},\n\tabstract = {Low-temperature phonon thermal conductance (PTC) of any 1D system increases proportionally to the temperature. However, here we show that in single- and double-walled carbon nanotubes (CNTs), starting from 3–6 K, the PTC increases faster than the linear function, since the low-frequency modes of dispersion curves, which do not tend to zero together with the wave vector, are excited. To develop the PTC theory, we combine the Landauer&#x27;s ballistic approach with the simple continuous model proposed for the calculation of the low-frequency phonon spectra of both free nanotubes and those interacting with an environment. The approach obtained is valid not only for commensurate double-walled CNTs, but also for incommensurate ones. The temperature-dependent relation between the PTC of double-walled CNT and those of its constituent SWNTs is obtained and discussed. The low-temperature heat transfer in bulk materials originated from CNTs is also considered and the upper limit of thermal conductivity of such materials is determined. We argue that the ideal material consisting of CNTs can challenge diamond only when the mean length of its defect-free nanotubes reaches at least one hundred of micrometers.},\n\tnumber = {15},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Chalin, D. V. and Avramenko, M. V. and Rochal, S. B.},\n\tmonth = oct,\n\tyear = {2017},\n\tnote = {Publisher: American Physical Society},\n\tpages = {155413},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Low-temperature phonon thermal conductance (PTC) of any 1D system increases proportionally to the temperature. However, here we show that in single- and double-walled carbon nanotubes (CNTs), starting from 3–6 K, the PTC increases faster than the linear function, since the low-frequency modes of dispersion curves, which do not tend to zero together with the wave vector, are excited. To develop the PTC theory, we combine the Landauer's ballistic approach with the simple continuous model proposed for the calculation of the low-frequency phonon spectra of both free nanotubes and those interacting with an environment. The approach obtained is valid not only for commensurate double-walled CNTs, but also for incommensurate ones. The temperature-dependent relation between the PTC of double-walled CNT and those of its constituent SWNTs is obtained and discussed. The low-temperature heat transfer in bulk materials originated from CNTs is also considered and the upper limit of thermal conductivity of such materials is determined. We argue that the ideal material consisting of CNTs can challenge diamond only when the mean length of its defect-free nanotubes reaches at least one hundred of micrometers.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"konevtsova-pimonov-lorman-rochal-quasicrystallineandcrystallinetypesoflocalproteinorderincapsidsofsmallviruses-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/1361-648X/aa7211\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'konevtsova-pimonov-lorman-rochal-quasicrystallineandcrystallinetypesoflocalproteinorderincapsidsofsmallviruses-2017', 'https://dx.doi.org/10.1088/1361-648X/aa7211', event);\">\n    Quasicrystalline and crystalline types of local protein order in capsids of small viruses.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Konevtsova, O. V.; Pimonov, V. V.; Lorman, V. L.;  and Rochal, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics: Condensed Matter</i>, 29(28): 284002. June 2017.\n  <span class=\"note\">Publisher: IOP Publishing</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/1361-648X/aa7211\"\n     onclick=\"log_download('konevtsova-pimonov-lorman-rochal-quasicrystallineandcrystallinetypesoflocalproteinorderincapsidsofsmallviruses-2017', 'https://dx.doi.org/10.1088/1361-648X/aa7211', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Quasicrystalline and crystalline types of local protein order in capsids of small viruses [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/1361-648X/aa7211\"\n     onclick=\"log_download('konevtsova-pimonov-lorman-rochal-quasicrystallineandcrystallinetypesoflocalproteinorderincapsidsofsmallviruses-2017', 'http://doi.org/10.1088/1361-648X/aa7211', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/konevtsova-pimonov-lorman-rochal-quasicrystallineandcrystallinetypesoflocalproteinorderincapsidsofsmallviruses-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('konevtsova-pimonov-lorman-rochal-quasicrystallineandcrystallinetypesoflocalproteinorderincapsidsofsmallviruses-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{konevtsova_quasicrystalline_2017,\n\ttitle = {Quasicrystalline and crystalline types of local protein order in capsids of small viruses},\n\tvolume = {29},\n\tissn = {0953-8984},\n\turl = {https://dx.doi.org/10.1088/1361-648X/aa7211},\n\tdoi = {10.1088/1361-648X/aa7211},\n\tabstract = {Like metal alloys and micellar systems in soft matter, the viral capsid structures can be of crystalline and quasicrystalline types. We reveal the local quasicrystalline order of proteins in small spherical viral capsids using their nets of dodecahedral type. We show that the structure of some of the viral shells is well described in terms of a chiral pentagonal tiling, whose nodes coincide with centers of mass of protein molecules. The chiral protein packing found in these capsids originates from the pentagonal Penrose tiling (PPT), due to a specific phason reconstruction needed to fit the protein order at the adjacent dodecahedron faces. Via examples of small spherical viral shells and geminate capsid of a Maize Streak virus, we discuss the benefits and shortcomings of the usage of a dodecahedral net in comparison to icosahedral one, which is commonly applied for the modeling of viral shells with a crystalline local order.},\n\tlanguage = {en},\n\tnumber = {28},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics: Condensed Matter},\n\tauthor = {Konevtsova, O. V. and Pimonov, V. V. and Lorman, V. L. and Rochal, S. B.},\n\tmonth = jun,\n\tyear = {2017},\n\tnote = {Publisher: IOP Publishing},\n\tpages = {284002},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Like metal alloys and micellar systems in soft matter, the viral capsid structures can be of crystalline and quasicrystalline types. We reveal the local quasicrystalline order of proteins in small spherical viral capsids using their nets of dodecahedral type. We show that the structure of some of the viral shells is well described in terms of a chiral pentagonal tiling, whose nodes coincide with centers of mass of protein molecules. The chiral protein packing found in these capsids originates from the pentagonal Penrose tiling (PPT), due to a specific phason reconstruction needed to fit the protein order at the adjacent dodecahedron faces. Via examples of small spherical viral shells and geminate capsid of a Maize Streak virus, we discuss the benefits and shortcomings of the usage of a dodecahedral net in comparison to icosahedral one, which is commonly applied for the modeling of viral shells with a crystalline local order.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"akbaeva-sitalo-gavrilyachenko-panchenko-dielectricspectrumofmulticomponentrelaxorceramicsbasedonpzt-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/00150193.2017.1290499\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'akbaeva-sitalo-gavrilyachenko-panchenko-dielectricspectrumofmulticomponentrelaxorceramicsbasedonpzt-2017', 'https://doi.org/10.1080/00150193.2017.1290499', event);\">\n    Dielectric spectrum of multicomponent relaxor ceramics based on PZT.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Akbaeva, G.; Sitalo, E.; Gavrilyachenko, V.;  and Panchenko, E.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 509(1): 10–13. March 2017.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2017.1290499</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/00150193.2017.1290499\"\n     onclick=\"log_download('akbaeva-sitalo-gavrilyachenko-panchenko-dielectricspectrumofmulticomponentrelaxorceramicsbasedonpzt-2017', 'https://doi.org/10.1080/00150193.2017.1290499', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Dielectric spectrum of multicomponent relaxor ceramics based on PZT [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150193.2017.1290499\"\n     onclick=\"log_download('akbaeva-sitalo-gavrilyachenko-panchenko-dielectricspectrumofmulticomponentrelaxorceramicsbasedonpzt-2017', 'http://doi.org/10.1080/00150193.2017.1290499', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/akbaeva-sitalo-gavrilyachenko-panchenko-dielectricspectrumofmulticomponentrelaxorceramicsbasedonpzt-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('akbaeva-sitalo-gavrilyachenko-panchenko-dielectricspectrumofmulticomponentrelaxorceramicsbasedonpzt-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{akbaeva_dielectric_2017,\n\ttitle = {Dielectric spectrum of multicomponent relaxor ceramics based on {PZT}},\n\tvolume = {509},\n\tissn = {0015-0193},\n\turl = {https://doi.org/10.1080/00150193.2017.1290499},\n\tdoi = {10.1080/00150193.2017.1290499},\n\tabstract = {The dielectric spectrum of multicomponent relaxor ceramic based on PZT was studied. In non-polarized sample, Debye-type dispersion region is found with the dispersion frequency of the order of 106 Hz. During polarization of the sample, this dispersion is suppressed. It is assumed that upon cooling from the paraphrase, without applied electric field, the relaxor ceramics transition to the dipole glass state occurs. Polarization converts it into a ferroelectric state, which is confirmed by characteristic piezoresonance response in the dielectric spectrum.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Ferroelectrics},\n\tauthor = {Akbaeva, G.M. and Sitalo, E.I. and Gavrilyachenko, V.G. and Panchenko, E.M.},\n\tmonth = mar,\n\tyear = {2017},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/00150193.2017.1290499},\n\tkeywords = {dielectric properties, Lead zirconate titanate, relaxor},\n\tpages = {10--13},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The dielectric spectrum of multicomponent relaxor ceramic based on PZT was studied. In non-polarized sample, Debye-type dispersion region is found with the dispersion frequency of the order of 106 Hz. During polarization of the sample, this dispersion is suppressed. It is assumed that upon cooling from the paraphrase, without applied electric field, the relaxor ceramics transition to the dipole glass state occurs. Polarization converts it into a ferroelectric state, which is confirmed by characteristic piezoresonance response in the dielectric spectrum.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"rochal-konevtsova-lorman-staticanddynamichiddensymmetriesoficosahedralviralcapsids-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://pubs.rsc.org/en/content/articlelanding/2017/nr/c7nr04020b\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'rochal-konevtsova-lorman-staticanddynamichiddensymmetriesoficosahedralviralcapsids-2017', 'https://pubs.rsc.org/en/content/articlelanding/2017/nr/c7nr04020b', event);\">\n    Static and dynamic hidden symmetries of icosahedral viral capsids.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Rochal, S. B.; Konevtsova, O. V.;  and Lorman, V. L.\n</span>\n\n  \n\n</span>\n\n  <i>Nanoscale</i>, 9(34): 12449–12460. August 2017.\n  <span class=\"note\">Publisher: The Royal Society of Chemistry</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://pubs.rsc.org/en/content/articlelanding/2017/nr/c7nr04020b\"\n     onclick=\"log_download('rochal-konevtsova-lorman-staticanddynamichiddensymmetriesoficosahedralviralcapsids-2017', 'https://pubs.rsc.org/en/content/articlelanding/2017/nr/c7nr04020b', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Static and dynamic hidden symmetries of icosahedral viral capsids [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1039/C7NR04020B\"\n     onclick=\"log_download('rochal-konevtsova-lorman-staticanddynamichiddensymmetriesoficosahedralviralcapsids-2017', 'http://doi.org/10.1039/C7NR04020B', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/rochal-konevtsova-lorman-staticanddynamichiddensymmetriesoficosahedralviralcapsids-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('rochal-konevtsova-lorman-staticanddynamichiddensymmetriesoficosahedralviralcapsids-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{rochal_static_2017,\n\ttitle = {Static and dynamic hidden symmetries of icosahedral viral capsids},\n\tvolume = {9},\n\tissn = {2040-3372},\n\turl = {https://pubs.rsc.org/en/content/articlelanding/2017/nr/c7nr04020b},\n\tdoi = {10.1039/C7NR04020B},\n\tabstract = {Viral shells self-assemble from identical proteins, which tend to form equivalent environments in the resulting assembly. However, in icosahedral capsids containing more than 60 proteins, they are enforced to occupy not only the symmetrically equivalent locations but also the quasi-equivalent ones. Due to this important fact, static and dynamic symmetries of viral shells can include additional hidden components. Here, developing the Caspar and Klug ideas concerning the quasi-equivalence of protein environments, we derive the simplest hexagonal tilings, that in principle could correspond to the local protein order in viral shells, and apply the resulting theory to nucleocytoplasmic large dsDNA viruses. In addition, analyzing the dynamic symmetry of the P22 viral shell, we demonstrate that the collective critical modes responsible for the protein reorganization during the procapsid maturation are approximately equivalent to the normal modes of the isotropic spherical membrane with O(3) symmetry. Furthermore, we establish the relationship between the dynamic symmetry of the P22 procapsid and the protein arrangement regularities that appear only in the mature capsid.},\n\tlanguage = {en},\n\tnumber = {34},\n\turldate = {2023-11-11},\n\tjournal = {Nanoscale},\n\tauthor = {Rochal, Sergey B. and Konevtsova, Olga V. and Lorman, Vladimir L.},\n\tmonth = aug,\n\tyear = {2017},\n\tnote = {Publisher: The Royal Society of Chemistry},\n\tpages = {12449--12460},\n\tfile = {Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\BKZZ384I\\\\Rochal и др. - 2017 - Static and dynamic hidden symmetries of icosahedra.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Viral shells self-assemble from identical proteins, which tend to form equivalent environments in the resulting assembly. However, in icosahedral capsids containing more than 60 proteins, they are enforced to occupy not only the symmetrically equivalent locations but also the quasi-equivalent ones. Due to this important fact, static and dynamic symmetries of viral shells can include additional hidden components. Here, developing the Caspar and Klug ideas concerning the quasi-equivalence of protein environments, we derive the simplest hexagonal tilings, that in principle could correspond to the local protein order in viral shells, and apply the resulting theory to nucleocytoplasmic large dsDNA viruses. In addition, analyzing the dynamic symmetry of the P22 viral shell, we demonstrate that the collective critical modes responsible for the protein reorganization during the procapsid maturation are approximately equivalent to the normal modes of the isotropic spherical membrane with O(3) symmetry. Furthermore, we establish the relationship between the dynamic symmetry of the P22 procapsid and the protein arrangement regularities that appear only in the mature capsid.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shpanko-sidorenko-semenchev-lyanguzov-anisimova-anticorrosionpropertiesandphysicochemicalcharacteristicsoforganicfilmsbasedonheterocyclicimidazolederivative-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S207020511702023X\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shpanko-sidorenko-semenchev-lyanguzov-anisimova-anticorrosionpropertiesandphysicochemicalcharacteristicsoforganicfilmsbasedonheterocyclicimidazolederivative-2017', 'https://doi.org/10.1134/S207020511702023X', event);\">\n    Anticorrosion properties and physicochemical characteristics of organic films based on heterocyclic imidazole derivative.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shpan’ko, S. P.; Sidorenko, E. N.; Semenchev, A. F.; Lyanguzov, N. V.;  and Anisimova, V. A.\n</span>\n\n  \n\n</span>\n\n  <i>Protection of Metals and Physical Chemistry of Surfaces</i>, 53(2): 335–342. March 2017.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S207020511702023X\"\n     onclick=\"log_download('shpanko-sidorenko-semenchev-lyanguzov-anisimova-anticorrosionpropertiesandphysicochemicalcharacteristicsoforganicfilmsbasedonheterocyclicimidazolederivative-2017', 'https://doi.org/10.1134/S207020511702023X', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Anticorrosion properties and physicochemical characteristics of organic films based on heterocyclic imidazole derivative [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S207020511702023X\"\n     onclick=\"log_download('shpanko-sidorenko-semenchev-lyanguzov-anisimova-anticorrosionpropertiesandphysicochemicalcharacteristicsoforganicfilmsbasedonheterocyclicimidazolederivative-2017', 'http://doi.org/10.1134/S207020511702023X', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shpanko-sidorenko-semenchev-lyanguzov-anisimova-anticorrosionpropertiesandphysicochemicalcharacteristicsoforganicfilmsbasedonheterocyclicimidazolederivative-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shpanko-sidorenko-semenchev-lyanguzov-anisimova-anticorrosionpropertiesandphysicochemicalcharacteristicsoforganicfilmsbasedonheterocyclicimidazolederivative-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shpanko_anticorrosion_2017,\n\ttitle = {Anticorrosion properties and physicochemical characteristics of organic films based on heterocyclic imidazole derivative},\n\tvolume = {53},\n\tissn = {2070-206X},\n\turl = {https://doi.org/10.1134/S207020511702023X},\n\tdoi = {10.1134/S207020511702023X},\n\tlanguage = {en},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Protection of Metals and Physical Chemistry of Surfaces},\n\tauthor = {Shpan’ko, S. P. and Sidorenko, E. N. and Semenchev, A. F. and Lyanguzov, N. V. and Anisimova, V. A.},\n\tmonth = mar,\n\tyear = {2017},\n\tpages = {335--342},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"tran-levshov-nguyen-paillet-arenal-than-zahab-yuzyuk-etal-intrinsicphononpropertiesofdoublewalledcarbonnanotubes-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/2043-6254/aa5957\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'tran-levshov-nguyen-paillet-arenal-than-zahab-yuzyuk-etal-intrinsicphononpropertiesofdoublewalledcarbonnanotubes-2017', 'https://dx.doi.org/10.1088/2043-6254/aa5957', event);\">\n    Intrinsic phonon properties of double-walled carbon nanotubes*.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Tran, H. N.; Levshov, D. I.; Nguyen, V. C.; Paillet, M.; Arenal, R.; Than, X. T.; Zahab, A. A.; Yuzyuk, Y. I.; Phan, N. M.; Sauvajol, J.;  and Michel, T.\n</span>\n\n  \n\n</span>\n\n  <i>Advances in Natural Sciences: Nanoscience and Nanotechnology</i>, 8(1): 015018. March 2017.\n  <span class=\"note\">Publisher: IOP Publishing</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/2043-6254/aa5957\"\n     onclick=\"log_download('tran-levshov-nguyen-paillet-arenal-than-zahab-yuzyuk-etal-intrinsicphononpropertiesofdoublewalledcarbonnanotubes-2017', 'https://dx.doi.org/10.1088/2043-6254/aa5957', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Intrinsic phonon properties of double-walled carbon nanotubes* [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/2043-6254/aa5957\"\n     onclick=\"log_download('tran-levshov-nguyen-paillet-arenal-than-zahab-yuzyuk-etal-intrinsicphononpropertiesofdoublewalledcarbonnanotubes-2017', 'http://doi.org/10.1088/2043-6254/aa5957', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/tran-levshov-nguyen-paillet-arenal-than-zahab-yuzyuk-etal-intrinsicphononpropertiesofdoublewalledcarbonnanotubes-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('tran-levshov-nguyen-paillet-arenal-than-zahab-yuzyuk-etal-intrinsicphononpropertiesofdoublewalledcarbonnanotubes-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{tran_intrinsic_2017,\n\ttitle = {Intrinsic phonon properties of double-walled carbon nanotubes*},\n\tvolume = {8},\n\tissn = {2043-6262},\n\turl = {https://dx.doi.org/10.1088/2043-6254/aa5957},\n\tdoi = {10.1088/2043-6254/aa5957},\n\tabstract = {Double-walled carbon nanotubes (DWNT) are made of two concentric and weakly van der Waals coupled single-walled carbon nanotubes (SWNT). DWNTs are the simplest systems for studying the mechanical and electronic interactions between concentric carbon layers. In this paper we review recent results concerning the intrinsic features of phonons of DWNTs obtained from Raman experiments performed on index-identified DWNTs. The effect of the interlayer distance on the strength of the mechanical and electronic coupling between the layers, and thus on the frequencies of the Raman-active modes, namely the radial breathing-like modes (RBLMs) and G-modes, are evidenced and discussed.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Advances in Natural Sciences: Nanoscience and Nanotechnology},\n\tauthor = {Tran, H. N. and Levshov, D. I. and Nguyen, V. C. and Paillet, M. and Arenal, R. and Than, X. T. and Zahab, A. A. and Yuzyuk, Y. I. and Phan, N. M. and Sauvajol, J.-L. and Michel, T.},\n\tmonth = mar,\n\tyear = {2017},\n\tnote = {Publisher: IOP Publishing},\n\tpages = {015018},\n\tfile = {IOP Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\5JJ685FU\\\\Tran и др. - 2017 - Intrinsic phonon properties of double-walled carbo.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Double-walled carbon nanotubes (DWNT) are made of two concentric and weakly van der Waals coupled single-walled carbon nanotubes (SWNT). DWNTs are the simplest systems for studying the mechanical and electronic interactions between concentric carbon layers. In this paper we review recent results concerning the intrinsic features of phonons of DWNTs obtained from Raman experiments performed on index-identified DWNTs. The effect of the interlayer distance on the strength of the mechanical and electronic coupling between the layers, and thus on the frequencies of the Raman-active modes, namely the radial breathing-like modes (RBLMs) and G-modes, are evidenced and discussed.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-razumnaya-yuzyuk-tunablepyroelectricpropertiesofbariumstrontiumtitanatethinfilms-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/1361-648X/aa5711\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-razumnaya-yuzyuk-tunablepyroelectricpropertiesofbariumstrontiumtitanatethinfilms-2017', 'https://dx.doi.org/10.1088/1361-648X/aa5711', event);\">\n    Tunable pyroelectric properties of barium strontium titanate thin films.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.; Razumnaya, A. G.;  and Yuzyuk, Y. I.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics: Condensed Matter</i>, 29(18): 185701. March 2017.\n  <span class=\"note\">Publisher: IOP Publishing</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/1361-648X/aa5711\"\n     onclick=\"log_download('shirokov-razumnaya-yuzyuk-tunablepyroelectricpropertiesofbariumstrontiumtitanatethinfilms-2017', 'https://dx.doi.org/10.1088/1361-648X/aa5711', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Tunable pyroelectric properties of barium strontium titanate thin films [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/1361-648X/aa5711\"\n     onclick=\"log_download('shirokov-razumnaya-yuzyuk-tunablepyroelectricpropertiesofbariumstrontiumtitanatethinfilms-2017', 'http://doi.org/10.1088/1361-648X/aa5711', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-razumnaya-yuzyuk-tunablepyroelectricpropertiesofbariumstrontiumtitanatethinfilms-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-razumnaya-yuzyuk-tunablepyroelectricpropertiesofbariumstrontiumtitanatethinfilms-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_tunable_2017,\n\ttitle = {Tunable pyroelectric properties of barium strontium titanate thin films},\n\tvolume = {29},\n\tissn = {0953-8984},\n\turl = {https://dx.doi.org/10.1088/1361-648X/aa5711},\n\tdoi = {10.1088/1361-648X/aa5711},\n\tabstract = {We studied the influence of the induced strain and applied electric field on the ground state of ferroelectric Ba0.7Sr0.3TiO3 thin films, deposited on the cubic (0 0 1) substrate. The dependence of the pyroelectric coefficient on the applied field is calculated for the different values of the induced strain. We found that tuning of the misfit strain in the film under the dielectric bolometer mode by the proper selection of substrate makes it possible to create the structures with very large values of the pyroelectric coefficient.},\n\tlanguage = {en},\n\tnumber = {18},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics: Condensed Matter},\n\tauthor = {Shirokov, V. B. and Razumnaya, A. G. and Yuzyuk, Yu I.},\n\tmonth = mar,\n\tyear = {2017},\n\tnote = {Publisher: IOP Publishing},\n\tpages = {185701},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We studied the influence of the induced strain and applied electric field on the ground state of ferroelectric Ba0.7Sr0.3TiO3 thin films, deposited on the cubic (0 0 1) substrate. The dependence of the pyroelectric coefficient on the applied field is calculated for the different values of the induced strain. We found that tuning of the misfit strain in the film under the dielectric bolometer mode by the proper selection of substrate makes it possible to create the structures with very large values of the pyroelectric coefficient.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"karapetyan-kaydashev-zhilin-minasyan-abdulvakhidov-kaidashev-useofmultipleacousticreflectionstoenhancesawuvphotodetectorsensitivity-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/1361-665X/26/3/035029\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'karapetyan-kaydashev-zhilin-minasyan-abdulvakhidov-kaidashev-useofmultipleacousticreflectionstoenhancesawuvphotodetectorsensitivity-2017', 'https://dx.doi.org/10.1088/1361-665X/26/3/035029', event);\">\n    Use of multiple acoustic reflections to enhance SAW UV photo-detector sensitivity.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Karapetyan, G. Y.; Kaydashev, V. E.; Zhilin, D. A.; Minasyan, T. A.; Abdulvakhidov, K. G.;  and Kaidashev, E. M.\n</span>\n\n  \n\n</span>\n\n  <i>Smart Materials and Structures</i>, 26(3): 035029. February 2017.\n  <span class=\"note\">Publisher: IOP Publishing</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/1361-665X/26/3/035029\"\n     onclick=\"log_download('karapetyan-kaydashev-zhilin-minasyan-abdulvakhidov-kaidashev-useofmultipleacousticreflectionstoenhancesawuvphotodetectorsensitivity-2017', 'https://dx.doi.org/10.1088/1361-665X/26/3/035029', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Use of multiple acoustic reflections to enhance SAW UV photo-detector sensitivity [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/1361-665X/26/3/035029\"\n     onclick=\"log_download('karapetyan-kaydashev-zhilin-minasyan-abdulvakhidov-kaidashev-useofmultipleacousticreflectionstoenhancesawuvphotodetectorsensitivity-2017', 'http://doi.org/10.1088/1361-665X/26/3/035029', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/karapetyan-kaydashev-zhilin-minasyan-abdulvakhidov-kaidashev-useofmultipleacousticreflectionstoenhancesawuvphotodetectorsensitivity-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('karapetyan-kaydashev-zhilin-minasyan-abdulvakhidov-kaidashev-useofmultipleacousticreflectionstoenhancesawuvphotodetectorsensitivity-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{karapetyan_use_2017,\n\ttitle = {Use of multiple acoustic reflections to enhance {SAW} {UV} photo-detector sensitivity},\n\tvolume = {26},\n\tissn = {0964-1726},\n\turl = {https://dx.doi.org/10.1088/1361-665X/26/3/035029},\n\tdoi = {10.1088/1361-665X/26/3/035029},\n\tabstract = {A new approach to enhance the sensitivity of existing SAW UV-visible photo-detectors based on the monitoring of the multiple reflections of the acoustic waves in the Fourier transform of the frequency response (S21) is demonstrated. By using this concept, it is possible to monitor the UV-visible light in a wide intensity range from very high to ultralow. We present a strategy to obtain an ultrafast SAW UV photo-detector with millisecond response by tuning the deposition conditions of the ZnO film and using the multiple-reflections concept.},\n\tlanguage = {en},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Smart Materials and Structures},\n\tauthor = {Karapetyan, G. Y. and Kaydashev, V. E. and Zhilin, D. A. and Minasyan, T. A. and Abdulvakhidov, K. G. and Kaidashev, E. M.},\n\tmonth = feb,\n\tyear = {2017},\n\tnote = {Publisher: IOP Publishing},\n\tpages = {035029},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A new approach to enhance the sensitivity of existing SAW UV-visible photo-detectors based on the monitoring of the multiple reflections of the acoustic waves in the Fourier transform of the frequency response (S21) is demonstrated. By using this concept, it is possible to monitor the UV-visible light in a wide intensity range from very high to ultralow. We present a strategy to obtain an ultrafast SAW UV photo-detector with millisecond response by tuning the deposition conditions of the ZnO film and using the multiple-reflections concept.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"leontyev-kulbakov-allix-rakhmatullin-kuriganova-maslova-smirnova-thermalexpansioncoefficientofcarbonsupportedptnanoparticlesinsituxraydiffractionstudy-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201600695\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'leontyev-kulbakov-allix-rakhmatullin-kuriganova-maslova-smirnova-thermalexpansioncoefficientofcarbonsupportedptnanoparticlesinsituxraydiffractionstudy-2017', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201600695', event);\">\n    Thermal expansion coefficient of carbon-supported Pt nanoparticles: In-situ X-ray diffraction study.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Leontyev, I. N.; Kulbakov, A. A.; Allix, M.; Rakhmatullin, A.; Kuriganova, A. B.; Maslova, O. A.;  and Smirnova, N. V.\n</span>\n\n  \n\n</span>\n\n  <i>physica status solidi (b)</i>, 254(5): 1600695.  2017.\n  <span class=\"note\">_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201600695</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201600695\"\n     onclick=\"log_download('leontyev-kulbakov-allix-rakhmatullin-kuriganova-maslova-smirnova-thermalexpansioncoefficientofcarbonsupportedptnanoparticlesinsituxraydiffractionstudy-2017', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201600695', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Thermal expansion coefficient of carbon-supported Pt nanoparticles: In-situ X-ray diffraction study [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1002/pssb.201600695\"\n     onclick=\"log_download('leontyev-kulbakov-allix-rakhmatullin-kuriganova-maslova-smirnova-thermalexpansioncoefficientofcarbonsupportedptnanoparticlesinsituxraydiffractionstudy-2017', 'http://doi.org/10.1002/pssb.201600695', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/leontyev-kulbakov-allix-rakhmatullin-kuriganova-maslova-smirnova-thermalexpansioncoefficientofcarbonsupportedptnanoparticlesinsituxraydiffractionstudy-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('leontyev-kulbakov-allix-rakhmatullin-kuriganova-maslova-smirnova-thermalexpansioncoefficientofcarbonsupportedptnanoparticlesinsituxraydiffractionstudy-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{leontyev_thermal_2017,\n\ttitle = {Thermal expansion coefficient of carbon-supported {Pt} nanoparticles: {In}-situ {X}-ray diffraction study},\n\tvolume = {254},\n\tcopyright = {© 2017 WILEY-VCH Verlag GmbH \\&amp; Co. KGaA, Weinheim},\n\tissn = {1521-3951},\n\tshorttitle = {Thermal expansion coefficient of carbon-supported {Pt} nanoparticles},\n\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201600695},\n\tdoi = {10.1002/pssb.201600695},\n\tabstract = {The thermal expansion of carbon-supported Pt nanoparticles with different particle size has been studied in-situ via X-ray diffraction at temperatures from 100 to 300 K. The thermal expansion coefficient (TEC) of investigated Pt/C nanoparticles is always superior to that of bulk Pt. When the grain size D decreases from 11 to 3 nm, the TEC nonlinearly increases by about 1.66 × 10−6 K−1 which corresponds to a variation of ∼20\\% from bulk Pt. The obtained experimental dependence of TEC for Pt/C nanoparticles has been interpreted using different theoretical approaches. A comparison of the considered models with the experimental data reveals the best agreement from the binding order–length–strength model with the size dependence of TEC experimentally found in carbon-supported Pt nanoparticles.},\n\tlanguage = {en},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {physica status solidi (b)},\n\tauthor = {Leontyev, I. N. and Kulbakov, A. A. and Allix, M. and Rakhmatullin, A. and Kuriganova, A. B. and Maslova, O. A. and Smirnova, N. V.},\n\tyear = {2017},\n\tnote = {\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201600695},\n\tkeywords = {X-ray diffraction, platinum, nanoparticles, surface relaxation, thermal expansion},\n\tpages = {1600695},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The thermal expansion of carbon-supported Pt nanoparticles with different particle size has been studied in-situ via X-ray diffraction at temperatures from 100 to 300 K. The thermal expansion coefficient (TEC) of investigated Pt/C nanoparticles is always superior to that of bulk Pt. When the grain size D decreases from 11 to 3 nm, the TEC nonlinearly increases by about 1.66 × 10−6 K−1 which corresponds to a variation of ∼20% from bulk Pt. The obtained experimental dependence of TEC for Pt/C nanoparticles has been interpreted using different theoretical approaches. A comparison of the considered models with the experimental data reveals the best agreement from the binding order–length–strength model with the size dependence of TEC experimentally found in carbon-supported Pt nanoparticles.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"razumnaya-mikheykin-lukyanchuk-shirokov-golovko-mukhortov-marssi-yuzyuk-unexpectedlyhighcurietemperatureinweaklystrainedferroelectricfilm-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201600413\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'razumnaya-mikheykin-lukyanchuk-shirokov-golovko-mukhortov-marssi-yuzyuk-unexpectedlyhighcurietemperatureinweaklystrainedferroelectricfilm-2017', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201600413', event);\">\n    Unexpectedly high Curie temperature in weakly strained ferroelectric film.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Razumnaya, A. G.; Mikheykin, A. S.; Lukyanchuk, I. A.; Shirokov, V. B.; Golovko, Y. I.; Mukhortov, V. M.; Marssi, M. E.;  and Yuzyuk, Y. I.\n</span>\n\n  \n\n</span>\n\n  <i>physica status solidi (b)</i>, 254(4): 1600413.  2017.\n  <span class=\"note\">_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201600413</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201600413\"\n     onclick=\"log_download('razumnaya-mikheykin-lukyanchuk-shirokov-golovko-mukhortov-marssi-yuzyuk-unexpectedlyhighcurietemperatureinweaklystrainedferroelectricfilm-2017', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201600413', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Unexpectedly high Curie temperature in weakly strained ferroelectric film [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1002/pssb.201600413\"\n     onclick=\"log_download('razumnaya-mikheykin-lukyanchuk-shirokov-golovko-mukhortov-marssi-yuzyuk-unexpectedlyhighcurietemperatureinweaklystrainedferroelectricfilm-2017', 'http://doi.org/10.1002/pssb.201600413', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/razumnaya-mikheykin-lukyanchuk-shirokov-golovko-mukhortov-marssi-yuzyuk-unexpectedlyhighcurietemperatureinweaklystrainedferroelectricfilm-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('razumnaya-mikheykin-lukyanchuk-shirokov-golovko-mukhortov-marssi-yuzyuk-unexpectedlyhighcurietemperatureinweaklystrainedferroelectricfilm-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{razumnaya_unexpectedly_2017,\n\ttitle = {Unexpectedly high {Curie} temperature in weakly strained ferroelectric film},\n\tvolume = {254},\n\tcopyright = {© 2016 WILEY-VCH Verlag GmbH \\&amp; Co. KGaA, Weinheim},\n\tissn = {1521-3951},\n\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201600413},\n\tdoi = {10.1002/pssb.201600413},\n\tabstract = {Polarized Raman spectra of the epitaxial Ba0.4Sr0.6TiO3 film grown on MgO substrate with thickness of 600 nm were studied in a broad temperature range of 80–600 K and the phase transition from paraelectric to tetragonal ferroelectric phase was observed at about 500 K. This critical temperature is substantially higher than that calculated from the lattice-mismatch strain theory. In addition, the predicted from the theory low-temperature orthorhombic and rhombohedral phases were not observed. We ascribe the strengthening of the tetragonal ferroelectric phase to the effect of the interface-induced build-in electric field resulted from the interface-accumulated charges.},\n\tlanguage = {en},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {physica status solidi (b)},\n\tauthor = {Razumnaya, Anna G. and Mikheykin, Alexey S. and Lukyanchuk, Igor A. and Shirokov, Vladimir B. and Golovko, Yury I. and Mukhortov, Vladimir M. and Marssi, Mimoun El and Yuzyuk, Yury I.},\n\tyear = {2017},\n\tnote = {\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201600413},\n\tkeywords = {thin films, Raman spectroscopy, strain, BaTiO3, soft mode, Curie temperature, ferroelectric transition},\n\tpages = {1600413},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Polarized Raman spectra of the epitaxial Ba0.4Sr0.6TiO3 film grown on MgO substrate with thickness of 600 nm were studied in a broad temperature range of 80–600 K and the phase transition from paraelectric to tetragonal ferroelectric phase was observed at about 500 K. This critical temperature is substantially higher than that calculated from the lattice-mismatch strain theory. In addition, the predicted from the theory low-temperature orthorhombic and rhombohedral phases were not observed. We ascribe the strengthening of the tetragonal ferroelectric phase to the effect of the interface-induced build-in electric field resulted from the interface-accumulated charges.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"levshov-tran-michel-cao-nguyen-arenal-popov-sauvajol-etal-interlayerinteractioneffectsonthegmodesindoublewalledcarbonnanotubeswithdifferentelectronicconfigurations-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201700251\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'levshov-tran-michel-cao-nguyen-arenal-popov-sauvajol-etal-interlayerinteractioneffectsonthegmodesindoublewalledcarbonnanotubeswithdifferentelectronicconfigurations-2017', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201700251', event);\">\n    Interlayer Interaction Effects on the G Modes in Double-Walled Carbon Nanotubes With Different Electronic Configurations.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Levshov, D. I.; Tran, H.; Michel, T.; Cao, T. T.; Nguyen, V. C.; Arenal, R.; Popov, V. N.; Sauvajol, J.; Zahab, A.;  and Paillet, M.\n</span>\n\n  \n\n</span>\n\n  <i>physica status solidi (b)</i>, 254(11): 1700251.  2017.\n  <span class=\"note\">_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201700251</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201700251\"\n     onclick=\"log_download('levshov-tran-michel-cao-nguyen-arenal-popov-sauvajol-etal-interlayerinteractioneffectsonthegmodesindoublewalledcarbonnanotubeswithdifferentelectronicconfigurations-2017', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201700251', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Interlayer Interaction Effects on the G Modes in Double-Walled Carbon Nanotubes With Different Electronic Configurations [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1002/pssb.201700251\"\n     onclick=\"log_download('levshov-tran-michel-cao-nguyen-arenal-popov-sauvajol-etal-interlayerinteractioneffectsonthegmodesindoublewalledcarbonnanotubeswithdifferentelectronicconfigurations-2017', 'http://doi.org/10.1002/pssb.201700251', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/levshov-tran-michel-cao-nguyen-arenal-popov-sauvajol-etal-interlayerinteractioneffectsonthegmodesindoublewalledcarbonnanotubeswithdifferentelectronicconfigurations-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('levshov-tran-michel-cao-nguyen-arenal-popov-sauvajol-etal-interlayerinteractioneffectsonthegmodesindoublewalledcarbonnanotubeswithdifferentelectronicconfigurations-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{levshov_interlayer_2017,\n\ttitle = {Interlayer {Interaction} {Effects} on the {G} {Modes} in {Double}-{Walled} {Carbon} {Nanotubes} {With} {Different} {Electronic} {Configurations}},\n\tvolume = {254},\n\tcopyright = {© 2017 WILEY-VCH Verlag GmbH \\&amp; Co. KGaA, Weinheim},\n\tissn = {1521-3951},\n\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.201700251},\n\tdoi = {10.1002/pssb.201700251},\n\tabstract = {We present experimental measurements of the features of G band in individual index-identified free-standing double-walled carbon nanotubes. We examine Raman spectra of different electronic configurations of DWNTs, namely: SC@SC, SC@M, M@SC, M@M, and clearly establish that, as in SWNTs, the profile of LO G-mode of each layer is broad (narrow) when the layer is metallic (semiconducting). The dependence of G-modes on the diameter and inter-layer distance in several SC@SC, SC@M, M@SC, M@M index-identified DWNTs is reported. We find, that, independently of the metallic or semiconducting nature of the layers, the frequencies of LO and TO G-mode of the inner and outer layers shift significantly with respect to the frequencies of the same modes in the constituent SWNTs.},\n\tlanguage = {en},\n\tnumber = {11},\n\turldate = {2023-11-11},\n\tjournal = {physica status solidi (b)},\n\tauthor = {Levshov, Dmitry I. and Tran, Huy-Nam and Michel, Thierry and Cao, Thi Thanh and Nguyen, Van Chuc and Arenal, Raul and Popov, Valentin N. and Sauvajol, Jean-Louis and Zahab, Ahmed-Azmi and Paillet, Matthieu},\n\tyear = {2017},\n\tnote = {\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.201700251},\n\tkeywords = {Raman spectroscopy, double-walled carbon nanotubes, interlayer interaction},\n\tpages = {1700251},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We present experimental measurements of the features of G band in individual index-identified free-standing double-walled carbon nanotubes. We examine Raman spectra of different electronic configurations of DWNTs, namely: SC@SC, SC@M, M@SC, M@M, and clearly establish that, as in SWNTs, the profile of LO G-mode of each layer is broad (narrow) when the layer is metallic (semiconducting). The dependence of G-modes on the diameter and inter-layer distance in several SC@SC, SC@M, M@SC, M@M index-identified DWNTs is reported. We find, that, independently of the metallic or semiconducting nature of the layers, the frequencies of LO and TO G-mode of the inner and outer layers shift significantly with respect to the frequencies of the same modes in the constituent SWNTs.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kuriganova-leontyev-avramenko-popov-maslova-koval-smirnova-onestepsimultaneoussynthesisofgrapheneandptnanoparticlesundertheactionofpulsedalternatingcurrentandelectrochemicalperformanceofptgraphenecatalysts-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201701186\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kuriganova-leontyev-avramenko-popov-maslova-koval-smirnova-onestepsimultaneoussynthesisofgrapheneandptnanoparticlesundertheactionofpulsedalternatingcurrentandelectrochemicalperformanceofptgraphenecatalysts-2017', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201701186', event);\">\n    One-step Simultaneous Synthesis of Graphene and Pt Nanoparticles under the Action of Pulsed Alternating Current and Electrochemical Performance of Pt/Graphene Catalysts.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kuriganova, A. B.; Leontyev, I. N.; Avramenko, M. V.; Popov, Y.; Maslova, O. A.; Koval, O. Y.;  and Smirnova, N. V.\n</span>\n\n  \n\n</span>\n\n  <i>ChemistrySelect</i>, 2(24): 6979–6983.  2017.\n  <span class=\"note\">_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/slct.201701186</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201701186\"\n     onclick=\"log_download('kuriganova-leontyev-avramenko-popov-maslova-koval-smirnova-onestepsimultaneoussynthesisofgrapheneandptnanoparticlesundertheactionofpulsedalternatingcurrentandelectrochemicalperformanceofptgraphenecatalysts-2017', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201701186', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"One-step Simultaneous Synthesis of Graphene and Pt Nanoparticles under the Action of Pulsed Alternating Current and Electrochemical Performance of Pt/Graphene Catalysts [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1002/slct.201701186\"\n     onclick=\"log_download('kuriganova-leontyev-avramenko-popov-maslova-koval-smirnova-onestepsimultaneoussynthesisofgrapheneandptnanoparticlesundertheactionofpulsedalternatingcurrentandelectrochemicalperformanceofptgraphenecatalysts-2017', 'http://doi.org/10.1002/slct.201701186', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kuriganova-leontyev-avramenko-popov-maslova-koval-smirnova-onestepsimultaneoussynthesisofgrapheneandptnanoparticlesundertheactionofpulsedalternatingcurrentandelectrochemicalperformanceofptgraphenecatalysts-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kuriganova-leontyev-avramenko-popov-maslova-koval-smirnova-onestepsimultaneoussynthesisofgrapheneandptnanoparticlesundertheactionofpulsedalternatingcurrentandelectrochemicalperformanceofptgraphenecatalysts-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kuriganova_one-step_2017,\n\ttitle = {One-step {Simultaneous} {Synthesis} of {Graphene} and {Pt} {Nanoparticles} under the {Action} of {Pulsed} {Alternating} {Current} and {Electrochemical} {Performance} of {Pt}/{Graphene} {Catalysts}},\n\tvolume = {2},\n\tcopyright = {© 2017 Wiley-VCH Verlag GmbH \\&amp; Co. KGaA, Weinheim},\n\tissn = {2365-6549},\n\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/slct.201701186},\n\tdoi = {10.1002/slct.201701186},\n\tabstract = {Pt/graphene electrocatalyst for fuel elements has been obtained via the simultaneously electrochemical dispersion of Pt foil and expanded graphite by applying the alternating current. Raman spectroscopy and transmission electron microscopy (TEM) have revealed multilayered structure of graphene (3-5 layers) with linear defects of graphene sheets near 1 μm. The microstructural characteristics and catalytic activity of synthesized Pt/graphene catalyst have been compared with those of Pt/Vulcan catalyst prepared under the same conditions. Pt nanoparticles of Pt/Graphene catalyst exhibit smaller average dimensions and narrower particle size distribution. It follows from the electrochemical study that the electrochemical surface area of Pt/graphene catalyst is 2.5 times higher than for Pt/Vulcan. Besides this, the activity in the electrooxidation of methanol and the stability of Pt/graphene catalyst are found to be superior to the analogous parameters of Pt/Vulcan specimen.},\n\tlanguage = {en},\n\tnumber = {24},\n\turldate = {2023-11-11},\n\tjournal = {ChemistrySelect},\n\tauthor = {Kuriganova, Alexandra B. and Leontyev, Igor N. and Avramenko, Marina V. and Popov, Yuri and Maslova, Olga A. and Koval, Olga Yu. and Smirnova, Nina V.},\n\tyear = {2017},\n\tnote = {\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/slct.201701186},\n\tkeywords = {electrochemical dispersion, fuel cell, platinum, Graphene, Pt/graphene catalysts},\n\tpages = {6979--6983},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Pt/graphene electrocatalyst for fuel elements has been obtained via the simultaneously electrochemical dispersion of Pt foil and expanded graphite by applying the alternating current. Raman spectroscopy and transmission electron microscopy (TEM) have revealed multilayered structure of graphene (3-5 layers) with linear defects of graphene sheets near 1 μm. The microstructural characteristics and catalytic activity of synthesized Pt/graphene catalyst have been compared with those of Pt/Vulcan catalyst prepared under the same conditions. Pt nanoparticles of Pt/Graphene catalyst exhibit smaller average dimensions and narrower particle size distribution. It follows from the electrochemical study that the electrochemical surface area of Pt/graphene catalyst is 2.5 times higher than for Pt/Vulcan. Besides this, the activity in the electrooxidation of methanol and the stability of Pt/graphene catalyst are found to be superior to the analogous parameters of Pt/Vulcan specimen.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---------2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/44998\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---------2017', 'http://journals.ioffe.ru/articles/44998', event);\">\n    Формирование магнитных никелевых наночастиц и изменения матрицы фталоцианина никеля при допировании натрием.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Колпачева, Н.; Авраменко, М.; Авакян, Л.; Зубавичус, Я.; Мирзаханян, А.; Манукян, А.; Шароян, Э.;  and Бугаев, Л.\n</span>\n\n  \n\n</span>\n\n  <i>Журнал технической физики</i>, 87(10): 1532.  2017.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/44998\"\n     onclick=\"log_download('---------2017', 'http://journals.ioffe.ru/articles/44998', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Формирование магнитных никелевых наночастиц и изменения матрицы фталоцианина никеля при допировании натрием [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.21883/JTF.2017.10.44998.2149\"\n     onclick=\"log_download('---------2017', 'http://doi.org/10.21883/JTF.2017.10.44998.2149', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---------2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---------2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2017,\n\ttitle = {Формирование магнитных никелевых наночастиц и изменения матрицы фталоцианина никеля при допировании натрием},\n\tvolume = {87},\n\tissn = {0044-4642},\n\turl = {http://journals.ioffe.ru/articles/44998},\n\tdoi = {10.21883/JTF.2017.10.44998.2149},\n\tlanguage = {ru},\n\tnumber = {10},\n\turldate = {2023-11-11},\n\tjournal = {Журнал технической физики},\n\tauthor = {Колпачева, Н.А. and Авраменко, М.В. and Авакян, Л.А. and Зубавичус, Я.В. and Мирзаханян, А.А. and Манукян, А.С. and Шароян, Э.Г. and Бугаев, Л.А.},\n\tyear = {2017},\n\tpages = {1532},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\EXHSE7C9\\\\Колпачева и др. - 2017 - Формирование магнитных никелевых наночастиц и изме.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-tran-----g-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/44057\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-tran-----g-2017', 'https://journals.ioffe.ru/articles/44057', event);\">\n    Экспериментальное исследование динамики решетки индивидуальных полупроводниковых двустенных углеродных нанотрубок: тангенциальные G-моды.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Левшов, Д.; Tran, H.; Слабодян, Ю.; Осадчий, А.; Рошаль, С.;  and Юзюк, Ю.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 59(2): 328.  2017.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/44057\"\n     onclick=\"log_download('-tran-----g-2017', 'https://journals.ioffe.ru/articles/44057', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Экспериментальное исследование динамики решетки индивидуальных полупроводниковых двустенных углеродных нанотрубок: тангенциальные G-моды [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.21883/FTT.2017.02.44057.274\"\n     onclick=\"log_download('-tran-----g-2017', 'http://doi.org/10.21883/FTT.2017.02.44057.274', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-tran-----g-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-tran-----g-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2017-1,\n\ttitle = {Экспериментальное исследование динамики решетки индивидуальных полупроводниковых двустенных углеродных нанотрубок: тангенциальные {G}-моды},\n\tvolume = {59},\n\tissn = {0367-3294},\n\tshorttitle = {Экспериментальное исследование динамики решетки индивидуальных полупроводниковых двустенных углеродных нанотрубок},\n\turl = {https://journals.ioffe.ru/articles/44057},\n\tdoi = {10.21883/FTT.2017.02.44057.274},\n\tabstract = {Проведены исследования тангенциальных G-мод индивидуальных полупроводниковых двустенных углеродных нанотрубок методом резонансной спектроскопии комбинационного рассеяния света в широком диапазоне длин волн лазерного возбуждения. Индивидуальные подвешенные нанотрубки синтезированы методом химического осаждения из парогазовой фазы. Индексы хиральности (n,m) нанотрубок определялись методами электронной дифракции и просвечивающей электронной микроскопии высокого разрешения. В спектрах комбинационного рассеяния двустенных нанотрубок наблюдается существенный сдвиг тангенциальных мод в сравнении с аналогичными модами одностенных нанотрубок. Показано, что величина сдвига зависит от межслойного расстояния и от величины ван-дер-ваальсова взаимодействия между слоями двустенной нанотрубки. Исследование выполнено за счет гранта Российского фонда фундаментальных исследований (проект N 15-02-08340). DOI: 10.21883/FTT.2017.02.44057.274},\n\tlanguage = {ru},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Левшов, Д.И. and Tran, H.N. and Слабодян, Ю.С. and Осадчий, А.В. and Рошаль, С.Б. and Юзюк, Ю.И.},\n\tyear = {2017},\n\tpages = {328},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\CPU38V3F\\\\Левшов и др. - 2017 - Экспериментальное исследование динамики решетки ин.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Проведены исследования тангенциальных G-мод индивидуальных полупроводниковых двустенных углеродных нанотрубок методом резонансной спектроскопии комбинационного рассеяния света в широком диапазоне длин волн лазерного возбуждения. Индивидуальные подвешенные нанотрубки синтезированы методом химического осаждения из парогазовой фазы. Индексы хиральности (n,m) нанотрубок определялись методами электронной дифракции и просвечивающей электронной микроскопии высокого разрешения. В спектрах комбинационного рассеяния двустенных нанотрубок наблюдается существенный сдвиг тангенциальных мод в сравнении с аналогичными модами одностенных нанотрубок. Показано, что величина сдвига зависит от межслойного расстояния и от величины ван-дер-ваальсова взаимодействия между слоями двустенной нанотрубки. Исследование выполнено за счет гранта Российского фонда фундаментальных исследований (проект N 15-02-08340). DOI: 10.21883/FTT.2017.02.44057.274\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"ulyankina-leontyev-smirnova-electrochemicalsynthesisandphotocatalyticactivityofdifferentlyshapedcuoxparticles-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.scientific.net/NHC.13.330\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'ulyankina-leontyev-smirnova-electrochemicalsynthesisandphotocatalyticactivityofdifferentlyshapedcuoxparticles-2017', 'https://www.scientific.net/NHC.13.330', event);\">\n    Electrochemical Synthesis and Photocatalytic Activity of Differently Shaped CuOx Particles.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Ulyankina, A.; Leontyev, I.;  and Smirnova, N. V.\n</span>\n\n  \n\n</span>\n\n  <i>Nano Hybrids and Composites</i>, 13: 330–333.  2017.\n  <span class=\"note\">Publisher: Trans Tech Publications Ltd</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.scientific.net/NHC.13.330\"\n     onclick=\"log_download('ulyankina-leontyev-smirnova-electrochemicalsynthesisandphotocatalyticactivityofdifferentlyshapedcuoxparticles-2017', 'https://www.scientific.net/NHC.13.330', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Electrochemical Synthesis and Photocatalytic Activity of Differently Shaped CuOx Particles [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.4028/www.scientific.net/NHC.13.330\"\n     onclick=\"log_download('ulyankina-leontyev-smirnova-electrochemicalsynthesisandphotocatalyticactivityofdifferentlyshapedcuoxparticles-2017', 'http://doi.org/10.4028/www.scientific.net/NHC.13.330', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/ulyankina-leontyev-smirnova-electrochemicalsynthesisandphotocatalyticactivityofdifferentlyshapedcuoxparticles-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('ulyankina-leontyev-smirnova-electrochemicalsynthesisandphotocatalyticactivityofdifferentlyshapedcuoxparticles-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{ulyankina_electrochemical_2017,\n\ttitle = {Electrochemical {Synthesis} and {Photocatalytic} {Activity} of {Differently} {Shaped} {CuOx} {Particles}},\n\tvolume = {13},\n\tissn = {2297-3400},\n\turl = {https://www.scientific.net/NHC.13.330},\n\tdoi = {10.4028/www.scientific.net/NHC.13.330},\n\tabstract = {CuOx powders with diff erently shaped particles were firstly prepared via an electrochemical method by oxidation and dispersion of copper electrodes in an electrolyte solution under pulse alternating current (PAC). By means of X-ray diffraction (XRD) and scanning electron microscopy (SEM) the current density is found to have an influence on the morphology and composition of CuOx particles. Photocatalytic efficiency of CuOx towards methyl orange (MO) degradation under visible light was investigated. The prepared polyhedral particles show the best photocatalytic activity of 81 \\% towards MO comparing to octahedral and spherical particles with 70 and 61 \\%, respectively.},\n\tlanguage = {en},\n\turldate = {2023-11-11},\n\tjournal = {Nano Hybrids and Composites},\n\tauthor = {Ulyankina, Anna and Leontyev, Igor and Smirnova, Nina V.},\n\tyear = {2017},\n\tnote = {Publisher: Trans Tech Publications Ltd},\n\tpages = {330--333},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  CuOx powders with diff erently shaped particles were firstly prepared via an electrochemical method by oxidation and dispersion of copper electrodes in an electrolyte solution under pulse alternating current (PAC). By means of X-ray diffraction (XRD) and scanning electron microscopy (SEM) the current density is found to have an influence on the morphology and composition of CuOx particles. Photocatalytic efficiency of CuOx towards methyl orange (MO) degradation under visible light was investigated. The prepared polyhedral particles show the best photocatalytic activity of 81 % towards MO comparing to octahedral and spherical particles with 70 and 61 %, respectively.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---michel----2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/44173\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---michel----2017', 'https://journals.ioffe.ru/articles/44173', event);\">\n    Особенности тангенциальных мод в спектрах комбинационного рассеяния света одностенных полупроводниковых углеродных нанотрубок большого диаметра.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Левшов, Д.; Слабодян, Ю.; Тонких, А.; Michel, T.; Рошаль, С.;  and Юзюк, Ю.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 59(3): 575.  2017.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/44173\"\n     onclick=\"log_download('---michel----2017', 'https://journals.ioffe.ru/articles/44173', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Особенности тангенциальных мод в спектрах комбинационного рассеяния света одностенных полупроводниковых углеродных нанотрубок большого диаметра [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.21883/FTT.2017.03.44173.137\"\n     onclick=\"log_download('---michel----2017', 'http://doi.org/10.21883/FTT.2017.03.44173.137', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---michel----2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---michel----2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2017-2,\n\ttitle = {Особенности тангенциальных мод в спектрах комбинационного рассеяния света одностенных полупроводниковых углеродных нанотрубок большого диаметра},\n\tvolume = {59},\n\tissn = {0367-3294},\n\turl = {https://journals.ioffe.ru/articles/44173},\n\tdoi = {10.21883/FTT.2017.03.44173.137},\n\tabstract = {Методом резонансной спектроскопии комбинационного рассеяния света в широком диапазоне длин волн лазерного возбуждения исследована динамика решетки и оптические свойства индивидуальных полупроводниковых одностенных углеродных нанотрубок с диаметрами более 2.0 nm. Индивидуальные подвешенные нанотрубки синтезированы методом химического осаждения из парогазовой фазы. Индексы хиральности (n,m) нанотрубок определялись методом электронной дифракции. Обнаружена зависимость отношения абсолютных интенсивностей поперечной и продольной оптических тангенциальных мод как от энергии возбуждения, так и от структурных параметров нанотрубок (диаметра и хирального угла). Наблюдаемые зависимости отличаются от спектральных данных, полученных ранее для индивидуальных полупроводниковых структурно идентифицированных нанотрубок с диаметрами менее 1.1 nm. Работа выполнена за счет гранта Российского научного фонда (проект N 15-12-10004). DOI: 10.21883/FTT.2017.03.44173.137},\n\tlanguage = {ru},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Левшов, Д.И. and Слабодян, Ю.С. and Тонких, А.А. and Michel, T. and Рошаль, С.Б. and Юзюк, Ю.И.},\n\tyear = {2017},\n\tpages = {575},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\RFCMW9MW\\\\Левшов и др. - 2017 - Особенности тангенциальных мод в спектрах комбинац.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Методом резонансной спектроскопии комбинационного рассеяния света в широком диапазоне длин волн лазерного возбуждения исследована динамика решетки и оптические свойства индивидуальных полупроводниковых одностенных углеродных нанотрубок с диаметрами более 2.0 nm. Индивидуальные подвешенные нанотрубки синтезированы методом химического осаждения из парогазовой фазы. Индексы хиральности (n,m) нанотрубок определялись методом электронной дифракции. Обнаружена зависимость отношения абсолютных интенсивностей поперечной и продольной оптических тангенциальных мод как от энергии возбуждения, так и от структурных параметров нанотрубок (диаметра и хирального угла). Наблюдаемые зависимости отличаются от спектральных данных, полученных ранее для индивидуальных полупроводниковых структурно идентифицированных нанотрубок с диаметрами менее 1.1 nm. Работа выполнена за счет гранта Российского научного фонда (проект N 15-12-10004). DOI: 10.21883/FTT.2017.03.44173.137\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"levshov-tran-paillet-arenal-than-zahab-yuzyuk-sauvajol-etal-accuratedeterminationofthechiralindicesofindividualcarbonnanotubesbycombiningelectrondiffractionandresonantramanspectroscopy-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0008622316310570\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'levshov-tran-paillet-arenal-than-zahab-yuzyuk-sauvajol-etal-accuratedeterminationofthechiralindicesofindividualcarbonnanotubesbycombiningelectrondiffractionandresonantramanspectroscopy-2017', 'https://www.sciencedirect.com/science/article/pii/S0008622316310570', event);\">\n    Accurate determination of the chiral indices of individual carbon nanotubes by combining electron diffraction and Resonant Raman spectroscopy.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Levshov, D. I.; Tran, H. N.; Paillet, M.; Arenal, R.; Than, X. T.; Zahab, A. A.; Yuzyuk, Y. I.; Sauvajol, J. -.;  and Michel, T.\n</span>\n\n  \n\n</span>\n\n  <i>Carbon</i>, 114: 141–159. April 2017.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0008622316310570\"\n     onclick=\"log_download('levshov-tran-paillet-arenal-than-zahab-yuzyuk-sauvajol-etal-accuratedeterminationofthechiralindicesofindividualcarbonnanotubesbycombiningelectrondiffractionandresonantramanspectroscopy-2017', 'https://www.sciencedirect.com/science/article/pii/S0008622316310570', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Accurate determination of the chiral indices of individual carbon nanotubes by combining electron diffraction and Resonant Raman spectroscopy [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.carbon.2016.11.076\"\n     onclick=\"log_download('levshov-tran-paillet-arenal-than-zahab-yuzyuk-sauvajol-etal-accuratedeterminationofthechiralindicesofindividualcarbonnanotubesbycombiningelectrondiffractionandresonantramanspectroscopy-2017', 'http://doi.org/10.1016/j.carbon.2016.11.076', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/levshov-tran-paillet-arenal-than-zahab-yuzyuk-sauvajol-etal-accuratedeterminationofthechiralindicesofindividualcarbonnanotubesbycombiningelectrondiffractionandresonantramanspectroscopy-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('levshov-tran-paillet-arenal-than-zahab-yuzyuk-sauvajol-etal-accuratedeterminationofthechiralindicesofindividualcarbonnanotubesbycombiningelectrondiffractionandresonantramanspectroscopy-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{levshov_accurate_2017,\n\ttitle = {Accurate determination of the chiral indices of individual carbon nanotubes by combining electron diffraction and {Resonant} {Raman} spectroscopy},\n\tvolume = {114},\n\tissn = {0008-6223},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0008622316310570},\n\tdoi = {10.1016/j.carbon.2016.11.076},\n\tabstract = {The experimental approach combining high resolution transmission electron microscopy (HRTEM), electron diffraction (ED) and resonant Raman spectroscopy (RRS) on the same free-standing individual carbon nanotubes (CNT) is the most efficient method to determine unambiguously the intrinsic features of the Raman-active phonons. In this paper, we review the main results obtained by the approach regarding the intrinsic features of the phonons of single-walled (SWNT) and double-walled carbon nanotubes (DWNT). First, we detail the different methods to identify the structure of SWNTs and DWNTs from the analysis of their electron diffraction patterns (EDP). In the following, we remind the principal features of the Raman response of SWNTs, unambiguously index-identified by ED. A special attention is devoted to the effect of the inter-layer interaction on the frequencies of the Raman-active phonons in index-identified DWNTs. The information obtained on index-identified SWNT and DWNT allows us to propose Raman criteria, which help identifying CNT when the ED fails to propose a single assignment. The efficiency of the Raman criteria as the complement to the ED information for the index-assignment of a few SWNTs and DWNTs is shown. The same approach to index-assign a triple-walled carbon nanotube (TWNT), by combining ED and RRS information, is reported.},\n\turldate = {2023-11-11},\n\tjournal = {Carbon},\n\tauthor = {Levshov, D. I. and Tran, H. N. and Paillet, M. and Arenal, R. and Than, X. T. and Zahab, A. A. and Yuzyuk, Y. I. and Sauvajol, J. -L. and Michel, T.},\n\tmonth = apr,\n\tyear = {2017},\n\tpages = {141--159},\n\tfile = {Принятая версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\2BU26V7I\\\\Levshov и др. - 2017 - Accurate determination of the chiral indices of in.pdf:application/pdf;Принятая версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\75XGRBXA\\\\Levshov и др. - 2017 - Accurate determination of the chiral indices of in.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The experimental approach combining high resolution transmission electron microscopy (HRTEM), electron diffraction (ED) and resonant Raman spectroscopy (RRS) on the same free-standing individual carbon nanotubes (CNT) is the most efficient method to determine unambiguously the intrinsic features of the Raman-active phonons. In this paper, we review the main results obtained by the approach regarding the intrinsic features of the phonons of single-walled (SWNT) and double-walled carbon nanotubes (DWNT). First, we detail the different methods to identify the structure of SWNTs and DWNTs from the analysis of their electron diffraction patterns (EDP). In the following, we remind the principal features of the Raman response of SWNTs, unambiguously index-identified by ED. A special attention is devoted to the effect of the inter-layer interaction on the frequencies of the Raman-active phonons in index-identified DWNTs. The information obtained on index-identified SWNT and DWNT allows us to propose Raman criteria, which help identifying CNT when the ED fails to propose a single assignment. The efficiency of the Raman criteria as the complement to the ED information for the index-assignment of a few SWNTs and DWNTs is shown. The same approach to index-assign a triple-walled carbon nanotube (TWNT), by combining ED and RRS information, is reported.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=30304556\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----2017', 'https://elibrary.ru/item.asp?id=30304556', event);\">\n    Уникальный атомный порядок гиперкагоме в геометрически фрустрированных иридиевых шпинелеподобных структурах.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Таланов, М. В.; Таланов, В. М.;  and Широков, В. Б.\n</span>\n\n  \n\n</span>\n\n  <i>Известия Академии Наук. Серия Химическая</i>, (10): 1719–1727.  2017.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=30304556\"\n     onclick=\"log_download('----2017', 'https://elibrary.ru/item.asp?id=30304556', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Уникальный атомный порядок гиперкагоме в геометрически фрустрированных иридиевых шпинелеподобных структурах [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>8 downloads</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2017-3,\n\ttitle = {Уникальный атомный порядок гиперкагоме в геометрически фрустрированных иридиевых шпинелеподобных структурах},\n\tissn = {1026-3500, 2658-784X},\n\turl = {https://elibrary.ru/item.asp?id=30304556},\n\tabstract = {Представлен краткий авторский обзор результатов теоретического исследования уникального атомного и орбитального порядка гиперкагоме в геометрически фрустрированных иридиевых шпинелеподобных структурах. Установлен структурный механизм образования атомного порядка гиперкагоме. Показано, что фундаментальной структурной особенностью иридиевых шпинелеподобных структур является существование замкнутых контуров химических связей Ir-Ir, каждый из которых состоит из десяти атомов - декагонов. Высказано предположение, что декагоны обусловливают аномальные химические и физические свойства кристаллов. Сделан прогноз структурных типов кристаллов, в которых может существовать атомный порядок гиперкагоме.},\n\tlanguage = {ru},\n\tnumber = {10},\n\turldate = {2023-11-11},\n\tjournal = {Известия Академии Наук. Серия Химическая},\n\tauthor = {Таланов, М. В. and Таланов, В. М. and Широков, В. Б.},\n\tyear = {2017},\n\tkeywords = {Геометрическая Фрустрация, Декагоны, Порядок Гиперкагоме, Упорядоченные Шпинели, ⛔ No DOI found},\n\tpages = {1719--1727},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Представлен краткий авторский обзор результатов теоретического исследования уникального атомного и орбитального порядка гиперкагоме в геометрически фрустрированных иридиевых шпинелеподобных структурах. Установлен структурный механизм образования атомного порядка гиперкагоме. Показано, что фундаментальной структурной особенностью иридиевых шпинелеподобных структур является существование замкнутых контуров химических связей Ir-Ir, каждый из которых состоит из десяти атомов - декагонов. Высказано предположение, что декагоны обусловливают аномальные химические и физические свойства кристаллов. Сделан прогноз структурных типов кристаллов, в которых может существовать атомный порядок гиперкагоме.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-------2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=29911660\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-------2017', 'https://elibrary.ru/item.asp?id=29911660', event);\">\n    Влияние барьерных веществ на магниторезистивные свойства композитов на основе манганита лантана стронция.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Кабиров, Ю. В.; Гавриляченко, В. Г.; Богатин, А. С.; Чебанова, Е. В.; Пруцакова, Н. В.;  and Русакова, Е. Б.\n</span>\n\n  \n\n</span>\n\n  <i>Инженерный Вестник Дона</i>, (2 (45)): 4.  2017.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=29911660\"\n     onclick=\"log_download('-------2017', 'https://elibrary.ru/item.asp?id=29911660', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Влияние барьерных веществ на магниторезистивные свойства композитов на основе манганита лантана стронция [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-------2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>1 download</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-------2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2017-4,\n\ttitle = {Влияние барьерных веществ на магниторезистивные свойства композитов на основе манганита лантана стронция},\n\tissn = {2073-8633},\n\turl = {https://elibrary.ru/item.asp?id=29911660},\n\tabstract = {Based on our own, as well as literary experimental data, the analysis of the Influence of a barrier material used to create heterogeneous composites based on La0.7Sr0.3MnO3 on their magnetoresistive properties is carried out. Such composites differ in existence of an isotropic negative magnitorezistivnost (MR) connected from backs - dependent tunneling of carriers in magnetic field. The largest value MR up to 15\\% in the field of 15 kOe are shown when using glass-like GeO2 oxide at a percolation ratio of components.},\n\tlanguage = {ru},\n\tnumber = {2 (45)},\n\turldate = {2023-11-11},\n\tjournal = {Инженерный Вестник Дона},\n\tauthor = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Богатин, А. С. and Чебанова, Е. В. and Пруцакова, Н. В. and Русакова, Е. Б.},\n\tyear = {2017},\n\tkeywords = {Барьерный Слой, Диэлектрическая Проницаемость, Керамика, Композитный Материал, Магниторезистивность, Манганит Лантана Стронция, Одношаговый Синтез, Порог Перколяции, Спиновая Поляризация, Туннелирование, ⛔ No DOI found},\n\tpages = {4},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Based on our own, as well as literary experimental data, the analysis of the Influence of a barrier material used to create heterogeneous composites based on La0.7Sr0.3MnO3 on their magnetoresistive properties is carried out. Such composites differ in existence of an isotropic negative magnitorezistivnost (MR) connected from backs - dependent tunneling of carriers in magnetic field. The largest value MR up to 15% in the field of 15 kOe are shown when using glass-like GeO2 oxide at a percolation ratio of components.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"tikhonov-zakharchenko-razumnaya-yuzyuk-pavunny-ortega-kumar-katiyar-acomparativexraydiffractionstudyofferroelectricthinfilmsandsuperlattices-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.tandfonline.com/doi/abs/10.1080/00150193.2017.1289764\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'tikhonov-zakharchenko-razumnaya-yuzyuk-pavunny-ortega-kumar-katiyar-acomparativexraydiffractionstudyofferroelectricthinfilmsandsuperlattices-2017', 'https://www.tandfonline.com/doi/abs/10.1080/00150193.2017.1289764', event);\">\n    A comparative X-ray diffraction study of ferroelectric thin films and superlattices.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Tikhonov, Y. A.; Zakharchenko, I. N.; Razumnaya, A. G.; Yuzyuk, Y. I.; Pavunny, S.; Ortega, N.; Kumar, A.;  and Katiyar, R. S.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>. February 2017.\n  <span class=\"note\">Publisher: Taylor & Francis</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.tandfonline.com/doi/abs/10.1080/00150193.2017.1289764\"\n     onclick=\"log_download('tikhonov-zakharchenko-razumnaya-yuzyuk-pavunny-ortega-kumar-katiyar-acomparativexraydiffractionstudyofferroelectricthinfilmsandsuperlattices-2017', 'https://www.tandfonline.com/doi/abs/10.1080/00150193.2017.1289764', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"A comparative X-ray diffraction study of ferroelectric thin films and superlattices [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/tikhonov-zakharchenko-razumnaya-yuzyuk-pavunny-ortega-kumar-katiyar-acomparativexraydiffractionstudyofferroelectricthinfilmsandsuperlattices-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('tikhonov-zakharchenko-razumnaya-yuzyuk-pavunny-ortega-kumar-katiyar-acomparativexraydiffractionstudyofferroelectricthinfilmsandsuperlattices-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{tikhonov_comparative_2017,\n\ttitle = {A comparative {X}-ray diffraction study of ferroelectric thin films and superlattices},\n\tcopyright = {© 2017 Taylor \\&amp; Francis Group, LLC},\n\tissn = {0015-0193},\n\turl = {https://www.tandfonline.com/doi/abs/10.1080/00150193.2017.1289764},\n\tabstract = {A number of ferroelectric thin films with various barium concentration and two sets of superlattices with different composition and number of constituent layers were investigated using X-ray diffra...},\n\tlanguage = {EN},\n\turldate = {2023-11-11},\n\tjournal = {Ferroelectrics},\n\tauthor = {Tikhonov, Yu A. and Zakharchenko, I. N. and Razumnaya, A. G. and Yuzyuk, Y. I. and Pavunny, Sh and Ortega, N. and Kumar, A. and Katiyar, R. S.},\n\tmonth = feb,\n\tyear = {2017},\n\tnote = {Publisher: Taylor \\&amp; Francis},\n\tkeywords = {⛔ No DOI found},\n\tfile = {Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\VRJ96NXD\\\\full.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A number of ferroelectric thin films with various barium concentration and two sets of superlattices with different composition and number of constituent layers were investigated using X-ray diffra...\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"ru-ru-ru-ru--2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://findpatent.ru/patent/261/2613590.html\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'ru-ru-ru-ru--2017', 'https://findpatent.ru/patent/261/2613590.html', event);\">\n    Пассивный беспроводный датчик ультрафиолетового излучения на поверхностных акустических волнах.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Кайдашев Евгений Михайлович (RU); Кайдашев Владимир Евгеньевич (RU); Карапетьян Геворк Яковлевич (RU);  and Жилин Денис Анатольевич (RU)\n</span>\n\n  \n\n</span>\n\n  March 2017.<!-- NOTE FROM BIBBASE: This entry has an invalid bibtex entry type: patent. Therefore, we don't know how to render it properly. Please consider fixing this. -->\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://findpatent.ru/patent/261/2613590.html\"\n     onclick=\"log_download('ru-ru-ru-ru--2017', 'https://findpatent.ru/patent/261/2613590.html', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Пассивный беспроводный датчик ультрафиолетового излучения на поверхностных акустических волнах [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/ru-ru-ru-ru--2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('ru-ru-ru-ru--2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@patent{___ru__2017,\n\ttitle = {Пассивный беспроводный датчик ультрафиолетового излучения на поверхностных акустических волнах},\n\turl = {https://findpatent.ru/patent/261/2613590.html},\n\tnumber = {RU 2613590},\n\tauthor = {{Кайдашев Евгений Михайлович (RU)} and {Кайдашев Владимир Евгеньевич (RU)} and {Карапетьян Геворк Яковлевич (RU)} and {Жилин Денис Анатольевич (RU)}},\n\tmonth = mar,\n\tyear = {2017},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"nazarenko-zaletov-yuv-chagovets-ananyeva-rudskaya-kupriyanov-thestructureandparamagnetismof1xbifeotextrm3xymnotextrm3solidsolutions-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=30471203\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'nazarenko-zaletov-yuv-chagovets-ananyeva-rudskaya-kupriyanov-thestructureandparamagnetismof1xbifeotextrm3xymnotextrm3solidsolutions-2017', 'https://elibrary.ru/item.asp?id=30471203', event);\">\n    THE STRUCTURE AND PARAMAGNETISM OF (1-x)BiFeO$_{\\textrm{3}}$ – xYMnO$_{\\textrm{3}}$ SOLID SOLUTIONS.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Nazarenko, A. V.; Zaletov, V. G.; Yu.v., K.; Chagovets, S. V.; Ananyeva, E. V.; Rudskaya, A. G.;  and Kupriyanov, M. F.\n</span>\n\n  \n\n</span>\n\n  In  2017. \n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=30471203\"\n     onclick=\"log_download('nazarenko-zaletov-yuv-chagovets-ananyeva-rudskaya-kupriyanov-thestructureandparamagnetismof1xbifeotextrm3xymnotextrm3solidsolutions-2017', 'https://elibrary.ru/item.asp?id=30471203', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"THE STRUCTURE AND PARAMAGNETISM OF (1-x)BiFeO$_{\\textrm{3}}$ – xYMnO$_{\\textrm{3}}$ SOLID SOLUTIONS [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/nazarenko-zaletov-yuv-chagovets-ananyeva-rudskaya-kupriyanov-thestructureandparamagnetismof1xbifeotextrm3xymnotextrm3solidsolutions-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('nazarenko-zaletov-yuv-chagovets-ananyeva-rudskaya-kupriyanov-thestructureandparamagnetismof1xbifeotextrm3xymnotextrm3solidsolutions-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{nazarenko_structure_2017,\n\ttitle = {{THE} {STRUCTURE} {AND} {PARAMAGNETISM} {OF} (1-x){BiFeO}$_{\\textrm{3}}$ – {xYMnO}$_{\\textrm{3}}$ {SOLID} {SOLUTIONS}},\n\turl = {https://elibrary.ru/item.asp?id=30471203},\n\tabstract = {In solid solutions of (1–x)BiFeO 3 –xYMnO 3 around x = 0.5 the monoclinic phase with C2 symmetry is detected. It was found that the Lande parameter values of the electronic paramagnetic resonance signals (g-factors) of compositions with 0 {\\textless} x {\\textless} 0.8 differ from g-factor of the free electron (g e = 2.0023) and depend on concentration of x with the maximum value for x = 0.5. Also paramagnetic parameters correlate with bond lengths and angles between Fe/Mn-centred octahedron in the perovskite structures.},\n\tlanguage = {en},\n\turldate = {2023-11-11},\n\tauthor = {Nazarenko, A. V. and Zaletov, V. G. and Kabirov Yu.v. and Chagovets, S. V. and Ananyeva, E. V. and Rudskaya, A. G. and Kupriyanov, M. F.},\n\tyear = {2017},\n\tkeywords = {Perovskite, (1-X)bifeo3 -Xymno3, Bifeo3, Epr, Multiferroics, Xrd, Ymno3, ⛔ No DOI found},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  In solid solutions of (1–x)BiFeO 3 –xYMnO 3 around x = 0.5 the monoclinic phase with C2 symmetry is detected. It was found that the Lande parameter values of the electronic paramagnetic resonance signals (g-factors) of compositions with 0 \\textless x \\textless 0.8 differ from g-factor of the free electron (g e = 2.0023) and depend on concentration of x with the maximum value for x = 0.5. Also paramagnetic parameters correlate with bond lengths and angles between Fe/Mn-centred octahedron in the perovskite structures.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kadyrov-zhukova-torgashev-zhang-gagkaeva-dressel-gorshunov-terahertzspectroscopyoflowenergyexcitationsineutextrm042srtextrm058mnotextrm3-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.96.245120\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kadyrov-zhukova-torgashev-zhang-gagkaeva-dressel-gorshunov-terahertzspectroscopyoflowenergyexcitationsineutextrm042srtextrm058mnotextrm3-2017', 'https://link.aps.org/doi/10.1103/PhysRevB.96.245120', event);\">\n    Terahertz spectroscopy of low-energy excitations in Eu$_{\\textrm{0.42}}$Sr$_{\\textrm{0.58}}$MnO$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kadyrov, L. S.; Zhukova, E. S.; Torgashev, V. I.; Zhang, T.; Gagkaeva, Z. V.; Dressel, M.;  and Gorshunov, B. P.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 96(24): 245120. December 2017.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.96.245120\"\n     onclick=\"log_download('kadyrov-zhukova-torgashev-zhang-gagkaeva-dressel-gorshunov-terahertzspectroscopyoflowenergyexcitationsineutextrm042srtextrm058mnotextrm3-2017', 'https://link.aps.org/doi/10.1103/PhysRevB.96.245120', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Terahertz spectroscopy of low-energy excitations in Eu$_{\\textrm{0.42}}$Sr$_{\\textrm{0.58}}$MnO$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.96.245120\"\n     onclick=\"log_download('kadyrov-zhukova-torgashev-zhang-gagkaeva-dressel-gorshunov-terahertzspectroscopyoflowenergyexcitationsineutextrm042srtextrm058mnotextrm3-2017', 'http://doi.org/10.1103/PhysRevB.96.245120', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kadyrov-zhukova-torgashev-zhang-gagkaeva-dressel-gorshunov-terahertzspectroscopyoflowenergyexcitationsineutextrm042srtextrm058mnotextrm3-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kadyrov-zhukova-torgashev-zhang-gagkaeva-dressel-gorshunov-terahertzspectroscopyoflowenergyexcitationsineutextrm042srtextrm058mnotextrm3-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kadyrov_terahertz_2017,\n\ttitle = {Terahertz spectroscopy of low-energy excitations in {Eu}$_{\\textrm{0.42}}${Sr}$_{\\textrm{0.58}}${MnO}$_{\\textrm{3}}$},\n\tvolume = {96},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.96.245120},\n\tdoi = {10.1103/PhysRevB.96.245120},\n\tabstract = {The origin of low-energy excitations in the polycrystalline Eu0.42Sr0.58MnO3 manganite is explored by terahertz and infrared spectroscopies. The transition from the charge and/or orbital to antiferromagnetic order (TN=130−140K) is seen as smooth (spread over a temperature range from 50 to 100 K) decrease of free-carrier conductivity with the activation energy change from 86 meV (high temperatures) to 0.52 meV (low temperatures). A broad relaxation is observed at around 10cm−1 which we associate with the dynamics of free charge carriers in the presence of random localizing potential. We discover an absorption resonance at ≈50cm−1 below TN that is assigned to the formation of hybridized “acoustic phonon-magnon” quasiparticles.},\n\tnumber = {24},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Kadyrov, L. S. and Zhukova, E. S. and Torgashev, V. I. and Zhang, T. and Gagkaeva, Z. V. and Dressel, M. and Gorshunov, B. P.},\n\tmonth = dec,\n\tyear = {2017},\n\tnote = {Publisher: American Physical Society},\n\tpages = {245120},\n\tfile = {APS Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\GFXPT7MJ\\\\PhysRevB.96.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The origin of low-energy excitations in the polycrystalline Eu0.42Sr0.58MnO3 manganite is explored by terahertz and infrared spectroscopies. The transition from the charge and/or orbital to antiferromagnetic order (TN=130−140K) is seen as smooth (spread over a temperature range from 50 to 100 K) decrease of free-carrier conductivity with the activation energy change from 86 meV (high temperatures) to 0.52 meV (low temperatures). A broad relaxation is observed at around 10cm−1 which we associate with the dynamics of free charge carriers in the presence of random localizing potential. We discover an absorption resonance at ≈50cm−1 below TN that is assigned to the formation of hybridized “acoustic phonon-magnon” quasiparticles.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"chagovets-nazarenko-kozarenko-rudskaya-kupriyanov-reconstructivephasetransitioninymnotextrm3bifeotextrm3solidsolutions-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=30471067\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'chagovets-nazarenko-kozarenko-rudskaya-kupriyanov-reconstructivephasetransitioninymnotextrm3bifeotextrm3solidsolutions-2017', 'https://elibrary.ru/item.asp?id=30471067', event);\">\n    Reconstructive Phase Transition in YMnO$_{\\textrm{3}}$ –BiFeO$_{\\textrm{3}}$ Solid Solutions.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Chagovets, S. V.; Nazarenko, A. V.; Kozarenko, S. S.; Rudskaya, A. G.;  and Kupriyanov, M. F.\n</span>\n\n  \n\n</span>\n\n  In  2017. \n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=30471067\"\n     onclick=\"log_download('chagovets-nazarenko-kozarenko-rudskaya-kupriyanov-reconstructivephasetransitioninymnotextrm3bifeotextrm3solidsolutions-2017', 'https://elibrary.ru/item.asp?id=30471067', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Reconstructive Phase Transition in YMnO$_{\\textrm{3}}$ –BiFeO$_{\\textrm{3}}$ Solid Solutions [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/chagovets-nazarenko-kozarenko-rudskaya-kupriyanov-reconstructivephasetransitioninymnotextrm3bifeotextrm3solidsolutions-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('chagovets-nazarenko-kozarenko-rudskaya-kupriyanov-reconstructivephasetransitioninymnotextrm3bifeotextrm3solidsolutions-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{chagovets_reconstructive_2017,\n\ttitle = {Reconstructive {Phase} {Transition} in {YMnO}$_{\\textrm{3}}$ –{BiFeO}$_{\\textrm{3}}$ {Solid} {Solutions}},\n\turl = {https://elibrary.ru/item.asp?id=30471067},\n\tabstract = {The structures of the (1–x)YMnO 3 –xBiFeO 3 (0.05 ≤ x ≤ 0.25) solid solutions have been studied by means of the X-ray diffraction method. It was established that in the compounds of the (1–x)YMnO 3 –xBiFeO 3 system the P6 3 cm, the Pbam and Pnma phases are observed at room temperature after annealing at T 1 = 950 °C. The results revealed that in the compounds of the (1–x)YMnO 3 –xBiFeO 3 system the P6 3 cm and Pnma phases take place at room temperature after annealing at T 2 = 1100 °C. The symmetry of the phases, the unit cell parameters, the positional atomic parameters have been determined.},\n\tlanguage = {en},\n\turldate = {2023-11-11},\n\tauthor = {Chagovets, S. V. and Nazarenko, A. V. and Kozarenko, S. S. and Rudskaya, A. G. and Kupriyanov, M. F.},\n\tyear = {2017},\n\tkeywords = {(1-X)bifeo 3 -Xymno 3, Multiferroic, Phase Transition, X-Ray Diffraction, ⛔ No DOI found},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The structures of the (1–x)YMnO 3 –xBiFeO 3 (0.05 ≤ x ≤ 0.25) solid solutions have been studied by means of the X-ray diffraction method. It was established that in the compounds of the (1–x)YMnO 3 –xBiFeO 3 system the P6 3 cm, the Pbam and Pnma phases are observed at room temperature after annealing at T 1 = 950 °C. The results revealed that in the compounds of the (1–x)YMnO 3 –xBiFeO 3 system the P6 3 cm and Pnma phases take place at room temperature after annealing at T 2 = 1100 °C. The symmetry of the phases, the unit cell parameters, the positional atomic parameters have been determined.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"stryukov-razumnaya-golovko-anokhin-lukyanchuk-shirokov-mukhortov-latticedynamicsandstructuraldistortionsinthemultiferroicbasrtiotextrm3bindfeotextrm3heterostructures-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0040609017304443\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'stryukov-razumnaya-golovko-anokhin-lukyanchuk-shirokov-mukhortov-latticedynamicsandstructuraldistortionsinthemultiferroicbasrtiotextrm3bindfeotextrm3heterostructures-2017', 'https://www.sciencedirect.com/science/article/pii/S0040609017304443', event);\">\n    Lattice dynamics and structural distortions in the multiferroic (Ba,Sr)TiO$_{\\textrm{3}}$/(Bi,Nd)FeO$_{\\textrm{3}}$ heterostructures.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Stryukov, D. V.; Razumnaya, A. G.; Golovko, Y. I.; Anokhin, A. S.; Lukyanchuk, I. A.; Shirokov, V. B.;  and Mukhortov, V. M.\n</span>\n\n  \n\n</span>\n\n  <i>Thin Solid Films</i>, 636: 220–224. August 2017.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0040609017304443\"\n     onclick=\"log_download('stryukov-razumnaya-golovko-anokhin-lukyanchuk-shirokov-mukhortov-latticedynamicsandstructuraldistortionsinthemultiferroicbasrtiotextrm3bindfeotextrm3heterostructures-2017', 'https://www.sciencedirect.com/science/article/pii/S0040609017304443', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Lattice dynamics and structural distortions in the multiferroic (Ba,Sr)TiO$_{\\textrm{3}}$/(Bi,Nd)FeO$_{\\textrm{3}}$ heterostructures [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.tsf.2017.06.009\"\n     onclick=\"log_download('stryukov-razumnaya-golovko-anokhin-lukyanchuk-shirokov-mukhortov-latticedynamicsandstructuraldistortionsinthemultiferroicbasrtiotextrm3bindfeotextrm3heterostructures-2017', 'http://doi.org/10.1016/j.tsf.2017.06.009', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/stryukov-razumnaya-golovko-anokhin-lukyanchuk-shirokov-mukhortov-latticedynamicsandstructuraldistortionsinthemultiferroicbasrtiotextrm3bindfeotextrm3heterostructures-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('stryukov-razumnaya-golovko-anokhin-lukyanchuk-shirokov-mukhortov-latticedynamicsandstructuraldistortionsinthemultiferroicbasrtiotextrm3bindfeotextrm3heterostructures-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{stryukov_lattice_2017,\n\ttitle = {Lattice dynamics and structural distortions in the multiferroic ({Ba},{Sr}){TiO}$_{\\textrm{3}}$/({Bi},{Nd}){FeO}$_{\\textrm{3}}$ heterostructures},\n\tvolume = {636},\n\tissn = {0040-6090},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0040609017304443},\n\tdoi = {10.1016/j.tsf.2017.06.009},\n\tabstract = {We report the synthesis, the structure and phonon spectra studies of epitaxial double-layer heterostructures consisting of Bi0.98Nd0.02FeO3 and Ba0.8Sr0.2TiO3 layers deposited on (100) MgO substrates. The results of x-ray diffraction and the polarization characteristics of Raman spectra suggest a monoclinic symmetry of the systems at room temperature. The observed spectra demonstrate the non-monotonous dependence on the layer thickness that apparently can be related with specificity of the light propagation in the layered thin-film systems.},\n\turldate = {2023-11-11},\n\tjournal = {Thin Solid Films},\n\tauthor = {Stryukov, D. V. and Razumnaya, A. G. and Golovko, Yu I. and Anokhin, A. S. and Lukyanchuk, I. A. and Shirokov, V. B. and Mukhortov, V. M.},\n\tmonth = aug,\n\tyear = {2017},\n\tkeywords = {X-ray diffraction, Raman spectroscopy, Bismuth ferrite, Heterostructures, Lattice distortions, Lattice dynamics, Sputtering},\n\tpages = {220--224},\n\tfile = {ScienceDirect Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\TD9K6CTD\\\\S0040609017304443.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We report the synthesis, the structure and phonon spectra studies of epitaxial double-layer heterostructures consisting of Bi0.98Nd0.02FeO3 and Ba0.8Sr0.2TiO3 layers deposited on (100) MgO substrates. The results of x-ray diffraction and the polarization characteristics of Raman spectra suggest a monoclinic symmetry of the systems at room temperature. The observed spectra demonstrate the non-monotonous dependence on the layer thickness that apparently can be related with specificity of the light propagation in the layered thin-film systems.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"trotsenko-mikheykin-shirokov-razumnaya-elmarssi-gorshunov-bush-torgashev-invareffectaccompanyingchargeorderinlatextrm025catextrm075mnotextrm3-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S1293255817305381\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'trotsenko-mikheykin-shirokov-razumnaya-elmarssi-gorshunov-bush-torgashev-invareffectaccompanyingchargeorderinlatextrm025catextrm075mnotextrm3-2017', 'https://www.sciencedirect.com/science/article/pii/S1293255817305381', event);\">\n    Invar effect accompanying charge order in La$_{\\textrm{0.25}}$Ca$_{\\textrm{0.75}}$MnO$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Trotsenko, V. G.; Mikheykin, A. S.; Shirokov, V. B.; Razumnaya, A. G.; El Marssi, M.; Gorshunov, B. P.; Bush, A. A.;  and Torgashev, V. I.\n</span>\n\n  \n\n</span>\n\n  <i>Solid State Sciences</i>, 72: 144–149. October 2017.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S1293255817305381\"\n     onclick=\"log_download('trotsenko-mikheykin-shirokov-razumnaya-elmarssi-gorshunov-bush-torgashev-invareffectaccompanyingchargeorderinlatextrm025catextrm075mnotextrm3-2017', 'https://www.sciencedirect.com/science/article/pii/S1293255817305381', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Invar effect accompanying charge order in La$_{\\textrm{0.25}}$Ca$_{\\textrm{0.75}}$MnO$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.solidstatesciences.2017.08.020\"\n     onclick=\"log_download('trotsenko-mikheykin-shirokov-razumnaya-elmarssi-gorshunov-bush-torgashev-invareffectaccompanyingchargeorderinlatextrm025catextrm075mnotextrm3-2017', 'http://doi.org/10.1016/j.solidstatesciences.2017.08.020', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/trotsenko-mikheykin-shirokov-razumnaya-elmarssi-gorshunov-bush-torgashev-invareffectaccompanyingchargeorderinlatextrm025catextrm075mnotextrm3-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('trotsenko-mikheykin-shirokov-razumnaya-elmarssi-gorshunov-bush-torgashev-invareffectaccompanyingchargeorderinlatextrm025catextrm075mnotextrm3-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{trotsenko_invar_2017,\n\ttitle = {Invar effect accompanying charge order in {La}$_{\\textrm{0.25}}${Ca}$_{\\textrm{0.75}}${MnO}$_{\\textrm{3}}$},\n\tvolume = {72},\n\tissn = {1293-2558},\n\turl = {https://www.sciencedirect.com/science/article/pii/S1293255817305381},\n\tdoi = {10.1016/j.solidstatesciences.2017.08.020},\n\tabstract = {To determine the role of the Jahn-Teller effect in the orbital and charge ordering of mixed crystals of the strongly correlated La1-xCaxMnO3 system, we have used the diffraction of synchrotron radiation and the subsequent Rietveld analysis of diffraction patterns in order to obtain structural data for La0.25Ca0.75MnO3 compound in the temperature range from 90 to 325 K with a step of ∼2 K. For the first time for this compound, an Invar effect was observed below the charge-order temperature. In the entire temperature range, atomic displacements were analyzed and correlations between charge ordering and deformational modes were made, on the basis of which the secondary role of the Jahn-Teller effect in observed structure distortions was established. A hypothesis of a spin crossover in the vicinity of the charge-ordering temperature is proposed that describes adequately both the obtained structural data and the results of measurements of the macroscopic magnetic and elastic properties of the studied compound as well as related materials with charge ordering.},\n\turldate = {2023-11-11},\n\tjournal = {Solid State Sciences},\n\tauthor = {Trotsenko, V. G. and Mikheykin, A. S. and Shirokov, V. B. and Razumnaya, A. G. and El Marssi, M. and Gorshunov, B. P. and Bush, A. A. and Torgashev, V. I.},\n\tmonth = oct,\n\tyear = {2017},\n\tkeywords = {Charge ordering, Correlated electron systems, Invar effect, Spin crossover},\n\tpages = {144--149},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  To determine the role of the Jahn-Teller effect in the orbital and charge ordering of mixed crystals of the strongly correlated La1-xCaxMnO3 system, we have used the diffraction of synchrotron radiation and the subsequent Rietveld analysis of diffraction patterns in order to obtain structural data for La0.25Ca0.75MnO3 compound in the temperature range from 90 to 325 K with a step of ∼2 K. For the first time for this compound, an Invar effect was observed below the charge-order temperature. In the entire temperature range, atomic displacements were analyzed and correlations between charge ordering and deformational modes were made, on the basis of which the secondary role of the Jahn-Teller effect in observed structure distortions was established. A hypothesis of a spin crossover in the vicinity of the charge-ordering temperature is proposed that describes adequately both the obtained structural data and the results of measurements of the macroscopic magnetic and elastic properties of the studied compound as well as related materials with charge ordering.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"mikheykin-chernyshov-makarova-grebenev-komornikov-selezneva-fastprotonconductionincstextrm3hsotextrm4textrm2htextrm2potextrm4andcstextrm4hsotextrm4textrm3htextrm2potextrm4-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0167273816307147\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'mikheykin-chernyshov-makarova-grebenev-komornikov-selezneva-fastprotonconductionincstextrm3hsotextrm4textrm2htextrm2potextrm4andcstextrm4hsotextrm4textrm3htextrm2potextrm4-2017', 'https://www.sciencedirect.com/science/article/pii/S0167273816307147', event);\">\n    Fast proton conduction in Cs$_{\\textrm{3}}$(HSO$_{\\textrm{4}}$)$_{\\textrm{2}}$(H$_{\\textrm{2}}$PO$_{\\textrm{4}}$) and Cs$_{\\textrm{4}}$(HSO$_{\\textrm{4}}$)$_{\\textrm{3}}$(H$_{\\textrm{2}}$PO$_{\\textrm{4}}$).\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Mikheykin, A. S.; Chernyshov, D. Y.; Makarova, I. P.; Grebenev, V. V.; Komornikov, V. A.;  and Selezneva, E. V.\n</span>\n\n  \n\n</span>\n\n  <i>Solid State Ionics</i>, 305: 30–35. July 2017.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0167273816307147\"\n     onclick=\"log_download('mikheykin-chernyshov-makarova-grebenev-komornikov-selezneva-fastprotonconductionincstextrm3hsotextrm4textrm2htextrm2potextrm4andcstextrm4hsotextrm4textrm3htextrm2potextrm4-2017', 'https://www.sciencedirect.com/science/article/pii/S0167273816307147', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Fast proton conduction in Cs$_{\\textrm{3}}$(HSO$_{\\textrm{4}}$)$_{\\textrm{2}}$(H$_{\\textrm{2}}$PO$_{\\textrm{4}}$) and Cs$_{\\textrm{4}}$(HSO$_{\\textrm{4}}$)$_{\\textrm{3}}$(H$_{\\textrm{2}}$PO$_{\\textrm{4}}$) [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.ssi.2017.04.017\"\n     onclick=\"log_download('mikheykin-chernyshov-makarova-grebenev-komornikov-selezneva-fastprotonconductionincstextrm3hsotextrm4textrm2htextrm2potextrm4andcstextrm4hsotextrm4textrm3htextrm2potextrm4-2017', 'http://doi.org/10.1016/j.ssi.2017.04.017', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/mikheykin-chernyshov-makarova-grebenev-komornikov-selezneva-fastprotonconductionincstextrm3hsotextrm4textrm2htextrm2potextrm4andcstextrm4hsotextrm4textrm3htextrm2potextrm4-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('mikheykin-chernyshov-makarova-grebenev-komornikov-selezneva-fastprotonconductionincstextrm3hsotextrm4textrm2htextrm2potextrm4andcstextrm4hsotextrm4textrm3htextrm2potextrm4-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{mikheykin_fast_2017,\n\ttitle = {Fast proton conduction in {Cs}$_{\\textrm{3}}$({HSO}$_{\\textrm{4}}$)$_{\\textrm{2}}$({H}$_{\\textrm{2}}${PO}$_{\\textrm{4}}$) and {Cs}$_{\\textrm{4}}$({HSO}$_{\\textrm{4}}$)$_{\\textrm{3}}$({H}$_{\\textrm{2}}${PO}$_{\\textrm{4}}$)},\n\tvolume = {305},\n\tissn = {0167-2738},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0167273816307147},\n\tdoi = {10.1016/j.ssi.2017.04.017},\n\tabstract = {X-ray powder diffraction studies were performed on Cs3(HSO4)2(H2PO4) and Cs4(HSO4)3(H2PO4) in the range 340–440K. For the both compounds a first order phase transition from the monoclinic C2/c phase to the mixture of cubic Pm-3m and tetragonal I41/amd superprotonic phases takes place at 408–414 and 412–414K respectively; the ratio between cubic and tetragonal depends on material and temperature. The tetragonal phase transforms to the cubic modification on heating and this transition is reversible.},\n\turldate = {2023-11-11},\n\tjournal = {Solid State Ionics},\n\tauthor = {Mikheykin, A. S. and Chernyshov, D. Yu. and Makarova, I. P. and Grebenev, V. V. and Komornikov, V. A. and Selezneva, E. V.},\n\tmonth = jul,\n\tyear = {2017},\n\tkeywords = {Solid solutions, Phase transition, Superprotonics, XRPD},\n\tpages = {30--35},\n\tfile = {ScienceDirect Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\ZKIPJH5U\\\\S0167273816307147.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  X-ray powder diffraction studies were performed on Cs3(HSO4)2(H2PO4) and Cs4(HSO4)3(H2PO4) in the range 340–440K. For the both compounds a first order phase transition from the monoclinic C2/c phase to the mixture of cubic Pm-3m and tetragonal I41/amd superprotonic phases takes place at 408–414 and 412–414K respectively; the ratio between cubic and tetragonal depends on material and temperature. The tetragonal phase transforms to the cubic modification on heating and this transition is reversible.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kuriganova-leontyev-alexandrin-maslova-rakhmatullin-smirnova-electrochemicallysynthesizedpttiotextrm2ccatalystsfordirectmethanolfuelcellapplications-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0959943617300214\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kuriganova-leontyev-alexandrin-maslova-rakhmatullin-smirnova-electrochemicallysynthesizedpttiotextrm2ccatalystsfordirectmethanolfuelcellapplications-2017', 'https://www.sciencedirect.com/science/article/pii/S0959943617300214', event);\">\n    Electrochemically synthesized Pt/TiO$_{\\textrm{2}}$-C catalysts for direct methanol fuel cell applications.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kuriganova, A. B.; Leontyev, I. N.; Alexandrin, A. S.; Maslova, O. A.; Rakhmatullin, A. I.;  and Smirnova, N. V.\n</span>\n\n  \n\n</span>\n\n  <i>Mendeleev Communications</i>, 27(1): 67–69. January 2017.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0959943617300214\"\n     onclick=\"log_download('kuriganova-leontyev-alexandrin-maslova-rakhmatullin-smirnova-electrochemicallysynthesizedpttiotextrm2ccatalystsfordirectmethanolfuelcellapplications-2017', 'https://www.sciencedirect.com/science/article/pii/S0959943617300214', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Electrochemically synthesized Pt/TiO$_{\\textrm{2}}$-C catalysts for direct methanol fuel cell applications [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.mencom.2017.01.021\"\n     onclick=\"log_download('kuriganova-leontyev-alexandrin-maslova-rakhmatullin-smirnova-electrochemicallysynthesizedpttiotextrm2ccatalystsfordirectmethanolfuelcellapplications-2017', 'http://doi.org/10.1016/j.mencom.2017.01.021', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kuriganova-leontyev-alexandrin-maslova-rakhmatullin-smirnova-electrochemicallysynthesizedpttiotextrm2ccatalystsfordirectmethanolfuelcellapplications-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kuriganova-leontyev-alexandrin-maslova-rakhmatullin-smirnova-electrochemicallysynthesizedpttiotextrm2ccatalystsfordirectmethanolfuelcellapplications-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kuriganova_electrochemically_2017,\n\ttitle = {Electrochemically synthesized {Pt}/{TiO}$_{\\textrm{2}}$-{C} catalysts for direct methanol fuel cell applications},\n\tvolume = {27},\n\tissn = {0959-9436},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0959943617300214},\n\tdoi = {10.1016/j.mencom.2017.01.021},\n\tabstract = {The Pt/TiO2-C catalysts with different TiO2 loadings have been prepared by electrochemical oxidation/dispersion, and their good catalytic activity in CO stripping and methanol electrooxidation reactions has been shown.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Mendeleev Communications},\n\tauthor = {Kuriganova, Alexandra B. and Leontyev, Igor N. and Alexandrin, Alexander S. and Maslova, Olga A. and Rakhmatullin, Aydar I. and Smirnova, Nina V.},\n\tmonth = jan,\n\tyear = {2017},\n\tpages = {67--69},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The Pt/TiO2-C catalysts with different TiO2 loadings have been prepared by electrochemical oxidation/dispersion, and their good catalytic activity in CO stripping and methanol electrooxidation reactions has been shown.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kozakov-kochur-torgashev-kubrin-trotsenko-bush-nikolskii-crystalstructurephaseandelementalcompositionandchemicalbondinginbitextrm1xatextrmxfeotextrm3ysystemsasrca0x1fromxraydiffractionmssbauerandxrayphotoelectronspectra-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  Crystal Structure, Phase and Elemental Composition and Chemical Bonding in Bi$_{\\textrm{1−{X}}}$A$_{\\textrm{{X}}}$FeO$_{\\textrm{3±{Y}}}$ Systems (A = Sr, Ca; 0 ≤X ≤ 1) from X-ray Diffraction, Mössbauer, and X-ray Photoelectron Spectra.\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kozakov, A. T.; Kochur, A. G.; Torgashev, V. I.; Kubrin, S. P.; Trotsenko, V. G.; Bush, A. A.;  and Nikolskii, A. V.\n</span>\n\n  \n\n</span>\n\n  In Parinov, I. A.; Chang, S.;  and Jani, M. A., editor(s), <i>Advanced Materials</i>, of <i>Springer Proceedings in Physics</i>, pages 145–153, Cham,  2017. Springer International Publishing\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n\n  \n  <a href=\"http://doi.org/10.1007/978-3-319-56062-5_13\"\n     onclick=\"log_download('kozakov-kochur-torgashev-kubrin-trotsenko-bush-nikolskii-crystalstructurephaseandelementalcompositionandchemicalbondinginbitextrm1xatextrmxfeotextrm3ysystemsasrca0x1fromxraydiffractionmssbauerandxrayphotoelectronspectra-2017', 'http://doi.org/10.1007/978-3-319-56062-5_13', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kozakov-kochur-torgashev-kubrin-trotsenko-bush-nikolskii-crystalstructurephaseandelementalcompositionandchemicalbondinginbitextrm1xatextrmxfeotextrm3ysystemsasrca0x1fromxraydiffractionmssbauerandxrayphotoelectronspectra-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kozakov-kochur-torgashev-kubrin-trotsenko-bush-nikolskii-crystalstructurephaseandelementalcompositionandchemicalbondinginbitextrm1xatextrmxfeotextrm3ysystemsasrca0x1fromxraydiffractionmssbauerandxrayphotoelectronspectra-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{kozakov_crystal_2017,\n\taddress = {Cham},\n\tseries = {Springer {Proceedings} in {Physics}},\n\ttitle = {Crystal {Structure}, {Phase} and {Elemental} {Composition} and {Chemical} {Bonding} in {Bi}$_{\\textrm{1−{X}}}${A}$_{\\textrm{{X}}}${FeO}$_{\\textrm{3±{Y}}}$ {Systems} ({A} = {Sr}, {Ca}; 0 ≤{X} ≤ 1) from {X}-ray {Diffraction}, {Mössbauer}, and {X}-ray {Photoelectron} {Spectra}},\n\tisbn = {978-3-319-56062-5},\n\tdoi = {10.1007/978-3-319-56062-5_13},\n\tabstract = {An integrated study of samples of Bi1−xAxFeO3±y(A = Sr, Ca) systems for 0 ≤ x ≤ 1 (step 0.1) is performed using X-ray diffractionX-ray diffraction (XRD)(XRD), Mössbauer spectroscopy (MS), and X-ray photoelectron spectroscopyX-ray photoelectron spectroscopy (XPS)(XPS). Considerable deviations of actual elemental compositions from nominal ones in the samples of both systems are discovered. Both Fe3+ and Fe4+ ions are found to be present in the samples of the Bi1−xSrxFeO3±ysystem with x {\\textgreater} 0. No Fe4+ ions are discovered upon substitution of Bi3+ by Ca2+ in Bi1−xCaxFeO3±y, neither by Mössbauer spectroscopy, nor by XPS. Charge compensation in Bi1−xCaxFeO3±ytakes place mostly via creation of oxygen vacancies.},\n\tlanguage = {en},\n\tbooktitle = {Advanced {Materials}},\n\tpublisher = {Springer International Publishing},\n\tauthor = {Kozakov, A. T. and Kochur, A. G. and Torgashev, V. I. and Kubrin, S. P. and Trotsenko, V. G. and Bush, A. A. and Nikolskii, A. V.},\n\teditor = {Parinov, Ivan A. and Chang, Shun-Hsyung and Jani, Muaffaq A.},\n\tyear = {2017},\n\tkeywords = {Actual Elemental Composition, concentrationsConcentration, Mössbauer Spectroscopy, Octahedral Oxygen Environment, xCa xFeO},\n\tpages = {145--153},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  An integrated study of samples of Bi1−xAxFeO3±y(A = Sr, Ca) systems for 0 ≤ x ≤ 1 (step 0.1) is performed using X-ray diffractionX-ray diffraction (XRD)(XRD), Mössbauer spectroscopy (MS), and X-ray photoelectron spectroscopyX-ray photoelectron spectroscopy (XPS)(XPS). Considerable deviations of actual elemental compositions from nominal ones in the samples of both systems are discovered. Both Fe3+ and Fe4+ ions are found to be present in the samples of the Bi1−xSrxFeO3±ysystem with x \\textgreater 0. No Fe4+ ions are discovered upon substitution of Bi3+ by Ca2+ in Bi1−xCaxFeO3±y, neither by Mössbauer spectroscopy, nor by XPS. Charge compensation in Bi1−xCaxFeO3±ytakes place mostly via creation of oxygen vacancies.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=28843943\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----2017', 'https://elibrary.ru/item.asp?id=28843943', event);\">\n    Эффект поля в структуре металл - сегнетоэлектрик - полупроводник с использованием многослойного сегнетоэлектрика.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Стрюков, Д. В.; Мухортов, В. М.; Бирюков, С. В.;  and Головко, Ю. И.\n</span>\n\n  \n\n</span>\n\n  <i>Наука Юга России</i>, 13(1): 18–24.  2017.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=28843943\"\n     onclick=\"log_download('-----2017', 'https://elibrary.ru/item.asp?id=28843943', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Эффект поля в структуре металл - сегнетоэлектрик - полупроводник с использованием многослойного сегнетоэлектрика [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.23885/2500-0640-2017-13-1-18-24\"\n     onclick=\"log_download('-----2017', 'http://doi.org/10.23885/2500-0640-2017-13-1-18-24', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2017-5,\n\ttitle = {Эффект поля в структуре металл - сегнетоэлектрик - полупроводник с использованием многослойного сегнетоэлектрика},\n\tvolume = {13},\n\tissn = {2500-0640},\n\turl = {https://elibrary.ru/item.asp?id=28843943},\n\tdoi = {10.23885/2500-0640-2017-13-1-18-24},\n\tabstract = {Одной из важнейших концепций использования сегнетоэлектрических гетероструктур в микроэлектронике является энергонезависимая память (FeRAM), где в качестве подзатворного диэлектрика в полевом транзисторе используется сегнетоэлектрическая пленка. Вторым важным применением сегнетоэлектрических пленок является их использование при создании принципиально новых микроэлектромеханических устройств (МЕМС). Реализация МЕМС с использованием сегнетоэлектрических наноразмерных пленок в качестве активного элемента по своим параметрам в десятки раз будет превосходить существующие аналоги. В последние годы вопросам стабильности поляризованного состояния и динамики переключения поляризации придается большое значение. В данной работе впервые приведены результаты по исследованию эффекта поля в структуре металл - сегнетоэлектрик - полупроводник, где в качестве сегнетоэлектрика использованы многослойные сегнетоэлектрические слои. Использование многослойных сегнетоэлектрических гетероструктур приводит к самосогласованию поверхностных состояний на границах полупроводник - сегнетоэлектрик и сегнетоэлектрик - сегнетоэлектрик с переключаемой под действием внешнего поля спонтанной поляризацией. Это позволяет создать устойчивое поляризованное состояние с незначительной ее релаксацией.},\n\tlanguage = {ru},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Наука Юга России},\n\tauthor = {Стрюков, Д. В. and Мухортов, В. М. and Бирюков, С. В. and Головко, Ю. И.},\n\tyear = {2017},\n\tkeywords = {Двумерные Напряжения, Двухслойные Сегнетоэлектрики, Сегнетоэлектрическая Пленка, Структура, Эффект Поля},\n\tpages = {18--24},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\A5UM2STP\\\\Стрюков и др. - 2017 - Эффект Поля В Структуре Металл - Сегнетоэлектрик -.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Одной из важнейших концепций использования сегнетоэлектрических гетероструктур в микроэлектронике является энергонезависимая память (FeRAM), где в качестве подзатворного диэлектрика в полевом транзисторе используется сегнетоэлектрическая пленка. Вторым важным применением сегнетоэлектрических пленок является их использование при создании принципиально новых микроэлектромеханических устройств (МЕМС). Реализация МЕМС с использованием сегнетоэлектрических наноразмерных пленок в качестве активного элемента по своим параметрам в десятки раз будет превосходить существующие аналоги. В последние годы вопросам стабильности поляризованного состояния и динамики переключения поляризации придается большое значение. В данной работе впервые приведены результаты по исследованию эффекта поля в структуре металл - сегнетоэлектрик - полупроводник, где в качестве сегнетоэлектрика использованы многослойные сегнетоэлектрические слои. Использование многослойных сегнетоэлектрических гетероструктур приводит к самосогласованию поверхностных состояний на границах полупроводник - сегнетоэлектрик и сегнетоэлектрик - сегнетоэлектрик с переключаемой под действием внешнего поля спонтанной поляризацией. Это позволяет создать устойчивое поляризованное состояние с незначительной ее релаксацией.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------zno-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.libnauka.ru/item.php?doi=10.7868/S0033849417110055\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------zno-2017', 'https://www.libnauka.ru/item.php?doi=10.7868/S0033849417110055', event);\">\n    Экспериментальное и теоретическое исследование оптических антенн на основе наностержней ZnO покрытых тонкой пленкой серебра.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Кайдашев, Е. М.; Лерер, А.; Головачева, Е. В.; Кайдашев, В. Е.; Лянгузов, Н.;  and Цветянский, Е. А.\n</span>\n\n  \n\n</span>\n\n  <i>Радиотехника и электроника</i>, (12): 1173–1181.  2017.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.libnauka.ru/item.php?doi=10.7868/S0033849417110055\"\n     onclick=\"log_download('------zno-2017', 'https://www.libnauka.ru/item.php?doi=10.7868/S0033849417110055', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Экспериментальное и теоретическое исследование оптических антенн на основе наностержней ZnO покрытых тонкой пленкой серебра [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.7868/S0033849417110055\"\n     onclick=\"log_download('------zno-2017', 'http://doi.org/10.7868/S0033849417110055', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------zno-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------zno-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2017-6,\n\ttitle = {Экспериментальное и теоретическое исследование оптических антенн на основе наностержней {ZnO} покрытых тонкой пленкой серебра},\n\tissn = {0033-8494},\n\turl = {https://www.libnauka.ru/item.php?doi=10.7868/S0033849417110055},\n\tdoi = {10.7868/S0033849417110055},\n\tlanguage = {ru},\n\tnumber = {12},\n\turldate = {2023-11-11},\n\tjournal = {Радиотехника и электроника},\n\tauthor = {Кайдашев, Е. М. and Лерер, А.М. and Головачева, Е. В. and Кайдашев, В. Е. and Лянгузов, Н.В. and Цветянский, Е. А.},\n\tyear = {2017},\n\tpages = {1173--1181},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------srtextrm05batextrm05nbtextrm2otextrm6-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/44376\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------srtextrm05batextrm05nbtextrm2otextrm6-2017', 'https://journals.ioffe.ru/articles/44376', event);\">\n    Структура, динамика решетки и диэлектрические характеристики пленок Sr$_{\\textrm{0.5}}$Ba$_{\\textrm{0.5}}$Nb$_{\\textrm{2}}$O$_{\\textrm{6}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Павленко, А.; Захарченко, И.; Анохин, А.; Куприна, Ю.; Киселева, Л.;  and Юзюк, Ю.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 59(5): 888.  2017.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/44376\"\n     onclick=\"log_download('------srtextrm05batextrm05nbtextrm2otextrm6-2017', 'https://journals.ioffe.ru/articles/44376', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Структура, динамика решетки и диэлектрические характеристики пленок Sr$_{\\textrm{0.5}}$Ba$_{\\textrm{0.5}}$Nb$_{\\textrm{2}}$O$_{\\textrm{6}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.21883/FTT.2017.05.44376.382\"\n     onclick=\"log_download('------srtextrm05batextrm05nbtextrm2otextrm6-2017', 'http://doi.org/10.21883/FTT.2017.05.44376.382', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------srtextrm05batextrm05nbtextrm2otextrm6-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------srtextrm05batextrm05nbtextrm2otextrm6-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2017-7,\n\ttitle = {Структура, динамика решетки и диэлектрические характеристики пленок {Sr}$_{\\textrm{0.5}}${Ba}$_{\\textrm{0.5}}${Nb}$_{\\textrm{2}}${O}$_{\\textrm{6}}$},\n\tvolume = {59},\n\tissn = {0367-3294},\n\turl = {https://journals.ioffe.ru/articles/44376},\n\tdoi = {10.21883/FTT.2017.05.44376.382},\n\tabstract = {Методом высокочастотного напыления в атмосфере кислорода получены пленки твердого раствора Sr\n              0.5\n              Ba\n              0.5\n              Nb\n              2\n              O\n              6\n              на подложке (111)Pt/(001)Si. Изучены их деполяризованные спектры комбинационного рассеяния света, структура и диэлектрические характеристики в широком диапазоне температур. Установлено, что пленки однофазны, обладают структурой тетрагональной вольфрамовой бронзы, имеют ярко выраженную аксиальную текстуру с осью 001, направленной перпендикулярно поверхности подложки. Показано, что в интервале температур 300-425 K в материале пленки происходит размытый фазовый переход в состояние сегнетоэлектрика-релаксора. Обсуждаются возможные причины выявленных закономерностей. Работа выполнена в рамках реализации государственного задания на 2016 г N 007-01114-16 ПР (проект N 0256-2014-0002) и гранта РФФИ N 16-32-60095 мол{\\textbackslash}\\_а{\\textbackslash}\\_дк. DOI: 10.21883/FTT.2017.05.44376.382},\n\tlanguage = {ru},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Павленко, А.В. and Захарченко, И.Н. and Анохин, А.С. and Куприна, Ю.А. and Киселева, Л.И and Юзюк, Ю.И.},\n\tyear = {2017},\n\tpages = {888},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\BGRS77V9\\\\Павленко и др. - 2017 - Структура, динамика решетки и диэлектрические хара.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Методом высокочастотного напыления в атмосфере кислорода получены пленки твердого раствора Sr 0.5 Ba 0.5 Nb 2 O 6 на подложке (111)Pt/(001)Si. Изучены их деполяризованные спектры комбинационного рассеяния света, структура и диэлектрические характеристики в широком диапазоне температур. Установлено, что пленки однофазны, обладают структурой тетрагональной вольфрамовой бронзы, имеют ярко выраженную аксиальную текстуру с осью 001, направленной перпендикулярно поверхности подложки. Показано, что в интервале температур 300-425 K в материале пленки происходит размытый фазовый переход в состояние сегнетоэлектрика-релаксора. Обсуждаются возможные причины выявленных закономерностей. Работа выполнена в рамках реализации государственного задания на 2016 г N 007-01114-16 ПР (проект N 0256-2014-0002) и гранта РФФИ N 16-32-60095 мол\\_а\\_дк. DOI: 10.21883/FTT.2017.05.44376.382\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----pbmgtextrm13nbtextrm23otextrm3si001-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=29946411\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----pbmgtextrm13nbtextrm23otextrm3si001-2017', 'https://elibrary.ru/item.asp?id=29946411', event);\">\n    Получение, структура и диэлектрические свойства керамики и тонких поликристаллических пленок PbMg$_{\\textrm{1/3}}$Nb$_{\\textrm{2/3}}$O$_{\\textrm{3}}$ на подложке Si(001).\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Павленко, А. В.; Лянгузов, Н. В.; Новиковский, Н. В.; Смотраков, В. Г.;  and Ковтун, А. П.\n</span>\n\n  \n\n</span>\n\n  <i>Наука Юга России</i>, 13(3): 27–33.  2017.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=29946411\"\n     onclick=\"log_download('-----pbmgtextrm13nbtextrm23otextrm3si001-2017', 'https://elibrary.ru/item.asp?id=29946411', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Получение, структура и диэлектрические свойства керамики и тонких поликристаллических пленок PbMg$_{\\textrm{1/3}}$Nb$_{\\textrm{2/3}}$O$_{\\textrm{3}}$ на подложке Si(001) [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.23885/2500-0640-2017-13-3-27-33\"\n     onclick=\"log_download('-----pbmgtextrm13nbtextrm23otextrm3si001-2017', 'http://doi.org/10.23885/2500-0640-2017-13-3-27-33', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----pbmgtextrm13nbtextrm23otextrm3si001-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----pbmgtextrm13nbtextrm23otextrm3si001-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2017-8,\n\ttitle = {Получение, структура и диэлектрические свойства керамики и тонких поликристаллических пленок {PbMg}$_{\\textrm{1/3}}${Nb}$_{\\textrm{2/3}}${O}$_{\\textrm{3}}$ на подложке {Si}(001)},\n\tvolume = {13},\n\tissn = {2500-0640},\n\turl = {https://elibrary.ru/item.asp?id=29946411},\n\tdoi = {10.23885/2500-0640-2017-13-3-27-33},\n\tabstract = {Методом газоразрядного RF-напыления в атмосфере чистого кислорода осуществлено напыление пленок сегнетоэлектрика-релаксора PbMg1/3Nb2/3O3 (PMN) на подложки (001)Si (p-тип). PMN-пленки являются поликристаллическими с параметрами ячейки, близкими к объемному материалу PMN. Следов примесных фаз в обоих объектах не выявлено. Количественный анализ характеристического рентгеновского спектра образцов показал, что соотношение катионного состава по Pb и Nb в пленке соответствует составу распыляемой мишени. Проведены измерения температурно-частотных зависимостей относительной диэлектрической проницаемости (ε/ε0) и тангенса угла диэлектрических потерь (tg δ) керамики PMN. При комнатной температуре керамике свойственны высокие значения ε/ε0 ≈ 5500 и низкие tg δ ≈ 0,02, при этом дисперсия ε/ε0 в исследуемом диапазоне f отсутствовала, а температура Бёрнса составила ≈300 °С. При электронно-микроскопическом исследовании поверхности и скола гетероструктуры PMN/Si установлено, что пленка однофазная, поликристаллическая с характерным размером кристаллитов 50... 70 нм, при этом следов присутствия переходного слоя оксида кремния на границе раздела пленка - подложка не выявлено. Проведены исследования вольт-фарадных характеристик гетероструктуры PMN/Si. Обсуждаются причины выявленных аномалий.},\n\tlanguage = {ru},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Наука Юга России},\n\tauthor = {Павленко, А. В. and Лянгузов, Н. В. and Новиковский, Н. В. and Смотраков, В. Г. and Ковтун, А. П.},\n\tyear = {2017},\n\tkeywords = {Диэлектрическая Проницаемость, Магнониобат Свинца, Релаксор, Тонкие Пленки},\n\tpages = {27--33},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\K4J6BNEW\\\\Павленко и др. - 2017 - ПОЛУЧЕНИЕ, СТРУКТУРА И ДИЭЛЕКТРИЧЕСКИЕ СВОЙСТВА КЕ.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Методом газоразрядного RF-напыления в атмосфере чистого кислорода осуществлено напыление пленок сегнетоэлектрика-релаксора PbMg1/3Nb2/3O3 (PMN) на подложки (001)Si (p-тип). PMN-пленки являются поликристаллическими с параметрами ячейки, близкими к объемному материалу PMN. Следов примесных фаз в обоих объектах не выявлено. Количественный анализ характеристического рентгеновского спектра образцов показал, что соотношение катионного состава по Pb и Nb в пленке соответствует составу распыляемой мишени. Проведены измерения температурно-частотных зависимостей относительной диэлектрической проницаемости (ε/ε0) и тангенса угла диэлектрических потерь (tg δ) керамики PMN. При комнатной температуре керамике свойственны высокие значения ε/ε0 ≈ 5500 и низкие tg δ ≈ 0,02, при этом дисперсия ε/ε0 в исследуемом диапазоне f отсутствовала, а температура Бёрнса составила ≈300 °С. При электронно-микроскопическом исследовании поверхности и скола гетероструктуры PMN/Si установлено, что пленка однофазная, поликристаллическая с характерным размером кристаллитов 50... 70 нм, при этом следов присутствия переходного слоя оксида кремния на границе раздела пленка - подложка не выявлено. Проведены исследования вольт-фарадных характеристик гетероструктуры PMN/Si. Обсуждаются причины выявленных аномалий.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---batiotextrm3srtiotextrm3-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=29647718\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---batiotextrm3srtiotextrm3-2017', 'https://elibrary.ru/item.asp?id=29647718', event);\">\n    Особенности фазового перехода в сегнетоэлектрической сверхрешетке BaTiO$_{\\textrm{3}}$/SrTiO$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Разумная, А. Г.; Горьковая, Е. Д.;  and Тихонов, Ю. А.\n</span>\n\n  \n\n</span>\n\n  In  2017. Российский государственный педагогический университет им. А. И. Герцена\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=29647718\"\n     onclick=\"log_download('---batiotextrm3srtiotextrm3-2017', 'https://elibrary.ru/item.asp?id=29647718', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Особенности фазового перехода в сегнетоэлектрической сверхрешетке BaTiO$_{\\textrm{3}}$/SrTiO$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---batiotextrm3srtiotextrm3-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---batiotextrm3srtiotextrm3-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{__2017-9,\n\ttitle = {Особенности фазового перехода в сегнетоэлектрической сверхрешетке {BaTiO}$_{\\textrm{3}}$/{SrTiO}$_{\\textrm{3}}$},\n\turl = {https://elibrary.ru/item.asp?id=29647718},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tpublisher = {Российский государственный педагогический университет им. А. И. Герцена},\n\tauthor = {Разумная, А. Г. and Горьковая, Е. Д. and Тихонов, Ю. А.},\n\tyear = {2017},\n\tkeywords = {⛔ No DOI found},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----bsn50-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=29401602\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----bsn50-2017', 'https://elibrary.ru/item.asp?id=29401602', event);\">\n    Оптические Свойства Тонких Пленок BSn50.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Широков, В. Б.; Павленко, А. В.; Михейкин, А. С.; Изюмский, К. С.;  and Ревинский, Ю. В.\n</span>\n\n  \n\n</span>\n\n  In  2017. Российский государственный педагогический университет им. А. И. Герцена\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=29401602\"\n     onclick=\"log_download('-----bsn50-2017', 'https://elibrary.ru/item.asp?id=29401602', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Оптические Свойства Тонких Пленок BSn50 [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----bsn50-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----bsn50-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{__2017-10,\n\ttitle = {Оптические Свойства Тонких Пленок {BSn50}},\n\turl = {https://elibrary.ru/item.asp?id=29401602},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tpublisher = {Российский государственный педагогический университет им. А. И. Герцена},\n\tauthor = {Широков, В. Б. and Павленко, А. В. and Михейкин, А. С. and Изюмский, К. С. and Ревинский, Ю. В.},\n\tyear = {2017},\n\tkeywords = {⛔ No DOI found},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=29647696\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----2017', 'https://elibrary.ru/item.asp?id=29647696', event);\">\n    Многослойные структуры мультиферроик-сегнетоэлектрик: КРС исследования.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Анохин, А. С.; Разумная, А. Г.; Головко, Ю. И.;  and Мухортов, В. М.\n</span>\n\n  \n\n</span>\n\n  In  2017. Российский государственный педагогический университет им. А. И. Герцена\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=29647696\"\n     onclick=\"log_download('-----2017', 'https://elibrary.ru/item.asp?id=29647696', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Многослойные структуры мультиферроик-сегнетоэлектрик: КРС исследования [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{__2017-11,\n\ttitle = {Многослойные структуры мультиферроик-сегнетоэлектрик: КРС исследования},\n\tshorttitle = {Многослойные Структуры Мультиферроик-Сегнетоэлектрик},\n\turl = {https://elibrary.ru/item.asp?id=29647696},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tpublisher = {Российский государственный педагогический университет им. А. И. Герцена},\n\tauthor = {Анохин, А. С. and Разумная, А. Г. and Головко, Ю. И. and Мухортов, В. М.},\n\tyear = {2017},\n\tkeywords = {⛔ No DOI found},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------lsmogeotextrm2-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=29647737\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------lsmogeotextrm2-2017', 'https://elibrary.ru/item.asp?id=29647737', event);\">\n    Магнитодиэлектрические свойства керамики LSMO/GeO$_{\\textrm{2}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Кабиров, Ю. В.; Гавриляченко, В. Г.; Богатин, А. С.; Яценко, В. К.; Пруцакова, Н. В.;  and Чебанова, Е. В.\n</span>\n\n  \n\n</span>\n\n  In  2017. Российский государственный педагогический университет им. А. И. Герцена\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=29647737\"\n     onclick=\"log_download('------lsmogeotextrm2-2017', 'https://elibrary.ru/item.asp?id=29647737', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Магнитодиэлектрические свойства керамики LSMO/GeO$_{\\textrm{2}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------lsmogeotextrm2-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------lsmogeotextrm2-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{__2017-12,\n\ttitle = {Магнитодиэлектрические свойства керамики {LSMO}/{GeO}$_{\\textrm{2}}$},\n\turl = {https://elibrary.ru/item.asp?id=29647737},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tpublisher = {Российский государственный педагогический университет им. А. И. Герцена},\n\tauthor = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Богатин, А. С. and Яценко, В. К. and Пруцакова, Н. В. and Чебанова, Е. В.},\n\tyear = {2017},\n\tkeywords = {⛔ No DOI found},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---ii300700-2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=29760083\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---ii300700-2017', 'https://elibrary.ru/item.asp?id=29760083', event);\">\n    Динамика решетки в пленках ниобата бария-стронция <i>Т </i>= 300-700 К.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Анохин, А. С.; Лянгузов, Н. В.;  and Павленко, А. В.\n</span>\n\n  \n\n</span>\n\n  <i>Наука Юга России</i>, 13(2): 21–28.  2017.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=29760083\"\n     onclick=\"log_download('---ii300700-2017', 'https://elibrary.ru/item.asp?id=29760083', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Динамика решетки в пленках ниобата бария-стронция &lt;i&gt;Т &lt;/i&gt;= 300-700 К [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.23885/2500-0640-2017-13-2-21-28\"\n     onclick=\"log_download('---ii300700-2017', 'http://doi.org/10.23885/2500-0640-2017-13-2-21-28', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---ii300700-2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---ii300700-2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2017-13,\n\ttitle = {Динамика решетки в пленках ниобата бария-стронция \\textit{Т }= 300-700 К},\n\tvolume = {13},\n\tissn = {2500-0640},\n\turl = {https://elibrary.ru/item.asp?id=29760083},\n\tdoi = {10.23885/2500-0640-2017-13-2-21-28},\n\tabstract = {Методом газоразрядного RF-напыления в атмосфере чистого кислорода осуществлено напыление пленки твердого раствора сегнетоэлектрика-релаксора Ba0,5Sr0,5Nb2O6 (BSN-50) на предварительно подготовленную подложку (111)Pt/(001)Si. Пленке BSN-50 свойственна аксиальная текстура, основные элементы (Ba, Sr, Nb) по ее толщине распределены равномерно, а количественный анализ характеристического рентгеновского спектра показал, что соотношение катионного состава соответствует составу BSN-50. При исследовании температурных зависимостей относительной диэлектрической проницаемости (ε′/ε0) и остаточной поляризации (PR) гетероструктуры Al/BSN-50/Pt/Si установлено, что фазовый переход из сегнетоэлектрической в параэлектрическую фазу достаточно сильно размыт (ширина максимума ε′/ε0(Тm) на полувысоте ΔT = 263 K) и происходит при температуре {\\textasciitilde}427 К, намного превышающей температуру максимума диэлектрической проницаемости Tm = 334 K...\n\nМетодом газоразрядного RF-напыления в атмосфере чистого кислорода осуществлено напыление пленки твердого раствора сегнетоэлектрика-релаксора Ba0,5Sr0,5Nb2O6 (BSN-50) на предварительно подготовленную подложку (111)Pt/(001)Si. Пленке BSN-50 свойственна аксиальная текстура, основные элементы (Ba, Sr, Nb) по ее толщине распределены равномерно, а количественный анализ характеристического рентгеновского спектра показал, что соотношение катионного состава соответствует составу BSN-50. При исследовании температурных зависимостей относительной диэлектрической проницаемости (ε′/ε0) и остаточной поляризации (PR) гетероструктуры Al/BSN-50/Pt/Si установлено, что фазовый переход из сегнетоэлектрической в параэлектрическую фазу достаточно сильно размыт (ширина максимума ε′/ε0(Тm) на полувысоте ΔT = 263 K) и происходит при температуре {\\textasciitilde}427 К, намного превышающей температуру максимума диэлектрической проницаемости Tm = 334 K. В диапазоне температур 300-700 K методом спектроскопии комбинационного рассеяния света изучена динамика решетки пленки BSN-50. Наибольший вклад в интенсивность спектра пленки BSN вносят три широкие полосы в районе 230 cm-1, 630 cm-1 и 850 cm-1, каждая из которых состоит из набора линий (всего 13 мод). Температурная зависимость частоты и полуширины полосы 630 cm-1 в спектре комбинационного рассеяния пленки BSN показывают четкую аномалию при сегнетоэлектрическом фазовом переходе.},\n\tlanguage = {ru},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Наука Юга России},\n\tauthor = {Анохин, А. С. and Лянгузов, Н. В. and Павленко, А. В.},\n\tyear = {2017},\n\tkeywords = {Диэлектрическая Проницаемость, Пленки, Спектроскопия Крс},\n\tpages = {21--28},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\TM7MF7DI\\\\Анохин и др. - 2017 - ДИНАМИКА РЕШЕТКИ В ПЛЕНКАХ НИОБАТА БАРИЯ - СТРОНЦИ.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Методом газоразрядного RF-напыления в атмосфере чистого кислорода осуществлено напыление пленки твердого раствора сегнетоэлектрика-релаксора Ba0,5Sr0,5Nb2O6 (BSN-50) на предварительно подготовленную подложку (111)Pt/(001)Si. Пленке BSN-50 свойственна аксиальная текстура, основные элементы (Ba, Sr, Nb) по ее толщине распределены равномерно, а количественный анализ характеристического рентгеновского спектра показал, что соотношение катионного состава соответствует составу BSN-50. При исследовании температурных зависимостей относительной диэлектрической проницаемости (ε′/ε0) и остаточной поляризации (PR) гетероструктуры Al/BSN-50/Pt/Si установлено, что фазовый переход из сегнетоэлектрической в параэлектрическую фазу достаточно сильно размыт (ширина максимума ε′/ε0(Тm) на полувысоте ΔT = 263 K) и происходит при температуре ~427 К, намного превышающей температуру максимума диэлектрической проницаемости Tm = 334 K... Методом газоразрядного RF-напыления в атмосфере чистого кислорода осуществлено напыление пленки твердого раствора сегнетоэлектрика-релаксора Ba0,5Sr0,5Nb2O6 (BSN-50) на предварительно подготовленную подложку (111)Pt/(001)Si. Пленке BSN-50 свойственна аксиальная текстура, основные элементы (Ba, Sr, Nb) по ее толщине распределены равномерно, а количественный анализ характеристического рентгеновского спектра показал, что соотношение катионного состава соответствует составу BSN-50. При исследовании температурных зависимостей относительной диэлектрической проницаемости (ε′/ε0) и остаточной поляризации (PR) гетероструктуры Al/BSN-50/Pt/Si установлено, что фазовый переход из сегнетоэлектрической в параэлектрическую фазу достаточно сильно размыт (ширина максимума ε′/ε0(Тm) на полувысоте ΔT = 263 K) и происходит при температуре ~427 К, намного превышающей температуру максимума диэлектрической проницаемости Tm = 334 K. В диапазоне температур 300-700 K методом спектроскопии комбинационного рассеяния света изучена динамика решетки пленки BSN-50. Наибольший вклад в интенсивность спектра пленки BSN вносят три широкие полосы в районе 230 cm-1, 630 cm-1 и 850 cm-1, каждая из которых состоит из набора линий (всего 13 мод). Температурная зависимость частоты и полуширины полосы 630 cm-1 в спектре комбинационного рассеяния пленки BSN показывают четкую аномалию при сегнетоэлектрическом фазовом переходе.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----2017\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/44377\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----2017', 'https://journals.ioffe.ru/articles/44377', event);\">\n    Вынужденный пироэффект в планарном поле.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Широков, В.; Разумная, А.;  and Юзюк, Ю.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 59(5): 892.  2017.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/44377\"\n     onclick=\"log_download('----2017', 'https://journals.ioffe.ru/articles/44377', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Вынужденный пироэффект в планарном поле [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.21883/FTT.2017.05.44377.397\"\n     onclick=\"log_download('----2017', 'http://doi.org/10.21883/FTT.2017.05.44377.397', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----2017\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>8 downloads</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----2017')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2017-14,\n\ttitle = {Вынужденный пироэффект в планарном поле},\n\tvolume = {59},\n\tissn = {0367-3294},\n\turl = {https://journals.ioffe.ru/articles/44377},\n\tdoi = {10.21883/FTT.2017.05.44377.397},\n\tabstract = {Исследованы действие вынужденной деформации и влияние планарного электрического поля на основное состояние сегнетоэлектрических тонких пленок Ba0.7Sr0.3O3, осажденных на (001)-ориентированные кубические подложки. Для значений вынужденной деформации, соответствующих различным основным состояниям, построена зависимость пироэлектрического коэффициента от величины электрического поля Ex в плоскости пленки. В областях, где пленка может работать в режиме диэлектрического болометра, наблюдается значение поля, при котором пирокоэффициент достигает экстремального значения. Существует значение вынужденной деформации, при котором пироэффект проявляется наиболее ярко. Работа выполнена за счет средств Российского научного фонда (грант N 14-12-00258). DOI: 10.21883/FTT.2017.05.44377.397},\n\tlanguage = {ru},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Широков, В.Б. and Разумная, А.Г. and Юзюк, Ю.И.},\n\tyear = {2017},\n\tpages = {892},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\WFDZMDZ3\\\\Широков и др. - 2017 - Вынужденный пироэффект в планарном поле.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследованы действие вынужденной деформации и влияние планарного электрического поля на основное состояние сегнетоэлектрических тонких пленок Ba0.7Sr0.3O3, осажденных на (001)-ориентированные кубические подложки. Для значений вынужденной деформации, соответствующих различным основным состояниям, построена зависимость пироэлектрического коэффициента от величины электрического поля Ex в плоскости пленки. В областях, где пленка может работать в режиме диэлектрического болометра, наблюдается значение поля, при котором пирокоэффициент достигает экстремального значения. Существует значение вынужденной деформации, при котором пироэффект проявляется наиболее ярко. Работа выполнена за счет средств Российского научного фонда (грант N 14-12-00258). DOI: 10.21883/FTT.2017.05.44377.397\n</div>\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2016\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2016')\"\n      onkeypress=\"toggleGroup('group_2016')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2016</span>\n      <span class=\"bibbase_group_count\">\n        \n        (44)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"gya-dneprovsky-kaidashev-investigationofthewirelessreadingfromsignalpassivesawsensorswithreflectiveinterdigitaltransducers-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=43958874\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'gya-dneprovsky-kaidashev-investigationofthewirelessreadingfromsignalpassivesawsensorswithreflectiveinterdigitaltransducers-2016', 'https://elibrary.ru/item.asp?id=43958874', event);\">\n    Investigation of the Wireless Reading from Signal Passive SAW Sensors with Reflective Interdigital Transducers.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  G.ya., K.; Dneprovsky, V. G.;  and Kaidashev, E. M.\n</span>\n\n  \n\n</span>\n\n  .  2016.\n  <span class=\"note\">Publisher: Южный федеральный университет</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=43958874\"\n     onclick=\"log_download('gya-dneprovsky-kaidashev-investigationofthewirelessreadingfromsignalpassivesawsensorswithreflectiveinterdigitaltransducers-2016', 'https://elibrary.ru/item.asp?id=43958874', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Investigation of the Wireless Reading from Signal Passive SAW Sensors with Reflective Interdigital Transducers [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/gya-dneprovsky-kaidashev-investigationofthewirelessreadingfromsignalpassivesawsensorswithreflectiveinterdigitaltransducers-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('gya-dneprovsky-kaidashev-investigationofthewirelessreadingfromsignalpassivesawsensorswithreflectiveinterdigitaltransducers-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{karapetyan_gya_investigation_2016,\n\ttitle = {Investigation of the {Wireless} {Reading} from {Signal} {Passive} {SAW} {Sensors} with {Reflective} {Interdigital} {Transducers}},\n\turl = {https://elibrary.ru/item.asp?id=43958874},\n\tlanguage = {en},\n\turldate = {2023-11-11},\n\tauthor = {Karapetyan G.ya. and Dneprovsky, V. G. and Kaidashev, E. M.},\n\tyear = {2016},\n\tnote = {Publisher: Южный федеральный университет},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"nikolaev-kazmina-minasyan-kaidashev-gya-kaidashev-designofconstructionelementsforpiezoelectricresonatorsandchemisensorsbasedonzincoxidenanorods-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=44011645\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'nikolaev-kazmina-minasyan-kaidashev-gya-kaidashev-designofconstructionelementsforpiezoelectricresonatorsandchemisensorsbasedonzincoxidenanorods-2016', 'https://elibrary.ru/item.asp?id=44011645', event);\">\n    Design of Construction Elements for Piezoelectric Resonators and Chemisensors Based on Zinc Oxide Nanorods.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Nikolaev, A. L.; Kazmina, M. A.; Minasyan, T. A.; Kaidashev, V. E.; G.ya., K.;  and Kaidashev, E. M.\n</span>\n\n  \n\n</span>\n\n  .  2016.\n  <span class=\"note\">Publisher: Южный федеральный университет</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=44011645\"\n     onclick=\"log_download('nikolaev-kazmina-minasyan-kaidashev-gya-kaidashev-designofconstructionelementsforpiezoelectricresonatorsandchemisensorsbasedonzincoxidenanorods-2016', 'https://elibrary.ru/item.asp?id=44011645', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Design of Construction Elements for Piezoelectric Resonators and Chemisensors Based on Zinc Oxide Nanorods [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/nikolaev-kazmina-minasyan-kaidashev-gya-kaidashev-designofconstructionelementsforpiezoelectricresonatorsandchemisensorsbasedonzincoxidenanorods-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('nikolaev-kazmina-minasyan-kaidashev-gya-kaidashev-designofconstructionelementsforpiezoelectricresonatorsandchemisensorsbasedonzincoxidenanorods-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{nikolaev_design_2016,\n\ttitle = {Design of {Construction} {Elements} for {Piezoelectric} {Resonators} and {Chemisensors} {Based} on {Zinc} {Oxide} {Nanorods}},\n\turl = {https://elibrary.ru/item.asp?id=44011645},\n\tlanguage = {en},\n\turldate = {2023-11-11},\n\tauthor = {Nikolaev, A. L. and Kazmina, M. A. and Minasyan, T. A. and Kaidashev, V. E. and Karapetyan G.ya. and Kaidashev, E. M.},\n\tyear = {2016},\n\tnote = {Publisher: Южный федеральный университет},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"lerer-timoshenko-golovacheva-kaidashev-refractivepropertiesofnanorodtype2dphotoniccrystals-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=43962934\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'lerer-timoshenko-golovacheva-kaidashev-refractivepropertiesofnanorodtype2dphotoniccrystals-2016', 'https://elibrary.ru/item.asp?id=43962934', event);\">\n    Refractive Properties of Nanorod-Type 2D Photonic Crystals.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Lerer, A. M.; Timoshenko, P. E.; Golovacheva, E. V.;  and Kaidashev, E. M.\n</span>\n\n  \n\n</span>\n\n  .  2016.\n  <span class=\"note\">Publisher: Южный федеральный университет</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=43962934\"\n     onclick=\"log_download('lerer-timoshenko-golovacheva-kaidashev-refractivepropertiesofnanorodtype2dphotoniccrystals-2016', 'https://elibrary.ru/item.asp?id=43962934', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Refractive Properties of Nanorod-Type 2D Photonic Crystals [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/lerer-timoshenko-golovacheva-kaidashev-refractivepropertiesofnanorodtype2dphotoniccrystals-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('lerer-timoshenko-golovacheva-kaidashev-refractivepropertiesofnanorodtype2dphotoniccrystals-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{lerer_refractive_2016,\n\ttitle = {Refractive {Properties} of {Nanorod}-{Type} {2D} {Photonic} {Crystals}},\n\turl = {https://elibrary.ru/item.asp?id=43962934},\n\tlanguage = {en},\n\turldate = {2023-11-11},\n\tauthor = {Lerer, A. M. and Timoshenko, P. E. and Golovacheva, E. V. and Kaidashev, E. M.},\n\tyear = {2016},\n\tnote = {Publisher: Южный федеральный университет},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"zhukova-mikheykin-torgashev-bush-yuzyuk-sashin-prokhorov-dressel-etal-crucialinfluenceofcrystalsitedisorderondynamicalspectralresponseinartificialmagnetoplumbites-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S1293255816305465\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'zhukova-mikheykin-torgashev-bush-yuzyuk-sashin-prokhorov-dressel-etal-crucialinfluenceofcrystalsitedisorderondynamicalspectralresponseinartificialmagnetoplumbites-2016', 'https://www.sciencedirect.com/science/article/pii/S1293255816305465', event);\">\n    Crucial influence of crystal site disorder on dynamical spectral response in artificial magnetoplumbites.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Zhukova, E. S.; Mikheykin, A. S.; Torgashev, V. I.; Bush, A. A.; Yuzyuk, Y. I.; Sashin, A. E.; Prokhorov, A. S.; Dressel, M.;  and Gorshunov, B. P.\n</span>\n\n  \n\n</span>\n\n  <i>Solid State Sciences</i>, 62: 13–21. December 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S1293255816305465\"\n     onclick=\"log_download('zhukova-mikheykin-torgashev-bush-yuzyuk-sashin-prokhorov-dressel-etal-crucialinfluenceofcrystalsitedisorderondynamicalspectralresponseinartificialmagnetoplumbites-2016', 'https://www.sciencedirect.com/science/article/pii/S1293255816305465', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Crucial influence of crystal site disorder on dynamical spectral response in artificial magnetoplumbites [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.solidstatesciences.2016.10.012\"\n     onclick=\"log_download('zhukova-mikheykin-torgashev-bush-yuzyuk-sashin-prokhorov-dressel-etal-crucialinfluenceofcrystalsitedisorderondynamicalspectralresponseinartificialmagnetoplumbites-2016', 'http://doi.org/10.1016/j.solidstatesciences.2016.10.012', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/zhukova-mikheykin-torgashev-bush-yuzyuk-sashin-prokhorov-dressel-etal-crucialinfluenceofcrystalsitedisorderondynamicalspectralresponseinartificialmagnetoplumbites-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('zhukova-mikheykin-torgashev-bush-yuzyuk-sashin-prokhorov-dressel-etal-crucialinfluenceofcrystalsitedisorderondynamicalspectralresponseinartificialmagnetoplumbites-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{zhukova_crucial_2016,\n\ttitle = {Crucial influence of crystal site disorder on dynamical spectral response in artificial magnetoplumbites},\n\tvolume = {62},\n\tissn = {1293-2558},\n\turl = {https://www.sciencedirect.com/science/article/pii/S1293255816305465},\n\tdoi = {10.1016/j.solidstatesciences.2016.10.012},\n\tabstract = {High quality PbFe12O19 single crystals were grown by a solution-melt crystallization technique and characterized by synchrotron radiation diffraction structural studies, Mössbauer, Raman and infrared spectral measurements. In the terahertz and sub-terahertz range two absorption bands are observed, which are associated with the dynamics of structurally disordered lead and iron ions. We develop a structural model that comprises Fe2+ ions at the (1/2 × 4e) (0, 0, z) position with bipyramidal oxygen environment, and Pb ions at the (24l) (x, y, z) position with generic strongly distorted 12 vertex polyhedron of oxygen. The atomic displacement ellipsoids of the oxygen surrounding the lead ion are stretched towards the Pb ion within the plane perpendicular to the hexagonal axis. The suggested model is in full agreement with the local symmetry of the Fe2 and Pb ions and with the chemical composition of the sample determined by X-ray analysis.},\n\turldate = {2023-11-11},\n\tjournal = {Solid State Sciences},\n\tauthor = {Zhukova, E. S. and Mikheykin, A. S. and Torgashev, V. I. and Bush, A. A. and Yuzyuk, Yu. I. and Sashin, A. E. and Prokhorov, A. S. and Dressel, M. and Gorshunov, B. P.},\n\tmonth = dec,\n\tyear = {2016},\n\tkeywords = {X-ray diffraction, Hexaferrites, Magnetoplumbite, Single crystal, Terahertz-infrared spectroscopy},\n\tpages = {13--21},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  High quality PbFe12O19 single crystals were grown by a solution-melt crystallization technique and characterized by synchrotron radiation diffraction structural studies, Mössbauer, Raman and infrared spectral measurements. In the terahertz and sub-terahertz range two absorption bands are observed, which are associated with the dynamics of structurally disordered lead and iron ions. We develop a structural model that comprises Fe2+ ions at the (1/2 × 4e) (0, 0, z) position with bipyramidal oxygen environment, and Pb ions at the (24l) (x, y, z) position with generic strongly distorted 12 vertex polyhedron of oxygen. The atomic displacement ellipsoids of the oxygen surrounding the lead ion are stretched towards the Pb ion within the plane perpendicular to the hexagonal axis. The suggested model is in full agreement with the local symmetry of the Fe2 and Pb ions and with the chemical composition of the sample determined by X-ray analysis.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"roshal-konevtsova-myasnikova-rochal-assemblyofthemosttopologicallyregulartwodimensionalmicroandnanocrystalswithsphericalconicalandtubularshapes-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevE.94.052605\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'roshal-konevtsova-myasnikova-rochal-assemblyofthemosttopologicallyregulartwodimensionalmicroandnanocrystalswithsphericalconicalandtubularshapes-2016', 'https://link.aps.org/doi/10.1103/PhysRevE.94.052605', event);\">\n    Assembly of the most topologically regular two-dimensional micro and nanocrystals with spherical, conical, and tubular shapes.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Roshal, D. S.; Konevtsova, O. V.; Myasnikova, A. E.;  and Rochal, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review E</i>, 94(5): 052605. November 2016.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevE.94.052605\"\n     onclick=\"log_download('roshal-konevtsova-myasnikova-rochal-assemblyofthemosttopologicallyregulartwodimensionalmicroandnanocrystalswithsphericalconicalandtubularshapes-2016', 'https://link.aps.org/doi/10.1103/PhysRevE.94.052605', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Assembly of the most topologically regular two-dimensional micro and nanocrystals with spherical, conical, and tubular shapes [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevE.94.052605\"\n     onclick=\"log_download('roshal-konevtsova-myasnikova-rochal-assemblyofthemosttopologicallyregulartwodimensionalmicroandnanocrystalswithsphericalconicalandtubularshapes-2016', 'http://doi.org/10.1103/PhysRevE.94.052605', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/roshal-konevtsova-myasnikova-rochal-assemblyofthemosttopologicallyregulartwodimensionalmicroandnanocrystalswithsphericalconicalandtubularshapes-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('roshal-konevtsova-myasnikova-rochal-assemblyofthemosttopologicallyregulartwodimensionalmicroandnanocrystalswithsphericalconicalandtubularshapes-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{roshal_assembly_2016,\n\ttitle = {Assembly of the most topologically regular two-dimensional micro and nanocrystals with spherical, conical, and tubular shapes},\n\tvolume = {94},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevE.94.052605},\n\tdoi = {10.1103/PhysRevE.94.052605},\n\tabstract = {We consider how to control the extension of curvature-induced defects in the hexagonal order covering different curved surfaces. In these frames we propose a physical mechanism for improving structures of two-dimensional spherical colloidal crystals (SCCs). For any SCC comprising of about 300 or less particles the mechanism transforms all extended topological defects (ETDs) in the hexagonal order into the point disclinations. Perfecting the structure is carried out by successive cycles of the particle implantation and subsequent relaxation of the crystal. The mechanism is potentially suitable for obtaining colloidosomes with better selective permeability. Our approach enables modeling the most topologically regular tubular and conical two-dimensional nanocrystals including various possible polymorphic forms of the HIV viral capsid. Different HIV-like shells with an arbitrary number of structural units (SUs) and desired geometrical parameters are easily formed. Faceting of the obtained structures is performed by minimizing the suggested elastic energy.},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review E},\n\tauthor = {Roshal, D. S. and Konevtsova, O. V. and Myasnikova, A. E. and Rochal, S. B.},\n\tmonth = nov,\n\tyear = {2016},\n\tnote = {Publisher: American Physical Society},\n\tpages = {052605},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We consider how to control the extension of curvature-induced defects in the hexagonal order covering different curved surfaces. In these frames we propose a physical mechanism for improving structures of two-dimensional spherical colloidal crystals (SCCs). For any SCC comprising of about 300 or less particles the mechanism transforms all extended topological defects (ETDs) in the hexagonal order into the point disclinations. Perfecting the structure is carried out by successive cycles of the particle implantation and subsequent relaxation of the crystal. The mechanism is potentially suitable for obtaining colloidosomes with better selective permeability. Our approach enables modeling the most topologically regular tubular and conical two-dimensional nanocrystals including various possible polymorphic forms of the HIV viral capsid. Different HIV-like shells with an arbitrary number of structural units (SUs) and desired geometrical parameters are easily formed. Faceting of the obtained structures is performed by minimizing the suggested elastic energy.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"tonkikh-rybkovskiy-orekhov-chernov-khomich-ewels-kauppinen-rochal-etal-opticalpropertiesandchargetransfereffectsinsinglewalledcarbonnanotubesfilledwithfunctionalizedadamantanemolecules-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0008622316306261\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'tonkikh-rybkovskiy-orekhov-chernov-khomich-ewels-kauppinen-rochal-etal-opticalpropertiesandchargetransfereffectsinsinglewalledcarbonnanotubesfilledwithfunctionalizedadamantanemolecules-2016', 'https://www.sciencedirect.com/science/article/pii/S0008622316306261', event);\">\n    Optical properties and charge transfer effects in single-walled carbon nanotubes filled with functionalized adamantane molecules.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Tonkikh, A. A.; Rybkovskiy, D. V.; Orekhov, A. S.; Chernov, A. I.; Khomich, A. A.; Ewels, C. P.; Kauppinen, E. I.; Rochal, S. B.; Chuvilin, A. L.;  and Obraztsova, E. D.\n</span>\n\n  \n\n</span>\n\n  <i>Carbon</i>, 109: 87–97. November 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0008622316306261\"\n     onclick=\"log_download('tonkikh-rybkovskiy-orekhov-chernov-khomich-ewels-kauppinen-rochal-etal-opticalpropertiesandchargetransfereffectsinsinglewalledcarbonnanotubesfilledwithfunctionalizedadamantanemolecules-2016', 'https://www.sciencedirect.com/science/article/pii/S0008622316306261', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Optical properties and charge transfer effects in single-walled carbon nanotubes filled with functionalized adamantane molecules [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.carbon.2016.07.053\"\n     onclick=\"log_download('tonkikh-rybkovskiy-orekhov-chernov-khomich-ewels-kauppinen-rochal-etal-opticalpropertiesandchargetransfereffectsinsinglewalledcarbonnanotubesfilledwithfunctionalizedadamantanemolecules-2016', 'http://doi.org/10.1016/j.carbon.2016.07.053', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/tonkikh-rybkovskiy-orekhov-chernov-khomich-ewels-kauppinen-rochal-etal-opticalpropertiesandchargetransfereffectsinsinglewalledcarbonnanotubesfilledwithfunctionalizedadamantanemolecules-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('tonkikh-rybkovskiy-orekhov-chernov-khomich-ewels-kauppinen-rochal-etal-opticalpropertiesandchargetransfereffectsinsinglewalledcarbonnanotubesfilledwithfunctionalizedadamantanemolecules-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{tonkikh_optical_2016,\n\ttitle = {Optical properties and charge transfer effects in single-walled carbon nanotubes filled with functionalized adamantane molecules},\n\tvolume = {109},\n\tissn = {0008-6223},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0008622316306261},\n\tdoi = {10.1016/j.carbon.2016.07.053},\n\tabstract = {The filling of single-walled carbon nanotube films with 1-adamantanemethanol and 1-bromoadamantane molecules was carried out by a gas-phase procedure. Optical absorption and Raman spectroscopies revealed the effects of charge transfer for samples treated with 1-bromoadamantane. Using density functional simulations we show that the charge transfer takes place when bromine is detached from the carbon cage and accepts electrons as free-standing atoms or as polybromide structures. Transmission electron microscope images confirm the presence of individual bromine atoms inside carbon nanotubes, treated with 1-bromoadamantane molecules. The observed charge transfer is, therefore, a marker of the dehalogenization reaction, a critical step in the synthesis process of narrow 1D sp3 nanostructures.},\n\turldate = {2023-11-11},\n\tjournal = {Carbon},\n\tauthor = {Tonkikh, A. A. and Rybkovskiy, D. V. and Orekhov, A. S. and Chernov, A. I. and Khomich, A. A. and Ewels, C. P. and Kauppinen, E. I. and Rochal, S. B. and Chuvilin, A. L. and Obraztsova, E. D.},\n\tmonth = nov,\n\tyear = {2016},\n\tpages = {87--97},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The filling of single-walled carbon nanotube films with 1-adamantanemethanol and 1-bromoadamantane molecules was carried out by a gas-phase procedure. Optical absorption and Raman spectroscopies revealed the effects of charge transfer for samples treated with 1-bromoadamantane. Using density functional simulations we show that the charge transfer takes place when bromine is detached from the carbon cage and accepts electrons as free-standing atoms or as polybromide structures. Transmission electron microscope images confirm the presence of individual bromine atoms inside carbon nanotubes, treated with 1-bromoadamantane molecules. The observed charge transfer is, therefore, a marker of the dehalogenization reaction, a critical step in the synthesis process of narrow 1D sp3 nanostructures.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"andronikova-bronwald-burkovsky-leontiev-leontiev-bosak-filimonov-vakhrushev-pretransitionalevolutionofcentralpeaksandtransverseacousticphononbranchinsinglecrystalleadzirconatetitanatewithticoncentration07-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/769/1/012070\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'andronikova-bronwald-burkovsky-leontiev-leontiev-bosak-filimonov-vakhrushev-pretransitionalevolutionofcentralpeaksandtransverseacousticphononbranchinsinglecrystalleadzirconatetitanatewithticoncentration07-2016', 'https://dx.doi.org/10.1088/1742-6596/769/1/012070', event);\">\n    Pre-transitional evolution of central peaks and transverse acoustic phonon branch in single crystal lead zirconate titanate with Ti concentration 0.7%.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Andronikova, D. A.; Bronwald, I. A.; Burkovsky, R. G.; Leontiev, I. N.; Leontiev, N. G.; Bosak, A. A.; Filimonov, A. V.;  and Vakhrushev, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics: Conference Series</i>, 769(1): 012070. November 2016.\n  <span class=\"note\">Publisher: IOP Publishing</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/769/1/012070\"\n     onclick=\"log_download('andronikova-bronwald-burkovsky-leontiev-leontiev-bosak-filimonov-vakhrushev-pretransitionalevolutionofcentralpeaksandtransverseacousticphononbranchinsinglecrystalleadzirconatetitanatewithticoncentration07-2016', 'https://dx.doi.org/10.1088/1742-6596/769/1/012070', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Pre-transitional evolution of central peaks and transverse acoustic phonon branch in single crystal lead zirconate titanate with Ti concentration 0.7% [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/1742-6596/769/1/012070\"\n     onclick=\"log_download('andronikova-bronwald-burkovsky-leontiev-leontiev-bosak-filimonov-vakhrushev-pretransitionalevolutionofcentralpeaksandtransverseacousticphononbranchinsinglecrystalleadzirconatetitanatewithticoncentration07-2016', 'http://doi.org/10.1088/1742-6596/769/1/012070', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/andronikova-bronwald-burkovsky-leontiev-leontiev-bosak-filimonov-vakhrushev-pretransitionalevolutionofcentralpeaksandtransverseacousticphononbranchinsinglecrystalleadzirconatetitanatewithticoncentration07-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('andronikova-bronwald-burkovsky-leontiev-leontiev-bosak-filimonov-vakhrushev-pretransitionalevolutionofcentralpeaksandtransverseacousticphononbranchinsinglecrystalleadzirconatetitanatewithticoncentration07-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{andronikova_pre-transitional_2016,\n\ttitle = {Pre-transitional evolution of central peaks and transverse acoustic phonon branch in single crystal lead zirconate titanate with {Ti} concentration 0.7\\%},\n\tvolume = {769},\n\tissn = {1742-6596},\n\turl = {https://dx.doi.org/10.1088/1742-6596/769/1/012070},\n\tdoi = {10.1088/1742-6596/769/1/012070},\n\tabstract = {Inelastic X-ray scattering measurements have been done to study the lattice dynamics in lead zirconate titanate solid solution with 0.7\\% of PbTiO3. The temperature evolution of central peak and low-energy transverse phonon branches has been traced. Temperature dependent in-plane transverse polarized acoustic phonon branch in {\\textless}1 1 0{\\textgreater} direction has been revealed. The central peaks of two types have been found. The central peak at small wave vectors can be attributed to the relaxational-type soft ferroelectric mode, while the latter at Q = (1.5 -0.5 0) could be linked to the formation of M-superstructure in the intermediate ferroelectric phase.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics: Conference Series},\n\tauthor = {Andronikova, D. A. and Bronwald, I. A. and Burkovsky, R. G. and Leontiev, I. N. and Leontiev, N. G. and Bosak, A. A. and Filimonov, A. V. and Vakhrushev, S. B.},\n\tmonth = nov,\n\tyear = {2016},\n\tnote = {Publisher: IOP Publishing},\n\tpages = {012070},\n\tfile = {IOP Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\77XA23P4\\\\Andronikova и др. - 2016 - Pre-transitional evolution of central peaks and tr.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Inelastic X-ray scattering measurements have been done to study the lattice dynamics in lead zirconate titanate solid solution with 0.7% of PbTiO3. The temperature evolution of central peak and low-energy transverse phonon branches has been traced. Temperature dependent in-plane transverse polarized acoustic phonon branch in \\textless1 1 0\\textgreater direction has been revealed. The central peaks of two types have been found. The central peak at small wave vectors can be attributed to the relaxational-type soft ferroelectric mode, while the latter at Q = (1.5 -0.5 0) could be linked to the formation of M-superstructure in the intermediate ferroelectric phase.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"rochal-konevtsova-myasnikova-lorman-hiddensymmetryofsmallsphericalvirusesandorganizationprinciplesinanomalousanddoubleshelledcapsidnanoassemblies-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://pubs.rsc.org/en/content/articlelanding/2016/nr/c6nr04930c\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'rochal-konevtsova-myasnikova-lorman-hiddensymmetryofsmallsphericalvirusesandorganizationprinciplesinanomalousanddoubleshelledcapsidnanoassemblies-2016', 'https://pubs.rsc.org/en/content/articlelanding/2016/nr/c6nr04930c', event);\">\n    Hidden symmetry of small spherical viruses and organization principles in “anomalous” and double-shelled capsid nanoassemblies.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Rochal, S. B.; Konevtsova, O. V.; Myasnikova, A. E.;  and Lorman, V. L.\n</span>\n\n  \n\n</span>\n\n  <i>Nanoscale</i>, 8(38): 16976–16988. September 2016.\n  <span class=\"note\">Publisher: The Royal Society of Chemistry</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://pubs.rsc.org/en/content/articlelanding/2016/nr/c6nr04930c\"\n     onclick=\"log_download('rochal-konevtsova-myasnikova-lorman-hiddensymmetryofsmallsphericalvirusesandorganizationprinciplesinanomalousanddoubleshelledcapsidnanoassemblies-2016', 'https://pubs.rsc.org/en/content/articlelanding/2016/nr/c6nr04930c', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Hidden symmetry of small spherical viruses and organization principles in “anomalous” and double-shelled capsid nanoassemblies [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1039/C6NR04930C\"\n     onclick=\"log_download('rochal-konevtsova-myasnikova-lorman-hiddensymmetryofsmallsphericalvirusesandorganizationprinciplesinanomalousanddoubleshelledcapsidnanoassemblies-2016', 'http://doi.org/10.1039/C6NR04930C', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/rochal-konevtsova-myasnikova-lorman-hiddensymmetryofsmallsphericalvirusesandorganizationprinciplesinanomalousanddoubleshelledcapsidnanoassemblies-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('rochal-konevtsova-myasnikova-lorman-hiddensymmetryofsmallsphericalvirusesandorganizationprinciplesinanomalousanddoubleshelledcapsidnanoassemblies-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{rochal_hidden_2016,\n\ttitle = {Hidden symmetry of small spherical viruses and organization principles in “anomalous” and double-shelled capsid nanoassemblies},\n\tvolume = {8},\n\tissn = {2040-3372},\n\turl = {https://pubs.rsc.org/en/content/articlelanding/2016/nr/c6nr04930c},\n\tdoi = {10.1039/C6NR04930C},\n\tabstract = {We propose the principles of structural organization in spherical nanoassemblies with icosahedral symmetry constituted by asymmetric protein molecules. The approach modifies the paradigmatic geometrical Caspar and Klug (CK) model of icosahedral viral capsids and demonstrates the common origin of both the “anomalous” and conventional capsid structures. In contrast to all previous models of “anomalous” viral capsids the proposed modified model conserves the basic structural principles of the CK approach and reveals the common hidden symmetry underlying all small viral shells. We demonstrate the common genesis of the “anomalous” and conventional capsids and explain their structures in the same frame. The organization principles are derived from the group theory analysis of the positional order on the spherical surface. The relationship between the modified CK geometrical model and the theory of two-dimensional spherical crystallization is discussed. We also apply the proposed approach to complex double-shelled capsids and capsids with protruding knob-like proteins. The introduced notion of commensurability for the concentric nanoshells explains the peculiarities of their organization and helps to predict analogous, but yet undiscovered, double-shelled viral capsid nanostructures.},\n\tlanguage = {en},\n\tnumber = {38},\n\turldate = {2023-11-11},\n\tjournal = {Nanoscale},\n\tauthor = {Rochal, S. B. and Konevtsova, O. V. and Myasnikova, A. E. and Lorman, V. L.},\n\tmonth = sep,\n\tyear = {2016},\n\tnote = {Publisher: The Royal Society of Chemistry},\n\tpages = {16976--16988},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We propose the principles of structural organization in spherical nanoassemblies with icosahedral symmetry constituted by asymmetric protein molecules. The approach modifies the paradigmatic geometrical Caspar and Klug (CK) model of icosahedral viral capsids and demonstrates the common origin of both the “anomalous” and conventional capsid structures. In contrast to all previous models of “anomalous” viral capsids the proposed modified model conserves the basic structural principles of the CK approach and reveals the common hidden symmetry underlying all small viral shells. We demonstrate the common genesis of the “anomalous” and conventional capsids and explain their structures in the same frame. The organization principles are derived from the group theory analysis of the positional order on the spherical surface. The relationship between the modified CK geometrical model and the theory of two-dimensional spherical crystallization is discussed. We also apply the proposed approach to complex double-shelled capsids and capsids with protruding knob-like proteins. The introduced notion of commensurability for the concentric nanoshells explains the peculiarities of their organization and helps to predict analogous, but yet undiscovered, double-shelled viral capsid nanostructures.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"anokhin-razumnaya-yuzyuk-golovko-mukhortov-phasetransitionsinbariumstrontiumtitanatefilmsonmgosubstrateswithvariousorientations-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1063783416100048\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'anokhin-razumnaya-yuzyuk-golovko-mukhortov-phasetransitionsinbariumstrontiumtitanatefilmsonmgosubstrateswithvariousorientations-2016', 'https://doi.org/10.1134/S1063783416100048', event);\">\n    Phase transitions in barium–strontium titanate films on MgO substrates with various orientations.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Anokhin, A. S.; Razumnaya, A. G.; Yuzyuk, Y. I.; Golovko, Y. I.;  and Mukhortov, V. M.\n</span>\n\n  \n\n</span>\n\n  <i>Physics of the Solid State</i>, 58(10): 2027–2034. October 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1063783416100048\"\n     onclick=\"log_download('anokhin-razumnaya-yuzyuk-golovko-mukhortov-phasetransitionsinbariumstrontiumtitanatefilmsonmgosubstrateswithvariousorientations-2016', 'https://doi.org/10.1134/S1063783416100048', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Phase transitions in barium–strontium titanate films on MgO substrates with various orientations [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1063783416100048\"\n     onclick=\"log_download('anokhin-razumnaya-yuzyuk-golovko-mukhortov-phasetransitionsinbariumstrontiumtitanatefilmsonmgosubstrateswithvariousorientations-2016', 'http://doi.org/10.1134/S1063783416100048', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/anokhin-razumnaya-yuzyuk-golovko-mukhortov-phasetransitionsinbariumstrontiumtitanatefilmsonmgosubstrateswithvariousorientations-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('anokhin-razumnaya-yuzyuk-golovko-mukhortov-phasetransitionsinbariumstrontiumtitanatefilmsonmgosubstrateswithvariousorientations-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{anokhin_phase_2016,\n\ttitle = {Phase transitions in barium–strontium titanate films on {MgO} substrates with various orientations},\n\tvolume = {58},\n\tissn = {1090-6460},\n\turl = {https://doi.org/10.1134/S1063783416100048},\n\tdoi = {10.1134/S1063783416100048},\n\tabstract = {A comparative study of the lattice dynamic upon phase transitions in a polycrystalline Ba0.8Sr0.2TiO3 (BST) film on a Pt substrate and in epitaxial BST films grown on various sections of an MgO substrate has been performed by Raman spectroscopy. It has been found that different sequences of phase transitions take place in these films. The BST/Pt films demonstrate the same sequence of phase transitions that is observed in the bulk ceramics. The hardening of a soft mode in BST/(001)MgO and BST/Pt films shows that the transition from the tetragonal ferroelectric phase to the paraelectric phase has features of the displacement-type phase transition and also the order–disorder phase transition. When approaching the ferroelectric transition temperature, the soft mode in the BST/(111)MgO film is softened, following the Cockran law, which indicates the displacement-type phase transition.},\n\tlanguage = {en},\n\tnumber = {10},\n\turldate = {2023-11-11},\n\tjournal = {Physics of the Solid State},\n\tauthor = {Anokhin, A. S. and Razumnaya, A. G. and Yuzyuk, Yu. I. and Golovko, Yu. I. and Mukhortov, V. M.},\n\tmonth = oct,\n\tyear = {2016},\n\tpages = {2027--2034},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A comparative study of the lattice dynamic upon phase transitions in a polycrystalline Ba0.8Sr0.2TiO3 (BST) film on a Pt substrate and in epitaxial BST films grown on various sections of an MgO substrate has been performed by Raman spectroscopy. It has been found that different sequences of phase transitions take place in these films. The BST/Pt films demonstrate the same sequence of phase transitions that is observed in the bulk ceramics. The hardening of a soft mode in BST/(001)MgO and BST/Pt films shows that the transition from the tetragonal ferroelectric phase to the paraelectric phase has features of the displacement-type phase transition and also the order–disorder phase transition. When approaching the ferroelectric transition temperature, the soft mode in the BST/(111)MgO film is softened, following the Cockran law, which indicates the displacement-type phase transition.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"gorshunov-torgashev-zhukova-thomas-belyanchikov-kadlec-kadlec-savinov-etal-incipientferroelectricityofwatermoleculesconfinedtonanochannelsofberyl-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.nature.com/articles/ncomms12842\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'gorshunov-torgashev-zhukova-thomas-belyanchikov-kadlec-kadlec-savinov-etal-incipientferroelectricityofwatermoleculesconfinedtonanochannelsofberyl-2016', 'https://www.nature.com/articles/ncomms12842', event);\">\n    Incipient ferroelectricity of water molecules confined to nano-channels of beryl.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Gorshunov, B. P.; Torgashev, V. I.; Zhukova, E. S.; Thomas, V. G.; Belyanchikov, M. A.; Kadlec, C.; Kadlec, F.; Savinov, M.; Ostapchuk, T.; Petzelt, J.; Prokleška, J.; Tomas, P. V.; Pestrjakov, E. V.; Fursenko, D. A.; Shakurov, G. S.; Prokhorov, A. S.; Gorelik, V. S.; Kadyrov, L. S.; Uskov, V. V.; Kremer, R. K.;  and Dressel, M.\n</span>\n\n  \n\n</span>\n\n  <i>Nature Communications</i>, 7(1): 12842. September 2016.\n  <span class=\"note\">Number: 1 Publisher: Nature Publishing Group</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.nature.com/articles/ncomms12842\"\n     onclick=\"log_download('gorshunov-torgashev-zhukova-thomas-belyanchikov-kadlec-kadlec-savinov-etal-incipientferroelectricityofwatermoleculesconfinedtonanochannelsofberyl-2016', 'https://www.nature.com/articles/ncomms12842', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Incipient ferroelectricity of water molecules confined to nano-channels of beryl [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1038/ncomms12842\"\n     onclick=\"log_download('gorshunov-torgashev-zhukova-thomas-belyanchikov-kadlec-kadlec-savinov-etal-incipientferroelectricityofwatermoleculesconfinedtonanochannelsofberyl-2016', 'http://doi.org/10.1038/ncomms12842', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/gorshunov-torgashev-zhukova-thomas-belyanchikov-kadlec-kadlec-savinov-etal-incipientferroelectricityofwatermoleculesconfinedtonanochannelsofberyl-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('gorshunov-torgashev-zhukova-thomas-belyanchikov-kadlec-kadlec-savinov-etal-incipientferroelectricityofwatermoleculesconfinedtonanochannelsofberyl-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{gorshunov_incipient_2016,\n\ttitle = {Incipient ferroelectricity of water molecules confined to nano-channels of beryl},\n\tvolume = {7},\n\tcopyright = {2016 The Author(s)},\n\tissn = {2041-1723},\n\turl = {https://www.nature.com/articles/ncomms12842},\n\tdoi = {10.1038/ncomms12842},\n\tabstract = {Water is characterized by large molecular electric dipole moments and strong interactions between molecules; however, hydrogen bonds screen the dipole–dipole coupling and suppress the ferroelectric order. The situation changes drastically when water is confined: in this case ordering of the molecular dipoles has been predicted, but never unambiguously detected experimentally. In the present study we place separate H2O molecules in the structural channels of a beryl single crystal so that they are located far enough to prevent hydrogen bonding, but close enough to keep the dipole–dipole interaction, resulting in incipient ferroelectricity in the water molecular subsystem. We observe a ferroelectric soft mode that causes Curie–Weiss behaviour of the static permittivity, which saturates below 10 K due to quantum fluctuations. The ferroelectricity of water molecules may play a key role in the functioning of biological systems and find applications in fuel and memory cells, light emitters and other nanoscale electronic devices.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Nature Communications},\n\tauthor = {Gorshunov, B. P. and Torgashev, V. I. and Zhukova, E. S. and Thomas, V. G. and Belyanchikov, M. A. and Kadlec, C. and Kadlec, F. and Savinov, M. and Ostapchuk, T. and Petzelt, J. and Prokleška, J. and Tomas, P. V. and Pestrjakov, E. V. and Fursenko, D. A. and Shakurov, G. S. and Prokhorov, A. S. and Gorelik, V. S. and Kadyrov, L. S. and Uskov, V. V. and Kremer, R. K. and Dressel, M.},\n\tmonth = sep,\n\tyear = {2016},\n\tnote = {Number: 1\nPublisher: Nature Publishing Group},\n\tkeywords = {Ferroelectrics and multiferroics, Electronic devices, Electronic properties and materials},\n\tpages = {12842},\n\tfile = {Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\QJNV8X4R\\\\Gorshunov и др. - 2016 - Incipient ferroelectricity of water molecules conf.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Water is characterized by large molecular electric dipole moments and strong interactions between molecules; however, hydrogen bonds screen the dipole–dipole coupling and suppress the ferroelectric order. The situation changes drastically when water is confined: in this case ordering of the molecular dipoles has been predicted, but never unambiguously detected experimentally. In the present study we place separate H2O molecules in the structural channels of a beryl single crystal so that they are located far enough to prevent hydrogen bonding, but close enough to keep the dipole–dipole interaction, resulting in incipient ferroelectricity in the water molecular subsystem. We observe a ferroelectric soft mode that causes Curie–Weiss behaviour of the static permittivity, which saturates below 10 K due to quantum fluctuations. The ferroelectricity of water molecules may play a key role in the functioning of biological systems and find applications in fuel and memory cells, light emitters and other nanoscale electronic devices.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"lerer-timoshenko-chernikova-dispersioncharacteristicsofopticalwaveguidesbasedonznonanorods-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1064226916060140\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'lerer-timoshenko-chernikova-dispersioncharacteristicsofopticalwaveguidesbasedonznonanorods-2016', 'https://doi.org/10.1134/S1064226916060140', event);\">\n    Dispersion characteristics of optical waveguides based on ZnO nanorods.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Lerer, A. M.; Timoshenko, P. E.;  and Chernikova, T. Y.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Communications Technology and Electronics</i>, 61(6): 619–623. June 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1064226916060140\"\n     onclick=\"log_download('lerer-timoshenko-chernikova-dispersioncharacteristicsofopticalwaveguidesbasedonznonanorods-2016', 'https://doi.org/10.1134/S1064226916060140', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Dispersion characteristics of optical waveguides based on ZnO nanorods [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1064226916060140\"\n     onclick=\"log_download('lerer-timoshenko-chernikova-dispersioncharacteristicsofopticalwaveguidesbasedonznonanorods-2016', 'http://doi.org/10.1134/S1064226916060140', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/lerer-timoshenko-chernikova-dispersioncharacteristicsofopticalwaveguidesbasedonznonanorods-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('lerer-timoshenko-chernikova-dispersioncharacteristicsofopticalwaveguidesbasedonznonanorods-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{lerer_dispersion_2016,\n\ttitle = {Dispersion characteristics of optical waveguides based on {ZnO} nanorods},\n\tvolume = {61},\n\tissn = {1555-6557},\n\turl = {https://doi.org/10.1134/S1064226916060140},\n\tdoi = {10.1134/S1064226916060140},\n\tabstract = {Using the method of separation of variables in the cylindrical coordinate system, the problem of propagation of electromagnetic waves in a 2D periodic lattice of ZnO nanwaveguides covered with a thin metal film is solved. Comparison of calculation results with results of simulation with the use of the COMSOL Multiphysics™ package based on the finite-element method is performed. The obtained results are used for forecasting the resonance wavelengths of a 2D periodic lattice of ZnO nanorods grown on a dielectric substrate.},\n\tlanguage = {en},\n\tnumber = {6},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Communications Technology and Electronics},\n\tauthor = {Lerer, A. M. and Timoshenko, P. E. and Chernikova, T. Yu.},\n\tmonth = jun,\n\tyear = {2016},\n\tpages = {619--623},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Using the method of separation of variables in the cylindrical coordinate system, the problem of propagation of electromagnetic waves in a 2D periodic lattice of ZnO nanwaveguides covered with a thin metal film is solved. Comparison of calculation results with results of simulation with the use of the COMSOL Multiphysics™ package based on the finite-element method is performed. The obtained results are used for forecasting the resonance wavelengths of a 2D periodic lattice of ZnO nanorods grown on a dielectric substrate.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"zhukova-belyanchikov-torgashev-thomas-savinov-kadlec-kadlec-prokhorov-etal-terahertzdynamicsofnanoconfinedwatermolecules-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://ieeexplore.ieee.org/document/7758778\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'zhukova-belyanchikov-torgashev-thomas-savinov-kadlec-kadlec-prokhorov-etal-terahertzdynamicsofnanoconfinedwatermolecules-2016', 'https://ieeexplore.ieee.org/document/7758778', event);\">\n    Terahertz dynamics of nanoconfined water molecules.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Zhukova, E. S.; Belyanchikov, M. A.; Torgashev, V. I.; Thomas, V. G.; Savinov, M.; Kadlec, C.; Kadlec, F.; Prokhorov, A. S.; Kadyrov, L. S.; Petzelt, J.; Ostapchuk, T.; Fursenko, D. A.; Thomas, P. V.; Shakurov, G. S.; Dressel, M.;  and Gorshunov, B. P.\n</span>\n\n  \n\n</span>\n\n  In <i>2016 41st International Conference on Infrared, Millimeter, and Terahertz waves (IRMMW-THz)</i>, pages 1–2, September 2016. \n  <span class=\"note\">ISSN: 2162-2035</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://ieeexplore.ieee.org/document/7758778\"\n     onclick=\"log_download('zhukova-belyanchikov-torgashev-thomas-savinov-kadlec-kadlec-prokhorov-etal-terahertzdynamicsofnanoconfinedwatermolecules-2016', 'https://ieeexplore.ieee.org/document/7758778', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Terahertz dynamics of nanoconfined water molecules [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1109/IRMMW-THz.2016.7758778\"\n     onclick=\"log_download('zhukova-belyanchikov-torgashev-thomas-savinov-kadlec-kadlec-prokhorov-etal-terahertzdynamicsofnanoconfinedwatermolecules-2016', 'http://doi.org/10.1109/IRMMW-THz.2016.7758778', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/zhukova-belyanchikov-torgashev-thomas-savinov-kadlec-kadlec-prokhorov-etal-terahertzdynamicsofnanoconfinedwatermolecules-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('zhukova-belyanchikov-torgashev-thomas-savinov-kadlec-kadlec-prokhorov-etal-terahertzdynamicsofnanoconfinedwatermolecules-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{zhukova_terahertz_2016,\n\ttitle = {Terahertz dynamics of nanoconfined water molecules},\n\turl = {https://ieeexplore.ieee.org/document/7758778},\n\tdoi = {10.1109/IRMMW-THz.2016.7758778},\n\tabstract = {We performed spectroscopic studies of water-containing beryl crystals. At terahertz frequencies, we observed a strongly temperature-dependent spectral feature, corresponding to a collective excitation caused by dipole-dipole interactions between separate H2O molecules. We associate the excitation with a soft mode signaling an incipient ferroelectric state within the water molecular subsystem. Single-particle excitations of nanocaged H2O molecules are also observed at terahertz and infrared frequencies; using DFT analysis, their origin is assigned to translational and librational vibrational states.},\n\turldate = {2023-11-11},\n\tbooktitle = {2016 41st {International} {Conference} on {Infrared}, {Millimeter}, and {Terahertz} waves ({IRMMW}-{THz})},\n\tauthor = {Zhukova, Elena S. and Belyanchikov, Mikhail A. and Torgashev, Victor I. and Thomas, Victor G. and Savinov, Maksim and Kadlec, Christelle and Kadlec, Filip and Prokhorov, Anatoly S. and Kadyrov, Lenar S. and Petzelt, Jan and Ostapchuk, Tatyana and Fursenko, Dmitry A. and Thomas, Pavel V. and Shakurov, Gilman S. and Dressel, Martin and Gorshunov, Boris P.},\n\tmonth = sep,\n\tyear = {2016},\n\tnote = {ISSN: 2162-2035},\n\tpages = {1--2},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We performed spectroscopic studies of water-containing beryl crystals. At terahertz frequencies, we observed a strongly temperature-dependent spectral feature, corresponding to a collective excitation caused by dipole-dipole interactions between separate H2O molecules. We associate the excitation with a soft mode signaling an incipient ferroelectric state within the water molecular subsystem. Single-particle excitations of nanocaged H2O molecules are also observed at terahertz and infrared frequencies; using DFT analysis, their origin is assigned to translational and librational vibrational states.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"motovilov-pronin-zhukova-gagkaeva-torgashev-savinov-grinenko-belyanchikov-etal-ontheissueofuniversaldielectricresponsesinproteins-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://ieeexplore.ieee.org/document/7758865\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'motovilov-pronin-zhukova-gagkaeva-torgashev-savinov-grinenko-belyanchikov-etal-ontheissueofuniversaldielectricresponsesinproteins-2016', 'https://ieeexplore.ieee.org/document/7758865', event);\">\n    On the issue of universal dielectric responses in proteins.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Motovilov, K. A.; Pronin, A. A.; Zhukova, E. S.; Gagkaeva, Z. V.; Torgashev, V. I.; Savinov, M.; Grinenko, V.; Belyanchikov, M. A.; Grebenko, A. K.; Sidoruk, K. V.; Dressel, M.;  and Gorshunov, B. P.\n</span>\n\n  \n\n</span>\n\n  In <i>2016 41st International Conference on Infrared, Millimeter, and Terahertz waves (IRMMW-THz)</i>, pages 1–1, September 2016. \n  <span class=\"note\">ISSN: 2162-2035</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://ieeexplore.ieee.org/document/7758865\"\n     onclick=\"log_download('motovilov-pronin-zhukova-gagkaeva-torgashev-savinov-grinenko-belyanchikov-etal-ontheissueofuniversaldielectricresponsesinproteins-2016', 'https://ieeexplore.ieee.org/document/7758865', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"On the issue of universal dielectric responses in proteins [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1109/IRMMW-THz.2016.7758865\"\n     onclick=\"log_download('motovilov-pronin-zhukova-gagkaeva-torgashev-savinov-grinenko-belyanchikov-etal-ontheissueofuniversaldielectricresponsesinproteins-2016', 'http://doi.org/10.1109/IRMMW-THz.2016.7758865', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/motovilov-pronin-zhukova-gagkaeva-torgashev-savinov-grinenko-belyanchikov-etal-ontheissueofuniversaldielectricresponsesinproteins-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('motovilov-pronin-zhukova-gagkaeva-torgashev-savinov-grinenko-belyanchikov-etal-ontheissueofuniversaldielectricresponsesinproteins-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{motovilov_issue_2016,\n\ttitle = {On the issue of universal dielectric responses in proteins},\n\turl = {https://ieeexplore.ieee.org/document/7758865},\n\tdoi = {10.1109/IRMMW-THz.2016.7758865},\n\tabstract = {Ac conductivity and dielectric permittivity of bovine serum albumin, cytochrome c and extracellular matrix synthesized by electrogenic bacteria Shewanella oneidensis MR-1 are measured at frequencies 1-1012 Hz and temperatures 10-300 K. Two types of conductivity mechanisms are observed as well as nearly constant loss (NCL) phenomenon, universal dielectric response (UDR) and signatures of boson peak depending on the temperature and water/ion contents in the samples.},\n\turldate = {2023-11-11},\n\tbooktitle = {2016 41st {International} {Conference} on {Infrared}, {Millimeter}, and {Terahertz} waves ({IRMMW}-{THz})},\n\tauthor = {Motovilov, Konstantin A. and Pronin, Aleksei A. and Zhukova, Elena S. and Gagkaeva, Zarina V. and Torgashev, Victor I. and Savinov, Maxim and Grinenko, Vadim and Belyanchikov, Mikhail A. and Grebenko, Artem K. and Sidoruk, Konstantin V. and Dressel, Martin and Gorshunov, Boris P.},\n\tmonth = sep,\n\tyear = {2016},\n\tnote = {ISSN: 2162-2035},\n\tpages = {1--1},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Ac conductivity and dielectric permittivity of bovine serum albumin, cytochrome c and extracellular matrix synthesized by electrogenic bacteria Shewanella oneidensis MR-1 are measured at frequencies 1-1012 Hz and temperatures 10-300 K. Two types of conductivity mechanisms are observed as well as nearly constant loss (NCL) phenomenon, universal dielectric response (UDR) and signatures of boson peak depending on the temperature and water/ion contents in the samples.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"lerer-timoshenko-chernikova-kaidashev-puzanov-opticalnanowaveguidesbasedonzincoxideplasmonicmaterials-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/741/1/012159\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'lerer-timoshenko-chernikova-kaidashev-puzanov-opticalnanowaveguidesbasedonzincoxideplasmonicmaterials-2016', 'https://dx.doi.org/10.1088/1742-6596/741/1/012159', event);\">\n    Optical Nanowaveguides Based on Zinc Oxide Plasmonic Materials.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Lerer, A. M.; Timoshenko, P. E.; Chernikova, T. Y.; Kaidashev, E. M.;  and Puzanov, A. S.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics: Conference Series</i>, 741(1): 012159. August 2016.\n  <span class=\"note\">Publisher: IOP Publishing</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/741/1/012159\"\n     onclick=\"log_download('lerer-timoshenko-chernikova-kaidashev-puzanov-opticalnanowaveguidesbasedonzincoxideplasmonicmaterials-2016', 'https://dx.doi.org/10.1088/1742-6596/741/1/012159', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Optical Nanowaveguides Based on Zinc Oxide Plasmonic Materials [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/1742-6596/741/1/012159\"\n     onclick=\"log_download('lerer-timoshenko-chernikova-kaidashev-puzanov-opticalnanowaveguidesbasedonzincoxideplasmonicmaterials-2016', 'http://doi.org/10.1088/1742-6596/741/1/012159', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/lerer-timoshenko-chernikova-kaidashev-puzanov-opticalnanowaveguidesbasedonzincoxideplasmonicmaterials-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('lerer-timoshenko-chernikova-kaidashev-puzanov-opticalnanowaveguidesbasedonzincoxideplasmonicmaterials-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{lerer_optical_2016,\n\ttitle = {Optical {Nanowaveguides} {Based} on {Zinc} {Oxide} {Plasmonic} {Materials}},\n\tvolume = {741},\n\tissn = {1742-6596},\n\turl = {https://dx.doi.org/10.1088/1742-6596/741/1/012159},\n\tdoi = {10.1088/1742-6596/741/1/012159},\n\tabstract = {The numerical study of nanowaveguides containing ZO, AZO, GZO and other materials are studied in infrared range. The dispersion relation for the waveguides contained an arbitrary number of layers are solved numerically. The integral-differential equations in vector form of the electromagnetic waves propagation in nanowaveguides containing a finite width plasmon films are calculated by the Galerkin’ method and the effective dielectric constants method. The opportunity of surface plasmon-polariton propagation with a large deceleration ratio are shown.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics: Conference Series},\n\tauthor = {Lerer, A. M. and Timoshenko, P. E. and Chernikova, T. Yu and Kaidashev, E. M. and Puzanov, A. S.},\n\tmonth = aug,\n\tyear = {2016},\n\tnote = {Publisher: IOP Publishing},\n\tpages = {012159},\n\tfile = {IOP Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\V8WUEVR3\\\\Lerer и др. - 2016 - Optical Nanowaveguides Based on Zinc Oxide Plasmon.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The numerical study of nanowaveguides containing ZO, AZO, GZO and other materials are studied in infrared range. The dispersion relation for the waveguides contained an arbitrary number of layers are solved numerically. The integral-differential equations in vector form of the electromagnetic waves propagation in nanowaveguides containing a finite width plasmon films are calculated by the Galerkin’ method and the effective dielectric constants method. The opportunity of surface plasmon-polariton propagation with a large deceleration ratio are shown.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-pavlenko-yuzyuk-phenomenologicaltheoryofuniaxialrelaxorferroelectrics-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/0953-8984/28/39/395902\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-pavlenko-yuzyuk-phenomenologicaltheoryofuniaxialrelaxorferroelectrics-2016', 'https://dx.doi.org/10.1088/0953-8984/28/39/395902', event);\">\n    Phenomenological theory of uniaxial relaxor ferroelectrics.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.; Pavlenko, A. V.;  and Yuzyuk, Y. I.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics: Condensed Matter</i>, 28(39): 395902. August 2016.\n  <span class=\"note\">Publisher: IOP Publishing</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/0953-8984/28/39/395902\"\n     onclick=\"log_download('shirokov-pavlenko-yuzyuk-phenomenologicaltheoryofuniaxialrelaxorferroelectrics-2016', 'https://dx.doi.org/10.1088/0953-8984/28/39/395902', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Phenomenological theory of uniaxial relaxor ferroelectrics [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/0953-8984/28/39/395902\"\n     onclick=\"log_download('shirokov-pavlenko-yuzyuk-phenomenologicaltheoryofuniaxialrelaxorferroelectrics-2016', 'http://doi.org/10.1088/0953-8984/28/39/395902', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-pavlenko-yuzyuk-phenomenologicaltheoryofuniaxialrelaxorferroelectrics-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-pavlenko-yuzyuk-phenomenologicaltheoryofuniaxialrelaxorferroelectrics-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_phenomenological_2016,\n\ttitle = {Phenomenological theory of uniaxial relaxor ferroelectrics},\n\tvolume = {28},\n\tissn = {0953-8984},\n\turl = {https://dx.doi.org/10.1088/0953-8984/28/39/395902},\n\tdoi = {10.1088/0953-8984/28/39/395902},\n\tabstract = {A phenomenological thermodynamic theory of uniaxial relaxor strontium barium niobate is developed using the Landau–Devonshire approach with two order parameters. The fourth-order thermodynamic potential allowed to explain the shape of the polarization hysteresis loops experimentally observed at different temperatures. We show that the broad maximum of the dielectric permittivity is not related to the phase transition and arise due to the coupling between polarization and true order parameter which has antiferroelectric nature. We found that the phase transition temperature is much higher than the maximum of the dielectric permittivity and very likely corresponds to so-called Burn’s temperature. True order parameter has no simple relation with polar modes.},\n\tlanguage = {en},\n\tnumber = {39},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics: Condensed Matter},\n\tauthor = {Shirokov, V. B. and Pavlenko, A. V. and Yuzyuk, Yu I.},\n\tmonth = aug,\n\tyear = {2016},\n\tnote = {Publisher: IOP Publishing},\n\tpages = {395902},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A phenomenological thermodynamic theory of uniaxial relaxor strontium barium niobate is developed using the Landau–Devonshire approach with two order parameters. The fourth-order thermodynamic potential allowed to explain the shape of the polarization hysteresis loops experimentally observed at different temperatures. We show that the broad maximum of the dielectric permittivity is not related to the phase transition and arise due to the coupling between polarization and true order parameter which has antiferroelectric nature. We found that the phase transition temperature is much higher than the maximum of the dielectric permittivity and very likely corresponds to so-called Burn’s temperature. True order parameter has no simple relation with polar modes.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-kalinchuk-shakhovoi-yuzyuk-physicalstatesandpropertiesofbariumtitanatefilmsinaplaneelectricfield-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1063784216070240\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-kalinchuk-shakhovoi-yuzyuk-physicalstatesandpropertiesofbariumtitanatefilmsinaplaneelectricfield-2016', 'https://doi.org/10.1134/S1063784216070240', event);\">\n    Physical states and properties of barium titanate films in a plane electric field.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.; Kalinchuk, V. V.; Shakhovoi, R. A.;  and Yuzyuk, Y. I.\n</span>\n\n  \n\n</span>\n\n  <i>Technical Physics</i>, 61(7): 1073–1078. July 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1063784216070240\"\n     onclick=\"log_download('shirokov-kalinchuk-shakhovoi-yuzyuk-physicalstatesandpropertiesofbariumtitanatefilmsinaplaneelectricfield-2016', 'https://doi.org/10.1134/S1063784216070240', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Physical states and properties of barium titanate films in a plane electric field [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1063784216070240\"\n     onclick=\"log_download('shirokov-kalinchuk-shakhovoi-yuzyuk-physicalstatesandpropertiesofbariumtitanatefilmsinaplaneelectricfield-2016', 'http://doi.org/10.1134/S1063784216070240', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-kalinchuk-shakhovoi-yuzyuk-physicalstatesandpropertiesofbariumtitanatefilmsinaplaneelectricfield-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-kalinchuk-shakhovoi-yuzyuk-physicalstatesandpropertiesofbariumtitanatefilmsinaplaneelectricfield-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_physical_2016,\n\ttitle = {Physical states and properties of barium titanate films in a plane electric field},\n\tvolume = {61},\n\tissn = {1090-6525},\n\turl = {https://doi.org/10.1134/S1063784216070240},\n\tdoi = {10.1134/S1063784216070240},\n\tabstract = {The influence of a plane electric field on the phase states of barium titanate thin films under the conditions of forced deformation has been studied. The field dependence of a complete set of material constants has been taken in the region of the c-phase, where polarization losses are absent. The material constants are calculated using equations of the piezoelectric effect derived by linearizing the nonlinear equations of state from the phenomenological; theory for barium titanate. It has been shown that there is a critical value of the field at which the electromechanical coupling coefficient reaches a maximum.},\n\tlanguage = {en},\n\tnumber = {7},\n\turldate = {2023-11-11},\n\tjournal = {Technical Physics},\n\tauthor = {Shirokov, V. B. and Kalinchuk, V. V. and Shakhovoi, R. A. and Yuzyuk, Yu. I.},\n\tmonth = jul,\n\tyear = {2016},\n\tpages = {1073--1078},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The influence of a plane electric field on the phase states of barium titanate thin films under the conditions of forced deformation has been studied. The field dependence of a complete set of material constants has been taken in the region of the c-phase, where polarization losses are absent. The material constants are calculated using equations of the piezoelectric effect derived by linearizing the nonlinear equations of state from the phenomenological; theory for barium titanate. It has been shown that there is a critical value of the field at which the electromechanical coupling coefficient reaches a maximum.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"konevtsova-lorman-rochal-theoryofmorphologicaltransformationofviralcapsidshellduringthematurationprocessinthehk97bacteriophageandsimilarviruses-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevE.93.052412\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'konevtsova-lorman-rochal-theoryofmorphologicaltransformationofviralcapsidshellduringthematurationprocessinthehk97bacteriophageandsimilarviruses-2016', 'https://link.aps.org/doi/10.1103/PhysRevE.93.052412', event);\">\n    Theory of morphological transformation of viral capsid shell during the maturation process in the HK97 bacteriophage and similar viruses.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Konevtsova, O. V.; Lorman, V. L.;  and Rochal, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review E</i>, 93(5): 052412. May 2016.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevE.93.052412\"\n     onclick=\"log_download('konevtsova-lorman-rochal-theoryofmorphologicaltransformationofviralcapsidshellduringthematurationprocessinthehk97bacteriophageandsimilarviruses-2016', 'https://link.aps.org/doi/10.1103/PhysRevE.93.052412', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Theory of morphological transformation of viral capsid shell during the maturation process in the HK97 bacteriophage and similar viruses [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevE.93.052412\"\n     onclick=\"log_download('konevtsova-lorman-rochal-theoryofmorphologicaltransformationofviralcapsidshellduringthematurationprocessinthehk97bacteriophageandsimilarviruses-2016', 'http://doi.org/10.1103/PhysRevE.93.052412', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/konevtsova-lorman-rochal-theoryofmorphologicaltransformationofviralcapsidshellduringthematurationprocessinthehk97bacteriophageandsimilarviruses-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('konevtsova-lorman-rochal-theoryofmorphologicaltransformationofviralcapsidshellduringthematurationprocessinthehk97bacteriophageandsimilarviruses-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{konevtsova_theory_2016,\n\ttitle = {Theory of morphological transformation of viral capsid shell during the maturation process in the {HK97} bacteriophage and similar viruses},\n\tvolume = {93},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevE.93.052412},\n\tdoi = {10.1103/PhysRevE.93.052412},\n\tabstract = {We consider the symmetry and physical origin of collective displacement modes playing a crucial role in the morphological transformation during the maturation of the HK97 bacteriophage and similar viruses. It is shown that the experimentally observed hexamer deformation and pentamer twist in the HK97 procapsid correspond to the simplest irreducible shear strain mode of a spherical shell. We also show that the icosahedral faceting of the bacteriophage capsid shell is driven by the simplest irreducible radial displacement field. The shear field has the rotational icosahedral symmetry group I while the radial field has the full icosahedral symmetry Ih. This difference makes their actions independent. The radial field sign discriminates between the icosahedral and the dodecahedral shapes of the faceted capsid shell, thus making the approach relevant not only for the HK97-like viruses but also for the parvovirus family. In the frame of the Landau-Ginzburg formalism we propose a simple phenomenological model valid for the first reversible step of the HK97 maturation process. The calculated phase diagram illustrates the discontinuous character of the virus shape transformation. The characteristics of the virus shell faceting and expansion obtained in the in vitro and in vivo experiments are related to the decrease in the capsid shell thickness and to the increase of the internal capsid pressure.},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review E},\n\tauthor = {Konevtsova, O. V. and Lorman, V. L. and Rochal, S. B.},\n\tmonth = may,\n\tyear = {2016},\n\tnote = {Publisher: American Physical Society},\n\tpages = {052412},\n\tfile = {Принятая версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\UA4NGX4T\\\\Konevtsova и др. - 2016 - Theory of morphological transformation of viral ca.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We consider the symmetry and physical origin of collective displacement modes playing a crucial role in the morphological transformation during the maturation of the HK97 bacteriophage and similar viruses. It is shown that the experimentally observed hexamer deformation and pentamer twist in the HK97 procapsid correspond to the simplest irreducible shear strain mode of a spherical shell. We also show that the icosahedral faceting of the bacteriophage capsid shell is driven by the simplest irreducible radial displacement field. The shear field has the rotational icosahedral symmetry group I while the radial field has the full icosahedral symmetry Ih. This difference makes their actions independent. The radial field sign discriminates between the icosahedral and the dodecahedral shapes of the faceted capsid shell, thus making the approach relevant not only for the HK97-like viruses but also for the parvovirus family. In the frame of the Landau-Ginzburg formalism we propose a simple phenomenological model valid for the first reversible step of the HK97 maturation process. The calculated phase diagram illustrates the discontinuous character of the virus shape transformation. The characteristics of the virus shell faceting and expansion obtained in the in vitro and in vivo experiments are related to the decrease in the capsid shell thickness and to the increase of the internal capsid pressure.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"talanov-shirokov-talanov-phenomenologicalthermodynamicsandthestructureformationmechanismofthecuti2s4rhombohedralphase-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://pubs.rsc.org/en/content/articlelanding/2016/cp/c6cp00387g\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'talanov-shirokov-talanov-phenomenologicalthermodynamicsandthestructureformationmechanismofthecuti2s4rhombohedralphase-2016', 'https://pubs.rsc.org/en/content/articlelanding/2016/cp/c6cp00387g', event);\">\n    Phenomenological thermodynamics and the structure formation mechanism of the CuTi2S4 rhombohedral phase.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Talanov, M. V.; Shirokov, V. B.;  and Talanov, V. M.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Chemistry Chemical Physics</i>, 18(15): 10600–10606. April 2016.\n  <span class=\"note\">Publisher: The Royal Society of Chemistry</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://pubs.rsc.org/en/content/articlelanding/2016/cp/c6cp00387g\"\n     onclick=\"log_download('talanov-shirokov-talanov-phenomenologicalthermodynamicsandthestructureformationmechanismofthecuti2s4rhombohedralphase-2016', 'https://pubs.rsc.org/en/content/articlelanding/2016/cp/c6cp00387g', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Phenomenological thermodynamics and the structure formation mechanism of the CuTi2S4 rhombohedral phase [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1039/C6CP00387G\"\n     onclick=\"log_download('talanov-shirokov-talanov-phenomenologicalthermodynamicsandthestructureformationmechanismofthecuti2s4rhombohedralphase-2016', 'http://doi.org/10.1039/C6CP00387G', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/talanov-shirokov-talanov-phenomenologicalthermodynamicsandthestructureformationmechanismofthecuti2s4rhombohedralphase-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('talanov-shirokov-talanov-phenomenologicalthermodynamicsandthestructureformationmechanismofthecuti2s4rhombohedralphase-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{talanov_phenomenological_2016,\n\ttitle = {Phenomenological thermodynamics and the structure formation mechanism of the {CuTi2S4} rhombohedral phase},\n\tvolume = {18},\n\tissn = {1463-9084},\n\turl = {https://pubs.rsc.org/en/content/articlelanding/2016/cp/c6cp00387g},\n\tdoi = {10.1039/C6CP00387G},\n\tabstract = {The theory of structural phase transition in CuTi2S4 is proposed. The symmetry of order parameters, thermodynamics and the mechanism of the atomic structure formation of the rhombohedral Cu–Ti–thiospinel have been studied. The critical order parameter inducing the phase transition has been found. Within the Landau theory of phase transitions, it is shown that the phase state may change from the high-symmetry cubic disordered Fdm phase to the low-symmetry ordered rhombohedral Rm phase as a result of phase transition of the first order close to the second order. It is shown that the rhombohedral structure of CuTi2S4 is formed as a result of the displacements of all types of atoms and the ordering of Cu-atoms (1 : 1 order type in tetrahedral spinel sites), Ti-atoms (1 : 1 : 6 order type in octahedral spinel sites), and S-atoms (1 : 1 : 3 : 3 order type). The Cu- and Ti-atoms form metal nanoclusters which are named a “bunch” of dimers. The “bunch” of dimers in CuTi2S4 is a new type of self-organization of atoms in frustrated spinel-like structures. It is shown that Ti-atoms also form other types of metal nanoclusters: trimers and tetrahedra.},\n\tlanguage = {en},\n\tnumber = {15},\n\turldate = {2023-11-11},\n\tjournal = {Physical Chemistry Chemical Physics},\n\tauthor = {Talanov, Michail V. and Shirokov, Vladimir B. and Talanov, Valery M.},\n\tmonth = apr,\n\tyear = {2016},\n\tnote = {Publisher: The Royal Society of Chemistry},\n\tpages = {10600--10606},\n\tfile = {Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\IESXZ2EA\\\\Talanov и др. - 2016 - Phenomenological thermodynamics and the structure .pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The theory of structural phase transition in CuTi2S4 is proposed. The symmetry of order parameters, thermodynamics and the mechanism of the atomic structure formation of the rhombohedral Cu–Ti–thiospinel have been studied. The critical order parameter inducing the phase transition has been found. Within the Landau theory of phase transitions, it is shown that the phase state may change from the high-symmetry cubic disordered Fdm phase to the low-symmetry ordered rhombohedral Rm phase as a result of phase transition of the first order close to the second order. It is shown that the rhombohedral structure of CuTi2S4 is formed as a result of the displacements of all types of atoms and the ordering of Cu-atoms (1 : 1 order type in tetrahedral spinel sites), Ti-atoms (1 : 1 : 6 order type in octahedral spinel sites), and S-atoms (1 : 1 : 3 : 3 order type). The Cu- and Ti-atoms form metal nanoclusters which are named a “bunch” of dimers. The “bunch” of dimers in CuTi2S4 is a new type of self-organization of atoms in frustrated spinel-like structures. It is shown that Ti-atoms also form other types of metal nanoclusters: trimers and tetrahedra.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"mirzakhanyan-manukyan-gyulasaryan-ginoyan-nurijanyan-yuzyuk-kaniukov-sharoyan-characterizationofzincandzinccyanidenanoparticlesincarbonmatricespreparedbysolidphasepyrolysisofzincphthalocyanine-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.3103/S1068337216020134\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'mirzakhanyan-manukyan-gyulasaryan-ginoyan-nurijanyan-yuzyuk-kaniukov-sharoyan-characterizationofzincandzinccyanidenanoparticlesincarbonmatricespreparedbysolidphasepyrolysisofzincphthalocyanine-2016', 'https://doi.org/10.3103/S1068337216020134', event);\">\n    Characterization of zinc and zinc cyanide nanoparticles in carbon matrices prepared by solid-phase pyrolysis of zinc-phthalocyanine.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Mirzakhanyan, A. A.; Manukyan, A. S.; Gyulasaryan, H. T.; Ginoyan, A. K.; Nurijanyan, M. K.; Yuzyuk, Y. I.; Kaniukov, E. Y.;  and Sharoyan, E. G.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Contemporary Physics (Armenian Academy of Sciences)</i>, 51(2): 191–195. April 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.3103/S1068337216020134\"\n     onclick=\"log_download('mirzakhanyan-manukyan-gyulasaryan-ginoyan-nurijanyan-yuzyuk-kaniukov-sharoyan-characterizationofzincandzinccyanidenanoparticlesincarbonmatricespreparedbysolidphasepyrolysisofzincphthalocyanine-2016', 'https://doi.org/10.3103/S1068337216020134', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Characterization of zinc and zinc cyanide nanoparticles in carbon matrices prepared by solid-phase pyrolysis of zinc-phthalocyanine [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3103/S1068337216020134\"\n     onclick=\"log_download('mirzakhanyan-manukyan-gyulasaryan-ginoyan-nurijanyan-yuzyuk-kaniukov-sharoyan-characterizationofzincandzinccyanidenanoparticlesincarbonmatricespreparedbysolidphasepyrolysisofzincphthalocyanine-2016', 'http://doi.org/10.3103/S1068337216020134', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/mirzakhanyan-manukyan-gyulasaryan-ginoyan-nurijanyan-yuzyuk-kaniukov-sharoyan-characterizationofzincandzinccyanidenanoparticlesincarbonmatricespreparedbysolidphasepyrolysisofzincphthalocyanine-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('mirzakhanyan-manukyan-gyulasaryan-ginoyan-nurijanyan-yuzyuk-kaniukov-sharoyan-characterizationofzincandzinccyanidenanoparticlesincarbonmatricespreparedbysolidphasepyrolysisofzincphthalocyanine-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{mirzakhanyan_characterization_2016,\n\ttitle = {Characterization of zinc and zinc cyanide nanoparticles in carbon matrices prepared by solid-phase pyrolysis of zinc-phthalocyanine},\n\tvolume = {51},\n\tissn = {1934-9378},\n\turl = {https://doi.org/10.3103/S1068337216020134},\n\tdoi = {10.3103/S1068337216020134},\n\tabstract = {Using solid-phase pyrolysis of Zn-phthalocyanine (ZnC32H16N8), we have prepared zinc and zinc cyanide nanoparticles in carbon matrices with a zinc concentration of 3 at \\%. The structure and composition of samples were investigated by the methods of scanning electron microscopy, X-ray diffraction, and Raman spectroscopy. It is shown that at low pyrolysis temperature (700°C) only the Zn nanoparticles are formed, whereas at higher temperature (900°C) a certain amount of Zn(CN)2 nanoparticles are also synthesized. The mean diameter of nanoparticles is about 150 nm, and their size distribution has a logarithmically normal shape.},\n\tlanguage = {en},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Contemporary Physics (Armenian Academy of Sciences)},\n\tauthor = {Mirzakhanyan, A. A. and Manukyan, A. S. and Gyulasaryan, H. T. and Ginoyan, A. K. and Nurijanyan, M. Kh. and Yuzyuk, Yu. I. and Kaniukov, E. Yu. and Sharoyan, E. G.},\n\tmonth = apr,\n\tyear = {2016},\n\tkeywords = {X-ray diffraction, Raman shift, SEM images, size distribution, solid-phase pyrolysis, zinc and zinc cyanide nanoparticles},\n\tpages = {191--195},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\MAWN25GC\\\\Mirzakhanyan и др. - 2016 - Characterization of zinc and zinc cyanide nanopart.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Using solid-phase pyrolysis of Zn-phthalocyanine (ZnC32H16N8), we have prepared zinc and zinc cyanide nanoparticles in carbon matrices with a zinc concentration of 3 at %. The structure and composition of samples were investigated by the methods of scanning electron microscopy, X-ray diffraction, and Raman spectroscopy. It is shown that at low pyrolysis temperature (700°C) only the Zn nanoparticles are formed, whereas at higher temperature (900°C) a certain amount of Zn(CN)2 nanoparticles are also synthesized. The mean diameter of nanoparticles is about 150 nm, and their size distribution has a logarithmically normal shape.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"bokovasirosh-kuznetsov-romanenko-kazakova-krasnikov-tkachev-yuzyuk-obraztsova-investigationofdefectivenessofmultiwalledcarbonnanotubesproducedwithfecocatalystsofdifferentcomposition-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.spiedigitallibrary.org/journals/journal-of-nanophotonics/volume-10/issue-1/012526/Investigation-of-defectiveness-of-multiwalled-carbon-nanotubes-produced-with-FeCo/10.1117/1.JNP.10.012526.full\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'bokovasirosh-kuznetsov-romanenko-kazakova-krasnikov-tkachev-yuzyuk-obraztsova-investigationofdefectivenessofmultiwalledcarbonnanotubesproducedwithfecocatalystsofdifferentcomposition-2016', 'https://www.spiedigitallibrary.org/journals/journal-of-nanophotonics/volume-10/issue-1/012526/Investigation-of-defectiveness-of-multiwalled-carbon-nanotubes-produced-with-FeCo/10.1117/1.JNP.10.012526.full', event);\">\n    Investigation of defectiveness of multiwalled carbon nanotubes produced with Fe–Co catalysts of different composition.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Bokova-Sirosh, S. N.; Kuznetsov, V. L.; Romanenko, A. I.; Kazakova, M. A.; Krasnikov, D. V.; Tkachev, E. N.; Yuzyuk, Y. I.;  and Obraztsova, E. D.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Nanophotonics</i>, 10(1): 012526. March 2016.\n  <span class=\"note\">Publisher: SPIE</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.spiedigitallibrary.org/journals/journal-of-nanophotonics/volume-10/issue-1/012526/Investigation-of-defectiveness-of-multiwalled-carbon-nanotubes-produced-with-FeCo/10.1117/1.JNP.10.012526.full\"\n     onclick=\"log_download('bokovasirosh-kuznetsov-romanenko-kazakova-krasnikov-tkachev-yuzyuk-obraztsova-investigationofdefectivenessofmultiwalledcarbonnanotubesproducedwithfecocatalystsofdifferentcomposition-2016', 'https://www.spiedigitallibrary.org/journals/journal-of-nanophotonics/volume-10/issue-1/012526/Investigation-of-defectiveness-of-multiwalled-carbon-nanotubes-produced-with-FeCo/10.1117/1.JNP.10.012526.full', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Investigation of defectiveness of multiwalled carbon nanotubes produced with Fe–Co catalysts of different composition [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1117/1.JNP.10.012526\"\n     onclick=\"log_download('bokovasirosh-kuznetsov-romanenko-kazakova-krasnikov-tkachev-yuzyuk-obraztsova-investigationofdefectivenessofmultiwalledcarbonnanotubesproducedwithfecocatalystsofdifferentcomposition-2016', 'http://doi.org/10.1117/1.JNP.10.012526', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/bokovasirosh-kuznetsov-romanenko-kazakova-krasnikov-tkachev-yuzyuk-obraztsova-investigationofdefectivenessofmultiwalledcarbonnanotubesproducedwithfecocatalystsofdifferentcomposition-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('bokovasirosh-kuznetsov-romanenko-kazakova-krasnikov-tkachev-yuzyuk-obraztsova-investigationofdefectivenessofmultiwalledcarbonnanotubesproducedwithfecocatalystsofdifferentcomposition-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{bokova-sirosh_investigation_2016,\n\ttitle = {Investigation of defectiveness of multiwalled carbon nanotubes produced with {Fe}–{Co} catalysts of different composition},\n\tvolume = {10},\n\tissn = {1934-2608, 1934-2608},\n\turl = {https://www.spiedigitallibrary.org/journals/journal-of-nanophotonics/volume-10/issue-1/012526/Investigation-of-defectiveness-of-multiwalled-carbon-nanotubes-produced-with-FeCo/10.1117/1.JNP.10.012526.full},\n\tdoi = {10.1117/1.JNP.10.012526},\n\tabstract = {We have performed a study of CVD multiwalled carbon nanotubes (MWCNTs) produced with Fe–Co catalysts with a variable ratio of active metals. The Raman data were considered in combination with the temperature dependence of MWCNT conductivity. The data analysis is based on the point that the value of I2D/ID ratio correlates with the graphene fragment size. The fragments are considered as building blocks of MWCNTs. We showed that MWCNT defectiveness depends on the ratio of bimetallic active components in the Fe–Co catalyst. Thus, the ratio of I2D/ID increases and the D-mode intensity decreases while the Fe content in the catalyst increases. This also points to the reduction of defect number in the bigger graphene fragments. These results correlate with the data on conductivity temperature dependence. Namely, the increase of Fe content in the active component of the Fe–Co catalyst results in the increase of charge carrier concentration, which, in turn, indicates a decrease in MWCNT defectiveness.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Nanophotonics},\n\tauthor = {Bokova-Sirosh, Sofya N. and Kuznetsov, Vladimir L. and Romanenko, Anatoly I. and Kazakova, Mariya A. and Krasnikov, Dmitry V. and Tkachev, Evgeniy N. and Yuzyuk, Yuri I. and Obraztsova, Elena D.},\n\tmonth = mar,\n\tyear = {2016},\n\tnote = {Publisher: SPIE},\n\tpages = {012526},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We have performed a study of CVD multiwalled carbon nanotubes (MWCNTs) produced with Fe–Co catalysts with a variable ratio of active metals. The Raman data were considered in combination with the temperature dependence of MWCNT conductivity. The data analysis is based on the point that the value of I2D/ID ratio correlates with the graphene fragment size. The fragments are considered as building blocks of MWCNTs. We showed that MWCNT defectiveness depends on the ratio of bimetallic active components in the Fe–Co catalyst. Thus, the ratio of I2D/ID increases and the D-mode intensity decreases while the Fe content in the catalyst increases. This also points to the reduction of defect number in the bigger graphene fragments. These results correlate with the data on conductivity temperature dependence. Namely, the increase of Fe content in the active component of the Fe–Co catalyst results in the increase of charge carrier concentration, which, in turn, indicates a decrease in MWCNT defectiveness.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"rochal-konevtsova-shevchenko-lorman-softsphericalnanostructureswithadodecagonalquasicrystallikeorder-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://pubs.rsc.org/en/content/articlelanding/2016/sm/c5sm02265g\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'rochal-konevtsova-shevchenko-lorman-softsphericalnanostructureswithadodecagonalquasicrystallikeorder-2016', 'https://pubs.rsc.org/en/content/articlelanding/2016/sm/c5sm02265g', event);\">\n    Soft spherical nanostructures with a dodecagonal quasicrystal-like order.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Rochal, S. B.; Konevtsova, O. V.; Shevchenko, I. A.;  and Lorman, V. L.\n</span>\n\n  \n\n</span>\n\n  <i>Soft Matter</i>, 12(4): 1238–1247. January 2016.\n  <span class=\"note\">Publisher: The Royal Society of Chemistry</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://pubs.rsc.org/en/content/articlelanding/2016/sm/c5sm02265g\"\n     onclick=\"log_download('rochal-konevtsova-shevchenko-lorman-softsphericalnanostructureswithadodecagonalquasicrystallikeorder-2016', 'https://pubs.rsc.org/en/content/articlelanding/2016/sm/c5sm02265g', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Soft spherical nanostructures with a dodecagonal quasicrystal-like order [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1039/C5SM02265G\"\n     onclick=\"log_download('rochal-konevtsova-shevchenko-lorman-softsphericalnanostructureswithadodecagonalquasicrystallikeorder-2016', 'http://doi.org/10.1039/C5SM02265G', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/rochal-konevtsova-shevchenko-lorman-softsphericalnanostructureswithadodecagonalquasicrystallikeorder-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('rochal-konevtsova-shevchenko-lorman-softsphericalnanostructureswithadodecagonalquasicrystallikeorder-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{rochal_soft_2016,\n\ttitle = {Soft spherical nanostructures with a dodecagonal quasicrystal-like order},\n\tvolume = {12},\n\tissn = {1744-6848},\n\turl = {https://pubs.rsc.org/en/content/articlelanding/2016/sm/c5sm02265g},\n\tdoi = {10.1039/C5SM02265G},\n\tabstract = {We develop a theory which predicts curvature-related structural peculiarities of soft spherical nanostructures with a dodecagonal local arrangement of subunits. Spherical templates coated with a thin film of a soft quasicrystal (QC)-forming material constitute the most promising direction to realize these nanostructures. Disordered and perfect spherical nanostructures are simulated using two approaches. The first of them models a random QC-like spherical nanostructure with extended curvature-induced topological defects similar to scars in colloidal spherical crystals. The second approach is inspired by the physics of viral capsids. It deals with the most regular spherical nanostructures with a local QC-like order derived from three well-known planar dodecagonal tilings. We explain how the additional QC-like degrees of freedom assist the nanostructure stabilization and determine the point defect number and location without extended scar formation. Unusual for nanoassemblies snub cube geometry is shown to be the most energetically favorable global organization of these spherical QC nanostructures.},\n\tlanguage = {en},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Soft Matter},\n\tauthor = {Rochal, S. B. and Konevtsova, O. V. and Shevchenko, I. A. and Lorman, V. L.},\n\tmonth = jan,\n\tyear = {2016},\n\tnote = {Publisher: The Royal Society of Chemistry},\n\tpages = {1238--1247},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We develop a theory which predicts curvature-related structural peculiarities of soft spherical nanostructures with a dodecagonal local arrangement of subunits. Spherical templates coated with a thin film of a soft quasicrystal (QC)-forming material constitute the most promising direction to realize these nanostructures. Disordered and perfect spherical nanostructures are simulated using two approaches. The first of them models a random QC-like spherical nanostructure with extended curvature-induced topological defects similar to scars in colloidal spherical crystals. The second approach is inspired by the physics of viral capsids. It deals with the most regular spherical nanostructures with a local QC-like order derived from three well-known planar dodecagonal tilings. We explain how the additional QC-like degrees of freedom assist the nanostructure stabilization and determine the point defect number and location without extended scar formation. Unusual for nanoassemblies snub cube geometry is shown to be the most energetically favorable global organization of these spherical QC nanostructures.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"mukhortov-golovko-biryukov-anokhin-yuzyuk-effectofgrowthmechanismsonthedeformationofaunitcellandpolarizationreversalinbariumstrontiumtitanateheterostructuresonmagnesiumoxide-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S106378421601014X\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'mukhortov-golovko-biryukov-anokhin-yuzyuk-effectofgrowthmechanismsonthedeformationofaunitcellandpolarizationreversalinbariumstrontiumtitanateheterostructuresonmagnesiumoxide-2016', 'https://doi.org/10.1134/S106378421601014X', event);\">\n    Effect of growth mechanisms on the deformation of a unit cell and polarization reversal in barium–strontium titanate heterostructures on magnesium oxide.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Mukhortov, V. M.; Golovko, Y. I.; Biryukov, S. V.; Anokhin, A.;  and Yuzyuk, Y. I.\n</span>\n\n  \n\n</span>\n\n  <i>Technical Physics</i>, 61(1): 91–96. January 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S106378421601014X\"\n     onclick=\"log_download('mukhortov-golovko-biryukov-anokhin-yuzyuk-effectofgrowthmechanismsonthedeformationofaunitcellandpolarizationreversalinbariumstrontiumtitanateheterostructuresonmagnesiumoxide-2016', 'https://doi.org/10.1134/S106378421601014X', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Effect of growth mechanisms on the deformation of a unit cell and polarization reversal in barium–strontium titanate heterostructures on magnesium oxide [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S106378421601014X\"\n     onclick=\"log_download('mukhortov-golovko-biryukov-anokhin-yuzyuk-effectofgrowthmechanismsonthedeformationofaunitcellandpolarizationreversalinbariumstrontiumtitanateheterostructuresonmagnesiumoxide-2016', 'http://doi.org/10.1134/S106378421601014X', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/mukhortov-golovko-biryukov-anokhin-yuzyuk-effectofgrowthmechanismsonthedeformationofaunitcellandpolarizationreversalinbariumstrontiumtitanateheterostructuresonmagnesiumoxide-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('mukhortov-golovko-biryukov-anokhin-yuzyuk-effectofgrowthmechanismsonthedeformationofaunitcellandpolarizationreversalinbariumstrontiumtitanateheterostructuresonmagnesiumoxide-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{mukhortov_effect_2016,\n\ttitle = {Effect of growth mechanisms on the deformation of a unit cell and polarization reversal in barium–strontium titanate heterostructures on magnesium oxide},\n\tvolume = {61},\n\tissn = {1090-6525},\n\turl = {https://doi.org/10.1134/S106378421601014X},\n\tdoi = {10.1134/S106378421601014X},\n\tabstract = {The effect of a growth mechanism on the unit cell strain and the related change in the properties of single-crystal Ba0.8Sr0.2TiO3 films grown on MgO substrates according to the Frank–van der Merwe and Volmer–Weber growth mechanisms is studied. The unit cell strain is shown to depend substantially on the film thickness and the growth mechanism. It is found that the same film–substrate pair can be used to vary stresses in the film from two-dimensional tensile to compressive stresses due to a change in the growth mechanism and the film thickness.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Technical Physics},\n\tauthor = {Mukhortov, V. M. and Golovko, Yu. I. and Biryukov, S. V. and Anokhin, A. and Yuzyuk, Yu. I.},\n\tmonth = jan,\n\tyear = {2016},\n\tkeywords = {Strontium Titanate, Growth Mechanism, Paraelectric Phase, Remanent Polarization, Substrate Plane},\n\tpages = {91--96},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The effect of a growth mechanism on the unit cell strain and the related change in the properties of single-crystal Ba0.8Sr0.2TiO3 films grown on MgO substrates according to the Frank–van der Merwe and Volmer–Weber growth mechanisms is studied. The unit cell strain is shown to depend substantially on the film thickness and the growth mechanism. It is found that the same film–substrate pair can be used to vary stresses in the film from two-dimensional tensile to compressive stresses due to a change in the growth mechanism and the film thickness.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"roshal-myasnikova-rochal-relaxationofinterstitialsinsphericalcolloidalcrystals-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S1386947715302174\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'roshal-myasnikova-rochal-relaxationofinterstitialsinsphericalcolloidalcrystals-2016', 'https://www.sciencedirect.com/science/article/pii/S1386947715302174', event);\">\n    Relaxation of interstitials in spherical colloidal crystals.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Roshal, D. S.; Myasnikova, A. E.;  and Rochal, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Physica E: Low-dimensional Systems and Nanostructures</i>, 75: 295–301. January 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S1386947715302174\"\n     onclick=\"log_download('roshal-myasnikova-rochal-relaxationofinterstitialsinsphericalcolloidalcrystals-2016', 'https://www.sciencedirect.com/science/article/pii/S1386947715302174', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Relaxation of interstitials in spherical colloidal crystals [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.physe.2015.09.036\"\n     onclick=\"log_download('roshal-myasnikova-rochal-relaxationofinterstitialsinsphericalcolloidalcrystals-2016', 'http://doi.org/10.1016/j.physe.2015.09.036', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/roshal-myasnikova-rochal-relaxationofinterstitialsinsphericalcolloidalcrystals-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('roshal-myasnikova-rochal-relaxationofinterstitialsinsphericalcolloidalcrystals-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{roshal_relaxation_2016,\n\ttitle = {Relaxation of interstitials in spherical colloidal crystals},\n\tvolume = {75},\n\tissn = {1386-9477},\n\turl = {https://www.sciencedirect.com/science/article/pii/S1386947715302174},\n\tdoi = {10.1016/j.physe.2015.09.036},\n\tabstract = {Spherical colloidal crystals (CCs) self-assemble on the interface between two liquids. These 2D structures unconventionally combine local hexagonal order and spherical geometry. Nowadays CCs are actively studied by altering their structures. However, the statistical analysis of such experiments results is limited by uniqueness of self-assembled structures and their short lifetime. Here we perform numerical experiments to investigate pathways of CC structure relaxation after the intrusion of interstitial. The process is simulated in the frames of overdamped molecular dynamics method. The relaxation occurs due to interaction with extended topological defects (ETDs) mandatory induced in spherical CCs by their intrinsic Gaussian curvature. Types of relaxation pathways are classified and their probabilities are estimated in the low-temperature region. To analyze the structural changes during the relaxation we use a parent phase approach allowing us to describe the global organization of spherical order. This organization is preserved by only the most typical relaxation pathway resulting in filling one of vacancies integrated inside the ETD areas. In contrast with this pathway the other ones shift the ETDs centers and can strongly reconstruct the internal structure of ETDs. Temperature dependence of the relaxation processes and the mechanism of dislocation unbinding are discussed. Common peculiarities in relaxation of spherical structures and particular fragments of planar hexagonal lattice are found.},\n\turldate = {2023-11-11},\n\tjournal = {Physica E: Low-dimensional Systems and Nanostructures},\n\tauthor = {Roshal, D. S. and Myasnikova, A. E. and Rochal, S. B.},\n\tmonth = jan,\n\tyear = {2016},\n\tkeywords = {Topological defects, Self-assembly, Interstitial, Parent phase, Relaxation, Spherical colloidal crystals},\n\tpages = {295--301},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\BC5X78BR\\\\Roshal и др. - 2016 - Relaxation of interstitials in spherical colloidal.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Spherical colloidal crystals (CCs) self-assemble on the interface between two liquids. These 2D structures unconventionally combine local hexagonal order and spherical geometry. Nowadays CCs are actively studied by altering their structures. However, the statistical analysis of such experiments results is limited by uniqueness of self-assembled structures and their short lifetime. Here we perform numerical experiments to investigate pathways of CC structure relaxation after the intrusion of interstitial. The process is simulated in the frames of overdamped molecular dynamics method. The relaxation occurs due to interaction with extended topological defects (ETDs) mandatory induced in spherical CCs by their intrinsic Gaussian curvature. Types of relaxation pathways are classified and their probabilities are estimated in the low-temperature region. To analyze the structural changes during the relaxation we use a parent phase approach allowing us to describe the global organization of spherical order. This organization is preserved by only the most typical relaxation pathway resulting in filling one of vacancies integrated inside the ETD areas. In contrast with this pathway the other ones shift the ETDs centers and can strongly reconstruct the internal structure of ETDs. Temperature dependence of the relaxation processes and the mechanism of dislocation unbinding are discussed. Common peculiarities in relaxation of spherical structures and particular fragments of planar hexagonal lattice are found.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?doi=10.7868/S0367676516090039\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----2016', 'https://elibrary.ru/item.asp?doi=10.7868/S0367676516090039', event);\">\n    Электрофизические свойства шестикомпонентного состава сегнетомягкой керамики на основе ЦТС.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Акбаева, Г. М.; Гавриляченко, В. Г.; Захаров, Ю. Н.;  and Лутохин, А. Г.\n</span>\n\n  \n\n</span>\n\n  <i>Известия Российской Академии Наук. Серия Физическая</i>, 80(9): 1179–1182.  2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?doi=10.7868/S0367676516090039\"\n     onclick=\"log_download('-----2016', 'https://elibrary.ru/item.asp?doi=10.7868/S0367676516090039', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Электрофизические свойства шестикомпонентного состава сегнетомягкой керамики на основе ЦТС [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.7868/S0367676516090039\"\n     onclick=\"log_download('-----2016', 'http://doi.org/10.7868/S0367676516090039', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>1 download</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2016,\n\ttitle = {Электрофизические свойства шестикомпонентного состава сегнетомягкой керамики на основе ЦТС},\n\tvolume = {80},\n\tissn = {0367-6765},\n\turl = {https://elibrary.ru/item.asp?doi=10.7868/S0367676516090039},\n\tdoi = {10.7868/S0367676516090039},\n\tabstract = {Изучены свойства шестикомпонентного состава сегнетомягкой керамики на основе ЦТС. Установлено, что этот состав проявляет свойства сегнетоэлектрика-релаксора. В сегнетоэлекрической фазе материала обнаружен фазовый переход между двумя ромбоэдрическими фазами R3c → R3m. Поляризация образцов постоянным электрическим полем при охлаждении через точку Кюри расширяет температурный интервал существования фазы R3m по сравнению с поляризацией при комнатной температуре.},\n\tlanguage = {ru},\n\tnumber = {9},\n\turldate = {2023-11-11},\n\tjournal = {Известия Российской Академии Наук. Серия Физическая},\n\tauthor = {Акбаева, Г. М. and Гавриляченко, В. Г. and Захаров, Ю. Н. and Лутохин, А. Г.},\n\tyear = {2016},\n\tpages = {1179--1182},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Изучены свойства шестикомпонентного состава сегнетомягкой керамики на основе ЦТС. Установлено, что этот состав проявляет свойства сегнетоэлектрика-релаксора. В сегнетоэлекрической фазе материала обнаружен фазовый переход между двумя ромбоэдрическими фазами R3c → R3m. Поляризация образцов постоянным электрическим полем при охлаждении через точку Кюри расширяет температурный интервал существования фазы R3m по сравнению с поляризацией при комнатной температуре.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"lerer-timoshenko-kaidashev-puzanov-chernikova-dispersioncharacteristicsofzincoxidenanorodscoatedwiththinsilverlayerandorganizedintwodimensionaluniformarrays-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  Dispersion Characteristics of Zinc Oxide Nanorods Coated with Thin Silver Layer and Organized in Two-Dimensional Uniform Arrays.\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Lerer, A. M.; Timoshenko, P. E.; Kaidashev, E. M.; Puzanov, A. S.;  and Chernikova, T. Y.\n</span>\n\n  \n\n</span>\n\n  In Parinov, I. A.; Chang, S.;  and Topolov, V. Y., editor(s), <i>Advanced Materials</i>, of <i>Springer Proceedings in Physics</i>, pages 317–327, Cham,  2016. Springer International Publishing\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n\n  \n  <a href=\"http://doi.org/10.1007/978-3-319-26324-3_22\"\n     onclick=\"log_download('lerer-timoshenko-kaidashev-puzanov-chernikova-dispersioncharacteristicsofzincoxidenanorodscoatedwiththinsilverlayerandorganizedintwodimensionaluniformarrays-2016', 'http://doi.org/10.1007/978-3-319-26324-3_22', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/lerer-timoshenko-kaidashev-puzanov-chernikova-dispersioncharacteristicsofzincoxidenanorodscoatedwiththinsilverlayerandorganizedintwodimensionaluniformarrays-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('lerer-timoshenko-kaidashev-puzanov-chernikova-dispersioncharacteristicsofzincoxidenanorodscoatedwiththinsilverlayerandorganizedintwodimensionaluniformarrays-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{lerer_dispersion_2016-1,\n\taddress = {Cham},\n\tseries = {Springer {Proceedings} in {Physics}},\n\ttitle = {Dispersion {Characteristics} of {Zinc} {Oxide} {Nanorods} {Coated} with {Thin} {Silver} {Layer} and {Organized} in {Two}-{Dimensional} {Uniform} {Arrays}},\n\tisbn = {978-3-319-26324-3},\n\tdoi = {10.1007/978-3-319-26324-3_22},\n\tabstract = {The problem on electromagnetic waves propagation in a two-dimensional periodic array of zinc oxide nano-waveguides covered with a thin metal film is solved by the method of variables separationMethod of variables separationin cylindrical coordinates. The numerical results obtained by the method are in good agreement with the results computed by the commercial software COMSOL MultiphysicsTM over all optical range and have minor deviations for the wavelength range close to the critical wavelength. Resonances located at the amplitude-frequency characteristics of optical nano-antennas may be interpreted as resonances of circular bilayer nano-wave-guide segments with the ZnO core covered with thin metal shell. The results may also be used to predict the resonance wavelength of two-dimensional periodic arrays of ZnO nanorodsZnO nanorods, coated with a thin metal layer and grown on a dielectric substrate.},\n\tlanguage = {en},\n\tbooktitle = {Advanced {Materials}},\n\tpublisher = {Springer International Publishing},\n\tauthor = {Lerer, A. M. and Timoshenko, P. E. and Kaidashev, E. M. and Puzanov, A. S. and Chernikova, T. Y.},\n\teditor = {Parinov, Ivan A. and Chang, Shun-Hsyung and Topolov, Vitaly Yu.},\n\tyear = {2016},\n\tkeywords = {Complex Dielectric Constant, Critical Wavelength, Resonant Wavelength, Thin Metal Film, Unknown Coefficient},\n\tpages = {317--327},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The problem on electromagnetic waves propagation in a two-dimensional periodic array of zinc oxide nano-waveguides covered with a thin metal film is solved by the method of variables separationMethod of variables separationin cylindrical coordinates. The numerical results obtained by the method are in good agreement with the results computed by the commercial software COMSOL MultiphysicsTM over all optical range and have minor deviations for the wavelength range close to the critical wavelength. Resonances located at the amplitude-frequency characteristics of optical nano-antennas may be interpreted as resonances of circular bilayer nano-wave-guide segments with the ZnO core covered with thin metal shell. The results may also be used to predict the resonance wavelength of two-dimensional periodic arrays of ZnO nanorodsZnO nanorods, coated with a thin metal layer and grown on a dielectric substrate.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=26607463\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------2016', 'https://elibrary.ru/item.asp?id=26607463', event);\">\n    Оптические наноантенны на новых плазмонных материалах на основе оксида цинка.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Лерер, А. М.; Тимошенко, П. Е.; Головачева, Е. В.; Кайдашев, Е. М.;  and Пузанов, А. С.\n</span>\n\n  \n\n</span>\n\n  <i>Электроника И Микроэлектроника Свч</i>, 1: 279–282.  2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=26607463\"\n     onclick=\"log_download('------2016', 'https://elibrary.ru/item.asp?id=26607463', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Оптические наноантенны на новых плазмонных материалах на основе оксида цинка [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2016-1,\n\ttitle = {Оптические наноантенны на новых плазмонных материалах на основе оксида цинка},\n\tvolume = {1},\n\turl = {https://elibrary.ru/item.asp?id=26607463},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tjournal = {Электроника И Микроэлектроника Свч},\n\tauthor = {Лерер, А. М. and Тимошенко, П. Е. and Головачева, Е. В. and Кайдашев, Е. М. and Пузанов, А. С.},\n\tyear = {2016},\n\tkeywords = {Дифракция, Оптические Наноантенны, Конечно-Элементное Моделирование, Фотонно-Кристаллические Структуры, Zno Наностержни, ⛔ No DOI found},\n\tpages = {279--282},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-kalinchuck-timoshenko-shirokov-timoshenko-yuzyuk-acousticpropertiesofbst0textrm8filmstunablebybiaselectricfield-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://ieeexplore.ieee.org/document/7819084?reload=true\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-kalinchuck-timoshenko-shirokov-timoshenko-yuzyuk-acousticpropertiesofbst0textrm8filmstunablebybiaselectricfield-2016', 'https://ieeexplore.ieee.org/document/7819084?reload=true', event);\">\n    Acoustic properties of BST0$_{\\textrm{8}}$ films tunable by bias electric field.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B; Kalinchuck, V. V.; Timoshenko, P. E.; Shirokov, V. B.; Timoshenko, P. E.;  and Yuzyuk, Y. I.\n</span>\n\n  \n\n</span>\n\n  In <i>2016 Dynamics of Systems, Mechanisms and Machines (Dynamics)</i>, pages 1–4, November 2016. \n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://ieeexplore.ieee.org/document/7819084?reload=true\"\n     onclick=\"log_download('shirokov-kalinchuck-timoshenko-shirokov-timoshenko-yuzyuk-acousticpropertiesofbst0textrm8filmstunablebybiaselectricfield-2016', 'https://ieeexplore.ieee.org/document/7819084?reload=true', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Acoustic properties of BST0$_{\\textrm{8}}$ films tunable by bias electric field [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1109/Dynamics.2016.7819084\"\n     onclick=\"log_download('shirokov-kalinchuck-timoshenko-shirokov-timoshenko-yuzyuk-acousticpropertiesofbst0textrm8filmstunablebybiaselectricfield-2016', 'http://doi.org/10.1109/Dynamics.2016.7819084', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-kalinchuck-timoshenko-shirokov-timoshenko-yuzyuk-acousticpropertiesofbst0textrm8filmstunablebybiaselectricfield-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-kalinchuck-timoshenko-shirokov-timoshenko-yuzyuk-acousticpropertiesofbst0textrm8filmstunablebybiaselectricfield-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{shirokov_acoustic_2016,\n\ttitle = {Acoustic properties of {BST0}$_{\\textrm{8}}$ films tunable by bias electric field},\n\turl = {https://ieeexplore.ieee.org/document/7819084?reload=true},\n\tdoi = {10.1109/Dynamics.2016.7819084},\n\tabstract = {The effect of a bias electric field on the material coefficients of Ba0.8Sr0.2O3 (BST08) thin films was studied. The material constants are derived from piezoelectric effect equations by the linearization of nonlinear phenomenological state equations. The numerical results are obtained for the case of BST08 film with a misfit strain value equal to −4×10−3 located on a cubic substrate for the (001) cut plane in the electric field up to 5×107V/m applied along [100] direction in the film plane. The electromechanical coupling coefficient k11 reaches a maximum under applied electric field.},\n\turldate = {2023-11-11},\n\tbooktitle = {2016 {Dynamics} of {Systems}, {Mechanisms} and {Machines} ({Dynamics})},\n\tauthor = {Shirokov, V. B and Kalinchuck, V. V. and Timoshenko, P. E. and Shirokov, V. B. and Timoshenko, P. E. and Yuzyuk, Yu. I.},\n\tmonth = nov,\n\tyear = {2016},\n\tpages = {1--4},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The effect of a bias electric field on the material coefficients of Ba0.8Sr0.2O3 (BST08) thin films was studied. The material constants are derived from piezoelectric effect equations by the linearization of nonlinear phenomenological state equations. The numerical results are obtained for the case of BST08 film with a misfit strain value equal to −4×10−3 located on a cubic substrate for the (001) cut plane in the electric field up to 5×107V/m applied along [100] direction in the film plane. The electromechanical coupling coefficient k11 reaches a maximum under applied electric field.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"talanov-talanov-shirokov-theoryoftheformationofptextrm4textlesssubtextgreater132textlesssubtextgreaterptextrm4textlesssubtextgreater332textlesssubtextgreaterphasespinels-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1063774516020280\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'talanov-talanov-shirokov-theoryoftheformationofptextrm4textlesssubtextgreater132textlesssubtextgreaterptextrm4textlesssubtextgreater332textlesssubtextgreaterphasespinels-2016', 'https://doi.org/10.1134/S1063774516020280', event);\">\n    Theory of the formation of P$_{\\textrm{4{\\textless}sub{\\textgreater}1}}$32\\textless/sub\\textgreater(P$_{\\textrm{4{\\textless}sub{\\textgreater}3}}$32\\textless/sub\\textgreater)-phase spinels.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Talanov, V. M.; Talanov, M. V.;  and Shirokov, V. B.\n</span>\n\n  \n\n</span>\n\n  <i>Crystallography Reports</i>, 61(2): 159–169. March 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1063774516020280\"\n     onclick=\"log_download('talanov-talanov-shirokov-theoryoftheformationofptextrm4textlesssubtextgreater132textlesssubtextgreaterptextrm4textlesssubtextgreater332textlesssubtextgreaterphasespinels-2016', 'https://doi.org/10.1134/S1063774516020280', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Theory of the formation of P$_{\\textrm{4{\\textless}sub{\\textgreater}1}}$32\\textless/sub\\textgreater(P$_{\\textrm{4{\\textless}sub{\\textgreater}3}}$32\\textless/sub\\textgreater)-phase spinels [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1063774516020280\"\n     onclick=\"log_download('talanov-talanov-shirokov-theoryoftheformationofptextrm4textlesssubtextgreater132textlesssubtextgreaterptextrm4textlesssubtextgreater332textlesssubtextgreaterphasespinels-2016', 'http://doi.org/10.1134/S1063774516020280', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/talanov-talanov-shirokov-theoryoftheformationofptextrm4textlesssubtextgreater132textlesssubtextgreaterptextrm4textlesssubtextgreater332textlesssubtextgreaterphasespinels-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('talanov-talanov-shirokov-theoryoftheformationofptextrm4textlesssubtextgreater132textlesssubtextgreaterptextrm4textlesssubtextgreater332textlesssubtextgreaterphasespinels-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{talanov_theory_2016,\n\ttitle = {Theory of the formation of {P}$_{\\textrm{4{\\textless}sub{\\textgreater}1}}$32{\\textless}/sub{\\textgreater}({P}$_{\\textrm{4{\\textless}sub{\\textgreater}3}}$32{\\textless}/sub{\\textgreater})-phase spinels},\n\tvolume = {61},\n\tissn = {1562-689X},\n\turl = {https://doi.org/10.1134/S1063774516020280},\n\tdoi = {10.1134/S1063774516020280},\n\tabstract = {A group-theoretical, thermodynamic, and structural study of the formation of P4132(P4332) spinel modification has been performed. In particular, the occurrence of unique hyper-kagome atomic order is analyzed. The critical order parameter inducing a phase transition is established. It is shown that the calculated structure of the low-symmetry P4132(P4332) phase is formed as a result of displacements of atoms of all types and due to the cation and anion ordering. The problem of the occurrence of unique hyper-kagome atomic order in the structures of P4132(P4332) spinel modifications is considered theoretically. It is proven within the Landau theory of phase transitions that the P4132(P4332) phase can be formed from the high-symmetry Fd3m phase with an ideal spinel structure only as a result of first-order phase transition. Therefore, the formation of hyper-kagome sublattice in the P4132(P4332) phase is accompanied by a significant transformation of the spinel structure.},\n\tlanguage = {en},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Crystallography Reports},\n\tauthor = {Talanov, V. M. and Talanov, M. V. and Shirokov, V. B.},\n\tmonth = mar,\n\tyear = {2016},\n\tkeywords = {Crystallography Report, Ible Representation, Multicritical Point, Spinel Structure, Unusual Physical Property},\n\tpages = {159--169},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A group-theoretical, thermodynamic, and structural study of the formation of P4132(P4332) spinel modification has been performed. In particular, the occurrence of unique hyper-kagome atomic order is analyzed. The critical order parameter inducing a phase transition is established. It is shown that the calculated structure of the low-symmetry P4132(P4332) phase is formed as a result of displacements of atoms of all types and due to the cation and anion ordering. The problem of the occurrence of unique hyper-kagome atomic order in the structures of P4132(P4332) spinel modifications is considered theoretically. It is proven within the Landau theory of phase transitions that the P4132(P4332) phase can be formed from the high-symmetry Fd3m phase with an ideal spinel structure only as a result of first-order phase transition. Therefore, the formation of hyper-kagome sublattice in the P4132(P4332) phase is accompanied by a significant transformation of the spinel structure.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"makarova-grebenev-vasilev-dmitricheva-komornikov-dolbinina-mikheikin-structureofcstextrm4hsotextrm4textrm3htextrm2potextrm4singlecrystals-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1063774516010119\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'makarova-grebenev-vasilev-dmitricheva-komornikov-dolbinina-mikheikin-structureofcstextrm4hsotextrm4textrm3htextrm2potextrm4singlecrystals-2016', 'https://doi.org/10.1134/S1063774516010119', event);\">\n    Structure of Cs$_{\\textrm{4}}$(HSO$_{\\textrm{4}}$)$_{\\textrm{3}}$(H$_{\\textrm{2}}$PO$_{\\textrm{4}}$) single crystals.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Makarova, I. P.; Grebenev, V. V.; Vasil’ev, I. I.; Dmitricheva, E. V.; Komornikov, V. A.; Dolbinina, V. V.;  and Mikheikin, A. S.\n</span>\n\n  \n\n</span>\n\n  <i>Crystallography Reports</i>, 61(1): 18–23. January 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1063774516010119\"\n     onclick=\"log_download('makarova-grebenev-vasilev-dmitricheva-komornikov-dolbinina-mikheikin-structureofcstextrm4hsotextrm4textrm3htextrm2potextrm4singlecrystals-2016', 'https://doi.org/10.1134/S1063774516010119', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Structure of Cs$_{\\textrm{4}}$(HSO$_{\\textrm{4}}$)$_{\\textrm{3}}$(H$_{\\textrm{2}}$PO$_{\\textrm{4}}$) single crystals [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1063774516010119\"\n     onclick=\"log_download('makarova-grebenev-vasilev-dmitricheva-komornikov-dolbinina-mikheikin-structureofcstextrm4hsotextrm4textrm3htextrm2potextrm4singlecrystals-2016', 'http://doi.org/10.1134/S1063774516010119', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/makarova-grebenev-vasilev-dmitricheva-komornikov-dolbinina-mikheikin-structureofcstextrm4hsotextrm4textrm3htextrm2potextrm4singlecrystals-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('makarova-grebenev-vasilev-dmitricheva-komornikov-dolbinina-mikheikin-structureofcstextrm4hsotextrm4textrm3htextrm2potextrm4singlecrystals-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{makarova_structure_2016,\n\ttitle = {Structure of {Cs}$_{\\textrm{4}}$({HSO}$_{\\textrm{4}}$)$_{\\textrm{3}}$({H}$_{\\textrm{2}}${PO}$_{\\textrm{4}}$) single crystals},\n\tvolume = {61},\n\tissn = {1562-689X},\n\turl = {https://doi.org/10.1134/S1063774516010119},\n\tdoi = {10.1134/S1063774516010119},\n\tabstract = {Single crystals of Cs4(HSO4)3(H2PO4) are synthesized and studied for the first time. The new compound is found in the course of studies of the phase diagram of the CsHSO4–CsH2PO4–H2O triple system. Data on the atomic crystal structure of single-crystalline and powder specimens, as well as on structural phase transitions, are obtained.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Crystallography Reports},\n\tauthor = {Makarova, I. P. and Grebenev, V. V. and Vasil’ev, I. I. and Dmitricheva, E. V. and Komornikov, V. A. and Dolbinina, V. V. and Mikheikin, A. S.},\n\tmonth = jan,\n\tyear = {2016},\n\tkeywords = {Crystallography Report, High Protonic Conductivity, Potassium Atom, Structural Phase Transition, Thermal Vibration},\n\tpages = {18--23},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Single crystals of Cs4(HSO4)3(H2PO4) are synthesized and studied for the first time. The new compound is found in the course of studies of the phase diagram of the CsHSO4–CsH2PO4–H2O triple system. Data on the atomic crystal structure of single-crystalline and powder specimens, as well as on structural phase transitions, are obtained.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-kalinchuk-shakhovoi-yuzyuk-physicalpropertiesofbatextrm08srtextrm02tiotextrm3thinfilms-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1063783416100346\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-kalinchuk-shakhovoi-yuzyuk-physicalpropertiesofbatextrm08srtextrm02tiotextrm3thinfilms-2016', 'https://doi.org/10.1134/S1063783416100346', event);\">\n    Physical properties of Ba$_{\\textrm{0.8}}$Sr$_{\\textrm{0.2}}$TiO$_{\\textrm{3}}$ thin films.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.; Kalinchuk, V. V.; Shakhovoi, R. A.;  and Yuzyuk, Y. I.\n</span>\n\n  \n\n</span>\n\n  <i>Physics of the Solid State</i>, 58(10): 2035–2039. October 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1063783416100346\"\n     onclick=\"log_download('shirokov-kalinchuk-shakhovoi-yuzyuk-physicalpropertiesofbatextrm08srtextrm02tiotextrm3thinfilms-2016', 'https://doi.org/10.1134/S1063783416100346', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Physical properties of Ba$_{\\textrm{0.8}}$Sr$_{\\textrm{0.2}}$TiO$_{\\textrm{3}}$ thin films [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1063783416100346\"\n     onclick=\"log_download('shirokov-kalinchuk-shakhovoi-yuzyuk-physicalpropertiesofbatextrm08srtextrm02tiotextrm3thinfilms-2016', 'http://doi.org/10.1134/S1063783416100346', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-kalinchuk-shakhovoi-yuzyuk-physicalpropertiesofbatextrm08srtextrm02tiotextrm3thinfilms-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-kalinchuk-shakhovoi-yuzyuk-physicalpropertiesofbatextrm08srtextrm02tiotextrm3thinfilms-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_physical_2016-1,\n\ttitle = {Physical properties of {Ba}$_{\\textrm{0.8}}${Sr}$_{\\textrm{0.2}}${TiO}$_{\\textrm{3}}$ thin films},\n\tvolume = {58},\n\tissn = {1090-6460},\n\turl = {https://doi.org/10.1134/S1063783416100346},\n\tdoi = {10.1134/S1063783416100346},\n\tabstract = {The behavior of material constants in ferroelectric Ba0.8Sr0.2TiO3 thin films is studied depending on the misfit strain at room temperature in the context of nonlinear thermodynamic potential of the phenomenological theory. Some constants are found to undergo drastic changes with the alternating strain at the interfaces. The gathered results allow one to evaluate the material constants for a specific film and to outline the direction in searching the ways to synthesize films with the needed properties.},\n\tlanguage = {en},\n\tnumber = {10},\n\turldate = {2023-11-11},\n\tjournal = {Physics of the Solid State},\n\tauthor = {Shirokov, V. B. and Kalinchuk, V. V. and Shakhovoi, R. A. and Yuzyuk, Yu. I.},\n\tmonth = oct,\n\tyear = {2016},\n\tpages = {2035--2039},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The behavior of material constants in ferroelectric Ba0.8Sr0.2TiO3 thin films is studied depending on the misfit strain at room temperature in the context of nonlinear thermodynamic potential of the phenomenological theory. Some constants are found to undergo drastic changes with the alternating strain at the interfaces. The gathered results allow one to evaluate the material constants for a specific film and to outline the direction in searching the ways to synthesize films with the needed properties.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"razumnaya-yuzyuk-zakharchenko-tikhonov-ortega-kumar-katiyar-elmarssi-etal-phasetransitioninferroelectricbatiotextrm3srtiotextrm3superlatticeramanspectroscopystudies-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/00150193.2016.1199201\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'razumnaya-yuzyuk-zakharchenko-tikhonov-ortega-kumar-katiyar-elmarssi-etal-phasetransitioninferroelectricbatiotextrm3srtiotextrm3superlatticeramanspectroscopystudies-2016', 'https://doi.org/10.1080/00150193.2016.1199201', event);\">\n    Phase transition in ferroelectric BaTiO$_{\\textrm{3}}$/SrTiO$_{\\textrm{3}}$ superlattice: Raman spectroscopy studies.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Razumnaya, A. G.; Yuzyuk, Y. I.; Zakharchenko, I. N.; Tikhonov, Y. A.; Ortega, N.; Kumar, A.; Katiyar, R. S.; El Marssi, M.;  and Lukyanchuk, I. A.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 501(1): 61–69. September 2016.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2016.1199201</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/00150193.2016.1199201\"\n     onclick=\"log_download('razumnaya-yuzyuk-zakharchenko-tikhonov-ortega-kumar-katiyar-elmarssi-etal-phasetransitioninferroelectricbatiotextrm3srtiotextrm3superlatticeramanspectroscopystudies-2016', 'https://doi.org/10.1080/00150193.2016.1199201', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Phase transition in ferroelectric BaTiO$_{\\textrm{3}}$/SrTiO$_{\\textrm{3}}$ superlattice: Raman spectroscopy studies [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150193.2016.1199201\"\n     onclick=\"log_download('razumnaya-yuzyuk-zakharchenko-tikhonov-ortega-kumar-katiyar-elmarssi-etal-phasetransitioninferroelectricbatiotextrm3srtiotextrm3superlatticeramanspectroscopystudies-2016', 'http://doi.org/10.1080/00150193.2016.1199201', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/razumnaya-yuzyuk-zakharchenko-tikhonov-ortega-kumar-katiyar-elmarssi-etal-phasetransitioninferroelectricbatiotextrm3srtiotextrm3superlatticeramanspectroscopystudies-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('razumnaya-yuzyuk-zakharchenko-tikhonov-ortega-kumar-katiyar-elmarssi-etal-phasetransitioninferroelectricbatiotextrm3srtiotextrm3superlatticeramanspectroscopystudies-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{razumnaya_phase_2016,\n\ttitle = {Phase transition in ferroelectric {BaTiO}$_{\\textrm{3}}$/{SrTiO}$_{\\textrm{3}}$ superlattice: {Raman} spectroscopy studies},\n\tvolume = {501},\n\tissn = {0015-0193},\n\tshorttitle = {Phase transition in ferroelectric {BaTiO3}/{SrTiO3} superlattice},\n\turl = {https://doi.org/10.1080/00150193.2016.1199201},\n\tdoi = {10.1080/00150193.2016.1199201},\n\tabstract = {BaTiO3/SrTiO3 superlattice has been grown on (001)MgO substrate by pulsed laser deposition. The unit cell parameters of BaTiO3 and SrTiO3 layers and modulation period have been determined using X-ray diffraction. It was found that BaTiO3 and SrTiO3 layers revealed the pseudo-tetragonal distortion with out-of-plane and in-plane polarization, respectively. Electrostatic interaction of the alternating layers leads to the polarization rotations and to the symmetry lowering of the superlattice to orthorhombic or monoclinic with partial depolarization of the Raman spectra. It was found that the phase transition to the paraelectric phase occurs at ∼480 K.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Ferroelectrics},\n\tauthor = {Razumnaya, A. G. and Yuzyuk, Yu. I. and Zakharchenko, I. N. and Tikhonov, Yu. A. and Ortega, N. and Kumar, A. and Katiyar, R. S. and El Marssi, M. and Lukyanchuk, I. A.},\n\tmonth = sep,\n\tyear = {2016},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/00150193.2016.1199201},\n\tkeywords = {Raman spectroscopy, soft mode, superlattices},\n\tpages = {61--69},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  BaTiO3/SrTiO3 superlattice has been grown on (001)MgO substrate by pulsed laser deposition. The unit cell parameters of BaTiO3 and SrTiO3 layers and modulation period have been determined using X-ray diffraction. It was found that BaTiO3 and SrTiO3 layers revealed the pseudo-tetragonal distortion with out-of-plane and in-plane polarization, respectively. Electrostatic interaction of the alternating layers leads to the polarization rotations and to the symmetry lowering of the superlattice to orthorhombic or monoclinic with partial depolarization of the Raman spectra. It was found that the phase transition to the paraelectric phase occurs at ∼480 K.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"makarova-grebenev-dmitricheva-vasiliev-komornikov-dolbinina-mikheykin-mtextrmmhtextrmnxotextrm4textrmmn2crystalsstructurephasetransitionshydrogenbondsconductivityiistructureandpropertiesofcstextrm3hsotextrm4textrm2htextrm2potextrm4andcstextrm4hsotextrm4textrm3htextrm2potextrm4singlecrystals-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://scripts.iucr.org/cgi-bin/paper?bp5085\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'makarova-grebenev-dmitricheva-vasiliev-komornikov-dolbinina-mikheykin-mtextrmmhtextrmnxotextrm4textrmmn2crystalsstructurephasetransitionshydrogenbondsconductivityiistructureandpropertiesofcstextrm3hsotextrm4textrm2htextrm2potextrm4andcstextrm4hsotextrm4textrm3htextrm2potextrm4singlecrystals-2016', 'http://scripts.iucr.org/cgi-bin/paper?bp5085', event);\">\n    M$_{\\textrm{m}}$H$_{\\textrm{n}}$(XO$_{\\textrm{4}}$)$_{\\textrm{(m + n)/2}}$ crystals: structure, phase transitions, hydrogen bonds, conductivity. II. Structure and properties of Cs$_{\\textrm{3}}$(HSO$_{\\textrm{4}}$)$_{\\textrm{2}}$(H$_{\\textrm{2}}$PO$_{\\textrm{4}}$) and Cs$_{\\textrm{4}}$(HSO$_{\\textrm{4}}$)$_{\\textrm{3}}$(H$_{\\textrm{2}}$PO$_{\\textrm{4}}$) single crystals.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Makarova, I.; Grebenev, V.; Dmitricheva, E.; Vasiliev, I.; Komornikov, V.; Dolbinina, V.;  and Mikheykin, A.\n</span>\n\n  \n\n</span>\n\n  <i>Acta Crystallographica Section B: Structural Science, Crystal Engineering and Materials</i>, 72(1): 133–141. February 2016.\n  <span class=\"note\">Number: 1 Publisher: International Union of Crystallography</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://scripts.iucr.org/cgi-bin/paper?bp5085\"\n     onclick=\"log_download('makarova-grebenev-dmitricheva-vasiliev-komornikov-dolbinina-mikheykin-mtextrmmhtextrmnxotextrm4textrmmn2crystalsstructurephasetransitionshydrogenbondsconductivityiistructureandpropertiesofcstextrm3hsotextrm4textrm2htextrm2potextrm4andcstextrm4hsotextrm4textrm3htextrm2potextrm4singlecrystals-2016', 'http://scripts.iucr.org/cgi-bin/paper?bp5085', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"M$_{\\textrm{m}}$H$_{\\textrm{n}}$(XO$_{\\textrm{4}}$)$_{\\textrm{(m + n)/2}}$ crystals: structure, phase transitions, hydrogen bonds, conductivity. II. Structure and properties of Cs$_{\\textrm{3}}$(HSO$_{\\textrm{4}}$)$_{\\textrm{2}}$(H$_{\\textrm{2}}$PO$_{\\textrm{4}}$) and Cs$_{\\textrm{4}}$(HSO$_{\\textrm{4}}$)$_{\\textrm{3}}$(H$_{\\textrm{2}}$PO$_{\\textrm{4}}$) single crystals [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1107/S2052520615023069\"\n     onclick=\"log_download('makarova-grebenev-dmitricheva-vasiliev-komornikov-dolbinina-mikheykin-mtextrmmhtextrmnxotextrm4textrmmn2crystalsstructurephasetransitionshydrogenbondsconductivityiistructureandpropertiesofcstextrm3hsotextrm4textrm2htextrm2potextrm4andcstextrm4hsotextrm4textrm3htextrm2potextrm4singlecrystals-2016', 'http://doi.org/10.1107/S2052520615023069', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/makarova-grebenev-dmitricheva-vasiliev-komornikov-dolbinina-mikheykin-mtextrmmhtextrmnxotextrm4textrmmn2crystalsstructurephasetransitionshydrogenbondsconductivityiistructureandpropertiesofcstextrm3hsotextrm4textrm2htextrm2potextrm4andcstextrm4hsotextrm4textrm3htextrm2potextrm4singlecrystals-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('makarova-grebenev-dmitricheva-vasiliev-komornikov-dolbinina-mikheykin-mtextrmmhtextrmnxotextrm4textrmmn2crystalsstructurephasetransitionshydrogenbondsconductivityiistructureandpropertiesofcstextrm3hsotextrm4textrm2htextrm2potextrm4andcstextrm4hsotextrm4textrm3htextrm2potextrm4singlecrystals-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{makarova_mmhnxo4m_2016,\n\ttitle = {M$_{\\textrm{m}}${H}$_{\\textrm{n}}$({XO}$_{\\textrm{4}}$)$_{\\textrm{(m + n)/2}}$ crystals: structure, phase transitions, hydrogen bonds, conductivity. {II}. {Structure} and properties of {Cs}$_{\\textrm{3}}$({HSO}$_{\\textrm{4}}$)$_{\\textrm{2}}$({H}$_{\\textrm{2}}${PO}$_{\\textrm{4}}$) and {Cs}$_{\\textrm{4}}$({HSO}$_{\\textrm{4}}$)$_{\\textrm{3}}$({H}$_{\\textrm{2}}${PO}$_{\\textrm{4}}$) single crystals},\n\tvolume = {72},\n\tcopyright = {Copyright (c) 2016 International Union of Crystallography},\n\tissn = {2052-5206},\n\tshorttitle = {{MmHn}({XO4})(m + n)/2 crystals},\n\turl = {http://scripts.iucr.org/cgi-bin/paper?bp5085},\n\tdoi = {10.1107/S2052520615023069},\n\tabstract = {Cs3(HSO4)2(H2PO4) and Cs4(HSO4)3(H2PO4) single crystals were obtained for the first time based on a systematic study of the phase diagram of the CsHSO4–CsH2PO4–H2O ternary system. To reveal the structural conditionality for anomalies in physical properties, including dielectric and optical properties, diffraction studies of the crystal structure of Cs3(HSO4)2(H2PO4) and Cs4(HSO4)3(H2PO4) were performed, and their common structural features and differences were analyzed.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Acta Crystallographica Section B: Structural Science, Crystal Engineering and Materials},\n\tauthor = {Makarova, I. and Grebenev, V. and Dmitricheva, E. and Vasiliev, I. and Komornikov, V. and Dolbinina, V. and Mikheykin, A.},\n\tmonth = feb,\n\tyear = {2016},\n\tnote = {Number: 1\nPublisher: International Union of Crystallography},\n\tpages = {133--141},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Cs3(HSO4)2(H2PO4) and Cs4(HSO4)3(H2PO4) single crystals were obtained for the first time based on a systematic study of the phase diagram of the CsHSO4–CsH2PO4–H2O ternary system. To reveal the structural conditionality for anomalies in physical properties, including dielectric and optical properties, diffraction studies of the crystal structure of Cs3(HSO4)2(H2PO4) and Cs4(HSO4)3(H2PO4) were performed, and their common structural features and differences were analyzed.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"andreeva-pertsev-andronikova-filimonov-leontiev-leontyev-vakhrushev-domainstructuresandcorrelatedoutofplaneandinplanepolarizationreorientationsinpbzrtextrm096titextrm004otextrm3singlecrystalviapiezoresponseforcemicroscopy-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.4962991\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'andreeva-pertsev-andronikova-filimonov-leontiev-leontyev-vakhrushev-domainstructuresandcorrelatedoutofplaneandinplanepolarizationreorientationsinpbzrtextrm096titextrm004otextrm3singlecrystalviapiezoresponseforcemicroscopy-2016', 'https://doi.org/10.1063/1.4962991', event);\">\n    Domain structures and correlated out-of-plane and in-plane polarization reorientations in Pb(Zr$_{\\textrm{0.96}}$Ti$_{\\textrm{0.04}}$)O$_{\\textrm{3}}$ single crystal via piezoresponse force microscopy.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Andreeva, N. V.; Pertsev, N. A.; Andronikova, D. A.; Filimonov, A. V.; Leontiev, N. G.; Leontyev, I. N.;  and Vakhrushev, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>AIP Advances</i>, 6(9): 095211. September 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.4962991\"\n     onclick=\"log_download('andreeva-pertsev-andronikova-filimonov-leontiev-leontyev-vakhrushev-domainstructuresandcorrelatedoutofplaneandinplanepolarizationreorientationsinpbzrtextrm096titextrm004otextrm3singlecrystalviapiezoresponseforcemicroscopy-2016', 'https://doi.org/10.1063/1.4962991', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Domain structures and correlated out-of-plane and in-plane polarization reorientations in Pb(Zr$_{\\textrm{0.96}}$Ti$_{\\textrm{0.04}}$)O$_{\\textrm{3}}$ single crystal via piezoresponse force microscopy [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.4962991\"\n     onclick=\"log_download('andreeva-pertsev-andronikova-filimonov-leontiev-leontyev-vakhrushev-domainstructuresandcorrelatedoutofplaneandinplanepolarizationreorientationsinpbzrtextrm096titextrm004otextrm3singlecrystalviapiezoresponseforcemicroscopy-2016', 'http://doi.org/10.1063/1.4962991', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/andreeva-pertsev-andronikova-filimonov-leontiev-leontyev-vakhrushev-domainstructuresandcorrelatedoutofplaneandinplanepolarizationreorientationsinpbzrtextrm096titextrm004otextrm3singlecrystalviapiezoresponseforcemicroscopy-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('andreeva-pertsev-andronikova-filimonov-leontiev-leontyev-vakhrushev-domainstructuresandcorrelatedoutofplaneandinplanepolarizationreorientationsinpbzrtextrm096titextrm004otextrm3singlecrystalviapiezoresponseforcemicroscopy-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{andreeva_domain_2016,\n\ttitle = {Domain structures and correlated out-of-plane and in-plane polarization reorientations in {Pb}({Zr}$_{\\textrm{0.96}}${Ti}$_{\\textrm{0.04}}$){O}$_{\\textrm{3}}$ single crystal via piezoresponse force microscopy},\n\tvolume = {6},\n\tissn = {2158-3226},\n\turl = {https://doi.org/10.1063/1.4962991},\n\tdoi = {10.1063/1.4962991},\n\tabstract = {Pb(Zr1-xTix)O3 single crystal with a low titanium content (x = 4\\%) was studied by the piezoresponse force microscopy (PFM) and X-ray diffraction (XRD). The XRD studies showed that the crystal faces are orthogonal to the principal cubic axes and confirmed the existence of an intermediate phase between the high-temperature paraelectric (PE) phase and the low-temperature antiferroelectric (AFE) one. A significant temperature hysteresis of phase transitions was observed by the XRD: On heating, the AFE state transforms into the intermediate one at about 373 K and the PE phase appears at 508 K, whereas on cooling the intermediate phase forms at 503 K and persists down to at least 313 K. The PFM investigation was focused on the intermediate phase and involved measurements of both out-of-plane and in-plane electromechanical responses of the (001)-oriented crystal face. The PFM images revealed the presence of polarization patterns switchable by an applied electric field, which confirms the ferroelectric character of the intermediate phase. Importantly, two types of regular domain structures were found, which differ by the spatial orientation of domain walls. The reconstruction of polarization configurations in the observed domain structures showed that one of them is a purely ferroelectric 180° structure with domain walls orthogonal to the crystal surface and parallel to one of the ⟨111⟩ pseudocubic directions. Another one is a ferroelectric-ferroelastic domain structure with the 71° walls parallel to the \\{101\\} or \\{011\\} crystallographic planes. Remarkably, this domain structure shows correlated out-of-plane and in-plane polarization reorientations after the poling with the aid of the microscope tip.},\n\tnumber = {9},\n\turldate = {2023-11-11},\n\tjournal = {AIP Advances},\n\tauthor = {Andreeva, N. V. and Pertsev, N. A. and Andronikova, D. A. and Filimonov, A. V. and Leontiev, N. G. and Leontyev, I. N. and Vakhrushev, S. B.},\n\tmonth = sep,\n\tyear = {2016},\n\tpages = {095211},\n\tfile = {Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\QV2ANVMG\\\\Andreeva и др. - 2016 - Domain structures and correlated out-of-plane and .pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Pb(Zr1-xTix)O3 single crystal with a low titanium content (x = 4%) was studied by the piezoresponse force microscopy (PFM) and X-ray diffraction (XRD). The XRD studies showed that the crystal faces are orthogonal to the principal cubic axes and confirmed the existence of an intermediate phase between the high-temperature paraelectric (PE) phase and the low-temperature antiferroelectric (AFE) one. A significant temperature hysteresis of phase transitions was observed by the XRD: On heating, the AFE state transforms into the intermediate one at about 373 K and the PE phase appears at 508 K, whereas on cooling the intermediate phase forms at 503 K and persists down to at least 313 K. The PFM investigation was focused on the intermediate phase and involved measurements of both out-of-plane and in-plane electromechanical responses of the (001)-oriented crystal face. The PFM images revealed the presence of polarization patterns switchable by an applied electric field, which confirms the ferroelectric character of the intermediate phase. Importantly, two types of regular domain structures were found, which differ by the spatial orientation of domain walls. The reconstruction of polarization configurations in the observed domain structures showed that one of them is a purely ferroelectric 180° structure with domain walls orthogonal to the crystal surface and parallel to one of the ⟨111⟩ pseudocubic directions. Another one is a ferroelectric-ferroelastic domain structure with the 71° walls parallel to the \\101\\ or \\011\\ crystallographic planes. Remarkably, this domain structure shows correlated out-of-plane and in-plane polarization reorientations after the poling with the aid of the microscope tip.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"googlev-kozakov-kochur-nikolskii-torgashev-zvolenskaya-determiningthevalencestateofmanganeseionsincomplexoxideslatextrm1xcatextrmxmnotextrm3x0507085and09basedonmn2pandmn3sxrayphotoelectronspectra-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.3103/S1062873816060125\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'googlev-kozakov-kochur-nikolskii-torgashev-zvolenskaya-determiningthevalencestateofmanganeseionsincomplexoxideslatextrm1xcatextrmxmnotextrm3x0507085and09basedonmn2pandmn3sxrayphotoelectronspectra-2016', 'https://doi.org/10.3103/S1062873816060125', event);\">\n    Determining the valence state of manganese ions in complex oxides La$_{\\textrm{1–x}}$Ca$_{\\textrm{x}}$MnO$_{\\textrm{3}}$ (x = 0.5, 0.7, 0.85, and 0.9) based on Mn2p and Mn3s X-ray photoelectron spectra.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Googlev, K. A.; Kozakov, A. T.; Kochur, A. G.; Nikolskii, A. V.; Torgashev, V. I.;  and Zvolenskaya, A. A.\n</span>\n\n  \n\n</span>\n\n  <i>Bulletin of the Russian Academy of Sciences: Physics</i>, 80(6): 638–640. June 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.3103/S1062873816060125\"\n     onclick=\"log_download('googlev-kozakov-kochur-nikolskii-torgashev-zvolenskaya-determiningthevalencestateofmanganeseionsincomplexoxideslatextrm1xcatextrmxmnotextrm3x0507085and09basedonmn2pandmn3sxrayphotoelectronspectra-2016', 'https://doi.org/10.3103/S1062873816060125', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Determining the valence state of manganese ions in complex oxides La$_{\\textrm{1–x}}$Ca$_{\\textrm{x}}$MnO$_{\\textrm{3}}$ (x = 0.5, 0.7, 0.85, and 0.9) based on Mn2p and Mn3s X-ray photoelectron spectra [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3103/S1062873816060125\"\n     onclick=\"log_download('googlev-kozakov-kochur-nikolskii-torgashev-zvolenskaya-determiningthevalencestateofmanganeseionsincomplexoxideslatextrm1xcatextrmxmnotextrm3x0507085and09basedonmn2pandmn3sxrayphotoelectronspectra-2016', 'http://doi.org/10.3103/S1062873816060125', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/googlev-kozakov-kochur-nikolskii-torgashev-zvolenskaya-determiningthevalencestateofmanganeseionsincomplexoxideslatextrm1xcatextrmxmnotextrm3x0507085and09basedonmn2pandmn3sxrayphotoelectronspectra-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('googlev-kozakov-kochur-nikolskii-torgashev-zvolenskaya-determiningthevalencestateofmanganeseionsincomplexoxideslatextrm1xcatextrmxmnotextrm3x0507085and09basedonmn2pandmn3sxrayphotoelectronspectra-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{googlev_determining_2016,\n\ttitle = {Determining the valence state of manganese ions in complex oxides {La}$_{\\textrm{1–x}}${Ca}$_{\\textrm{x}}${MnO}$_{\\textrm{3}}$ (x = 0.5, 0.7, 0.85, and 0.9) based on {Mn2p} and {Mn3s} {X}-ray photoelectron spectra},\n\tvolume = {80},\n\tissn = {1934-9432},\n\turl = {https://doi.org/10.3103/S1062873816060125},\n\tdoi = {10.3103/S1062873816060125},\n\tabstract = {The valence state of manganese ions in complex oxides La1–xCaxMnO3 (x = 0.5, 0.7, 0.85, and 0.9) is studied on the basis of Mn2p and Mn3s X-ray photoelectron spectra. It is shown that manganese ions have the valence of Mn3+ and Mn4+ in the studied compounds. The relative Mn3+/Mn4+ content is determined.},\n\tlanguage = {en},\n\tnumber = {6},\n\turldate = {2023-11-11},\n\tjournal = {Bulletin of the Russian Academy of Sciences: Physics},\n\tauthor = {Googlev, K. A. and Kozakov, A. T. and Kochur, A. G. and Nikolskii, A. V. and Torgashev, V. I. and Zvolenskaya, A. A.},\n\tmonth = jun,\n\tyear = {2016},\n\tpages = {638--640},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The valence state of manganese ions in complex oxides La1–xCaxMnO3 (x = 0.5, 0.7, 0.85, and 0.9) is studied on the basis of Mn2p and Mn3s X-ray photoelectron spectra. It is shown that manganese ions have the valence of Mn3+ and Mn4+ in the studied compounds. The relative Mn3+/Mn4+ content is determined.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"bronwald-andronikova-burkovsky-chernyshev-leontiev-leontiev-ye-vakhrushev-compositiondependenceofthediffusescatteringincubicpbzrtextrm1xtitextrmxotextrm3-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/00150193.2016.1217723\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'bronwald-andronikova-burkovsky-chernyshev-leontiev-leontiev-ye-vakhrushev-compositiondependenceofthediffusescatteringincubicpbzrtextrm1xtitextrmxotextrm3-2016', 'https://doi.org/10.1080/00150193.2016.1217723', event);\">\n    Composition dependence of the diffuse scattering in cubic PbZr$_{\\textrm{1-x}}$Ti$_{\\textrm{x}}$O$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Bronwald, I.; Andronikova, D.; Burkovsky, R.; Chernyshev, D.; Leontiev, N. G.; Leontiev, I. N.; Ye, Z.;  and Vakhrushev, S.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 503(1): 45–51. October 2016.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2016.1217723</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/00150193.2016.1217723\"\n     onclick=\"log_download('bronwald-andronikova-burkovsky-chernyshev-leontiev-leontiev-ye-vakhrushev-compositiondependenceofthediffusescatteringincubicpbzrtextrm1xtitextrmxotextrm3-2016', 'https://doi.org/10.1080/00150193.2016.1217723', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Composition dependence of the diffuse scattering in cubic PbZr$_{\\textrm{1-x}}$Ti$_{\\textrm{x}}$O$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150193.2016.1217723\"\n     onclick=\"log_download('bronwald-andronikova-burkovsky-chernyshev-leontiev-leontiev-ye-vakhrushev-compositiondependenceofthediffusescatteringincubicpbzrtextrm1xtitextrmxotextrm3-2016', 'http://doi.org/10.1080/00150193.2016.1217723', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/bronwald-andronikova-burkovsky-chernyshev-leontiev-leontiev-ye-vakhrushev-compositiondependenceofthediffusescatteringincubicpbzrtextrm1xtitextrmxotextrm3-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('bronwald-andronikova-burkovsky-chernyshev-leontiev-leontiev-ye-vakhrushev-compositiondependenceofthediffusescatteringincubicpbzrtextrm1xtitextrmxotextrm3-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{bronwald_composition_2016,\n\ttitle = {Composition dependence of the diffuse scattering in cubic {PbZr}$_{\\textrm{1-x}}${Ti}$_{\\textrm{x}}${O}$_{\\textrm{3}}$},\n\tvolume = {503},\n\tissn = {0015-0193},\n\turl = {https://doi.org/10.1080/00150193.2016.1217723},\n\tdoi = {10.1080/00150193.2016.1217723},\n\tabstract = {The results of the experimental study of the diffuse scattering in ferroelectric solid solutions PbZr1-xTixO3 are reported. We have used X-ray diffraction to characterize the diffuse scattering in six single-crystals with . The comparison of diffuse intensity maps in almost pure lead zirconate and PbZr1-xTixO3 compounds with significant titanium doping shows that increasing lead titanate concentration gradually scales down the shape anisotropy of the scattering, but some details of the diffuse scattering that are not observed in pure PbTiO3 still remain.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Ferroelectrics},\n\tauthor = {Bronwald, Iurii and Andronikova, Daria and Burkovsky, Roman and Chernyshev, Dmitry and Leontiev, N. G. and Leontiev, I. N. and Ye, Zuo-Guang and Vakhrushev, Sergey},\n\tmonth = oct,\n\tyear = {2016},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/00150193.2016.1217723},\n\tkeywords = {diffuse scattering, Lead zirconat-titanate, morphotropic phase boundary, PZT},\n\tpages = {45--51},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The results of the experimental study of the diffuse scattering in ferroelectric solid solutions PbZr1-xTixO3 are reported. We have used X-ray diffraction to characterize the diffuse scattering in six single-crystals with . The comparison of diffuse intensity maps in almost pure lead zirconate and PbZr1-xTixO3 compounds with significant titanium doping shows that increasing lead titanate concentration gradually scales down the shape anisotropy of the scattering, but some details of the diffuse scattering that are not observed in pure PbTiO3 still remain.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kozakov-kochur-torgashev-googlev-kubrin-trotsenko-bush-nikolskii-bitextrm1xcatextrmxfeotextrm30x1ceramicscrystalstructurephaseandelementalcompositionandchemicalbondingfromxraydiffractionramanscatteringmssbauerandxrayphotoelectronspectra-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0925838815320314\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kozakov-kochur-torgashev-googlev-kubrin-trotsenko-bush-nikolskii-bitextrm1xcatextrmxfeotextrm30x1ceramicscrystalstructurephaseandelementalcompositionandchemicalbondingfromxraydiffractionramanscatteringmssbauerandxrayphotoelectronspectra-2016', 'https://www.sciencedirect.com/science/article/pii/S0925838815320314', event);\">\n    Bi$_{\\textrm{1-x}}$Ca$_{\\textrm{x}}$FeO$_{\\textrm{3-δ}}$ (0 ≤ x ≤ 1) ceramics: Crystal structure, phase and elemental composition, and chemical bonding from X-ray diffraction, Raman scattering, Mössbauer, and X-ray photoelectron spectra.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kozakov, A. T.; Kochur, A. G.; Torgashev, V. I.; Googlev, K. A.; Kubrin, S. P.; Trotsenko, V. G.; Bush, A. A.;  and Nikolskii, A. V.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Alloys and Compounds</i>, 664: 392–405. April 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0925838815320314\"\n     onclick=\"log_download('kozakov-kochur-torgashev-googlev-kubrin-trotsenko-bush-nikolskii-bitextrm1xcatextrmxfeotextrm30x1ceramicscrystalstructurephaseandelementalcompositionandchemicalbondingfromxraydiffractionramanscatteringmssbauerandxrayphotoelectronspectra-2016', 'https://www.sciencedirect.com/science/article/pii/S0925838815320314', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Bi$_{\\textrm{1-x}}$Ca$_{\\textrm{x}}$FeO$_{\\textrm{3-δ}}$ (0 ≤ x ≤ 1) ceramics: Crystal structure, phase and elemental composition, and chemical bonding from X-ray diffraction, Raman scattering, Mössbauer, and X-ray photoelectron spectra [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.jallcom.2015.12.241\"\n     onclick=\"log_download('kozakov-kochur-torgashev-googlev-kubrin-trotsenko-bush-nikolskii-bitextrm1xcatextrmxfeotextrm30x1ceramicscrystalstructurephaseandelementalcompositionandchemicalbondingfromxraydiffractionramanscatteringmssbauerandxrayphotoelectronspectra-2016', 'http://doi.org/10.1016/j.jallcom.2015.12.241', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kozakov-kochur-torgashev-googlev-kubrin-trotsenko-bush-nikolskii-bitextrm1xcatextrmxfeotextrm30x1ceramicscrystalstructurephaseandelementalcompositionandchemicalbondingfromxraydiffractionramanscatteringmssbauerandxrayphotoelectronspectra-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kozakov-kochur-torgashev-googlev-kubrin-trotsenko-bush-nikolskii-bitextrm1xcatextrmxfeotextrm30x1ceramicscrystalstructurephaseandelementalcompositionandchemicalbondingfromxraydiffractionramanscatteringmssbauerandxrayphotoelectronspectra-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kozakov_bi1-xcaxfeo3-_2016,\n\ttitle = {Bi$_{\\textrm{1-x}}${Ca}$_{\\textrm{x}}${FeO}$_{\\textrm{3-δ}}$ (0 ≤ x ≤ 1) ceramics: {Crystal} structure, phase and elemental composition, and chemical bonding from {X}-ray diffraction, {Raman} scattering, {Mössbauer}, and {X}-ray photoelectron spectra},\n\tvolume = {664},\n\tissn = {0925-8388},\n\tshorttitle = {Bi1-{xCaxFeO3}-δ (0 ≤ x ≤ 1) ceramics},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0925838815320314},\n\tdoi = {10.1016/j.jallcom.2015.12.241},\n\tabstract = {An integrated study of samples of Bi1−хCaхFeO3-δ (BCFO) system for 0 ≤ x ≤ 1 (step 0.1) is performed using X-ray diffraction (XRD), Raman scattering, Mössbauer spectroscopy, and X-ray photoelectron spectroscopy (XPS). Measured elemental compositions of samples were found to deviate substantially from nominal ones. X-ray structure analysis discovered a continuous series of solid solutions with perovskite structure (or its derivatives) on the interval of nominal Ca content 0 ≤ x ≤ 0.9. However, the analysis of the data from all the methods used, limits the region of single phase samples (in presence of insignificant amount of foreign ones) to nominal Ca content interval 0.1 {\\textless} x {\\textless} 0.4. No Fe4+ ions are discovered upon substitution of Bi3+ by Ca2+, neither by Mössbauer spectroscopy, nor by XPS. Charge compensation in Bi1−хCaхFeO3-δ takes place mostly via creation of oxygen vacancies. Charge transfer satellites position in Ca2p XPS is shown to be sensitive to a number of oxygen ions in the immediate environment of Ca.},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Alloys and Compounds},\n\tauthor = {Kozakov, A. T. and Kochur, A. G. and Torgashev, V. I. and Googlev, K. A. and Kubrin, S. P. and Trotsenko, V. G. and Bush, A. A. and Nikolskii, A. V.},\n\tmonth = apr,\n\tyear = {2016},\n\tkeywords = {XPS, Mössbauer spectroscopy, Elemental composition, Vacancies, XRD, BiCaFeO, BiFeO, CaFeO, Phase analysis, Raman scattering},\n\tpages = {392--405},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  An integrated study of samples of Bi1−хCaхFeO3-δ (BCFO) system for 0 ≤ x ≤ 1 (step 0.1) is performed using X-ray diffraction (XRD), Raman scattering, Mössbauer spectroscopy, and X-ray photoelectron spectroscopy (XPS). Measured elemental compositions of samples were found to deviate substantially from nominal ones. X-ray structure analysis discovered a continuous series of solid solutions with perovskite structure (or its derivatives) on the interval of nominal Ca content 0 ≤ x ≤ 0.9. However, the analysis of the data from all the methods used, limits the region of single phase samples (in presence of insignificant amount of foreign ones) to nominal Ca content interval 0.1 \\textless x \\textless 0.4. No Fe4+ ions are discovered upon substitution of Bi3+ by Ca2+, neither by Mössbauer spectroscopy, nor by XPS. Charge compensation in Bi1−хCaхFeO3-δ takes place mostly via creation of oxygen vacancies. Charge transfer satellites position in Ca2p XPS is shown to be sensitive to a number of oxygen ions in the immediate environment of Ca.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kadyrov-zhang-zhukova-anzin-trotsenko-torgashev-dressel-gorshunov-bandlikeelectricaltransportinprtextrm1xcatextrmxmnotextrm3manganites-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.93.184303\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kadyrov-zhang-zhukova-anzin-trotsenko-torgashev-dressel-gorshunov-bandlikeelectricaltransportinprtextrm1xcatextrmxmnotextrm3manganites-2016', 'https://link.aps.org/doi/10.1103/PhysRevB.93.184303', event);\">\n    Bandlike electrical transport in Pr$_{\\textrm{1-x}}$Ca$_{\\textrm{x}}$MnO$_{\\textrm{3}}$ manganites.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kadyrov, L. S.; Zhang, T.; Zhukova, E. S.; Anzin, V. B.; Trotsenko, V. G.; Torgashev, V. I.; Dressel, M.;  and Gorshunov, B. P.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 93(18): 184303. May 2016.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.93.184303\"\n     onclick=\"log_download('kadyrov-zhang-zhukova-anzin-trotsenko-torgashev-dressel-gorshunov-bandlikeelectricaltransportinprtextrm1xcatextrmxmnotextrm3manganites-2016', 'https://link.aps.org/doi/10.1103/PhysRevB.93.184303', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Bandlike electrical transport in Pr$_{\\textrm{1-x}}$Ca$_{\\textrm{x}}$MnO$_{\\textrm{3}}$ manganites [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.93.184303\"\n     onclick=\"log_download('kadyrov-zhang-zhukova-anzin-trotsenko-torgashev-dressel-gorshunov-bandlikeelectricaltransportinprtextrm1xcatextrmxmnotextrm3manganites-2016', 'http://doi.org/10.1103/PhysRevB.93.184303', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kadyrov-zhang-zhukova-anzin-trotsenko-torgashev-dressel-gorshunov-bandlikeelectricaltransportinprtextrm1xcatextrmxmnotextrm3manganites-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kadyrov-zhang-zhukova-anzin-trotsenko-torgashev-dressel-gorshunov-bandlikeelectricaltransportinprtextrm1xcatextrmxmnotextrm3manganites-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kadyrov_bandlike_2016,\n\ttitle = {Bandlike electrical transport in {Pr}$_{\\textrm{1-x}}${Ca}$_{\\textrm{x}}${MnO}$_{\\textrm{3}}$ manganites},\n\tvolume = {93},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.93.184303},\n\tdoi = {10.1103/PhysRevB.93.184303},\n\tabstract = {The conductivity and dielectric permittivity spectra of polycrystalline manganites Pr1−xCaxMnO3 with x=0.3, 0.4, and 0.5 have been measured in a broad frequency range (5–3000cm−1) down to low temperatures. From the dispersion analysis the existence of a Drude component can be established that is associated with small polarons coherently moving within a band several meV wide. The temperature-dependent conductivity shows an activated behavior with an activation energy of approximately 165 meV above 170 K and 4.8 meV below 120 K. The change in the activation energy is assigned to the onset of magnetic order at 120 K. In all three samples an absorption band is discovered at 40–60cm−1 that is associated with the transition between Stark-split Pr3+ electron states which gain optical activity due to coupling to acoustical phonons.},\n\tnumber = {18},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Kadyrov, L. S. and Zhang, T. and Zhukova, E. S. and Anzin, V. B. and Trotsenko, V. G. and Torgashev, V. I. and Dressel, M. and Gorshunov, B. P.},\n\tmonth = may,\n\tyear = {2016},\n\tnote = {Publisher: American Physical Society},\n\tpages = {184303},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The conductivity and dielectric permittivity spectra of polycrystalline manganites Pr1−xCaxMnO3 with x=0.3, 0.4, and 0.5 have been measured in a broad frequency range (5–3000cm−1) down to low temperatures. From the dispersion analysis the existence of a Drude component can be established that is associated with small polarons coherently moving within a band several meV wide. The temperature-dependent conductivity shows an activated behavior with an activation energy of approximately 165 meV above 170 K and 4.8 meV below 120 K. The change in the activation energy is assigned to the onset of magnetic order at 120 K. In all three samples an absorption band is discovered at 40–60cm−1 that is associated with the transition between Stark-split Pr3+ electron states which gain optical activity due to coupling to acoustical phonons.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----lamnotextrm3-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=26160197\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----lamnotextrm3-2016', 'https://elibrary.ru/item.asp?id=26160197', event);\">\n    Эффекты изменения стехиометрии LaMnO$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Рудская, А. Г.; Чаговец, С. В.; Ананьева, Е. В.;  and Куприянов, М. Ф.\n</span>\n\n  \n\n</span>\n\n  <i>Известия Российской Академии Наук. Серия Физическая</i>, 80(6): 807.  2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=26160197\"\n     onclick=\"log_download('----lamnotextrm3-2016', 'https://elibrary.ru/item.asp?id=26160197', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Эффекты изменения стехиометрии LaMnO$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.7868/S0367676516060284\"\n     onclick=\"log_download('----lamnotextrm3-2016', 'http://doi.org/10.7868/S0367676516060284', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----lamnotextrm3-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----lamnotextrm3-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2016-2,\n\ttitle = {Эффекты изменения стехиометрии {LaMnO}$_{\\textrm{3}}$},\n\tvolume = {80},\n\tissn = {0367-6765},\n\turl = {https://elibrary.ru/item.asp?id=26160197},\n\tdoi = {10.7868/S0367676516060284},\n\tabstract = {Установлено, что в результате синтеза LaMnO3 из разных прекурсоров, приготовленных методом твердофазной реакции и методами совместного осаждения и сорбции, в зависимости от температур синтеза образуются перовскитовые фазы с разными отклонениями от стехиометрии, что приводит к существованию при комнатной температуре фаз разной симметрии: орторомбической (твердофазный синтез) и ромбоэдрической (влажные методы синтеза).},\n\tlanguage = {ru},\n\tnumber = {6},\n\turldate = {2023-11-11},\n\tjournal = {Известия Российской Академии Наук. Серия Физическая},\n\tauthor = {Рудская, А. Г. and Чаговец, С. В. and Ананьева, Е. В. and Куприянов, М. Ф.},\n\tyear = {2016},\n\tpages = {807},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Установлено, что в результате синтеза LaMnO3 из разных прекурсоров, приготовленных методом твердофазной реакции и методами совместного осаждения и сорбции, в зависимости от температур синтеза образуются перовскитовые фазы с разными отклонениями от стехиометрии, что приводит к существованию при комнатной температуре фаз разной симметрии: орторомбической (твердофазный синтез) и ромбоэдрической (влажные методы синтеза).\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"--------etal-265-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://ivdon.ru/ru/magazine/archive/n4y2016/3820\"\n     onclick=\"return trackOutboundLink('publications', 'click', '--------etal-265-2016', 'http://ivdon.ru/ru/magazine/archive/n4y2016/3820', event);\">\n    Электрические свойства и структура новых слоистых оксидов 26,5 ( , , ).\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Чупахина, Т. И.; Мельникова, Н. В.; Гырдасова, О. И.; Никитина, Ю. А.; Гавриляченко, В. Г.; Кабиров, Ю. В.; Пруцакова, Н. В.; Чебанова, Е. В.;  and Русакова, Е. Б.\n</span>\n\n  \n\n</span>\n\n  . October 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://ivdon.ru/ru/magazine/archive/n4y2016/3820\"\n     onclick=\"log_download('--------etal-265-2016', 'http://ivdon.ru/ru/magazine/archive/n4y2016/3820', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Электрические свойства и структура новых слоистых оксидов 26,5 ( , , ) [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/--------etal-265-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('--------etal-265-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2016-3,\n\ttitle = {Электрические свойства и структура новых слоистых оксидов 26,5 ( , , )},\n\turl = {http://ivdon.ru/ru/magazine/archive/n4y2016/3820},\n\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tauthor = {Чупахина, Т. И. and Мельникова, Н. В. and Гырдасова, О. И. and Никитина, Ю. А. and Гавриляченко, В. Г. and Кабиров, Ю. В. and Пруцакова, Н. В. and Чебанова, Е. В. and Русакова, Е. Б.},\n\tmonth = oct,\n\tyear = {2016},\n\tkeywords = {⛔ No DOI found},\n\tfile = {Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\2RRFFXDG\\\\3820.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Сетевой научный журнал «Инженерный вестник Дона»\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/43055\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---2016', 'http://journals.ioffe.ru/articles/43055', event);\">\n    Особенности низкочастотной колебательной динамики и низкотемпературная теплоемкость двустенных углеродных нанотрубок.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Авраменко, М. В.;  and Рошаль, С. Б.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 58(5): 979–986. April 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/43055\"\n     onclick=\"log_download('---2016', 'http://journals.ioffe.ru/articles/43055', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Особенности низкочастотной колебательной динамики и низкотемпературная теплоемкость двустенных углеродных нанотрубок [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2016-4,\n\ttitle = {Особенности низкочастотной колебательной динамики и низкотемпературная теплоемкость двустенных углеродных нанотрубок},\n\tvolume = {58},\n\turl = {http://journals.ioffe.ru/articles/43055},\n\tabstract = {Построена континуальная модель низкочастотной динамики двустенной углеродной нанотрубки. В рамках предложенного подхода рассмотрено образование низкочастотной части фононного спектра двустенной нанотрубки из фононных спектров образующих ее одностенных нанотрубок. Рассмотрено влияние окружения на фононный спектр одиночной двустенной углеродной нанотрубки. Предложен комбинированный способ оценки коэффициентов ван-дер-ваальсова взаимодействия между стенками нанотрубки на основе спектроскопических данных и известных величин упругих модулей графита. Также рассчитана низкотемпературная удельная теплоемкость двустенных углеродных нанотрубок, которая в области применимости модели (T{\\textless}35 K) оказывается значительно меньше, чем сумма удельных теплоемкостей двух образующих ее индивидуальных одностенных нанотрубок. Работа выполнена при поддержке Российского научного фонда (грант N 15-12-10004).},\n\tlanguage = {ru},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Авраменко, М. В. and Рошаль, С. Б.},\n\tmonth = apr,\n\tyear = {2016},\n\tpages = {979--986},\n\tfile = {Физика твердого тела:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\7ERGJUQT\\\\43055.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Построена континуальная модель низкочастотной динамики двустенной углеродной нанотрубки. В рамках предложенного подхода рассмотрено образование низкочастотной части фононного спектра двустенной нанотрубки из фононных спектров образующих ее одностенных нанотрубок. Рассмотрено влияние окружения на фононный спектр одиночной двустенной углеродной нанотрубки. Предложен комбинированный способ оценки коэффициентов ван-дер-ваальсова взаимодействия между стенками нанотрубки на основе спектроскопических данных и известных величин упругих модулей графита. Также рассчитана низкотемпературная удельная теплоемкость двустенных углеродных нанотрубок, которая в области применимости модели (T\\textless35 K) оказывается значительно меньше, чем сумма удельных теплоемкостей двух образующих ее индивидуальных одностенных нанотрубок. Работа выполнена при поддержке Российского научного фонда (грант N 15-12-10004).\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----latextrm07srtextrm03mnotextrm3c-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/43238\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----latextrm07srtextrm03mnotextrm3c-2016', 'http://journals.ioffe.ru/articles/43238', event);\">\n    Положительное магнитосопротивление композитов La$_{\\textrm{0.7}}$Sr$_{\\textrm{0.3}}$MnO$_{\\textrm{3}}$/C при комнатной температуре.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Кабиров, Ю. В.; Гавриляченко, В. Г.; Богатин, А. С.; Лянгузов, Н. В.;  and Гавриляченко, Т. В.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 58(7): 1263–1265. June 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/43238\"\n     onclick=\"log_download('-----latextrm07srtextrm03mnotextrm3c-2016', 'http://journals.ioffe.ru/articles/43238', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Положительное магнитосопротивление композитов La$_{\\textrm{0.7}}$Sr$_{\\textrm{0.3}}$MnO$_{\\textrm{3}}$/C при комнатной температуре [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----latextrm07srtextrm03mnotextrm3c-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----latextrm07srtextrm03mnotextrm3c-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2016-5,\n\ttitle = {Положительное магнитосопротивление композитов {La}$_{\\textrm{0.7}}${Sr}$_{\\textrm{0.3}}${MnO}$_{\\textrm{3}}$/{C} при комнатной температуре},\n\tvolume = {58},\n\turl = {http://journals.ioffe.ru/articles/43238},\n\tabstract = {Синтезированы двухфазные композиты xLa0.7Sr0.3MnO3/(100-x)C (x=5-85 mass/\\%). Изучены их магниторезистивные свойства в магнитных полях от 0 до 15 kOe. При комнатной температуре значения положительного изотропного магнитосопротивления для образцов с x=50-60 mass\\% достигают 15\\%. Работа выполнена при финансовой поддержке РФФИ (проект N 14-03-00103).},\n\tlanguage = {ru},\n\tnumber = {7},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Богатин, А. С. and Лянгузов, Н. В. and Гавриляченко, Т. В.},\n\tmonth = jun,\n\tyear = {2016},\n\tpages = {1263--1265},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Синтезированы двухфазные композиты xLa0.7Sr0.3MnO3/(100-x)C (x=5-85 mass/%). Изучены их магниторезистивные свойства в магнитных полях от 0 до 15 kOe. При комнатной температуре значения положительного изотропного магнитосопротивления для образцов с x=50-60 mass% достигают 15%. Работа выполнена при финансовой поддержке РФФИ (проект N 14-03-00103).\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------1xlatextrm07srtextrm03mnotextrm3xgeotextrm2litextrm4ptextrm2otextrm7-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/43008\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------1xlatextrm07srtextrm03mnotextrm3xgeotextrm2litextrm4ptextrm2otextrm7-2016', 'http://journals.ioffe.ru/articles/43008', event);\">\n    Отрицательная магниторезистивность композитной керамики (1-x)La$_{\\textrm{0.7}}$Sr$_{\\textrm{0.3}}$MnO$_{\\textrm{3}}$/x(GeO$_{\\textrm{2}}$, Li$_{\\textrm{4}}$P$_{\\textrm{2}}$O$_{\\textrm{7}}$).\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Кабиров, Ю. В.; Гавриляченко, В. Г.; Богатин, А. С.; Лянгузов, Н. В.; Гавриляченко, Т. В.;  and Медведев, Б. С.\n</span>\n\n  \n\n</span>\n\n  <i>Письма в ЖТФ</i>, 42(6): 1–5. February 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/43008\"\n     onclick=\"log_download('------1xlatextrm07srtextrm03mnotextrm3xgeotextrm2litextrm4ptextrm2otextrm7-2016', 'http://journals.ioffe.ru/articles/43008', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Отрицательная магниторезистивность композитной керамики (1-x)La$_{\\textrm{0.7}}$Sr$_{\\textrm{0.3}}$MnO$_{\\textrm{3}}$/x(GeO$_{\\textrm{2}}$, Li$_{\\textrm{4}}$P$_{\\textrm{2}}$O$_{\\textrm{7}}$) [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------1xlatextrm07srtextrm03mnotextrm3xgeotextrm2litextrm4ptextrm2otextrm7-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------1xlatextrm07srtextrm03mnotextrm3xgeotextrm2litextrm4ptextrm2otextrm7-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2016-6,\n\ttitle = {Отрицательная магниторезистивность композитной керамики (1-x){La}$_{\\textrm{0.7}}${Sr}$_{\\textrm{0.3}}${MnO}$_{\\textrm{3}}$/x({GeO}$_{\\textrm{2}}$, {Li}$_{\\textrm{4}}${P}$_{\\textrm{2}}${O}$_{\\textrm{7}}$)},\n\tvolume = {42},\n\turl = {http://journals.ioffe.ru/articles/43008},\n\tabstract = {Синтезированы керамические композиты (1-x)La0.7Sr0.3MnO3/x(GeO2) и (1-x)La0.7Sr0.3MnO3/x(Li4P2 O7), где x=0.1-0.3, отличающиеся высокими значениями отрицательной изотропной магниторезистивности (MR) при комнатной температуре. В композите, где в качестве барьерной компоненты с массовой долей 20\\% использован GeO2, MR=15\\% в магнитном поле 18 kOe, а в композите с Li4P2O7 при тех же условиях MR=16\\%.},\n\tlanguage = {ru},\n\tnumber = {6},\n\turldate = {2023-11-11},\n\tjournal = {Письма в ЖТФ},\n\tauthor = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Богатин, А. С. and Лянгузов, Н. В. and Гавриляченко, Т. В. and Медведев, Б. С.},\n\tmonth = feb,\n\tyear = {2016},\n\tpages = {1--5},\n\tfile = {Письма в журнал технической физики:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\4JRHC3G5\\\\43008.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Синтезированы керамические композиты (1-x)La0.7Sr0.3MnO3/x(GeO2) и (1-x)La0.7Sr0.3MnO3/x(Li4P2 O7), где x=0.1-0.3, отличающиеся высокими значениями отрицательной изотропной магниторезистивности (MR) при комнатной температуре. В композите, где в качестве барьерной компоненты с массовой долей 20% использован GeO2, MR=15% в магнитном поле 18 kOe, а в композите с Li4P2O7 при тех же условиях MR=16%.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------latextrm07srtextrm03mnotextrm3geotextrm2-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://fundamental-research.ru/ru/article/view?id=40689\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------latextrm07srtextrm03mnotextrm3geotextrm2-2016', 'https://fundamental-research.ru/ru/article/view?id=40689', event);\">\n    Одношаговый синтез магниторезистивных композитных материалов La$_{\\textrm{0.7}}$Sr$_{\\textrm{0.3}}$MnO$_{\\textrm{3}}$/GeO$_{\\textrm{2}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Кабиров, Ю. В.; Гавриляченко, В. Г.; Пруцакова, Н. В.; Гуда, А. А.; Попов, Ю. В.;  and Чебанова, Е. В.\n</span>\n\n  \n\n</span>\n\n  <i>Технические науки</i>, (9): 26–30. September 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://fundamental-research.ru/ru/article/view?id=40689\"\n     onclick=\"log_download('------latextrm07srtextrm03mnotextrm3geotextrm2-2016', 'https://fundamental-research.ru/ru/article/view?id=40689', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Одношаговый синтез магниторезистивных композитных материалов La$_{\\textrm{0.7}}$Sr$_{\\textrm{0.3}}$MnO$_{\\textrm{3}}$/GeO$_{\\textrm{2}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------latextrm07srtextrm03mnotextrm3geotextrm2-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------latextrm07srtextrm03mnotextrm3geotextrm2-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2016-7,\n\ttitle = {Одношаговый синтез магниторезистивных композитных материалов {La}$_{\\textrm{0.7}}${Sr}$_{\\textrm{0.3}}${MnO}$_{\\textrm{3}}$/{GeO}$_{\\textrm{2}}$},\n\turl = {https://fundamental-research.ru/ru/article/view?id=40689},\n\tlanguage = {ru},\n\tnumber = {9},\n\turldate = {2023-11-11},\n\tjournal = {Технические науки},\n\tauthor = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Пруцакова, Н. В. and Гуда, А. А. and Попов, Ю. В. and Чебанова, Е. В.},\n\tmonth = sep,\n\tyear = {2016},\n\tpages = {26--30},\n\tfile = {ОДНОШАГОВЫЙ СИНТЕЗ МАГНИТОРЕЗИСТИВНЫХ КОМПОЗИТНЫХ МАТЕРИАЛОВ LA0.7SR0.3MNO3/GEO2 - Фундаментальные исследования (научный журнал):C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\T72K4G94\\\\view.html:text/html},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"doronkin-kuriganova-leontyev-baier-lichtenberg-smirnova-grunwaldt-electrochemicallysynthesizedptaltextrm2otextrm3oxidationcatalysts-2016\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1007/s10562-015-1651-z\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'doronkin-kuriganova-leontyev-baier-lichtenberg-smirnova-grunwaldt-electrochemicallysynthesizedptaltextrm2otextrm3oxidationcatalysts-2016', 'https://doi.org/10.1007/s10562-015-1651-z', event);\">\n    Electrochemically Synthesized Pt/Al$_{\\textrm{2}}$O$_{\\textrm{3}}$ Oxidation Catalysts.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Doronkin, D. E.; Kuriganova, A. B.; Leontyev, I. N.; Baier, S.; Lichtenberg, H.; Smirnova, N. V.;  and Grunwaldt, J.\n</span>\n\n  \n\n</span>\n\n  <i>Catalysis Letters</i>, 146(2): 452–463. February 2016.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1007/s10562-015-1651-z\"\n     onclick=\"log_download('doronkin-kuriganova-leontyev-baier-lichtenberg-smirnova-grunwaldt-electrochemicallysynthesizedptaltextrm2otextrm3oxidationcatalysts-2016', 'https://doi.org/10.1007/s10562-015-1651-z', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Electrochemically Synthesized Pt/Al$_{\\textrm{2}}$O$_{\\textrm{3}}$ Oxidation Catalysts [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1007/s10562-015-1651-z\"\n     onclick=\"log_download('doronkin-kuriganova-leontyev-baier-lichtenberg-smirnova-grunwaldt-electrochemicallysynthesizedptaltextrm2otextrm3oxidationcatalysts-2016', 'http://doi.org/10.1007/s10562-015-1651-z', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/doronkin-kuriganova-leontyev-baier-lichtenberg-smirnova-grunwaldt-electrochemicallysynthesizedptaltextrm2otextrm3oxidationcatalysts-2016\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('doronkin-kuriganova-leontyev-baier-lichtenberg-smirnova-grunwaldt-electrochemicallysynthesizedptaltextrm2otextrm3oxidationcatalysts-2016')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{doronkin_electrochemically_2016,\n\ttitle = {Electrochemically {Synthesized} {Pt}/{Al}$_{\\textrm{2}}${O}$_{\\textrm{3}}$ {Oxidation} {Catalysts}},\n\tvolume = {146},\n\tissn = {1572-879X},\n\turl = {https://doi.org/10.1007/s10562-015-1651-z},\n\tdoi = {10.1007/s10562-015-1651-z},\n\tabstract = {Pt/γ–Al2O3 catalysts made by fast and simple electrochemical dispersion method were characterized using X-ray absorption spectroscopy, CO chemisorption, transmission electron microscopy and X-ray diffraction, and compared with an impregnated catalyst with respect to oxidation of CO and NO. A combination of techniques revealed average particle sizes of 3–4 nm for 0.81–3.8 wt\\% Pt/γ–Al2O3 catalysts. Electrochemically prepared materials demonstrated catalytic activity comparable to that of conventional impregnated catalyst and reasonable stability.},\n\tlanguage = {en},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Catalysis Letters},\n\tauthor = {Doronkin, Dmitry E. and Kuriganova, Aleksandra B. and Leontyev, Igor N. and Baier, Sina and Lichtenberg, Henning and Smirnova, Nina V. and Grunwaldt, Jan-Dierk},\n\tmonth = feb,\n\tyear = {2016},\n\tkeywords = {DOC, Electrochemical dispersion, Oxidation, Platinum},\n\tpages = {452--463},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Pt/γ–Al2O3 catalysts made by fast and simple electrochemical dispersion method were characterized using X-ray absorption spectroscopy, CO chemisorption, transmission electron microscopy and X-ray diffraction, and compared with an impregnated catalyst with respect to oxidation of CO and NO. A combination of techniques revealed average particle sizes of 3–4 nm for 0.81–3.8 wt% Pt/γ–Al2O3 catalysts. Electrochemically prepared materials demonstrated catalytic activity comparable to that of conventional impregnated catalyst and reasonable stability.\n</div>\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2015\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2015')\"\n      onkeypress=\"toggleGroup('group_2015')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2015</span>\n      <span class=\"bibbase_group_count\">\n        \n        (34)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"levshov-avramenko-than-michel-arenal-paillet-rybkovskiy-osadchy-etal-studyofcollectiveradialbreathinglikemodesindoublewalledcarbonnanotubescombinationofcontinuoustwodimensionalmembranetheoryandramanspectroscopy-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.spiedigitallibrary.org/journals/journal-of-nanophotonics/volume-10/issue-1/012502/Study-of-collective-radial-breathing-like-modes-in-double-walled/10.1117/1.JNP.10.012502.full\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'levshov-avramenko-than-michel-arenal-paillet-rybkovskiy-osadchy-etal-studyofcollectiveradialbreathinglikemodesindoublewalledcarbonnanotubescombinationofcontinuoustwodimensionalmembranetheoryandramanspectroscopy-2015', 'https://www.spiedigitallibrary.org/journals/journal-of-nanophotonics/volume-10/issue-1/012502/Study-of-collective-radial-breathing-like-modes-in-double-walled/10.1117/1.JNP.10.012502.full', event);\">\n    Study of collective radial breathing-like modes in double-walled carbon nanotubes: combination of continuous two-dimensional membrane theory and Raman spectroscopy.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Levshov, D. I.; Avramenko, M. V.; Than, X.; Michel, T.; Arenal, R.; Paillet, M.; Rybkovskiy, D. V.; Osadchy, A. V.; Rochal, S. B.; Yuzyuk, Y. I.;  and Sauvajol, J.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Nanophotonics</i>, 10(1): 012502. September 2015.\n  <span class=\"note\">Publisher: SPIE</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.spiedigitallibrary.org/journals/journal-of-nanophotonics/volume-10/issue-1/012502/Study-of-collective-radial-breathing-like-modes-in-double-walled/10.1117/1.JNP.10.012502.full\"\n     onclick=\"log_download('levshov-avramenko-than-michel-arenal-paillet-rybkovskiy-osadchy-etal-studyofcollectiveradialbreathinglikemodesindoublewalledcarbonnanotubescombinationofcontinuoustwodimensionalmembranetheoryandramanspectroscopy-2015', 'https://www.spiedigitallibrary.org/journals/journal-of-nanophotonics/volume-10/issue-1/012502/Study-of-collective-radial-breathing-like-modes-in-double-walled/10.1117/1.JNP.10.012502.full', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Study of collective radial breathing-like modes in double-walled carbon nanotubes: combination of continuous two-dimensional membrane theory and Raman spectroscopy [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1117/1.JNP.10.012502\"\n     onclick=\"log_download('levshov-avramenko-than-michel-arenal-paillet-rybkovskiy-osadchy-etal-studyofcollectiveradialbreathinglikemodesindoublewalledcarbonnanotubescombinationofcontinuoustwodimensionalmembranetheoryandramanspectroscopy-2015', 'http://doi.org/10.1117/1.JNP.10.012502', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/levshov-avramenko-than-michel-arenal-paillet-rybkovskiy-osadchy-etal-studyofcollectiveradialbreathinglikemodesindoublewalledcarbonnanotubescombinationofcontinuoustwodimensionalmembranetheoryandramanspectroscopy-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('levshov-avramenko-than-michel-arenal-paillet-rybkovskiy-osadchy-etal-studyofcollectiveradialbreathinglikemodesindoublewalledcarbonnanotubescombinationofcontinuoustwodimensionalmembranetheoryandramanspectroscopy-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{levshov_study_2015,\n\ttitle = {Study of collective radial breathing-like modes in double-walled carbon nanotubes: combination of continuous two-dimensional membrane theory and {Raman} spectroscopy},\n\tvolume = {10},\n\tissn = {1934-2608, 1934-2608},\n\tshorttitle = {Study of collective radial breathing-like modes in double-walled carbon nanotubes},\n\turl = {https://www.spiedigitallibrary.org/journals/journal-of-nanophotonics/volume-10/issue-1/012502/Study-of-collective-radial-breathing-like-modes-in-double-walled/10.1117/1.JNP.10.012502.full},\n\tdoi = {10.1117/1.JNP.10.012502},\n\tabstract = {Radial breathing modes (RBMs) are widely used for the atomic structure characterization and index assignment of single-walled carbon nanotubes (SWNTs) from resonant Raman spectroscopy. However, for double-walled carbon nanotubes (DWNTs), the use of conventional ωRBM(d) formulas is complicated due to the van der Waals interaction between the layers, which strongly affects the frequencies of radial modes and leads to new collective vibrations. This paper presents an alternative way to theoretically study the collective radial breathing-like modes (RBLMs) of DWNTs and to account for interlayer interaction, namely the continuous two-dimensional membrane theory. We obtain an analytical ωRBLM(do,di) relation, being the equivalent of the conventional ωRBM(d) expressions, established for SWNTs. We compare our theoretical predictions with Raman data, measured on individual index-identified suspended DWNTs, and find a good agreement between experiment and theory. Moreover, we show that the interlayer coupling in individual DWNTs strongly depends on the interlayer distance, which is manifested in the frequency shifts of the RBLMs with respect to the RBMs of the individual inner and outer tubes. In terms of characterization, this means that the combination of Raman spectroscopy data and predictions of continuous membrane theory may give additional criteria for the index identification of DWNTs, namely the interlayer distance.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Nanophotonics},\n\tauthor = {Levshov, Dmitry I. and Avramenko, Marina V. and Than, Xuan-Tinh and Michel, Thierry and Arenal, Raul and Paillet, Matthieu and Rybkovskiy, Dmitry V. and Osadchy, Alexander V. and Rochal, Sergei B. and Yuzyuk, Yuri I. and Sauvajol, Jean-Louis},\n\tmonth = sep,\n\tyear = {2015},\n\tnote = {Publisher: SPIE},\n\tpages = {012502},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Radial breathing modes (RBMs) are widely used for the atomic structure characterization and index assignment of single-walled carbon nanotubes (SWNTs) from resonant Raman spectroscopy. However, for double-walled carbon nanotubes (DWNTs), the use of conventional ωRBM(d) formulas is complicated due to the van der Waals interaction between the layers, which strongly affects the frequencies of radial modes and leads to new collective vibrations. This paper presents an alternative way to theoretically study the collective radial breathing-like modes (RBLMs) of DWNTs and to account for interlayer interaction, namely the continuous two-dimensional membrane theory. We obtain an analytical ωRBLM(do,di) relation, being the equivalent of the conventional ωRBM(d) expressions, established for SWNTs. We compare our theoretical predictions with Raman data, measured on individual index-identified suspended DWNTs, and find a good agreement between experiment and theory. Moreover, we show that the interlayer coupling in individual DWNTs strongly depends on the interlayer distance, which is manifested in the frequency shifts of the RBLMs with respect to the RBMs of the individual inner and outer tubes. In terms of characterization, this means that the combination of Raman spectroscopy data and predictions of continuous membrane theory may give additional criteria for the index identification of DWNTs, namely the interlayer distance.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-kalinchuk-shakhovoi-yuzyuk-anomalouschangeinthematerialmoduliofthinfilmsofbariumtitanate-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S0021894415060218\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-kalinchuk-shakhovoi-yuzyuk-anomalouschangeinthematerialmoduliofthinfilmsofbariumtitanate-2015', 'https://doi.org/10.1134/S0021894415060218', event);\">\n    Anomalous change in the material moduli of thin films of barium titanate.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.; Kalinchuk, V. V.; Shakhovoi, R. A.;  and Yuzyuk, Y. I.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Applied Mechanics and Technical Physics</i>, 56(6): 1103–1110. November 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S0021894415060218\"\n     onclick=\"log_download('shirokov-kalinchuk-shakhovoi-yuzyuk-anomalouschangeinthematerialmoduliofthinfilmsofbariumtitanate-2015', 'https://doi.org/10.1134/S0021894415060218', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Anomalous change in the material moduli of thin films of barium titanate [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S0021894415060218\"\n     onclick=\"log_download('shirokov-kalinchuk-shakhovoi-yuzyuk-anomalouschangeinthematerialmoduliofthinfilmsofbariumtitanate-2015', 'http://doi.org/10.1134/S0021894415060218', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-kalinchuk-shakhovoi-yuzyuk-anomalouschangeinthematerialmoduliofthinfilmsofbariumtitanate-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-kalinchuk-shakhovoi-yuzyuk-anomalouschangeinthematerialmoduliofthinfilmsofbariumtitanate-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_anomalous_2015,\n\ttitle = {Anomalous change in the material moduli of thin films of barium titanate},\n\tvolume = {56},\n\tissn = {1573-8620},\n\turl = {https://doi.org/10.1134/S0021894415060218},\n\tdoi = {10.1134/S0021894415060218},\n\tabstract = {A method is proposed to determine the moduli of thin ferroelectric films subjected to forced deformation due to the mismatch between the crystal lattice sizes of the film and substrate materials and the difference of their thermal expansion coefficients. Models of single-crystal films of barium titanate are studied using the eighth-degree Landau thermodynamic potential. It is shown that in the considered range of forced strain of the barium titanate film, three main states exist: a tetragonal phase (c phase) of 4mm symmetry with spontaneous polarization directed along the normal to the film plane; an orthorhombic phase (aa phase) of 2 mm symmetry with polarization oriented along the diagonal plane of the film; monoclinic phase (r phase) of Cmsymmetry with the intermediate direction of polarization. All phases are separated by the lines of transitions of the second kind. Dependences of the elastic, electric and piezoelectric moduli on the magnitude of forced strain are plotted. It is shown that at the phase boundaries there is an anomalous change in the constants of the ferroelectric film and in the region of existence of the r phase, some moduli reach extreme values.},\n\tlanguage = {en},\n\tnumber = {6},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Applied Mechanics and Technical Physics},\n\tauthor = {Shirokov, V. B. and Kalinchuk, V. V. and Shakhovoi, R. A. and Yuzyuk, Yu. I.},\n\tmonth = nov,\n\tyear = {2015},\n\tkeywords = {thin films, elastic moduli, ferroelectrics, forced strain, material constants, piezoelectric moduli},\n\tpages = {1103--1110},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A method is proposed to determine the moduli of thin ferroelectric films subjected to forced deformation due to the mismatch between the crystal lattice sizes of the film and substrate materials and the difference of their thermal expansion coefficients. Models of single-crystal films of barium titanate are studied using the eighth-degree Landau thermodynamic potential. It is shown that in the considered range of forced strain of the barium titanate film, three main states exist: a tetragonal phase (c phase) of 4mm symmetry with spontaneous polarization directed along the normal to the film plane; an orthorhombic phase (aa phase) of 2 mm symmetry with polarization oriented along the diagonal plane of the film; monoclinic phase (r phase) of Cmsymmetry with the intermediate direction of polarization. All phases are separated by the lines of transitions of the second kind. Dependences of the elastic, electric and piezoelectric moduli on the magnitude of forced strain are plotted. It is shown that at the phase boundaries there is an anomalous change in the constants of the ferroelectric film and in the region of existence of the r phase, some moduli reach extreme values.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"leontyev-leontyeva-kuriganova-popov-maslova-glebova-nechitailov-zelenina-etal-characterizationoftheelectrocatalyticactivityofcarbonsupportedplatinumbasedcatalystsbythermalgravimetricanalysis-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0959943615002229\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'leontyev-leontyeva-kuriganova-popov-maslova-glebova-nechitailov-zelenina-etal-characterizationoftheelectrocatalyticactivityofcarbonsupportedplatinumbasedcatalystsbythermalgravimetricanalysis-2015', 'https://www.sciencedirect.com/science/article/pii/S0959943615002229', event);\">\n    Characterization of the electrocatalytic activity of carbon-supported platinum-based catalysts by thermal gravimetric analysis.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Leontyev, I. N.; Leontyeva, D. V.; Kuriganova, A. B.; Popov, Y. V.; Maslova, O. A.; Glebova, N. V.; Nechitailov, A. A.; Zelenina, N. K.; Tomasov, A. A.; Hennet, L.;  and Smirnova, N. V.\n</span>\n\n  \n\n</span>\n\n  <i>Mendeleev Communications</i>, 25(6): 468–469. November 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0959943615002229\"\n     onclick=\"log_download('leontyev-leontyeva-kuriganova-popov-maslova-glebova-nechitailov-zelenina-etal-characterizationoftheelectrocatalyticactivityofcarbonsupportedplatinumbasedcatalystsbythermalgravimetricanalysis-2015', 'https://www.sciencedirect.com/science/article/pii/S0959943615002229', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Characterization of the electrocatalytic activity of carbon-supported platinum-based catalysts by thermal gravimetric analysis [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.mencom.2015.11.024\"\n     onclick=\"log_download('leontyev-leontyeva-kuriganova-popov-maslova-glebova-nechitailov-zelenina-etal-characterizationoftheelectrocatalyticactivityofcarbonsupportedplatinumbasedcatalystsbythermalgravimetricanalysis-2015', 'http://doi.org/10.1016/j.mencom.2015.11.024', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/leontyev-leontyeva-kuriganova-popov-maslova-glebova-nechitailov-zelenina-etal-characterizationoftheelectrocatalyticactivityofcarbonsupportedplatinumbasedcatalystsbythermalgravimetricanalysis-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('leontyev-leontyeva-kuriganova-popov-maslova-glebova-nechitailov-zelenina-etal-characterizationoftheelectrocatalyticactivityofcarbonsupportedplatinumbasedcatalystsbythermalgravimetricanalysis-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{leontyev_characterization_2015,\n\ttitle = {Characterization of the electrocatalytic activity of carbon-supported platinum-based catalysts by thermal gravimetric analysis},\n\tvolume = {25},\n\tissn = {0959-9436},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0959943615002229},\n\tdoi = {10.1016/j.mencom.2015.11.024},\n\tabstract = {Investigations of carbon-supported Pt, Pt3Co, and Pt3Ni electrocatalysts using thermal gravimetric analysis (TGA) in combination with electrochemical measurements of the membrane electrode assemblies (MEA) for proton exchange membrane fuel cells have demonstrated that the onset temperature of the carbon support thermal oxidation and apparent activation energy of this reaction decrease in the following orders: Pt(20\\%)/C {\\textgreater} Pt(35\\%)/C {\\textgreater} Pt(46\\%)/C and Pt3Ni/C {\\textgreater} Pt3Co/C {\\textgreater} Pt/C, while MEA power density increases. Thus, TGA can be used as a simple and express technique for analysis of the electrocatalytic activity of carbon-supported Pt-based catalysts for proton exchange membrane fuel cells.},\n\tnumber = {6},\n\turldate = {2023-11-11},\n\tjournal = {Mendeleev Communications},\n\tauthor = {Leontyev, Igor N. and Leontyeva, Daria V. and Kuriganova, Alexandra B. and Popov, Yurii V. and Maslova, Olga A. and Glebova, Nadezhda V. and Nechitailov, Andrei A. and Zelenina, Natalia K. and Tomasov, Alexander A. and Hennet, Louis and Smirnova, Nina V.},\n\tmonth = nov,\n\tyear = {2015},\n\tpages = {468--469},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Investigations of carbon-supported Pt, Pt3Co, and Pt3Ni electrocatalysts using thermal gravimetric analysis (TGA) in combination with electrochemical measurements of the membrane electrode assemblies (MEA) for proton exchange membrane fuel cells have demonstrated that the onset temperature of the carbon support thermal oxidation and apparent activation energy of this reaction decrease in the following orders: Pt(20%)/C \\textgreater Pt(35%)/C \\textgreater Pt(46%)/C and Pt3Ni/C \\textgreater Pt3Co/C \\textgreater Pt/C, while MEA power density increases. Thus, TGA can be used as a simple and express technique for analysis of the electrocatalytic activity of carbon-supported Pt-based catalysts for proton exchange membrane fuel cells.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"golushko-rochal-lorman-complexinstabilityofaxiallycompressedtubularlipidmembranewithcontrolledspontaneouscurvature-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1140/epje/i2015-15112-6\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'golushko-rochal-lorman-complexinstabilityofaxiallycompressedtubularlipidmembranewithcontrolledspontaneouscurvature-2015', 'https://doi.org/10.1140/epje/i2015-15112-6', event);\">\n    Complex instability of axially compressed tubular lipid membrane with controlled spontaneous curvature.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Golushko, I. Y.; Rochal, S. B.;  and Lorman, V. L.\n</span>\n\n  \n\n</span>\n\n  <i>The European Physical Journal E</i>, 38(10): 112. October 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1140/epje/i2015-15112-6\"\n     onclick=\"log_download('golushko-rochal-lorman-complexinstabilityofaxiallycompressedtubularlipidmembranewithcontrolledspontaneouscurvature-2015', 'https://doi.org/10.1140/epje/i2015-15112-6', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Complex instability of axially compressed tubular lipid membrane with controlled spontaneous curvature [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1140/epje/i2015-15112-6\"\n     onclick=\"log_download('golushko-rochal-lorman-complexinstabilityofaxiallycompressedtubularlipidmembranewithcontrolledspontaneouscurvature-2015', 'http://doi.org/10.1140/epje/i2015-15112-6', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/golushko-rochal-lorman-complexinstabilityofaxiallycompressedtubularlipidmembranewithcontrolledspontaneouscurvature-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('golushko-rochal-lorman-complexinstabilityofaxiallycompressedtubularlipidmembranewithcontrolledspontaneouscurvature-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{golushko_complex_2015,\n\ttitle = {Complex instability of axially compressed tubular lipid membrane with controlled spontaneous curvature},\n\tvolume = {38},\n\tissn = {1292-895X},\n\turl = {https://doi.org/10.1140/epje/i2015-15112-6},\n\tdoi = {10.1140/epje/i2015-15112-6},\n\tabstract = {Tubular lipid membranes (TLMs) are formed by an external pulling force from artificial or biological bilayer vesicles and can be subsequently stabilized by incorporating proteins or amphiphilic polymers into the lipid bilayer. The arising spontaneous curvature of the lipid sheet allows switching off the pulling force without TLM destabilization. However, here we show that during this process two different thermal fluctuation modes drastically increase their amplitudes making fluctuations of the TLM much greater than its radius. Due to the system’s proximity to the critical fluctuation point, a weak axial compressive force is sufficient to destabilize the TLM. Its absolute value is shown to be much smaller than that of the pulling force required for the initial lipid nanotube formation. Induced complex instability was studied in the frame of Landau phase transition theory. The process involves two consecutive second-order phase transitions and leads to the tube deformation combining annular corrugation with completely unconventional chiral buckling.},\n\tlanguage = {en},\n\tnumber = {10},\n\turldate = {2023-11-11},\n\tjournal = {The European Physical Journal E},\n\tauthor = {Golushko, I. Yu. and Rochal, S. B. and Lorman, V. L.},\n\tmonth = oct,\n\tyear = {2015},\n\tkeywords = {Living systems: Biological Matter},\n\tpages = {112},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Tubular lipid membranes (TLMs) are formed by an external pulling force from artificial or biological bilayer vesicles and can be subsequently stabilized by incorporating proteins or amphiphilic polymers into the lipid bilayer. The arising spontaneous curvature of the lipid sheet allows switching off the pulling force without TLM destabilization. However, here we show that during this process two different thermal fluctuation modes drastically increase their amplitudes making fluctuations of the TLM much greater than its radius. Due to the system’s proximity to the critical fluctuation point, a weak axial compressive force is sufficient to destabilize the TLM. Its absolute value is shown to be much smaller than that of the pulling force required for the initial lipid nanotube formation. Induced complex instability was studied in the frame of Landau phase transition theory. The process involves two consecutive second-order phase transitions and leads to the tube deformation combining annular corrugation with completely unconventional chiral buckling.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"levshov-michel-arenal-tran-than-paillet-yuzyuk-sauvajol-interlayerdependenceofgmodesinsemiconductingdoublewalledcarbonnanotubes-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1021/acs.jpcc.5b05888\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'levshov-michel-arenal-tran-than-paillet-yuzyuk-sauvajol-interlayerdependenceofgmodesinsemiconductingdoublewalledcarbonnanotubes-2015', 'https://doi.org/10.1021/acs.jpcc.5b05888', event);\">\n    Interlayer Dependence of G-Modes in Semiconducting Double-Walled Carbon Nanotubes.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Levshov, D. I.; Michel, T.; Arenal, R.; Tran, H. N.; Than, T. X.; Paillet, M.; Yuzyuk, Y. I.;  and Sauvajol, J.\n</span>\n\n  \n\n</span>\n\n  <i>The Journal of Physical Chemistry C</i>, 119(40): 23196–23202. October 2015.\n  <span class=\"note\">Publisher: American Chemical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1021/acs.jpcc.5b05888\"\n     onclick=\"log_download('levshov-michel-arenal-tran-than-paillet-yuzyuk-sauvajol-interlayerdependenceofgmodesinsemiconductingdoublewalledcarbonnanotubes-2015', 'https://doi.org/10.1021/acs.jpcc.5b05888', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Interlayer Dependence of G-Modes in Semiconducting Double-Walled Carbon Nanotubes [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1021/acs.jpcc.5b05888\"\n     onclick=\"log_download('levshov-michel-arenal-tran-than-paillet-yuzyuk-sauvajol-interlayerdependenceofgmodesinsemiconductingdoublewalledcarbonnanotubes-2015', 'http://doi.org/10.1021/acs.jpcc.5b05888', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/levshov-michel-arenal-tran-than-paillet-yuzyuk-sauvajol-interlayerdependenceofgmodesinsemiconductingdoublewalledcarbonnanotubes-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('levshov-michel-arenal-tran-than-paillet-yuzyuk-sauvajol-interlayerdependenceofgmodesinsemiconductingdoublewalledcarbonnanotubes-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{levshov_interlayer_2015,\n\ttitle = {Interlayer {Dependence} of {G}-{Modes} in {Semiconducting} {Double}-{Walled} {Carbon} {Nanotubes}},\n\tvolume = {119},\n\tissn = {1932-7447},\n\turl = {https://doi.org/10.1021/acs.jpcc.5b05888},\n\tdoi = {10.1021/acs.jpcc.5b05888},\n\tabstract = {A double-walled carbon nanotube (DWNT), a coaxial composite of two single-walled carbon nanotubes (SWNT), provides a unique model to study interactions between the two constituent SWNTs. Combining high resolution transmission electron microscopy (HRTEM), electron diffraction (ED), and resonant Raman scattering (RRS) experiments on the same individual suspended DWNT is the ultimate way to relate unambiguously its atomic structure, defined by the chiral indices of the coaxial outer/inner SWNTs, and its Raman-active vibration modes. This approach is used to investigate the intertube distance dependence of the G-modes of individual index-identified DWNTs composed of two semiconducting SWNTs. We state the main features of the dependence of the G-mode frequencies on the distance between the inner and outer layers: (i) When the interlayer distance is larger than the nominal van der Waals distance (close to 0.34 nm), a downshift of the inner-layer G-modes with respect to the G-modes in the equivalent SWNTs is measured. (ii) The amplitude of the downshift depends on the interlayer distance, or in other words, on the negative pressure felt by the inner layer in DWNT. (iii) No shift is observed for an intertube distance close to 0.34 nm.},\n\tnumber = {40},\n\turldate = {2023-11-11},\n\tjournal = {The Journal of Physical Chemistry C},\n\tauthor = {Levshov, D. I. and Michel, T. and Arenal, R. and Tran, H. N. and Than, T. X. and Paillet, M. and Yuzyuk, Yu. I. and Sauvajol, J.-L.},\n\tmonth = oct,\n\tyear = {2015},\n\tnote = {Publisher: American Chemical Society},\n\tpages = {23196--23202},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\M5V5TPZR\\\\Levshov и др. - 2015 - Interlayer Dependence of G-Modes in Semiconducting.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A double-walled carbon nanotube (DWNT), a coaxial composite of two single-walled carbon nanotubes (SWNT), provides a unique model to study interactions between the two constituent SWNTs. Combining high resolution transmission electron microscopy (HRTEM), electron diffraction (ED), and resonant Raman scattering (RRS) experiments on the same individual suspended DWNT is the ultimate way to relate unambiguously its atomic structure, defined by the chiral indices of the coaxial outer/inner SWNTs, and its Raman-active vibration modes. This approach is used to investigate the intertube distance dependence of the G-modes of individual index-identified DWNTs composed of two semiconducting SWNTs. We state the main features of the dependence of the G-mode frequencies on the distance between the inner and outer layers: (i) When the interlayer distance is larger than the nominal van der Waals distance (close to 0.34 nm), a downshift of the inner-layer G-modes with respect to the G-modes in the equivalent SWNTs is measured. (ii) The amplitude of the downshift depends on the interlayer distance, or in other words, on the negative pressure felt by the inner layer in DWNT. (iii) No shift is observed for an intertube distance close to 0.34 nm.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-kalinchuk-shakhovoy-yuzyuk-theproblemofdeterminingelasticconstantsofthinferroelectricfilms-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1028335815080108\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-kalinchuk-shakhovoy-yuzyuk-theproblemofdeterminingelasticconstantsofthinferroelectricfilms-2015', 'https://doi.org/10.1134/S1028335815080108', event);\">\n    The problem of determining elastic constants of thin ferroelectric films.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.; Kalinchuk, V. V.; Shakhovoy, R. A.;  and Yuzyuk, Y. I.\n</span>\n\n  \n\n</span>\n\n  <i>Doklady Physics</i>, 60(8): 349–354. August 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1028335815080108\"\n     onclick=\"log_download('shirokov-kalinchuk-shakhovoy-yuzyuk-theproblemofdeterminingelasticconstantsofthinferroelectricfilms-2015', 'https://doi.org/10.1134/S1028335815080108', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"The problem of determining elastic constants of thin ferroelectric films [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1028335815080108\"\n     onclick=\"log_download('shirokov-kalinchuk-shakhovoy-yuzyuk-theproblemofdeterminingelasticconstantsofthinferroelectricfilms-2015', 'http://doi.org/10.1134/S1028335815080108', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-kalinchuk-shakhovoy-yuzyuk-theproblemofdeterminingelasticconstantsofthinferroelectricfilms-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-kalinchuk-shakhovoy-yuzyuk-theproblemofdeterminingelasticconstantsofthinferroelectricfilms-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_problem_2015,\n\ttitle = {The problem of determining elastic constants of thin ferroelectric films},\n\tvolume = {60},\n\tissn = {1562-6903},\n\turl = {https://doi.org/10.1134/S1028335815080108},\n\tdoi = {10.1134/S1028335815080108},\n\tabstract = {A method of determining the constants of the linear equations of the piezoelectric effect dependent on the external conditions is proposed for thin ferroelectric films on the basis of the Landau potential of the phenomenological theory of phase transitions. By the example of single-crystalline barium—titanate thin films, the behavior of material constants is investigated in dependence on the value of the misfit strain. The investigation of material equations is implemented on the basis of the Landau potential of the eighth degree at room temperature. The substantial difference in the elastic, electric, and piezoelectric properties of a thin film from those of a bulk material is shown; the anomalous behavior of constants on the phase boundaries and the extremal behavior inside the r-phase is revealed.},\n\tlanguage = {en},\n\tnumber = {8},\n\turldate = {2023-11-11},\n\tjournal = {Doklady Physics},\n\tauthor = {Shirokov, V. B. and Kalinchuk, V. V. and Shakhovoy, R. A. and Yuzyuk, Yu. I.},\n\tmonth = aug,\n\tyear = {2015},\n\tkeywords = {Barium Titanate, DOKLADY Physic, Elastic Constant, Misfit Strain, Piezoelectric Effect},\n\tpages = {349--354},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A method of determining the constants of the linear equations of the piezoelectric effect dependent on the external conditions is proposed for thin ferroelectric films on the basis of the Landau potential of the phenomenological theory of phase transitions. By the example of single-crystalline barium—titanate thin films, the behavior of material constants is investigated in dependence on the value of the misfit strain. The investigation of material equations is implemented on the basis of the Landau potential of the eighth degree at room temperature. The substantial difference in the elastic, electric, and piezoelectric properties of a thin film from those of a bulk material is shown; the anomalous behavior of constants on the phase boundaries and the extremal behavior inside the r-phase is revealed.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"motovilov-gagkaeva-kadyrov-zhukova-tobokhova-torgashev-savinov-grinenko-etal-terahertzandinfraredspectroscopyofbacterialnanofilaments-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://ieeexplore.ieee.org/document/7327875\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'motovilov-gagkaeva-kadyrov-zhukova-tobokhova-torgashev-savinov-grinenko-etal-terahertzandinfraredspectroscopyofbacterialnanofilaments-2015', 'https://ieeexplore.ieee.org/document/7327875', event);\">\n    Terahertz and infrared spectroscopy of bacterial nanofilaments.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Motovilov, K. A.; Gagkaeva, Z. V.; Kadyrov, L. S.; Zhukova, E. S.; Tobokhova, A. S.; Torgashev, V. I.; Savinov, M.; Grinenko, V.; Belyanchikov, M. A.; Sidoruk, K. V.; Dressel, M.;  and Gorshunov, B. P.\n</span>\n\n  \n\n</span>\n\n  In <i>2015 40th International Conference on Infrared, Millimeter, and Terahertz waves (IRMMW-THz)</i>, pages 1–2, August 2015. \n  <span class=\"note\">ISSN: 2162-2035</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://ieeexplore.ieee.org/document/7327875\"\n     onclick=\"log_download('motovilov-gagkaeva-kadyrov-zhukova-tobokhova-torgashev-savinov-grinenko-etal-terahertzandinfraredspectroscopyofbacterialnanofilaments-2015', 'https://ieeexplore.ieee.org/document/7327875', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Terahertz and infrared spectroscopy of bacterial nanofilaments [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1109/IRMMW-THz.2015.7327875\"\n     onclick=\"log_download('motovilov-gagkaeva-kadyrov-zhukova-tobokhova-torgashev-savinov-grinenko-etal-terahertzandinfraredspectroscopyofbacterialnanofilaments-2015', 'http://doi.org/10.1109/IRMMW-THz.2015.7327875', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/motovilov-gagkaeva-kadyrov-zhukova-tobokhova-torgashev-savinov-grinenko-etal-terahertzandinfraredspectroscopyofbacterialnanofilaments-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('motovilov-gagkaeva-kadyrov-zhukova-tobokhova-torgashev-savinov-grinenko-etal-terahertzandinfraredspectroscopyofbacterialnanofilaments-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{motovilov_terahertz_2015,\n\ttitle = {Terahertz and infrared spectroscopy of bacterial nanofilaments},\n\turl = {https://ieeexplore.ieee.org/document/7327875},\n\tdoi = {10.1109/IRMMW-THz.2015.7327875},\n\tabstract = {By means of terahertz and infrared (THz, IR) spectroscopies we have measured the dielectric response of nano-filaments of electrogenic bacteria Shewanella oneidensis MR-1 in a wide frequency and temperature ranges. THz-far-IR spectra are dominated by absorption due to bound water. At helium temperatures and at sub-THz frequencies a boson-peak-like excitation is detected that is typical for disordered materials. The observation is in agreement with the heat capacity measurements.},\n\turldate = {2023-11-11},\n\tbooktitle = {2015 40th {International} {Conference} on {Infrared}, {Millimeter}, and {Terahertz} waves ({IRMMW}-{THz})},\n\tauthor = {Motovilov, Konstantin A. and Gagkaeva, Zarina V. and Kadyrov, Lenar S. and Zhukova, Elena S. and Tobokhova, Aiyyna S. and Torgashev, Victor I. and Savinov, Maxim and Grinenko, Vadim and Belyanchikov, Mikhail A. and Sidoruk, Konstantin V. and Dressel, Martin and Gorshunov, Boris P.},\n\tmonth = aug,\n\tyear = {2015},\n\tnote = {ISSN: 2162-2035},\n\tpages = {1--2},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  By means of terahertz and infrared (THz, IR) spectroscopies we have measured the dielectric response of nano-filaments of electrogenic bacteria Shewanella oneidensis MR-1 in a wide frequency and temperature ranges. THz-far-IR spectra are dominated by absorption due to bound water. At helium temperatures and at sub-THz frequencies a boson-peak-like excitation is detected that is typical for disordered materials. The observation is in agreement with the heat capacity measurements.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"yohannes-belenov-guterman-skibina-volotchaev-lyanguzov-effectofethyleneglycolonelectrochemicalandmorphologicalfeaturesofplatinumelectrodepositsfromchloroplatinicacid-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1007/s10800-015-0820-5\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'yohannes-belenov-guterman-skibina-volotchaev-lyanguzov-effectofethyleneglycolonelectrochemicalandmorphologicalfeaturesofplatinumelectrodepositsfromchloroplatinicacid-2015', 'https://doi.org/10.1007/s10800-015-0820-5', event);\">\n    Effect of ethylene glycol on electrochemical and morphological features of platinum electrodeposits from chloroplatinic acid.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Yohannes, W.; Belenov, S. V.; Guterman, V. E.; Skibina, L. M.; Volotchaev, V. A.;  and Lyanguzov, N. V.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Applied Electrochemistry</i>, 45(6): 623–633. June 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1007/s10800-015-0820-5\"\n     onclick=\"log_download('yohannes-belenov-guterman-skibina-volotchaev-lyanguzov-effectofethyleneglycolonelectrochemicalandmorphologicalfeaturesofplatinumelectrodepositsfromchloroplatinicacid-2015', 'https://doi.org/10.1007/s10800-015-0820-5', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Effect of ethylene glycol on electrochemical and morphological features of platinum electrodeposits from chloroplatinic acid [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1007/s10800-015-0820-5\"\n     onclick=\"log_download('yohannes-belenov-guterman-skibina-volotchaev-lyanguzov-effectofethyleneglycolonelectrochemicalandmorphologicalfeaturesofplatinumelectrodepositsfromchloroplatinicacid-2015', 'http://doi.org/10.1007/s10800-015-0820-5', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/yohannes-belenov-guterman-skibina-volotchaev-lyanguzov-effectofethyleneglycolonelectrochemicalandmorphologicalfeaturesofplatinumelectrodepositsfromchloroplatinicacid-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('yohannes-belenov-guterman-skibina-volotchaev-lyanguzov-effectofethyleneglycolonelectrochemicalandmorphologicalfeaturesofplatinumelectrodepositsfromchloroplatinicacid-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{yohannes_effect_2015,\n\ttitle = {Effect of ethylene glycol on electrochemical and morphological features of platinum electrodeposits from chloroplatinic acid},\n\tvolume = {45},\n\tissn = {1572-8838},\n\turl = {https://doi.org/10.1007/s10800-015-0820-5},\n\tdoi = {10.1007/s10800-015-0820-5},\n\tabstract = {The aim of this work was to investigate the morphology, average size, and the electrochemical behavior of platinum nanoparticles electrodeposited from water and mixed water–ethylene glycol solutions of the electrolyte of H2PtCl6 and H2SO4 at a rotating disk electrode coated with Vulcan XC-72 carbon powder. Cyclic voltammetry and linear sweep voltammetry were used to determine the electrochemically active surface area (ESA) and oxygen reduction reaction (ORR) activity of the prepared Pt/C materials, respectively. XRD and scanning electron microscopy were used to study the influence of the electrodeposition methods applied on the morphology of platinum particles deposited in water and mixed water–ethylene glycol solutions. The average size of Pt crystallites was in the range of ca. 6–10 nm, and the average size of deposited Pt particles was in the range of ca. 30–150 nm. It was found that the presence of ethylene glycol in the electrolyte solution increased the overpotential of electrodeposition and it also strongly affected the morphology of Pt deposits when constant current electrodeposition was employed. Moreover, it was shown that pulse current electrodeposition is a more effective method compared to constant current electrodeposition method for the preparation of the Pt/Vulcan electrode with high ESA of Pt and enhanced catalytic activity toward ORR. The results obtained concerning the morphology and the spatial distribution of platinum particles electrodeposited on the surface of carbon support at different conditions demonstrate new possibilities to improve synthesis of Pt/C by electrodeposition methods.},\n\tlanguage = {en},\n\tnumber = {6},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Applied Electrochemistry},\n\tauthor = {Yohannes, Weldegebriel and Belenov, S. V. and Guterman, V. E. and Skibina, L. M. and Volotchaev, V. A. and Lyanguzov, N. V.},\n\tmonth = jun,\n\tyear = {2015},\n\tkeywords = {Platinum, Electrocatalyst, Galvanostatic electrodeposition, ORR, Vulcan XC-72},\n\tpages = {623--633},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The aim of this work was to investigate the morphology, average size, and the electrochemical behavior of platinum nanoparticles electrodeposited from water and mixed water–ethylene glycol solutions of the electrolyte of H2PtCl6 and H2SO4 at a rotating disk electrode coated with Vulcan XC-72 carbon powder. Cyclic voltammetry and linear sweep voltammetry were used to determine the electrochemically active surface area (ESA) and oxygen reduction reaction (ORR) activity of the prepared Pt/C materials, respectively. XRD and scanning electron microscopy were used to study the influence of the electrodeposition methods applied on the morphology of platinum particles deposited in water and mixed water–ethylene glycol solutions. The average size of Pt crystallites was in the range of ca. 6–10 nm, and the average size of deposited Pt particles was in the range of ca. 30–150 nm. It was found that the presence of ethylene glycol in the electrolyte solution increased the overpotential of electrodeposition and it also strongly affected the morphology of Pt deposits when constant current electrodeposition was employed. Moreover, it was shown that pulse current electrodeposition is a more effective method compared to constant current electrodeposition method for the preparation of the Pt/Vulcan electrode with high ESA of Pt and enhanced catalytic activity toward ORR. The results obtained concerning the morphology and the spatial distribution of platinum particles electrodeposited on the surface of carbon support at different conditions demonstrate new possibilities to improve synthesis of Pt/C by electrodeposition methods.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"avramenko-golushko-myasnikova-rochal-vibrationalheatcapacityofcarbonnanotubesatlowandultralowtemperatures-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S138694771400472X\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'avramenko-golushko-myasnikova-rochal-vibrationalheatcapacityofcarbonnanotubesatlowandultralowtemperatures-2015', 'https://www.sciencedirect.com/science/article/pii/S138694771400472X', event);\">\n    Vibrational heat capacity of carbon nanotubes at low and ultra-low temperatures.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Avramenko, M. V.; Golushko, I. Y.; Myasnikova, A. E.;  and Rochal, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Physica E: Low-dimensional Systems and Nanostructures</i>, 68: 133–139. April 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S138694771400472X\"\n     onclick=\"log_download('avramenko-golushko-myasnikova-rochal-vibrationalheatcapacityofcarbonnanotubesatlowandultralowtemperatures-2015', 'https://www.sciencedirect.com/science/article/pii/S138694771400472X', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Vibrational heat capacity of carbon nanotubes at low and ultra-low temperatures [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.physe.2014.12.033\"\n     onclick=\"log_download('avramenko-golushko-myasnikova-rochal-vibrationalheatcapacityofcarbonnanotubesatlowandultralowtemperatures-2015', 'http://doi.org/10.1016/j.physe.2014.12.033', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/avramenko-golushko-myasnikova-rochal-vibrationalheatcapacityofcarbonnanotubesatlowandultralowtemperatures-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('avramenko-golushko-myasnikova-rochal-vibrationalheatcapacityofcarbonnanotubesatlowandultralowtemperatures-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{avramenko_vibrational_2015,\n\ttitle = {Vibrational heat capacity of carbon nanotubes at low and ultra-low temperatures},\n\tvolume = {68},\n\tissn = {1386-9477},\n\turl = {https://www.sciencedirect.com/science/article/pii/S138694771400472X},\n\tdoi = {10.1016/j.physe.2014.12.033},\n\tabstract = {To measure a heat capacity of a single carbon nanotube is impossible nowadays and experiments are performed with the nanotubes bundles. However, the existing theories of carbon nanotubes heat capacity do not take into account an interaction between an individual nanotube and its environment. Here we show that due to this fact the known theories overestimate the heat capacity in the ultra-low temperature limit. In this region the main contribution to heat capacity of a single free nanotube is caused by the bending phonon mode with a quadratic dispersion. At T=1K different known models of the phonon dynamics lead to the theoretical specific heat which is at least 10 times greater than the experimentally measured value. To overcome this contradiction we take into account the interaction between an individual nanotube and its environment. As a result, the nanotube loses its Goldstone degrees of freedom and essential reconstruction of the lowest-energy part of its phonon spectrum occurs. The theory proposed explains experimental data on thermal capacity in the ultra-low temperature range and simultaneously demonstrates better agreement with experiments in the region 2.5K{\\textless}T{\\textless}40K than the preceding models.},\n\turldate = {2023-11-11},\n\tjournal = {Physica E: Low-dimensional Systems and Nanostructures},\n\tauthor = {Avramenko, M. V. and Golushko, I. Yu. and Myasnikova, A. E. and Rochal, S. B.},\n\tmonth = apr,\n\tyear = {2015},\n\tkeywords = {2D membranes, Carbon nanotubes, Heat capacity, Low temperatures, Phonon spectrum, Pinning},\n\tpages = {133--139},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\QUQ3BBJ9\\\\Avramenko и др. - 2015 - Vibrational heat capacity of carbon nanotubes at l.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  To measure a heat capacity of a single carbon nanotube is impossible nowadays and experiments are performed with the nanotubes bundles. However, the existing theories of carbon nanotubes heat capacity do not take into account an interaction between an individual nanotube and its environment. Here we show that due to this fact the known theories overestimate the heat capacity in the ultra-low temperature limit. In this region the main contribution to heat capacity of a single free nanotube is caused by the bending phonon mode with a quadratic dispersion. At T=1K different known models of the phonon dynamics lead to the theoretical specific heat which is at least 10 times greater than the experimentally measured value. To overcome this contradiction we take into account the interaction between an individual nanotube and its environment. As a result, the nanotube loses its Goldstone degrees of freedom and essential reconstruction of the lowest-energy part of its phonon spectrum occurs. The theory proposed explains experimental data on thermal capacity in the ultra-low temperature range and simultaneously demonstrates better agreement with experiments in the region 2.5K\\textlessT\\textless40K than the preceding models.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"chernovyants-starikova-kolesnikova-karginova-lyanguzov-synthesisandstructureofinteractionproductsofquinoline21hthionewithmoleculariodine-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S1386142514018551\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'chernovyants-starikova-kolesnikova-karginova-lyanguzov-synthesisandstructureofinteractionproductsofquinoline21hthionewithmoleculariodine-2015', 'https://www.sciencedirect.com/science/article/pii/S1386142514018551', event);\">\n    Synthesis and structure of interaction products of quinoline-2(1H)-thione with molecular iodine.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Chernov’yants, M. S.; Starikova, Z. A.; Kolesnikova, T. S.; Karginova, A. O.;  and Lyanguzov, N. V.\n</span>\n\n  \n\n</span>\n\n  <i>Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy</i>, 139: 533–538. March 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S1386142514018551\"\n     onclick=\"log_download('chernovyants-starikova-kolesnikova-karginova-lyanguzov-synthesisandstructureofinteractionproductsofquinoline21hthionewithmoleculariodine-2015', 'https://www.sciencedirect.com/science/article/pii/S1386142514018551', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Synthesis and structure of interaction products of quinoline-2(1H)-thione with molecular iodine [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.saa.2014.12.075\"\n     onclick=\"log_download('chernovyants-starikova-kolesnikova-karginova-lyanguzov-synthesisandstructureofinteractionproductsofquinoline21hthionewithmoleculariodine-2015', 'http://doi.org/10.1016/j.saa.2014.12.075', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/chernovyants-starikova-kolesnikova-karginova-lyanguzov-synthesisandstructureofinteractionproductsofquinoline21hthionewithmoleculariodine-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('chernovyants-starikova-kolesnikova-karginova-lyanguzov-synthesisandstructureofinteractionproductsofquinoline21hthionewithmoleculariodine-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{chernovyants_synthesis_2015,\n\ttitle = {Synthesis and structure of interaction products of quinoline-2({1H})-thione with molecular iodine},\n\tvolume = {139},\n\tissn = {1386-1425},\n\turl = {https://www.sciencedirect.com/science/article/pii/S1386142514018551},\n\tdoi = {10.1016/j.saa.2014.12.075},\n\tabstract = {The behavior of quinoline-2(1H)-thione, which is a potential antithyroid drug toward molecular iodine, was investigated. The ability of quinoline-2(1H)-thione to form the outer-sphere charge-transfer complex C9H7NS·I2 with iodine molecular in dilute chloroform solution has been studied by UV–vis spectroscopy (lgβ=3.85). The crystal structure of the new salt 2-(quinoline-2-yldisulfanyl)quinolinium triiodide – product of irreversible oxidation of quinoline-2(1H)-thione was determined by X-ray diffraction. The 2-(quinoline-2-yldisulfanyl)quinolinium cations form dimers through π–π–stacking interaction between quinoline rings. Strong intramolecular interactions are observed between iodine – sulfur atoms and iodine – hydrogen atoms with shortened contacts (less of sum of van der Waals contacts). It is noteworthy that two perfectly centrosymmetrical anions I3− form a very short contact I(3)⋯I(3′) 3.7550(5) so we can state the formation of the dianion I62−. Therefore the formation and topology of polyiodide species depend on the characteristics, such as shape, size and charge, etc., of the counter cation, 2-(quinoline-2-yldisulfanyl)quinolinium, which is considered as templating agent.},\n\turldate = {2023-11-11},\n\tjournal = {Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy},\n\tauthor = {Chernov’yants, Margarita S. and Starikova, Zoya A. and Kolesnikova, Tatiana S. and Karginova, Anastasia O. and Lyanguzov, Nikolay V.},\n\tmonth = mar,\n\tyear = {2015},\n\tkeywords = {X-ray diffraction, Raman spectroscopy, 2-(quinoline-2-yldisulfanyl)quinolinium triiodide, Charge-transfer complex, IR, Quinoline-2(1)-thione},\n\tpages = {533--538},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The behavior of quinoline-2(1H)-thione, which is a potential antithyroid drug toward molecular iodine, was investigated. The ability of quinoline-2(1H)-thione to form the outer-sphere charge-transfer complex C9H7NS·I2 with iodine molecular in dilute chloroform solution has been studied by UV–vis spectroscopy (lgβ=3.85). The crystal structure of the new salt 2-(quinoline-2-yldisulfanyl)quinolinium triiodide – product of irreversible oxidation of quinoline-2(1H)-thione was determined by X-ray diffraction. The 2-(quinoline-2-yldisulfanyl)quinolinium cations form dimers through π–π–stacking interaction between quinoline rings. Strong intramolecular interactions are observed between iodine – sulfur atoms and iodine – hydrogen atoms with shortened contacts (less of sum of van der Waals contacts). It is noteworthy that two perfectly centrosymmetrical anions I3− form a very short contact I(3)⋯I(3′) 3.7550(5) so we can state the formation of the dianion I62−. Therefore the formation and topology of polyiodide species depend on the characteristics, such as shape, size and charge, etc., of the counter cation, 2-(quinoline-2-yldisulfanyl)quinolinium, which is considered as templating agent.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"roshal-myasnikova-rochal-slightlybrokenicosahedralsymmetryadvancesthomsonproblem-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0375960114011682\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'roshal-myasnikova-rochal-slightlybrokenicosahedralsymmetryadvancesthomsonproblem-2015', 'https://www.sciencedirect.com/science/article/pii/S0375960114011682', event);\">\n    Slightly broken icosahedral symmetry advances Thomson problem.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Roshal, D. S.; Myasnikova, A. E.;  and Rochal, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Physics Letters A</i>, 379(4): 372–376. February 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0375960114011682\"\n     onclick=\"log_download('roshal-myasnikova-rochal-slightlybrokenicosahedralsymmetryadvancesthomsonproblem-2015', 'https://www.sciencedirect.com/science/article/pii/S0375960114011682', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Slightly broken icosahedral symmetry advances Thomson problem [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.physleta.2014.11.039\"\n     onclick=\"log_download('roshal-myasnikova-rochal-slightlybrokenicosahedralsymmetryadvancesthomsonproblem-2015', 'http://doi.org/10.1016/j.physleta.2014.11.039', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/roshal-myasnikova-rochal-slightlybrokenicosahedralsymmetryadvancesthomsonproblem-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('roshal-myasnikova-rochal-slightlybrokenicosahedralsymmetryadvancesthomsonproblem-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{roshal_slightly_2015,\n\ttitle = {Slightly broken icosahedral symmetry advances {Thomson} problem},\n\tvolume = {379},\n\tissn = {0375-9601},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0375960114011682},\n\tdoi = {10.1016/j.physleta.2014.11.039},\n\tabstract = {To advance Thomson problem we generalize physical principles suggested by Caspar and Klug (CK) to model icosahedral capsids. Proposed simplest distortions of the CK spherical arrangements yield new-type trial structures very close to the lowest energy ones. In the region 600≤N≤1000, where N is the number of particles in the structure, we found 40 new spherical crystals with the lowest ever seen energies and curvature-induced topological defects being not the well-known elongated scars but flatten pentagons. These crystals have N values prohibited in the CK model and demonstrate a new way to combine the local hexagonal order and spherical geometry.},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Physics Letters A},\n\tauthor = {Roshal, D. S. and Myasnikova, A. E. and Rochal, S. B.},\n\tmonth = feb,\n\tyear = {2015},\n\tkeywords = {Topological defects, Caspar and Klug theory, Self-assembly, Spherical crystals, Thomson problem, Viral capsids},\n\tpages = {372--376},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\I3PW53KV\\\\Roshal и др. - 2015 - Slightly broken icosahedral symmetry advances Thom.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  To advance Thomson problem we generalize physical principles suggested by Caspar and Klug (CK) to model icosahedral capsids. Proposed simplest distortions of the CK spherical arrangements yield new-type trial structures very close to the lowest energy ones. In the region 600≤N≤1000, where N is the number of particles in the structure, we found 40 new spherical crystals with the lowest ever seen energies and curvature-induced topological defects being not the well-known elongated scars but flatten pentagons. These crystals have N values prohibited in the CK model and demonstrate a new way to combine the local hexagonal order and spherical geometry.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"anokhin-gorelik-dovbeshko-pyatyshev-yuzyuk-differenceramanspectroscopyofdnamolecules-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/584/1/012022\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'anokhin-gorelik-dovbeshko-pyatyshev-yuzyuk-differenceramanspectroscopyofdnamolecules-2015', 'https://dx.doi.org/10.1088/1742-6596/584/1/012022', event);\">\n    Difference Raman spectroscopy of DNA molecules.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Anokhin, A. S.; Gorelik, V. S.; Dovbeshko, G. I.; Pyatyshev, A. Y.;  and Yuzyuk, Y. I.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics: Conference Series</i>, 584(1): 012022. January 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/584/1/012022\"\n     onclick=\"log_download('anokhin-gorelik-dovbeshko-pyatyshev-yuzyuk-differenceramanspectroscopyofdnamolecules-2015', 'https://dx.doi.org/10.1088/1742-6596/584/1/012022', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Difference Raman spectroscopy of DNA molecules [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/1742-6596/584/1/012022\"\n     onclick=\"log_download('anokhin-gorelik-dovbeshko-pyatyshev-yuzyuk-differenceramanspectroscopyofdnamolecules-2015', 'http://doi.org/10.1088/1742-6596/584/1/012022', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/anokhin-gorelik-dovbeshko-pyatyshev-yuzyuk-differenceramanspectroscopyofdnamolecules-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('anokhin-gorelik-dovbeshko-pyatyshev-yuzyuk-differenceramanspectroscopyofdnamolecules-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{anokhin_difference_2015,\n\ttitle = {Difference {Raman} spectroscopy of {DNA} molecules},\n\tvolume = {584},\n\tissn = {1742-6596},\n\turl = {https://dx.doi.org/10.1088/1742-6596/584/1/012022},\n\tdoi = {10.1088/1742-6596/584/1/012022},\n\tabstract = {In this paper the micro-Raman spectra of calf DNA for different points of DNA sample have been recorded. The Raman spectra were made with help of difference Raman spectroscopy technique. Raman spectra were recorded with high spatial resolution from different points of the wet and dry samples in different spectral range (100÷4000cm−1) using two lasers: argon (514.5 nm) and helium -neon (632.8 nm). The significant differences in the Raman spectra for dry and wet DNA and for different points of DNA molecules were observed. The obtained data on difference Raman scattering spectra of DNA molecules may be used for identification of DNA types and for analysis of genetic information associated with the molecular structure of this molecule.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics: Conference Series},\n\tauthor = {Anokhin, Andrey S. and Gorelik, Vladimir S. and Dovbeshko, Galina I. and Pyatyshev, Alexander Yu and Yuzyuk, Yury I.},\n\tmonth = jan,\n\tyear = {2015},\n\tpages = {012022},\n\tfile = {IOP Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\B6MCEJV5\\\\Anokhin и др. - 2015 - Difference Raman spectroscopy of DNA molecules.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  In this paper the micro-Raman spectra of calf DNA for different points of DNA sample have been recorded. The Raman spectra were made with help of difference Raman spectroscopy technique. Raman spectra were recorded with high spatial resolution from different points of the wet and dry samples in different spectral range (100÷4000cm−1) using two lasers: argon (514.5 nm) and helium -neon (632.8 nm). The significant differences in the Raman spectra for dry and wet DNA and for different points of DNA molecules were observed. The obtained data on difference Raman scattering spectra of DNA molecules may be used for identification of DNA types and for analysis of genetic information associated with the molecular structure of this molecule.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"baudry-lukyanchuk-razumnaya-dynamicsoffieldinducedpolarizationreversalinthinstrainedperovskiteferroelectricfilmswithiiorientedpolarization-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.91.144110\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'baudry-lukyanchuk-razumnaya-dynamicsoffieldinducedpolarizationreversalinthinstrainedperovskiteferroelectricfilmswithiiorientedpolarization-2015', 'https://link.aps.org/doi/10.1103/PhysRevB.91.144110', event);\">\n    Dynamics of field-induced polarization reversal in thin strained perovskite ferroelectric films with <i>с</i>-oriented polarization.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Baudry, L.; Luk'yanchuk, I. A.;  and Razumnaya, A.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 91(14): 144110. April 2015.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.91.144110\"\n     onclick=\"log_download('baudry-lukyanchuk-razumnaya-dynamicsoffieldinducedpolarizationreversalinthinstrainedperovskiteferroelectricfilmswithiiorientedpolarization-2015', 'https://link.aps.org/doi/10.1103/PhysRevB.91.144110', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Dynamics of field-induced polarization reversal in thin strained perovskite ferroelectric films with &lt;i&gt;с&lt;/i&gt;-oriented polarization [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.91.144110\"\n     onclick=\"log_download('baudry-lukyanchuk-razumnaya-dynamicsoffieldinducedpolarizationreversalinthinstrainedperovskiteferroelectricfilmswithiiorientedpolarization-2015', 'http://doi.org/10.1103/PhysRevB.91.144110', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/baudry-lukyanchuk-razumnaya-dynamicsoffieldinducedpolarizationreversalinthinstrainedperovskiteferroelectricfilmswithiiorientedpolarization-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('baudry-lukyanchuk-razumnaya-dynamicsoffieldinducedpolarizationreversalinthinstrainedperovskiteferroelectricfilmswithiiorientedpolarization-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{baudry_dynamics_2015,\n\ttitle = {Dynamics of field-induced polarization reversal in thin strained perovskite ferroelectric films with \\textit{с}-oriented polarization},\n\tvolume = {91},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.91.144110},\n\tdoi = {10.1103/PhysRevB.91.144110},\n\tabstract = {The field-induced polarization reversal in the c-oriented ferroelectric phase of strained perovskite film has been studied. We show that in addition to the conventional longitudinal switching mechanism, when the c-oriented polarization vector changes its modulus, the longitudinal-transversal and transversal mechanisms when the perpendicular component of polarization is dynamically admixed are possible. The latter process can occur either via the straight-abrupt or initially continues polarization turnover scenario. We specified the obtained results for the case of PbTiO3 and BaTiO3 ferroelectrics and propose the experimental methods for their investigation.},\n\tnumber = {14},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Baudry, Laurent and Luk&#x27;yanchuk, Igor A. and Razumnaya, Anna},\n\tmonth = apr,\n\tyear = {2015},\n\tnote = {Publisher: American Physical Society},\n\tpages = {144110},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\TC6IA8BZ\\\\Baudry и др. - 2015 - Dynamics of field-induced polarization reversal in.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The field-induced polarization reversal in the c-oriented ferroelectric phase of strained perovskite film has been studied. We show that in addition to the conventional longitudinal switching mechanism, when the c-oriented polarization vector changes its modulus, the longitudinal-transversal and transversal mechanisms when the perpendicular component of polarization is dynamically admixed are possible. The latter process can occur either via the straight-abrupt or initially continues polarization turnover scenario. We specified the obtained results for the case of PbTiO3 and BaTiO3 ferroelectrics and propose the experimental methods for their investigation.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------cotextrm1xfetextrmxcrtextrm2o4x010205-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/42621\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------cotextrm1xfetextrmxcrtextrm2o4x010205-2015', 'http://journals.ioffe.ru/articles/42621', event);\">\n    Рентгеноэлектронное и мессбауэровское исследования валентного состояния ионов переходных металлов в керамиках Co$_{\\textrm{1-x}}$Fe$_{\\textrm{x}}$Cr$_{\\textrm{2}}$O4 (x=0.1,0.2, 0.5).\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Кочур, А. Г.; Гуглев, К. А.; Козаков, А. Т.; Кубрин, С. П.; Никольский, А. В.;  and Торгашев, В. И.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 58(1): 108–113. December 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/42621\"\n     onclick=\"log_download('------cotextrm1xfetextrmxcrtextrm2o4x010205-2015', 'http://journals.ioffe.ru/articles/42621', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Рентгеноэлектронное и мессбауэровское исследования валентного состояния ионов переходных металлов в керамиках Co$_{\\textrm{1-x}}$Fe$_{\\textrm{x}}$Cr$_{\\textrm{2}}$O4 (x=0.1,0.2, 0.5) [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------cotextrm1xfetextrmxcrtextrm2o4x010205-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------cotextrm1xfetextrmxcrtextrm2o4x010205-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2015,\n\ttitle = {Рентгеноэлектронное и мессбауэровское исследования валентного состояния ионов переходных металлов в керамиках {Co}$_{\\textrm{1-x}}${Fe}$_{\\textrm{x}}${Cr}$_{\\textrm{2}}${O4} (x=0.1,0.2, 0.5)},\n\tvolume = {58},\n\turl = {http://journals.ioffe.ru/articles/42621},\n\tabstract = {Валентное состояние ионов переходных металлов в системе Сo1-xFexCr2O4 (x = 0.1, 0.2, 0.5) изучено с помощью рентгеновской фотоэлектронной и мессбауэровской спектроскопии. Показано присутствие в этой системе ионов Fe2+ и Fe3+. Относительные содержания Fe3+/Fe2+ определены путем подгонки экспериментальных Fe2p-спектров суперпозицией теоретических спектров Fe2+ и Fe3+, а также методом мессбауэровской спектроскопии. Работа выполнена при частичной поддержке Минобрнауки РФ проект 1880 и в рамках проектной части государственного задания Департамента науки и технологий Минобрнауки России N 3.1137.2014К, а также соглашения N 14.607.21.0110 от 27.11.2014 г., уникальный идентификатор соглашения RFMEFI60714X0110.},\n\tlanguage = {ru},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Кочур, А. Г. and Гуглев, К. А. and Козаков, А. Т. and Кубрин, С. П. and Никольский, А. В. and Торгашев, В. И.},\n\tmonth = dec,\n\tyear = {2015},\n\tpages = {108--113},\n\tfile = {Физика твердого тела:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\39KQTSIS\\\\42621.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Валентное состояние ионов переходных металлов в системе Сo1-xFexCr2O4 (x = 0.1, 0.2, 0.5) изучено с помощью рентгеновской фотоэлектронной и мессбауэровской спектроскопии. Показано присутствие в этой системе ионов Fe2+ и Fe3+. Относительные содержания Fe3+/Fe2+ определены путем подгонки экспериментальных Fe2p-спектров суперпозицией теоретических спектров Fe2+ и Fe3+, а также методом мессбауэровской спектроскопии. Работа выполнена при частичной поддержке Минобрнауки РФ проект 1880 и в рамках проектной части государственного задания Департамента науки и технологий Минобрнауки России N 3.1137.2014К, а также соглашения N 14.607.21.0110 от 27.11.2014 г., уникальный идентификатор соглашения RFMEFI60714X0110.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/42648\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------2015', 'http://journals.ioffe.ru/articles/42648', event);\">\n    Влияние механизмов роста на деформацию элементарной ячейки и переключение поляризации в гетероструктурах титаната бария-стронция на оксиде магния.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Мухортов, В. М.; Головко, Ю. И.; Бирюков, С. В.; Анохин, А. С.;  and Юзюк, Ю. И.\n</span>\n\n  \n\n</span>\n\n  <i>Журнал технической физики</i>, 86(1): 93–98. December 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/42648\"\n     onclick=\"log_download('------2015', 'http://journals.ioffe.ru/articles/42648', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Влияние механизмов роста на деформацию элементарной ячейки и переключение поляризации в гетероструктурах титаната бария-стронция на оксиде магния [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2015-1,\n\ttitle = {Влияние механизмов роста на деформацию элементарной ячейки и переключение поляризации в гетероструктурах титаната бария-стронция на оксиде магния},\n\tvolume = {86},\n\turl = {http://journals.ioffe.ru/articles/42648},\n\tabstract = {Исследованы влияние механизмов роста на деформацию ячейки и связанное с этим изменение свойств монокристаллических пленок Ba0.8Sr0.2TiO3, выращенных на подложках MgO по механизмам роста Франка-Ван дер Мерве и Вольмера-Вебера. Показано, что деформация ячейки существенно зависит от толщины пленки и в значительной мере определяется механизмами роста. Установлено, что в рамках одной пары пленка-подложка можно варьировать напряжения в пленке от двумерно-растягивающих до сжимающих за счет изменения механизмов роста и толщины пленки.},\n\tlanguage = {ru},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Журнал технической физики},\n\tauthor = {Мухортов, В. М. and Головко, Ю. И. and Бирюков, С. В. and Анохин, А. С. and Юзюк, Ю. И.},\n\tmonth = dec,\n\tyear = {2015},\n\tpages = {93--98},\n\tfile = {Журнал технической физики:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\RVFMF3E9\\\\42648.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследованы влияние механизмов роста на деформацию ячейки и связанное с этим изменение свойств монокристаллических пленок Ba0.8Sr0.2TiO3, выращенных на подложках MgO по механизмам роста Франка-Ван дер Мерве и Вольмера-Вебера. Показано, что деформация ячейки существенно зависит от толщины пленки и в значительной мере определяется механизмами роста. Установлено, что в рамках одной пары пленка-подложка можно варьировать напряжения в пленке от двумерно-растягивающих до сжимающих за счет изменения механизмов роста и толщины пленки.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kochur-kozakov-googlev-kubrin-nikolskii-torgashev-bush-shkuratov-etal-valencestateoftransitionmetalionsincotextrm1xfetextrmxcrtextrm2otextrm4x010205ceramicsfromxrayphotoelectronandmssbauerspectroscopydata-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0925838815005903\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kochur-kozakov-googlev-kubrin-nikolskii-torgashev-bush-shkuratov-etal-valencestateoftransitionmetalionsincotextrm1xfetextrmxcrtextrm2otextrm4x010205ceramicsfromxrayphotoelectronandmssbauerspectroscopydata-2015', 'https://www.sciencedirect.com/science/article/pii/S0925838815005903', event);\">\n    Valence state of transition metal ions in Co$_{\\textrm{1−x}}$Fe$_{\\textrm{x}}$Cr$_{\\textrm{2}}$O$_{\\textrm{4}}$ (x=0.1, 0.2, 0.5) ceramics from X-ray photoelectron and Mössbauer spectroscopy data.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kochur, A. G.; Kozakov, A. T.; Googlev, K. A.; Kubrin, S. P.; Nikolskii, A. V.; Torgashev, V. I.; Bush, A. A.; Shkuratov, V. Y.;  and Shevtsova, S. I.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Alloys and Compounds</i>, 636: 241–248. July 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0925838815005903\"\n     onclick=\"log_download('kochur-kozakov-googlev-kubrin-nikolskii-torgashev-bush-shkuratov-etal-valencestateoftransitionmetalionsincotextrm1xfetextrmxcrtextrm2otextrm4x010205ceramicsfromxrayphotoelectronandmssbauerspectroscopydata-2015', 'https://www.sciencedirect.com/science/article/pii/S0925838815005903', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Valence state of transition metal ions in Co$_{\\textrm{1−x}}$Fe$_{\\textrm{x}}$Cr$_{\\textrm{2}}$O$_{\\textrm{4}}$ (x=0.1, 0.2, 0.5) ceramics from X-ray photoelectron and Mössbauer spectroscopy data [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.jallcom.2015.02.150\"\n     onclick=\"log_download('kochur-kozakov-googlev-kubrin-nikolskii-torgashev-bush-shkuratov-etal-valencestateoftransitionmetalionsincotextrm1xfetextrmxcrtextrm2otextrm4x010205ceramicsfromxrayphotoelectronandmssbauerspectroscopydata-2015', 'http://doi.org/10.1016/j.jallcom.2015.02.150', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kochur-kozakov-googlev-kubrin-nikolskii-torgashev-bush-shkuratov-etal-valencestateoftransitionmetalionsincotextrm1xfetextrmxcrtextrm2otextrm4x010205ceramicsfromxrayphotoelectronandmssbauerspectroscopydata-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kochur-kozakov-googlev-kubrin-nikolskii-torgashev-bush-shkuratov-etal-valencestateoftransitionmetalionsincotextrm1xfetextrmxcrtextrm2otextrm4x010205ceramicsfromxrayphotoelectronandmssbauerspectroscopydata-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kochur_valence_2015,\n\ttitle = {Valence state of transition metal ions in {Co}$_{\\textrm{1−x}}${Fe}$_{\\textrm{x}}${Cr}$_{\\textrm{2}}${O}$_{\\textrm{4}}$ (x=0.1, 0.2, 0.5) ceramics from {X}-ray photoelectron and {Mössbauer} spectroscopy data},\n\tvolume = {636},\n\tissn = {0925-8388},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0925838815005903},\n\tdoi = {10.1016/j.jallcom.2015.02.150},\n\tabstract = {Ceramics with nominal composition Co1−xFexCr2O4 (x=0.1, 0.2, 0.5) are synthesized via a solid state reaction method. Crystal structure of samples is studied with X-ray diffraction. Actual elemental composition is determined using X-ray microanalysis and X-ray photoelectron spectroscopy (XPS). Samples’ morphology is studied with scanning electron microscopy. Valence state of the Co, Fe and Cr ions is determined from 2p X-ray photoelectron spectra and Mössbauer spectra. XPS are assigned based on calculations with allowance for the multiplet splitting, crystal field, and the charge-transfer effects. Cobalt ions are found to be bivalent in tetrahedral coordination; chromium ions are trivalent in octahedral coordination. Fe ions are mostly in trivalent states, although Fe2+ ions are also present in significant amounts. Fe2+ ions are in tetrahedral coordination while Fe3+ ions occupy both tetrahedral and octahedral sites. Bulk and near-surface elemental compositions of the ceramic grains are noticeably different. Relative Fe3+/Fe2+ contents are the same in the volume and at the surface of the samples; relative number of Fe3+ ions increases upon the increase of x. A model of partly inverse spinel structure is suggested where the atoms of iron substitute both Co and Cr atoms.},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Alloys and Compounds},\n\tauthor = {Kochur, A. G. and Kozakov, A. T. and Googlev, K. A. and Kubrin, S. P. and Nikolskii, A. V. and Torgashev, V. I. and Bush, A. A. and Shkuratov, V. Ya. and Shevtsova, S. I.},\n\tmonth = jul,\n\tyear = {2015},\n\tkeywords = {X-ray diffraction, XPS, CoFeCrO ceramics, Ions valence state, Mössbauer spectroscopy, X-ray microanalysis},\n\tpages = {241--248},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Ceramics with nominal composition Co1−xFexCr2O4 (x=0.1, 0.2, 0.5) are synthesized via a solid state reaction method. Crystal structure of samples is studied with X-ray diffraction. Actual elemental composition is determined using X-ray microanalysis and X-ray photoelectron spectroscopy (XPS). Samples’ morphology is studied with scanning electron microscopy. Valence state of the Co, Fe and Cr ions is determined from 2p X-ray photoelectron spectra and Mössbauer spectra. XPS are assigned based on calculations with allowance for the multiplet splitting, crystal field, and the charge-transfer effects. Cobalt ions are found to be bivalent in tetrahedral coordination; chromium ions are trivalent in octahedral coordination. Fe ions are mostly in trivalent states, although Fe2+ ions are also present in significant amounts. Fe2+ ions are in tetrahedral coordination while Fe3+ ions occupy both tetrahedral and octahedral sites. Bulk and near-surface elemental compositions of the ceramic grains are noticeably different. Relative Fe3+/Fe2+ contents are the same in the volume and at the surface of the samples; relative number of Fe3+ ions increases upon the increase of x. A model of partly inverse spinel structure is suggested where the atoms of iron substitute both Co and Cr atoms.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kozakov-kochur-googlev-nikolskii-torgashev-trotsenko-bush-valencestateofmanganeseandironionsinlatextrm1xatextrmxmnotextrm3acasrandbitextrm1xsrtextrmxfeotextrm3systemsfrommn2pmn3sfe2pandfe3sxrayphotoelectronspectraeffectofdelocalizationonfe3sspectrasplitting-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0925838815302772\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kozakov-kochur-googlev-nikolskii-torgashev-trotsenko-bush-valencestateofmanganeseandironionsinlatextrm1xatextrmxmnotextrm3acasrandbitextrm1xsrtextrmxfeotextrm3systemsfrommn2pmn3sfe2pandfe3sxrayphotoelectronspectraeffectofdelocalizationonfe3sspectrasplitting-2015', 'https://www.sciencedirect.com/science/article/pii/S0925838815302772', event);\">\n    Valence state of manganese and iron ions in La$_{\\textrm{1−x}}$A$_{\\textrm{x}}$MnO$_{\\textrm{3}}$ (A = Ca, Sr) and Bi$_{\\textrm{1−x}}$Sr$_{\\textrm{x}}$FeO$_{\\textrm{3}}$ systems from Mn2p, Mn3s, Fe2p and Fe3s X-ray photoelectron spectra. Effect of delocalization on Fe3s spectra splitting.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kozakov, A. T.; Kochur, A. G.; Googlev, K. A.; Nikolskii, A. V.; Torgashev, V. I.; Trotsenko, V. G.;  and Bush, A. A.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Alloys and Compounds</i>, 647: 947–955. October 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0925838815302772\"\n     onclick=\"log_download('kozakov-kochur-googlev-nikolskii-torgashev-trotsenko-bush-valencestateofmanganeseandironionsinlatextrm1xatextrmxmnotextrm3acasrandbitextrm1xsrtextrmxfeotextrm3systemsfrommn2pmn3sfe2pandfe3sxrayphotoelectronspectraeffectofdelocalizationonfe3sspectrasplitting-2015', 'https://www.sciencedirect.com/science/article/pii/S0925838815302772', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Valence state of manganese and iron ions in La$_{\\textrm{1−x}}$A$_{\\textrm{x}}$MnO$_{\\textrm{3}}$ (A = Ca, Sr) and Bi$_{\\textrm{1−x}}$Sr$_{\\textrm{x}}$FeO$_{\\textrm{3}}$ systems from Mn2p, Mn3s, Fe2p and Fe3s X-ray photoelectron spectra. Effect of delocalization on Fe3s spectra splitting [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.jallcom.2015.06.161\"\n     onclick=\"log_download('kozakov-kochur-googlev-nikolskii-torgashev-trotsenko-bush-valencestateofmanganeseandironionsinlatextrm1xatextrmxmnotextrm3acasrandbitextrm1xsrtextrmxfeotextrm3systemsfrommn2pmn3sfe2pandfe3sxrayphotoelectronspectraeffectofdelocalizationonfe3sspectrasplitting-2015', 'http://doi.org/10.1016/j.jallcom.2015.06.161', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kozakov-kochur-googlev-nikolskii-torgashev-trotsenko-bush-valencestateofmanganeseandironionsinlatextrm1xatextrmxmnotextrm3acasrandbitextrm1xsrtextrmxfeotextrm3systemsfrommn2pmn3sfe2pandfe3sxrayphotoelectronspectraeffectofdelocalizationonfe3sspectrasplitting-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kozakov-kochur-googlev-nikolskii-torgashev-trotsenko-bush-valencestateofmanganeseandironionsinlatextrm1xatextrmxmnotextrm3acasrandbitextrm1xsrtextrmxfeotextrm3systemsfrommn2pmn3sfe2pandfe3sxrayphotoelectronspectraeffectofdelocalizationonfe3sspectrasplitting-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kozakov_valence_2015,\n\ttitle = {Valence state of manganese and iron ions in {La}$_{\\textrm{1−x}}${A}$_{\\textrm{x}}${MnO}$_{\\textrm{3}}$ ({A} = {Ca}, {Sr}) and {Bi}$_{\\textrm{1−x}}${Sr}$_{\\textrm{x}}${FeO}$_{\\textrm{3}}$ systems from {Mn2p}, {Mn3s}, {Fe2p} and {Fe3s} {X}-ray photoelectron spectra. {Effect} of delocalization on {Fe3s} spectra splitting},\n\tvolume = {647},\n\tissn = {0925-8388},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0925838815302772},\n\tdoi = {10.1016/j.jallcom.2015.06.161},\n\tabstract = {La1−xCaxMnO3 (x = 0.5, 0.7, 0.85, 0.95) ceramic samples are synthesized by solid state reaction method. Mn3s and Mn2p X-ray photoelectron spectra (XPS) of La1−xCaxMnO3, and Fe3s-spectra of Bi1−xSrxFeO3 (0 ≤ x ≤ 1) are measured at room temperature. Both Mn3+ and Mn4+ ions are discovered in La1−xCaxMnO3 similarly to the case of Fe3+ and Fe4+ found earlier in Bi1−xSrxFeO3 ceramics. Relative Mn3+/Mn4+ contents are determined by fitting measured Mn2p spectra with combinations of Mn2p spectra of compounds containing tri- and quadrivalent Mn ions. Relative portion of Mn4+ is shown to increase with the increase of x. Fe3s spectrum splitting in Bi1−xSrxFeO3 increases with x in contrast to the Mn3s-spectrum splitting in La1−xCaxMnO3 and La1−xSrxMnO3. Anomalous behavior of Fe3s splitting is explained in the frame of the model of partly itinerant 3d-electrons by strong effect of 3d electron delocalization on electron correlation interaction in final state of 3s photoabsorption.},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Alloys and Compounds},\n\tauthor = {Kozakov, A. T. and Kochur, A. G. and Googlev, K. A. and Nikolskii, A. V. and Torgashev, V. I. and Trotsenko, V. G. and Bush, A. A.},\n\tmonth = oct,\n\tyear = {2015},\n\tkeywords = {XPS, BiSrFeO, Delocalization, Electron correlation, Fe3s, Itinerant 3d electrons, LaAMnO (A = Ca,Sr), Mn2p, Mn3s},\n\tpages = {947--955},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  La1−xCaxMnO3 (x = 0.5, 0.7, 0.85, 0.95) ceramic samples are synthesized by solid state reaction method. Mn3s and Mn2p X-ray photoelectron spectra (XPS) of La1−xCaxMnO3, and Fe3s-spectra of Bi1−xSrxFeO3 (0 ≤ x ≤ 1) are measured at room temperature. Both Mn3+ and Mn4+ ions are discovered in La1−xCaxMnO3 similarly to the case of Fe3+ and Fe4+ found earlier in Bi1−xSrxFeO3 ceramics. Relative Mn3+/Mn4+ contents are determined by fitting measured Mn2p spectra with combinations of Mn2p spectra of compounds containing tri- and quadrivalent Mn ions. Relative portion of Mn4+ is shown to increase with the increase of x. Fe3s spectrum splitting in Bi1−xSrxFeO3 increases with x in contrast to the Mn3s-spectrum splitting in La1−xCaxMnO3 and La1−xSrxMnO3. Anomalous behavior of Fe3s splitting is explained in the frame of the model of partly itinerant 3d-electrons by strong effect of 3d electron delocalization on electron correlation interaction in final state of 3s photoabsorption.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"mikheykin-torgashev-yuzyuk-bush-talanov-cervellino-dmitriev-thecooperativejahntellereffectandantiisostructuralphasesinnitextrm1xcotextrmxcrtextrm2otextrm4solidsolutionssynchrotronxraydiffractionstudy-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0022369715001651\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'mikheykin-torgashev-yuzyuk-bush-talanov-cervellino-dmitriev-thecooperativejahntellereffectandantiisostructuralphasesinnitextrm1xcotextrmxcrtextrm2otextrm4solidsolutionssynchrotronxraydiffractionstudy-2015', 'https://www.sciencedirect.com/science/article/pii/S0022369715001651', event);\">\n    The cooperative Jahn–Teller effect and anti-isostructural phases in Ni$_{\\textrm{1−x}}$Co$_{\\textrm{x}}$Cr$_{\\textrm{2}}$O$_{\\textrm{4}}$ solid solutions: Synchrotron X-ray diffraction study.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Mikheykin, A. S.; Torgashev, V. I.; Yuzyuk, Y. I.; Bush, A. A.; Talanov, V. M.; Cervellino, A.;  and Dmitriev, V. P.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics and Chemistry of Solids</i>, 86: 42–48. November 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0022369715001651\"\n     onclick=\"log_download('mikheykin-torgashev-yuzyuk-bush-talanov-cervellino-dmitriev-thecooperativejahntellereffectandantiisostructuralphasesinnitextrm1xcotextrmxcrtextrm2otextrm4solidsolutionssynchrotronxraydiffractionstudy-2015', 'https://www.sciencedirect.com/science/article/pii/S0022369715001651', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"The cooperative Jahn–Teller effect and anti-isostructural phases in Ni$_{\\textrm{1−x}}$Co$_{\\textrm{x}}$Cr$_{\\textrm{2}}$O$_{\\textrm{4}}$ solid solutions: Synchrotron X-ray diffraction study [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.jpcs.2015.06.015\"\n     onclick=\"log_download('mikheykin-torgashev-yuzyuk-bush-talanov-cervellino-dmitriev-thecooperativejahntellereffectandantiisostructuralphasesinnitextrm1xcotextrmxcrtextrm2otextrm4solidsolutionssynchrotronxraydiffractionstudy-2015', 'http://doi.org/10.1016/j.jpcs.2015.06.015', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/mikheykin-torgashev-yuzyuk-bush-talanov-cervellino-dmitriev-thecooperativejahntellereffectandantiisostructuralphasesinnitextrm1xcotextrmxcrtextrm2otextrm4solidsolutionssynchrotronxraydiffractionstudy-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('mikheykin-torgashev-yuzyuk-bush-talanov-cervellino-dmitriev-thecooperativejahntellereffectandantiisostructuralphasesinnitextrm1xcotextrmxcrtextrm2otextrm4solidsolutionssynchrotronxraydiffractionstudy-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{mikheykin_cooperative_2015,\n\ttitle = {The cooperative {Jahn}–{Teller} effect and anti-isostructural phases in {Ni}$_{\\textrm{1−x}}${Co}$_{\\textrm{x}}${Cr}$_{\\textrm{2}}${O}$_{\\textrm{4}}$ solid solutions: {Synchrotron} {X}-ray diffraction study},\n\tvolume = {86},\n\tissn = {0022-3697},\n\tshorttitle = {The cooperative {Jahn}–{Teller} effect and anti-isostructural phases in {Ni1}−{xCoxCr2O4} solid solutions},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0022369715001651},\n\tdoi = {10.1016/j.jpcs.2015.06.015},\n\tabstract = {A low-temperature high-resolution powder diffraction study has been carried out on a system of Ni1−xCoxCr2O4 solid solutions with x≤0.1 down to 5K. The tetragonal phase (I41/amd) with c/a{\\textless}1 was experimentally observed in Ni0.9Co0.1Cr2O4 below ∼64K. The new phase is anti-isostructural to the well-known tetragonal phase of NiCr2O4. A unified phenomenological model has been applied to structural phase transitions in Ni1−xCoxCr2O4 solid solutions. It shows that the appearing of such a phase is justified from a structural point of view. Analysis of atomic displacements confirms predictions of the symmetry-based model-free consideration.},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics and Chemistry of Solids},\n\tauthor = {Mikheykin, A. S. and Torgashev, V. I. and Yuzyuk, Yu. I. and Bush, A. A. and Talanov, V. M. and Cervellino, A. and Dmitriev, V. P.},\n\tmonth = nov,\n\tyear = {2015},\n\tkeywords = {A. Ceramics, C. X-ray diffraction, D. Crystal field, D. Crystal structure, D. Phase transitions},\n\tpages = {42--48},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A low-temperature high-resolution powder diffraction study has been carried out on a system of Ni1−xCoxCr2O4 solid solutions with x≤0.1 down to 5K. The tetragonal phase (I41/amd) with c/a\\textless1 was experimentally observed in Ni0.9Co0.1Cr2O4 below ∼64K. The new phase is anti-isostructural to the well-known tetragonal phase of NiCr2O4. A unified phenomenological model has been applied to structural phase transitions in Ni1−xCoxCr2O4 solid solutions. It shows that the appearing of such a phase is justified from a structural point of view. Analysis of atomic displacements confirms predictions of the symmetry-based model-free consideration.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kadyrov-zhukova-torgashev-gorshunov-prokhorov-motovilova-fischgrabe-moshnyaga-etal-terahertzinfraredspectroscopyofoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0921452614009041\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kadyrov-zhukova-torgashev-gorshunov-prokhorov-motovilova-fischgrabe-moshnyaga-etal-terahertzinfraredspectroscopyofoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2015', 'https://www.sciencedirect.com/science/article/pii/S0921452614009041', event);\">\n    Terahertz-infrared spectroscopy of overdoped manganites La$_{\\textrm{1−x}}$Ca$_{\\textrm{x}}$MnO$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kadyrov, L. S.; Zhukova, E. S.; Torgashev, V. I.; Gorshunov, B. P.; Prokhorov, A. S.; Motovilova, E. A.; Fischgrabe, F.; Moshnyaga, V.; Zhang, T.; Kremer, R.; Pracht, U.; Zapf, S.; Pokorný, J.; Untereiner, G.; Kamba, S.;  and Dressel, M.\n</span>\n\n  \n\n</span>\n\n  <i>Physica B: Condensed Matter</i>, 460: 199–201. March 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0921452614009041\"\n     onclick=\"log_download('kadyrov-zhukova-torgashev-gorshunov-prokhorov-motovilova-fischgrabe-moshnyaga-etal-terahertzinfraredspectroscopyofoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2015', 'https://www.sciencedirect.com/science/article/pii/S0921452614009041', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Terahertz-infrared spectroscopy of overdoped manganites La$_{\\textrm{1−x}}$Ca$_{\\textrm{x}}$MnO$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.physb.2014.11.070\"\n     onclick=\"log_download('kadyrov-zhukova-torgashev-gorshunov-prokhorov-motovilova-fischgrabe-moshnyaga-etal-terahertzinfraredspectroscopyofoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2015', 'http://doi.org/10.1016/j.physb.2014.11.070', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kadyrov-zhukova-torgashev-gorshunov-prokhorov-motovilova-fischgrabe-moshnyaga-etal-terahertzinfraredspectroscopyofoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kadyrov-zhukova-torgashev-gorshunov-prokhorov-motovilova-fischgrabe-moshnyaga-etal-terahertzinfraredspectroscopyofoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kadyrov_terahertz-infrared_2015,\n\tseries = {Special {Issue} on {Electronic} {Crystals} ({ECRYS}-2014)},\n\ttitle = {Terahertz-infrared spectroscopy of overdoped manganites {La}$_{\\textrm{1−x}}${Ca}$_{\\textrm{x}}${MnO}$_{\\textrm{3}}$},\n\tvolume = {460},\n\tissn = {0921-4526},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0921452614009041},\n\tdoi = {10.1016/j.physb.2014.11.070},\n\tabstract = {Terahertz and infrared spectra of dielectric permittivity and optical conductivity of overdoped manganites La1−xCaxMnO3 (0.5≤x≤1) have been measured at frequencies ν from 4cm−1 to 700cm−1 and at temperatures T from 5K to 300K. The samples were prepared in the form of bulk polycrystals (ceramics) and epitaxial films (free-standing and on MgO substrates). Strongly asymmetric absorption bands have been found in the compounds which are in charge-ordered state (0.5{\\textless}x{\\textless}0.85) and have commensurate calcium doping. The bands are located close to the position of lowest energy van Hove singularity of the folded Brillouin zone. The bands are associated with a boson peak, i.e., with the excess of lattice acoustical vibrational states over the standard Debye contribution ({\\textasciitilde}ν2). In addition, Raman scattering measurements on ceramic samples have been conducted, which confirmed our assignment of the bands’ origin. We firmly identify contribution to the low energy spectra due to quasi-free charge carriers. In the paramagnetic phase all samples show a Drude-like response corresponding to the band type of charge transport. At low temperatures, for the range of dopings 0.5≤x{\\textless}0.85, the conductivity spectra show signatures of variable-range hopping mechanisms of transport.},\n\turldate = {2023-11-11},\n\tjournal = {Physica B: Condensed Matter},\n\tauthor = {Kadyrov, Lenar S. and Zhukova, Elena S. and Torgashev, Victor I. and Gorshunov, Boris P. and Prokhorov, Anatoly S. and Motovilova, Elizaveta A. and Fischgrabe, Florian and Moshnyaga, Vasily and Zhang, Tao and Kremer, Reinhard and Pracht, Uwe and Zapf, Sina and Pokorný, Jan and Untereiner, Gabriele and Kamba, Stanislav and Dressel, Martin},\n\tmonth = mar,\n\tyear = {2015},\n\tkeywords = {Raman spectroscopy, Manganites, Terahertz spectroscopy},\n\tpages = {199--201},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Terahertz and infrared spectra of dielectric permittivity and optical conductivity of overdoped manganites La1−xCaxMnO3 (0.5≤x≤1) have been measured at frequencies ν from 4cm−1 to 700cm−1 and at temperatures T from 5K to 300K. The samples were prepared in the form of bulk polycrystals (ceramics) and epitaxial films (free-standing and on MgO substrates). Strongly asymmetric absorption bands have been found in the compounds which are in charge-ordered state (0.5\\textlessx\\textless0.85) and have commensurate calcium doping. The bands are located close to the position of lowest energy van Hove singularity of the folded Brillouin zone. The bands are associated with a boson peak, i.e., with the excess of lattice acoustical vibrational states over the standard Debye contribution (~ν2). In addition, Raman scattering measurements on ceramic samples have been conducted, which confirmed our assignment of the bands’ origin. We firmly identify contribution to the low energy spectra due to quasi-free charge carriers. In the paramagnetic phase all samples show a Drude-like response corresponding to the band type of charge transport. At low temperatures, for the range of dopings 0.5≤x\\textless0.85, the conductivity spectra show signatures of variable-range hopping mechanisms of transport.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-shakhovoy-razumnaya-yuzyuk-phenomenologicaltheoryofphasetransitionsinepitaxialbatextrmxsrtextrm1xtiotextrm3thinfilmson111orientedcubicsubstrates-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.4926788\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-shakhovoy-razumnaya-yuzyuk-phenomenologicaltheoryofphasetransitionsinepitaxialbatextrmxsrtextrm1xtiotextrm3thinfilmson111orientedcubicsubstrates-2015', 'https://doi.org/10.1063/1.4926788', event);\">\n    Phenomenological theory of phase transitions in epitaxial Ba$_{\\textrm{x}}$Sr$_{\\textrm{1−x}}$TiO$_{\\textrm{3}}$ thin films on (111)-oriented cubic substrates.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.; Shakhovoy, R. A.; Razumnaya, A. G.;  and Yuzyuk, Y. I.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Applied Physics</i>, 118(2): 024101. July 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.4926788\"\n     onclick=\"log_download('shirokov-shakhovoy-razumnaya-yuzyuk-phenomenologicaltheoryofphasetransitionsinepitaxialbatextrmxsrtextrm1xtiotextrm3thinfilmson111orientedcubicsubstrates-2015', 'https://doi.org/10.1063/1.4926788', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Phenomenological theory of phase transitions in epitaxial Ba$_{\\textrm{x}}$Sr$_{\\textrm{1−x}}$TiO$_{\\textrm{3}}$ thin films on (111)-oriented cubic substrates [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.4926788\"\n     onclick=\"log_download('shirokov-shakhovoy-razumnaya-yuzyuk-phenomenologicaltheoryofphasetransitionsinepitaxialbatextrmxsrtextrm1xtiotextrm3thinfilmson111orientedcubicsubstrates-2015', 'http://doi.org/10.1063/1.4926788', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-shakhovoy-razumnaya-yuzyuk-phenomenologicaltheoryofphasetransitionsinepitaxialbatextrmxsrtextrm1xtiotextrm3thinfilmson111orientedcubicsubstrates-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-shakhovoy-razumnaya-yuzyuk-phenomenologicaltheoryofphasetransitionsinepitaxialbatextrmxsrtextrm1xtiotextrm3thinfilmson111orientedcubicsubstrates-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_phenomenological_2015,\n\ttitle = {Phenomenological theory of phase transitions in epitaxial {Ba}$_{\\textrm{x}}${Sr}$_{\\textrm{1−x}}${TiO}$_{\\textrm{3}}$ thin films on (111)-oriented cubic substrates},\n\tvolume = {118},\n\tissn = {0021-8979},\n\turl = {https://doi.org/10.1063/1.4926788},\n\tdoi = {10.1063/1.4926788},\n\tabstract = {A phenomenological thermodynamic theory of BaxSr1−xTiO3 (BST-x) thin films epitaxially grown on (111)-oriented cubic substrates is developed using the Landau-Devonshire approach. The group-theoretical analysis of the low-symmetry phases was performed taking into account two order parameters: the polarization related to ionic shifts in polar zone-center F1u mode and the out-of-phase rotation of TiO6 octahedra corresponding to the R25 zone-boundary mode in the parent cubic phase Pm3¯m. The eight-order thermodynamic potential for BST-x solid solutions was developed and analyzed. We constructed the “concentration-misfit strain” phase diagram for BST-x thin films at room temperature and found that polar rhombohedral R3m phase with the polarization normal to the substrate is stable for x \\&amp;gt; 0.72 and negative misfit strains, while ferroelectric monoclinic C2 and Cm phases with in-plane polarization are stable for much smaller x and positive or slightly negative misfit strains. We constructed the “temperature-misfit strain” phase diagrams for several concentrations (x = 1, 0.8, 0.6, 0.4, and 0.2). Systematic changes of the phase transition lines between the paraelectric and ferroelectric phases are discussed. The phase diagrams are useful for practical applications in thin-film engineering.},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Applied Physics},\n\tauthor = {Shirokov, V. B. and Shakhovoy, R. A. and Razumnaya, A. G. and Yuzyuk, Yu. I.},\n\tmonth = jul,\n\tyear = {2015},\n\tpages = {024101},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A phenomenological thermodynamic theory of BaxSr1−xTiO3 (BST-x) thin films epitaxially grown on (111)-oriented cubic substrates is developed using the Landau-Devonshire approach. The group-theoretical analysis of the low-symmetry phases was performed taking into account two order parameters: the polarization related to ionic shifts in polar zone-center F1u mode and the out-of-phase rotation of TiO6 octahedra corresponding to the R25 zone-boundary mode in the parent cubic phase Pm3¯m. The eight-order thermodynamic potential for BST-x solid solutions was developed and analyzed. We constructed the “concentration-misfit strain” phase diagram for BST-x thin films at room temperature and found that polar rhombohedral R3m phase with the polarization normal to the substrate is stable for x &gt; 0.72 and negative misfit strains, while ferroelectric monoclinic C2 and Cm phases with in-plane polarization are stable for much smaller x and positive or slightly negative misfit strains. We constructed the “temperature-misfit strain” phase diagrams for several concentrations (x = 1, 0.8, 0.6, 0.4, and 0.2). Systematic changes of the phase transition lines between the paraelectric and ferroelectric phases are discussed. The phase diagrams are useful for practical applications in thin-film engineering.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"rudskaya-kofanova-kupriyanov-insitustudiesoflamnotextrm3phasesformationwhenusedofdifferentprecursors-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.semanticscholar.org/paper/In-Situ-Studies-of-LaMnO-3-Phases-Formation-When-of-Rudskaya-Kofanova/3b5d3dfeb83398cd0265cf3d59a70448d257bdf0\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'rudskaya-kofanova-kupriyanov-insitustudiesoflamnotextrm3phasesformationwhenusedofdifferentprecursors-2015', 'https://www.semanticscholar.org/paper/In-Situ-Studies-of-LaMnO-3-Phases-Formation-When-of-Rudskaya-Kofanova/3b5d3dfeb83398cd0265cf3d59a70448d257bdf0', event);\">\n    In Situ Studies of LaMnO$_{\\textrm{3}}$ Phases Formation When used of Different Precursors.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Rudskaya, A.; Kofanova, N. B.;  and Kupriyanov, M.\n</span>\n\n  \n\n</span>\n\n  <i>International Journal of Advanced Research in Chemical Science</i>.  2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.semanticscholar.org/paper/In-Situ-Studies-of-LaMnO-3-Phases-Formation-When-of-Rudskaya-Kofanova/3b5d3dfeb83398cd0265cf3d59a70448d257bdf0\"\n     onclick=\"log_download('rudskaya-kofanova-kupriyanov-insitustudiesoflamnotextrm3phasesformationwhenusedofdifferentprecursors-2015', 'https://www.semanticscholar.org/paper/In-Situ-Studies-of-LaMnO-3-Phases-Formation-When-of-Rudskaya-Kofanova/3b5d3dfeb83398cd0265cf3d59a70448d257bdf0', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"In Situ Studies of LaMnO$_{\\textrm{3}}$ Phases Formation When used of Different Precursors [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/rudskaya-kofanova-kupriyanov-insitustudiesoflamnotextrm3phasesformationwhenusedofdifferentprecursors-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('rudskaya-kofanova-kupriyanov-insitustudiesoflamnotextrm3phasesformationwhenusedofdifferentprecursors-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{rudskaya_situ_2015,\n\ttitle = {In {Situ} {Studies} of {LaMnO}$_{\\textrm{3}}$ {Phases} {Formation} {When} used of {Different} {Precursors}},\n\turl = {https://www.semanticscholar.org/paper/In-Situ-Studies-of-LaMnO-3-Phases-Formation-When-of-Rudskaya-Kofanova/3b5d3dfeb83398cd0265cf3d59a70448d257bdf0},\n\tabstract = {LaMnO3 specimens were synthesized with using of different precursors on X-ray diffractometer (method in situ). It was established that the cubic nanoand microcrystalline perovskite phases starts to form in the temperature range 400 – 600 °C. Synthesized LaMnO3 specimens at room temperature have stoichiometric and nonstoichiometric perovskite-type phases of different symmetry: Pnma (solid state synthesis) and R 3 c (wet methods of precursors’ preparation – sorption, co-precipitation and sol-gel)},\n\turldate = {2023-11-11},\n\tjournal = {International Journal of Advanced Research in Chemical Science},\n\tauthor = {Rudskaya, A. and Kofanova, N. B. and Kupriyanov, M.},\n\tyear = {2015},\n\tfile = {Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\FT2R3G3W\\\\Rudskaya и др. - 2015 - In Situ Studies of LaMnO 3 Phases Formation When u.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  LaMnO3 specimens were synthesized with using of different precursors on X-ray diffractometer (method in situ). It was established that the cubic nanoand microcrystalline perovskite phases starts to form in the temperature range 400 – 600 °C. Synthesized LaMnO3 specimens at room temperature have stoichiometric and nonstoichiometric perovskite-type phases of different symmetry: Pnma (solid state synthesis) and R 3 c (wet methods of precursors’ preparation – sorption, co-precipitation and sol-gel)\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kozakov-kochur-googlev-nikolskii-torgashev-shevcova-finestructureofthexrayphotoelectronni2textrmpspectruminnitextrm1xcotextrmxcrtextrm2otextrm4compounds-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.3103/S106287381511012X\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kozakov-kochur-googlev-nikolskii-torgashev-shevcova-finestructureofthexrayphotoelectronni2textrmpspectruminnitextrm1xcotextrmxcrtextrm2otextrm4compounds-2015', 'https://doi.org/10.3103/S106287381511012X', event);\">\n    Fine structure of the X-ray photoelectron Ni 2$_{\\textrm{p}}$ spectrum in Ni$_{\\textrm{1–x}}$Co$_{\\textrm{x}}$Cr$_{\\textrm{2}}$O$_{\\textrm{4}}$ compounds.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kozakov, A. T.; Kochur, A. G.; Googlev, K. A.; Nikolskii, A. V.; Torgashev, V. I.;  and Shevcova, S. I.\n</span>\n\n  \n\n</span>\n\n  <i>Bulletin of the Russian Academy of Sciences: Physics</i>, 79(11): 1371–1375. November 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.3103/S106287381511012X\"\n     onclick=\"log_download('kozakov-kochur-googlev-nikolskii-torgashev-shevcova-finestructureofthexrayphotoelectronni2textrmpspectruminnitextrm1xcotextrmxcrtextrm2otextrm4compounds-2015', 'https://doi.org/10.3103/S106287381511012X', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Fine structure of the X-ray photoelectron Ni 2$_{\\textrm{p}}$ spectrum in Ni$_{\\textrm{1–x}}$Co$_{\\textrm{x}}$Cr$_{\\textrm{2}}$O$_{\\textrm{4}}$ compounds [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3103/S106287381511012X\"\n     onclick=\"log_download('kozakov-kochur-googlev-nikolskii-torgashev-shevcova-finestructureofthexrayphotoelectronni2textrmpspectruminnitextrm1xcotextrmxcrtextrm2otextrm4compounds-2015', 'http://doi.org/10.3103/S106287381511012X', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kozakov-kochur-googlev-nikolskii-torgashev-shevcova-finestructureofthexrayphotoelectronni2textrmpspectruminnitextrm1xcotextrmxcrtextrm2otextrm4compounds-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kozakov-kochur-googlev-nikolskii-torgashev-shevcova-finestructureofthexrayphotoelectronni2textrmpspectruminnitextrm1xcotextrmxcrtextrm2otextrm4compounds-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kozakov_fine_2015,\n\ttitle = {Fine structure of the {X}-ray photoelectron {Ni} 2$_{\\textrm{p}}$ spectrum in {Ni}$_{\\textrm{1–x}}${Co}$_{\\textrm{x}}${Cr}$_{\\textrm{2}}${O}$_{\\textrm{4}}$ compounds},\n\tvolume = {79},\n\tissn = {1934-9432},\n\turl = {https://doi.org/10.3103/S106287381511012X},\n\tdoi = {10.3103/S106287381511012X},\n\tabstract = {An interpretation of the components of the fine structure of X-ray photoelectron Ni \\$\\$\\{2\\_\\{\\{p\\_\\{3/1,1/2\\}\\}\\}\\}\\$\\$spectra of Ni1–xCoxCr2O4 solid solutions (x = 0.8, 0.5, 0.3, 0.02, 0.01, 0.005, 0.0) is given. It is shown that the A and B components of the fine structure in Ni \\$\\$\\{2\\_\\{\\{p\\_\\{3/2\\}\\}\\}\\}\\$\\$spectra originate from the Ni2+ ions located in the octahedral and tetrahedral environments, respectively. The fraction of Ni2+ ions that occupy octahedral positions in ceramics of different composition is determined.},\n\tlanguage = {en},\n\tnumber = {11},\n\turldate = {2023-11-11},\n\tjournal = {Bulletin of the Russian Academy of Sciences: Physics},\n\tauthor = {Kozakov, A. T. and Kochur, A. G. and Googlev, K. A. and Nikolskii, A. V. and Torgashev, V. I. and Shevcova, S. I.},\n\tmonth = nov,\n\tyear = {2015},\n\tkeywords = {Cr2O4 Solid Solution, Divalent Nickel, Hedral Position, Octahedral Crystal Field, Octahedral Position},\n\tpages = {1371--1375},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  An interpretation of the components of the fine structure of X-ray photoelectron Ni $$\\2_\\\\p_\\3/1,1/2\\\\\\\\$$spectra of Ni1–xCoxCr2O4 solid solutions (x = 0.8, 0.5, 0.3, 0.02, 0.01, 0.005, 0.0) is given. It is shown that the A and B components of the fine structure in Ni $$\\2_\\\\p_\\3/2\\\\\\\\$$spectra originate from the Ni2+ ions located in the octahedral and tetrahedral environments, respectively. The fraction of Ni2+ ions that occupy octahedral positions in ceramics of different composition is determined.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"tikhonov-razumnaya-torgashev-zakharchenko-yuzyuk-elmarssi-ortega-kumar-etal-emergenceofthesubthzcentralpeakatphasetransitionsinartificialbatiotextrm3basrtiotextrm3superlattices-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssr.201409505\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'tikhonov-razumnaya-torgashev-zakharchenko-yuzyuk-elmarssi-ortega-kumar-etal-emergenceofthesubthzcentralpeakatphasetransitionsinartificialbatiotextrm3basrtiotextrm3superlattices-2015', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/pssr.201409505', event);\">\n    Emergence of the sub-THz central peak at phase transitions in artificial BaTiO$_{\\textrm{3}}$/(Ba,Sr)TiO$_{\\textrm{3}}$ superlattices.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Tikhonov, Y. A.; Razumnaya, A. G.; Torgashev, V. I.; Zakharchenko, I. N.; Yuzyuk, Y. I.; El Marssi, M.; Ortega, N.; Kumar, A.;  and Katiyar, R. S.\n</span>\n\n  \n\n</span>\n\n  <i>physica status solidi (RRL) – Rapid Research Letters</i>, 9(1): 68–71.  2015.\n  <span class=\"note\">_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssr.201409505</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssr.201409505\"\n     onclick=\"log_download('tikhonov-razumnaya-torgashev-zakharchenko-yuzyuk-elmarssi-ortega-kumar-etal-emergenceofthesubthzcentralpeakatphasetransitionsinartificialbatiotextrm3basrtiotextrm3superlattices-2015', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/pssr.201409505', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Emergence of the sub-THz central peak at phase transitions in artificial BaTiO$_{\\textrm{3}}$/(Ba,Sr)TiO$_{\\textrm{3}}$ superlattices [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1002/pssr.201409505\"\n     onclick=\"log_download('tikhonov-razumnaya-torgashev-zakharchenko-yuzyuk-elmarssi-ortega-kumar-etal-emergenceofthesubthzcentralpeakatphasetransitionsinartificialbatiotextrm3basrtiotextrm3superlattices-2015', 'http://doi.org/10.1002/pssr.201409505', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/tikhonov-razumnaya-torgashev-zakharchenko-yuzyuk-elmarssi-ortega-kumar-etal-emergenceofthesubthzcentralpeakatphasetransitionsinartificialbatiotextrm3basrtiotextrm3superlattices-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('tikhonov-razumnaya-torgashev-zakharchenko-yuzyuk-elmarssi-ortega-kumar-etal-emergenceofthesubthzcentralpeakatphasetransitionsinartificialbatiotextrm3basrtiotextrm3superlattices-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{tikhonov_emergence_2015,\n\ttitle = {Emergence of the sub-{THz} central peak at phase transitions in artificial {BaTiO}$_{\\textrm{3}}$/({Ba},{Sr}){TiO}$_{\\textrm{3}}$ superlattices},\n\tvolume = {9},\n\tcopyright = {© 2015 WILEY-VCH Verlag GmbH \\&amp; Co. KGaA, Weinheim},\n\tissn = {1862-6270},\n\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssr.201409505},\n\tdoi = {10.1002/pssr.201409505},\n\tabstract = {A prominent central peak in the sub-THz frequency range was observed in the Raman spectra of BaTiO3/(Ba,Sr)TiO3 (BT/BST) superlattice grown on (001)MgO substrate. Both soft and central mode show an anomaly around 200 K and 280 K, which can be correlated with orthorhombic to monoclinic phase transition of BST and BT, respectively. The observed temperature dependence of the central mode enabled us to explain rather broad temperature dependence of the dielectric permittivity previously observed in BT/BST superlattices. (© 2015 WILEY-VCH Verlag GmbH \\&amp;Co. KGaA, Weinheim)},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {physica status solidi (RRL) – Rapid Research Letters},\n\tauthor = {Tikhonov, Yu. A. and Razumnaya, A. G. and Torgashev, V. I. and Zakharchenko, I. N. and Yuzyuk, Yu. I. and El Marssi, M. and Ortega, N. and Kumar, A. and Katiyar, R. S.},\n\tyear = {2015},\n\tnote = {\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssr.201409505},\n\tkeywords = {Raman spectroscopy, ferroelectrics, BaTiO3, phase transitions, soft mode, superlattices},\n\tpages = {68--71},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A prominent central peak in the sub-THz frequency range was observed in the Raman spectra of BaTiO3/(Ba,Sr)TiO3 (BT/BST) superlattice grown on (001)MgO substrate. Both soft and central mode show an anomaly around 200 K and 280 K, which can be correlated with orthorhombic to monoclinic phase transition of BST and BT, respectively. The observed temperature dependence of the central mode enabled us to explain rather broad temperature dependence of the dielectric permittivity previously observed in BT/BST superlattices. (© 2015 WILEY-VCH Verlag GmbH &Co. KGaA, Weinheim)\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"anokhin-yuzyuk-lyanguzov-razumnaya-stryukov-bunina-golovko-shirokov-etal-directtransitionfromtherhombohedralferroelectrictotheparaelectricphaseinabasrtiotextrm3thinfilmona111mgosubstrate-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1209/0295-5075/112/47001\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'anokhin-yuzyuk-lyanguzov-razumnaya-stryukov-bunina-golovko-shirokov-etal-directtransitionfromtherhombohedralferroelectrictotheparaelectricphaseinabasrtiotextrm3thinfilmona111mgosubstrate-2015', 'https://dx.doi.org/10.1209/0295-5075/112/47001', event);\">\n    Direct transition from the rhombohedral ferroelectric to the paraelectric phase in a (Ba,Sr)TiO$_{\\textrm{3}}$ thin film on a (111)MgO substrate.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Anokhin, A. S.; Yuzyuk, Y. I.; Lyanguzov, N. V.; Razumnaya, A. G.; Stryukov, D. V.; Bunina, O. A.; Golovko, Y. I.; Shirokov, V. B.; Mukhortov, V. M.;  and Marssi, M. E.\n</span>\n\n  \n\n</span>\n\n  <i>Europhysics Letters</i>, 112(4): 47001. November 2015.\n  <span class=\"note\">Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1209/0295-5075/112/47001\"\n     onclick=\"log_download('anokhin-yuzyuk-lyanguzov-razumnaya-stryukov-bunina-golovko-shirokov-etal-directtransitionfromtherhombohedralferroelectrictotheparaelectricphaseinabasrtiotextrm3thinfilmona111mgosubstrate-2015', 'https://dx.doi.org/10.1209/0295-5075/112/47001', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Direct transition from the rhombohedral ferroelectric to the paraelectric phase in a (Ba,Sr)TiO$_{\\textrm{3}}$ thin film on a (111)MgO substrate [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1209/0295-5075/112/47001\"\n     onclick=\"log_download('anokhin-yuzyuk-lyanguzov-razumnaya-stryukov-bunina-golovko-shirokov-etal-directtransitionfromtherhombohedralferroelectrictotheparaelectricphaseinabasrtiotextrm3thinfilmona111mgosubstrate-2015', 'http://doi.org/10.1209/0295-5075/112/47001', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/anokhin-yuzyuk-lyanguzov-razumnaya-stryukov-bunina-golovko-shirokov-etal-directtransitionfromtherhombohedralferroelectrictotheparaelectricphaseinabasrtiotextrm3thinfilmona111mgosubstrate-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('anokhin-yuzyuk-lyanguzov-razumnaya-stryukov-bunina-golovko-shirokov-etal-directtransitionfromtherhombohedralferroelectrictotheparaelectricphaseinabasrtiotextrm3thinfilmona111mgosubstrate-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{anokhin_direct_2015,\n\ttitle = {Direct transition from the rhombohedral ferroelectric to the paraelectric phase in a ({Ba},{Sr}){TiO}$_{\\textrm{3}}$ thin film on a (111){MgO} substrate},\n\tvolume = {112},\n\tissn = {0295-5075},\n\turl = {https://dx.doi.org/10.1209/0295-5075/112/47001},\n\tdoi = {10.1209/0295-5075/112/47001},\n\tabstract = {A heteroepitaxial (200 nm thick) (BST) thin film was deposited on a (111)MgO substrate using rf sputtering. X-ray diffraction examinations confirmed epitaxial growth and rhombohedral symmetry of the film ( and ) at room temperature. Polarized Raman spectra of the film were studied in the temperature range from 100 to 420 K. In contrast to a BST thin film grown on (001)MgO, the observed linear temperature dependence of the squared soft mode frequency suggests the displacive character of the ferroelectric-paraelectric phase transition in a BST thin film on (111)MgO.},\n\tlanguage = {en},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Europhysics Letters},\n\tauthor = {Anokhin, A. S. and Yuzyuk, Yu I. and Lyanguzov, N. V. and Razumnaya, A. G. and Stryukov, D. V. and Bunina, O. A. and Golovko, Yu I. and Shirokov, V. B. and Mukhortov, V. M. and Marssi, M. El},\n\tmonth = nov,\n\tyear = {2015},\n\tnote = {Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica},\n\tpages = {47001},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A heteroepitaxial (200 nm thick) (BST) thin film was deposited on a (111)MgO substrate using rf sputtering. X-ray diffraction examinations confirmed epitaxial growth and rhombohedral symmetry of the film ( and ) at room temperature. Polarized Raman spectra of the film were studied in the temperature range from 100 to 420 K. In contrast to a BST thin film grown on (001)MgO, the observed linear temperature dependence of the squared soft mode frequency suggests the displacive character of the ferroelectric-paraelectric phase transition in a BST thin film on (111)MgO.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-kalinchuk-shakhovoy-yuzyuk-controlofacousticpropertiesofabatiotextrm3thinfilmbyaplanarelectricfield-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1209/0295-5075/111/16002\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-kalinchuk-shakhovoy-yuzyuk-controlofacousticpropertiesofabatiotextrm3thinfilmbyaplanarelectricfield-2015', 'https://dx.doi.org/10.1209/0295-5075/111/16002', event);\">\n    Control of acoustic properties of a BaTiO$_{\\textrm{3}}$ thin film by a planar electric field.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V.; Kalinchuk, V.; Shakhovoy, R.;  and Yuzyuk, Y.\n</span>\n\n  \n\n</span>\n\n  <i>Europhysics Letters</i>, 111(1): 16002. July 2015.\n  <span class=\"note\">Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1209/0295-5075/111/16002\"\n     onclick=\"log_download('shirokov-kalinchuk-shakhovoy-yuzyuk-controlofacousticpropertiesofabatiotextrm3thinfilmbyaplanarelectricfield-2015', 'https://dx.doi.org/10.1209/0295-5075/111/16002', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Control of acoustic properties of a BaTiO$_{\\textrm{3}}$ thin film by a planar electric field [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1209/0295-5075/111/16002\"\n     onclick=\"log_download('shirokov-kalinchuk-shakhovoy-yuzyuk-controlofacousticpropertiesofabatiotextrm3thinfilmbyaplanarelectricfield-2015', 'http://doi.org/10.1209/0295-5075/111/16002', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-kalinchuk-shakhovoy-yuzyuk-controlofacousticpropertiesofabatiotextrm3thinfilmbyaplanarelectricfield-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-kalinchuk-shakhovoy-yuzyuk-controlofacousticpropertiesofabatiotextrm3thinfilmbyaplanarelectricfield-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_control_2015,\n\ttitle = {Control of acoustic properties of a {BaTiO}$_{\\textrm{3}}$ thin film by a planar electric field},\n\tvolume = {111},\n\tissn = {0295-5075},\n\turl = {https://dx.doi.org/10.1209/0295-5075/111/16002},\n\tdoi = {10.1209/0295-5075/111/16002},\n\tabstract = {An influence of a planar electric field on material coefficients of a barium titanate film has been studied. Electric-field dependences of dielectric constants, elastic and piezoelectric moduli were built for the (001)-oriented film on a cubic substrate with a misfit strain value equal to . It was revealed that an electromechanical coupling coefficient, k11, has a maximum at some value of the electric field, which depends on the clamping stress. The misfit strain dependence of the maximum value of the k11 coefficient was studied at strains below (c-phase).},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Europhysics Letters},\n\tauthor = {Shirokov, Vladimir and Kalinchuk, Valery and Shakhovoy, Roman and Yuzyuk, Yury},\n\tmonth = jul,\n\tyear = {2015},\n\tnote = {Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica},\n\tpages = {16002},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  An influence of a planar electric field on material coefficients of a barium titanate film has been studied. Electric-field dependences of dielectric constants, elastic and piezoelectric moduli were built for the (001)-oriented film on a cubic substrate with a misfit strain value equal to . It was revealed that an electromechanical coupling coefficient, k11, has a maximum at some value of the electric field, which depends on the clamping stress. The misfit strain dependence of the maximum value of the k11 coefficient was studied at strains below (c-phase).\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"razumnaya-tikhonov-yuzyuk-zakharchenko-torgashev-ortega-kumar-katiyar-etal-coexistenceofthesoftmodeandsubthzcentralpeakinferroelectricbatiotextrm3basrtiotextrm3superlattices-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0749603615301117\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'razumnaya-tikhonov-yuzyuk-zakharchenko-torgashev-ortega-kumar-katiyar-etal-coexistenceofthesoftmodeandsubthzcentralpeakinferroelectricbatiotextrm3basrtiotextrm3superlattices-2015', 'https://www.sciencedirect.com/science/article/pii/S0749603615301117', event);\">\n    Coexistence of the soft mode and sub-THz central peak in ferroelectric BaTiO$_{\\textrm{3}}$/(Ba,Sr)TiO$_{\\textrm{3}}$ superlattices.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Razumnaya, A. G.; Tikhonov, Y. A.; Yuzyuk, Y. I.; Zakharchenko, I. N.; Torgashev, V. I.; Ortega, N.; Kumar, A.; Katiyar, R. S.; El Marssi, M.;  and Lukyanchuk, I. A.\n</span>\n\n  \n\n</span>\n\n  <i>Superlattices and Microstructures</i>, 87: 19–24. November 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0749603615301117\"\n     onclick=\"log_download('razumnaya-tikhonov-yuzyuk-zakharchenko-torgashev-ortega-kumar-katiyar-etal-coexistenceofthesoftmodeandsubthzcentralpeakinferroelectricbatiotextrm3basrtiotextrm3superlattices-2015', 'https://www.sciencedirect.com/science/article/pii/S0749603615301117', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Coexistence of the soft mode and sub-THz central peak in ferroelectric BaTiO$_{\\textrm{3}}$/(Ba,Sr)TiO$_{\\textrm{3}}$ superlattices [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.spmi.2015.07.038\"\n     onclick=\"log_download('razumnaya-tikhonov-yuzyuk-zakharchenko-torgashev-ortega-kumar-katiyar-etal-coexistenceofthesoftmodeandsubthzcentralpeakinferroelectricbatiotextrm3basrtiotextrm3superlattices-2015', 'http://doi.org/10.1016/j.spmi.2015.07.038', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/razumnaya-tikhonov-yuzyuk-zakharchenko-torgashev-ortega-kumar-katiyar-etal-coexistenceofthesoftmodeandsubthzcentralpeakinferroelectricbatiotextrm3basrtiotextrm3superlattices-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('razumnaya-tikhonov-yuzyuk-zakharchenko-torgashev-ortega-kumar-katiyar-etal-coexistenceofthesoftmodeandsubthzcentralpeakinferroelectricbatiotextrm3basrtiotextrm3superlattices-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{razumnaya_coexistence_2015,\n\tseries = {Proceedings of the 16th {International} {Conference} on the {Physics} of {Light}–{Matter} {Coupling} in {Nanostructures}, {PLMCN} 2015 ({Medellín}, {Colombia}), 3-8 {February}, 2015},\n\ttitle = {Coexistence of the soft mode and sub-{THz} central peak in ferroelectric {BaTiO}$_{\\textrm{3}}$/({Ba},{Sr}){TiO}$_{\\textrm{3}}$ superlattices},\n\tvolume = {87},\n\tissn = {0749-6036},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0749603615301117},\n\tdoi = {10.1016/j.spmi.2015.07.038},\n\tabstract = {Near- and sub-Terahertz dynamics of soft and Debye-type central modes was studied by the polarized Raman spectroscopy in ferroelectric BaTiO3/Ba0.3Sr0.7TiO3 (BT/BST) superlattice in the temperature range of 80–400K where system undergoes the series of phase transitions: paraelectric-tetragonal–monoclinic in BT layers and paraelectric-orthorhombic-monoclinic in BST layers. It was shown that temperature evolution of these modes can be described within the model of coexisted damped harmonic oscillator and Debye relaxator. The occurrence of the pronounced central mode can explain the recently observed relaxor-like dielectric anomaly in such superlattice.},\n\turldate = {2023-11-11},\n\tjournal = {Superlattices and Microstructures},\n\tauthor = {Razumnaya, A. G. and Tikhonov, Yu. A. and Yuzyuk, Yu. I. and Zakharchenko, I. N. and Torgashev, V. I. and Ortega, N. and Kumar, A. and Katiyar, R. S. and El Marssi, M. and Lukyanchuk, I. A.},\n\tmonth = nov,\n\tyear = {2015},\n\tkeywords = {Ferroelectrics, Raman spectroscopy, Debye relaxator, Phase transitions, Soft mode, Superlattice},\n\tpages = {19--24},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Near- and sub-Terahertz dynamics of soft and Debye-type central modes was studied by the polarized Raman spectroscopy in ferroelectric BaTiO3/Ba0.3Sr0.7TiO3 (BT/BST) superlattice in the temperature range of 80–400K where system undergoes the series of phase transitions: paraelectric-tetragonal–monoclinic in BT layers and paraelectric-orthorhombic-monoclinic in BST layers. It was shown that temperature evolution of these modes can be described within the model of coexisted damped harmonic oscillator and Debye relaxator. The occurrence of the pronounced central mode can explain the recently observed relaxor-like dielectric anomaly in such superlattice.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----ortega-kumar-katiyar--2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/41506\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----ortega-kumar-katiyar--2015', 'http://journals.ioffe.ru/articles/41506', event);\">\n    Фазовые переходы в двух- и трехкомпонентных сверхрешетках перовскитов.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Тихонов, Ю. А.; Разумная, А. Г.; Маслова, О. А.; Захарченко, И. Н.; Юзюк, Ю. И.; Ortega, N.; Kumar, A.;  and Katiyar, R. S.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 57(3): 475–480. February 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/41506\"\n     onclick=\"log_download('-----ortega-kumar-katiyar--2015', 'http://journals.ioffe.ru/articles/41506', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Фазовые переходы в двух- и трехкомпонентных сверхрешетках перовскитов [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----ortega-kumar-katiyar--2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----ortega-kumar-katiyar--2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2015-2,\n\ttitle = {Фазовые переходы в двух- и трехкомпонентных сверхрешетках перовскитов},\n\tvolume = {57},\n\turl = {http://journals.ioffe.ru/articles/41506},\n\tabstract = {Исследовано температурное поведение поляризационных спектров комбинационного рассеяния света двухслойной BaTiO3/Ba0.5Sr0.5TiO3 и трехслойной BaTiO3/Ba0.5Sr0.5TiO3/SrTiO3 сверхрешеток, полученных методом импульсного лазерного напыления на подложках (001)MgO. Установлено, что в трехслойной сверхрешетке частота мягкой моды E(TO) при комнатной температуре значительно выше (94 cm-1), чем в двухслойной (70 cm-1), что свидетельствует об увеличении двумерных напряжений в эпитаксиальных слоях трехслойной сверхрешетки. Анализ температурной зависимости интегральной интенсивности мягкой моды E(TO) позволяет предполагать, что в сверхрешетке BaTiO3/Ba0.5Sr0.5TiO3 переход из сегнетоэлектрической в параэлектрическую фазу происходит при {\\textasciitilde}540 K, а в сверхрешетке BaTiO3/Ba0.5Sr0.5TiO3/SrTiO3 температура фазового перехода повышается до {\\textasciitilde} 610 K из-за деформаций эпитаксиальных слоев. Работа выполнена за счет гранта Российского научного фонда (проект N 14-12-00258).},\n\tlanguage = {ru},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Тихонов, Ю. А. and Разумная, А. Г. and Маслова, О. А. and Захарченко, И. Н. and Юзюк, Ю. И. and Ortega, N. and Kumar, A. and Katiyar, R. S.},\n\tmonth = feb,\n\tyear = {2015},\n\tpages = {475--480},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследовано температурное поведение поляризационных спектров комбинационного рассеяния света двухслойной BaTiO3/Ba0.5Sr0.5TiO3 и трехслойной BaTiO3/Ba0.5Sr0.5TiO3/SrTiO3 сверхрешеток, полученных методом импульсного лазерного напыления на подложках (001)MgO. Установлено, что в трехслойной сверхрешетке частота мягкой моды E(TO) при комнатной температуре значительно выше (94 cm-1), чем в двухслойной (70 cm-1), что свидетельствует об увеличении двумерных напряжений в эпитаксиальных слоях трехслойной сверхрешетки. Анализ температурной зависимости интегральной интенсивности мягкой моды E(TO) позволяет предполагать, что в сверхрешетке BaTiO3/Ba0.5Sr0.5TiO3 переход из сегнетоэлектрической в параэлектрическую фазу происходит при ~540 K, а в сверхрешетке BaTiO3/Ba0.5Sr0.5TiO3/SrTiO3 температура фазового перехода повышается до ~ 610 K из-за деформаций эпитаксиальных слоев. Работа выполнена за счет гранта Российского научного фонда (проект N 14-12-00258).\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----janolin-dkhil--2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://bibbase.org/f/NkS9m4R3ieFPicBbH/Зависимость%20свойств%20эпитаксиальных%20тонких%20пленок%20титаната%20бария-стронция%20при%20изменении%20толщины\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----janolin-dkhil--2015', 'https://bibbase.org/f/NkS9m4R3ieFPicBbH/Зависимость%20свойств%20эпитаксиальных%20тонких%20пленок%20титаната%20бария-стронция%20при%20изменении%20толщины', event);\">\n    Зависимость свойств эпитаксиальных тонких пленок титаната бария-стронция при изменении толщины.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Широков, В. Б.; Головко, Ю. И.; Мухортов, В. М.; Юзюк, Ю. И.; Janolin, P. E.;  and Dkhil, B.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 57(8): 1503–1508. July 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://bibbase.org/f/NkS9m4R3ieFPicBbH/Зависимость%20свойств%20эпитаксиальных%20тонких%20пленок%20титаната%20бария-стронция%20при%20изменении%20толщины\"\n     onclick=\"log_download('----janolin-dkhil--2015', 'https://bibbase.org/f/NkS9m4R3ieFPicBbH/Зависимость%20свойств%20эпитаксиальных%20тонких%20пленок%20титаната%20бария-стронция%20при%20изменении%20толщины', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Зависимость свойств эпитаксиальных тонких пленок титаната бария-стронция при изменении толщины [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----janolin-dkhil--2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----janolin-dkhil--2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2015-3,\n\ttitle = {Зависимость свойств эпитаксиальных тонких пленок титаната бария-стронция при изменении толщины},\n\tvolume = {57},\n\turl = {Зависимость свойств эпитаксиальных тонких пленок титаната бария-стронция при изменении толщины},\n\tabstract = {Проведены исследования гетероэпитаксиальных тонких пленок BaxSr1-xTiO3 различной толщины в параэлектрической фазе при температуре 600oC. Параметры решетки пленки показывают нелинейную зависимость от толщины. С уменьшением толщины происходит увеличение вынужденной деформации и увеличивается объем элементарной ячейки. Поведение вынужденной деформации при изменении толщины хорошо описывается в модели двойного электрического слоя, образовавшегося в процессе синтеза пленки на границе с подложкой. Работа выполнена при поддержке РФФИ (гранты N 13-02-00251а, 13-02-12085-ОФИ\\_М и 13-01-90619 Арм\\_а).},\n\tlanguage = {ru},\n\tnumber = {8},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Широков, В. Б. and Головко, Ю. И. and Мухортов, В. М. and Юзюк, Ю. И. and Janolin, P. E. and Dkhil, B.},\n\tmonth = jul,\n\tyear = {2015},\n\tpages = {1503--1508},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Проведены исследования гетероэпитаксиальных тонких пленок BaxSr1-xTiO3 различной толщины в параэлектрической фазе при температуре 600oC. Параметры решетки пленки показывают нелинейную зависимость от толщины. С уменьшением толщины происходит увеличение вынужденной деформации и увеличивается объем элементарной ячейки. Поведение вынужденной деформации при изменении толщины хорошо описывается в модели двойного электрического слоя, образовавшегося в процессе синтеза пленки на границе с подложкой. Работа выполнена при поддержке РФФИ (гранты N 13-02-00251а, 13-02-12085-ОФИ_М и 13-01-90619 Арм_а).\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/41613\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----2015', 'http://journals.ioffe.ru/articles/41613', event);\">\n    Структуры капсидов сферических вирусов как квазикристаллические укладки.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Коневцова, О. В.; Лорман, В. Л.;  and Рошаль, С. Б.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 57(4): 790–795. March 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/41613\"\n     onclick=\"log_download('----2015', 'http://journals.ioffe.ru/articles/41613', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Структуры капсидов сферических вирусов как квазикристаллические укладки [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2015-4,\n\ttitle = {Структуры капсидов сферических вирусов как квазикристаллические укладки},\n\tvolume = {57},\n\turl = {http://journals.ioffe.ru/articles/41613},\n\tabstract = {Рассматрены вирусные сферические оболочки с икосаэдрической симметрией как квазикристаллические укладки. Аналогично известной теории квазиэквивалентности Каспара и Клуга данный подход также минимизирует количество конформаций, необходимых белковой молекуле для образования связей с соседями в оболочке, но основан на отличных геометрических принципах. Предполагается, что центры белковых молекул находятся в вершинах плиток с одинаковыми ребрами, а количество разных сортов плиток минимально. Получены идеализированные координаты симметрийно-неэквивалентных позиций протеинов в шести различных типах капсидов. Подход описывает единообразно как структуры, удовлетворяющие хорошо известной геометрической модели Каспара и Клуга, так и противоречащие ей. Работа выполнена при поддержке РФФИ (грант N 13-02-12085офи\\_м). В.Л. благодарит Labex NUMEV за финансовую поддержку.},\n\tlanguage = {ru},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Коневцова, О. В. and Лорман, В. Л. and Рошаль, С. Б.},\n\tmonth = mar,\n\tyear = {2015},\n\tpages = {790--795},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Рассматрены вирусные сферические оболочки с икосаэдрической симметрией как квазикристаллические укладки. Аналогично известной теории квазиэквивалентности Каспара и Клуга данный подход также минимизирует количество конформаций, необходимых белковой молекуле для образования связей с соседями в оболочке, но основан на отличных геометрических принципах. Предполагается, что центры белковых молекул находятся в вершинах плиток с одинаковыми ребрами, а количество разных сортов плиток минимально. Получены идеализированные координаты симметрийно-неэквивалентных позиций протеинов в шести различных типах капсидов. Подход описывает единообразно как структуры, удовлетворяющие хорошо известной геометрической модели Каспара и Клуга, так и противоречащие ей. Работа выполнена при поддержке РФФИ (грант N 13-02-12085офи_м). В.Л. благодарит Labex NUMEV за финансовую поддержку.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/42109\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----2015', 'http://journals.ioffe.ru/articles/42109', event);\">\n    Материальные константы тонких пленок титаната бария.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Широков, В. Б.; Калинчук, В. В.; Шаховой, Р. А.;  and Юзюк, Ю. И.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 57(8): 1509–1514. July 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/42109\"\n     onclick=\"log_download('-----2015', 'http://journals.ioffe.ru/articles/42109', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Материальные константы тонких пленок титаната бария [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2015-5,\n\ttitle = {Материальные константы тонких пленок титаната бария},\n\tvolume = {57},\n\turl = {http://journals.ioffe.ru/articles/42109},\n\tabstract = {Нелинейные свойства титаната бария приводят к изменению материальных постоянных линейных уравнений пьезоэффекта для тонких пленок. На основе потенциала Ландау феноменологической теории исследовано поведение материальных постоянных монокристаллических тонких пленок титаната бария при комнатной температуре в зависимости от величины вынужденной деформации. Большинство материальных постоянных при изменении деформации испытывают аномалии на границах фаз. Внутри r-фазы некоторые упругие и электроупругие постоянные достигают экстремума. Полученные результаты позволяют определить направление поиска для получения пленок с необходимыми свойствами. Работа выполнена при финансовой поддержке Российского научного фонда, грант N 14-19-01676.},\n\tlanguage = {ru},\n\tnumber = {8},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Широков, В. Б. and Калинчук, В. В. and Шаховой, Р. А. and Юзюк, Ю. И.},\n\tmonth = jul,\n\tyear = {2015},\n\tpages = {1509--1514},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Нелинейные свойства титаната бария приводят к изменению материальных постоянных линейных уравнений пьезоэффекта для тонких пленок. На основе потенциала Ландау феноменологической теории исследовано поведение материальных постоянных монокристаллических тонких пленок титаната бария при комнатной температуре в зависимости от величины вынужденной деформации. Большинство материальных постоянных при изменении деформации испытывают аномалии на границах фаз. Внутри r-фазы некоторые упругие и электроупругие постоянные достигают экстремума. Полученные результаты позволяют определить направление поиска для получения пленок с необходимыми свойствами. Работа выполнена при финансовой поддержке Российского научного фонда, грант N 14-19-01676.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"--------etal--2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/42491\"\n     onclick=\"return trackOutboundLink('publications', 'click', '--------etal--2015', 'http://journals.ioffe.ru/articles/42491', event);\">\n    Критическое рассеяние синхротронного излучения в цирконате-титанате свинца с малой концентрацией титана.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Андроникова, Д. А.; Босак, А. А.; Бронвальд, Ю. А.; Бурковский, Р. Г.; Вахрушев, С. Б.; Леонтьев, Н. Г.; Леонтьев, И. Н.; Таганцев, А. К.; Филимонов, А. В.;  and Чернышов, Д. Ю.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 57(12): 2368–2373. November 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/42491\"\n     onclick=\"log_download('--------etal--2015', 'http://journals.ioffe.ru/articles/42491', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Критическое рассеяние синхротронного излучения в цирконате-титанате свинца с малой концентрацией титана [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/--------etal--2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('--------etal--2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2015-6,\n\ttitle = {Критическое рассеяние синхротронного излучения в цирконате-титанате свинца с малой концентрацией титана},\n\tvolume = {57},\n\turl = {http://journals.ioffe.ru/articles/42491},\n\tabstract = {Методом рассеяния синхротронного излучения исследовано диффузное рассеяние в монокристалле цирконата-титаната свинца с концентрацией титана 0.7 at.\\%. Измерения проводились как в окрестности центра зоны Бриллюэна, так и в M-точке. В параэлектрической фазе вблизи центра зоны Бриллюэна выявлено сильно анизотропное диффузное рассеяние, анизотропия диффузного рассеяния сходна с наблюдаемой ранее в чистом цирконате свинца. Температурная зависимость этого диффузного рассеяния имеет критический вид с температурой Tc{\\textasciitilde} 480 K. Диффузное рассеяние в окрестности M-точки слабо зависит от температуры, причем эта зависимость имеет различный характер в M-точках с различными индексами. Д.А. Андроникова благодарит за финансовую поддержку Правительство РФ (грант N 14.Б25.31.0025), С.Б. Вахрушев и Ю.А. Бронвальд благодарят РФФИ за финансовую поддержу в рамках научного проекта N 14-02-01208.},\n\tlanguage = {ru},\n\tnumber = {12},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Андроникова, Д. А. and Босак, А. А. and Бронвальд, Ю. А. and Бурковский, Р. Г. and Вахрушев, С. Б. and Леонтьев, Н. Г. and Леонтьев, И. Н. and Таганцев, А. К. and Филимонов, А. В. and Чернышов, Д. Ю.},\n\tmonth = nov,\n\tyear = {2015},\n\tpages = {2368--2373},\n\tfile = {Физика твердого тела:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\AKG5ZVNI\\\\42491.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Методом рассеяния синхротронного излучения исследовано диффузное рассеяние в монокристалле цирконата-титаната свинца с концентрацией титана 0.7 at.%. Измерения проводились как в окрестности центра зоны Бриллюэна, так и в M-точке. В параэлектрической фазе вблизи центра зоны Бриллюэна выявлено сильно анизотропное диффузное рассеяние, анизотропия диффузного рассеяния сходна с наблюдаемой ранее в чистом цирконате свинца. Температурная зависимость этого диффузного рассеяния имеет критический вид с температурой Tc~ 480 K. Диффузное рассеяние в окрестности M-точки слабо зависит от температуры, причем эта зависимость имеет различный характер в M-точках с различными индексами. Д.А. Андроникова благодарит за финансовую поддержку Правительство РФ (грант N 14.Б25.31.0025), С.Б. Вахрушев и Ю.А. Бронвальд благодарят РФФИ за финансовую поддержу в рамках научного проекта N 14-02-01208.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------elmarssi--2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/42408\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------elmarssi--2015', 'http://journals.ioffe.ru/articles/42408', event);\">\n    Сегнетоэлектрическая сверхрешетка на основе твердых растворов титаната бария-стронция.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Разумная, А. Г.; Головко, Ю. И.; Лянгузов, Н. В.; Юзюк, Ю. И.; Широков, В. Б.; Мухортов, В. М.;  and El Marssi, M.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 57(11): 2181–2185. October 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/42408\"\n     onclick=\"log_download('------elmarssi--2015', 'http://journals.ioffe.ru/articles/42408', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Сегнетоэлектрическая сверхрешетка на основе твердых растворов титаната бария-стронция [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------elmarssi--2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------elmarssi--2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2015-7,\n\ttitle = {Сегнетоэлектрическая сверхрешетка на основе твердых растворов титаната бария-стронция},\n\tvolume = {57},\n\turl = {http://journals.ioffe.ru/articles/42408},\n\tabstract = {Сверхрешетка состава Ba0.8Sr0.2TiO3/Ba0.4Sr0.6TiO3 выращена методом высокочастотного катодного распыления на подложке (001)MgO. С помощью рентгеновской дифракции определены параметры элементарных ячеек слоев сверхрешетки по нормали к подложке, период модуляции и ориентационные соотношения между пленкой и подложкой. На основе температурной зависимости поляризованных спектров комбинационного рассеяния света обнаружено, что наблюдается ужесточение мягкой моды E(TO) от 79 до 97 cm-1 в интервале температур 80-350 K. Характерных признаков последовательности фазовых переходов, которые имеют место в объемных образцах твердых растворов титаната бария-стронция аналогичных составов, не обнаружено, а переход из сегнетоэлектрической в параэлектрическую фазу в сверхрешетке происходит при температуре {\\textasciitilde}350 K. Работа выполнена за счет средств Российского научного фонда (проект N 14-12-00258).},\n\tlanguage = {ru},\n\tnumber = {11},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Разумная, А. Г. and Головко, Ю. И. and Лянгузов, Н. В. and Юзюк, Ю. И. and Широков, В. Б. and Мухортов, В. М. and El Marssi, M.},\n\tmonth = oct,\n\tyear = {2015},\n\tpages = {2181--2185},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Сверхрешетка состава Ba0.8Sr0.2TiO3/Ba0.4Sr0.6TiO3 выращена методом высокочастотного катодного распыления на подложке (001)MgO. С помощью рентгеновской дифракции определены параметры элементарных ячеек слоев сверхрешетки по нормали к подложке, период модуляции и ориентационные соотношения между пленкой и подложкой. На основе температурной зависимости поляризованных спектров комбинационного рассеяния света обнаружено, что наблюдается ужесточение мягкой моды E(TO) от 79 до 97 cm-1 в интервале температур 80-350 K. Характерных признаков последовательности фазовых переходов, которые имеют место в объемных образцах твердых растворов титаната бария-стронция аналогичных составов, не обнаружено, а переход из сегнетоэлектрической в параэлектрическую фазу в сверхрешетке происходит при температуре ~350 K. Работа выполнена за счет средств Российского научного фонда (проект N 14-12-00258).\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"torgashev-gorshunov-zhukova-savinov-kadlec-kadlec-skoromets-prokleka-etal-broadbandspectroscopyofhtextrm2omoleculeconfinedinnanocagesofcrystallatticelowenergydynamicsandincipientferroelectricbehavior-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://ieeexplore.ieee.org/document/7327553?arnumber=7327553\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'torgashev-gorshunov-zhukova-savinov-kadlec-kadlec-skoromets-prokleka-etal-broadbandspectroscopyofhtextrm2omoleculeconfinedinnanocagesofcrystallatticelowenergydynamicsandincipientferroelectricbehavior-2015', 'https://ieeexplore.ieee.org/document/7327553?arnumber=7327553', event);\">\n    Broadband spectroscopy of H$_{\\textrm{2}}$O molecule confined in nano-cages of crystal lattice: Low-energy dynamics and incipient ferroelectric behavior.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Torgashev, V. I.; Gorshunov, B. P.; Zhukova, E. S.; Savinov, M.; Kadlec, C.; Kadlec, F.; Skoromets, V.; Prokleška, J.; Thomas, V. G.; Fursenko, D. A.; Pestrjakov, E. V.; Uskov, V. V.; Shakurov, G. S.; Kremer, R. K.; Kadyrov, L. S.; Belyanchikov, M. A.; Prokhorov, A. S.; Gorelik, V. S.;  and Dressel, M.\n</span>\n\n  \n\n</span>\n\n  In <i>2015 40th International Conference on Infrared, Millimeter, and Terahertz waves (IRMMW-THz)</i>, pages 1–2, August 2015. \n  <span class=\"note\">ISSN: 2162-2035</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://ieeexplore.ieee.org/document/7327553?arnumber=7327553\"\n     onclick=\"log_download('torgashev-gorshunov-zhukova-savinov-kadlec-kadlec-skoromets-prokleka-etal-broadbandspectroscopyofhtextrm2omoleculeconfinedinnanocagesofcrystallatticelowenergydynamicsandincipientferroelectricbehavior-2015', 'https://ieeexplore.ieee.org/document/7327553?arnumber=7327553', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Broadband spectroscopy of H$_{\\textrm{2}}$O molecule confined in nano-cages of crystal lattice: Low-energy dynamics and incipient ferroelectric behavior [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1109/IRMMW-THz.2015.7327553\"\n     onclick=\"log_download('torgashev-gorshunov-zhukova-savinov-kadlec-kadlec-skoromets-prokleka-etal-broadbandspectroscopyofhtextrm2omoleculeconfinedinnanocagesofcrystallatticelowenergydynamicsandincipientferroelectricbehavior-2015', 'http://doi.org/10.1109/IRMMW-THz.2015.7327553', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/torgashev-gorshunov-zhukova-savinov-kadlec-kadlec-skoromets-prokleka-etal-broadbandspectroscopyofhtextrm2omoleculeconfinedinnanocagesofcrystallatticelowenergydynamicsandincipientferroelectricbehavior-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('torgashev-gorshunov-zhukova-savinov-kadlec-kadlec-skoromets-prokleka-etal-broadbandspectroscopyofhtextrm2omoleculeconfinedinnanocagesofcrystallatticelowenergydynamicsandincipientferroelectricbehavior-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{torgashev_broadband_2015,\n\ttitle = {Broadband spectroscopy of {H}$_{\\textrm{2}}${O} molecule confined in nano-cages of crystal lattice: {Low}-energy dynamics and incipient ferroelectric behavior},\n\tshorttitle = {Broadband spectroscopy of {H2O} molecule confined in nano-cages of crystal lattice},\n\turl = {https://ieeexplore.ieee.org/document/7327553?arnumber=7327553},\n\tdoi = {10.1109/IRMMW-THz.2015.7327553},\n\tabstract = {Broadband (1 Hz to 100 THz) dielectric response of water-containing beryl crystals was measured at temperatures from 300 K down to 0.3 K. The low-energy dynamics of H2O molecules confined within nano-cages of the crystalline lattice was studied. We observe a THz-range soft mode indicating an incipient ferroelectric behavior due to interacting dipole moments of confined water molecules.},\n\turldate = {2023-11-11},\n\tbooktitle = {2015 40th {International} {Conference} on {Infrared}, {Millimeter}, and {Terahertz} waves ({IRMMW}-{THz})},\n\tauthor = {Torgashev, Victor I. and Gorshunov, Boris P. and Zhukova, Elena S. and Savinov, Maxim and Kadlec, Christelle and Kadlec, Filip and Skoromets, Volodymyr and Prokleška, J. and Thomas, Victor G. and Fursenko, Dmitry A. and Pestrjakov, Efim V. and Uskov, Vladimir V. and Shakurov, Gil&#x27;man S. and Kremer, Reinhard K. and Kadyrov, Lenar S. and Belyanchikov, Mikhail A. and Prokhorov, Anatoliy S. and Gorelik, Vladimir S. and Dressel, Martin},\n\tmonth = aug,\n\tyear = {2015},\n\tnote = {ISSN: 2162-2035},\n\tpages = {1--2},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Broadband (1 Hz to 100 THz) dielectric response of water-containing beryl crystals was measured at temperatures from 300 K down to 0.3 K. The low-energy dynamics of H2O molecules confined within nano-cages of the crystalline lattice was studied. We observe a THz-range soft mode indicating an incipient ferroelectric behavior due to interacting dipole moments of confined water molecules.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-------zno-2015\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/42455\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-------zno-2015', 'https://journals.ioffe.ru/articles/42455', event);\">\n    Влияние процессов самоорганизации, дефектов, примесей, а также автокаталитических процессов на параметры пленок и наностержней ZnO.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Мездрогина, М. М.; Еременко, М. В.; Петров, В. Н.; Теруков, Е. И.; Левицкий, В. С.; Кайдашев, Е. М.;  and Лянгузов, Н. В.\n</span>\n\n  \n\n</span>\n\n  <i>Физика и техника полупроводников</i>, 49(11): 1521–1530. October 2015.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/42455\"\n     onclick=\"log_download('-------zno-2015', 'https://journals.ioffe.ru/articles/42455', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Влияние процессов самоорганизации, дефектов, примесей, а также автокаталитических процессов на параметры пленок и наностержней ZnO [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-------zno-2015\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-------zno-2015')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2015-8,\n\ttitle = {Влияние процессов самоорганизации, дефектов, примесей, а также автокаталитических процессов на параметры пленок и наностержней {ZnO}},\n\tvolume = {49},\n\turl = {https://journals.ioffe.ru/articles/42455},\n\tabstract = {Исследовано влияние параметров нанесения пленок ZnO на различные материалы подложек при использовании магнетронного распыления на переменном токе в газовой смеси аргона и кислорода. Наблюдалось явление самоорганизации, приводящее к неизменности морфологии поверхности пленок ZnO при варьировании материалов подложки и параметров нанесения. Параметры спектров макро- и микрофотолюминесценции исследованных пленок ZnO незначительно отличались от параметров спектров фотолюминесценции объемных кристаллов ZnO, полученных методом гидротермального роста. Наличие интенсивного излучения с малой величиной FWHM в разных областях спектра дает возможность рассматривать пленки ZnO, полученные магнетронным распылением, легированные РЗИ, как перспективный материал при создании оптоэлектронных приборов, работающих в широком спектральном диапазоне. Возможность реализации магнитного упорядочения при легировании РЗИ существенно расширяет функциональные возможности пленок ZnO. Параметры спектров фотолюминесценции наностержней ZnO определяются геометрическими параметрами, концентрацией и типом введенных примесей.},\n\tlanguage = {ru},\n\tnumber = {11},\n\turldate = {2023-11-11},\n\tjournal = {Физика и техника полупроводников},\n\tauthor = {Мездрогина, М. М. and Еременко, М. В. and Петров, В. Н. and Теруков, Е. И. and Левицкий, В. С. and Кайдашев, Е. М. and Лянгузов, Н. В.},\n\tmonth = oct,\n\tyear = {2015},\n\tpages = {1521--1530},\n\tfile = {Физика и техника полупроводников:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\5XEFAQZX\\\\42455.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследовано влияние параметров нанесения пленок ZnO на различные материалы подложек при использовании магнетронного распыления на переменном токе в газовой смеси аргона и кислорода. Наблюдалось явление самоорганизации, приводящее к неизменности морфологии поверхности пленок ZnO при варьировании материалов подложки и параметров нанесения. Параметры спектров макро- и микрофотолюминесценции исследованных пленок ZnO незначительно отличались от параметров спектров фотолюминесценции объемных кристаллов ZnO, полученных методом гидротермального роста. Наличие интенсивного излучения с малой величиной FWHM в разных областях спектра дает возможность рассматривать пленки ZnO, полученные магнетронным распылением, легированные РЗИ, как перспективный материал при создании оптоэлектронных приборов, работающих в широком спектральном диапазоне. Возможность реализации магнитного упорядочения при легировании РЗИ существенно расширяет функциональные возможности пленок ZnO. Параметры спектров фотолюминесценции наностержней ZnO определяются геометрическими параметрами, концентрацией и типом введенных примесей.\n</div>\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2014\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2014')\"\n      onkeypress=\"toggleGroup('group_2014')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2014</span>\n      <span class=\"bibbase_group_count\">\n        \n        (44)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"shirokov-kalinchuk-shakhovoy-yuzyuk-anomaliesofpiezoelectriccoefficientsinbariumtitanatethinfilms-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1209/0295-5075/108/47008\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-kalinchuk-shakhovoy-yuzyuk-anomaliesofpiezoelectriccoefficientsinbariumtitanatethinfilms-2014', 'https://dx.doi.org/10.1209/0295-5075/108/47008', event);\">\n    Anomalies of piezoelectric coefficients in barium titanate thin films.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V.; Kalinchuk, V.; Shakhovoy, R.;  and Yuzyuk, Y.\n</span>\n\n  \n\n</span>\n\n  <i>Europhysics Letters</i>, 108(4): 47008. November 2014.\n  <span class=\"note\">Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1209/0295-5075/108/47008\"\n     onclick=\"log_download('shirokov-kalinchuk-shakhovoy-yuzyuk-anomaliesofpiezoelectriccoefficientsinbariumtitanatethinfilms-2014', 'https://dx.doi.org/10.1209/0295-5075/108/47008', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Anomalies of piezoelectric coefficients in barium titanate thin films [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1209/0295-5075/108/47008\"\n     onclick=\"log_download('shirokov-kalinchuk-shakhovoy-yuzyuk-anomaliesofpiezoelectriccoefficientsinbariumtitanatethinfilms-2014', 'http://doi.org/10.1209/0295-5075/108/47008', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-kalinchuk-shakhovoy-yuzyuk-anomaliesofpiezoelectriccoefficientsinbariumtitanatethinfilms-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>1 download</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-kalinchuk-shakhovoy-yuzyuk-anomaliesofpiezoelectriccoefficientsinbariumtitanatethinfilms-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_anomalies_2014,\n\ttitle = {Anomalies of piezoelectric coefficients in barium titanate thin films},\n\tvolume = {108},\n\tissn = {0295-5075},\n\turl = {https://dx.doi.org/10.1209/0295-5075/108/47008},\n\tdoi = {10.1209/0295-5075/108/47008},\n\tabstract = {Modeling of electromechanical devices involves the use of different material coefficients, whose measurement is a difficult task, especially when the problem concerns thin films. Required coefficients of thin films could be found theoretically, using known values of the bulk constants. Electromechanical coefficients of barium titanate thin films are still unknown; therefore, it is expedient to carry out their calculations. We give here the full set of electromechanical coefficients of barium titanate thin films for the whole range of technologically available misfit strains. In the present paper, piezoelectric coefficients as functions of a misfit strain were calculated. It was revealed that piezoelectric coefficients exhibit anomalies at phase boundaries and inside the monoclinic r-phase as well. The obtained results allow finding the required values of the thin-film parameters, varying the misfit strain.},\n\tlanguage = {en},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Europhysics Letters},\n\tauthor = {Shirokov, Vladimir and Kalinchuk, Valery and Shakhovoy, Roman and Yuzyuk, Yury},\n\tmonth = nov,\n\tyear = {2014},\n\tnote = {Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica},\n\tpages = {47008},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Modeling of electromechanical devices involves the use of different material coefficients, whose measurement is a difficult task, especially when the problem concerns thin films. Required coefficients of thin films could be found theoretically, using known values of the bulk constants. Electromechanical coefficients of barium titanate thin films are still unknown; therefore, it is expedient to carry out their calculations. We give here the full set of electromechanical coefficients of barium titanate thin films for the whole range of technologically available misfit strains. In the present paper, piezoelectric coefficients as functions of a misfit strain were calculated. It was revealed that piezoelectric coefficients exhibit anomalies at phase boundaries and inside the monoclinic r-phase as well. The obtained results allow finding the required values of the thin-film parameters, varying the misfit strain.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"gorshunov-zhukova-torgashev-motovilova-lebedev-prokhorov-shakurov-kremer-etal-thzirspectroscopyofsingleh2omoleculesconfinedinnanocageofberylcrystallattice-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/01411594.2014.954247\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'gorshunov-zhukova-torgashev-motovilova-lebedev-prokhorov-shakurov-kremer-etal-thzirspectroscopyofsingleh2omoleculesconfinedinnanocageofberylcrystallattice-2014', 'https://doi.org/10.1080/01411594.2014.954247', event);\">\n    THz–IR spectroscopy of single H2O molecules confined in nanocage of beryl crystal lattice.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Gorshunov, B. P.; Zhukova, E. S.; Torgashev, V. I.; Motovilova, E. A.; Lebedev, V. V.; Prokhorov, A. S.; Shakurov, G. S.; Kremer, R. K.; Uskov, V. V.; Pestrjakov, E. V.; Thomas, V. G.; Fursenko, D. A.; Kadlec, C.; Kadlec, F.;  and Dressel, M.\n</span>\n\n  \n\n</span>\n\n  <i>Phase Transitions</i>, 87(10-11): 966–972. November 2014.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/01411594.2014.954247</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/01411594.2014.954247\"\n     onclick=\"log_download('gorshunov-zhukova-torgashev-motovilova-lebedev-prokhorov-shakurov-kremer-etal-thzirspectroscopyofsingleh2omoleculesconfinedinnanocageofberylcrystallattice-2014', 'https://doi.org/10.1080/01411594.2014.954247', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"THz–IR spectroscopy of single H2O molecules confined in nanocage of beryl crystal lattice [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/01411594.2014.954247\"\n     onclick=\"log_download('gorshunov-zhukova-torgashev-motovilova-lebedev-prokhorov-shakurov-kremer-etal-thzirspectroscopyofsingleh2omoleculesconfinedinnanocageofberylcrystallattice-2014', 'http://doi.org/10.1080/01411594.2014.954247', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/gorshunov-zhukova-torgashev-motovilova-lebedev-prokhorov-shakurov-kremer-etal-thzirspectroscopyofsingleh2omoleculesconfinedinnanocageofberylcrystallattice-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('gorshunov-zhukova-torgashev-motovilova-lebedev-prokhorov-shakurov-kremer-etal-thzirspectroscopyofsingleh2omoleculesconfinedinnanocageofberylcrystallattice-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{gorshunov_thzir_2014,\n\ttitle = {{THz}–{IR} spectroscopy of single {H2O} molecules confined in nanocage of beryl crystal lattice},\n\tvolume = {87},\n\tissn = {0141-1594},\n\turl = {https://doi.org/10.1080/01411594.2014.954247},\n\tdoi = {10.1080/01411594.2014.954247},\n\tabstract = {We have measured the terahertz–infrared (3–7000 cm−1) spectra of the optical conductivity of iron-doped single crystals of beryl, (Mn,Fe):Be3Al2Si6O18, that contain lone water molecules isolated within nanometer-sized cages formed by the ions of beryl crystal lattice. By comparing the spectra with those of dehydrated crystals, we exclude phonon resonances and reconstruct the spectra determined exclusively by vibrations of the water molecules. At liquid-helium temperatures, well-known intramolecular H2O modes are observed above 1000 cm−1 and accompanied with satellite resonances that are combinations of intramolecular and external vibrations of H2O molecules. At terahertz frequencies, a broad bump centred around 20 cm−1 (at 5 K) is observed with three rather narrow resonances at its high-frequency shoulder (38, 42 and 46 cm−1). The origin of these low-energy excitations is discussed.},\n\tnumber = {10-11},\n\turldate = {2023-11-11},\n\tjournal = {Phase Transitions},\n\tauthor = {Gorshunov, Boris P. and Zhukova, Elena S. and Torgashev, Victor I. and Motovilova, Elizaveta A. and Lebedev, Vladimir V. and Prokhorov, Anatoly S. and Shakurov, Gil’man S. and Kremer, Reinhard K. and Uskov, Vladimir V. and Pestrjakov, Efim V. and Thomas, Victor G. and Fursenko, Dimitri A. and Kadlec, Christelle and Kadlec, Filip and Dressel, Martin},\n\tmonth = nov,\n\tyear = {2014},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/01411594.2014.954247},\n\tkeywords = {nano-confined water molecule, terahertz spectroscopy},\n\tpages = {966--972},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We have measured the terahertz–infrared (3–7000 cm−1) spectra of the optical conductivity of iron-doped single crystals of beryl, (Mn,Fe):Be3Al2Si6O18, that contain lone water molecules isolated within nanometer-sized cages formed by the ions of beryl crystal lattice. By comparing the spectra with those of dehydrated crystals, we exclude phonon resonances and reconstruct the spectra determined exclusively by vibrations of the water molecules. At liquid-helium temperatures, well-known intramolecular H2O modes are observed above 1000 cm−1 and accompanied with satellite resonances that are combinations of intramolecular and external vibrations of H2O molecules. At terahertz frequencies, a broad bump centred around 20 cm−1 (at 5 K) is observed with three rather narrow resonances at its high-frequency shoulder (38, 42 and 46 cm−1). The origin of these low-energy excitations is discussed.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"mikheykin-torgashev-talanov-bush-chernyshov-yuzyuk-dmitriev-highpressurexraydiffractionstudyofnickelcopperchromitessolidsolutions-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/0953-8984/26/50/505401\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'mikheykin-torgashev-talanov-bush-chernyshov-yuzyuk-dmitriev-highpressurexraydiffractionstudyofnickelcopperchromitessolidsolutions-2014', 'https://dx.doi.org/10.1088/0953-8984/26/50/505401', event);\">\n    High pressure x-ray diffraction study of nickel–copper chromites solid solutions.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Mikheykin, A. S.; Torgashev, V. I.; Talanov, V. M.; Bush, A. A.; Chernyshov, D.; Yuzyuk, I. Y.;  and Dmitriev, V. P.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics: Condensed Matter</i>, 26(50): 505401. November 2014.\n  <span class=\"note\">Publisher: IOP Publishing</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/0953-8984/26/50/505401\"\n     onclick=\"log_download('mikheykin-torgashev-talanov-bush-chernyshov-yuzyuk-dmitriev-highpressurexraydiffractionstudyofnickelcopperchromitessolidsolutions-2014', 'https://dx.doi.org/10.1088/0953-8984/26/50/505401', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"High pressure x-ray diffraction study of nickel–copper chromites solid solutions [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/0953-8984/26/50/505401\"\n     onclick=\"log_download('mikheykin-torgashev-talanov-bush-chernyshov-yuzyuk-dmitriev-highpressurexraydiffractionstudyofnickelcopperchromitessolidsolutions-2014', 'http://doi.org/10.1088/0953-8984/26/50/505401', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/mikheykin-torgashev-talanov-bush-chernyshov-yuzyuk-dmitriev-highpressurexraydiffractionstudyofnickelcopperchromitessolidsolutions-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('mikheykin-torgashev-talanov-bush-chernyshov-yuzyuk-dmitriev-highpressurexraydiffractionstudyofnickelcopperchromitessolidsolutions-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{mikheykin_high_2014,\n\ttitle = {High pressure x-ray diffraction study of nickel–copper chromites solid solutions},\n\tvolume = {26},\n\tissn = {0953-8984},\n\turl = {https://dx.doi.org/10.1088/0953-8984/26/50/505401},\n\tdoi = {10.1088/0953-8984/26/50/505401},\n\tabstract = {A high-pressure synchrotron radiation diffraction study has been carried out on Ni1−xCuxCr2O4 solid solutions. Observed pressure-controlled phase transitions, along with data previously collected for temperature-induced phase transitions, are analyzed in the framework of the unified phenomenological model that results in mapping of the generic phase diagram for the whole family of Ni1−xCuxCr2O4 solid solutions.},\n\tlanguage = {en},\n\tnumber = {50},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics: Condensed Matter},\n\tauthor = {Mikheykin, A. S. and Torgashev, V. I. and Talanov, V. M. and Bush, A. A. and Chernyshov, D. and Yuzyuk, I. Yu and Dmitriev, V. P.},\n\tmonth = nov,\n\tyear = {2014},\n\tnote = {Publisher: IOP Publishing},\n\tpages = {505401},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A high-pressure synchrotron radiation diffraction study has been carried out on Ni1−xCuxCr2O4 solid solutions. Observed pressure-controlled phase transitions, along with data previously collected for temperature-induced phase transitions, are analyzed in the framework of the unified phenomenological model that results in mapping of the generic phase diagram for the whole family of Ni1−xCuxCr2O4 solid solutions.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"zhilin-lyanguzov-nikolaev-pushkariov-kaidashev-photoelectricpropertiesofmsmstructurebasedonznonanorodsreceivedbythermalevaporationandcarbothermalsyntesis-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/541/1/012038\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'zhilin-lyanguzov-nikolaev-pushkariov-kaidashev-photoelectricpropertiesofmsmstructurebasedonznonanorodsreceivedbythermalevaporationandcarbothermalsyntesis-2014', 'https://dx.doi.org/10.1088/1742-6596/541/1/012038', event);\">\n    Photoelectric properties of MSM structure based on ZnO nanorods, received by thermal evaporation and carbothermal syntesis.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Zhilin, D. A.; Lyanguzov, N. V.; Nikolaev, L. A.; Pushkariov, V. I.;  and Kaidashev, E. M.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics: Conference Series</i>, 541(1): 012038. October 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/541/1/012038\"\n     onclick=\"log_download('zhilin-lyanguzov-nikolaev-pushkariov-kaidashev-photoelectricpropertiesofmsmstructurebasedonznonanorodsreceivedbythermalevaporationandcarbothermalsyntesis-2014', 'https://dx.doi.org/10.1088/1742-6596/541/1/012038', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Photoelectric properties of MSM structure based on ZnO nanorods, received by thermal evaporation and carbothermal syntesis [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/1742-6596/541/1/012038\"\n     onclick=\"log_download('zhilin-lyanguzov-nikolaev-pushkariov-kaidashev-photoelectricpropertiesofmsmstructurebasedonznonanorodsreceivedbythermalevaporationandcarbothermalsyntesis-2014', 'http://doi.org/10.1088/1742-6596/541/1/012038', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/zhilin-lyanguzov-nikolaev-pushkariov-kaidashev-photoelectricpropertiesofmsmstructurebasedonznonanorodsreceivedbythermalevaporationandcarbothermalsyntesis-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('zhilin-lyanguzov-nikolaev-pushkariov-kaidashev-photoelectricpropertiesofmsmstructurebasedonznonanorodsreceivedbythermalevaporationandcarbothermalsyntesis-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{zhilin_photoelectric_2014,\n\ttitle = {Photoelectric properties of {MSM} structure based on {ZnO} nanorods, received by thermal evaporation and carbothermal syntesis},\n\tvolume = {541},\n\tissn = {1742-6596},\n\turl = {https://dx.doi.org/10.1088/1742-6596/541/1/012038},\n\tdoi = {10.1088/1742-6596/541/1/012038},\n\tabstract = {Photoelectric characteristics of metal-semiconductor-metal (MSM) structures: Au/ZnO(nanorods)/ZnO(film)/ZnO(nanorods)/Au were investigated. Synthesis of ZnO nanorods (NR&#x27;s) was carried out by two different methods, such as catalyst-free carbothermal synthesis (t = 950°C, precursor – ZnO:C) and catalyst-free thermal evaporation of metallic Zn (t = 600°C, precursor Zn). Photoluminescence spectra have shown that the ZnO NR&#x27;s obtained by means of thermal evaporation technique have a lower concentration of point defects related with oxygen vacancies, than ZnO NR&#x27;s prepared by carbothermal synthesis. MSM structure with ZnO NR&#x27;s obtained by thermal evaporation technique have photosensitivity 97 mA/W at 325 nm illumination and 44 mA/W at 518 nm illumination at a bias 5V. For MSM structure with ZnO NR&#x27;s obtained by method of carbothermal synthesis, the photosensitivity values were 22 mA/W, and 103 mA/W, respectively.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics: Conference Series},\n\tauthor = {Zhilin, D. A. and Lyanguzov, N. V. and Nikolaev, L. A. and Pushkariov, V. I. and Kaidashev, E. M.},\n\tmonth = oct,\n\tyear = {2014},\n\tpages = {012038},\n\tfile = {IOP Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\49KV5PK9\\\\Zhilin и др. - 2014 - Photoelectric properties of MSM structure based on.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Photoelectric characteristics of metal-semiconductor-metal (MSM) structures: Au/ZnO(nanorods)/ZnO(film)/ZnO(nanorods)/Au were investigated. Synthesis of ZnO nanorods (NR's) was carried out by two different methods, such as catalyst-free carbothermal synthesis (t = 950°C, precursor – ZnO:C) and catalyst-free thermal evaporation of metallic Zn (t = 600°C, precursor Zn). Photoluminescence spectra have shown that the ZnO NR's obtained by means of thermal evaporation technique have a lower concentration of point defects related with oxygen vacancies, than ZnO NR's prepared by carbothermal synthesis. MSM structure with ZnO NR's obtained by thermal evaporation technique have photosensitivity 97 mA/W at 325 nm illumination and 44 mA/W at 518 nm illumination at a bias 5V. For MSM structure with ZnO NR's obtained by method of carbothermal synthesis, the photosensitivity values were 22 mA/W, and 103 mA/W, respectively.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"talanov-shirokov-talanov-combinedatomicorderingintheaandbsublatticesofperovskitestructure-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1063774514050198\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'talanov-shirokov-talanov-combinedatomicorderingintheaandbsublatticesofperovskitestructure-2014', 'https://doi.org/10.1134/S1063774514050198', event);\">\n    Combined atomic ordering in the A and B sublattices of perovskite structure.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Talanov, M. V.; Shirokov, V. B.;  and Talanov, V. M.\n</span>\n\n  \n\n</span>\n\n  <i>Crystallography Reports</i>, 59(5): 662–678. September 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1063774514050198\"\n     onclick=\"log_download('talanov-shirokov-talanov-combinedatomicorderingintheaandbsublatticesofperovskitestructure-2014', 'https://doi.org/10.1134/S1063774514050198', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Combined atomic ordering in the A and B sublattices of perovskite structure [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1063774514050198\"\n     onclick=\"log_download('talanov-shirokov-talanov-combinedatomicorderingintheaandbsublatticesofperovskitestructure-2014', 'http://doi.org/10.1134/S1063774514050198', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/talanov-shirokov-talanov-combinedatomicorderingintheaandbsublatticesofperovskitestructure-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('talanov-shirokov-talanov-combinedatomicorderingintheaandbsublatticesofperovskitestructure-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{talanov_combined_2014,\n\ttitle = {Combined atomic ordering in the {A} and {B} sublattices of perovskite structure},\n\tvolume = {59},\n\tissn = {1562-689X},\n\turl = {https://doi.org/10.1134/S1063774514050198},\n\tdoi = {10.1134/S1063774514050198},\n\tabstract = {The simultaneous ordering of cations in the A and B sublattices of cubic perovskite structure has been investigated by the group-theoretical method. It is found that 147 ordered phases may exist. Among them, there may be 121 phases with simultaneous cation ordering in the 1(a)- and 1(c) positions of perovskite structure. It is shown that 53 phases are described by improper order parameters related to cation ordering, the formation of 56 phases is related to improper rotations of octahedra, and 15 phases are improper ferroelectrics. Calculated structures of some types of ordered low-symmetry perovskite modifications are presented.},\n\tlanguage = {en},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Crystallography Reports},\n\tauthor = {Talanov, M. V. and Shirokov, V. B. and Talanov, V. M.},\n\tmonth = sep,\n\tyear = {2014},\n\tkeywords = {Crystallography Report, Group Theoretical Method, Permutation Representation, Perovskite, Perovskite Structure},\n\tpages = {662--678},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The simultaneous ordering of cations in the A and B sublattices of cubic perovskite structure has been investigated by the group-theoretical method. It is found that 147 ordered phases may exist. Among them, there may be 121 phases with simultaneous cation ordering in the 1(a)- and 1(c) positions of perovskite structure. It is shown that 53 phases are described by improper order parameters related to cation ordering, the formation of 56 phases is related to improper rotations of octahedra, and 15 phases are improper ferroelectrics. Calculated structures of some types of ordered low-symmetry perovskite modifications are presented.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"talanov-talanov-shirokov-grouptheoreticalstudyofcationicorderinginperovskitestructure-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1063774514050186\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'talanov-talanov-shirokov-grouptheoreticalstudyofcationicorderinginperovskitestructure-2014', 'https://doi.org/10.1134/S1063774514050186', event);\">\n    Group-theoretical study of cationic ordering in perovskite structure.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Talanov, V. M.; Talanov, M. V.;  and Shirokov, V. B.\n</span>\n\n  \n\n</span>\n\n  <i>Crystallography Reports</i>, 59(5): 650–661. September 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1063774514050186\"\n     onclick=\"log_download('talanov-talanov-shirokov-grouptheoreticalstudyofcationicorderinginperovskitestructure-2014', 'https://doi.org/10.1134/S1063774514050186', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Group-theoretical study of cationic ordering in perovskite structure [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1063774514050186\"\n     onclick=\"log_download('talanov-talanov-shirokov-grouptheoreticalstudyofcationicorderinginperovskitestructure-2014', 'http://doi.org/10.1134/S1063774514050186', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/talanov-talanov-shirokov-grouptheoreticalstudyofcationicorderinginperovskitestructure-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('talanov-talanov-shirokov-grouptheoreticalstudyofcationicorderinginperovskitestructure-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{talanov_group-theoretical_2014,\n\ttitle = {Group-theoretical study of cationic ordering in perovskite structure},\n\tvolume = {59},\n\tissn = {1562-689X},\n\turl = {https://doi.org/10.1134/S1063774514050186},\n\tdoi = {10.1134/S1063774514050186},\n\tabstract = {Atomic ordering in the structure of cubic perovskite has been investigated by the group-theoretical method. The possibility of existence of 13 ordered phases in the 1(a) position (including four binary, two ternary, and five quaternary cationic superstructures) and 13 phases with different types of ordering in the 1(b) position (including four binary, two ternary, and five quaternary cationic superstructures) is established. Calculated structures of some types of ordered low-symmetry perovskite modifications are reported.},\n\tlanguage = {en},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Crystallography Reports},\n\tauthor = {Talanov, V. M. and Talanov, M. V. and Shirokov, V. B.},\n\tmonth = sep,\n\tyear = {2014},\n\tkeywords = {Crystallography Report, Perovskite, Perovskite Structure, CaCu, Central Atom},\n\tpages = {650--661},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Atomic ordering in the structure of cubic perovskite has been investigated by the group-theoretical method. The possibility of existence of 13 ordered phases in the 1(a) position (including four binary, two ternary, and five quaternary cationic superstructures) and 13 phases with different types of ordering in the 1(b) position (including four binary, two ternary, and five quaternary cationic superstructures) is established. Calculated structures of some types of ordered low-symmetry perovskite modifications are reported.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"timoshenko-babichev-vyatkina-scatteringofmagnetostaticwavesbydefectsofthesurfaceofaferromagneticfilm-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://ieeexplore.ieee.org/document/6958761\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'timoshenko-babichev-vyatkina-scatteringofmagnetostaticwavesbydefectsofthesurfaceofaferromagneticfilm-2014', 'https://ieeexplore.ieee.org/document/6958761', event);\">\n    Scattering of magnetostatic waves by defects of the surface of a ferromagnetic film.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Timoshenko, P. E.; Babichev, R. K.;  and Vyatkina, S. A.\n</span>\n\n  \n\n</span>\n\n  In <i>2014 International Conference on Actual Problems of Electron Devices Engineering (APEDE)</i>, volume 1, pages 279–283, September 2014. \n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://ieeexplore.ieee.org/document/6958761\"\n     onclick=\"log_download('timoshenko-babichev-vyatkina-scatteringofmagnetostaticwavesbydefectsofthesurfaceofaferromagneticfilm-2014', 'https://ieeexplore.ieee.org/document/6958761', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Scattering of magnetostatic waves by defects of the surface of a ferromagnetic film [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1109/APEDE.2014.6958761\"\n     onclick=\"log_download('timoshenko-babichev-vyatkina-scatteringofmagnetostaticwavesbydefectsofthesurfaceofaferromagneticfilm-2014', 'http://doi.org/10.1109/APEDE.2014.6958761', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/timoshenko-babichev-vyatkina-scatteringofmagnetostaticwavesbydefectsofthesurfaceofaferromagneticfilm-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('timoshenko-babichev-vyatkina-scatteringofmagnetostaticwavesbydefectsofthesurfaceofaferromagneticfilm-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{timoshenko_scattering_2014,\n\ttitle = {Scattering of magnetostatic waves by defects of the surface of a ferromagnetic film},\n\tvolume = {1},\n\turl = {https://ieeexplore.ieee.org/document/6958761},\n\tdoi = {10.1109/APEDE.2014.6958761},\n\tabstract = {The solution for the diffraction problem of scattering of magnetostatic waves by an arbitrary shallow defect situated under the surface of a ferromagnetic film magnetized at an arbitrary angle is obtained in the quasi-static approximation. Expressions for the energy flux density of scattered magnetostatic waves in the far-field zone are found.},\n\turldate = {2023-11-11},\n\tbooktitle = {2014 {International} {Conference} on {Actual} {Problems} of {Electron} {Devices} {Engineering} ({APEDE})},\n\tauthor = {Timoshenko, P. E. and Babichev, R. K. and Vyatkina, S. A.},\n\tmonth = sep,\n\tyear = {2014},\n\tpages = {279--283},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The solution for the diffraction problem of scattering of magnetostatic waves by an arbitrary shallow defect situated under the surface of a ferromagnetic film magnetized at an arbitrary angle is obtained in the quasi-static approximation. Expressions for the energy flux density of scattered magnetostatic waves in the far-field zone are found.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"timoshenko-kalinchuk-shirokov-levi-pankin-donets-finiteelementsimulationofsurfaceacousticwavesexcitedinbariumstrontiumtitanatefilmsfabricatedonmagnesiumoxidesubstratebyinterdigitaltransducers-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://ieeexplore.ieee.org/document/6958762\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'timoshenko-kalinchuk-shirokov-levi-pankin-donets-finiteelementsimulationofsurfaceacousticwavesexcitedinbariumstrontiumtitanatefilmsfabricatedonmagnesiumoxidesubstratebyinterdigitaltransducers-2014', 'https://ieeexplore.ieee.org/document/6958762', event);\">\n    Finite element simulation of surface acoustic waves excited in barium-strontium titanate films fabricated on magnesium oxide substrate by interdigital transducers.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Timoshenko, P. E.; Kalinchuk, V. V.; Shirokov, V. B.; Levi, M. O.; Pan'kin, A. V.;  and Donets, A. V.\n</span>\n\n  \n\n</span>\n\n  In <i>2014 International Conference on Actual Problems of Electron Devices Engineering (APEDE)</i>, volume 1, pages 283–289, September 2014. \n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://ieeexplore.ieee.org/document/6958762\"\n     onclick=\"log_download('timoshenko-kalinchuk-shirokov-levi-pankin-donets-finiteelementsimulationofsurfaceacousticwavesexcitedinbariumstrontiumtitanatefilmsfabricatedonmagnesiumoxidesubstratebyinterdigitaltransducers-2014', 'https://ieeexplore.ieee.org/document/6958762', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Finite element simulation of surface acoustic waves excited in barium-strontium titanate films fabricated on magnesium oxide substrate by interdigital transducers [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1109/APEDE.2014.6958762\"\n     onclick=\"log_download('timoshenko-kalinchuk-shirokov-levi-pankin-donets-finiteelementsimulationofsurfaceacousticwavesexcitedinbariumstrontiumtitanatefilmsfabricatedonmagnesiumoxidesubstratebyinterdigitaltransducers-2014', 'http://doi.org/10.1109/APEDE.2014.6958762', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/timoshenko-kalinchuk-shirokov-levi-pankin-donets-finiteelementsimulationofsurfaceacousticwavesexcitedinbariumstrontiumtitanatefilmsfabricatedonmagnesiumoxidesubstratebyinterdigitaltransducers-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('timoshenko-kalinchuk-shirokov-levi-pankin-donets-finiteelementsimulationofsurfaceacousticwavesexcitedinbariumstrontiumtitanatefilmsfabricatedonmagnesiumoxidesubstratebyinterdigitaltransducers-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{timoshenko_finite_2014,\n\ttitle = {Finite element simulation of surface acoustic waves excited in barium-strontium titanate films fabricated on magnesium oxide substrate by interdigital transducers},\n\tvolume = {1},\n\turl = {https://ieeexplore.ieee.org/document/6958762},\n\tdoi = {10.1109/APEDE.2014.6958762},\n\tabstract = {In this paper, we present study on surface acoustic waves excited in barium — strontium titanate films fabricated on magnesium oxide substrate by interdigital transducers. The surface acoustic waves propagation was simulated by using COMSOL Multiphysics™. The presence of bias, since the oscillations are not considered as sagittal polarized, is the principal difference between considered problem and standard problem that implemented in many finite element packages. The calculations of mechanic displacement and electric field potential for the first Eigen frequencies for different planes are shown. The methods of modeling in COMSOL Multiphysics™ software package are presented in this paper can be used for calculations of other systems that have different complex configuration.},\n\turldate = {2023-11-11},\n\tbooktitle = {2014 {International} {Conference} on {Actual} {Problems} of {Electron} {Devices} {Engineering} ({APEDE})},\n\tauthor = {Timoshenko, P. E. and Kalinchuk, V. V. and Shirokov, V. B. and Levi, M. O. and Pan&#x27;kin, A. V. and Donets, A. V.},\n\tmonth = sep,\n\tyear = {2014},\n\tpages = {283--289},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  In this paper, we present study on surface acoustic waves excited in barium — strontium titanate films fabricated on magnesium oxide substrate by interdigital transducers. The surface acoustic waves propagation was simulated by using COMSOL Multiphysics™. The presence of bias, since the oscillations are not considered as sagittal polarized, is the principal difference between considered problem and standard problem that implemented in many finite element packages. The calculations of mechanic displacement and electric field potential for the first Eigen frequencies for different planes are shown. The methods of modeling in COMSOL Multiphysics™ software package are presented in this paper can be used for calculations of other systems that have different complex configuration.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"pushkariov-nikolaev-kaidashev-synthesisandcharacterizationofznonanorodsobtainedbycatalystfreethermaltechnique-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/541/1/012031\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'pushkariov-nikolaev-kaidashev-synthesisandcharacterizationofznonanorodsobtainedbycatalystfreethermaltechnique-2014', 'https://dx.doi.org/10.1088/1742-6596/541/1/012031', event);\">\n    Synthesis and characterization of ZnO nanorods obtained by catalyst-free thermal technique.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Pushkariov, V. I.; Nikolaev, A. L.;  and Kaidashev, E. M.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics: Conference Series</i>, 541(1): 012031. October 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/541/1/012031\"\n     onclick=\"log_download('pushkariov-nikolaev-kaidashev-synthesisandcharacterizationofznonanorodsobtainedbycatalystfreethermaltechnique-2014', 'https://dx.doi.org/10.1088/1742-6596/541/1/012031', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Synthesis and characterization of ZnO nanorods obtained by catalyst-free thermal technique [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/1742-6596/541/1/012031\"\n     onclick=\"log_download('pushkariov-nikolaev-kaidashev-synthesisandcharacterizationofznonanorodsobtainedbycatalystfreethermaltechnique-2014', 'http://doi.org/10.1088/1742-6596/541/1/012031', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/pushkariov-nikolaev-kaidashev-synthesisandcharacterizationofznonanorodsobtainedbycatalystfreethermaltechnique-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('pushkariov-nikolaev-kaidashev-synthesisandcharacterizationofznonanorodsobtainedbycatalystfreethermaltechnique-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{pushkariov_synthesis_2014,\n\ttitle = {Synthesis and characterization of {ZnO} nanorods obtained by catalyst-free thermal technique},\n\tvolume = {541},\n\tissn = {1742-6596},\n\turl = {https://dx.doi.org/10.1088/1742-6596/541/1/012031},\n\tdoi = {10.1088/1742-6596/541/1/012031},\n\tabstract = {ZnO nanorod arrays have been synthesized on silicon wafers by catalyst free thermal vapor deposition with different temperature values. Vertical-aligned ZnO nanostructures were grown at the quite low temperatures by this method. Modification of the method allowed to place silicon substrates in areas with different ratios of concentrations Ar and O2 molecules in the vapor phase. Photoluminescence spectroscopy and electron microscopy studies have shown that morphologies and optical properties of nanorods depends on different ratios of concentrations of the molecules in the vapor phase.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics: Conference Series},\n\tauthor = {Pushkariov, V. I. and Nikolaev, A. L. and Kaidashev, E. M.},\n\tmonth = oct,\n\tyear = {2014},\n\tpages = {012031},\n\tfile = {IOP Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\7WR58HGN\\\\Pushkariov и др. - 2014 - Synthesis and characterization of ZnO nanorods obt.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  ZnO nanorod arrays have been synthesized on silicon wafers by catalyst free thermal vapor deposition with different temperature values. Vertical-aligned ZnO nanostructures were grown at the quite low temperatures by this method. Modification of the method allowed to place silicon substrates in areas with different ratios of concentrations Ar and O2 molecules in the vapor phase. Photoluminescence spectroscopy and electron microscopy studies have shown that morphologies and optical properties of nanorods depends on different ratios of concentrations of the molecules in the vapor phase.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"puzikov-lyanguzov-kaidashev-pulsedlaserdepositionandinvestigationofantimonydopedznofilms-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/541/1/012004\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'puzikov-lyanguzov-kaidashev-pulsedlaserdepositionandinvestigationofantimonydopedznofilms-2014', 'https://dx.doi.org/10.1088/1742-6596/541/1/012004', event);\">\n    Pulsed laser deposition and investigation of antimony-doped ZnO films.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Puzikov, A. S.; Lyanguzov, N. V.;  and Kaidashev, E. M.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics: Conference Series</i>, 541(1): 012004. October 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/541/1/012004\"\n     onclick=\"log_download('puzikov-lyanguzov-kaidashev-pulsedlaserdepositionandinvestigationofantimonydopedznofilms-2014', 'https://dx.doi.org/10.1088/1742-6596/541/1/012004', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Pulsed laser deposition and investigation of antimony-doped ZnO films [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/1742-6596/541/1/012004\"\n     onclick=\"log_download('puzikov-lyanguzov-kaidashev-pulsedlaserdepositionandinvestigationofantimonydopedznofilms-2014', 'http://doi.org/10.1088/1742-6596/541/1/012004', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/puzikov-lyanguzov-kaidashev-pulsedlaserdepositionandinvestigationofantimonydopedznofilms-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('puzikov-lyanguzov-kaidashev-pulsedlaserdepositionandinvestigationofantimonydopedznofilms-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{puzikov_pulsed_2014,\n\ttitle = {Pulsed laser deposition and investigation of antimony-doped {ZnO} films},\n\tvolume = {541},\n\tissn = {1742-6596},\n\turl = {https://dx.doi.org/10.1088/1742-6596/541/1/012004},\n\tdoi = {10.1088/1742-6596/541/1/012004},\n\tabstract = {We have investigated the influence of oxygen partial pressure, temperature of synthesis and annealing conditions on nanocsrystallineSb-doped thin films, grown by pulsed laser deposition. It is shown that the minimum resistivity ( 8·10−3Ω·cm) and the maximum carriers density ( 2·1019 cm-3) corresponds to the pressure range 5·10−3-7·10−3 mbar, to the temperature 550 ° C and in situ annealing at 700 °C.Also we show the features of the crystal lattice&#x27;s dynamics, which are found in the Raman research.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics: Conference Series},\n\tauthor = {Puzikov, A. S. and Lyanguzov, N. V. and Kaidashev, E. M.},\n\tmonth = oct,\n\tyear = {2014},\n\tpages = {012004},\n\tfile = {IOP Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\H6J3GSQ8\\\\Puzikov и др. - 2014 - Pulsed laser deposition and investigation of antim.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We have investigated the influence of oxygen partial pressure, temperature of synthesis and annealing conditions on nanocsrystallineSb-doped thin films, grown by pulsed laser deposition. It is shown that the minimum resistivity ( 8·10−3Ω·cm) and the maximum carriers density ( 2·1019 cm-3) corresponds to the pressure range 5·10−3-7·10−3 mbar, to the temperature 550 ° C and in situ annealing at 700 °C.Also we show the features of the crystal lattice's dynamics, which are found in the Raman research.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"nistratov-vyatkina-babichev-timoshenko-experimentalinvestigationofmagnetostaticbackwardvolumewavesexcitedbythenarrowtransducer-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://ieeexplore.ieee.org/document/6958745\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'nistratov-vyatkina-babichev-timoshenko-experimentalinvestigationofmagnetostaticbackwardvolumewavesexcitedbythenarrowtransducer-2014', 'https://ieeexplore.ieee.org/document/6958745', event);\">\n    Experimental investigation of magnetostatic backward volume waves excited by the narrow transducer.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Nistratov, N. P.; Vyatkina, S. A.; Babichev, R. K.;  and Timoshenko, P. E.\n</span>\n\n  \n\n</span>\n\n  In <i>2014 International Conference on Actual Problems of Electron Devices Engineering (APEDE)</i>, volume 1, pages 199–204, September 2014. \n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://ieeexplore.ieee.org/document/6958745\"\n     onclick=\"log_download('nistratov-vyatkina-babichev-timoshenko-experimentalinvestigationofmagnetostaticbackwardvolumewavesexcitedbythenarrowtransducer-2014', 'https://ieeexplore.ieee.org/document/6958745', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Experimental investigation of magnetostatic backward volume waves excited by the narrow transducer [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1109/APEDE.2014.6958745\"\n     onclick=\"log_download('nistratov-vyatkina-babichev-timoshenko-experimentalinvestigationofmagnetostaticbackwardvolumewavesexcitedbythenarrowtransducer-2014', 'http://doi.org/10.1109/APEDE.2014.6958745', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/nistratov-vyatkina-babichev-timoshenko-experimentalinvestigationofmagnetostaticbackwardvolumewavesexcitedbythenarrowtransducer-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('nistratov-vyatkina-babichev-timoshenko-experimentalinvestigationofmagnetostaticbackwardvolumewavesexcitedbythenarrowtransducer-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{nistratov_experimental_2014,\n\ttitle = {Experimental investigation of magnetostatic backward volume waves excited by the narrow transducer},\n\tvolume = {1},\n\turl = {https://ieeexplore.ieee.org/document/6958745},\n\tdoi = {10.1109/APEDE.2014.6958745},\n\tabstract = {The results of experimental investigation of diffraction profiles of magnetostatic backward volume waves (MSBVW) exited by the linear transducer with finite length located at the surface of ferrite-dielectric structure are presented. The comparison of experimental data obtained and theoretical calculations is reported.},\n\turldate = {2023-11-11},\n\tbooktitle = {2014 {International} {Conference} on {Actual} {Problems} of {Electron} {Devices} {Engineering} ({APEDE})},\n\tauthor = {Nistratov, N. P. and Vyatkina, S. A. and Babichev, R. K. and Timoshenko, P. E.},\n\tmonth = sep,\n\tyear = {2014},\n\tpages = {199--204},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The results of experimental investigation of diffraction profiles of magnetostatic backward volume waves (MSBVW) exited by the linear transducer with finite length located at the surface of ferrite-dielectric structure are presented. The comparison of experimental data obtained and theoretical calculations is reported.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"zhukova-torgashev-gorshunov-lebedev-shakurov-kremer-pestrjakov-thomas-etal-vibrationalstatesofawatermoleculeinananocavityofberylcrystallattice-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.4882062\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'zhukova-torgashev-gorshunov-lebedev-shakurov-kremer-pestrjakov-thomas-etal-vibrationalstatesofawatermoleculeinananocavityofberylcrystallattice-2014', 'https://doi.org/10.1063/1.4882062', event);\">\n    Vibrational states of a water molecule in a nano-cavity of beryl crystal lattice.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Zhukova, E. S.; Torgashev, V. I.; Gorshunov, B. P.; Lebedev, V. V.; Shakurov, G. S.; Kremer, R. K.; Pestrjakov, E. V.; Thomas, V. G.; Fursenko, D. A.; Prokhorov, A. S.;  and Dressel, M.\n</span>\n\n  \n\n</span>\n\n  <i>The Journal of Chemical Physics</i>, 140(22): 224317. June 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.4882062\"\n     onclick=\"log_download('zhukova-torgashev-gorshunov-lebedev-shakurov-kremer-pestrjakov-thomas-etal-vibrationalstatesofawatermoleculeinananocavityofberylcrystallattice-2014', 'https://doi.org/10.1063/1.4882062', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Vibrational states of a water molecule in a nano-cavity of beryl crystal lattice [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.4882062\"\n     onclick=\"log_download('zhukova-torgashev-gorshunov-lebedev-shakurov-kremer-pestrjakov-thomas-etal-vibrationalstatesofawatermoleculeinananocavityofberylcrystallattice-2014', 'http://doi.org/10.1063/1.4882062', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/zhukova-torgashev-gorshunov-lebedev-shakurov-kremer-pestrjakov-thomas-etal-vibrationalstatesofawatermoleculeinananocavityofberylcrystallattice-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('zhukova-torgashev-gorshunov-lebedev-shakurov-kremer-pestrjakov-thomas-etal-vibrationalstatesofawatermoleculeinananocavityofberylcrystallattice-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{zhukova_vibrational_2014,\n\ttitle = {Vibrational states of a water molecule in a nano-cavity of beryl crystal lattice},\n\tvolume = {140},\n\tissn = {0021-9606},\n\turl = {https://doi.org/10.1063/1.4882062},\n\tdoi = {10.1063/1.4882062},\n\tabstract = {Low-energy excitations of a single water molecule are studied when confined within a nano-size cavity formed by the ionic crystal lattice. Optical spectra are measured of manganese doped beryl single crystal Mn:Be3Al2Si6O18, that contains water molecules individually isolated in 0.51 nm diameter voids within the crystal lattice. Two types of orientation are distinguished: water-I molecules have their dipole moments aligned perpendicular to the c axis and dipole moments of water-II molecules are parallel to the c-axis. The optical conductivity σ(ν) and permittivity ɛ′(ν) spectra are recorded in terahertz and infrared ranges, at frequencies from several wavenumbers up to ν = 7000 cm−1, at temperatures 5–300 K and for two polarizations, when the electric vector E of the radiation is parallel and perpendicular to the c-axis. Comparative experiments on as-grown and on dehydrated samples allow to identify the spectra of σ(ν) and ɛ′(ν) caused exclusively by water molecules. In the infrared range, well-known internal modes ν1, ν2, and ν3 of the H2O molecule are observed for both polarizations, indicating the presence of water-I and water-II molecules in the crystal. Spectra recorded below 1000 cm−1 reveal a rich set of highly anisotropic features in the low-energy response of H2O molecule in a crystalline nano-cavity. While for E∥c only two absorption peaks are detected, at ∼90 cm−1 and ∼160 cm−1, several absorption bands are discovered for E⊥c, each consisting of narrower resonances. The bands are assigned to librational (400–500 cm−1) and translational (150–200 cm−1) vibrations of water-I molecule that is weakly coupled to the nano-cavity “walls.” A model is presented that explains the “fine structure” of the bands by a splitting of the energy levels due to quantum tunneling between the minima in a six-well potential relief felt by a molecule within the cavity.},\n\tnumber = {22},\n\turldate = {2023-11-11},\n\tjournal = {The Journal of Chemical Physics},\n\tauthor = {Zhukova, Elena S. and Torgashev, Victor I. and Gorshunov, Boris P. and Lebedev, Vladimir V. and Shakurov, Gil&#x27;man S. and Kremer, Reinhard K. and Pestrjakov, Efim V. and Thomas, Victor G. and Fursenko, Dimitry A. and Prokhorov, Anatoly S. and Dressel, Martin},\n\tmonth = jun,\n\tyear = {2014},\n\tpages = {224317},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\776RNGVS\\\\Zhukova и др. - 2014 - Vibrational states of a water molecule in a nano-c.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Low-energy excitations of a single water molecule are studied when confined within a nano-size cavity formed by the ionic crystal lattice. Optical spectra are measured of manganese doped beryl single crystal Mn:Be3Al2Si6O18, that contains water molecules individually isolated in 0.51 nm diameter voids within the crystal lattice. Two types of orientation are distinguished: water-I molecules have their dipole moments aligned perpendicular to the c axis and dipole moments of water-II molecules are parallel to the c-axis. The optical conductivity σ(ν) and permittivity ɛ′(ν) spectra are recorded in terahertz and infrared ranges, at frequencies from several wavenumbers up to ν = 7000 cm−1, at temperatures 5–300 K and for two polarizations, when the electric vector E of the radiation is parallel and perpendicular to the c-axis. Comparative experiments on as-grown and on dehydrated samples allow to identify the spectra of σ(ν) and ɛ′(ν) caused exclusively by water molecules. In the infrared range, well-known internal modes ν1, ν2, and ν3 of the H2O molecule are observed for both polarizations, indicating the presence of water-I and water-II molecules in the crystal. Spectra recorded below 1000 cm−1 reveal a rich set of highly anisotropic features in the low-energy response of H2O molecule in a crystalline nano-cavity. While for E∥c only two absorption peaks are detected, at ∼90 cm−1 and ∼160 cm−1, several absorption bands are discovered for E⊥c, each consisting of narrower resonances. The bands are assigned to librational (400–500 cm−1) and translational (150–200 cm−1) vibrations of water-I molecule that is weakly coupled to the nano-cavity “walls.” A model is presented that explains the “fine structure” of the bands by a splitting of the energy levels due to quantum tunneling between the minima in a six-well potential relief felt by a molecule within the cavity.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"leontyev-kuriganova-leontyev-hennet-rakhmatullin-smirnova-dmitriev-sizedependenceofthelatticeparametersofcarbonsupportedplatinumnanoparticlesxraydiffractionanalysisandtheoreticalconsiderations-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://pubs.rsc.org/en/content/articlelanding/2014/ra/c4ra04809a\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'leontyev-kuriganova-leontyev-hennet-rakhmatullin-smirnova-dmitriev-sizedependenceofthelatticeparametersofcarbonsupportedplatinumnanoparticlesxraydiffractionanalysisandtheoreticalconsiderations-2014', 'https://pubs.rsc.org/en/content/articlelanding/2014/ra/c4ra04809a', event);\">\n    Size dependence of the lattice parameters of carbon supported platinum nanoparticles: X-ray diffraction analysis and theoretical considerations.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Leontyev, I. N.; Kuriganova, A. B.; Leontyev, N. G.; Hennet, L.; Rakhmatullin, A.; Smirnova, N. V.;  and Dmitriev, V.\n</span>\n\n  \n\n</span>\n\n  <i>RSC Advances</i>, 4(68): 35959–35965. August 2014.\n  <span class=\"note\">Publisher: The Royal Society of Chemistry</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://pubs.rsc.org/en/content/articlelanding/2014/ra/c4ra04809a\"\n     onclick=\"log_download('leontyev-kuriganova-leontyev-hennet-rakhmatullin-smirnova-dmitriev-sizedependenceofthelatticeparametersofcarbonsupportedplatinumnanoparticlesxraydiffractionanalysisandtheoreticalconsiderations-2014', 'https://pubs.rsc.org/en/content/articlelanding/2014/ra/c4ra04809a', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Size dependence of the lattice parameters of carbon supported platinum nanoparticles: X-ray diffraction analysis and theoretical considerations [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1039/C4RA04809A\"\n     onclick=\"log_download('leontyev-kuriganova-leontyev-hennet-rakhmatullin-smirnova-dmitriev-sizedependenceofthelatticeparametersofcarbonsupportedplatinumnanoparticlesxraydiffractionanalysisandtheoreticalconsiderations-2014', 'http://doi.org/10.1039/C4RA04809A', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/leontyev-kuriganova-leontyev-hennet-rakhmatullin-smirnova-dmitriev-sizedependenceofthelatticeparametersofcarbonsupportedplatinumnanoparticlesxraydiffractionanalysisandtheoreticalconsiderations-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('leontyev-kuriganova-leontyev-hennet-rakhmatullin-smirnova-dmitriev-sizedependenceofthelatticeparametersofcarbonsupportedplatinumnanoparticlesxraydiffractionanalysisandtheoreticalconsiderations-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{leontyev_size_2014,\n\ttitle = {Size dependence of the lattice parameters of carbon supported platinum nanoparticles: {X}-ray diffraction analysis and theoretical considerations},\n\tvolume = {4},\n\tissn = {2046-2069},\n\tshorttitle = {Size dependence of the lattice parameters of carbon supported platinum nanoparticles},\n\turl = {https://pubs.rsc.org/en/content/articlelanding/2014/ra/c4ra04809a},\n\tdoi = {10.1039/C4RA04809A},\n\tabstract = {Carbon supported Pt nanoparticles with diameters ranging from 2 to 28 nm have been studied using X-ray diffraction. The unit cell parameter of synthesized Pt/C nanoparticles is always lower than that of bulk Pt. By decreasing the average particle size D to approximately 2 nm, the unit cell parameter a nonlinearly decreases by about 0.03 Å which corresponds to a variation of 0.7\\% in comparison to bulk Pt, and the size effect is predominant for sizes ranging from 2 to 10 nm. The dependence a(1/D) is approximated well using a straight line with a slope of −0.0555 ± 0.0067 nm−1 and an intercept of −3.9230 ± 0.0017 Å. For interpreting the obtained experimental dependence of the unit cell parameter of Pt/C nanoparticles, four different theoretical approaches such as the thermal vacancy mechanism, continuous-medium model, Laplace pressure, and bond order–length–strength correlation mechanism, were used. Comparison of the calculated dependencies, based on the above models, with the experimental ones, shows that the continuous-medium model agrees best with the experimentally found unit cell parameter dependence of our carbon supported Pt nanoparticles.},\n\tlanguage = {en},\n\tnumber = {68},\n\turldate = {2023-11-11},\n\tjournal = {RSC Advances},\n\tauthor = {Leontyev, I. N. and Kuriganova, A. B. and Leontyev, N. G. and Hennet, L. and Rakhmatullin, A. and Smirnova, N. V. and Dmitriev, V.},\n\tmonth = aug,\n\tyear = {2014},\n\tnote = {Publisher: The Royal Society of Chemistry},\n\tpages = {35959--35965},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Carbon supported Pt nanoparticles with diameters ranging from 2 to 28 nm have been studied using X-ray diffraction. The unit cell parameter of synthesized Pt/C nanoparticles is always lower than that of bulk Pt. By decreasing the average particle size D to approximately 2 nm, the unit cell parameter a nonlinearly decreases by about 0.03 Å which corresponds to a variation of 0.7% in comparison to bulk Pt, and the size effect is predominant for sizes ranging from 2 to 10 nm. The dependence a(1/D) is approximated well using a straight line with a slope of −0.0555 ± 0.0067 nm−1 and an intercept of −3.9230 ± 0.0017 Å. For interpreting the obtained experimental dependence of the unit cell parameter of Pt/C nanoparticles, four different theoretical approaches such as the thermal vacancy mechanism, continuous-medium model, Laplace pressure, and bond order–length–strength correlation mechanism, were used. Comparison of the calculated dependencies, based on the above models, with the experimental ones, shows that the continuous-medium model agrees best with the experimentally found unit cell parameter dependence of our carbon supported Pt nanoparticles.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"janolin-anokhin-gui-mukhortov-golovko-guiblin-ravy-marssi-etal-strainengineeringofperovskitethinfilmsusingasinglesubstrate-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/0953-8984/26/29/292201\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'janolin-anokhin-gui-mukhortov-golovko-guiblin-ravy-marssi-etal-strainengineeringofperovskitethinfilmsusingasinglesubstrate-2014', 'https://dx.doi.org/10.1088/0953-8984/26/29/292201', event);\">\n    Strain engineering of perovskite thin films using a single substrate.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Janolin, P.; Anokhin, A. S.; Gui, Z.; Mukhortov, V. M.; Golovko, Y. I.; Guiblin, N.; Ravy, S.; Marssi, M. E.; Yuzyuk, Y. I.; Bellaiche, L.;  and Dkhil, B.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics: Condensed Matter</i>, 26(29): 292201. June 2014.\n  <span class=\"note\">Publisher: IOP Publishing</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/0953-8984/26/29/292201\"\n     onclick=\"log_download('janolin-anokhin-gui-mukhortov-golovko-guiblin-ravy-marssi-etal-strainengineeringofperovskitethinfilmsusingasinglesubstrate-2014', 'https://dx.doi.org/10.1088/0953-8984/26/29/292201', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Strain engineering of perovskite thin films using a single substrate [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/0953-8984/26/29/292201\"\n     onclick=\"log_download('janolin-anokhin-gui-mukhortov-golovko-guiblin-ravy-marssi-etal-strainengineeringofperovskitethinfilmsusingasinglesubstrate-2014', 'http://doi.org/10.1088/0953-8984/26/29/292201', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/janolin-anokhin-gui-mukhortov-golovko-guiblin-ravy-marssi-etal-strainengineeringofperovskitethinfilmsusingasinglesubstrate-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('janolin-anokhin-gui-mukhortov-golovko-guiblin-ravy-marssi-etal-strainengineeringofperovskitethinfilmsusingasinglesubstrate-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{janolin_strain_2014,\n\ttitle = {Strain engineering of perovskite thin films using a single substrate},\n\tvolume = {26},\n\tissn = {0953-8984},\n\turl = {https://dx.doi.org/10.1088/0953-8984/26/29/292201},\n\tdoi = {10.1088/0953-8984/26/29/292201},\n\tabstract = {Combining temperature-dependent x-ray diffraction, Raman spectroscopy and first-principles-based effective Hamiltonian calculations, we show that varying the thickness of (Ba0.8Sr0.2)TiO3 (BST) thin films deposited on the same single substrate (namely, MgO) enables us to change not only the magnitude but also the sign of the misfit strain. Such previously overlooked control of the strain allows several properties of these films (e.g. Curie temperature, symmetry of ferroelectric phases, dielectric response) to be tuned and even optimized. Surprisingly, such desired control of the strain (and of the resulting properties) originates from an effect that is commonly believed to be detrimental to functionalities of films, namely the existence of misfit dislocations. The present study therefore provides a novel route to strain engineering, as well as leading us to revisit common beliefs.},\n\tlanguage = {en},\n\tnumber = {29},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics: Condensed Matter},\n\tauthor = {Janolin, P.-E. and Anokhin, A. S. and Gui, Z. and Mukhortov, V. M. and Golovko, Yu I. and Guiblin, N. and Ravy, S. and Marssi, M. El and Yuzyuk, Yu I. and Bellaiche, L. and Dkhil, B.},\n\tmonth = jun,\n\tyear = {2014},\n\tnote = {Publisher: IOP Publishing},\n\tpages = {292201},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Combining temperature-dependent x-ray diffraction, Raman spectroscopy and first-principles-based effective Hamiltonian calculations, we show that varying the thickness of (Ba0.8Sr0.2)TiO3 (BST) thin films deposited on the same single substrate (namely, MgO) enables us to change not only the magnitude but also the sign of the misfit strain. Such previously overlooked control of the strain allows several properties of these films (e.g. Curie temperature, symmetry of ferroelectric phases, dielectric response) to be tuned and even optimized. Surprisingly, such desired control of the strain (and of the resulting properties) originates from an effect that is commonly believed to be detrimental to functionalities of films, namely the existence of misfit dislocations. The present study therefore provides a novel route to strain engineering, as well as leading us to revisit common beliefs.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"roshal-petrov-myasnikova-rochal-extendedtopologicaldefectsassourcesandoutletsofdislocationsinsphericalhexagonalcrystals-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0375960114002941\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'roshal-petrov-myasnikova-rochal-extendedtopologicaldefectsassourcesandoutletsofdislocationsinsphericalhexagonalcrystals-2014', 'https://www.sciencedirect.com/science/article/pii/S0375960114002941', event);\">\n    Extended topological defects as sources and outlets of dislocations in spherical hexagonal crystals.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Roshal, D. S.; Petrov, K. Y.; Myasnikova, A. E.;  and Rochal, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Physics Letters A</i>, 378(21): 1548–1552. April 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0375960114002941\"\n     onclick=\"log_download('roshal-petrov-myasnikova-rochal-extendedtopologicaldefectsassourcesandoutletsofdislocationsinsphericalhexagonalcrystals-2014', 'https://www.sciencedirect.com/science/article/pii/S0375960114002941', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Extended topological defects as sources and outlets of dislocations in spherical hexagonal crystals [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.physleta.2014.03.037\"\n     onclick=\"log_download('roshal-petrov-myasnikova-rochal-extendedtopologicaldefectsassourcesandoutletsofdislocationsinsphericalhexagonalcrystals-2014', 'http://doi.org/10.1016/j.physleta.2014.03.037', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/roshal-petrov-myasnikova-rochal-extendedtopologicaldefectsassourcesandoutletsofdislocationsinsphericalhexagonalcrystals-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('roshal-petrov-myasnikova-rochal-extendedtopologicaldefectsassourcesandoutletsofdislocationsinsphericalhexagonalcrystals-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{roshal_extended_2014,\n\ttitle = {Extended topological defects as sources and outlets of dislocations in spherical hexagonal crystals},\n\tvolume = {378},\n\tissn = {0375-9601},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0375960114002941},\n\tdoi = {10.1016/j.physleta.2014.03.037},\n\tabstract = {Extended topological defects (ETDs) arising in spherical hexagonal crystals due to their curvature are considered. These prevalent defects carry a unit total topological charge and are surrounded by scalene pentagonal boundaries. Topological peculiarities of reactions between ETDs and dislocations are considered. Similarly to boundaries of the usual planar crystalline order the ETDs emit and absorb the dislocations without preservation of their dislocational charge. Dislocations located inside the ETD area lose it and the enforced ETD decay can proceed in different ways without conservation of the total Burgers vector of the dislocations emitted.},\n\tnumber = {21},\n\turldate = {2023-11-11},\n\tjournal = {Physics Letters A},\n\tauthor = {Roshal, D. S. and Petrov, K. Yu. and Myasnikova, A. E. and Rochal, S. B.},\n\tmonth = apr,\n\tyear = {2014},\n\tkeywords = {Colloidal crystals, Curvature, Disclinations, Dislocations, Spherical structures, Topological defects},\n\tpages = {1548--1552},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\VVC82RZB\\\\Roshal и др. - 2014 - Extended topological defects as sources and outlet.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Extended topological defects (ETDs) arising in spherical hexagonal crystals due to their curvature are considered. These prevalent defects carry a unit total topological charge and are surrounded by scalene pentagonal boundaries. Topological peculiarities of reactions between ETDs and dislocations are considered. Similarly to boundaries of the usual planar crystalline order the ETDs emit and absorb the dislocations without preservation of their dislocational charge. Dislocations located inside the ETD area lose it and the enforced ETD decay can proceed in different ways without conservation of the total Burgers vector of the dislocations emitted.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"baudry-lukyanchuk-razumnaya-longitudinalandtransversalpolarizationswitchinginstrainedferroelectrics-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/00150193.2014.889528\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'baudry-lukyanchuk-razumnaya-longitudinalandtransversalpolarizationswitchinginstrainedferroelectrics-2014', 'https://doi.org/10.1080/00150193.2014.889528', event);\">\n    Longitudinal and Transversal Polarization Switching in Strained Ferroelectrics.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Baudry, L.; Luk’yanchuk, I. A.;  and Razumnaya, A.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 461(1): 22–28. March 2014.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2014.889528</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/00150193.2014.889528\"\n     onclick=\"log_download('baudry-lukyanchuk-razumnaya-longitudinalandtransversalpolarizationswitchinginstrainedferroelectrics-2014', 'https://doi.org/10.1080/00150193.2014.889528', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Longitudinal and Transversal Polarization Switching in Strained Ferroelectrics [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150193.2014.889528\"\n     onclick=\"log_download('baudry-lukyanchuk-razumnaya-longitudinalandtransversalpolarizationswitchinginstrainedferroelectrics-2014', 'http://doi.org/10.1080/00150193.2014.889528', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/baudry-lukyanchuk-razumnaya-longitudinalandtransversalpolarizationswitchinginstrainedferroelectrics-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('baudry-lukyanchuk-razumnaya-longitudinalandtransversalpolarizationswitchinginstrainedferroelectrics-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{baudry_longitudinal_2014,\n\ttitle = {Longitudinal and {Transversal} {Polarization} {Switching} in {Strained} {Ferroelectrics}},\n\tvolume = {461},\n\tissn = {0015-0193},\n\turl = {https://doi.org/10.1080/00150193.2014.889528},\n\tdoi = {10.1080/00150193.2014.889528},\n\tabstract = {Using the multicomponent Landau-Devonshire functional we study the field-induced polarization switching in c-oriented ferroelectric phase of epitaxial perovskite film and found that two different regimes are possible: (i) longitudinal switching with change of the polarization modulus and (ii) transversal switching with virtual admixing of the a-component of polarization. The results are specified for the case of barium titanate oxide BaTiO3where the crossover line between two types of switching is found at strain-temperature phase diagram.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Ferroelectrics},\n\tauthor = {Baudry, L. and Luk’yanchuk, I. A. and Razumnaya, A.},\n\tmonth = mar,\n\tyear = {2014},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/00150193.2014.889528},\n\tkeywords = {Ferroelectric thin films, strain, switching},\n\tpages = {22--28},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\XAP4K9W5\\\\Baudry и др. - 2014 - Longitudinal and Transversal Polarization Switchin.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Using the multicomponent Landau-Devonshire functional we study the field-induced polarization switching in c-oriented ferroelectric phase of epitaxial perovskite film and found that two different regimes are possible: (i) longitudinal switching with change of the polarization modulus and (ii) transversal switching with virtual admixing of the a-component of polarization. The results are specified for the case of barium titanate oxide BaTiO3where the crossover line between two types of switching is found at strain-temperature phase diagram.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"zhukova-gorshunov-torgashev-lebedev-shakurov-kremer-pestrjakov-thomas-etal-quantumbehaviourofwatermoleculeingemstoneterahertzfingerprints-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/486/1/012019\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'zhukova-gorshunov-torgashev-lebedev-shakurov-kremer-pestrjakov-thomas-etal-quantumbehaviourofwatermoleculeingemstoneterahertzfingerprints-2014', 'https://dx.doi.org/10.1088/1742-6596/486/1/012019', event);\">\n    Quantum behaviour of water molecule in gemstone: terahertz fingerprints.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Zhukova, E. S.; Gorshunov, B. P.; Torgashev, V. I.; Lebedev, V. V.; Shakurov, G. S.; Kremer, R. K.; Pestrjakov, E. V.; Thomas, V. G.; Fursenko, D. A.;  and Dressel, M.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics: Conference Series</i>, 486(1): 012019. March 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/486/1/012019\"\n     onclick=\"log_download('zhukova-gorshunov-torgashev-lebedev-shakurov-kremer-pestrjakov-thomas-etal-quantumbehaviourofwatermoleculeingemstoneterahertzfingerprints-2014', 'https://dx.doi.org/10.1088/1742-6596/486/1/012019', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Quantum behaviour of water molecule in gemstone: terahertz fingerprints [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/1742-6596/486/1/012019\"\n     onclick=\"log_download('zhukova-gorshunov-torgashev-lebedev-shakurov-kremer-pestrjakov-thomas-etal-quantumbehaviourofwatermoleculeingemstoneterahertzfingerprints-2014', 'http://doi.org/10.1088/1742-6596/486/1/012019', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/zhukova-gorshunov-torgashev-lebedev-shakurov-kremer-pestrjakov-thomas-etal-quantumbehaviourofwatermoleculeingemstoneterahertzfingerprints-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('zhukova-gorshunov-torgashev-lebedev-shakurov-kremer-pestrjakov-thomas-etal-quantumbehaviourofwatermoleculeingemstoneterahertzfingerprints-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{zhukova_quantum_2014,\n\ttitle = {Quantum behaviour of water molecule in gemstone: terahertz fingerprints},\n\tvolume = {486},\n\tissn = {1742-6596},\n\tshorttitle = {Quantum behaviour of water molecule in gemstone},\n\turl = {https://dx.doi.org/10.1088/1742-6596/486/1/012019},\n\tdoi = {10.1088/1742-6596/486/1/012019},\n\tabstract = {We have shown that a weak interaction of a lone H2O molecule with the ‘‘walls’’ of nano-sized crystalline cage of gemstone (beryl) results in emergence of a rich set of molecular vibrational states. By analogy with translational and librational bands in liquid water and ice corresponding absorption bands are explained as due to translational (T) and librational (L) movements of the H2O molecule which is hydrogen bonded to the cage walls. In beryl crystal lattice, however, the six-fold symmetry of the cage brings about additional effect of splitting of the T and L bands into fine structure due to tunnelling within the six-well potential relief. The presented results will be of use for analysis of more complicated systems with confined water molecules like H2O chains in carbon nano-tubes, molecular clusters in e.g. zeolites, clays, silica gels and other natural or synthetic frameworks, as well as for interfacial water in biological systems.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics: Conference Series},\n\tauthor = {Zhukova, Elena S. and Gorshunov, Boris P. and Torgashev, Victor I. and Lebedev, Vladimir V. and Shakurov, Gil&#x27;man S. and Kremer, Reinhard K. and Pestrjakov, Efim V. and Thomas, Victor G. and Fursenko, Dimitry A. and Dressel, Martin},\n\tmonth = mar,\n\tyear = {2014},\n\tpages = {012019},\n\tfile = {IOP Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\E6MX2SN9\\\\Zhukova и др. - 2014 - Quantum behaviour of water molecule in gemstone t.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We have shown that a weak interaction of a lone H2O molecule with the ‘‘walls’’ of nano-sized crystalline cage of gemstone (beryl) results in emergence of a rich set of molecular vibrational states. By analogy with translational and librational bands in liquid water and ice corresponding absorption bands are explained as due to translational (T) and librational (L) movements of the H2O molecule which is hydrogen bonded to the cage walls. In beryl crystal lattice, however, the six-fold symmetry of the cage brings about additional effect of splitting of the T and L bands into fine structure due to tunnelling within the six-well potential relief. The presented results will be of use for analysis of more complicated systems with confined water molecules like H2O chains in carbon nano-tubes, molecular clusters in e.g. zeolites, clays, silica gels and other natural or synthetic frameworks, as well as for interfacial water in biological systems.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"talanov-shirokov-atomicorderinthespinelstructureagrouptheoreticalanalysis-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://scripts.iucr.org/cgi-bin/paper?kx5021\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'talanov-shirokov-atomicorderinthespinelstructureagrouptheoreticalanalysis-2014', 'http://scripts.iucr.org/cgi-bin/paper?kx5021', event);\">\n    Atomic order in the spinel structure – a group-theoretical analysis.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Talanov, V. M.;  and Shirokov, V. B.\n</span>\n\n  \n\n</span>\n\n  <i>Acta Crystallographica Section A: Foundations and Advances</i>, 70(1): 49–63. January 2014.\n  <span class=\"note\">Number: 1 Publisher: International Union of Crystallography</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://scripts.iucr.org/cgi-bin/paper?kx5021\"\n     onclick=\"log_download('talanov-shirokov-atomicorderinthespinelstructureagrouptheoreticalanalysis-2014', 'http://scripts.iucr.org/cgi-bin/paper?kx5021', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Atomic order in the spinel structure – a group-theoretical analysis [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1107/S2053273313027605\"\n     onclick=\"log_download('talanov-shirokov-atomicorderinthespinelstructureagrouptheoreticalanalysis-2014', 'http://doi.org/10.1107/S2053273313027605', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/talanov-shirokov-atomicorderinthespinelstructureagrouptheoreticalanalysis-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('talanov-shirokov-atomicorderinthespinelstructureagrouptheoreticalanalysis-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{talanov_atomic_2014,\n\ttitle = {Atomic order in the spinel structure – a group-theoretical analysis},\n\tvolume = {70},\n\tcopyright = {Copyright (c) 2014 International Union of Crystallography},\n\tissn = {2053-2733},\n\turl = {http://scripts.iucr.org/cgi-bin/paper?kx5021},\n\tdoi = {10.1107/S2053273313027605},\n\tabstract = {Group-theoretical methods of the Landau theory of phase transitions are used to investigate the structures of ordered spinels. The possibility of the existence is determined of 305 phases with different types of order in Wyckoff position 8a (including seven binary and seven ternary cation substructures), 537 phases in Wyckoff position 16d (including eight binary and 11 ternary cation substructures), 595 phases in Wyckoff position 32e (including seven binary and four ternary anion substructures) and 549 phases with simultaneous ordering in Wyckoff positions 8a and 16d (including five substructures with binary order in tetrahedral and octahedral sublattices, two substructures with ternary order in both spinel sublattices, and nine substructures with different combined types of binary and ternary order). Theoretical results and experimental data are compared. Calculated structures of the spread types of ordered low-symmetry spinel modifications are given.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Acta Crystallographica Section A: Foundations and Advances},\n\tauthor = {Talanov, V. M. and Shirokov, V. B.},\n\tmonth = jan,\n\tyear = {2014},\n\tnote = {Number: 1\nPublisher: International Union of Crystallography},\n\tpages = {49--63},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Group-theoretical methods of the Landau theory of phase transitions are used to investigate the structures of ordered spinels. The possibility of the existence is determined of 305 phases with different types of order in Wyckoff position 8a (including seven binary and seven ternary cation substructures), 537 phases in Wyckoff position 16d (including eight binary and 11 ternary cation substructures), 595 phases in Wyckoff position 32e (including seven binary and four ternary anion substructures) and 549 phases with simultaneous ordering in Wyckoff positions 8a and 16d (including five substructures with binary order in tetrahedral and octahedral sublattices, two substructures with ternary order in both spinel sublattices, and nine substructures with different combined types of binary and ternary order). Theoretical results and experimental data are compared. Calculated structures of the spread types of ordered low-symmetry spinel modifications are given.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"ponomareva-moshnikov-maslova-yuzyuk-suchaneck-effectofthermalannealingonthesurfaceofsolgelpreparedoxidefilmstudiedbyatomicforcemicroscopyandramanspectroscopy-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1087659614010192\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'ponomareva-moshnikov-maslova-yuzyuk-suchaneck-effectofthermalannealingonthesurfaceofsolgelpreparedoxidefilmstudiedbyatomicforcemicroscopyandramanspectroscopy-2014', 'https://doi.org/10.1134/S1087659614010192', event);\">\n    Effect of thermal annealing on the surface of sol-gel prepared oxide film studied by atomic force microscopy and Raman spectroscopy.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Ponomareva, A. A.; Moshnikov, V. A.; Maslova, O. A.; Yuzyuk, Y. I.;  and Suchaneck, G.\n</span>\n\n  \n\n</span>\n\n  <i>Glass Physics and Chemistry</i>, 40(1): 99–105. January 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1087659614010192\"\n     onclick=\"log_download('ponomareva-moshnikov-maslova-yuzyuk-suchaneck-effectofthermalannealingonthesurfaceofsolgelpreparedoxidefilmstudiedbyatomicforcemicroscopyandramanspectroscopy-2014', 'https://doi.org/10.1134/S1087659614010192', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Effect of thermal annealing on the surface of sol-gel prepared oxide film studied by atomic force microscopy and Raman spectroscopy [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1087659614010192\"\n     onclick=\"log_download('ponomareva-moshnikov-maslova-yuzyuk-suchaneck-effectofthermalannealingonthesurfaceofsolgelpreparedoxidefilmstudiedbyatomicforcemicroscopyandramanspectroscopy-2014', 'http://doi.org/10.1134/S1087659614010192', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/ponomareva-moshnikov-maslova-yuzyuk-suchaneck-effectofthermalannealingonthesurfaceofsolgelpreparedoxidefilmstudiedbyatomicforcemicroscopyandramanspectroscopy-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('ponomareva-moshnikov-maslova-yuzyuk-suchaneck-effectofthermalannealingonthesurfaceofsolgelpreparedoxidefilmstudiedbyatomicforcemicroscopyandramanspectroscopy-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{ponomareva_effect_2014,\n\ttitle = {Effect of thermal annealing on the surface of sol-gel prepared oxide film studied by atomic force microscopy and {Raman} spectroscopy},\n\tvolume = {40},\n\tissn = {1608-313X},\n\turl = {https://doi.org/10.1134/S1087659614010192},\n\tdoi = {10.1134/S1087659614010192},\n\tabstract = {In this work, we have investigated the surface topography evolution of sol-gel deposited SiO2-SnO2 nanocomposite films annealed in the temperature range 200–600°C. The fractal dimension of atomic force microscopy images of the films was determined by the cube counting method and the triangulation method. The fractal dimension was shown to be an appropriate and easy to use tool for the characterization of nanosized thin film structures. Raman spectroscopy revealed the formation of a SiO2 cage-like structure at 400°C and SnO2 crystallization above 500°C.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Glass Physics and Chemistry},\n\tauthor = {Ponomareva, A. A. and Moshnikov, V. A. and Maslova, O. A. and Yuzyuk, Yu. I. and Suchaneck, G.},\n\tmonth = jan,\n\tyear = {2014},\n\tkeywords = {nanocomposite SiO2-SnO2, the sol-gel method},\n\tpages = {99--105},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  In this work, we have investigated the surface topography evolution of sol-gel deposited SiO2-SnO2 nanocomposite films annealed in the temperature range 200–600°C. The fractal dimension of atomic force microscopy images of the films was determined by the cube counting method and the triangulation method. The fractal dimension was shown to be an appropriate and easy to use tool for the characterization of nanosized thin film structures. Raman spectroscopy revealed the formation of a SiO2 cage-like structure at 400°C and SnO2 crystallization above 500°C.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"gorshunov-zhukova-torgashev-kadyrov-motovilova-fischgrabe-moshnyaga-zhang-etal-bosonpeakinmanganites-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/486/1/012001\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'gorshunov-zhukova-torgashev-kadyrov-motovilova-fischgrabe-moshnyaga-zhang-etal-bosonpeakinmanganites-2014', 'https://dx.doi.org/10.1088/1742-6596/486/1/012001', event);\">\n    Boson peak in manganites.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Gorshunov, B. P.; Zhukova, E. S.; Torgashev, V. I.; Kadyrov, L. S.; Motovilova, E. A.; Fischgrabe, F.; Moshnyaga, V.; Zhang, T.; Kremer, R.; Pracht, U.; Zapf, S.;  and Dressel, M.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics: Conference Series</i>, 486(1): 012001. March 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/1742-6596/486/1/012001\"\n     onclick=\"log_download('gorshunov-zhukova-torgashev-kadyrov-motovilova-fischgrabe-moshnyaga-zhang-etal-bosonpeakinmanganites-2014', 'https://dx.doi.org/10.1088/1742-6596/486/1/012001', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Boson peak in manganites [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/1742-6596/486/1/012001\"\n     onclick=\"log_download('gorshunov-zhukova-torgashev-kadyrov-motovilova-fischgrabe-moshnyaga-zhang-etal-bosonpeakinmanganites-2014', 'http://doi.org/10.1088/1742-6596/486/1/012001', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/gorshunov-zhukova-torgashev-kadyrov-motovilova-fischgrabe-moshnyaga-zhang-etal-bosonpeakinmanganites-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('gorshunov-zhukova-torgashev-kadyrov-motovilova-fischgrabe-moshnyaga-zhang-etal-bosonpeakinmanganites-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{gorshunov_boson_2014,\n\ttitle = {Boson peak in manganites},\n\tvolume = {486},\n\tissn = {1742-6596},\n\turl = {https://dx.doi.org/10.1088/1742-6596/486/1/012001},\n\tdoi = {10.1088/1742-6596/486/1/012001},\n\tabstract = {After the phase transition occurs in manganites La1-xCaxMnO3 (x ≥ 0.5) into a dielectric phase with charge order, right below the corresponding temperature of TCO = 240 K a series of absorption lines appear in the terahertz spectral range, only in case of commensurate x values. We show that the lines originate from acoustic phonons that become optically active by folding of the Brillouin zone. At even lower temperatures, a strongly asymmetric extra absorption band develops at frequencies around 20 cm−1 – 30 cm−1 corresponding to the position of the lowest-energy van Hove singularity in the reduced Brillouin zone. The band is assigned to the Boson Peak, i.e. to the excess of lattice vibrational states over the standard Debye contribution. The folded phonons and the boson peak do not show up for incommensurate calcium.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics: Conference Series},\n\tauthor = {Gorshunov, Boris P. and Zhukova, Elena S. and Torgashev, Victor I. and Kadyrov, Lenar S. and Motovilova, Elizaveta A. and Fischgrabe, Florian and Moshnyaga, Vasiliy and Zhang, Tao and Kremer, Reinhard and Pracht, Uwe and Zapf, Sina and Dressel, Martin},\n\tmonth = mar,\n\tyear = {2014},\n\tpages = {012001},\n\tfile = {IOP Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\MKBKK4JA\\\\Gorshunov и др. - 2014 - Boson peak in manganites.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  After the phase transition occurs in manganites La1-xCaxMnO3 (x ≥ 0.5) into a dielectric phase with charge order, right below the corresponding temperature of TCO = 240 K a series of absorption lines appear in the terahertz spectral range, only in case of commensurate x values. We show that the lines originate from acoustic phonons that become optically active by folding of the Brillouin zone. At even lower temperatures, a strongly asymmetric extra absorption band develops at frequencies around 20 cm−1 – 30 cm−1 corresponding to the position of the lowest-energy van Hove singularity in the reduced Brillouin zone. The band is assigned to the Boson Peak, i.e. to the excess of lattice vibrational states over the standard Debye contribution. The folded phonons and the boson peak do not show up for incommensurate calcium.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"levshov-michel-paillet-than-tran-arenal-rahmani-boutahir-etal-coupledvibrationsinindexidentifiedcarbonnanotubes-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.cambridge.org/core/journals/mrs-online-proceedings-library-archive/article/abs/coupled-vibrations-in-indexidentified-carbon-nanotubes/2DD3B289A28698521E4E64C11E70F0DB\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'levshov-michel-paillet-than-tran-arenal-rahmani-boutahir-etal-coupledvibrationsinindexidentifiedcarbonnanotubes-2014', 'https://www.cambridge.org/core/journals/mrs-online-proceedings-library-archive/article/abs/coupled-vibrations-in-indexidentified-carbon-nanotubes/2DD3B289A28698521E4E64C11E70F0DB', event);\">\n    Coupled Vibrations in Index-Identified Carbon Nanotubes.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Levshov, D.; Michel, T.; Paillet, M.; Than, X. T.; Tran, H. N.; Arenal, R.; Rahmani, A.; Boutahir, M.; Zahab, A.;  and Sauvajol, J.\n</span>\n\n  \n\n</span>\n\n  <i>MRS Online Proceedings Library (OPL)</i>, 1700: 69–77. January 2014.\n  <span class=\"note\">Publisher: Cambridge University Press</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.cambridge.org/core/journals/mrs-online-proceedings-library-archive/article/abs/coupled-vibrations-in-indexidentified-carbon-nanotubes/2DD3B289A28698521E4E64C11E70F0DB\"\n     onclick=\"log_download('levshov-michel-paillet-than-tran-arenal-rahmani-boutahir-etal-coupledvibrationsinindexidentifiedcarbonnanotubes-2014', 'https://www.cambridge.org/core/journals/mrs-online-proceedings-library-archive/article/abs/coupled-vibrations-in-indexidentified-carbon-nanotubes/2DD3B289A28698521E4E64C11E70F0DB', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Coupled Vibrations in Index-Identified Carbon Nanotubes [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1557/opl.2014.574\"\n     onclick=\"log_download('levshov-michel-paillet-than-tran-arenal-rahmani-boutahir-etal-coupledvibrationsinindexidentifiedcarbonnanotubes-2014', 'http://doi.org/10.1557/opl.2014.574', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/levshov-michel-paillet-than-tran-arenal-rahmani-boutahir-etal-coupledvibrationsinindexidentifiedcarbonnanotubes-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('levshov-michel-paillet-than-tran-arenal-rahmani-boutahir-etal-coupledvibrationsinindexidentifiedcarbonnanotubes-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{levshov_coupled_2014,\n\ttitle = {Coupled {Vibrations} in {Index}-{Identified} {Carbon} {Nanotubes}},\n\tvolume = {1700},\n\tissn = {0272-9172, 1946-4274},\n\turl = {https://www.cambridge.org/core/journals/mrs-online-proceedings-library-archive/article/abs/coupled-vibrations-in-indexidentified-carbon-nanotubes/2DD3B289A28698521E4E64C11E70F0DB},\n\tdoi = {10.1557/opl.2014.574},\n\tabstract = {Combining high resolution transmission electron spectroscopy, electron diffraction, and resonant Raman spectroscopy experiments on the same suspended (free-standing) individual carbon nanotubes is the ultimate approach to relate unambiguously the structure and the intrinsic phonon features of these nano-systems.By using this approach, the effect of coupling between nanotubes on the phonons is investigated in two model nano-systems: (i) a bundle of two non-identical SWNTs (inhomogeneous dimer), (ii) double-walled carbon nanotubes.},\n\tlanguage = {en},\n\turldate = {2023-11-11},\n\tjournal = {MRS Online Proceedings Library (OPL)},\n\tauthor = {Levshov, Dmitry and Michel, Thierry and Paillet, Matthieu and Than, Xuan Tinh and Tran, Huy Nam and Arenal, Raul and Rahmani, Abdelali and Boutahir, Mourad and Zahab, Ahmed-Azmi and Sauvajol, Jean-Louis},\n\tmonth = jan,\n\tyear = {2014},\n\tnote = {Publisher: Cambridge University Press},\n\tkeywords = {C, nanoscale, Raman spectroscopy},\n\tpages = {69--77},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Combining high resolution transmission electron spectroscopy, electron diffraction, and resonant Raman spectroscopy experiments on the same suspended (free-standing) individual carbon nanotubes is the ultimate approach to relate unambiguously the structure and the intrinsic phonon features of these nano-systems.By using this approach, the effect of coupling between nanotubes on the phonons is investigated in two model nano-systems: (i) a bundle of two non-identical SWNTs (inhomogeneous dimer), (ii) double-walled carbon nanotubes.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"--------etal-1xbifeotextrm3xanbotextrm3akna-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/40748\"\n     onclick=\"return trackOutboundLink('publications', 'click', '--------etal-1xbifeotextrm3xanbotextrm3akna-2014', 'http://journals.ioffe.ru/articles/40748', event);\">\n    Структура и динамика решетки твердых растворов (1-x)BiFeO$_{\\textrm{3}}$-xANbO$_{\\textrm{3}}$ (A-K, Na).\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Тесленко, П. Ю.; Разумная, А. Г.; Пономоренко, В. О.; Рудская, А. Г.; Назаренко, А. В.; Анохин, А. С.; Авраменко, М. В.; Левшов, Д. И.; Куприянов, М. Ф.;  and Юзюк, Ю. И.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 56(9): 1804–18010. August 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/40748\"\n     onclick=\"log_download('--------etal-1xbifeotextrm3xanbotextrm3akna-2014', 'http://journals.ioffe.ru/articles/40748', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Структура и динамика решетки твердых растворов (1-x)BiFeO$_{\\textrm{3}}$-xANbO$_{\\textrm{3}}$ (A-K, Na) [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/--------etal-1xbifeotextrm3xanbotextrm3akna-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('--------etal-1xbifeotextrm3xanbotextrm3akna-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2014,\n\ttitle = {Структура и динамика решетки твердых растворов (1-x){BiFeO}$_{\\textrm{3}}$-{xANbO}$_{\\textrm{3}}$ ({A}-{K}, {Na})},\n\tvolume = {56},\n\turl = {http://journals.ioffe.ru/articles/40748},\n\tabstract = {Методами рентгеновской порошковой дифракции и комбинационного рассеяния света изучены структуры и динамические характеристики решеток составов двух систем твердых растворов мультиферроика BiFeO3 с сегнетоэлектриком KNbO3 и антисегнетоэлектриком NaNbO3: (1-x)BiFeO3-xKNbO3 и (1-x)BiFeO3-xNaNbO3. Для этих систем в составах с x=0.3, 0.5 и 0.7 при комнатной температуре определены симметрия, параметры элементарных ячеек. Из анализа колебательных спектров установлены последовательности ротационных искажений при изменении концентраций в этих системах твердых растворов.},\n\tlanguage = {ru},\n\tnumber = {9},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Тесленко, П. Ю. and Разумная, А. Г. and Пономоренко, В. О. and Рудская, А. Г. and Назаренко, А. В. and Анохин, А. С. and Авраменко, М. В. and Левшов, Д. И. and Куприянов, М. Ф. and Юзюк, Ю. И.},\n\tmonth = aug,\n\tyear = {2014},\n\tpages = {1804--18010},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Методами рентгеновской порошковой дифракции и комбинационного рассеяния света изучены структуры и динамические характеристики решеток составов двух систем твердых растворов мультиферроика BiFeO3 с сегнетоэлектриком KNbO3 и антисегнетоэлектриком NaNbO3: (1-x)BiFeO3-xKNbO3 и (1-x)BiFeO3-xNaNbO3. Для этих систем в составах с x=0.3, 0.5 и 0.7 при комнатной температуре определены симметрия, параметры элементарных ячеек. Из анализа колебательных спектров установлены последовательности ротационных искажений при изменении концентраций в этих системах твердых растворов.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://www.ivdon.ru/ru/magazine/archive/N4y2014/2679\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----2014', 'http://www.ivdon.ru/ru/magazine/archive/N4y2014/2679', event);\">\n    Анализ атомной структуры углеродных нанотрубок методами спектроскопии комбинационного рассеяния света и электронной дифракции.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Левшов, Д. И.; Авраменко, М. В.;  and Пимонов, В. В.\n</span>\n\n  \n\n</span>\n\n  <i>Инженерный Вестник Дона</i>, (4): 1–11. June 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://www.ivdon.ru/ru/magazine/archive/N4y2014/2679\"\n     onclick=\"log_download('----2014', 'http://www.ivdon.ru/ru/magazine/archive/N4y2014/2679', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Анализ атомной структуры углеродных нанотрубок методами спектроскопии комбинационного рассеяния света и электронной дифракции [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2014-1,\n\ttitle = {Анализ атомной структуры углеродных нанотрубок методами спектроскопии комбинационного рассеяния света и электронной дифракции},\n\turl = {http://www.ivdon.ru/ru/magazine/archive/N4y2014/2679},\n\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\n\tlanguage = {ru},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Инженерный Вестник Дона},\n\tauthor = {Левшов, Д. И. and Авраменко, М. В. and Пимонов, В. В.},\n\tmonth = jun,\n\tyear = {2014},\n\tkeywords = {⛔ No DOI found},\n\tpages = {1--11},\n\tfile = {Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\8MAPFW2E\\\\2679.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Сетевой научный журнал «Инженерный вестник Дона»\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://www.ivdon.ru/ru/magazine/archive/N4y2014/2680\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----2014', 'http://www.ivdon.ru/ru/magazine/archive/N4y2014/2680', event);\">\n    Влияние эффектов окружения на колебательные свойства индивидуальных углеродных нанотрубок.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Левшов, Д. И.; Авраменко, М. В.;  and Пимонов, В. В.\n</span>\n\n  \n\n</span>\n\n  <i>Инженерный Вестник Дона</i>, (4): 1–14. June 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://www.ivdon.ru/ru/magazine/archive/N4y2014/2680\"\n     onclick=\"log_download('----2014', 'http://www.ivdon.ru/ru/magazine/archive/N4y2014/2680', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Влияние эффектов окружения на колебательные свойства индивидуальных углеродных нанотрубок [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2014-2,\n\ttitle = {Влияние эффектов окружения на колебательные свойства индивидуальных углеродных нанотрубок},\n\turl = {http://www.ivdon.ru/ru/magazine/archive/N4y2014/2680},\n\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\n\tlanguage = {ru},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Инженерный Вестник Дона},\n\tauthor = {Левшов, Д. И. and Авраменко, М. В. and Пимонов, В. В.},\n\tmonth = jun,\n\tyear = {2014},\n\tkeywords = {⛔ No DOI found},\n\tpages = {1--14},\n\tfile = {Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\ZAP3J5ZW\\\\2680.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Сетевой научный журнал «Инженерный вестник Дона»\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://www.ivdon.ru/ru/magazine/archive/N4y2014/2681\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----2014', 'http://www.ivdon.ru/ru/magazine/archive/N4y2014/2681', event);\">\n    Температурная зависимость двухмагнонных возбуждений в пленках феррита висмута легированного неодимом.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Кхабири, Г.; Разумная, А. Г.;  and Юзюк, Ю. И.\n</span>\n\n  \n\n</span>\n\n  . May 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://www.ivdon.ru/ru/magazine/archive/N4y2014/2681\"\n     onclick=\"log_download('----2014', 'http://www.ivdon.ru/ru/magazine/archive/N4y2014/2681', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Температурная зависимость двухмагнонных возбуждений в пленках феррита висмута легированного неодимом [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2014-3,\n\ttitle = {Температурная зависимость двухмагнонных возбуждений в пленках феррита висмута легированного неодимом},\n\turl = {http://www.ivdon.ru/ru/magazine/archive/N4y2014/2681},\n\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tauthor = {Кхабири, Г. and Разумная, А. Г. and Юзюк, Ю. И.},\n\tmonth = may,\n\tyear = {2014},\n\tkeywords = {⛔ No DOI found},\n\tfile = {Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\NBC8JXKZ\\\\2681.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Сетевой научный журнал «Инженерный вестник Дона»\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kadyrov-gorshunov-zhukova-torgashev-prokhorov-motovilova-fischgrabe-moshnyaga-etal-terahertzinfraredelectrodynamicsofoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/01411594.2014.953508\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kadyrov-gorshunov-zhukova-torgashev-prokhorov-motovilova-fischgrabe-moshnyaga-etal-terahertzinfraredelectrodynamicsofoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2014', 'https://doi.org/10.1080/01411594.2014.953508', event);\">\n    Terahertz–infrared electrodynamics of overdoped manganites La$_{\\textrm{1–x}}$Ca$_{\\textrm{x}}$MnO$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kadyrov, L. S.; Gorshunov, B. P.; Zhukova, E. S.; Torgashev, V. I.; Prokhorov, A. S.; Motovilova, E. A.; Fischgrabe, F.; Moshnyaga, V. T.; Zhang, T.; Kremer, R. K.; Pracht, U.; Zapf, S.; Pokorný, J.; Untereiner, G.; Kamba, S.;  and Dressel, M.\n</span>\n\n  \n\n</span>\n\n  <i>Phase Transitions</i>, 87(10-11): 1050–1059. November 2014.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/01411594.2014.953508</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/01411594.2014.953508\"\n     onclick=\"log_download('kadyrov-gorshunov-zhukova-torgashev-prokhorov-motovilova-fischgrabe-moshnyaga-etal-terahertzinfraredelectrodynamicsofoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2014', 'https://doi.org/10.1080/01411594.2014.953508', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Terahertz–infrared electrodynamics of overdoped manganites La$_{\\textrm{1–x}}$Ca$_{\\textrm{x}}$MnO$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/01411594.2014.953508\"\n     onclick=\"log_download('kadyrov-gorshunov-zhukova-torgashev-prokhorov-motovilova-fischgrabe-moshnyaga-etal-terahertzinfraredelectrodynamicsofoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2014', 'http://doi.org/10.1080/01411594.2014.953508', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kadyrov-gorshunov-zhukova-torgashev-prokhorov-motovilova-fischgrabe-moshnyaga-etal-terahertzinfraredelectrodynamicsofoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kadyrov-gorshunov-zhukova-torgashev-prokhorov-motovilova-fischgrabe-moshnyaga-etal-terahertzinfraredelectrodynamicsofoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kadyrov_terahertzinfrared_2014,\n\ttitle = {Terahertz–infrared electrodynamics of overdoped manganites {La}$_{\\textrm{1–x}}${Ca}$_{\\textrm{x}}${MnO}$_{\\textrm{3}}$},\n\tvolume = {87},\n\tissn = {0141-1594},\n\turl = {https://doi.org/10.1080/01411594.2014.953508},\n\tdoi = {10.1080/01411594.2014.953508},\n\tabstract = {We have measured low-temperature terahertz and infrared spectra of La1–xCa xMnO3 with x = 0.5; 0.6; 2/3, 0.7; 3/4, 0.85; 0.9; 0.95; 0.98 and x = 1 in the form of ceramics and epitaxial films. In the charge-ordered state for commensurate dopings (x = 2/3 and 3/4), we observed an absorption band at frequencies corresponding to the position of the lowest energy van Hove singularity in the folded Brillouin zone. The band is assigned to the boson peak. We observed qualitatively the same boson peak in Raman spectra of La1/3Ca2/3MnO3 ceramics. In antiferromagnetic phase, for the 0.5 ≤ x {\\textless} 0.85 range of doping, the conductivity mechanism gradually changes from a hopping-like transport at low temperatures to the Drude behavior at elevated temperatures in the paramagnetic phase. For 0.85 ≤ x {\\textless} 1 (canted antiferromagnetic phase), the electrons behave as Drude-like carriers in the whole temperature interval 5–300 K.},\n\tnumber = {10-11},\n\turldate = {2023-11-11},\n\tjournal = {Phase Transitions},\n\tauthor = {Kadyrov, Lenar S. and Gorshunov, Boris P. and Zhukova, Elena S. and Torgashev, Victor I. and Prokhorov, Anatoly S. and Motovilova, Elizaveta A. and Fischgrabe, Florian and Moshnyaga, Vasily T. and Zhang, Tao and Kremer, Reinhard K. and Pracht, Uwe and Zapf, Sina and Pokorný, Jan and Untereiner, Gabriele and Kamba, Stanislav and Dressel, Martin},\n\tmonth = nov,\n\tyear = {2014},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/01411594.2014.953508},\n\tkeywords = {manganites, terahertz},\n\tpages = {1050--1059},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We have measured low-temperature terahertz and infrared spectra of La1–xCa xMnO3 with x = 0.5; 0.6; 2/3, 0.7; 3/4, 0.85; 0.9; 0.95; 0.98 and x = 1 in the form of ceramics and epitaxial films. In the charge-ordered state for commensurate dopings (x = 2/3 and 3/4), we observed an absorption band at frequencies corresponding to the position of the lowest energy van Hove singularity in the folded Brillouin zone. The band is assigned to the boson peak. We observed qualitatively the same boson peak in Raman spectra of La1/3Ca2/3MnO3 ceramics. In antiferromagnetic phase, for the 0.5 ≤ x \\textless 0.85 range of doping, the conductivity mechanism gradually changes from a hopping-like transport at low temperatures to the Drude behavior at elevated temperatures in the paramagnetic phase. For 0.85 ≤ x \\textless 1 (canted antiferromagnetic phase), the electrons behave as Drude-like carriers in the whole temperature interval 5–300 K.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"yuzyuk-sakhovoy-maslova-shirokov-zakharchenko-belhadi-elmarssi-phasetransitionsinbatiotextrm3thinfilmsandbatiotextrm3bazrotextrm3superlattices-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.4901207\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'yuzyuk-sakhovoy-maslova-shirokov-zakharchenko-belhadi-elmarssi-phasetransitionsinbatiotextrm3thinfilmsandbatiotextrm3bazrotextrm3superlattices-2014', 'https://doi.org/10.1063/1.4901207', event);\">\n    Phase transitions in BaTiO$_{\\textrm{3}}$ thin films and BaTiO$_{\\textrm{3}}$/BaZrO$_{\\textrm{3}}$ superlattices.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Yuzyuk, Y. I.; Sakhovoy, R. A.; Maslova, O. A.; Shirokov, V. B.; Zakharchenko, I. N.; Belhadi, J.;  and El Marssi, M.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Applied Physics</i>, 116(18): 184102. November 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.4901207\"\n     onclick=\"log_download('yuzyuk-sakhovoy-maslova-shirokov-zakharchenko-belhadi-elmarssi-phasetransitionsinbatiotextrm3thinfilmsandbatiotextrm3bazrotextrm3superlattices-2014', 'https://doi.org/10.1063/1.4901207', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Phase transitions in BaTiO$_{\\textrm{3}}$ thin films and BaTiO$_{\\textrm{3}}$/BaZrO$_{\\textrm{3}}$ superlattices [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.4901207\"\n     onclick=\"log_download('yuzyuk-sakhovoy-maslova-shirokov-zakharchenko-belhadi-elmarssi-phasetransitionsinbatiotextrm3thinfilmsandbatiotextrm3bazrotextrm3superlattices-2014', 'http://doi.org/10.1063/1.4901207', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/yuzyuk-sakhovoy-maslova-shirokov-zakharchenko-belhadi-elmarssi-phasetransitionsinbatiotextrm3thinfilmsandbatiotextrm3bazrotextrm3superlattices-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('yuzyuk-sakhovoy-maslova-shirokov-zakharchenko-belhadi-elmarssi-phasetransitionsinbatiotextrm3thinfilmsandbatiotextrm3bazrotextrm3superlattices-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{yuzyuk_phase_2014,\n\ttitle = {Phase transitions in {BaTiO}$_{\\textrm{3}}$ thin films and {BaTiO}$_{\\textrm{3}}$/{BaZrO}$_{\\textrm{3}}$ superlattices},\n\tvolume = {116},\n\tissn = {0021-8979},\n\turl = {https://doi.org/10.1063/1.4901207},\n\tdoi = {10.1063/1.4901207},\n\tabstract = {Using pulsed laser deposition, we grew a ferroelectric [BaTiO3]Λ/2/[BaZrO3]Λ/2 (BT/BZ) superlattice with a stacking periodicity of Λ = 256 Å and a BT single film on a La1/2Sr1/2CoO3-buffered (001)MgO substrate, and then studied the phase transitions of these materials. At room temperature, the polarized Raman spectra of the BT film corresponded to a ferroelectric orthorhombic C2V14 phase with the polar axis oriented in the plane of the substrate. A ferroelectric-paraelectric phase transition in the BT film occurred at ∼450 K. Upon cooling to ∼300 K, a phase transition to the monoclinic Cs3 phase occurred. These experimental results agree well with a theoretical “temperature-misfit strain” phase diagram of the BT film. We found no evidence of phase transitions in the BT/BZ superlattice below room temperature. The phase transition to the paraelectric phase in the BT/BZ superlattice increased in temperature because of lattice mismatch between the BT and BZ layers. A desirable Curie temperature can be tailored rather precisely by varying the layer thicknesses or the BT/BZ ratio in the superlattice. The BT/BZ superlattices are very good for device applications because their ferroelectric phase with in-plane polarization can remain stable at least from 0 K up to 723 K, and even at higher temperatures in superlattices with smaller periodicities.},\n\tnumber = {18},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Applied Physics},\n\tauthor = {Yuzyuk, Yu. I. and Sakhovoy, R. A. and Maslova, O. A. and Shirokov, V. B. and Zakharchenko, I. N. and Belhadi, J. and El Marssi, M.},\n\tmonth = nov,\n\tyear = {2014},\n\tpages = {184102},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Using pulsed laser deposition, we grew a ferroelectric [BaTiO3]Λ/2/[BaZrO3]Λ/2 (BT/BZ) superlattice with a stacking periodicity of Λ = 256 Å and a BT single film on a La1/2Sr1/2CoO3-buffered (001)MgO substrate, and then studied the phase transitions of these materials. At room temperature, the polarized Raman spectra of the BT film corresponded to a ferroelectric orthorhombic C2V14 phase with the polar axis oriented in the plane of the substrate. A ferroelectric-paraelectric phase transition in the BT film occurred at ∼450 K. Upon cooling to ∼300 K, a phase transition to the monoclinic Cs3 phase occurred. These experimental results agree well with a theoretical “temperature-misfit strain” phase diagram of the BT film. We found no evidence of phase transitions in the BT/BZ superlattice below room temperature. The phase transition to the paraelectric phase in the BT/BZ superlattice increased in temperature because of lattice mismatch between the BT and BZ layers. A desirable Curie temperature can be tailored rather precisely by varying the layer thicknesses or the BT/BZ ratio in the superlattice. The BT/BZ superlattices are very good for device applications because their ferroelectric phase with in-plane polarization can remain stable at least from 0 K up to 723 K, and even at higher temperatures in superlattices with smaller periodicities.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-golovko-mukhortov-revinskii-opticalpropertiesofthebatextrm08srtextrm02tiotextrm3bitextrm082ndtextrm002feotextrm3superlattice-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1063784214040239\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-golovko-mukhortov-revinskii-opticalpropertiesofthebatextrm08srtextrm02tiotextrm3bitextrm082ndtextrm002feotextrm3superlattice-2014', 'https://doi.org/10.1134/S1063784214040239', event);\">\n    Optical properties of the Ba$_{\\textrm{0.8}}$Sr$_{\\textrm{0.2}}$TiO$_{\\textrm{3}}$/(Bi$_{\\textrm{0.82}}$, Nd$_{\\textrm{0.02}}$)FeO$_{\\textrm{3}}$ superlattice.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.; Golovko, Y. I.; Mukhortov, V. M.;  and Revinskii, Y. V.\n</span>\n\n  \n\n</span>\n\n  <i>Technical Physics</i>, 59(4): 571–575. April 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1063784214040239\"\n     onclick=\"log_download('shirokov-golovko-mukhortov-revinskii-opticalpropertiesofthebatextrm08srtextrm02tiotextrm3bitextrm082ndtextrm002feotextrm3superlattice-2014', 'https://doi.org/10.1134/S1063784214040239', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Optical properties of the Ba$_{\\textrm{0.8}}$Sr$_{\\textrm{0.2}}$TiO$_{\\textrm{3}}$/(Bi$_{\\textrm{0.82}}$, Nd$_{\\textrm{0.02}}$)FeO$_{\\textrm{3}}$ superlattice [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1063784214040239\"\n     onclick=\"log_download('shirokov-golovko-mukhortov-revinskii-opticalpropertiesofthebatextrm08srtextrm02tiotextrm3bitextrm082ndtextrm002feotextrm3superlattice-2014', 'http://doi.org/10.1134/S1063784214040239', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-golovko-mukhortov-revinskii-opticalpropertiesofthebatextrm08srtextrm02tiotextrm3bitextrm082ndtextrm002feotextrm3superlattice-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-golovko-mukhortov-revinskii-opticalpropertiesofthebatextrm08srtextrm02tiotextrm3bitextrm082ndtextrm002feotextrm3superlattice-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_optical_2014,\n\ttitle = {Optical properties of the {Ba}$_{\\textrm{0.8}}${Sr}$_{\\textrm{0.2}}${TiO}$_{\\textrm{3}}$/({Bi}$_{\\textrm{0.82}}$, {Nd}$_{\\textrm{0.02}}$){FeO}$_{\\textrm{3}}$ superlattice},\n\tvolume = {59},\n\tissn = {1090-6525},\n\turl = {https://doi.org/10.1134/S1063784214040239},\n\tdoi = {10.1134/S1063784214040239},\n\tabstract = {A Ba0.8Sr0.2TiO3/(Bi0.82, Nd0.02)FeO3 multilayer heteroepitaxial structure is prepared by successively depositing 20 Ba0.8Sr0.2TiO3 and (Bi0.82, Nd0.02)FeO3 layers, each 4 nm thick, using the method of rf sputtering. The layers grow on a single-crystal MgO substrate following the layer-by-layer mechanism. The structural perfection of the layers is examined by X-ray diffraction. The optical transmission is studied in the wavelength interval 200–1100 nm. The spectra are processed using a dispersion formula for the permittivity represented as a superposition of two oscillators with regard to relaxation. Such an approach allows us to separate direct and indirect transitions. The absorption edge of the superlattice for direct transitions is 80 nm wide and is estimated to be 3.78 eV.},\n\tlanguage = {en},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Technical Physics},\n\tauthor = {Shirokov, V. B. and Golovko, Yu. I. and Mukhortov, V. M. and Revinskii, Yu. V.},\n\tmonth = apr,\n\tyear = {2014},\n\tkeywords = {Barium Strontium, Barium Strontium Titanate, Multilayer Structure, Strontium Titanate, Wavelength Interval},\n\tpages = {571--575},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A Ba0.8Sr0.2TiO3/(Bi0.82, Nd0.02)FeO3 multilayer heteroepitaxial structure is prepared by successively depositing 20 Ba0.8Sr0.2TiO3 and (Bi0.82, Nd0.02)FeO3 layers, each 4 nm thick, using the method of rf sputtering. The layers grow on a single-crystal MgO substrate following the layer-by-layer mechanism. The structural perfection of the layers is examined by X-ray diffraction. The optical transmission is studied in the wavelength interval 200–1100 nm. The spectra are processed using a dispersion formula for the permittivity represented as a superposition of two oscillators with regard to relaxation. Such an approach allows us to separate direct and indirect transitions. The absorption edge of the superlattice for direct transitions is 80 nm wide and is estimated to be 3.78 eV.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"gagou-amira-lukyanchuk-mezzane-courty-masquelier-yuzyuk-elmarssi-onthenatureofphasetransitionsinthetetragonaltungstenbronzegdktextrm2nbtextrm5otextrm15ceramics-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.4865741\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'gagou-amira-lukyanchuk-mezzane-courty-masquelier-yuzyuk-elmarssi-onthenatureofphasetransitionsinthetetragonaltungstenbronzegdktextrm2nbtextrm5otextrm15ceramics-2014', 'https://doi.org/10.1063/1.4865741', event);\">\n    On the nature of phase transitions in the tetragonal tungsten bronze GdK$_{\\textrm{2}}$Nb$_{\\textrm{5}}$O$_{\\textrm{15}}$ ceramics.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Gagou, Y.; Amira, Y.; Lukyanchuk, I.; Mezzane, D.; Courty, M.; Masquelier, C.; Yuzyuk, Y. I.;  and El Marssi, M.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Applied Physics</i>, 115(6): 064104. February 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.4865741\"\n     onclick=\"log_download('gagou-amira-lukyanchuk-mezzane-courty-masquelier-yuzyuk-elmarssi-onthenatureofphasetransitionsinthetetragonaltungstenbronzegdktextrm2nbtextrm5otextrm15ceramics-2014', 'https://doi.org/10.1063/1.4865741', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"On the nature of phase transitions in the tetragonal tungsten bronze GdK$_{\\textrm{2}}$Nb$_{\\textrm{5}}$O$_{\\textrm{15}}$ ceramics [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.4865741\"\n     onclick=\"log_download('gagou-amira-lukyanchuk-mezzane-courty-masquelier-yuzyuk-elmarssi-onthenatureofphasetransitionsinthetetragonaltungstenbronzegdktextrm2nbtextrm5otextrm15ceramics-2014', 'http://doi.org/10.1063/1.4865741', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/gagou-amira-lukyanchuk-mezzane-courty-masquelier-yuzyuk-elmarssi-onthenatureofphasetransitionsinthetetragonaltungstenbronzegdktextrm2nbtextrm5otextrm15ceramics-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('gagou-amira-lukyanchuk-mezzane-courty-masquelier-yuzyuk-elmarssi-onthenatureofphasetransitionsinthetetragonaltungstenbronzegdktextrm2nbtextrm5otextrm15ceramics-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{gagou_nature_2014,\n\ttitle = {On the nature of phase transitions in the tetragonal tungsten bronze {GdK}$_{\\textrm{2}}${Nb}$_{\\textrm{5}}${O}$_{\\textrm{15}}$ ceramics},\n\tvolume = {115},\n\tissn = {0021-8979},\n\turl = {https://doi.org/10.1063/1.4865741},\n\tdoi = {10.1063/1.4865741},\n\tabstract = {Phase transitions in gadolinium potassium niobate GdK2Nb5O15 (GKN) ceramics have been investigated by x-ray diffraction, dielectric susceptibility, differential scanning calorimetry, and Raman scattering. The results of our complementary studies show that GKN exhibits two phase transitions at Tc1 = 238 °C and Tc2 = 375 °C attributed to the ferroelectric-antiferroelectric-paraelectric (FE-AFE-PE) phase transitions. According to the x-ray diffraction analysis, the FE and PE phases were refined in the polar P4bm and centrosymmetric P4/mbm space groups. For the intermediate phase, the structure is refined in the space group P4nc with doubling of the c unit cell parameter, which is compatible with an AFE phase. This result was confirmed by Raman spectroscopy since new low-frequency lines are activated in the AFE phase due to the Brillouin zone-folding effect, typical for the modulated phases. The presence of the AFE phase between the FE and PE phases and the complex nature of tetragonal tungsten bronze crystal structure can explain the large thermal hysteresis observed at the FE-AFE transition between heating and cooling cycle and the strong depression of the Curie-Weiss temperature T0. The semi-phenomenological Ising-like model based on the obtained experimental data is proposed to account for the observed FE-AFE-PE transition sequence.},\n\tnumber = {6},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Applied Physics},\n\tauthor = {Gagou, Y. and Amira, Y. and Lukyanchuk, I. and Mezzane, D. and Courty, M. and Masquelier, C. and Yuzyuk, Yu. I. and El Marssi, M.},\n\tmonth = feb,\n\tyear = {2014},\n\tpages = {064104},\n\tfile = {Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\4WTIXGZJ\\\\On-the-nature-of-phase-transitions-in-the.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Phase transitions in gadolinium potassium niobate GdK2Nb5O15 (GKN) ceramics have been investigated by x-ray diffraction, dielectric susceptibility, differential scanning calorimetry, and Raman scattering. The results of our complementary studies show that GKN exhibits two phase transitions at Tc1 = 238 °C and Tc2 = 375 °C attributed to the ferroelectric-antiferroelectric-paraelectric (FE-AFE-PE) phase transitions. According to the x-ray diffraction analysis, the FE and PE phases were refined in the polar P4bm and centrosymmetric P4/mbm space groups. For the intermediate phase, the structure is refined in the space group P4nc with doubling of the c unit cell parameter, which is compatible with an AFE phase. This result was confirmed by Raman spectroscopy since new low-frequency lines are activated in the AFE phase due to the Brillouin zone-folding effect, typical for the modulated phases. The presence of the AFE phase between the FE and PE phases and the complex nature of tetragonal tungsten bronze crystal structure can explain the large thermal hysteresis observed at the FE-AFE transition between heating and cooling cycle and the strong depression of the Curie-Weiss temperature T0. The semi-phenomenological Ising-like model based on the obtained experimental data is proposed to account for the observed FE-AFE-PE transition sequence.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"mikheykin-zhukova-torgashev-razumnaya-yuzyuk-gorshunov-prokhorov-sashin-etal-latticeanharmonicityandpolarsoftmodeinferrimagneticmtypehexaferritebafetextrm12otextrm19singlecrystal-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1140/epjb/e2014-50329-4\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'mikheykin-zhukova-torgashev-razumnaya-yuzyuk-gorshunov-prokhorov-sashin-etal-latticeanharmonicityandpolarsoftmodeinferrimagneticmtypehexaferritebafetextrm12otextrm19singlecrystal-2014', 'https://doi.org/10.1140/epjb/e2014-50329-4', event);\">\n    Lattice anharmonicity and polar soft mode in ferrimagnetic M-type hexaferrite BaFe$_{\\textrm{12}}$O$_{\\textrm{19}}$ single crystal.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Mikheykin, A. S.; Zhukova, E. S.; Torgashev, V. I.; Razumnaya, A. G.; Yuzyuk, Y. I.; Gorshunov, B. P.; Prokhorov, A. S.; Sashin, A. E.; Bush, A. A.;  and Dressel, M.\n</span>\n\n  \n\n</span>\n\n  <i>The European Physical Journal B</i>, 87(10): 232. October 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1140/epjb/e2014-50329-4\"\n     onclick=\"log_download('mikheykin-zhukova-torgashev-razumnaya-yuzyuk-gorshunov-prokhorov-sashin-etal-latticeanharmonicityandpolarsoftmodeinferrimagneticmtypehexaferritebafetextrm12otextrm19singlecrystal-2014', 'https://doi.org/10.1140/epjb/e2014-50329-4', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Lattice anharmonicity and polar soft mode in ferrimagnetic M-type hexaferrite BaFe$_{\\textrm{12}}$O$_{\\textrm{19}}$ single crystal [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1140/epjb/e2014-50329-4\"\n     onclick=\"log_download('mikheykin-zhukova-torgashev-razumnaya-yuzyuk-gorshunov-prokhorov-sashin-etal-latticeanharmonicityandpolarsoftmodeinferrimagneticmtypehexaferritebafetextrm12otextrm19singlecrystal-2014', 'http://doi.org/10.1140/epjb/e2014-50329-4', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/mikheykin-zhukova-torgashev-razumnaya-yuzyuk-gorshunov-prokhorov-sashin-etal-latticeanharmonicityandpolarsoftmodeinferrimagneticmtypehexaferritebafetextrm12otextrm19singlecrystal-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('mikheykin-zhukova-torgashev-razumnaya-yuzyuk-gorshunov-prokhorov-sashin-etal-latticeanharmonicityandpolarsoftmodeinferrimagneticmtypehexaferritebafetextrm12otextrm19singlecrystal-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{mikheykin_lattice_2014,\n\ttitle = {Lattice anharmonicity and polar soft mode in ferrimagnetic {M}-type hexaferrite {BaFe}$_{\\textrm{12}}${O}$_{\\textrm{19}}$ single crystal},\n\tvolume = {87},\n\tissn = {1434-6036},\n\turl = {https://doi.org/10.1140/epjb/e2014-50329-4},\n\tdoi = {10.1140/epjb/e2014-50329-4},\n\tabstract = {The polar phonon modes in BaFe12O19 single crystal are studied in the temperature rangefrom 6 to 300 K by polarized infrared spectroscopy. The phonon spectrum of the crystal isstrongly anharmonic and unstable with respect to long-wavelength fluctuations ofthe dielectric permittivity along the hexagonal axis. Our results suggests that inBaFe12O19 hexaferrite symmetry lowering to the polar phase withthe space group P63mc can beexpected.},\n\tlanguage = {en},\n\tnumber = {10},\n\turldate = {2023-11-11},\n\tjournal = {The European Physical Journal B},\n\tauthor = {Mikheykin, Alexey S. and Zhukova, Elena S. and Torgashev, Viktor I. and Razumnaya, Anna G. and Yuzyuk, Yury I. and Gorshunov, Boris P. and Prokhorov, Anatoly S. and Sashin, Aleksandr E. and Bush, Alexandr A. and Dressel, Martin},\n\tmonth = oct,\n\tyear = {2014},\n\tkeywords = {Solid State and Materials},\n\tpages = {232},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The polar phonon modes in BaFe12O19 single crystal are studied in the temperature rangefrom 6 to 300 K by polarized infrared spectroscopy. The phonon spectrum of the crystal isstrongly anharmonic and unstable with respect to long-wavelength fluctuations ofthe dielectric permittivity along the hexagonal axis. Our results suggests that inBaFe12O19 hexaferrite symmetry lowering to the polar phase withthe space group P63mc can beexpected.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"li-yao-yuzyuk-jia-wang-xie-jing-investigationsofbatextrmxsrtextrm1xtiotextrm3ceramicsandpowderspreparedbydirectcurrentarcdischargetechnique-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.4894456\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'li-yao-yuzyuk-jia-wang-xie-jing-investigationsofbatextrmxsrtextrm1xtiotextrm3ceramicsandpowderspreparedbydirectcurrentarcdischargetechnique-2014', 'https://doi.org/10.1063/1.4894456', event);\">\n    Investigations of Ba$_{\\textrm{x}}$Sr$_{\\textrm{1−x}}$TiO$_{\\textrm{3}}$ ceramics and powders prepared by direct current arc discharge technique.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Li, S.; Yao, Y.; Yuzyuk, Y. I.; Jia, Y.; Wang, X.; Xie, S.;  and Jing, Y.\n</span>\n\n  \n\n</span>\n\n  <i>Applied Physics Letters</i>, 105(9): 092901. September 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.4894456\"\n     onclick=\"log_download('li-yao-yuzyuk-jia-wang-xie-jing-investigationsofbatextrmxsrtextrm1xtiotextrm3ceramicsandpowderspreparedbydirectcurrentarcdischargetechnique-2014', 'https://doi.org/10.1063/1.4894456', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Investigations of Ba$_{\\textrm{x}}$Sr$_{\\textrm{1−x}}$TiO$_{\\textrm{3}}$ ceramics and powders prepared by direct current arc discharge technique [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.4894456\"\n     onclick=\"log_download('li-yao-yuzyuk-jia-wang-xie-jing-investigationsofbatextrmxsrtextrm1xtiotextrm3ceramicsandpowderspreparedbydirectcurrentarcdischargetechnique-2014', 'http://doi.org/10.1063/1.4894456', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/li-yao-yuzyuk-jia-wang-xie-jing-investigationsofbatextrmxsrtextrm1xtiotextrm3ceramicsandpowderspreparedbydirectcurrentarcdischargetechnique-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('li-yao-yuzyuk-jia-wang-xie-jing-investigationsofbatextrmxsrtextrm1xtiotextrm3ceramicsandpowderspreparedbydirectcurrentarcdischargetechnique-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{li_investigations_2014,\n\ttitle = {Investigations of {Ba}$_{\\textrm{x}}${Sr}$_{\\textrm{1−x}}${TiO}$_{\\textrm{3}}$ ceramics and powders prepared by direct current arc discharge technique},\n\tvolume = {105},\n\tissn = {0003-6951},\n\turl = {https://doi.org/10.1063/1.4894456},\n\tdoi = {10.1063/1.4894456},\n\tabstract = {BaxSr1−xTiO3 ceramics with x ranging from 0 to 1 were prepared by direct current arc discharge technique and studied by means of x-ray diffraction (XRD) and Raman spectroscopy. The cubic-tetragonal ferroelectric phase transition in BaxSr1−xTiO3 ceramics was found to occur at x ≈ 0.75. XRD investigation of as-grown BaTiO3 ceramics revealed co-existence of tetragonal and hexagonal modifications with a small amount of impurity phase BaTi4O9. No evidences of hexagonal phase were observed in Raman spectra of as-grown BaTiO3 ceramics, while Raman peaks related to hexagonal phase were clearly observed in the spectrum of fine-grain powders prepared from the same ceramics. A core-shell model for BaTiO3 ceramics prepared by direct current arc discharge technique is proposed. Absence of the hexagonal phase in any BaxSr1−xTiO3 solid solution with x \\&amp;lt; 1 is discussed in the frame of specific atomic arrangement.},\n\tnumber = {9},\n\turldate = {2023-11-11},\n\tjournal = {Applied Physics Letters},\n\tauthor = {Li, Shuangbin and Yao, Ying and Yuzyuk, Yu. I. and Jia, Yongzhong and Wang, Xiaohan and Xie, Shaolei and Jing, Yan},\n\tmonth = sep,\n\tyear = {2014},\n\tpages = {092901},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  BaxSr1−xTiO3 ceramics with x ranging from 0 to 1 were prepared by direct current arc discharge technique and studied by means of x-ray diffraction (XRD) and Raman spectroscopy. The cubic-tetragonal ferroelectric phase transition in BaxSr1−xTiO3 ceramics was found to occur at x ≈ 0.75. XRD investigation of as-grown BaTiO3 ceramics revealed co-existence of tetragonal and hexagonal modifications with a small amount of impurity phase BaTi4O9. No evidences of hexagonal phase were observed in Raman spectra of as-grown BaTiO3 ceramics, while Raman peaks related to hexagonal phase were clearly observed in the spectrum of fine-grain powders prepared from the same ceramics. A core-shell model for BaTiO3 ceramics prepared by direct current arc discharge technique is proposed. Absence of the hexagonal phase in any BaxSr1−xTiO3 solid solution with x &lt; 1 is discussed in the frame of specific atomic arrangement.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"belhadi-elmarssi-gagou-yuzyuk-elmendili-raevski-bouyanfif-wolfman-highlyconstrainedferroelectricbatiotextrm3textrm1xbazrotextrm3textrmxsuperlatticesxraydiffractionandramanspectroscopy-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.4890513\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'belhadi-elmarssi-gagou-yuzyuk-elmendili-raevski-bouyanfif-wolfman-highlyconstrainedferroelectricbatiotextrm3textrm1xbazrotextrm3textrmxsuperlatticesxraydiffractionandramanspectroscopy-2014', 'https://doi.org/10.1063/1.4890513', event);\">\n    Highly constrained ferroelectric [BaTiO$_{\\textrm{3}}$]$_{\\textrm{(1−x)Λ}}$/[BaZrO$_{\\textrm{3}}$]$_{\\textrm{{xΛ}}}$ superlattices: X-ray diffraction and Raman spectroscopy.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Belhadi, J.; El Marssi, M.; Gagou, Y.; Yuzyuk, Y. I.; El Mendili, Y.; Raevski, I. P.; Bouyanfif, H.;  and Wolfman, J.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Applied Physics</i>, 116(3): 034108. July 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.4890513\"\n     onclick=\"log_download('belhadi-elmarssi-gagou-yuzyuk-elmendili-raevski-bouyanfif-wolfman-highlyconstrainedferroelectricbatiotextrm3textrm1xbazrotextrm3textrmxsuperlatticesxraydiffractionandramanspectroscopy-2014', 'https://doi.org/10.1063/1.4890513', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Highly constrained ferroelectric [BaTiO$_{\\textrm{3}}$]$_{\\textrm{(1−x)Λ}}$/[BaZrO$_{\\textrm{3}}$]$_{\\textrm{{xΛ}}}$ superlattices: X-ray diffraction and Raman spectroscopy [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.4890513\"\n     onclick=\"log_download('belhadi-elmarssi-gagou-yuzyuk-elmendili-raevski-bouyanfif-wolfman-highlyconstrainedferroelectricbatiotextrm3textrm1xbazrotextrm3textrmxsuperlatticesxraydiffractionandramanspectroscopy-2014', 'http://doi.org/10.1063/1.4890513', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/belhadi-elmarssi-gagou-yuzyuk-elmendili-raevski-bouyanfif-wolfman-highlyconstrainedferroelectricbatiotextrm3textrm1xbazrotextrm3textrmxsuperlatticesxraydiffractionandramanspectroscopy-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('belhadi-elmarssi-gagou-yuzyuk-elmendili-raevski-bouyanfif-wolfman-highlyconstrainedferroelectricbatiotextrm3textrm1xbazrotextrm3textrmxsuperlatticesxraydiffractionandramanspectroscopy-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{belhadi_highly_2014,\n\ttitle = {Highly constrained ferroelectric [{BaTiO}$_{\\textrm{3}}$]$_{\\textrm{(1−x)Λ}}$/[{BaZrO}$_{\\textrm{3}}$]$_{\\textrm{{xΛ}}}$ superlattices: {X}-ray diffraction and {Raman} spectroscopy},\n\tvolume = {116},\n\tissn = {0021-8979},\n\tshorttitle = {Highly constrained ferroelectric [{BaTiO3}](1−x)Λ/[{BaZrO3}]{xΛ} superlattices},\n\turl = {https://doi.org/10.1063/1.4890513},\n\tdoi = {10.1063/1.4890513},\n\tabstract = {We report an x-ray diffraction (XRD) and a Raman-scattering investigation of ferroelectric/paraelectric superlattices [BaTiO3] (1−x)Λ/[BaZrO3]xΛ for which the composition varied, 0.15 ≤ x ≤ 0.85, while the superlattice (SL) modulation period Λ was kept constant at about 100 Å. The samples were epitaxially grown by pulsed laser deposition on MgO substrates buffered with La0.5Sr0.5CoO3. Based on the XRD analysis and on polarized Raman spectra, we have showed that the large strain in SLs induced ferroelectricity in BaZrO3 (BZ) for all SLs, a material that is paraelectric in the bulk form at any temperature and in the single film. The induced polar axis in BZ layers is perpendicular to the plane of substrate while BaTiO3 (BT) layers exhibit in-plane polar orientation. Raman spectroscopy revealed a lattice ordering in SLs due to the misfit strain generated by the large lattice mismatch between the alternating BZ and BT layers. This strain induced a huge upward frequency of the lowest E(1TO) soft mode from 60 cm−1 in the BT single film to 215 cm−1 in the SL with x = 0.85. These results show that in spite of relatively large periodicity of SLs, they are highly constrained and the variation of BZ ratio allowed modifying strains between layers. The temperature dependence of the Raman spectra for BT0.3Λ/BZ0.7Λ and BT0.7Λ/BZ0.3Λ samples revealed giant shift of the ferroelectric phase transition. The phase transition temperature was found to be upshifted by about 300 °C with respect to BT single crystal.},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Applied Physics},\n\tauthor = {Belhadi, J. and El Marssi, M. and Gagou, Y. and Yuzyuk, Yu. I. and El Mendili, Y. and Raevski, I. P. and Bouyanfif, H. and Wolfman, J.},\n\tmonth = jul,\n\tyear = {2014},\n\tpages = {034108},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We report an x-ray diffraction (XRD) and a Raman-scattering investigation of ferroelectric/paraelectric superlattices [BaTiO3] (1−x)Λ/[BaZrO3]xΛ for which the composition varied, 0.15 ≤ x ≤ 0.85, while the superlattice (SL) modulation period Λ was kept constant at about 100 Å. The samples were epitaxially grown by pulsed laser deposition on MgO substrates buffered with La0.5Sr0.5CoO3. Based on the XRD analysis and on polarized Raman spectra, we have showed that the large strain in SLs induced ferroelectricity in BaZrO3 (BZ) for all SLs, a material that is paraelectric in the bulk form at any temperature and in the single film. The induced polar axis in BZ layers is perpendicular to the plane of substrate while BaTiO3 (BT) layers exhibit in-plane polar orientation. Raman spectroscopy revealed a lattice ordering in SLs due to the misfit strain generated by the large lattice mismatch between the alternating BZ and BT layers. This strain induced a huge upward frequency of the lowest E(1TO) soft mode from 60 cm−1 in the BT single film to 215 cm−1 in the SL with x = 0.85. These results show that in spite of relatively large periodicity of SLs, they are highly constrained and the variation of BZ ratio allowed modifying strains between layers. The temperature dependence of the Raman spectra for BT0.3Λ/BZ0.7Λ and BT0.7Λ/BZ0.3Λ samples revealed giant shift of the ferroelectric phase transition. The phase transition temperature was found to be upshifted by about 300 °C with respect to BT single crystal.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"belhadi-marssi-gagou-yuzyuk-raevski-giantincreaseofferroelectricphasetransitiontemperatureinhighlystrainedferroelectricbatiotextrm3textrm07bazrotextrm3textrm03superlattice-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1209/0295-5075/106/17004\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'belhadi-marssi-gagou-yuzyuk-raevski-giantincreaseofferroelectricphasetransitiontemperatureinhighlystrainedferroelectricbatiotextrm3textrm07bazrotextrm3textrm03superlattice-2014', 'https://dx.doi.org/10.1209/0295-5075/106/17004', event);\">\n    Giant increase of ferroelectric phase transition temperature in highly strained ferroelectric [BaTiO$_{\\textrm{3}}$]$_{\\textrm{0.{7Λ}}}$/[BaZrO$_{\\textrm{3}}$]$_{\\textrm{0.{3Λ}}}$ superlattice.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Belhadi, J.; Marssi, M. E.; Gagou, Y.; Yuzyuk, Y. I.;  and Raevski, I. P.\n</span>\n\n  \n\n</span>\n\n  <i>Europhysics Letters</i>, 106(1): 17004. April 2014.\n  <span class=\"note\">Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1209/0295-5075/106/17004\"\n     onclick=\"log_download('belhadi-marssi-gagou-yuzyuk-raevski-giantincreaseofferroelectricphasetransitiontemperatureinhighlystrainedferroelectricbatiotextrm3textrm07bazrotextrm3textrm03superlattice-2014', 'https://dx.doi.org/10.1209/0295-5075/106/17004', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Giant increase of ferroelectric phase transition temperature in highly strained ferroelectric [BaTiO$_{\\textrm{3}}$]$_{\\textrm{0.{7Λ}}}$/[BaZrO$_{\\textrm{3}}$]$_{\\textrm{0.{3Λ}}}$ superlattice [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1209/0295-5075/106/17004\"\n     onclick=\"log_download('belhadi-marssi-gagou-yuzyuk-raevski-giantincreaseofferroelectricphasetransitiontemperatureinhighlystrainedferroelectricbatiotextrm3textrm07bazrotextrm3textrm03superlattice-2014', 'http://doi.org/10.1209/0295-5075/106/17004', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/belhadi-marssi-gagou-yuzyuk-raevski-giantincreaseofferroelectricphasetransitiontemperatureinhighlystrainedferroelectricbatiotextrm3textrm07bazrotextrm3textrm03superlattice-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('belhadi-marssi-gagou-yuzyuk-raevski-giantincreaseofferroelectricphasetransitiontemperatureinhighlystrainedferroelectricbatiotextrm3textrm07bazrotextrm3textrm03superlattice-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{belhadi_giant_2014,\n\ttitle = {Giant increase of ferroelectric phase transition temperature in highly strained ferroelectric [{BaTiO}$_{\\textrm{3}}$]$_{\\textrm{0.{7Λ}}}$/[{BaZrO}$_{\\textrm{3}}$]$_{\\textrm{0.{3Λ}}}$ superlattice},\n\tvolume = {106},\n\tissn = {0295-5075},\n\turl = {https://dx.doi.org/10.1209/0295-5075/106/17004},\n\tdoi = {10.1209/0295-5075/106/17004},\n\tabstract = {We report epitaxial strain effects in the lead-free ferroelectric/paraelectric superlattice (SL) for a modulation period Λ of about 100 Å. We have demonstrated that the large strain in SL induces ferroelectricity in BaZrO3 layers, a material that is paraelectric at any temperature in the bulk form. The induced polar axis in BaZrO3 layers is perpendicular to the plane of the substrate while BaTiO3 layers exhibit in-plane polar orientation. Raman spectroscopy revealed a lattice ordering in SL due to the misfit strain generated by the large lattice mismatch between the alternating BaZrO3 and BaTiO3 layers. Such strain induces a huge upward frequency shift of the lowest E(1TO) soft mode from in the BaTiO3 single film to in the SL. The temperature of the ferroelectric phase transition in the SL was found to be upshifted by about with respect to the BaTiO3 single crystal.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Europhysics Letters},\n\tauthor = {Belhadi, J. and Marssi, M. El and Gagou, Y. and Yuzyuk, Yu I. and Raevski, I. P.},\n\tmonth = apr,\n\tyear = {2014},\n\tnote = {Publisher: EDP Sciences, IOP Publishing and Società Italiana di Fisica},\n\tpages = {17004},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We report epitaxial strain effects in the lead-free ferroelectric/paraelectric superlattice (SL) for a modulation period Λ of about 100 Å. We have demonstrated that the large strain in SL induces ferroelectricity in BaZrO3 layers, a material that is paraelectric at any temperature in the bulk form. The induced polar axis in BaZrO3 layers is perpendicular to the plane of the substrate while BaTiO3 layers exhibit in-plane polar orientation. Raman spectroscopy revealed a lattice ordering in SL due to the misfit strain generated by the large lattice mismatch between the alternating BaZrO3 and BaTiO3 layers. Such strain induces a huge upward frequency shift of the lowest E(1TO) soft mode from in the BaTiO3 single film to in the SL. The temperature of the ferroelectric phase transition in the SL was found to be upshifted by about with respect to the BaTiO3 single crystal.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kochur-kozakov-googlev-mikheykin-torgashev-bush-nikolskii-chemicalbondingandvalencestateof3dmetalionsinnitextrm1xcotextrmxcrtextrm2otextrm4spinelsfromxraydiffractionandxrayphotoelectronspectroscopydata-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0368204814001583\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kochur-kozakov-googlev-mikheykin-torgashev-bush-nikolskii-chemicalbondingandvalencestateof3dmetalionsinnitextrm1xcotextrmxcrtextrm2otextrm4spinelsfromxraydiffractionandxrayphotoelectronspectroscopydata-2014', 'https://www.sciencedirect.com/science/article/pii/S0368204814001583', event);\">\n    Chemical bonding and valence state of 3d-metal ions in Ni$_{\\textrm{1−x}}$Co$_{\\textrm{x}}$Cr$_{\\textrm{2}}$O$_{\\textrm{4}}$ spinels from X-ray diffraction and X-ray photoelectron spectroscopy data.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kochur, A. G.; Kozakov, A. T.; Googlev, K. A.; Mikheykin, A. S.; Torgashev, V. I.; Bush, A. A.;  and Nikolskii, A. V.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Electron Spectroscopy and Related Phenomena</i>, 195: 208–219. August 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0368204814001583\"\n     onclick=\"log_download('kochur-kozakov-googlev-mikheykin-torgashev-bush-nikolskii-chemicalbondingandvalencestateof3dmetalionsinnitextrm1xcotextrmxcrtextrm2otextrm4spinelsfromxraydiffractionandxrayphotoelectronspectroscopydata-2014', 'https://www.sciencedirect.com/science/article/pii/S0368204814001583', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Chemical bonding and valence state of 3d-metal ions in Ni$_{\\textrm{1−x}}$Co$_{\\textrm{x}}$Cr$_{\\textrm{2}}$O$_{\\textrm{4}}$ spinels from X-ray diffraction and X-ray photoelectron spectroscopy data [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.elspec.2014.07.010\"\n     onclick=\"log_download('kochur-kozakov-googlev-mikheykin-torgashev-bush-nikolskii-chemicalbondingandvalencestateof3dmetalionsinnitextrm1xcotextrmxcrtextrm2otextrm4spinelsfromxraydiffractionandxrayphotoelectronspectroscopydata-2014', 'http://doi.org/10.1016/j.elspec.2014.07.010', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kochur-kozakov-googlev-mikheykin-torgashev-bush-nikolskii-chemicalbondingandvalencestateof3dmetalionsinnitextrm1xcotextrmxcrtextrm2otextrm4spinelsfromxraydiffractionandxrayphotoelectronspectroscopydata-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kochur-kozakov-googlev-mikheykin-torgashev-bush-nikolskii-chemicalbondingandvalencestateof3dmetalionsinnitextrm1xcotextrmxcrtextrm2otextrm4spinelsfromxraydiffractionandxrayphotoelectronspectroscopydata-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kochur_chemical_2014,\n\ttitle = {Chemical bonding and valence state of 3d-metal ions in {Ni}$_{\\textrm{1−x}}${Co}$_{\\textrm{x}}${Cr}$_{\\textrm{2}}${O}$_{\\textrm{4}}$ spinels from {X}-ray diffraction and {X}-ray photoelectron spectroscopy data},\n\tvolume = {195},\n\tissn = {0368-2048},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0368204814001583},\n\tdoi = {10.1016/j.elspec.2014.07.010},\n\tabstract = {Ni1−xCoxCr2O4 solid solution samples with х=0, 0.005, 0.01, 0.02, 0.3, 0.5, 0.8 and 1 are studied by the methods of X-ray diffraction and X-ray photoelectron spectroscopy (XPS). Ni2p3/2,1/2, Co2p3/2,1/2, Cr2p3/2,1/2, and O1s spectra are measured. The spectra are calculated with allowance for multiplet splitting, crystal field, and charge-transfer effect. Ni2+ ions are found to be present in tetrahedral and octahedral positions. Relative numbers of Ni2+ ions in tetrahedral and octahedral sites are determined via fitting the experimental spectra with superposition of the spectra of Ni2+ ions calculated in tetrahedral and octahedral crystal field. Cobalt ions are bivalent and occupy mostly tetrahedral sites. Chromium ions are trivalent and occupy predominantly octahedral positions. However, due to a defective lattice, the samples may contain Cr ions in non-equivalent states, either chemically or structurally.},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Electron Spectroscopy and Related Phenomena},\n\tauthor = {Kochur, A. G. and Kozakov, A. T. and Googlev, K. A. and Mikheykin, A. S. and Torgashev, V. I. and Bush, A. A. and Nikolskii, A. V.},\n\tmonth = aug,\n\tyear = {2014},\n\tkeywords = {X-ray diffraction, Crystal structure, NiCoCrO spinels, Valence state, XPS},\n\tpages = {208--219},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Ni1−xCoxCr2O4 solid solution samples with х=0, 0.005, 0.01, 0.02, 0.3, 0.5, 0.8 and 1 are studied by the methods of X-ray diffraction and X-ray photoelectron spectroscopy (XPS). Ni2p3/2,1/2, Co2p3/2,1/2, Cr2p3/2,1/2, and O1s spectra are measured. The spectra are calculated with allowance for multiplet splitting, crystal field, and charge-transfer effect. Ni2+ ions are found to be present in tetrahedral and octahedral positions. Relative numbers of Ni2+ ions in tetrahedral and octahedral sites are determined via fitting the experimental spectra with superposition of the spectra of Ni2+ ions calculated in tetrahedral and octahedral crystal field. Cobalt ions are bivalent and occupy mostly tetrahedral sites. Chromium ions are trivalent and occupy predominantly octahedral positions. However, due to a defective lattice, the samples may contain Cr ions in non-equivalent states, either chemically or structurally.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----zno-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/27360\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----zno-2014', 'http://journals.ioffe.ru/articles/27360', event);\">\n    Экспериментальное и теоретическое исследование массивов наностержней ZnO, покрытых пленкой серебра, как антенн оптического и ближнего ИК-диапазона.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Кайдашев, Е. М.; Лянгузов, Н. В.; Лерер, А. М.;  and Распопова, Е. А.\n</span>\n\n  \n\n</span>\n\n  <i>Письма в ЖТФ</i>, 40(7): 79–86. March 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/27360\"\n     onclick=\"log_download('----zno-2014', 'http://journals.ioffe.ru/articles/27360', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Экспериментальное и теоретическое исследование массивов наностержней ZnO, покрытых пленкой серебра, как антенн оптического и ближнего ИК-диапазона [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----zno-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----zno-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2014-4,\n\ttitle = {Экспериментальное и теоретическое исследование массивов наностержней {ZnO}, покрытых пленкой серебра, как антенн оптического и ближнего ИК-диапазона},\n\tvolume = {40},\n\turl = {http://journals.ioffe.ru/articles/27360},\n\tabstract = {Предложена новая конструкция оптической антенны - наностержень ZnO, покрытый тонкой металлической пленкой. Методами карботермического синтеза и магнетронного напыления получены решетки высокоориентированных перпендикулярно подложке наностержней оксида цинка, покрытых тонкой пленкой серебра. Решены задачи дифракции электромагнитных волн на одиночном металлодиэлектрическом нановибраторе, расположенном на границе раздела диэлектриков и на двумерно-периодической решетке нановибраторов. Проведено сравнение расчетов электродинамических характеристик оптических наноантенн различной длины с экспериментально полученными.},\n\tlanguage = {ru},\n\tnumber = {7},\n\turldate = {2023-11-11},\n\tjournal = {Письма в ЖТФ},\n\tauthor = {Кайдашев, Е. М. and Лянгузов, Н. В. and Лерер, А. М. and Распопова, Е. А.},\n\tmonth = mar,\n\tyear = {2014},\n\tpages = {79--86},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Предложена новая конструкция оптической антенны - наностержень ZnO, покрытый тонкой металлической пленкой. Методами карботермического синтеза и магнетронного напыления получены решетки высокоориентированных перпендикулярно подложке наностержней оксида цинка, покрытых тонкой пленкой серебра. Решены задачи дифракции электромагнитных волн на одиночном металлодиэлектрическом нановибраторе, расположенном на границе раздела диэлектриков и на двумерно-периодической решетке нановибраторов. Проведено сравнение расчетов электродинамических характеристик оптических наноантенн различной длины с экспериментально полученными.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---marssi-jain-ortega-katiyar--2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/26768\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---marssi-jain-ortega-katiyar--2014', 'http://journals.ioffe.ru/articles/26768', event);\">\n    Исследование динамики решетки макро-, микро- и наноструктурированного титаната бария методом спектроскопии комбинационного рассеяния света.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Маслова, О. А.; Широков, В. Б.; Юзюк, Ю. И.; Marssi, M. E.; Jain, M.; Ortega, N.;  and Katiyar, R. S.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 56(2): 308–314. January 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/26768\"\n     onclick=\"log_download('---marssi-jain-ortega-katiyar--2014', 'http://journals.ioffe.ru/articles/26768', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Исследование динамики решетки макро-, микро- и наноструктурированного титаната бария методом спектроскопии комбинационного рассеяния света [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---marssi-jain-ortega-katiyar--2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---marssi-jain-ortega-katiyar--2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2014-5,\n\ttitle = {Исследование динамики решетки макро-, микро- и наноструктурированного титаната бария методом спектроскопии комбинационного рассеяния света},\n\tvolume = {56},\n\turl = {http://journals.ioffe.ru/articles/26768},\n\tlanguage = {ru},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Маслова, О. А. and Широков, В. Б. and Юзюк, Ю. И. and Marssi, M. El and Jain, M. and Ortega, N. and Katiyar, R. S.},\n\tmonth = jan,\n\tyear = {2014},\n\tpages = {308--314},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-------2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=21184158\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-------2014', 'https://elibrary.ru/item.asp?id=21184158', event);\">\n    Переключение поляризации в наноразмерных пленках титаната бария стронция.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Мухортов, В. М.; Сова, Е. М.; Широков, В. Б.; Головко, Ю. И.; Лянгузов, Н. В.;  and Юзюк, Ю. И.\n</span>\n\n  \n\n</span>\n\n  <i>Российские Нанотехнологии</i>, 9(1-2): 55–58.  2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=21184158\"\n     onclick=\"log_download('-------2014', 'https://elibrary.ru/item.asp?id=21184158', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Переключение поляризации в наноразмерных пленках титаната бария стронция [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-------2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-------2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2014-6,\n\ttitle = {Переключение поляризации в наноразмерных пленках титаната бария стронция},\n\tvolume = {9},\n\tissn = {1992-7223, 1993-4068},\n\turl = {https://elibrary.ru/item.asp?id=21184158},\n\tabstract = {Исследовано переключение поляризации сегнетоэлектрических тонких пленок Ba0.8Sr0.2TiO3 толщиной 2–150 нм, осажденных на Si(111) с Pt подслоем. Критическим параметром при переключении поляризации является площадь сегнетоэлектрического кристаллита. Пленки толщиной 2 нм обладают сегнетоэлектрическими свойствами.Polarization switching in Ba0.8Sr0.2TiO3 ferroelectric 2–150 nm-thick thin films deposited on Pt coated Si(111) substrates was studied. The area of the ferroelectric crystallite is shown to be a critical parameter for polarization switching. The 2 nm-thick films possess ferroelectric properties.},\n\tlanguage = {ru},\n\tnumber = {1-2},\n\turldate = {2023-11-11},\n\tjournal = {Российские Нанотехнологии},\n\tauthor = {Мухортов, В. М. and Сова, Е. М. and Широков, В. Б. and Головко, Ю. И. and Лянгузов, Н. В. and Юзюк, Ю. И.},\n\tyear = {2014},\n\tkeywords = {Кристаллит, Наноразмер, Наноразмерная Пленка, Поляризация, Сегнетоэлектрический, Титанат Бария Стронция, ⛔ No DOI found},\n\tpages = {55--58},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследовано переключение поляризации сегнетоэлектрических тонких пленок Ba0.8Sr0.2TiO3 толщиной 2–150 нм, осажденных на Si(111) с Pt подслоем. Критическим параметром при переключении поляризации является площадь сегнетоэлектрического кристаллита. Пленки толщиной 2 нм обладают сегнетоэлектрическими свойствами.Polarization switching in Ba0.8Sr0.2TiO3 ferroelectric 2–150 nm-thick thin films deposited on Pt coated Si(111) substrates was studied. The area of the ferroelectric crystallite is shown to be a critical parameter for polarization switching. The 2 nm-thick films possess ferroelectric properties.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----latextrm07srtextrm03mnotextrm3sbtextrm2otextrm3-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/41214\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----latextrm07srtextrm03mnotextrm3sbtextrm2otextrm3-2014', 'http://journals.ioffe.ru/articles/41214', event);\">\n    Магниторезистивность стеклокомпозитов La$_{\\textrm{0.7}}$Sr$_{\\textrm{0.3}}$MnO$_{\\textrm{3}}$/ Sb$_{\\textrm{2}}$O$_{\\textrm{3}}$ при комнатной температуре.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Кабиров, Ю. В.; Гавриляченко, В. Г.; Чупахина, Т. И.;  and Гавриляченко, Т. В.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 57(1): 16–18. December 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/41214\"\n     onclick=\"log_download('----latextrm07srtextrm03mnotextrm3sbtextrm2otextrm3-2014', 'http://journals.ioffe.ru/articles/41214', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Магниторезистивность стеклокомпозитов La$_{\\textrm{0.7}}$Sr$_{\\textrm{0.3}}$MnO$_{\\textrm{3}}$/ Sb$_{\\textrm{2}}$O$_{\\textrm{3}}$ при комнатной температуре [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----latextrm07srtextrm03mnotextrm3sbtextrm2otextrm3-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----latextrm07srtextrm03mnotextrm3sbtextrm2otextrm3-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2014-7,\n\ttitle = {Магниторезистивность стеклокомпозитов {La}$_{\\textrm{0.7}}${Sr}$_{\\textrm{0.3}}${MnO}$_{\\textrm{3}}$/ {Sb}$_{\\textrm{2}}${O}$_{\\textrm{3}}$ при комнатной температуре},\n\tvolume = {57},\n\turl = {http://journals.ioffe.ru/articles/41214},\n\tabstract = {Синтезированы керамические композиты La0.7Sr0.3MnO3/Sb2O3 с различными массовыми соотношениями компонентов. Исследованы их магниторезистивные свойства в слабых магнитных полях. Значения отрицательной изотропной магниторезистивности при комнатной температуре для композитов 90\\% La0.7Sr0.3MnO3/10\\%Sb2O3 составляют -1.2\\% при 0.25 kOe и -14\\% при 20 kOe. Рост магниторезистивности при увеличении поля имеет черты релаксационного процесса. Работа выполнена при финансовой поддержке проекта РФФИ N 14-03-00103.},\n\tlanguage = {ru},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Чупахина, Т. И. and Гавриляченко, Т. В.},\n\tmonth = dec,\n\tyear = {2014},\n\tpages = {16--18},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Синтезированы керамические композиты La0.7Sr0.3MnO3/Sb2O3 с различными массовыми соотношениями компонентов. Исследованы их магниторезистивные свойства в слабых магнитных полях. Значения отрицательной изотропной магниторезистивности при комнатной температуре для композитов 90% La0.7Sr0.3MnO3/10%Sb2O3 составляют -1.2% при 0.25 kOe и -14% при 20 kOe. Рост магниторезистивности при увеличении поля имеет черты релаксационного процесса. Работа выполнена при финансовой поддержке проекта РФФИ N 14-03-00103.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-------zno-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/26806\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-------zno-2014', 'http://journals.ioffe.ru/articles/26806', event);\">\n    Особенности оптических фононов в спектрах комбинационного рассеяния массива вертикальных микростержней ZnO на кремнии.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Лянгузов, Н. В.; Анохин, А. С.; Левшов, Д. И.; Кайдашев, Е. М.; Юзюк, Ю. И.; Захарченко, И. Н.;  and Бунина, О. А.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 56(3): 542–548. February 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/26806\"\n     onclick=\"log_download('-------zno-2014', 'http://journals.ioffe.ru/articles/26806', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Особенности оптических фононов в спектрах комбинационного рассеяния массива вертикальных микростержней ZnO на кремнии [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-------zno-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-------zno-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2014-8,\n\ttitle = {Особенности оптических фононов в спектрах комбинационного рассеяния массива вертикальных микростержней {ZnO} на кремнии},\n\tvolume = {56},\n\turl = {http://journals.ioffe.ru/articles/26806},\n\tabstract = {Исследованы поляризованные спектры комбинационного рассеяния массива вертикальных микростержней оксида цинка, синтезированного карботермическим методом на подложке Si (001). Длина стержней составляет 9±0.5 mum, а диаметр - 210±50 nm. Рентгенографические исследования подтвердили взаимную кристаллографическую ориентацию [001]ZnO{\\textbar}{\\textbar}[001]Si в направлении нормали к плоскости подложки. В спектрах комбинационного рассеяния света стержней наблюдаются запрещенные правилами отбора для монокристалла в геометрии x(yz)x-моды A1(TO) и Ehigh2 и в геометрии x(zz)x-мода E1(LO). Обнаружены квазимоды Q(TO) и Q(LO), спектральное положение которых смещается при изменении угла падения возбуждающего излучения. Путем сравнения спектрального сдвига квазимод с экспериментальными данными для монокристалла произведена оценка интервала углов распространения возбуждающего излучения в массиве стержней, составляющего {\\textasciitilde}25o при фиксированном угле падения. Работа выполнялась при финансовой поддержке Министерства образования и науки, тема N 2.5896 &quot;Развитие методов получения и исследование свойств полупроводниковых наноструктур для создания элементов устройств нанофотоники&quot;.},\n\tlanguage = {ru},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Лянгузов, Н. В. and Анохин, А. С. and Левшов, Д. И. and Кайдашев, Е. М. and Юзюк, Ю. И. and Захарченко, И. Н. and Бунина, О. А.},\n\tmonth = feb,\n\tyear = {2014},\n\tpages = {542--548},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследованы поляризованные спектры комбинационного рассеяния массива вертикальных микростержней оксида цинка, синтезированного карботермическим методом на подложке Si (001). Длина стержней составляет 9±0.5 mum, а диаметр - 210±50 nm. Рентгенографические исследования подтвердили взаимную кристаллографическую ориентацию [001]ZnO\\textbar\\textbar[001]Si в направлении нормали к плоскости подложки. В спектрах комбинационного рассеяния света стержней наблюдаются запрещенные правилами отбора для монокристалла в геометрии x(yz)x-моды A1(TO) и Ehigh2 и в геометрии x(zz)x-мода E1(LO). Обнаружены квазимоды Q(TO) и Q(LO), спектральное положение которых смещается при изменении угла падения возбуждающего излучения. Путем сравнения спектрального сдвига квазимод с экспериментальными данными для монокристалла произведена оценка интервала углов распространения возбуждающего излучения в массиве стержней, составляющего ~25o при фиксированном угле падения. Работа выполнялась при финансовой поддержке Министерства образования и науки, тема N 2.5896 \"Развитие методов получения и исследование свойств полупроводниковых наноструктур для создания элементов устройств нанофотоники\".\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"--------2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/26789\"\n     onclick=\"return trackOutboundLink('publications', 'click', '--------2014', 'http://journals.ioffe.ru/articles/26789', event);\">\n    Влияние редкоземельных ионов на диэлектрический отклик в стиллвеллитовых стеклах.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Командин, Г. А.; Торгашев, В. И.; Сигаев, В. Н.; Савинков, В. И.; Лотарев, С. В.; Породинков, О. Е.;  and Спектор, И. Е.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 56(3): 435–441. February 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/26789\"\n     onclick=\"log_download('--------2014', 'http://journals.ioffe.ru/articles/26789', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Влияние редкоземельных ионов на диэлектрический отклик в стиллвеллитовых стеклах [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/--------2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('--------2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2014-9,\n\ttitle = {Влияние редкоземельных ионов на диэлектрический отклик в стиллвеллитовых стеклах},\n\tvolume = {56},\n\turl = {http://journals.ioffe.ru/articles/26789},\n\tabstract = {Проведено сравнение экспериментально полученных спектров функции диэлектрического отклика стекол состава LnBGeO5 (Ln = La, Pr, Tb, Er, Sm) в терагерцевом и инфракрасном диапазонах. Выделены полосы поглощения и установлены их вклады в диэлектрическую проницаемость, определены контуры бозонного пика и зависимость диэлектрических потерь от типа редкоземельного иона. Работа выполнена при поддержке Министерства образования и науки РФ (грант N 11.G34.31.0027) и РФФИ (грант N 11-02-00810-а).},\n\tlanguage = {ru},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Командин, Г. А. and Торгашев, В. И. and Сигаев, В. Н. and Савинков, В. И. and Лотарев, С. В. and Породинков, О. Е. and Спектор, И. Е.},\n\tmonth = feb,\n\tyear = {2014},\n\tpages = {435--441},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Проведено сравнение экспериментально полученных спектров функции диэлектрического отклика стекол состава LnBGeO5 (Ln = La, Pr, Tb, Er, Sm) в терагерцевом и инфракрасном диапазонах. Выделены полосы поглощения и установлены их вклады в диэлектрическую проницаемость, определены контуры бозонного пика и зависимость диэлектрических потерь от типа редкоземельного иона. Работа выполнена при поддержке Министерства образования и науки РФ (грант N 11.G34.31.0027) и РФФИ (грант N 11-02-00810-а).\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------nitextrm1xcotextrmxcrtextrm2otextrm4-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/26843\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------nitextrm1xcotextrmxcrtextrm2otextrm4-2014', 'http://journals.ioffe.ru/articles/26843', event);\">\n    Особенности ян-теллеровского перехода в твердых растворах Ni$_{\\textrm{1-x}}$Co$_{\\textrm{x}}$Cr$_{\\textrm{2}}$O$_{\\textrm{4}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Михейкин, А. С.; Чернышов, Д. Ю.; Буш, А. А.; Прохоров, А. С.; Юзюк, Ю. И.;  and Дмитриев, В. П.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 56(4): 754–760. March 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/26843\"\n     onclick=\"log_download('------nitextrm1xcotextrmxcrtextrm2otextrm4-2014', 'http://journals.ioffe.ru/articles/26843', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Особенности ян-теллеровского перехода в твердых растворах Ni$_{\\textrm{1-x}}$Co$_{\\textrm{x}}$Cr$_{\\textrm{2}}$O$_{\\textrm{4}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------nitextrm1xcotextrmxcrtextrm2otextrm4-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------nitextrm1xcotextrmxcrtextrm2otextrm4-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2014-10,\n\ttitle = {Особенности ян-теллеровского перехода в твердых растворах {Ni}$_{\\textrm{1-x}}${Co}$_{\\textrm{x}}${Cr}$_{\\textrm{2}}${O}$_{\\textrm{4}}$},\n\tvolume = {56},\n\turl = {http://journals.ioffe.ru/articles/26843},\n\tabstract = {Методами синхротронной порошковой рентгеновской дифракции исследована структура твердых растворов Ni1-xCоxCr2O4 в температурном интервале 90-350 K для составов с x=0; 0.005; 0.01; 0.015; 0.02; 0.1; 0.5; 0.8 и проведено уточнение их структур с помощью полнопрофильного анализа Ритвельда. На основе полученных данных построена T-x-фазовая диаграмма для твердых растворов в исследованном диапазоне температур и концентраций. Обнаруженные структурные фазовые переходы объяснены с точки зрения теории кристаллического поля и кооперативного эффекта Яна-Теллера. Оценена величина искажений полиэдров, являющихся причиной структурного фазового перехода. Обсуждается применимость феноменологической теории Ландау и возможность использования в качестве параметра порядка величины спонтанных деформаций},\n\tlanguage = {ru},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Михейкин, А. С. and Чернышов, Д. Ю. and Буш, А. А. and Прохоров, А. С. and Юзюк, Ю. И. and Дмитриев, В. П.},\n\tmonth = mar,\n\tyear = {2014},\n\tpages = {754--760},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Методами синхротронной порошковой рентгеновской дифракции исследована структура твердых растворов Ni1-xCоxCr2O4 в температурном интервале 90-350 K для составов с x=0; 0.005; 0.01; 0.015; 0.02; 0.1; 0.5; 0.8 и проведено уточнение их структур с помощью полнопрофильного анализа Ритвельда. На основе полученных данных построена T-x-фазовая диаграмма для твердых растворов в исследованном диапазоне температур и концентраций. Обнаруженные структурные фазовые переходы объяснены с точки зрения теории кристаллического поля и кооперативного эффекта Яна-Теллера. Оценена величина искажений полиэдров, являющихся причиной структурного фазового перехода. Обсуждается применимость феноменологической теории Ландау и возможность использования в качестве параметра порядка величины спонтанных деформаций\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----gueye-carcan-bouyanfif-wolfman-etal--2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/41133\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----gueye-carcan-bouyanfif-wolfman-etal--2014', 'http://journals.ioffe.ru/articles/41133', event);\">\n    Фононные и магнонные возбуждения в спектрах комбинационного рассеяния света эпитаксиальной пленки феррита висмута.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Кхабири, Г.; Анохин, А. С.; Разумная, А. Г.; Юзюк, Ю. И.; Gueye, I.; Carcan, B.; Bouyanfif, H.; Wolfman, J.; Autret-Lambert, C.;  and El Marssi, M.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 56(12): 2420–2425. November 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/41133\"\n     onclick=\"log_download('----gueye-carcan-bouyanfif-wolfman-etal--2014', 'http://journals.ioffe.ru/articles/41133', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Фононные и магнонные возбуждения в спектрах комбинационного рассеяния света эпитаксиальной пленки феррита висмута [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----gueye-carcan-bouyanfif-wolfman-etal--2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----gueye-carcan-bouyanfif-wolfman-etal--2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2014-11,\n\ttitle = {Фононные и магнонные возбуждения в спектрах комбинационного рассеяния света эпитаксиальной пленки феррита висмута},\n\tvolume = {56},\n\turl = {http://journals.ioffe.ru/articles/41133},\n\tabstract = {Эпитаксиальная пленка феррита висмута BiFeO3 на монокристаллической подложке (001)MgO получена методом импульсного лазерного напыления с использованием буферных слоев SrTiO3 и SrRuO3. При комнатной температуре поляризационные характеристики спектров комбинационного рассеяния света исследованной пленки BiFeO3 предполагают моноклинную симметрию. Проведены высокотемпературные (295-1100 K) исследования спектров комбинационного рассеяния света в области частот 20{\\textless}nu{\\textless}1600 cm-1. Особое внимание уделено высокочастотной области, где наблюдаются полоса 610 cm-1, соответствующая максимуму плотности состояний магнонной ветви на границе зоны Бриллюэна, и интенсивная полоса в спектрах второго порядка с максимумом {\\textasciitilde}1250 cm-1, соответствующая плотности состояний двухмагнонных возбуждений. Установлено, что при повышении температуры интенсивность полосы {\\textasciitilde}1250 cm-1 линейно понижается и выше 650 K она отсутствует. Экстраполяция температурной зависимости интегральной интенсивности полосы 1250 cm-1 позволяет предполагать, что в данной пленке антиферромагнитный фазовый переход происходит при температуре {\\textasciitilde}670 K.},\n\tlanguage = {ru},\n\tnumber = {12},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Кхабири, Г. and Анохин, А. С. and Разумная, А. Г. and Юзюк, Ю. И. and Gueye, I. and Carcan, B. and Bouyanfif, H. and Wolfman, J. and Autret-Lambert, C. and El Marssi, M.},\n\tmonth = nov,\n\tyear = {2014},\n\tpages = {2420--2425},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Эпитаксиальная пленка феррита висмута BiFeO3 на монокристаллической подложке (001)MgO получена методом импульсного лазерного напыления с использованием буферных слоев SrTiO3 и SrRuO3. При комнатной температуре поляризационные характеристики спектров комбинационного рассеяния света исследованной пленки BiFeO3 предполагают моноклинную симметрию. Проведены высокотемпературные (295-1100 K) исследования спектров комбинационного рассеяния света в области частот 20\\textlessnu\\textless1600 cm-1. Особое внимание уделено высокочастотной области, где наблюдаются полоса 610 cm-1, соответствующая максимуму плотности состояний магнонной ветви на границе зоны Бриллюэна, и интенсивная полоса в спектрах второго порядка с максимумом ~1250 cm-1, соответствующая плотности состояний двухмагнонных возбуждений. Установлено, что при повышении температуры интенсивность полосы ~1250 cm-1 линейно понижается и выше 650 K она отсутствует. Экстраполяция температурной зависимости интегральной интенсивности полосы 1250 cm-1 позволяет предполагать, что в данной пленке антиферромагнитный фазовый переход происходит при температуре ~670 K.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----ortega-kumar-katiyar-batiotextrm3batextrm05srtextrm05tiotextrm3srtiotextrm3-2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/26811\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----ortega-kumar-katiyar-batiotextrm3batextrm05srtextrm05tiotextrm3srtiotextrm3-2014', 'http://journals.ioffe.ru/articles/26811', event);\">\n    Исследование сверхрешеток BaTiO$_{\\textrm{3}}$/(Ba$_{\\textrm{0.5}}$,Sr$_{\\textrm{0.5}}$)TiO$_{\\textrm{3}}$/ SrTiO$_{\\textrm{3}}$ методами рентгеновской дифракции и комбинационного рассеяния света.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Тихонов, Ю. А.; Захарченко, И. Н.; Маслова, О. А.; Юзюк, Ю. И.; Ortega, N.; Kumar, A.;  and Katiyar, R. S.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 56(3): 573–576. February 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/26811\"\n     onclick=\"log_download('----ortega-kumar-katiyar-batiotextrm3batextrm05srtextrm05tiotextrm3srtiotextrm3-2014', 'http://journals.ioffe.ru/articles/26811', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Исследование сверхрешеток BaTiO$_{\\textrm{3}}$/(Ba$_{\\textrm{0.5}}$,Sr$_{\\textrm{0.5}}$)TiO$_{\\textrm{3}}$/ SrTiO$_{\\textrm{3}}$ методами рентгеновской дифракции и комбинационного рассеяния света [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----ortega-kumar-katiyar-batiotextrm3batextrm05srtextrm05tiotextrm3srtiotextrm3-2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----ortega-kumar-katiyar-batiotextrm3batextrm05srtextrm05tiotextrm3srtiotextrm3-2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2014-12,\n\ttitle = {Исследование сверхрешеток {BaTiO}$_{\\textrm{3}}$/({Ba}$_{\\textrm{0.5}}$,{Sr}$_{\\textrm{0.5}}$){TiO}$_{\\textrm{3}}$/ {SrTiO}$_{\\textrm{3}}$ методами рентгеновской дифракции и комбинационного рассеяния света},\n\tvolume = {56},\n\turl = {http://journals.ioffe.ru/articles/26811},\n\tabstract = {Методами рентгеновской дифрактометрии определены структурные характеристики сверхрешетки BaTiO3/(Ba0.5,Sr0.5)TiO3/SrTiO3 на подложке (001) MgO. Получены период модуляции, параметры элементарных ячеек слоев, составляющих сверхрешетку, оценены величины областей когерентного рассеяния и средние микродеформации в направлении, перпендикулярном поверхности. Проведено сравнение с характеристиками двухслойной сверхрешетки BaTiO3/(Ba0.5,Sr0.5)TiO3. В спектрах комбинационного рассеяния света обнаружено существенное смещение мягкой E(TO)-моды в трехслойной сверхрешетке по сравнению с ее положением в двухслойной. Обнаруженные эффекты связываются с существенным увеличением температуры перехода трехслойной сверхрешетки в параэлектрическую фазу.},\n\tlanguage = {ru},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Тихонов, Ю. А. and Захарченко, И. Н. and Маслова, О. А. and Юзюк, Ю. И. and Ortega, N. and Kumar, A. and Katiyar, R. S.},\n\tmonth = feb,\n\tyear = {2014},\n\tpages = {573--576},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Методами рентгеновской дифрактометрии определены структурные характеристики сверхрешетки BaTiO3/(Ba0.5,Sr0.5)TiO3/SrTiO3 на подложке (001) MgO. Получены период модуляции, параметры элементарных ячеек слоев, составляющих сверхрешетку, оценены величины областей когерентного рассеяния и средние микродеформации в направлении, перпендикулярном поверхности. Проведено сравнение с характеристиками двухслойной сверхрешетки BaTiO3/(Ba0.5,Sr0.5)TiO3. В спектрах комбинационного рассеяния света обнаружено существенное смещение мягкой E(TO)-моды в трехслойной сверхрешетке по сравнению с ее положением в двухслойной. Обнаруженные эффекты связываются с существенным увеличением температуры перехода трехслойной сверхрешетки в параэлектрическую фазу.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---------2014\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/26909\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---------2014', 'http://journals.ioffe.ru/articles/26909', event);\">\n    Температурная эволюция спектров диэлектрического отклика стиллвеллитоподобных стекол в терагерцевом и инфракрасном диапазонах.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Командин, Г. А.; Породинков, О. Е.; Гончаров, Ю. Г.; Спектор, И. Е.; Исхакова, Л. Д.; Сигаев, В. Н.; Лотарев, С. В.;  and Торгашев, В. И.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 56(6): 1152–1157. May 2014.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/26909\"\n     onclick=\"log_download('---------2014', 'http://journals.ioffe.ru/articles/26909', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Температурная эволюция спектров диэлектрического отклика стиллвеллитоподобных стекол в терагерцевом и инфракрасном диапазонах [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---------2014\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---------2014')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2014-13,\n\ttitle = {Температурная эволюция спектров диэлектрического отклика стиллвеллитоподобных стекол в терагерцевом и инфракрасном диапазонах},\n\tvolume = {56},\n\turl = {http://journals.ioffe.ru/articles/26909},\n\tabstract = {Измерены спектры пропускания и отражения стекла PrBGeO5 в терагерцевом и инфракрасном диапазонах. При низких температурах зарегистрированы рост диэлектрической проницаемости и появление узких линий резонансного типа в терагерцевом диапазоне. Рассчитаны спектры комплексной диэлектрической проницаемости по формулам Френеля и Крамерса-Кронига.},\n\tlanguage = {ru},\n\tnumber = {6},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Командин, Г. А. and Породинков, О. Е. and Гончаров, Ю. Г. and Спектор, И. Е. and Исхакова, Л. Д. and Сигаев, В. Н. and Лотарев, С. В. and Торгашев, В. И.},\n\tmonth = may,\n\tyear = {2014},\n\tpages = {1152--1157},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Измерены спектры пропускания и отражения стекла PrBGeO5 в терагерцевом и инфракрасном диапазонах. При низких температурах зарегистрированы рост диэлектрической проницаемости и появление узких линий резонансного типа в терагерцевом диапазоне. Рассчитаны спектры комплексной диэлектрической проницаемости по формулам Френеля и Крамерса-Кронига.\n</div>\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2013\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2013')\"\n      onkeypress=\"toggleGroup('group_2013')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2013</span>\n      <span class=\"bibbase_group_count\">\n        \n        (35)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"rochal-lorman-yuzyuk-twodimensionalelasticitydeterminesthelowfrequencydynamicsofsingleanddoublewalledcarbonnanotubes-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.88.235435\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'rochal-lorman-yuzyuk-twodimensionalelasticitydeterminesthelowfrequencydynamicsofsingleanddoublewalledcarbonnanotubes-2013', 'https://link.aps.org/doi/10.1103/PhysRevB.88.235435', event);\">\n    Two-dimensional elasticity determines the low-frequency dynamics of single- and double-walled carbon nanotubes.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Rochal, S. B.; Lorman, V. L.;  and Yuzyuk, Y. I.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 88(23): 235435. December 2013.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.88.235435\"\n     onclick=\"log_download('rochal-lorman-yuzyuk-twodimensionalelasticitydeterminesthelowfrequencydynamicsofsingleanddoublewalledcarbonnanotubes-2013', 'https://link.aps.org/doi/10.1103/PhysRevB.88.235435', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Two-dimensional elasticity determines the low-frequency dynamics of single- and double-walled carbon nanotubes [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.88.235435\"\n     onclick=\"log_download('rochal-lorman-yuzyuk-twodimensionalelasticitydeterminesthelowfrequencydynamicsofsingleanddoublewalledcarbonnanotubes-2013', 'http://doi.org/10.1103/PhysRevB.88.235435', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/rochal-lorman-yuzyuk-twodimensionalelasticitydeterminesthelowfrequencydynamicsofsingleanddoublewalledcarbonnanotubes-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('rochal-lorman-yuzyuk-twodimensionalelasticitydeterminesthelowfrequencydynamicsofsingleanddoublewalledcarbonnanotubes-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{rochal_two-dimensional_2013,\n\ttitle = {Two-dimensional elasticity determines the low-frequency dynamics of single- and double-walled carbon nanotubes},\n\tvolume = {88},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.88.235435},\n\tdoi = {10.1103/PhysRevB.88.235435},\n\tabstract = {We develop a continuous theory of low-frequency dynamics for nanotubes with walls constituted by single-atom monolayer, the topological elasticity of which is not related to its vanishing macroscopic thickness. The applicability region of the theory proposed includes all truly two-dimensional materials such as graphene and MoS2. New comprehensive interpretation and analytical expressions for low-frequency modes in single-walled carbon nanotube (SWCNT) are given. The theory unambiguously relates the radial breathing modes of SWCNT and breathinglike modes of the double-walled carbon nanotube (DWCNT). The existing Raman data on DWCNTs are fitted better than in the frame of previous models.},\n\tnumber = {23},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Rochal, S. B. and Lorman, V. L. and Yuzyuk, Yu. I.},\n\tmonth = dec,\n\tyear = {2013},\n\tnote = {Publisher: American Physical Society},\n\tpages = {235435},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\IBZ3DB87\\\\Rochal и др. - 2013 - Two-dimensional elasticity determines the low-freq.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We develop a continuous theory of low-frequency dynamics for nanotubes with walls constituted by single-atom monolayer, the topological elasticity of which is not related to its vanishing macroscopic thickness. The applicability region of the theory proposed includes all truly two-dimensional materials such as graphene and MoS2. New comprehensive interpretation and analytical expressions for low-frequency modes in single-walled carbon nanotube (SWCNT) are given. The theory unambiguously relates the radial breathing modes of SWCNT and breathinglike modes of the double-walled carbon nanotube (DWCNT). The existing Raman data on DWCNTs are fitted better than in the frame of previous models.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"leontyeva-leontyev-avramenko-yuzyuk-kukushkina-smirnova-electrochemicaldispergationasasimpleandeffectivetechniquetowardpreparationofniobasednanocompositeforsupercapacitorapplication-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0013468613019725\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'leontyeva-leontyev-avramenko-yuzyuk-kukushkina-smirnova-electrochemicaldispergationasasimpleandeffectivetechniquetowardpreparationofniobasednanocompositeforsupercapacitorapplication-2013', 'https://www.sciencedirect.com/science/article/pii/S0013468613019725', event);\">\n    Electrochemical dispergation as a simple and effective technique toward preparation of NiO based nanocomposite for supercapacitor application.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Leontyeva, D. V.; Leontyev, I. N.; Avramenko, M. V.; Yuzyuk, Y. I.; Kukushkina, Y. A.;  and Smirnova, N. V.\n</span>\n\n  \n\n</span>\n\n  <i>Electrochimica Acta</i>, 114: 356–362. December 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0013468613019725\"\n     onclick=\"log_download('leontyeva-leontyev-avramenko-yuzyuk-kukushkina-smirnova-electrochemicaldispergationasasimpleandeffectivetechniquetowardpreparationofniobasednanocompositeforsupercapacitorapplication-2013', 'https://www.sciencedirect.com/science/article/pii/S0013468613019725', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Electrochemical dispergation as a simple and effective technique toward preparation of NiO based nanocomposite for supercapacitor application [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.electacta.2013.10.031\"\n     onclick=\"log_download('leontyeva-leontyev-avramenko-yuzyuk-kukushkina-smirnova-electrochemicaldispergationasasimpleandeffectivetechniquetowardpreparationofniobasednanocompositeforsupercapacitorapplication-2013', 'http://doi.org/10.1016/j.electacta.2013.10.031', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/leontyeva-leontyev-avramenko-yuzyuk-kukushkina-smirnova-electrochemicaldispergationasasimpleandeffectivetechniquetowardpreparationofniobasednanocompositeforsupercapacitorapplication-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('leontyeva-leontyev-avramenko-yuzyuk-kukushkina-smirnova-electrochemicaldispergationasasimpleandeffectivetechniquetowardpreparationofniobasednanocompositeforsupercapacitorapplication-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{leontyeva_electrochemical_2013,\n\ttitle = {Electrochemical dispergation as a simple and effective technique toward preparation of {NiO} based nanocomposite for supercapacitor application},\n\tvolume = {114},\n\tissn = {0013-4686},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0013468613019725},\n\tdoi = {10.1016/j.electacta.2013.10.031},\n\tabstract = {NiO/C nanocomposite was prepared directly by means a one-step electrochemical technique based on electrochemical dispergation of nickel by the alternating current. The prepared material was well characterized using different analytical techniques such as X-ray diffraction, Raman spectroscopy, scanning electron microscopy, and N2 adsorption/desorption. The X-ray diffraction and Raman scattering investigations of the freshly prepared sample confirmed the formation of β-NiO. The morphology of synthesized NiO/C can be described as dispersed on carbon support nano-leaves consisting of tightly packed array of nanoparticles (around 10nm in diam) with length of 500–2000nm and ∼20nm thick. NiO/C composite possesses high specific surface area of 137m2g−1 and a micro–meso–macroporous structure with a distribution of the pore size from 1 to 200nm. The electrochemical properties of the nanostructured NiO/C were investigated using cyclic voltammetry (CV) and galvanostatic charge-discharge tests. The synthesized NiO/C composite exhibited pseudo-capacitive behavior with the mass capacitance value as high as 1012Fg−1 and 750Fg−1 measured from CV and discharge curves, respectively. Compared with the theoretical specific capacitance of NiO 2573Fg−1, the degree of electrochemical utilization is 97\\% for NiO in the synthesized NiO/C composite. The superior electrochemical performance is attributed to the hierarchically porous structure of the synthesized NiO/C, its with a high specific surface area as well as a wide pore size distribution. Considering the excellent performance and facile preparation, this NiO/C composite should have great potential for application in energy storage and conversion devices.},\n\turldate = {2023-11-11},\n\tjournal = {Electrochimica Acta},\n\tauthor = {Leontyeva, D. V. and Leontyev, I. N. and Avramenko, M. V. and Yuzyuk, Yu. I. and Kukushkina, Yu. A. and Smirnova, N. V.},\n\tmonth = dec,\n\tyear = {2013},\n\tkeywords = {Electrochemical capacitors, Nanoplatelets, Nanostructured materials, Nickel oxide},\n\tpages = {356--362},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  NiO/C nanocomposite was prepared directly by means a one-step electrochemical technique based on electrochemical dispergation of nickel by the alternating current. The prepared material was well characterized using different analytical techniques such as X-ray diffraction, Raman spectroscopy, scanning electron microscopy, and N2 adsorption/desorption. The X-ray diffraction and Raman scattering investigations of the freshly prepared sample confirmed the formation of β-NiO. The morphology of synthesized NiO/C can be described as dispersed on carbon support nano-leaves consisting of tightly packed array of nanoparticles (around 10nm in diam) with length of 500–2000nm and ∼20nm thick. NiO/C composite possesses high specific surface area of 137m2g−1 and a micro–meso–macroporous structure with a distribution of the pore size from 1 to 200nm. The electrochemical properties of the nanostructured NiO/C were investigated using cyclic voltammetry (CV) and galvanostatic charge-discharge tests. The synthesized NiO/C composite exhibited pseudo-capacitive behavior with the mass capacitance value as high as 1012Fg−1 and 750Fg−1 measured from CV and discharge curves, respectively. Compared with the theoretical specific capacitance of NiO 2573Fg−1, the degree of electrochemical utilization is 97% for NiO in the synthesized NiO/C composite. The superior electrochemical performance is attributed to the hierarchically porous structure of the synthesized NiO/C, its with a high specific surface area as well as a wide pore size distribution. Considering the excellent performance and facile preparation, this NiO/C composite should have great potential for application in energy storage and conversion devices.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://www.ivdon.ru/magazine/archive/n4y2013/1883\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----2013', 'http://www.ivdon.ru/magazine/archive/n4y2013/1883', event);\">\n    УФ фотоприемник на основе наностержней и пленок оксида цинка.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Жилин, Д. А.; Лянгузов, Н. В.;  and Кайдашев, Е. М.\n</span>\n\n  \n\n</span>\n\n  . August 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://www.ivdon.ru/magazine/archive/n4y2013/1883\"\n     onclick=\"log_download('----2013', 'http://www.ivdon.ru/magazine/archive/n4y2013/1883', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"УФ фотоприемник на основе наностержней и пленок оксида цинка [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>3 downloads</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2013,\n\ttitle = {{УФ} фотоприемник на основе наностержней и пленок оксида цинка},\n\turl = {http://www.ivdon.ru/magazine/archive/n4y2013/1883},\n\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tauthor = {Жилин, Д. А. and Лянгузов, Н. В. and Кайдашев, Е. М.},\n\tmonth = aug,\n\tyear = {2013},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Сетевой научный журнал «Инженерный вестник Дона»\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://www.ivdon.ru/magazine/archive/n4y2013/1885\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----2013', 'http://www.ivdon.ru/magazine/archive/n4y2013/1885', event);\">\n    Импульсное лазерное напыление наноструктур.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Несветаев, Д. Г.; Кайдашев, Е. М.;  and Пузиков, А. С.\n</span>\n\n  \n\n</span>\n\n  . August 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://www.ivdon.ru/magazine/archive/n4y2013/1885\"\n     onclick=\"log_download('----2013', 'http://www.ivdon.ru/magazine/archive/n4y2013/1885', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Импульсное лазерное напыление наноструктур [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>3 downloads</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2013-1,\n\ttitle = {Импульсное лазерное напыление наноструктур},\n\turl = {http://www.ivdon.ru/magazine/archive/n4y2013/1885},\n\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tauthor = {Несветаев, Д. Г. and Кайдашев, Е. М. and Пузиков, А. С.},\n\tmonth = aug,\n\tyear = {2013},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Сетевой научный журнал «Инженерный вестник Дона»\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"konevtsova-rochal-lorman-unconventionallandautheoryofquasicrystallinestructureformation-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0375960113002417\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'konevtsova-rochal-lorman-unconventionallandautheoryofquasicrystallinestructureformation-2013', 'https://www.sciencedirect.com/science/article/pii/S0375960113002417', event);\">\n    Unconventional Landau theory of quasicrystalline structure formation.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Konevtsova, O. V.; Rochal, S. B.;  and Lorman, V. L.\n</span>\n\n  \n\n</span>\n\n  <i>Physics Letters A</i>, 377(16): 1215–1220. July 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0375960113002417\"\n     onclick=\"log_download('konevtsova-rochal-lorman-unconventionallandautheoryofquasicrystallinestructureformation-2013', 'https://www.sciencedirect.com/science/article/pii/S0375960113002417', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Unconventional Landau theory of quasicrystalline structure formation [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.physleta.2013.03.006\"\n     onclick=\"log_download('konevtsova-rochal-lorman-unconventionallandautheoryofquasicrystallinestructureformation-2013', 'http://doi.org/10.1016/j.physleta.2013.03.006', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/konevtsova-rochal-lorman-unconventionallandautheoryofquasicrystallinestructureformation-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('konevtsova-rochal-lorman-unconventionallandautheoryofquasicrystallinestructureformation-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{konevtsova_unconventional_2013,\n\ttitle = {Unconventional {Landau} theory of quasicrystalline structure formation},\n\tvolume = {377},\n\tissn = {0375-9601},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0375960113002417},\n\tdoi = {10.1016/j.physleta.2013.03.006},\n\tabstract = {We propose an unconventional theory which unifies the description of quasicrystal thermodynamics and quasicrystal structure formation by combining the Landau theory of crystallization and the cluster approach to quasicrystals. The theory is illustrated on the example of pentagonal Penrose quasilattice. It employs the notion of non-linear order parameter dependent on the atomic coordinates which was developed in the theory of reconstructive phase transitions. The coordinates of the quasilattice nodes are calculated by minimizing the Landau free energy with the constraint imposed by internal organization of clusters. The correspondence is shown between the theory proposed and the conventional projection method.},\n\tnumber = {16},\n\turldate = {2023-11-11},\n\tjournal = {Physics Letters A},\n\tauthor = {Konevtsova, O. V. and Rochal, S. B. and Lorman, V. L.},\n\tmonth = jul,\n\tyear = {2013},\n\tkeywords = {Cluster approach, Constrained minimization, Landau crystallization theory, Non-linear order parameter, Quasicrystal},\n\tpages = {1215--1220},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We propose an unconventional theory which unifies the description of quasicrystal thermodynamics and quasicrystal structure formation by combining the Landau theory of crystallization and the cluster approach to quasicrystals. The theory is illustrated on the example of pentagonal Penrose quasilattice. It employs the notion of non-linear order parameter dependent on the atomic coordinates which was developed in the theory of reconstructive phase transitions. The coordinates of the quasilattice nodes are calculated by minimizing the Landau free energy with the constraint imposed by internal organization of clusters. The correspondence is shown between the theory proposed and the conventional projection method.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"gorshunov-zhukova-torgashev-lebedev-shakurov-kremer-pestrjakov-thomas-etal-quantumbehaviorofwatermoleculesconfinedtonanocavitiesingemstones-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1021/jz400782j\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'gorshunov-zhukova-torgashev-lebedev-shakurov-kremer-pestrjakov-thomas-etal-quantumbehaviorofwatermoleculesconfinedtonanocavitiesingemstones-2013', 'https://doi.org/10.1021/jz400782j', event);\">\n    Quantum Behavior of Water Molecules Confined to Nanocavities in Gemstones.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Gorshunov, B. P.; Zhukova, E. S.; Torgashev, V. I.; Lebedev, V. V.; Shakurov, G. S.; Kremer, R. K.; Pestrjakov, E. V.; Thomas, V. G.; Fursenko, D. A.;  and Dressel, M.\n</span>\n\n  \n\n</span>\n\n  <i>The Journal of Physical Chemistry Letters</i>, 4(12): 2015–2020. June 2013.\n  <span class=\"note\">Publisher: American Chemical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1021/jz400782j\"\n     onclick=\"log_download('gorshunov-zhukova-torgashev-lebedev-shakurov-kremer-pestrjakov-thomas-etal-quantumbehaviorofwatermoleculesconfinedtonanocavitiesingemstones-2013', 'https://doi.org/10.1021/jz400782j', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Quantum Behavior of Water Molecules Confined to Nanocavities in Gemstones [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1021/jz400782j\"\n     onclick=\"log_download('gorshunov-zhukova-torgashev-lebedev-shakurov-kremer-pestrjakov-thomas-etal-quantumbehaviorofwatermoleculesconfinedtonanocavitiesingemstones-2013', 'http://doi.org/10.1021/jz400782j', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/gorshunov-zhukova-torgashev-lebedev-shakurov-kremer-pestrjakov-thomas-etal-quantumbehaviorofwatermoleculesconfinedtonanocavitiesingemstones-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('gorshunov-zhukova-torgashev-lebedev-shakurov-kremer-pestrjakov-thomas-etal-quantumbehaviorofwatermoleculesconfinedtonanocavitiesingemstones-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{gorshunov_quantum_2013,\n\ttitle = {Quantum {Behavior} of {Water} {Molecules} {Confined} to {Nanocavities} in {Gemstones}},\n\tvolume = {4},\n\turl = {https://doi.org/10.1021/jz400782j},\n\tdoi = {10.1021/jz400782j},\n\tabstract = {When water is confined to nanocavities, its quantum mechanical behavior can be revealed by terahertz spectroscopy. We place H2O molecules in the nanopores of a beryl crystal lattice and observe a rich and highly anisotropic set of absorption lines in the terahertz spectral range. Two bands can be identified, which originate from translational and librational motions of the water molecule isolated within the cage; they correspond to the analogous broad bands in liquid water and ice. In the present case of well-defined and highly symmetric nanocavities, the observed fine structure can be explained by macroscopic tunneling of the H2O molecules within a six-fold potential caused by the interaction of the molecule with the cavity walls.},\n\tnumber = {12},\n\turldate = {2023-11-11},\n\tjournal = {The Journal of Physical Chemistry Letters},\n\tauthor = {Gorshunov, Boris P. and Zhukova, Elena S. and Torgashev, Victor I. and Lebedev, Vladimir V. and Shakurov, Gil’man S. and Kremer, Reinhard K. and Pestrjakov, Efim V. and Thomas, Victor G. and Fursenko, Dimitry A. and Dressel, Martin},\n\tmonth = jun,\n\tyear = {2013},\n\tnote = {Publisher: American Chemical Society},\n\tpages = {2015--2020},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  When water is confined to nanocavities, its quantum mechanical behavior can be revealed by terahertz spectroscopy. We place H2O molecules in the nanopores of a beryl crystal lattice and observe a rich and highly anisotropic set of absorption lines in the terahertz spectral range. Two bands can be identified, which originate from translational and librational motions of the water molecule isolated within the cage; they correspond to the analogous broad bands in liquid water and ice. In the present case of well-defined and highly symmetric nanocavities, the observed fine structure can be explained by macroscopic tunneling of the H2O molecules within a six-fold potential caused by the interaction of the molecule with the cavity walls.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://www.ivdon.ru/magazine/archive/n4y2013/2006\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---2013', 'http://www.ivdon.ru/magazine/archive/n4y2013/2006', event);\">\n    Электронные методы структурного анализа индивидуальных углеродных нанотрубок.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Левшов, Д. И.;  and Авраменко, М. В.\n</span>\n\n  \n\n</span>\n\n  . June 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://www.ivdon.ru/magazine/archive/n4y2013/2006\"\n     onclick=\"log_download('---2013', 'http://www.ivdon.ru/magazine/archive/n4y2013/2006', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Электронные методы структурного анализа индивидуальных углеродных нанотрубок [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2013-2,\n\ttitle = {Электронные методы структурного анализа индивидуальных углеродных нанотрубок},\n\turl = {http://www.ivdon.ru/magazine/archive/n4y2013/2006},\n\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tauthor = {Левшов, Д. И. and Авраменко, М. В.},\n\tmonth = jun,\n\tyear = {2013},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Сетевой научный журнал «Инженерный вестник Дона»\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://www.ivdon.ru/magazine/archive/n3y2013/1844\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---2013', 'http://www.ivdon.ru/magazine/archive/n3y2013/1844', event);\">\n    Топологические дефекты в двумерных сферических кристаллах.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Петров, К. Ю.;  and Шевченко, И. А.\n</span>\n\n  \n\n</span>\n\n  . April 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://www.ivdon.ru/magazine/archive/n3y2013/1844\"\n     onclick=\"log_download('---2013', 'http://www.ivdon.ru/magazine/archive/n3y2013/1844', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Топологические дефекты в двумерных сферических кристаллах [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2013-3,\n\ttitle = {Топологические дефекты в двумерных сферических кристаллах},\n\turl = {http://www.ivdon.ru/magazine/archive/n3y2013/1844},\n\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tauthor = {Петров, К. Ю. and Шевченко, И. А.},\n\tmonth = apr,\n\tyear = {2013},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Сетевой научный журнал «Инженерный вестник Дона»\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"avramenko-rochal-yuzyuk-symmetryofthecarbonnanotubemodesandtheiroriginfromthephononbranchesofgraphene-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.87.035407\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'avramenko-rochal-yuzyuk-symmetryofthecarbonnanotubemodesandtheiroriginfromthephononbranchesofgraphene-2013', 'https://link.aps.org/doi/10.1103/PhysRevB.87.035407', event);\">\n    Symmetry of the carbon nanotube modes and their origin from the phonon branches of graphene.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Avramenko, M. V.; Rochal, S. B.;  and Yuzyuk, Y. I.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 87(3): 035407. January 2013.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.87.035407\"\n     onclick=\"log_download('avramenko-rochal-yuzyuk-symmetryofthecarbonnanotubemodesandtheiroriginfromthephononbranchesofgraphene-2013', 'https://link.aps.org/doi/10.1103/PhysRevB.87.035407', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Symmetry of the carbon nanotube modes and their origin from the phonon branches of graphene [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.87.035407\"\n     onclick=\"log_download('avramenko-rochal-yuzyuk-symmetryofthecarbonnanotubemodesandtheiroriginfromthephononbranchesofgraphene-2013', 'http://doi.org/10.1103/PhysRevB.87.035407', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/avramenko-rochal-yuzyuk-symmetryofthecarbonnanotubemodesandtheiroriginfromthephononbranchesofgraphene-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('avramenko-rochal-yuzyuk-symmetryofthecarbonnanotubemodesandtheiroriginfromthephononbranchesofgraphene-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{avramenko_symmetry_2013,\n\ttitle = {Symmetry of the carbon nanotube modes and their origin from the phonon branches of graphene},\n\tvolume = {87},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.87.035407},\n\tdoi = {10.1103/PhysRevB.87.035407},\n\tabstract = {A group-theory method to relate the spectra of tubular and parent planar structures is elaborated. The spectra correlation is obtained using a virtual intermediate planar periodic structure, which has a local symmetry coinciding with that of the tube surface. The method is applied to deduce the zone-center phonon modes of carbon nanotubes from the dispersion branches of the graphene monolayer. The results obtained open an additional way for experimental indexing of the carbon nanotubes by means of Raman spectroscopy, and the origin of the Raman-active modes in the achiral nanotubes is determined. We demonstrate that the number of modes in the G band and the relation between their frequencies are governed by the nanotube type. The proposed theory can be easily explored to understand the phonon and electron spectra of many other tubular structures (boron nitride, transition metal dichalcogenides) which have emerged in the past decade.},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Avramenko, M. V. and Rochal, S. B. and Yuzyuk, Yu. I.},\n\tmonth = jan,\n\tyear = {2013},\n\tnote = {Publisher: American Physical Society},\n\tpages = {035407},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\S37AE8AD\\\\Avramenko и др. - 2013 - Symmetry of the carbon nanotube modes and their or.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A group-theory method to relate the spectra of tubular and parent planar structures is elaborated. The spectra correlation is obtained using a virtual intermediate planar periodic structure, which has a local symmetry coinciding with that of the tube surface. The method is applied to deduce the zone-center phonon modes of carbon nanotubes from the dispersion branches of the graphene monolayer. The results obtained open an additional way for experimental indexing of the carbon nanotubes by means of Raman spectroscopy, and the origin of the Raman-active modes in the achiral nanotubes is determined. We demonstrate that the number of modes in the G band and the relation between their frequencies are governed by the nanotube type. The proposed theory can be easily explored to understand the phonon and electron spectra of many other tubular structures (boron nitride, transition metal dichalcogenides) which have emerged in the past decade.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"razumnaya-gagou-bouyanfif-carcan-allouche-wolfman-autretlambert-marssi-etal-resistiveswitchinghysteresisinthinfilmsofbismuthferrite-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/00150193.2013.790759\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'razumnaya-gagou-bouyanfif-carcan-allouche-wolfman-autretlambert-marssi-etal-resistiveswitchinghysteresisinthinfilmsofbismuthferrite-2013', 'https://doi.org/10.1080/00150193.2013.790759', event);\">\n    Resistive Switching Hysteresis in Thin Films of Bismuth Ferrite.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Razumnaya, A.; Gagou, Y.; Bouyanfif, H.; Carcan, B.; Allouche, B.; Wolfman, J.; Autret-Lambert, C.; Marssi, M. E.; Mezzane, D.;  and Luk'yanchuk, I.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 444(1): 183–189. January 2013.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2013.790759</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/00150193.2013.790759\"\n     onclick=\"log_download('razumnaya-gagou-bouyanfif-carcan-allouche-wolfman-autretlambert-marssi-etal-resistiveswitchinghysteresisinthinfilmsofbismuthferrite-2013', 'https://doi.org/10.1080/00150193.2013.790759', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Resistive Switching Hysteresis in Thin Films of Bismuth Ferrite [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150193.2013.790759\"\n     onclick=\"log_download('razumnaya-gagou-bouyanfif-carcan-allouche-wolfman-autretlambert-marssi-etal-resistiveswitchinghysteresisinthinfilmsofbismuthferrite-2013', 'http://doi.org/10.1080/00150193.2013.790759', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/razumnaya-gagou-bouyanfif-carcan-allouche-wolfman-autretlambert-marssi-etal-resistiveswitchinghysteresisinthinfilmsofbismuthferrite-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('razumnaya-gagou-bouyanfif-carcan-allouche-wolfman-autretlambert-marssi-etal-resistiveswitchinghysteresisinthinfilmsofbismuthferrite-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{razumnaya_resistive_2013,\n\ttitle = {Resistive {Switching} {Hysteresis} in {Thin} {Films} of {Bismuth} {Ferrite}},\n\tvolume = {444},\n\tissn = {0015-0193},\n\turl = {https://doi.org/10.1080/00150193.2013.790759},\n\tdoi = {10.1080/00150193.2013.790759},\n\tabstract = {We have studied the resistive switching (RS) phenomenon in series of BiFeO3 thin films of thickness of 40 – 154 nm deposited by PLD technique on conducting Nb-doped substrate of SrTiO3 and with Pt top electrodes. It was found that 154 nm film demonstrates the interface-provided I–V characteristic of Schottky diode when the applied voltage does not exceed the threshold value Vd = 1.3 V. The RS phenomenon appears as the current hysteresis loop during the 0 → Vm → 0 → −Vm → 0 voltage sweep cycle, provided that the maximal stop-voltage Vm is larger than Vd. For thinner films neither diode-like I–V behavior nor substantial RS effect were observed. The results are interpreted in terms of the filamentary model of the mobile oxygen vacancies.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Ferroelectrics},\n\tauthor = {Razumnaya, A. and Gagou, Y. and Bouyanfif, H. and Carcan, B. and Allouche, B. and Wolfman, J. and Autret-Lambert, C. and Marssi, M. El and Mezzane, D. and Luk&#x27;yanchuk, I.},\n\tmonth = jan,\n\tyear = {2013},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/00150193.2013.790759},\n\tkeywords = {multiferroics, oxides, Resistive switching, thin films},\n\tpages = {183--189},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We have studied the resistive switching (RS) phenomenon in series of BiFeO3 thin films of thickness of 40 – 154 nm deposited by PLD technique on conducting Nb-doped substrate of SrTiO3 and with Pt top electrodes. It was found that 154 nm film demonstrates the interface-provided I–V characteristic of Schottky diode when the applied voltage does not exceed the threshold value Vd = 1.3 V. The RS phenomenon appears as the current hysteresis loop during the 0 → Vm → 0 → −Vm → 0 voltage sweep cycle, provided that the maximal stop-voltage Vm is larger than Vd. For thinner films neither diode-like I–V behavior nor substantial RS effect were observed. The results are interpreted in terms of the filamentary model of the mobile oxygen vacancies.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"akbaeva-kabirov-milov-gavrilyachenko-phasestatesinmulticomponentpztbasedmaterialsdependingonpolingconditions-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/00150193.2013.778616\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'akbaeva-kabirov-milov-gavrilyachenko-phasestatesinmulticomponentpztbasedmaterialsdependingonpolingconditions-2013', 'https://doi.org/10.1080/00150193.2013.778616', event);\">\n    Phase States in Multicomponent PZT-Based Materials Depending on Poling Conditions.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Akbaeva, G. M.; Kabirov, Y. V.; Milov, E. V.;  and Gavrilyachenko, V. G.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 443(1): 57–62. January 2013.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2013.778616</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/00150193.2013.778616\"\n     onclick=\"log_download('akbaeva-kabirov-milov-gavrilyachenko-phasestatesinmulticomponentpztbasedmaterialsdependingonpolingconditions-2013', 'https://doi.org/10.1080/00150193.2013.778616', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Phase States in Multicomponent PZT-Based Materials Depending on Poling Conditions [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150193.2013.778616\"\n     onclick=\"log_download('akbaeva-kabirov-milov-gavrilyachenko-phasestatesinmulticomponentpztbasedmaterialsdependingonpolingconditions-2013', 'http://doi.org/10.1080/00150193.2013.778616', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/akbaeva-kabirov-milov-gavrilyachenko-phasestatesinmulticomponentpztbasedmaterialsdependingonpolingconditions-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('akbaeva-kabirov-milov-gavrilyachenko-phasestatesinmulticomponentpztbasedmaterialsdependingonpolingconditions-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{akbaeva_phase_2013,\n\ttitle = {Phase {States} in {Multicomponent} {PZT}-{Based} {Materials} {Depending} on {Poling} {Conditions}},\n\tvolume = {443},\n\tissn = {0015-0193},\n\turl = {https://doi.org/10.1080/00150193.2013.778616},\n\tdoi = {10.1080/00150193.2013.778616},\n\tabstract = {Phase states of the PZT-based multicomponent solid solutions belonging to the rhombohedral area of the phase х-Т diagram with low coercive field values are considered. The solid-solution samples in the initial state are proved to be heterophase (R3c and P4mm mixtures) and reveal relaxor properties. The anomalies of dielectric characteristics obtained in poled samples are due to the R3c→R3m phase transition. The manifestations of relaxor properties above the temperature of the dielectric permittivity maximum are caused by the R3m phase in the P4mm and Pm3m phase mixture.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Ferroelectrics},\n\tauthor = {Akbaeva, G. M. and Kabirov, Yu. V. and Milov, E. V. and Gavrilyachenko, V. G.},\n\tmonth = jan,\n\tyear = {2013},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/00150193.2013.778616},\n\tkeywords = {phase transition, X-ray diffraction, Phase state, poling condition},\n\tpages = {57--62},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Phase states of the PZT-based multicomponent solid solutions belonging to the rhombohedral area of the phase х-Т diagram with low coercive field values are considered. The solid-solution samples in the initial state are proved to be heterophase (R3c and P4mm mixtures) and reveal relaxor properties. The anomalies of dielectric characteristics obtained in poled samples are due to the R3c→R3m phase transition. The manifestations of relaxor properties above the temperature of the dielectric permittivity maximum are caused by the R3m phase in the P4mm and Pm3m phase mixture.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"levshov-michel-than-paillet-arenal-jourdain-yuzyuk-sauvajol-comparativeramanstudyofindividualdoublewalledcarbonnanotubesandsinglewalledcarbonnanotubes-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  Comparative Raman Study of Individual Double-Walled Carbon Nanotubes and Single-Walled Carbon Nanotubes.\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Levshov, D.; Michel, T.; Than, T.; Paillet, M.; Arenal, R.; Jourdain, V.; Yuzyuk, Y. I.;  and Sauvajol, J.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Nanoelectronics and Optoelectronics</i>, 8(1): 9–15. January 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n\n  \n  <a href=\"http://doi.org/10.1166/jno.2013.1423\"\n     onclick=\"log_download('levshov-michel-than-paillet-arenal-jourdain-yuzyuk-sauvajol-comparativeramanstudyofindividualdoublewalledcarbonnanotubesandsinglewalledcarbonnanotubes-2013', 'http://doi.org/10.1166/jno.2013.1423', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/levshov-michel-than-paillet-arenal-jourdain-yuzyuk-sauvajol-comparativeramanstudyofindividualdoublewalledcarbonnanotubesandsinglewalledcarbonnanotubes-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('levshov-michel-than-paillet-arenal-jourdain-yuzyuk-sauvajol-comparativeramanstudyofindividualdoublewalledcarbonnanotubesandsinglewalledcarbonnanotubes-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{levshov_comparative_2013,\n\ttitle = {Comparative {Raman} {Study} of {Individual} {Double}-{Walled} {Carbon} {Nanotubes} and {Single}-{Walled} {Carbon} {Nanotubes}},\n\tvolume = {8},\n\tdoi = {10.1166/jno.2013.1423},\n\tabstract = {In this paper, we compare the Raman responses obtained on individual suspended Single-Walled Carbon Nanotubes (SWNTs) and Double-Walled Carbon Nanotubes (DWNTs). We focus on the comparison of the frequencies, line widths, intensities and resonance conditions of the main Raman active\nmodes measured on an index-identified DWNT with those measured on SWNTs having atomic structures close to the inner and outer tubes of the DWNT. By this way, we state that the relation between the radial breathing mode frequencies and the diameters established for SWNTs do not work in DWNTs.\nWe found that resonance of only one tube can be sufficient to observe the response of the coupled layers in DWNTs. These results are understood in terms of mechanical coupling between the layers in DWNTs. We evidence that the spectral line widths of the Raman active modes are systematically\nnarrower for DWNTs compared to the corresponding SWNTs. Finally, we present the measurements of the G modes of two different DWNTs which behave in a different way. For the first one, the frequencies of the G modes are not significantly affected by the interaction between the\nlayers, while for the second one we evidence a downward shift of the LO and TO bands arising from the inner layer.},\n\tnumber = {1},\n\tjournal = {Journal of Nanoelectronics and Optoelectronics},\n\tauthor = {Levshov, D. and Michel, T. and Than, T. and Paillet, M. and Arenal, R. and Jourdain, V. and Yuzyuk, Yu. I. and Sauvajol, J.-L.},\n\tmonth = jan,\n\tyear = {2013},\n\tkeywords = {ELECTRON DIFFRACTION, INDIVIDUAL DOUBLE-WALLED CARBON NANOTUBES, INDIVIDUAL SINGLE-WALLED CARBON NANOTUBES, RAMAN SPECTROSCOPY},\n\tpages = {9--15},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  In this paper, we compare the Raman responses obtained on individual suspended Single-Walled Carbon Nanotubes (SWNTs) and Double-Walled Carbon Nanotubes (DWNTs). We focus on the comparison of the frequencies, line widths, intensities and resonance conditions of the main Raman active modes measured on an index-identified DWNT with those measured on SWNTs having atomic structures close to the inner and outer tubes of the DWNT. By this way, we state that the relation between the radial breathing mode frequencies and the diameters established for SWNTs do not work in DWNTs. We found that resonance of only one tube can be sufficient to observe the response of the coupled layers in DWNTs. These results are understood in terms of mechanical coupling between the layers in DWNTs. We evidence that the spectral line widths of the Raman active modes are systematically narrower for DWNTs compared to the corresponding SWNTs. Finally, we present the measurements of the G modes of two different DWNTs which behave in a different way. For the first one, the frequencies of the G modes are not significantly affected by the interaction between the layers, while for the second one we evidence a downward shift of the LO and TO bands arising from the inner layer.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----ptcptnic-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://www.maikonline.com/maik/showArticle.do?auid=VAHEB686WM&amp;lang=ru\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----ptcptnic-2013', 'http://www.maikonline.com/maik/showArticle.do?auid=VAHEB686WM&amp;lang=ru', event);\">\n    Структурные и электрокаталитические свойства катализаторов Pt/C и Pt–Ni/C, полученных методом электрохимического диспергирования.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Смирнова, Н. В.; Куриганова, А. Б.; Леонтьева, Д. В.; Леонтьев, И. Н.;  and Михейкин, А. С.\n</span>\n\n  \n\n</span>\n\n  In <i>Кинетика и катализ</i>, volume 54, pages 265–272,  2013. \n  <span class=\"note\">ISSN: 0453-8811 Issue: 2 Journal Abbreviation: Кинет. и катал.</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://www.maikonline.com/maik/showArticle.do?auid=VAHEB686WM&amp;lang=ru\"\n     onclick=\"log_download('-----ptcptnic-2013', 'http://www.maikonline.com/maik/showArticle.do?auid=VAHEB686WM&amp;lang=ru', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Структурные и электрокаталитические свойства катализаторов Pt/C и Pt–Ni/C, полученных методом электрохимического диспергирования [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.7868/S0453881113020147\"\n     onclick=\"log_download('-----ptcptnic-2013', 'http://doi.org/10.7868/S0453881113020147', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----ptcptnic-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----ptcptnic-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{__2013-4,\n\ttitle = {Структурные и электрокаталитические свойства катализаторов {Pt}/{C} и {Pt}–{Ni}/{C}, полученных методом электрохимического диспергирования},\n\tvolume = {54},\n\turl = {http://www.maikonline.com/maik/showArticle.do?auid=VAHEB686WM&amp;lang=ru},\n\tdoi = {10.7868/S0453881113020147},\n\tabstract = {Semantic Scholar extracted view of &quot;Структурные и электрокаталитические свойства катализаторов Pt/C и Pt–Ni/C, полученных методом электрохимического диспергирования&quot; by Наталья Владимировна Смирнова et al.},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tbooktitle = {Кинетика и катализ},\n\tauthor = {Смирнова, Н. В. and Куриганова, А. Б. and Леонтьева, Д. В. and Леонтьев, И. Н. and Михейкин, А. С.},\n\tyear = {2013},\n\tnote = {ISSN: 0453-8811\nIssue: 2\nJournal Abbreviation: Кинет. и катал.},\n\tpages = {265--272},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Semantic Scholar extracted view of \"Структурные и электрокаталитические свойства катализаторов Pt/C и Pt–Ni/C, полученных методом электрохимического диспергирования\" by Наталья Владимировна Смирнова et al.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"--------2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=18944350\"\n     onclick=\"return trackOutboundLink('publications', 'click', '--------2013', 'https://elibrary.ru/item.asp?id=18944350', event);\">\n    Синтез и свойства метаматериалов со структурой оболочка-ядро.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Кабиров, Ю. В.; Гавриляченко, В. Г.; Гутерман, В. Е.; Залетов, В. Г.; Сидоренко, Е. Н.; Лянгузов, Н. В.;  and Панченко, Е. М.\n</span>\n\n  \n\n</span>\n\n  <i>Конструкции Из Композиционных Материалов</i>, (2 (130)): 37–42.  2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=18944350\"\n     onclick=\"log_download('--------2013', 'https://elibrary.ru/item.asp?id=18944350', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Синтез и свойства метаматериалов со структурой оболочка-ядро [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/--------2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('--------2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2013-5,\n\ttitle = {Синтез и свойства метаматериалов со структурой оболочка-ядро},\n\tissn = {2073-2562},\n\turl = {https://elibrary.ru/item.asp?id=18944350},\n\tabstract = {Синтезированы поликристаллические и керамические композитные материалы (КМ) Pt ( PbZrO 3 ) и CaCu 3 Ti 4 O 12 ( SrFe 12 O 19 ), архитектурно представляющие собой структуру оболочка—ядро. В первых из них обнаружен парамагнетизм, обусловленный появлением парамагнитных центров при взаимодействии атомов платины и матрицы. Композитная керамика на основе гексаферрита стронция SrFe 12 O 19, структурированная по типу оболочка—ядро материалом с колоссальным значением диэлектрической проницаемости CaCu 3 Ti 4 O 12, приготовлена с использованием традиционной керамической технологии. Приведены результаты электронно-микроскопических и электрофизических исследований объектов},\n\tlanguage = {ru},\n\tnumber = {2 (130)},\n\turldate = {2023-11-11},\n\tjournal = {Конструкции Из Композиционных Материалов},\n\tauthor = {Кабиров, Ю. В. and Гавриляченко, В. Г. and Гутерман, В. Е. and Залетов, В. Г. and Сидоренко, Е. Н. and Лянгузов, Н. В. and Панченко, Е. М.},\n\tyear = {2013},\n\tkeywords = {Гексаферрит Стронция, Композиты, Метаматериалы},\n\tpages = {37--42},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Синтезированы поликристаллические и керамические композитные материалы (КМ) Pt ( PbZrO 3 ) и CaCu 3 Ti 4 O 12 ( SrFe 12 O 19 ), архитектурно представляющие собой структуру оболочка—ядро. В первых из них обнаружен парамагнетизм, обусловленный появлением парамагнитных центров при взаимодействии атомов платины и матрицы. Композитная керамика на основе гексаферрита стронция SrFe 12 O 19, структурированная по типу оболочка—ядро материалом с колоссальным значением диэлектрической проницаемости CaCu 3 Ti 4 O 12, приготовлена с использованием традиционной керамической технологии. Приведены результаты электронно-микроскопических и электрофизических исследований объектов\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://www.ivdon.ru/magazine/archive/n4y2013/1972\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---2013', 'http://www.ivdon.ru/magazine/archive/n4y2013/1972', event);\">\n    Спектроскопия комбинационного рассеяния света как метод диагностики структуры индивидуальных углеродных нанотрубок.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Левшов, Д. И.;  and Авраменко, М. В.\n</span>\n\n  \n\n</span>\n\n  , (4). July 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://www.ivdon.ru/magazine/archive/n4y2013/1972\"\n     onclick=\"log_download('---2013', 'http://www.ivdon.ru/magazine/archive/n4y2013/1972', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Спектроскопия комбинационного рассеяния света как метод диагностики структуры индивидуальных углеродных нанотрубок [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2013-6,\n\ttitle = {Спектроскопия комбинационного рассеяния света как метод диагностики структуры индивидуальных углеродных нанотрубок},\n\turl = {http://www.ivdon.ru/magazine/archive/n4y2013/1972},\n\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\n\tlanguage = {ru},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tauthor = {Левшов, Д. И. and Авраменко, М. В.},\n\tmonth = jul,\n\tyear = {2013},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Сетевой научный журнал «Инженерный вестник Дона»\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://www.ivdon.ru/magazine/archive/n4y2013/1884\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----2013', 'http://www.ivdon.ru/magazine/archive/n4y2013/1884', event);\">\n    Низкотемпературный термический синтез наностержней оксида цинка из паров цинка без катализатора.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Пушкарев, В. И.; Лянгузов, Н. В.;  and Кайдашев, Е. М.\n</span>\n\n  \n\n</span>\n\n  . August 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://www.ivdon.ru/magazine/archive/n4y2013/1884\"\n     onclick=\"log_download('----2013', 'http://www.ivdon.ru/magazine/archive/n4y2013/1884', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Низкотемпературный термический синтез наностержней оксида цинка из паров цинка без катализатора [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>3 downloads</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2013-7,\n\ttitle = {Низкотемпературный термический синтез наностержней оксида цинка из паров цинка без катализатора},\n\turl = {http://www.ivdon.ru/magazine/archive/n4y2013/1884},\n\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tauthor = {Пушкарев, В. И. and Лянгузов, Н. В. and Кайдашев, Е. М.},\n\tmonth = aug,\n\tyear = {2013},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Сетевой научный журнал «Инженерный вестник Дона»\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---bifeo3-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/27131\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---bifeo3-2013', 'http://journals.ioffe.ru/articles/27131', event);\">\n    Оптические свойства эпитаксиальных тонких пленок BiFeO3.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Широков, В. Б.; Головко, Ю. И.;  and Мухортов, В. М.\n</span>\n\n  \n\n</span>\n\n  <i>Журнал технической физики</i>, 84(1): 104–108. December 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/27131\"\n     onclick=\"log_download('---bifeo3-2013', 'http://journals.ioffe.ru/articles/27131', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Оптические свойства эпитаксиальных тонких пленок BiFeO3 [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---bifeo3-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---bifeo3-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2013-8,\n\ttitle = {Оптические свойства эпитаксиальных тонких пленок {BiFeO3}},\n\tvolume = {84},\n\turl = {http://journals.ioffe.ru/articles/27131},\n\tabstract = {Исследованы свойства наноразмерных пленок BiFeO3, допированных неодимом, на монокристаллических подложках оксида магния, полученных методом высокочастотного распыления по слоевому механизму роста. Структурное совершенство пленок изучено методами рентгеновской дифракции. Пропускание пленок различной толщины исследовано в диапазоне длин волн 200-1100 nm. Спектры обработаны с использованием дисперсионной формулы для диэлектрической проницаемости в виде суммы осцилляторов с учетом релаксации, что позволило выделить прямые и непрямые переходы. Край поглощения оценен для прямых переходов как 2.81 и 2.78 eV для пленок толщиной 14 и 60 nm соответственно.},\n\tlanguage = {ru},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Журнал технической физики},\n\tauthor = {Широков, В. Б. and Головко, Ю. И. and Мухортов, В. М.},\n\tmonth = dec,\n\tyear = {2013},\n\tpages = {104--108},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследованы свойства наноразмерных пленок BiFeO3, допированных неодимом, на монокристаллических подложках оксида магния, полученных методом высокочастотного распыления по слоевому механизму роста. Структурное совершенство пленок изучено методами рентгеновской дифракции. Пропускание пленок различной толщины исследовано в диапазоне длин волн 200-1100 nm. Спектры обработаны с использованием дисперсионной формулы для диэлектрической проницаемости в виде суммы осцилляторов с учетом релаксации, что позволило выделить прямые и непрямые переходы. Край поглощения оценен для прямых переходов как 2.81 и 2.78 eV для пленок толщиной 14 и 60 nm соответственно.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"--------etal-bitextrm1xsrtextrmxfeotextrm3delta03200thz-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/1093\"\n     onclick=\"return trackOutboundLink('publications', 'click', '--------etal-bitextrm1xsrtextrmxfeotextrm3delta03200thz-2013', 'http://journals.ioffe.ru/articles/1093', event);\">\n    Динамический спектральный отклик твердых растворов висмут-стронциевого феррита Bi$_{\\textrm{1-x}}$Sr$_{\\textrm{x}}$FeO$_{\\textrm{3-delta}}$ в диапазоне частот 0.3-200 THz.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Анохин, А. С.; Разумная, А. Г.; Торгашев, В. И.; Троценко, В. Г.; Юзюк, Ю. И.; Буш, А. А.; Шкуратов, В. Я.; Горшунов, Б. П.; Жукова, Е. С.; Кадыров, Л. С.;  and Командин, Г. А.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 55(7): 1320–1332. June 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/1093\"\n     onclick=\"log_download('--------etal-bitextrm1xsrtextrmxfeotextrm3delta03200thz-2013', 'http://journals.ioffe.ru/articles/1093', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Динамический спектральный отклик твердых растворов висмут-стронциевого феррита Bi$_{\\textrm{1-x}}$Sr$_{\\textrm{x}}$FeO$_{\\textrm{3-delta}}$ в диапазоне частот 0.3-200 THz [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/--------etal-bitextrm1xsrtextrmxfeotextrm3delta03200thz-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('--------etal-bitextrm1xsrtextrmxfeotextrm3delta03200thz-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2013-9,\n\ttitle = {Динамический спектральный отклик твердых растворов висмут-стронциевого феррита {Bi}$_{\\textrm{1-x}}${Sr}$_{\\textrm{x}}${FeO}$_{\\textrm{3-delta}}$ в диапазоне частот 0.3-200 {THz}},\n\tvolume = {55},\n\turl = {http://journals.ioffe.ru/articles/1093},\n\tlanguage = {ru},\n\tnumber = {7},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Анохин, А. С. and Разумная, А. Г. and Торгашев, В. И. and Троценко, В. Г. and Юзюк, Ю. И. and Буш, А. А. and Шкуратов, В. Я. and Горшунов, Б. П. and Жукова, Е. С. and Кадыров, Л. С. and Командин, Г. А.},\n\tmonth = jun,\n\tyear = {2013},\n\tpages = {1320--1332},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----batiotextrm3-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/1045\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----batiotextrm3-2013', 'http://journals.ioffe.ru/articles/1045', event);\">\n    Теплоемкость наноструктурированной керамики BaTiO$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Каллаев, С. Н.; Омаров, З. М.; Бакмаев, А. Г.;  and Абдулвахидов, К. Г.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 55(5): 1011–1013. April 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/1045\"\n     onclick=\"log_download('----batiotextrm3-2013', 'http://journals.ioffe.ru/articles/1045', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Теплоемкость наноструктурированной керамики BaTiO$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----batiotextrm3-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----batiotextrm3-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2013-10,\n\ttitle = {Теплоемкость наноструктурированной керамики {BaTiO}$_{\\textrm{3}}$},\n\tvolume = {55},\n\turl = {http://journals.ioffe.ru/articles/1045},\n\tabstract = {Исследована температурная зависимость теплоемкости наноструктурированной керамики BaTiO3, полученной твердофазным методом, спеканию которой предшествовала обработка при комнатной температуре синтезированной шихты в наковальнях Бриджмена силовым воздействием в сочетании со сдвиговой деформацией. Обнаружено существенное размытие сегнетоэлектрического перехода и нелинейное убывание температуры фазового перехода с увеличением приложенного давления. Показано, что дефектная структура играет доминирующую роль в формировании физических свойств керамики.},\n\tlanguage = {ru},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Каллаев, С. Н. and Омаров, З. М. and Бакмаев, А. Г. and Абдулвахидов, К. Г.},\n\tmonth = apr,\n\tyear = {2013},\n\tpages = {1011--1013},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследована температурная зависимость теплоемкости наноструктурированной керамики BaTiO3, полученной твердофазным методом, спеканию которой предшествовала обработка при комнатной температуре синтезированной шихты в наковальнях Бриджмена силовым воздействием в сочетании со сдвиговой деформацией. Обнаружено существенное размытие сегнетоэлектрического перехода и нелинейное убывание температуры фазового перехода с увеличением приложенного давления. Показано, что дефектная структура играет доминирующую роль в формировании физических свойств керамики.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----basrtiotextrm3-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/998\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----basrtiotextrm3-2013', 'http://journals.ioffe.ru/articles/998', event);\">\n    Материальные константы твердых растворов (Ba,Sr)TiO$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Широков, В. Б.; Юзюк, Ю. И.; Калинчук, В. В.;  and Леманов, В. В.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 55(4): 709–714. March 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/998\"\n     onclick=\"log_download('----basrtiotextrm3-2013', 'http://journals.ioffe.ru/articles/998', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Материальные константы твердых растворов (Ba,Sr)TiO$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----basrtiotextrm3-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----basrtiotextrm3-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2013-11,\n\ttitle = {Материальные константы твердых растворов ({Ba},{Sr}){TiO}$_{\\textrm{3}}$},\n\tvolume = {55},\n\turl = {http://journals.ioffe.ru/articles/998},\n\tabstract = {Феноменологическая теория твердого раствора использована для вычисления поведения материальных констант (упругих податливостей, восприимчивостей, пьезоэлектрических модулей, пироэлектрических коэффициентов) твердого раствора BaxSr1-xTiO3 во всей области изменения концентраций x при комнатной температуре. Для выделенных концентраций приведены константы феноменологического потенциала и численные значения материальных констант.},\n\tlanguage = {ru},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Широков, В. Б. and Юзюк, Ю. И. and Калинчук, В. В. and Леманов, В. В.},\n\tmonth = mar,\n\tyear = {2013},\n\tpages = {709--714},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Феноменологическая теория твердого раствора использована для вычисления поведения материальных констант (упругих податливостей, восприимчивостей, пьезоэлектрических модулей, пироэлектрических коэффициентов) твердого раствора BaxSr1-xTiO3 во всей области изменения концентраций x при комнатной температуре. Для выделенных концентраций приведены константы феноменологического потенциала и численные значения материальных констант.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/1117\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----2013', 'http://journals.ioffe.ru/articles/1117', event);\">\n    Теория кристаллизации Ландау и самосборка октагональных квазикристаллов.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Коневцова, О. В.; Рошаль, С. Б.;  and Лорман, В. Л.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 55(8): 1488–1493. July 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/1117\"\n     onclick=\"log_download('----2013', 'http://journals.ioffe.ru/articles/1117', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Теория кристаллизации Ландау и самосборка октагональных квазикристаллов [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>3 downloads</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2013-12,\n\ttitle = {Теория кристаллизации Ландау и самосборка октагональных квазикристаллов},\n\tvolume = {55},\n\turl = {http://journals.ioffe.ru/articles/1117},\n\tabstract = {Предложена теория кристаллизации квазикристаллических структур, не использующая для описания квазикристаллического порядка концепций многомерной кристаллографии. На примере структуры октагонального квазикристалла MnSiAl показано, что координаты узлов соответствующей квазикристаллической решетки (КР) можно рассчитать путем условной минимизации свободной энергии Ландау. Отказ от безусловной минимизации свободной энергии обосновывается особенностями локального атомного порядка в рассматриваемой структуре. Предложенная теория придает новый физический смысл традиционным понятиям многомерной кристаллографии и может быть также применена для объяснения образования квазикристаллических структур с другими КР.},\n\tlanguage = {ru},\n\tnumber = {8},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Коневцова, О. В. and Рошаль, С. Б. and Лорман, В. Л.},\n\tmonth = jul,\n\tyear = {2013},\n\tpages = {1488--1493},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Предложена теория кристаллизации квазикристаллических структур, не использующая для описания квазикристаллического порядка концепций многомерной кристаллографии. На примере структуры октагонального квазикристалла MnSiAl показано, что координаты узлов соответствующей квазикристаллической решетки (КР) можно рассчитать путем условной минимизации свободной энергии Ландау. Отказ от безусловной минимизации свободной энергии обосновывается особенностями локального атомного порядка в рассматриваемой структуре. Предложенная теория придает новый физический смысл традиционным понятиям многомерной кристаллографии и может быть также применена для объяснения образования квазикристаллических структур с другими КР.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-------cacutextrm3titextrm4otextrm12-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/1124\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-------cacutextrm3titextrm4otextrm12-2013', 'http://journals.ioffe.ru/articles/1124', event);\">\n    Особенности диэлектрического спектра CaCu$_{\\textrm{3}}$Ti$_{\\textrm{4}}$O$_{\\textrm{12}}$ в низкочастотном диапазоне.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Гавриляченко, В. Г.; Кабиров, Ю. В.; Панченко, Е. М.; Ситало, Е. И.; Гавриляченко, Т. В.; Милов, Е. В.;  and Лянгузов, Н. В.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 55(8): 1540–1543. July 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/1124\"\n     onclick=\"log_download('-------cacutextrm3titextrm4otextrm12-2013', 'http://journals.ioffe.ru/articles/1124', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Особенности диэлектрического спектра CaCu$_{\\textrm{3}}$Ti$_{\\textrm{4}}$O$_{\\textrm{12}}$ в низкочастотном диапазоне [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-------cacutextrm3titextrm4otextrm12-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-------cacutextrm3titextrm4otextrm12-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2013-13,\n\ttitle = {Особенности диэлектрического спектра {CaCu}$_{\\textrm{3}}${Ti}$_{\\textrm{4}}${O}$_{\\textrm{12}}$ в низкочастотном диапазоне},\n\tvolume = {55},\n\turl = {http://journals.ioffe.ru/articles/1124},\n\tabstract = {Представлены диэлектрические спектры керамики CaCu3Ti4O12, отличающейся гигантскими значениями диэлектрической проницаемости. В высокочастотной части спектра в области 106-107 Hz проявляется дисперсия дебаевского типа с энергией активации 0.075 eV, а также характерное плато в частотной зависимости диэлектрической проницаемости в области 104-105 Hz. В низкочастотной части спектра наблюдается значительное увеличение фактора потерь varepsilon&#x27;&#x27;, а при частоте менее 10-2 Hz в некоторых образцах обнаружен переход от импеданса емкостного типа к индуктивному. Обсуждаются причины такого перехода.},\n\tlanguage = {ru},\n\tnumber = {8},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Гавриляченко, В. Г. and Кабиров, Ю. В. and Панченко, Е. М. and Ситало, Е. И. and Гавриляченко, Т. В. and Милов, Е. В. and Лянгузов, Н. В.},\n\tmonth = jul,\n\tyear = {2013},\n\tpages = {1540--1543},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Представлены диэлектрические спектры керамики CaCu3Ti4O12, отличающейся гигантскими значениями диэлектрической проницаемости. В высокочастотной части спектра в области 106-107 Hz проявляется дисперсия дебаевского типа с энергией активации 0.075 eV, а также характерное плато в частотной зависимости диэлектрической проницаемости в области 104-105 Hz. В низкочастотной части спектра наблюдается значительное увеличение фактора потерь varepsilon'', а при частоте менее 10-2 Hz в некоторых образцах обнаружен переход от импеданса емкостного типа к индуктивному. Обсуждаются причины такого перехода.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"gorshunov-zhukova-torgashev-kadyrov-motovilova-fischgrabe-moshnyaga-zhang-etal-bosonpeakinoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.87.245124\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'gorshunov-zhukova-torgashev-kadyrov-motovilova-fischgrabe-moshnyaga-zhang-etal-bosonpeakinoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2013', 'https://link.aps.org/doi/10.1103/PhysRevB.87.245124', event);\">\n    Boson peak in overdoped manganites La$_{\\textrm{1-x}}$Ca$_{\\textrm{x}}$MnO$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Gorshunov, B.; Zhukova, E.; Torgashev, V. I.; Kadyrov, L. S.; Motovilova, E. A.; Fischgrabe, F.; Moshnyaga, V.; Zhang, T.; Kremer, R.; Pracht, U.; Zapf, S.;  and Dressel, M.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 87(24): 245124. June 2013.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.87.245124\"\n     onclick=\"log_download('gorshunov-zhukova-torgashev-kadyrov-motovilova-fischgrabe-moshnyaga-zhang-etal-bosonpeakinoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2013', 'https://link.aps.org/doi/10.1103/PhysRevB.87.245124', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Boson peak in overdoped manganites La$_{\\textrm{1-x}}$Ca$_{\\textrm{x}}$MnO$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.87.245124\"\n     onclick=\"log_download('gorshunov-zhukova-torgashev-kadyrov-motovilova-fischgrabe-moshnyaga-zhang-etal-bosonpeakinoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2013', 'http://doi.org/10.1103/PhysRevB.87.245124', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/gorshunov-zhukova-torgashev-kadyrov-motovilova-fischgrabe-moshnyaga-zhang-etal-bosonpeakinoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('gorshunov-zhukova-torgashev-kadyrov-motovilova-fischgrabe-moshnyaga-zhang-etal-bosonpeakinoverdopedmanganiteslatextrm1xcatextrmxmnotextrm3-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{gorshunov_boson_2013,\n\ttitle = {Boson peak in overdoped manganites {La}$_{\\textrm{1-x}}${Ca}$_{\\textrm{x}}${MnO}$_{\\textrm{3}}$},\n\tvolume = {87},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.87.245124},\n\tdoi = {10.1103/PhysRevB.87.245124},\n\tabstract = {In the charge-ordered phase of strongly doped manganites La1−xCaxMnO3 (x≥0.5) absorption lines appear in the terahertz spectral range for commensurate x values right below the charge-ordering temperature. They are connected to acoustic phonons that become optically active by folding of the Brillouin zone. At lower temperatures a strongly asymmetric extra absorption band develops at frequencies corresponding to the position of the lowest-energy van Hove singularity in the reduced Brillouin zone. The band is assigned to the boson peak, i.e., to the excess of lattice vibrational states over the standard Debye contribution. The folded phonons and the boson peak do not show up for incommensurate calcium contents when no distinct Brillouin zone folding exists.},\n\tnumber = {24},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Gorshunov, B. and Zhukova, E. and Torgashev, V. I. and Kadyrov, L. S. and Motovilova, E. A. and Fischgrabe, F. and Moshnyaga, V. and Zhang, T. and Kremer, R. and Pracht, U. and Zapf, S. and Dressel, M.},\n\tmonth = jun,\n\tyear = {2013},\n\tnote = {Publisher: American Physical Society},\n\tpages = {245124},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\G3SEUD2M\\\\Gorshunov и др. - 2013 - Boson peak in overdoped manganites La\\$ _ 1ensure.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  In the charge-ordered phase of strongly doped manganites La1−xCaxMnO3 (x≥0.5) absorption lines appear in the terahertz spectral range for commensurate x values right below the charge-ordering temperature. They are connected to acoustic phonons that become optically active by folding of the Brillouin zone. At lower temperatures a strongly asymmetric extra absorption band develops at frequencies corresponding to the position of the lowest-energy van Hove singularity in the reduced Brillouin zone. The band is assigned to the boson peak, i.e., to the excess of lattice vibrational states over the standard Debye contribution. The folded phonons and the boson peak do not show up for incommensurate calcium contents when no distinct Brillouin zone folding exists.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kozakov-kochur-torgashev-bush-shkuratov-kubrin-nikolskii-googlev-chemicalbondinginthebitextrm1xsrtextrmxfeotextrm3ysystembyxrayphotoelectronandmssbauerspectroscopy-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0368204813001369\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kozakov-kochur-torgashev-bush-shkuratov-kubrin-nikolskii-googlev-chemicalbondinginthebitextrm1xsrtextrmxfeotextrm3ysystembyxrayphotoelectronandmssbauerspectroscopy-2013', 'https://www.sciencedirect.com/science/article/pii/S0368204813001369', event);\">\n    Chemical bonding in the Bi$_{\\textrm{1−x}}$Sr$_{\\textrm{x}}$FeO$_{\\textrm{3±y}}$ system by X-ray photoelectron and Mössbauer spectroscopy.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kozakov, A. T.; Kochur, A. G.; Torgashev, V. I.; Bush, A. A.; Shkuratov, V. Y.; Kubrin, S. P.; Nikolskii, A. V.;  and Googlev, K. A.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Electron Spectroscopy and Related Phenomena</i>, 189: 106–115. August 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0368204813001369\"\n     onclick=\"log_download('kozakov-kochur-torgashev-bush-shkuratov-kubrin-nikolskii-googlev-chemicalbondinginthebitextrm1xsrtextrmxfeotextrm3ysystembyxrayphotoelectronandmssbauerspectroscopy-2013', 'https://www.sciencedirect.com/science/article/pii/S0368204813001369', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Chemical bonding in the Bi$_{\\textrm{1−x}}$Sr$_{\\textrm{x}}$FeO$_{\\textrm{3±y}}$ system by X-ray photoelectron and Mössbauer spectroscopy [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.elspec.2013.08.006\"\n     onclick=\"log_download('kozakov-kochur-torgashev-bush-shkuratov-kubrin-nikolskii-googlev-chemicalbondinginthebitextrm1xsrtextrmxfeotextrm3ysystembyxrayphotoelectronandmssbauerspectroscopy-2013', 'http://doi.org/10.1016/j.elspec.2013.08.006', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kozakov-kochur-torgashev-bush-shkuratov-kubrin-nikolskii-googlev-chemicalbondinginthebitextrm1xsrtextrmxfeotextrm3ysystembyxrayphotoelectronandmssbauerspectroscopy-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kozakov-kochur-torgashev-bush-shkuratov-kubrin-nikolskii-googlev-chemicalbondinginthebitextrm1xsrtextrmxfeotextrm3ysystembyxrayphotoelectronandmssbauerspectroscopy-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kozakov_chemical_2013,\n\ttitle = {Chemical bonding in the {Bi}$_{\\textrm{1−x}}${Sr}$_{\\textrm{x}}${FeO}$_{\\textrm{3±y}}$ system by {X}-ray photoelectron and {Mössbauer} spectroscopy},\n\tvolume = {189},\n\tissn = {0368-2048},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0368204813001369},\n\tdoi = {10.1016/j.elspec.2013.08.006},\n\tabstract = {Ceramic samples Bi1−xSrxFeO3±y are synthesized with 0≤x≤1 by the solid state reaction method. X-ray diffraction study of the samples is performed. Chemical bonding and the valence state of the Fe ions in the Bi1−xSrxFeO3±y ceramics are studied using X-ray photoelectron Fe2p-, Sr3d-, Bi4f-, and O1s-spectra, and Mössbauer spectroscopy. Fe2p-spectra for various ionic states of Fe are calculated in an isolated ion approximation. Considerable deviations of actual elemental compositions from nominal ones are discovered. Both Fe3+ and Fe4+ ions are found to be present in the samples with x{\\textgreater}0. Relative Fe3+/Fe4+ contents are determined by comparing the parameters of experimental and theoretical Fe2p-spectra. Concentration of Fe4+ ions in the samples correlates with that of the Sr atoms.},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Electron Spectroscopy and Related Phenomena},\n\tauthor = {Kozakov, A. T. and Kochur, A. G. and Torgashev, V. I. and Bush, A. A. and Shkuratov, V. Ya. and Kubrin, S. P. and Nikolskii, A. V. and Googlev, K. A.},\n\tmonth = aug,\n\tyear = {2013},\n\tkeywords = {X-ray diffraction, BiSrFeO ceramics, Fe valence state, Mössbauer spectra, X-ray photoelectron spectra},\n\tpages = {106--115},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Ceramic samples Bi1−xSrxFeO3±y are synthesized with 0≤x≤1 by the solid state reaction method. X-ray diffraction study of the samples is performed. Chemical bonding and the valence state of the Fe ions in the Bi1−xSrxFeO3±y ceramics are studied using X-ray photoelectron Fe2p-, Sr3d-, Bi4f-, and O1s-spectra, and Mössbauer spectroscopy. Fe2p-spectra for various ionic states of Fe are calculated in an isolated ion approximation. Considerable deviations of actual elemental compositions from nominal ones are discovered. Both Fe3+ and Fe4+ ions are found to be present in the samples with x\\textgreater0. Relative Fe3+/Fe4+ contents are determined by comparing the parameters of experimental and theoretical Fe2p-spectra. Concentration of Fe4+ ions in the samples correlates with that of the Sr atoms.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"ortega-kumar-resto-maslova-yuzyuk-scott-katiyar-compositionalengineeringofbatiotextrm3basrtiotextrm3ferroelectricsuperlattices-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.4820576\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'ortega-kumar-resto-maslova-yuzyuk-scott-katiyar-compositionalengineeringofbatiotextrm3basrtiotextrm3ferroelectricsuperlattices-2013', 'https://doi.org/10.1063/1.4820576', event);\">\n    Compositional engineering of BaTiO$_{\\textrm{3}}$/(Ba,Sr)TiO$_{\\textrm{3}}$ ferroelectric superlattices.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Ortega, N.; Kumar, A.; Resto, O.; Maslova, O. A.; Yuzyuk, Y. I.; Scott, J. F.;  and Katiyar, R. S.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Applied Physics</i>, 114(10): 104102. September 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.4820576\"\n     onclick=\"log_download('ortega-kumar-resto-maslova-yuzyuk-scott-katiyar-compositionalengineeringofbatiotextrm3basrtiotextrm3ferroelectricsuperlattices-2013', 'https://doi.org/10.1063/1.4820576', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Compositional engineering of BaTiO$_{\\textrm{3}}$/(Ba,Sr)TiO$_{\\textrm{3}}$ ferroelectric superlattices [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.4820576\"\n     onclick=\"log_download('ortega-kumar-resto-maslova-yuzyuk-scott-katiyar-compositionalengineeringofbatiotextrm3basrtiotextrm3ferroelectricsuperlattices-2013', 'http://doi.org/10.1063/1.4820576', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/ortega-kumar-resto-maslova-yuzyuk-scott-katiyar-compositionalengineeringofbatiotextrm3basrtiotextrm3ferroelectricsuperlattices-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('ortega-kumar-resto-maslova-yuzyuk-scott-katiyar-compositionalengineeringofbatiotextrm3basrtiotextrm3ferroelectricsuperlattices-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{ortega_compositional_2013,\n\ttitle = {Compositional engineering of {BaTiO}$_{\\textrm{3}}$/({Ba},{Sr}){TiO}$_{\\textrm{3}}$ ferroelectric superlattices},\n\tvolume = {114},\n\tissn = {0021-8979},\n\turl = {https://doi.org/10.1063/1.4820576},\n\tdoi = {10.1063/1.4820576},\n\tabstract = {Epitaxial strain is one of the major factors influencing physical properties of artificial superlattice (SL) structures. One way to control the local stress in epitaxial films is altering the lattice parameters by doping. Superlattices of BT/Ba(1−x)SrxTiO3 (BT/BST) with x = (0, 0.3, 0.4, 0.5, 0.6, 0.7, 1) with a modulation period of about 80–90 Å were grown on La0.67Sr0.33MnO3 coated (100) MgO substrates by pulsed laser deposition technique. The modulated structure of the thin films was confirmed by x-ray diffraction, Raman spectroscopy, and transmission electron microscopy. The increase in Sr concentration in BST layers of the SLs results in an increase in in-plane (a) and out-plane (c) compressive/tensile misfit strains in the BT/BST layers, respectively. The highest value of the dielectric constant was obtained for BT/Ba0.3Sr0.7TiO3 (BT/BST3070) and BT/Ba0.7Sr0.3TiO3 (BT/BST7030) SLs. Slim, asymmetric, but well-saturated ferroelectric hysteresis loops were observed in all SLs. Additionally, BT/BST SLs exhibited exceptionally high electric field stress sustainability over a wide range of frequency (10 kHz) and temperature (80–350 K). Temperature-dependent dielectric and ferroelectric properties show a ferroelectric relaxor behavior when the Sr content is increased in the BST layer of the SLs. Analysis of polarization versus temperature data using Landau-Devonshire theory suggests a second-order ferroelectric phase transition in these SLs. This structure can therefore be attractive in the design of a new kind of dielectric device capable in both high power and high energy density applications.},\n\tnumber = {10},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Applied Physics},\n\tauthor = {Ortega, N. and Kumar, Ashok and Resto, Oscar and Maslova, O. A. and Yuzyuk, Yu. I. and Scott, J. F. and Katiyar, Ram S.},\n\tmonth = sep,\n\tyear = {2013},\n\tpages = {104102},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Epitaxial strain is one of the major factors influencing physical properties of artificial superlattice (SL) structures. One way to control the local stress in epitaxial films is altering the lattice parameters by doping. Superlattices of BT/Ba(1−x)SrxTiO3 (BT/BST) with x = (0, 0.3, 0.4, 0.5, 0.6, 0.7, 1) with a modulation period of about 80–90 Å were grown on La0.67Sr0.33MnO3 coated (100) MgO substrates by pulsed laser deposition technique. The modulated structure of the thin films was confirmed by x-ray diffraction, Raman spectroscopy, and transmission electron microscopy. The increase in Sr concentration in BST layers of the SLs results in an increase in in-plane (a) and out-plane (c) compressive/tensile misfit strains in the BT/BST layers, respectively. The highest value of the dielectric constant was obtained for BT/Ba0.3Sr0.7TiO3 (BT/BST3070) and BT/Ba0.7Sr0.3TiO3 (BT/BST7030) SLs. Slim, asymmetric, but well-saturated ferroelectric hysteresis loops were observed in all SLs. Additionally, BT/BST SLs exhibited exceptionally high electric field stress sustainability over a wide range of frequency (10 kHz) and temperature (80–350 K). Temperature-dependent dielectric and ferroelectric properties show a ferroelectric relaxor behavior when the Sr content is increased in the BST layer of the SLs. Analysis of polarization versus temperature data using Landau-Devonshire theory suggests a second-order ferroelectric phase transition in these SLs. This structure can therefore be attractive in the design of a new kind of dielectric device capable in both high power and high energy density applications.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kamenskyi-engelkamp-fischer-uhlarz-wosnitza-gorshunov-komandin-prokhorov-etal-observationofanintersublatticeexchangemagnonincocrtextrm2otextrm4andanalysisofmagneticordering-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.87.134423\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kamenskyi-engelkamp-fischer-uhlarz-wosnitza-gorshunov-komandin-prokhorov-etal-observationofanintersublatticeexchangemagnonincocrtextrm2otextrm4andanalysisofmagneticordering-2013', 'https://link.aps.org/doi/10.1103/PhysRevB.87.134423', event);\">\n    Observation of an intersublattice exchange magnon in CoCr$_{\\textrm{2}}$O$_{\\textrm{4}}$ and analysis of magnetic ordering.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kamenskyi, D.; Engelkamp, H.; Fischer, T.; Uhlarz, M.; Wosnitza, J.; Gorshunov, B. P.; Komandin, G. A.; Prokhorov, A. S.; Dressel, M.; Bush, A. A.; Torgashev, V. I.;  and Pronin, A. V.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 87(13): 134423. April 2013.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.87.134423\"\n     onclick=\"log_download('kamenskyi-engelkamp-fischer-uhlarz-wosnitza-gorshunov-komandin-prokhorov-etal-observationofanintersublatticeexchangemagnonincocrtextrm2otextrm4andanalysisofmagneticordering-2013', 'https://link.aps.org/doi/10.1103/PhysRevB.87.134423', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Observation of an intersublattice exchange magnon in CoCr$_{\\textrm{2}}$O$_{\\textrm{4}}$ and analysis of magnetic ordering [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.87.134423\"\n     onclick=\"log_download('kamenskyi-engelkamp-fischer-uhlarz-wosnitza-gorshunov-komandin-prokhorov-etal-observationofanintersublatticeexchangemagnonincocrtextrm2otextrm4andanalysisofmagneticordering-2013', 'http://doi.org/10.1103/PhysRevB.87.134423', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kamenskyi-engelkamp-fischer-uhlarz-wosnitza-gorshunov-komandin-prokhorov-etal-observationofanintersublatticeexchangemagnonincocrtextrm2otextrm4andanalysisofmagneticordering-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kamenskyi-engelkamp-fischer-uhlarz-wosnitza-gorshunov-komandin-prokhorov-etal-observationofanintersublatticeexchangemagnonincocrtextrm2otextrm4andanalysisofmagneticordering-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kamenskyi_observation_2013,\n\ttitle = {Observation of an intersublattice exchange magnon in {CoCr}$_{\\textrm{2}}${O}$_{\\textrm{4}}$ and analysis of magnetic ordering},\n\tvolume = {87},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.87.134423},\n\tdoi = {10.1103/PhysRevB.87.134423},\n\tabstract = {We report on an investigation of optical properties of multiferroic CoCr2O4 at terahertz frequencies in magnetic fields up to 30 T. Below the ferrimagnetic transition (94 K), the terahertz response of CoCr2O4 is dominated by a magnon mode, which shows a steep magnetic-field dependence. We ascribe this mode to an exchange resonance between two magnetic sublattices with different g factors. In the framework of a simple two-sublattice model (the sublattices are formed by Co2+ and Cr3+ ions), we find the inter-sublattice coupling constant, λ=−(18±1) K, and trace the magnetization for each sublattice as a function of field. We show that the Curie temperature of the Cr3+ sublattice, Θ2 = (49±2) K, coincides with the temperature range, where anomalies of the dielectric and magnetic properties of CoCr2O4 have been reported in literature.},\n\tnumber = {13},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Kamenskyi, D. and Engelkamp, H. and Fischer, T. and Uhlarz, M. and Wosnitza, J. and Gorshunov, B. P. and Komandin, G. A. and Prokhorov, A. S. and Dressel, M. and Bush, A. A. and Torgashev, V. I. and Pronin, A. V.},\n\tmonth = apr,\n\tyear = {2013},\n\tnote = {Publisher: American Physical Society},\n\tpages = {134423},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\X6THP5XM\\\\Kamenskyi и др. - 2013 - Observation of an intersublattice exchange magnon .pdf:application/pdf;APS Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\3GBGXRM2\\\\PhysRevB.87.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We report on an investigation of optical properties of multiferroic CoCr2O4 at terahertz frequencies in magnetic fields up to 30 T. Below the ferrimagnetic transition (94 K), the terahertz response of CoCr2O4 is dominated by a magnon mode, which shows a steep magnetic-field dependence. We ascribe this mode to an exchange resonance between two magnetic sublattices with different g factors. In the framework of a simple two-sublattice model (the sublattices are formed by Co2+ and Cr3+ ions), we find the inter-sublattice coupling constant, λ=−(18±1) K, and trace the magnetization for each sublattice as a function of field. We show that the Curie temperature of the Cr3+ sublattice, Θ2 = (49±2) K, coincides with the temperature range, where anomalies of the dielectric and magnetic properties of CoCr2O4 have been reported in literature.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shakhovoy-shirokov-yuzyuk-phasediagramsofbatiotextrm3bazrotextrm3superlattices-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/10584587.2013.785795\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shakhovoy-shirokov-yuzyuk-phasediagramsofbatiotextrm3bazrotextrm3superlattices-2013', 'https://doi.org/10.1080/10584587.2013.785795', event);\">\n    Phase Diagrams of BaTiO$_{\\textrm{3}}$/BaZrO$_{\\textrm{3}}$ Superlattices.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shakhovoy, R. A.; Shirokov, V. B.;  and Yuzyuk, Y. I.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 444(1): 168–176. January 2013.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/10584587.2013.785795</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/10584587.2013.785795\"\n     onclick=\"log_download('shakhovoy-shirokov-yuzyuk-phasediagramsofbatiotextrm3bazrotextrm3superlattices-2013', 'https://doi.org/10.1080/10584587.2013.785795', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Phase Diagrams of BaTiO$_{\\textrm{3}}$/BaZrO$_{\\textrm{3}}$ Superlattices [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/10584587.2013.785795\"\n     onclick=\"log_download('shakhovoy-shirokov-yuzyuk-phasediagramsofbatiotextrm3bazrotextrm3superlattices-2013', 'http://doi.org/10.1080/10584587.2013.785795', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shakhovoy-shirokov-yuzyuk-phasediagramsofbatiotextrm3bazrotextrm3superlattices-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shakhovoy-shirokov-yuzyuk-phasediagramsofbatiotextrm3bazrotextrm3superlattices-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shakhovoy_phase_2013,\n\ttitle = {Phase {Diagrams} of {BaTiO}$_{\\textrm{3}}$/{BaZrO}$_{\\textrm{3}}$ {Superlattices}},\n\tvolume = {444},\n\tissn = {0015-0193},\n\turl = {https://doi.org/10.1080/10584587.2013.785795},\n\tdoi = {10.1080/10584587.2013.785795},\n\tabstract = {Temperature-misfit strain phase diagrams of BaTiO3/BaZrO3 superlattices were developed and an alteration of the “misfit strain-temperature” phase diagrams against the changing of ferroelectric layers volume fraction was investigated. The topology of developed phase diagrams is similar to that of single BaTiO3 film, but phase transition lines exhibit substation shifts. According to our approach, the main reason of this shift is the electrostatic interaction between the layers. It is revealed that only one polar phase remains stable in superlattices with volume fraction of BaTiO3 being less than 70\\%.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Ferroelectrics},\n\tauthor = {Shakhovoy, R. A. and Shirokov, V. B. and Yuzyuk, Yu. I.},\n\tmonth = jan,\n\tyear = {2013},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/10584587.2013.785795},\n\tkeywords = {ferroelectric superlattices, Phenomenological theory},\n\tpages = {168--176},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Temperature-misfit strain phase diagrams of BaTiO3/BaZrO3 superlattices were developed and an alteration of the “misfit strain-temperature” phase diagrams against the changing of ferroelectric layers volume fraction was investigated. The topology of developed phase diagrams is similar to that of single BaTiO3 film, but phase transition lines exhibit substation shifts. According to our approach, the main reason of this shift is the electrostatic interaction between the layers. It is revealed that only one polar phase remains stable in superlattices with volume fraction of BaTiO3 being less than 70%.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"anokhin-bunina-golovko-mukhortov-yuzyuk-simon-ramanandxraydiffractionstudyofbasrtiotextrm3bindfeotextrm3multilayerheterostructures-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0040609013013564\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'anokhin-bunina-golovko-mukhortov-yuzyuk-simon-ramanandxraydiffractionstudyofbasrtiotextrm3bindfeotextrm3multilayerheterostructures-2013', 'https://www.sciencedirect.com/science/article/pii/S0040609013013564', event);\">\n    Raman and X-ray diffraction study of (Ba,Sr)TiO$_{\\textrm{3}}$/(Bi,Nd)FeO$_{\\textrm{3}}$ multilayer heterostructures.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Anokhin, A. S.; Bunina, O. A.; Golovko, Y. I.; Mukhortov, V. M.; Yuzyuk, Y. I.;  and Simon, P.\n</span>\n\n  \n\n</span>\n\n  <i>Thin Solid Films</i>, 545: 267–271. October 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0040609013013564\"\n     onclick=\"log_download('anokhin-bunina-golovko-mukhortov-yuzyuk-simon-ramanandxraydiffractionstudyofbasrtiotextrm3bindfeotextrm3multilayerheterostructures-2013', 'https://www.sciencedirect.com/science/article/pii/S0040609013013564', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Raman and X-ray diffraction study of (Ba,Sr)TiO$_{\\textrm{3}}$/(Bi,Nd)FeO$_{\\textrm{3}}$ multilayer heterostructures [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.tsf.2013.08.057\"\n     onclick=\"log_download('anokhin-bunina-golovko-mukhortov-yuzyuk-simon-ramanandxraydiffractionstudyofbasrtiotextrm3bindfeotextrm3multilayerheterostructures-2013', 'http://doi.org/10.1016/j.tsf.2013.08.057', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/anokhin-bunina-golovko-mukhortov-yuzyuk-simon-ramanandxraydiffractionstudyofbasrtiotextrm3bindfeotextrm3multilayerheterostructures-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('anokhin-bunina-golovko-mukhortov-yuzyuk-simon-ramanandxraydiffractionstudyofbasrtiotextrm3bindfeotextrm3multilayerheterostructures-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{anokhin_raman_2013,\n\ttitle = {Raman and {X}-ray diffraction study of ({Ba},{Sr}){TiO}$_{\\textrm{3}}$/({Bi},{Nd}){FeO}$_{\\textrm{3}}$ multilayer heterostructures},\n\tvolume = {545},\n\tissn = {0040-6090},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0040609013013564},\n\tdoi = {10.1016/j.tsf.2013.08.057},\n\tabstract = {We report synthesis, X-ray diffraction (XRD) and Raman scattering characterisation of epitaxial heterostructures containing alternating (Bi0.98Nd0.02)FeO3 (BNFO) and (Ba0.8Sr0.2TiO3) (BST) layers deposited on (100) MgO substrates. A significant shift of the BST soft mode and partial depolarisation in the Raman spectra of multilayer heterostructures caused by epitaxial strains were observed. Satellite peaks typical for superlattices were observed in the XRD patterns of multilayer heterostructures with layer thicknesses below 30nm. Raman spectra of the BNFO/BST superlattice with a modulation period of 10nm revealed hardening of the soft mode and a dominating symmetric-stretching mode at 705cm−1 due to distortion in FeO6 octahedra enforced by the epitaxial strain in the superlattice.},\n\turldate = {2023-11-11},\n\tjournal = {Thin Solid Films},\n\tauthor = {Anokhin, A. S. and Bunina, O. A. and Golovko, Yu I. and Mukhortov, V. M. and Yuzyuk, Yu I. and Simon, P.},\n\tmonth = oct,\n\tyear = {2013},\n\tkeywords = {Raman spectroscopy, Thin films, Multiferroics, Sputtering, X-ray diffraction superlattices},\n\tpages = {267--271},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We report synthesis, X-ray diffraction (XRD) and Raman scattering characterisation of epitaxial heterostructures containing alternating (Bi0.98Nd0.02)FeO3 (BNFO) and (Ba0.8Sr0.2TiO3) (BST) layers deposited on (100) MgO substrates. A significant shift of the BST soft mode and partial depolarisation in the Raman spectra of multilayer heterostructures caused by epitaxial strains were observed. Satellite peaks typical for superlattices were observed in the XRD patterns of multilayer heterostructures with layer thicknesses below 30nm. Raman spectra of the BNFO/BST superlattice with a modulation period of 10nm revealed hardening of the soft mode and a dominating symmetric-stretching mode at 705cm−1 due to distortion in FeO6 octahedra enforced by the epitaxial strain in the superlattice.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"belboukhari-abkhar-choukri-gagou-abdelmoula-elmoznine-mezzane-khemakhem-etal-studiesofdiffusephasetransitioninferroelectricsolidsolutionpbtextrm1xktextrm2xnbtextrm2otextrm6x0102025and03-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/00150193.2013.786619\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'belboukhari-abkhar-choukri-gagou-abdelmoula-elmoznine-mezzane-khemakhem-etal-studiesofdiffusephasetransitioninferroelectricsolidsolutionpbtextrm1xktextrm2xnbtextrm2otextrm6x0102025and03-2013', 'https://doi.org/10.1080/00150193.2013.786619', event);\">\n    Studies of Diffuse Phase Transition in Ferroelectric Solid Solution Pb$_{\\textrm{1-x}}$K$_{\\textrm{2x}}$Nb$_{\\textrm{2}}$O$_{\\textrm{6}}$ (x = 0.1, 0.2, 0.25 and 0.3).\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Belboukhari, A.; Abkhar, Z.; Choukri, E.; Gagou, Y.; Abdelmoula, N.; Elmoznine, R.; Mezzane, D.; Khemakhem, H.; Marssi, M. E.; Razumnaya, A.; Raevski, I.;  and Luk'yanchuk, I.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 444(1): 116–124. January 2013.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2013.786619</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/00150193.2013.786619\"\n     onclick=\"log_download('belboukhari-abkhar-choukri-gagou-abdelmoula-elmoznine-mezzane-khemakhem-etal-studiesofdiffusephasetransitioninferroelectricsolidsolutionpbtextrm1xktextrm2xnbtextrm2otextrm6x0102025and03-2013', 'https://doi.org/10.1080/00150193.2013.786619', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Studies of Diffuse Phase Transition in Ferroelectric Solid Solution Pb$_{\\textrm{1-x}}$K$_{\\textrm{2x}}$Nb$_{\\textrm{2}}$O$_{\\textrm{6}}$ (x = 0.1, 0.2, 0.25 and 0.3) [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150193.2013.786619\"\n     onclick=\"log_download('belboukhari-abkhar-choukri-gagou-abdelmoula-elmoznine-mezzane-khemakhem-etal-studiesofdiffusephasetransitioninferroelectricsolidsolutionpbtextrm1xktextrm2xnbtextrm2otextrm6x0102025and03-2013', 'http://doi.org/10.1080/00150193.2013.786619', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/belboukhari-abkhar-choukri-gagou-abdelmoula-elmoznine-mezzane-khemakhem-etal-studiesofdiffusephasetransitioninferroelectricsolidsolutionpbtextrm1xktextrm2xnbtextrm2otextrm6x0102025and03-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('belboukhari-abkhar-choukri-gagou-abdelmoula-elmoznine-mezzane-khemakhem-etal-studiesofdiffusephasetransitioninferroelectricsolidsolutionpbtextrm1xktextrm2xnbtextrm2otextrm6x0102025and03-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{belboukhari_studies_2013,\n\ttitle = {Studies of {Diffuse} {Phase} {Transition} in {Ferroelectric} {Solid} {Solution} {Pb}$_{\\textrm{1-x}}${K}$_{\\textrm{2x}}${Nb}$_{\\textrm{2}}${O}$_{\\textrm{6}}$ (x = 0.1, 0.2, 0.25 and 0.3)},\n\tvolume = {444},\n\tissn = {0015-0193},\n\turl = {https://doi.org/10.1080/00150193.2013.786619},\n\tdoi = {10.1080/00150193.2013.786619},\n\tabstract = {New compositions of Tetragonal Tungsten Bronze (TTB) ferroelectrics Pb1-xK2xNb5O15 (PKN) with x = 0.1, 0.2, 0.25 and 0.3 were synthesized using the solid state reaction method. Structural and electrical properties were examined as a function of the ratio Pb/K using X-ray diffraction, Raman spectroscopy and dielectric measurements. The dielectric permittivity and the loss tangent of each composition have been measured in a frequency range 10 Hz–1 MH and in a temperatures range 25–600°C. It was shown that the Pb substitution induces the diffuse phase transition.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Ferroelectrics},\n\tauthor = {Belboukhari, A. and Abkhar, Z. and Choukri, E. and Gagou, Y. and Abdelmoula, N. and Elmoznine, R. and Mezzane, D. and Khemakhem, H. and Marssi, M. El and Razumnaya, A. and Raevski, I. and Luk&#x27;yanchuk, I.},\n\tmonth = jan,\n\tyear = {2013},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/00150193.2013.786619},\n\tkeywords = {dielectric spectroscopy, Ferroelectrics, phase transition, TTB compounds},\n\tpages = {116--124},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  New compositions of Tetragonal Tungsten Bronze (TTB) ferroelectrics Pb1-xK2xNb5O15 (PKN) with x = 0.1, 0.2, 0.25 and 0.3 were synthesized using the solid state reaction method. Structural and electrical properties were examined as a function of the ratio Pb/K using X-ray diffraction, Raman spectroscopy and dielectric measurements. The dielectric permittivity and the loss tangent of each composition have been measured in a frequency range 10 Hz–1 MH and in a temperatures range 25–600°C. It was shown that the Pb substitution induces the diffuse phase transition.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"komandin-zhukova-torgashev-boris-boris-motovilova-prokhorov-kadyrov-etal-terahertzinfraredspectraoftherareearthscandatedyscotextrm3singlecrystal-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.4813496\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'komandin-zhukova-torgashev-boris-boris-motovilova-prokhorov-kadyrov-etal-terahertzinfraredspectraoftherareearthscandatedyscotextrm3singlecrystal-2013', 'https://doi.org/10.1063/1.4813496', event);\">\n    Terahertz-infrared spectra of the rare-earth scandate DyScO$_{\\textrm{3}}$ single crystal.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Komandin, G. A.; Zhukova, E. S.; Torgashev, V. I.; Boris, A. V.; Boris, A. A.; Motovilova, E. A.; Prokhorov, A. S.; Kadyrov, L. S.; Gorshunov, B. P.;  and Dressel, M.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Applied Physics</i>, 114(2): 024102. July 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.4813496\"\n     onclick=\"log_download('komandin-zhukova-torgashev-boris-boris-motovilova-prokhorov-kadyrov-etal-terahertzinfraredspectraoftherareearthscandatedyscotextrm3singlecrystal-2013', 'https://doi.org/10.1063/1.4813496', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Terahertz-infrared spectra of the rare-earth scandate DyScO$_{\\textrm{3}}$ single crystal [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.4813496\"\n     onclick=\"log_download('komandin-zhukova-torgashev-boris-boris-motovilova-prokhorov-kadyrov-etal-terahertzinfraredspectraoftherareearthscandatedyscotextrm3singlecrystal-2013', 'http://doi.org/10.1063/1.4813496', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/komandin-zhukova-torgashev-boris-boris-motovilova-prokhorov-kadyrov-etal-terahertzinfraredspectraoftherareearthscandatedyscotextrm3singlecrystal-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('komandin-zhukova-torgashev-boris-boris-motovilova-prokhorov-kadyrov-etal-terahertzinfraredspectraoftherareearthscandatedyscotextrm3singlecrystal-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{komandin_terahertz-infrared_2013,\n\ttitle = {Terahertz-infrared spectra of the rare-earth scandate {DyScO}$_{\\textrm{3}}$ single crystal},\n\tvolume = {114},\n\tissn = {0021-8979},\n\turl = {https://doi.org/10.1063/1.4813496},\n\tdoi = {10.1063/1.4813496},\n\tabstract = {Terahertz and infrared spectra of the optical response of DyScO3 single crystal are measured at temperatures from 5 K to 300 K for two different polarizations E‖[1¯01] and E‖[010], i.e., along the two crystallographic directions of the DyScO3 substrates used for growing of thin films and heterostructures. Detailed reference data on the terahertz dielectric characteristics of the DyScO3 substrate are presented. We discuss the mechanisms responsible for electromagnetic absorption. Phonon spectra are analyzed along with the results of group-theoretical analysis of the crystal structure. Besides phonon modes, additional resonance absorptions are found and assigned to the electronic transitions between Kramers doublets in the three lowest-energy terms of the Dy3+ ion.},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Applied Physics},\n\tauthor = {Komandin, G. A. and Zhukova, E. S. and Torgashev, V. I. and Boris, A. V. and Boris, A. A. and Motovilova, E. A. and Prokhorov, A. S. and Kadyrov, L. S. and Gorshunov, B. P. and Dressel, M.},\n\tmonth = jul,\n\tyear = {2013},\n\tpages = {024102},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Terahertz and infrared spectra of the optical response of DyScO3 single crystal are measured at temperatures from 5 K to 300 K for two different polarizations E‖[1¯01] and E‖[010], i.e., along the two crystallographic directions of the DyScO3 substrates used for growing of thin films and heterostructures. Detailed reference data on the terahertz dielectric characteristics of the DyScO3 substrate are presented. We discuss the mechanisms responsible for electromagnetic absorption. Phonon spectra are analyzed along with the results of group-theoretical analysis of the crystal structure. Besides phonon modes, additional resonance absorptions are found and assigned to the electronic transitions between Kramers doublets in the three lowest-energy terms of the Dy3+ ion.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----pmnpt-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/929\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----pmnpt-2013', 'http://journals.ioffe.ru/articles/929', event);\">\n    Индуцированный электрическим полем фазовый переход в релаксорной керамике на основе PMN–PT.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Таланов, М. В.; Бунина, О. А.; Бунин, М. А.; Захарченко, И. Н.;  and Резниченко, Л. А.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 55(2): 288–294. January 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/929\"\n     onclick=\"log_download('-----pmnpt-2013', 'http://journals.ioffe.ru/articles/929', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Индуцированный электрическим полем фазовый переход в релаксорной керамике на основе PMN–PT [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----pmnpt-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----pmnpt-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2013-14,\n\ttitle = {Индуцированный электрическим полем фазовый переход в релаксорной керамике на основе {PMN}--{PT}},\n\tvolume = {55},\n\turl = {http://journals.ioffe.ru/articles/929},\n\tabstract = {Методами рентгеновской дифрактометрии и атомно-силовой микроскопии проанализированы механизмы формирования плато на зависимостях реверсивной диэлектрической проницаемости от величины напряженности внешнего электрического поля в керамическом образце системы yPZN-mPMN-nPNN-xPT (x=0,3, y =0.0982, m = 0.4541, n = 0.1477). Показано, что в электрических полях, соответствующих аномалии диэлектрической проницаемости, происходит индуцированный фазовый переход из гетерофазного (тетрагонального+псевдокубического) в монофазное (тетрагональное) состояние. При этом наблюдаются значительные деформации тетрагональной ячейки (до 0.1\\%) и прекращение 90o-ных доменных переключений. Представлена качественная модель формирования наблюдаемой диэлектрической аномалии, основанная на выделении двух процессов, протекающих при увеличении напряженности электрического поля: роста полярных областей тетрагональной фазы и их переключения.},\n\tlanguage = {ru},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Таланов, М. В. and Бунина, О. А. and Бунин, М. А. and Захарченко, И. Н. and Резниченко, Л. А.},\n\tmonth = jan,\n\tyear = {2013},\n\tpages = {288--294},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Методами рентгеновской дифрактометрии и атомно-силовой микроскопии проанализированы механизмы формирования плато на зависимостях реверсивной диэлектрической проницаемости от величины напряженности внешнего электрического поля в керамическом образце системы yPZN-mPMN-nPNN-xPT (x=0,3, y =0.0982, m = 0.4541, n = 0.1477). Показано, что в электрических полях, соответствующих аномалии диэлектрической проницаемости, происходит индуцированный фазовый переход из гетерофазного (тетрагонального+псевдокубического) в монофазное (тетрагональное) состояние. При этом наблюдаются значительные деформации тетрагональной ячейки (до 0.1%) и прекращение 90o-ных доменных переключений. Представлена качественная модель формирования наблюдаемой диэлектрической аномалии, основанная на выделении двух процессов, протекающих при увеличении напряженности электрического поля: роста полярных областей тетрагональной фазы и их переключения.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"zakharchenko-bunina-maslova-yuzyuk-ortega-kumar-katiyar-xraydiffractionstudyofbatiotextrm3batextrm1xsrtextrmxtiotextrm3artificialsuperlattices-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/00150193.2013.785833\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'zakharchenko-bunina-maslova-yuzyuk-ortega-kumar-katiyar-xraydiffractionstudyofbatiotextrm3batextrm1xsrtextrmxtiotextrm3artificialsuperlattices-2013', 'https://doi.org/10.1080/00150193.2013.785833', event);\">\n    X-ray Diffraction Study of BaTiO$_{\\textrm{3}}$/(Ba$_{\\textrm{1-x}}$Sr$_{\\textrm{x}}$)TiO$_{\\textrm{3}}$ Artificial Superlattices.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Zakharchenko, I. N.; Bunina, O. A.; Maslova, O. A.; Yuzyuk, Y. I.; Ortega, N.; Kumar, A.;  and Katiyar, R. S.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 444(1): 1–8. January 2013.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2013.785833</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/00150193.2013.785833\"\n     onclick=\"log_download('zakharchenko-bunina-maslova-yuzyuk-ortega-kumar-katiyar-xraydiffractionstudyofbatiotextrm3batextrm1xsrtextrmxtiotextrm3artificialsuperlattices-2013', 'https://doi.org/10.1080/00150193.2013.785833', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"X-ray Diffraction Study of BaTiO$_{\\textrm{3}}$/(Ba$_{\\textrm{1-x}}$Sr$_{\\textrm{x}}$)TiO$_{\\textrm{3}}$ Artificial Superlattices [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150193.2013.785833\"\n     onclick=\"log_download('zakharchenko-bunina-maslova-yuzyuk-ortega-kumar-katiyar-xraydiffractionstudyofbatiotextrm3batextrm1xsrtextrmxtiotextrm3artificialsuperlattices-2013', 'http://doi.org/10.1080/00150193.2013.785833', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/zakharchenko-bunina-maslova-yuzyuk-ortega-kumar-katiyar-xraydiffractionstudyofbatiotextrm3batextrm1xsrtextrmxtiotextrm3artificialsuperlattices-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('zakharchenko-bunina-maslova-yuzyuk-ortega-kumar-katiyar-xraydiffractionstudyofbatiotextrm3batextrm1xsrtextrmxtiotextrm3artificialsuperlattices-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{zakharchenko_x-ray_2013,\n\ttitle = {X-ray {Diffraction} {Study} of {BaTiO}$_{\\textrm{3}}$/({Ba}$_{\\textrm{1-x}}${Sr}$_{\\textrm{x}}$){TiO}$_{\\textrm{3}}$ {Artificial} {Superlattices}},\n\tvolume = {444},\n\tissn = {0015-0193},\n\turl = {https://doi.org/10.1080/00150193.2013.785833},\n\tdoi = {10.1080/00150193.2013.785833},\n\tabstract = {We report x-ray diffraction investigation of two sets of artificial BaTiO3/Ba1-x Sr x TiO3 (BT/BST-x) superlattices (SLs) grown on MgO substrates. The first set of SLs was deposited with the constant periodicity (about 150 Å) and the variable Ba/Sr content in BST layers. In the second set, the modulation period Λ was varied between 30 Å {\\textless} Λ {\\textless} 110 Å while Ba content was equal 0 in BST layers. It is shown that, fabrication of the artificial SLs with variable composition of the constituting layers even with large modulation period may provide enhanced variation of the ferroelectric properties comparing to the SLs with variable layers thickness.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Ferroelectrics},\n\tauthor = {Zakharchenko, I. N. and Bunina, O. A. and Maslova, O. A. and Yuzyuk, Yu. I. and Ortega, N. and Kumar, A. and Katiyar, R. S.},\n\tmonth = jan,\n\tyear = {2013},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/00150193.2013.785833},\n\tkeywords = {ferroelectric superlattices, X-ray diffraction},\n\tpages = {1--8},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We report x-ray diffraction investigation of two sets of artificial BaTiO3/Ba1-x Sr x TiO3 (BT/BST-x) superlattices (SLs) grown on MgO substrates. The first set of SLs was deposited with the constant periodicity (about 150 Å) and the variable Ba/Sr content in BST layers. In the second set, the modulation period Λ was varied between 30 Å \\textless Λ \\textless 110 Å while Ba content was equal 0 in BST layers. It is shown that, fabrication of the artificial SLs with variable composition of the constituting layers even with large modulation period may provide enhanced variation of the ferroelectric properties comparing to the SLs with variable layers thickness.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"--------lamnotextrm3-2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://www.ivdon.ru/magazine/archive/n2y2013/1724\"\n     onclick=\"return trackOutboundLink('publications', 'click', '--------lamnotextrm3-2013', 'http://www.ivdon.ru/magazine/archive/n2y2013/1724', event);\">\n    Методы синтеза LaMnO$_{\\textrm{3}}$ (обзор).\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Рудская, А. Г.; Власенко, М. П.; Чаговец, С. В.; Назаренко, А. В.; Тесленко, П. Ю.; Разумная, А. Г.; Кофанова, Н. Б.;  and Куприянов, М. Ф.\n</span>\n\n  \n\n</span>\n\n  . January 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://www.ivdon.ru/magazine/archive/n2y2013/1724\"\n     onclick=\"log_download('--------lamnotextrm3-2013', 'http://www.ivdon.ru/magazine/archive/n2y2013/1724', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Методы синтеза LaMnO$_{\\textrm{3}}$ (обзор) [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/--------lamnotextrm3-2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('--------lamnotextrm3-2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2013-15,\n\ttitle = {Методы синтеза {LaMnO}$_{\\textrm{3}}$ (обзор)},\n\turl = {http://www.ivdon.ru/magazine/archive/n2y2013/1724},\n\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tauthor = {Рудская, А. Г. and Власенко, М. П. and Чаговец, С. В. and Назаренко, А. В. and Тесленко, П. Ю. and Разумная, А. Г. and Кофанова, Н. Б. and Куприянов, М. Ф.},\n\tmonth = jan,\n\tyear = {2013},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Сетевой научный журнал «Инженерный вестник Дона»\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/14597\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----2013', 'http://journals.ioffe.ru/articles/14597', event);\">\n    Оптимизация карботермического синтеза массивов микро- и наностержней оксида цинка и их морфометрических параметров.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Лянгузов, Н. В.; Кайдашев, Е. М.; Захарченко, И. Н.;  and Бунина, О. А.\n</span>\n\n  \n\n</span>\n\n  <i>Письма в ЖТФ</i>, 39(17): 27–34. August 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/14597\"\n     onclick=\"log_download('-----2013', 'http://journals.ioffe.ru/articles/14597', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Оптимизация карботермического синтеза массивов микро- и наностержней оксида цинка и их морфометрических параметров [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2013-16,\n\ttitle = {Оптимизация карботермического синтеза массивов микро- и наностержней оксида цинка и их морфометрических параметров},\n\tvolume = {39},\n\turl = {http://journals.ioffe.ru/articles/14597},\n\tabstract = {Исследовано влияние буферного давления Ar и расстояния до источника вещества на морфометрические параметры массивов вертикально ориентированных нано- и микростержней ZnO, синтезированных карботермическим методом на подложках Si(100) с тонкопленочным подслоем ZnO. Проведены системные исследования бескаталитического роста, а также влияния катализаторов роста, таких как Au и Cu, на процесс формирования и размеры стержней. Продемонстрировано, что катализатор играет роль лишь на начальном этапе, и не участвует в дальнейшем росте стержней в применяемых условиях синтеза. Показана возможность управления средними диаметрами, длинами и плотностью поверхностного распределения стержней в диапазонах 100-300 nm, 1.5-9 mum и 2.8-5.3· 108 cm-2 соответственно.},\n\tlanguage = {ru},\n\tnumber = {17},\n\turldate = {2023-11-11},\n\tjournal = {Письма в ЖТФ},\n\tauthor = {Лянгузов, Н. В. and Кайдашев, Е. М. and Захарченко, И. Н. and Бунина, О. А.},\n\tmonth = aug,\n\tyear = {2013},\n\tpages = {27--34},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследовано влияние буферного давления Ar и расстояния до источника вещества на морфометрические параметры массивов вертикально ориентированных нано- и микростержней ZnO, синтезированных карботермическим методом на подложках Si(100) с тонкопленочным подслоем ZnO. Проведены системные исследования бескаталитического роста, а также влияния катализаторов роста, таких как Au и Cu, на процесс формирования и размеры стержней. Продемонстрировано, что катализатор играет роль лишь на начальном этапе, и не участвует в дальнейшем росте стержней в применяемых условиях синтеза. Показана возможность управления средними диаметрами, длинами и плотностью поверхностного распределения стержней в диапазонах 100-300 nm, 1.5-9 mum и 2.8-5.3· 108 cm-2 соответственно.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-------simon--2013\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/1254\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-------simon--2013', 'http://journals.ioffe.ru/articles/1254', event);\">\n    Структура и динамика решетки гетероструктур на основе феррита висмута и титаната бария-стронция.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Кхабири, Г.; Анохин, А. С.; Бунина, О. А.; Головко, Ю. И.; Мухортов, В. М.; Широков, В. Б.; Юзюк, Ю. И.;  and Simon, P.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 55(12): 2383–2391. November 2013.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/1254\"\n     onclick=\"log_download('-------simon--2013', 'http://journals.ioffe.ru/articles/1254', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Структура и динамика решетки гетероструктур на основе феррита висмута и титаната бария-стронция [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-------simon--2013\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-------simon--2013')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2013-17,\n\ttitle = {Структура и динамика решетки гетероструктур на основе феррита висмута и титаната бария-стронция},\n\tvolume = {55},\n\turl = {http://journals.ioffe.ru/articles/1254},\n\tabstract = {Исследования морфологии поверхности, параметров решетки и спектров комбинационного рассеяния выполнены на этапах последовательного формирования трехслойной гетероструктуры, состоящей из эпитаксиальных слоев Ba0.8Sr0.2TiO3 (BST) и (Bi0.98Nd0.02)FeO3 (BNFO). Методами рентгенографии определены структурные искажения, возникающие при последовательном осаждении слоев BST/BNFO/BST равной толщины. Обнаружено, что степень тетрагонального искажения пленки BST на MgO повышается после осаждения на ее поверхность пленки BNFO, что свидетельствует о появлении в BST сжимающих напряжений. На основании анализа поляризованных спектров КРС показано, что в слое BNFO наблюдается новое фазовое состояние, не реализующееся в объемных образцах. Показано, что в пленке BST, выращенной на поверхности BNFO степень тетрагональности оказывается выше, чем в такой же пленке, выращенной непосредственно на MgO.},\n\tlanguage = {ru},\n\tnumber = {12},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Кхабири, Г. and Анохин, А. С. and Бунина, О. А. and Головко, Ю. И. and Мухортов, В. М. and Широков, В. Б. and Юзюк, Ю. И. and Simon, P.},\n\tmonth = nov,\n\tyear = {2013},\n\tpages = {2383--2391},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследования морфологии поверхности, параметров решетки и спектров комбинационного рассеяния выполнены на этапах последовательного формирования трехслойной гетероструктуры, состоящей из эпитаксиальных слоев Ba0.8Sr0.2TiO3 (BST) и (Bi0.98Nd0.02)FeO3 (BNFO). Методами рентгенографии определены структурные искажения, возникающие при последовательном осаждении слоев BST/BNFO/BST равной толщины. Обнаружено, что степень тетрагонального искажения пленки BST на MgO повышается после осаждения на ее поверхность пленки BNFO, что свидетельствует о появлении в BST сжимающих напряжений. На основании анализа поляризованных спектров КРС показано, что в слое BNFO наблюдается новое фазовое состояние, не реализующееся в объемных образцах. Показано, что в пленке BST, выращенной на поверхности BNFO степень тетрагональности оказывается выше, чем в такой же пленке, выращенной непосредственно на MgO.\n</div>\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2012\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2012')\"\n      onkeypress=\"toggleGroup('group_2012')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2012</span>\n      <span class=\"bibbase_group_count\">\n        \n        (35)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"mikheykin-dmitriev-chagovets-kuriganova-smirnova-leontyev-thecompressibilityofnanocrystallinept-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.4758000\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'mikheykin-dmitriev-chagovets-kuriganova-smirnova-leontyev-thecompressibilityofnanocrystallinept-2012', 'https://doi.org/10.1063/1.4758000', event);\">\n    The compressibility of nanocrystalline Pt.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Mikheykin, A. S.; Dmitriev, V. P.; Chagovets, S. V.; Kuriganova, A. B.; Smirnova, N. V.;  and Leontyev, I. N.\n</span>\n\n  \n\n</span>\n\n  <i>Applied Physics Letters</i>, 101(17): 173111. October 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.4758000\"\n     onclick=\"log_download('mikheykin-dmitriev-chagovets-kuriganova-smirnova-leontyev-thecompressibilityofnanocrystallinept-2012', 'https://doi.org/10.1063/1.4758000', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"The compressibility of nanocrystalline Pt [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.4758000\"\n     onclick=\"log_download('mikheykin-dmitriev-chagovets-kuriganova-smirnova-leontyev-thecompressibilityofnanocrystallinept-2012', 'http://doi.org/10.1063/1.4758000', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/mikheykin-dmitriev-chagovets-kuriganova-smirnova-leontyev-thecompressibilityofnanocrystallinept-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('mikheykin-dmitriev-chagovets-kuriganova-smirnova-leontyev-thecompressibilityofnanocrystallinept-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{mikheykin_compressibility_2012,\n\ttitle = {The compressibility of nanocrystalline {Pt}},\n\tvolume = {101},\n\tissn = {0003-6951},\n\turl = {https://doi.org/10.1063/1.4758000},\n\tdoi = {10.1063/1.4758000},\n\tabstract = {High-pressure behavior of carbon supported Pt nanoparticles (Pt/C) with an average particle size of 10.6 nm was investigated by in situ high-pressure synchrotron radiation x-ray diffraction up to 14 GPa at ambient temperature. Our results show that the compressibility of Pt/C nanoparticles decreases substantially as the particle size decreases. An interpretation based upon the available mechanisms of structural compliance in nanoscale vs bulk materials was proposed.},\n\tnumber = {17},\n\turldate = {2023-11-11},\n\tjournal = {Applied Physics Letters},\n\tauthor = {Mikheykin, A. S. and Dmitriev, V. P. and Chagovets, S. V. and Kuriganova, A. B. and Smirnova, N. V. and Leontyev, I. N.},\n\tmonth = oct,\n\tyear = {2012},\n\tpages = {173111},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  High-pressure behavior of carbon supported Pt nanoparticles (Pt/C) with an average particle size of 10.6 nm was investigated by in situ high-pressure synchrotron radiation x-ray diffraction up to 14 GPa at ambient temperature. Our results show that the compressibility of Pt/C nanoparticles decreases substantially as the particle size decreases. An interpretation based upon the available mechanisms of structural compliance in nanoscale vs bulk materials was proposed.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://ivdon.ru/magazine/archive/n4p1y2012/1178\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----2012', 'http://ivdon.ru/magazine/archive/n4p1y2012/1178', event);\">\n    Исследование наностержней оксида цинка методом фотолюминесценции для оптимизации характеристик чувствительного элемента ПАВ сенсора.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Несветаев, Д. Г.; Лянгузов, Н. В.; Николаев, А. Л.;  and Кайдашев, Е. М.\n</span>\n\n  \n\n</span>\n\n  . August 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://ivdon.ru/magazine/archive/n4p1y2012/1178\"\n     onclick=\"log_download('-----2012', 'http://ivdon.ru/magazine/archive/n4p1y2012/1178', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Исследование наностержней оксида цинка методом фотолюминесценции для оптимизации характеристик чувствительного элемента ПАВ сенсора [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2012,\n\ttitle = {Исследование наностержней оксида цинка методом фотолюминесценции для оптимизации характеристик чувствительного элемента ПАВ сенсора},\n\turl = {http://ivdon.ru/magazine/archive/n4p1y2012/1178},\n\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tauthor = {Несветаев, Д. Г. and Лянгузов, Н. В. and Николаев, А. Л. and Кайдашев, Е. М.},\n\tmonth = aug,\n\tyear = {2012},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Сетевой научный журнал «Инженерный вестник Дона»\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"leontyev-kuriganova-kudryavtsev-dkhil-smirnova-newlifeofaforgottenmethodelectrochemicalroutetowardhighlyefficientptccatalystsforlowtemperaturefuelcells-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0926860X12002268\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'leontyev-kuriganova-kudryavtsev-dkhil-smirnova-newlifeofaforgottenmethodelectrochemicalroutetowardhighlyefficientptccatalystsforlowtemperaturefuelcells-2012', 'https://www.sciencedirect.com/science/article/pii/S0926860X12002268', event);\">\n    New life of a forgotten method: Electrochemical route toward highly efficient Pt/C catalysts for low-temperature fuel cells.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Leontyev, I.; Kuriganova, A.; Kudryavtsev, Y.; Dkhil, B.;  and Smirnova, N.\n</span>\n\n  \n\n</span>\n\n  <i>Applied Catalysis A: General</i>, 431-432: 120–125. July 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0926860X12002268\"\n     onclick=\"log_download('leontyev-kuriganova-kudryavtsev-dkhil-smirnova-newlifeofaforgottenmethodelectrochemicalroutetowardhighlyefficientptccatalystsforlowtemperaturefuelcells-2012', 'https://www.sciencedirect.com/science/article/pii/S0926860X12002268', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"New life of a forgotten method: Electrochemical route toward highly efficient Pt/C catalysts for low-temperature fuel cells [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.apcata.2012.04.025\"\n     onclick=\"log_download('leontyev-kuriganova-kudryavtsev-dkhil-smirnova-newlifeofaforgottenmethodelectrochemicalroutetowardhighlyefficientptccatalystsforlowtemperaturefuelcells-2012', 'http://doi.org/10.1016/j.apcata.2012.04.025', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/leontyev-kuriganova-kudryavtsev-dkhil-smirnova-newlifeofaforgottenmethodelectrochemicalroutetowardhighlyefficientptccatalystsforlowtemperaturefuelcells-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('leontyev-kuriganova-kudryavtsev-dkhil-smirnova-newlifeofaforgottenmethodelectrochemicalroutetowardhighlyefficientptccatalystsforlowtemperaturefuelcells-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{leontyev_new_2012,\n\ttitle = {New life of a forgotten method: {Electrochemical} route toward highly efficient {Pt}/{C} catalysts for low-temperature fuel cells},\n\tvolume = {431-432},\n\tissn = {0926-860X},\n\tshorttitle = {New life of a forgotten method},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0926860X12002268},\n\tdoi = {10.1016/j.apcata.2012.04.025},\n\tabstract = {Driven by global environmental concerns, great efforts are currently made to develop novel, cheap and practical means for producing highly efficient electrocatalysts, specifically for the low-temperature fuel-cell applications. Employing an old but yet unexplored method based on electrochemical dispergation of platinum by the alternating current, we show that the freshly prepared Pt/C catalysts exhibit greatly enhanced catalytic activity (up to 350\\% for oxygen reduction and up to 200\\% for ethylene glycol oxidation) as compared with that of a commercially available counterpart (E-TEK). A key role in these reactions is attributed to a specific nanoparticle morphology. These findings should provide a revival of an ancient but simple and efficient electrochemical process and motivate further researches in the field.},\n\turldate = {2023-11-11},\n\tjournal = {Applied Catalysis A: General},\n\tauthor = {Leontyev, Igor and Kuriganova, Aleksandra and Kudryavtsev, Yuri and Dkhil, Brahim and Smirnova, Nina},\n\tmonth = jul,\n\tyear = {2012},\n\tkeywords = {Electrocatalysis, Oxygen reduction reaction (ORR), X-ray diffraction (XRD), Low-temperature fuel cell, Platinum nanoparticles, Shape},\n\tpages = {120--125},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Driven by global environmental concerns, great efforts are currently made to develop novel, cheap and practical means for producing highly efficient electrocatalysts, specifically for the low-temperature fuel-cell applications. Employing an old but yet unexplored method based on electrochemical dispergation of platinum by the alternating current, we show that the freshly prepared Pt/C catalysts exhibit greatly enhanced catalytic activity (up to 350% for oxygen reduction and up to 200% for ethylene glycol oxidation) as compared with that of a commercially available counterpart (E-TEK). A key role in these reactions is attributed to a specific nanoparticle morphology. These findings should provide a revival of an ancient but simple and efficient electrochemical process and motivate further researches in the field.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://ivdon.ru/ru/magazine/archive/n4p1y2012/1189\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------2012', 'http://ivdon.ru/ru/magazine/archive/n4p1y2012/1189', event);\">\n    Исследование влияния адсорбции моноокиси углерода на характеристики линии задержки на ПАВ с чувствительным элементом из наностержней оксида цинка.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Карапетьян, Г. Я.; Николаев, А. Л.; Лянгузов, Н. В.; Несветаев, Д. Г.;  and Кайдашев, Е. М.\n</span>\n\n  \n\n</span>\n\n  . July 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://ivdon.ru/ru/magazine/archive/n4p1y2012/1189\"\n     onclick=\"log_download('------2012', 'http://ivdon.ru/ru/magazine/archive/n4p1y2012/1189', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Исследование влияния адсорбции моноокиси углерода на характеристики линии задержки на ПАВ с чувствительным элементом из наностержней оксида цинка [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>1 download</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2012-1,\n\ttitle = {Исследование влияния адсорбции моноокиси углерода на характеристики линии задержки на ПАВ с чувствительным элементом из наностержней оксида цинка},\n\turl = {http://ivdon.ru/ru/magazine/archive/n4p1y2012/1189},\n\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tauthor = {Карапетьян, Г. Я. and Николаев, А. Л. and Лянгузов, Н. В. and Несветаев, Д. Г. and Кайдашев, Е. М.},\n\tmonth = jul,\n\tyear = {2012},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Сетевой научный журнал «Инженерный вестник Дона»\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"timoshenko-ivanov-babichev-shloma-diffractionofsurfacemagnetostaticwavesbysurfacecavitiesonferromagneticfilm-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/S1064226912060137\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'timoshenko-ivanov-babichev-shloma-diffractionofsurfacemagnetostaticwavesbysurfacecavitiesonferromagneticfilm-2012', 'https://doi.org/10.1134/S1064226912060137', event);\">\n    Diffraction of surface magnetostatic waves by surface cavities on ferromagnetic film.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Timoshenko, P. E.; Ivanov, V. N.; Babichev, R. K.;  and Shloma, A. V.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Communications Technology and Electronics</i>, 57(7): 726–733. July 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/S1064226912060137\"\n     onclick=\"log_download('timoshenko-ivanov-babichev-shloma-diffractionofsurfacemagnetostaticwavesbysurfacecavitiesonferromagneticfilm-2012', 'https://doi.org/10.1134/S1064226912060137', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Diffraction of surface magnetostatic waves by surface cavities on ferromagnetic film [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/S1064226912060137\"\n     onclick=\"log_download('timoshenko-ivanov-babichev-shloma-diffractionofsurfacemagnetostaticwavesbysurfacecavitiesonferromagneticfilm-2012', 'http://doi.org/10.1134/S1064226912060137', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/timoshenko-ivanov-babichev-shloma-diffractionofsurfacemagnetostaticwavesbysurfacecavitiesonferromagneticfilm-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('timoshenko-ivanov-babichev-shloma-diffractionofsurfacemagnetostaticwavesbysurfacecavitiesonferromagneticfilm-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{timoshenko_diffraction_2012,\n\ttitle = {Diffraction of surface magnetostatic waves by surface cavities on ferromagnetic film},\n\tvolume = {57},\n\tissn = {1555-6557},\n\turl = {https://doi.org/10.1134/S1064226912060137},\n\tdoi = {10.1134/S1064226912060137},\n\tabstract = {The diffraction problem of the scattering of surface magnetostatic waves by shallow rectangular and circular cavities on the surface of a ferromagnetic film that is tangentially magnetized with respect to the surface is numerically analyzed in the magnetostatic approximation.},\n\tlanguage = {en},\n\tnumber = {7},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Communications Technology and Electronics},\n\tauthor = {Timoshenko, P. E. and Ivanov, V. N. and Babichev, R. K. and Shloma, A. V.},\n\tmonth = jul,\n\tyear = {2012},\n\tkeywords = {Circular Cavity, Lower Lobe, Rectangular Cavity, Reflection Coefficient, Surface Cavity},\n\tpages = {726--733},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The diffraction problem of the scattering of surface magnetostatic waves by shallow rectangular and circular cavities on the surface of a ferromagnetic film that is tangentially magnetized with respect to the surface is numerically analyzed in the magnetostatic approximation.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"manukyan-mirzakhanyan-badalyan-shirinyan-fedorenko-lianguzov-yuzyuk-bugaev-etal-nickelnanoparticlesincarbonstructurespreparedbysolidphasepyrolysisofnickelphthalocyanine-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1007/s11051-012-0982-6\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'manukyan-mirzakhanyan-badalyan-shirinyan-fedorenko-lianguzov-yuzyuk-bugaev-etal-nickelnanoparticlesincarbonstructurespreparedbysolidphasepyrolysisofnickelphthalocyanine-2012', 'https://doi.org/10.1007/s11051-012-0982-6', event);\">\n    Nickel nanoparticles in carbon structures prepared by solid-phase pyrolysis of nickel-phthalocyanine.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Manukyan, A. S.; Mirzakhanyan, A. A.; Badalyan, G. R.; Shirinyan, G. H.; Fedorenko, A. G.; Lianguzov, N. V.; Yuzyuk, Y. I.; Bugaev, L. A.;  and Sharoyan, E. G.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Nanoparticle Research</i>, 14(7): 982. June 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1007/s11051-012-0982-6\"\n     onclick=\"log_download('manukyan-mirzakhanyan-badalyan-shirinyan-fedorenko-lianguzov-yuzyuk-bugaev-etal-nickelnanoparticlesincarbonstructurespreparedbysolidphasepyrolysisofnickelphthalocyanine-2012', 'https://doi.org/10.1007/s11051-012-0982-6', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Nickel nanoparticles in carbon structures prepared by solid-phase pyrolysis of nickel-phthalocyanine [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1007/s11051-012-0982-6\"\n     onclick=\"log_download('manukyan-mirzakhanyan-badalyan-shirinyan-fedorenko-lianguzov-yuzyuk-bugaev-etal-nickelnanoparticlesincarbonstructurespreparedbysolidphasepyrolysisofnickelphthalocyanine-2012', 'http://doi.org/10.1007/s11051-012-0982-6', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/manukyan-mirzakhanyan-badalyan-shirinyan-fedorenko-lianguzov-yuzyuk-bugaev-etal-nickelnanoparticlesincarbonstructurespreparedbysolidphasepyrolysisofnickelphthalocyanine-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('manukyan-mirzakhanyan-badalyan-shirinyan-fedorenko-lianguzov-yuzyuk-bugaev-etal-nickelnanoparticlesincarbonstructurespreparedbysolidphasepyrolysisofnickelphthalocyanine-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{manukyan_nickel_2012,\n\ttitle = {Nickel nanoparticles in carbon structures prepared by solid-phase pyrolysis of nickel-phthalocyanine},\n\tvolume = {14},\n\tissn = {1572-896X},\n\turl = {https://doi.org/10.1007/s11051-012-0982-6},\n\tdoi = {10.1007/s11051-012-0982-6},\n\tabstract = {By using a modified method of solid-phase pyrolysis of metal-phthalocyanines, we have synthesized ferromagnetic Ni nanoparticles in different carbon structures: amorphous carbon plates, multiwall carbon nanotubes, carbon fibers, and graphitized capsules. The composition, structure and morphology of prepared composite materials have been studied by energy dispersive X-ray microanalysis, scanning and transmission electron microscopy, and X-ray diffraction technique. It has been found that the sizes of nickel nanoparticles (10–500 nm) and the type of carbon structures strongly depend on the pyrolysis conditions. By using the X-band ferromagnetic resonance measurements, we have revealed features of the temperature dependence of resonance spectra of single-domain and multi-domain Ni nanoparticles in Ni/C composites.},\n\tlanguage = {en},\n\tnumber = {7},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Nanoparticle Research},\n\tauthor = {Manukyan, A. S. and Mirzakhanyan, A. A. and Badalyan, G. R. and Shirinyan, G. H. and Fedorenko, A. G. and Lianguzov, N. V. and Yuzyuk, Yu I. and Bugaev, L. A. and Sharoyan, E. G.},\n\tmonth = jun,\n\tyear = {2012},\n\tkeywords = {Carbon nanostructures, Magnetic properties, Nickel nanoparticles, Nickel-phthalocyanine, Solid-phase pyrolysis},\n\tpages = {982},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  By using a modified method of solid-phase pyrolysis of metal-phthalocyanines, we have synthesized ferromagnetic Ni nanoparticles in different carbon structures: amorphous carbon plates, multiwall carbon nanotubes, carbon fibers, and graphitized capsules. The composition, structure and morphology of prepared composite materials have been studied by energy dispersive X-ray microanalysis, scanning and transmission electron microscopy, and X-ray diffraction technique. It has been found that the sizes of nickel nanoparticles (10–500 nm) and the type of carbon structures strongly depend on the pyrolysis conditions. By using the X-band ferromagnetic resonance measurements, we have revealed features of the temperature dependence of resonance spectra of single-domain and multi-domain Ni nanoparticles in Ni/C composites.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-------2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://ivdon.ru/magazine/archive/n2y2012/770\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-------2012', 'http://ivdon.ru/magazine/archive/n2y2012/770', event);\">\n    Пассивный беспроводный датчик на поверхностных акустических волнах для измерения параметров газовых и жидких сред.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Карапетьян, Г. Я.; Днепровский, В. Г.; Багдасарян, А. С.; Багдасарян, С. А.; Николаев, А. Л.;  and Кайдашев, Е. М.\n</span>\n\n  \n\n</span>\n\n  . March 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://ivdon.ru/magazine/archive/n2y2012/770\"\n     onclick=\"log_download('-------2012', 'http://ivdon.ru/magazine/archive/n2y2012/770', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Пассивный беспроводный датчик на поверхностных акустических волнах для измерения параметров газовых и жидких сред [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-------2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-------2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2012-2,\n\ttitle = {Пассивный беспроводный датчик на поверхностных акустических волнах для измерения параметров газовых и жидких сред},\n\turl = {http://ivdon.ru/magazine/archive/n2y2012/770},\n\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tauthor = {Карапетьян, Г. Я. and Днепровский, В. Г. and Багдасарян, А. С. and Багдасарян, С. А. and Николаев, А. Л. and Кайдашев, Е. М.},\n\tmonth = mar,\n\tyear = {2012},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Сетевой научный журнал «Инженерный вестник Дона»\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://ivdon.ru/magazine/archive/n2y2012/816\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---2012', 'http://ivdon.ru/magazine/archive/n2y2012/816', event);\">\n    Тригональная хиральная и гексагональная двумерные квазикристаллические укладки.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Рошаль, Д. С.;  and Рошаль, С. Б.\n</span>\n\n  \n\n</span>\n\n  . January 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://ivdon.ru/magazine/archive/n2y2012/816\"\n     onclick=\"log_download('---2012', 'http://ivdon.ru/magazine/archive/n2y2012/816', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Тригональная хиральная и гексагональная двумерные квазикристаллические укладки [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2012-3,\n\ttitle = {Тригональная хиральная и гексагональная двумерные квазикристаллические укладки},\n\turl = {http://ivdon.ru/magazine/archive/n2y2012/816},\n\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tauthor = {Рошаль, Д. С. and Рошаль, С. Б.},\n\tmonth = jan,\n\tyear = {2012},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Сетевой научный журнал «Инженерный вестник Дона»\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"konevtsova-rochal-lorman-chiralquasicrystallineorderanddodecahedralgeometryinexceptionalfamiliesofviruses-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevLett.108.038102\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'konevtsova-rochal-lorman-chiralquasicrystallineorderanddodecahedralgeometryinexceptionalfamiliesofviruses-2012', 'https://link.aps.org/doi/10.1103/PhysRevLett.108.038102', event);\">\n    Chiral Quasicrystalline Order and Dodecahedral Geometry in Exceptional Families of Viruses.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Konevtsova, O. V.; Rochal, S. B.;  and Lorman, V. L.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review Letters</i>, 108(3): 038102. January 2012.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevLett.108.038102\"\n     onclick=\"log_download('konevtsova-rochal-lorman-chiralquasicrystallineorderanddodecahedralgeometryinexceptionalfamiliesofviruses-2012', 'https://link.aps.org/doi/10.1103/PhysRevLett.108.038102', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Chiral Quasicrystalline Order and Dodecahedral Geometry in Exceptional Families of Viruses [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevLett.108.038102\"\n     onclick=\"log_download('konevtsova-rochal-lorman-chiralquasicrystallineorderanddodecahedralgeometryinexceptionalfamiliesofviruses-2012', 'http://doi.org/10.1103/PhysRevLett.108.038102', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/konevtsova-rochal-lorman-chiralquasicrystallineorderanddodecahedralgeometryinexceptionalfamiliesofviruses-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('konevtsova-rochal-lorman-chiralquasicrystallineorderanddodecahedralgeometryinexceptionalfamiliesofviruses-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{konevtsova_chiral_2012,\n\ttitle = {Chiral {Quasicrystalline} {Order} and {Dodecahedral} {Geometry} in {Exceptional} {Families} of {Viruses}},\n\tvolume = {108},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevLett.108.038102},\n\tdoi = {10.1103/PhysRevLett.108.038102},\n\tabstract = {On the example of exceptional families of viruses we (i) show the existence of a completely new type of matter organization in nanoparticles, in which the regions with a chiral pentagonal quasicrystalline order of protein positions are arranged in a structure commensurate with the spherical topology and dodecahedral geometry, (ii) generalize the classical theory of quasicrystals (QCs) to explain this organization, and (iii) establish the relation between local chiral QC order and nonzero curvature of the dodecahedral capsid faces.},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review Letters},\n\tauthor = {Konevtsova, O. V. and Rochal, S. B. and Lorman, V. L.},\n\tmonth = jan,\n\tyear = {2012},\n\tnote = {Publisher: American Physical Society},\n\tpages = {038102},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\T2BMSVJV\\\\Konevtsova и др. - 2012 - Chiral Quasicrystalline Order and Dodecahedral Geo.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  On the example of exceptional families of viruses we (i) show the existence of a completely new type of matter organization in nanoparticles, in which the regions with a chiral pentagonal quasicrystalline order of protein positions are arranged in a structure commensurate with the spherical topology and dodecahedral geometry, (ii) generalize the classical theory of quasicrystals (QCs) to explain this organization, and (iii) establish the relation between local chiral QC order and nonzero curvature of the dodecahedral capsid faces.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"firsova-mishina-sigov-senkevich-pronin-kholkin-bdikin-yuzyuk-femtosecondinfraredlaserannealingofpztfilmsonametalsubstrate-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/00150193.2012.696459\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'firsova-mishina-sigov-senkevich-pronin-kholkin-bdikin-yuzyuk-femtosecondinfraredlaserannealingofpztfilmsonametalsubstrate-2012', 'https://doi.org/10.1080/00150193.2012.696459', event);\">\n    Femtosecond Infrared Laser Annealing of PZT Films on a Metal Substrate.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Firsova, N. Y.; Mishina, E. D.; Sigov, A. S.; Senkevich, S. V.; Pronin, I. P.; Kholkin, A.; Bdikin, I.;  and Yuzyuk, Y. I.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 433(1): 164–169. January 2012.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2012.696459</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/00150193.2012.696459\"\n     onclick=\"log_download('firsova-mishina-sigov-senkevich-pronin-kholkin-bdikin-yuzyuk-femtosecondinfraredlaserannealingofpztfilmsonametalsubstrate-2012', 'https://doi.org/10.1080/00150193.2012.696459', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Femtosecond Infrared Laser Annealing of PZT Films on a Metal Substrate [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150193.2012.696459\"\n     onclick=\"log_download('firsova-mishina-sigov-senkevich-pronin-kholkin-bdikin-yuzyuk-femtosecondinfraredlaserannealingofpztfilmsonametalsubstrate-2012', 'http://doi.org/10.1080/00150193.2012.696459', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/firsova-mishina-sigov-senkevich-pronin-kholkin-bdikin-yuzyuk-femtosecondinfraredlaserannealingofpztfilmsonametalsubstrate-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('firsova-mishina-sigov-senkevich-pronin-kholkin-bdikin-yuzyuk-femtosecondinfraredlaserannealingofpztfilmsonametalsubstrate-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{firsova_femtosecond_2012,\n\ttitle = {Femtosecond {Infrared} {Laser} {Annealing} of {PZT} {Films} on a {Metal} {Substrate}},\n\tvolume = {433},\n\tissn = {0015-0193},\n\turl = {https://doi.org/10.1080/00150193.2012.696459},\n\tdoi = {10.1080/00150193.2012.696459},\n\tabstract = {The quazi-amorphous PbZrTiO2 (PZT) precursor film on a platinized silicon substrate is annealed by femtosecond laser at the wavelength falling into transparency band of PZT. Two areas are found within the laser spot: ferroelectric perovskite revealing strong hysteresis and coercivity in piezoelectric response and paraelectric with low piezoresponse and the absence of hysteresis and coercivity. Annealing takes place through platinum absorbing laser irradiation and acting as a heat source for transparent film on top of it.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Ferroelectrics},\n\tauthor = {Firsova, N. Yu. and Mishina, E. D. and Sigov, A. S. and Senkevich, S. V. and Pronin, I. P. and Kholkin, A. and Bdikin, I. and Yuzyuk, Yu. I.},\n\tmonth = jan,\n\tyear = {2012},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/00150193.2012.696459},\n\tkeywords = {thin films, Raman scattering, ferroelectric, femtosecond laser annealing, piezoelectric, second harmonic generation, Sol-gel},\n\tpages = {164--169},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The quazi-amorphous PbZrTiO2 (PZT) precursor film on a platinized silicon substrate is annealed by femtosecond laser at the wavelength falling into transparency band of PZT. Two areas are found within the laser spot: ferroelectric perovskite revealing strong hysteresis and coercivity in piezoelectric response and paraelectric with low piezoresponse and the absence of hysteresis and coercivity. Annealing takes place through platinum absorbing laser irradiation and acting as a heat source for transparent film on top of it.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"maslova-mikheykin-leontiev-yuzyuk-tkachev-diagnosticsofcarbonaceousnanomaterialtaunitbyramanspectroscopy-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  Diagnostics of Carbonaceous Nanomaterial “Taunit” by Raman Spectroscopy.\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Maslova, O. A.; Mikheykin, A. S.; Leontiev, I. N.; Yuzyuk, Y. I.;  and Tkachev, A. G.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Nanoelectronics and Optoelectronics</i>, 7(1): 95–98. January 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n\n  \n  <a href=\"http://doi.org/10.1166/jno.2012.1225\"\n     onclick=\"log_download('maslova-mikheykin-leontiev-yuzyuk-tkachev-diagnosticsofcarbonaceousnanomaterialtaunitbyramanspectroscopy-2012', 'http://doi.org/10.1166/jno.2012.1225', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/maslova-mikheykin-leontiev-yuzyuk-tkachev-diagnosticsofcarbonaceousnanomaterialtaunitbyramanspectroscopy-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('maslova-mikheykin-leontiev-yuzyuk-tkachev-diagnosticsofcarbonaceousnanomaterialtaunitbyramanspectroscopy-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{maslova_diagnostics_2012,\n\ttitle = {Diagnostics of {Carbonaceous} {Nanomaterial} “{Taunit}” by {Raman} {Spectroscopy}},\n\tvolume = {7},\n\tdoi = {10.1166/jno.2012.1225},\n\tabstract = {Crystalline structure perfection of carbonaceous nanomaterial (CNM) “Taunit” which constitutes the multi-walled nanotubes was studied using a Raman spectroscopy technique. CNM “Taunit” was synthesized by MOCVD method. The pristine material, the samples annealed\nat different temperatures and the samples functionalized by Pt-catalyst nanoparticles were investigated. It has been found that “Taunit” belongs to the poorly organized carbon materials but its crystalline structure was observed to order while the annealing temperature increased.\nD1 and G Raman band (at 1350 and 1580 cm–1, respectively) intensity ratios were calculated to estimate the crystal structure ordering of CNM “Taunit”. The investigation of the influence of functionalization by the catalyst nanoparticles shows that Pt-catalyst\nprecipitation on the surface of MWNTs leads to the increase of the defect band intensity due to an appearance of lattice defects.},\n\tnumber = {1},\n\tjournal = {Journal of Nanoelectronics and Optoelectronics},\n\tauthor = {Maslova, O. A. and Mikheykin, A. S. and Leontiev, I. N. and Yuzyuk, Yu. I. and Tkachev, A. G.},\n\tmonth = jan,\n\tyear = {2012},\n\tkeywords = {RAMAN SPECTROSCOPY, CRYSTALLINE STRUCTURE ORDERING, D- AND G-BAND INTENSITIES RATIOS, MULTI-WALLED CARBON NANOTUBES, PT-CATALYST NANOPARTICLES},\n\tpages = {95--98},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Crystalline structure perfection of carbonaceous nanomaterial (CNM) “Taunit” which constitutes the multi-walled nanotubes was studied using a Raman spectroscopy technique. CNM “Taunit” was synthesized by MOCVD method. The pristine material, the samples annealed at different temperatures and the samples functionalized by Pt-catalyst nanoparticles were investigated. It has been found that “Taunit” belongs to the poorly organized carbon materials but its crystalline structure was observed to order while the annealing temperature increased. D1 and G Raman band (at 1350 and 1580 cm–1, respectively) intensity ratios were calculated to estimate the crystal structure ordering of CNM “Taunit”. The investigation of the influence of functionalization by the catalyst nanoparticles shows that Pt-catalyst precipitation on the surface of MWNTs leads to the increase of the defect band intensity due to an appearance of lattice defects.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"levshov-yuzyuk-michel-voisin-alvarez-berger-roussignol-sauvajol-ramanstudyofuniaxialstraininindividualsinglewallcarbonnanotubesinducedbytemperaturechanges-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  Raman Study of Uniaxial Strain in Individual Single-Wall Carbon Nanotubes Induced by Temperature Changes.\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Levshov, D. I.; Yuzyuk, Y. I.; Michel, T.; Voisin, C.; Alvarez, L.; Berger, S.; Roussignol, P.;  and Sauvajol, J.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Nanoelectronics and Optoelectronics</i>, 7(1): 77–80. January 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n\n  \n  <a href=\"http://doi.org/10.1166/jno.2012.1221\"\n     onclick=\"log_download('levshov-yuzyuk-michel-voisin-alvarez-berger-roussignol-sauvajol-ramanstudyofuniaxialstraininindividualsinglewallcarbonnanotubesinducedbytemperaturechanges-2012', 'http://doi.org/10.1166/jno.2012.1221', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/levshov-yuzyuk-michel-voisin-alvarez-berger-roussignol-sauvajol-ramanstudyofuniaxialstraininindividualsinglewallcarbonnanotubesinducedbytemperaturechanges-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('levshov-yuzyuk-michel-voisin-alvarez-berger-roussignol-sauvajol-ramanstudyofuniaxialstraininindividualsinglewallcarbonnanotubesinducedbytemperaturechanges-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{levshov_raman_2012,\n\ttitle = {Raman {Study} of {Uniaxial} {Strain} in {Individual} {Single}-{Wall} {Carbon} {Nanotubes} {Induced} by {Temperature} {Changes}},\n\tvolume = {7},\n\tdoi = {10.1166/jno.2012.1221},\n\tabstract = {We report the temperature dependence of the Raman spectra of a gelatine-based composite material doped with single-walled carbon nanotubes (SWNT@gelatin). On decreasing the temperature from 290 to 20 K a significant up-shift of the G-mode and no changes in the radial breathing modes\nare observed. This behaviour cannot be understood by pure thermal effects. We explain these results in terms of an uniaxial strain of the nanotubes induced by the thermal expansion mismatch between the nanotubes and the surrounding matrix.},\n\tnumber = {1},\n\tjournal = {Journal of Nanoelectronics and Optoelectronics},\n\tauthor = {Levshov, D. I. and Yuzyuk, Yu. I. and Michel, T. and Voisin, C. and Alvarez, L. and Berger, S. and Roussignol, P. and Sauvajol, J.-L.},\n\tmonth = jan,\n\tyear = {2012},\n\tkeywords = {RAMAN SPECTROSCOPY, COMPOSITES, SINGLE-WALLED CARBON NANOTUBES, UNIAXIAL STRAIN},\n\tpages = {77--80},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We report the temperature dependence of the Raman spectra of a gelatine-based composite material doped with single-walled carbon nanotubes (SWNT@gelatin). On decreasing the temperature from 290 to 20 K a significant up-shift of the G-mode and no changes in the radial breathing modes are observed. This behaviour cannot be understood by pure thermal effects. We explain these results in terms of an uniaxial strain of the nanotubes induced by the thermal expansion mismatch between the nanotubes and the surrounding matrix.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"ivanov-sherstyuk-mishina-sigov-mukhortov-moshnyaga-enhancedmagnetizationandferroelectricswitchinginmultiferroicbstbnfosuperstructures-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/00150193.2012.696448\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'ivanov-sherstyuk-mishina-sigov-mukhortov-moshnyaga-enhancedmagnetizationandferroelectricswitchinginmultiferroicbstbnfosuperstructures-2012', 'https://doi.org/10.1080/00150193.2012.696448', event);\">\n    Enhanced Magnetization and Ferroelectric Switching in Multiferroic BST/BNFO Superstructures.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Ivanov, M. S.; Sherstyuk, N. E.; Mishina, E. D.; Sigov, A. S.; Mukhortov, V. M.;  and Moshnyaga, V. T.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 433(1): 158–163. January 2012.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2012.696448</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/00150193.2012.696448\"\n     onclick=\"log_download('ivanov-sherstyuk-mishina-sigov-mukhortov-moshnyaga-enhancedmagnetizationandferroelectricswitchinginmultiferroicbstbnfosuperstructures-2012', 'https://doi.org/10.1080/00150193.2012.696448', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Enhanced Magnetization and Ferroelectric Switching in Multiferroic BST/BNFO Superstructures [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150193.2012.696448\"\n     onclick=\"log_download('ivanov-sherstyuk-mishina-sigov-mukhortov-moshnyaga-enhancedmagnetizationandferroelectricswitchinginmultiferroicbstbnfosuperstructures-2012', 'http://doi.org/10.1080/00150193.2012.696448', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/ivanov-sherstyuk-mishina-sigov-mukhortov-moshnyaga-enhancedmagnetizationandferroelectricswitchinginmultiferroicbstbnfosuperstructures-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('ivanov-sherstyuk-mishina-sigov-mukhortov-moshnyaga-enhancedmagnetizationandferroelectricswitchinginmultiferroicbstbnfosuperstructures-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{ivanov_enhanced_2012,\n\ttitle = {Enhanced {Magnetization} and {Ferroelectric} {Switching} in {Multiferroic} {BST}/{BNFO} {Superstructures}},\n\tvolume = {433},\n\tissn = {0015-0193},\n\turl = {https://doi.org/10.1080/00150193.2012.696448},\n\tdoi = {10.1080/00150193.2012.696448},\n\tabstract = {Multiferroic BaSrTiO3/NdBiFeO3 (BST/BNFO) mulilayers with 3 nm and 6 nm layer thickness demonstrate superlattice structure in the XRD patterns. The break of the spin cycloide and interface strain results in ferromagnetic behavior and enhancement of magnetization. The total thickness of BNFO is varied in the range of 50–60 nm, and saturation magnetization is varied in the range of 50-60 emu/cm3, which is an order of magnitude higher than reported for BaTiO3/BiFeO3 superstructure [1]. Polarization hysteresis loop were obtained by second harmonic generation technique and show significant electro-optical switchability. Both magnetization and ferroelectric polarization possess bulk rather than interface localization.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Ferroelectrics},\n\tauthor = {Ivanov, M. S. and Sherstyuk, N. E. and Mishina, E. D. and Sigov, A. S. and Mukhortov, V. M. and Moshnyaga, V. T.},\n\tmonth = jan,\n\tyear = {2012},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/00150193.2012.696448},\n\tkeywords = {thin films, superlattice, polarization, Multiferroic, second harmonic generation, magnetization},\n\tpages = {158--163},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Multiferroic BaSrTiO3/NdBiFeO3 (BST/BNFO) mulilayers with 3 nm and 6 nm layer thickness demonstrate superlattice structure in the XRD patterns. The break of the spin cycloide and interface strain results in ferromagnetic behavior and enhancement of magnetization. The total thickness of BNFO is varied in the range of 50–60 nm, and saturation magnetization is varied in the range of 50-60 emu/cm3, which is an order of magnitude higher than reported for BaTiO3/BiFeO3 superstructure [1]. Polarization hysteresis loop were obtained by second harmonic generation technique and show significant electro-optical switchability. Both magnetization and ferroelectric polarization possess bulk rather than interface localization.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"--2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/598\"\n     onclick=\"return trackOutboundLink('publications', 'click', '--2012', 'http://journals.ioffe.ru/articles/598', event);\">\n    Спектры комбинационного рассеяния керамик, пленок и сверхрешеток сегнетоэлектрических перовскитов (О б з о р).\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Юзюк, Ю. И.\n</span>\n\n  \n\n</span>\n\n  . April 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/598\"\n     onclick=\"log_download('--2012', 'http://journals.ioffe.ru/articles/598', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Спектры комбинационного рассеяния керамик, пленок и сверхрешеток сегнетоэлектрических перовскитов (О б з о р) [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/--2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('--2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2012-4,\n\ttitle = {Спектры комбинационного рассеяния керамик, пленок и сверхрешеток сегнетоэлектрических перовскитов (О б з о р)},\n\turl = {http://journals.ioffe.ru/articles/598},\n\turldate = {2023-11-11},\n\tauthor = {Юзюк, Ю. И.},\n\tmonth = apr,\n\tyear = {2012},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----ortega-kumar-katiyar-batiotextrm3batiotextrm3batextrm07srtextrm03tiotextrm3-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  Сравнительное исследование пленки BaTiO$_{\\textrm{3}}$ и сверхрешетки BaTiO$_{\\textrm{3}}$/(Ba$_{\\textrm{0.7}}$Sr$_{\\textrm{0.3}}$)TiO$_{\\textrm{3}}$ методами дифракции рентгеновских лучей и спектроскопии комбинационного рассеяния света.\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Маслова, О. А.; Захарченко, И. Н.; Бунина, О. А.; Юзюк, Ю. И.; Ortega, N.; Kumar, A.;  and Katiyar, R. S.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 54(8): 1526–1532. July 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----ortega-kumar-katiyar-batiotextrm3batiotextrm3batextrm07srtextrm03tiotextrm3-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----ortega-kumar-katiyar-batiotextrm3batiotextrm3batextrm07srtextrm03tiotextrm3-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2012-5,\n\ttitle = {Сравнительное исследование пленки {BaTiO}$_{\\textrm{3}}$ и сверхрешетки {BaTiO}$_{\\textrm{3}}$/({Ba}$_{\\textrm{0.7}}${Sr}$_{\\textrm{0.3}}$){TiO}$_{\\textrm{3}}$ методами дифракции рентгеновских лучей и спектроскопии комбинационного рассеяния света},\n\tvolume = {54},\n\tabstract = {Проведено сравнительное исследование эпитаксиальной пленки BaTiO3 и сверхрешетки состава BaTiO3/(Ba0.7Sr0.3)TiO3, изготовленных методом импульсного лазерного осаждения на подложках (100) MgO. На основе данных рентгеновской дифрактометрии установлена полная параллельная ориентация пленки и подложки, определены период модуляции сверхрешетки Lambda=28 nm, параметры ячейки, усредненной по периоду Lambda, и параметры ячеек слоев сверхрешетки. Согласно рентгенографическим данным, ячейка однокомпонентной пленки BaTiO3 и усредненная по периоду Lambda ячейка сверхрешетки являются псевдокубическими, однако анализ поляризационных характеристик спектров комбинационного рассеяния света позволил предположить моноклинную симметрию (Px=Py\\#0, Pz\\#0) в пленке и сверхрешетке. Обсуждается трансформация компонент мягкой моды, обусловленная деформацией эпитаксиальных слоев, образующих сверхрешетку.},\n\tlanguage = {ru},\n\tnumber = {8},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Маслова, О. А. and Захарченко, И. Н. and Бунина, О. А. and Юзюк, Ю. И. and Ortega, N. and Kumar, A. and Katiyar, R. S.},\n\tmonth = jul,\n\tyear = {2012},\n\tpages = {1526--1532},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Проведено сравнительное исследование эпитаксиальной пленки BaTiO3 и сверхрешетки состава BaTiO3/(Ba0.7Sr0.3)TiO3, изготовленных методом импульсного лазерного осаждения на подложках (100) MgO. На основе данных рентгеновской дифрактометрии установлена полная параллельная ориентация пленки и подложки, определены период модуляции сверхрешетки Lambda=28 nm, параметры ячейки, усредненной по периоду Lambda, и параметры ячеек слоев сверхрешетки. Согласно рентгенографическим данным, ячейка однокомпонентной пленки BaTiO3 и усредненная по периоду Lambda ячейка сверхрешетки являются псевдокубическими, однако анализ поляризационных характеристик спектров комбинационного рассеяния света позволил предположить моноклинную симметрию (Px=Py#0, Pz#0) в пленке и сверхрешетке. Обсуждается трансформация компонент мягкой моды, обусловленная деформацией эпитаксиальных слоев, образующих сверхрешетку.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-------bifeotextrm3-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/623\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-------bifeotextrm3-2012', 'http://journals.ioffe.ru/articles/623', event);\">\n    Влияние морфологии керамик BiFeO$_{\\textrm{3}}$ на электродинамические свойства в терагерцевом диапазоне частот.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Командин, Г. А.; Торгашев, В. И.; Волков, А. А.; Породинков, О. Е.; Пронин, А. А.; Исхакова, Л. Д.;  and Буш, А. А.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 54(6): 1120–1127. May 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/623\"\n     onclick=\"log_download('-------bifeotextrm3-2012', 'http://journals.ioffe.ru/articles/623', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Влияние морфологии керамик BiFeO$_{\\textrm{3}}$ на электродинамические свойства в терагерцевом диапазоне частот [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-------bifeotextrm3-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-------bifeotextrm3-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2012-6,\n\ttitle = {Влияние морфологии керамик {BiFeO}$_{\\textrm{3}}$ на электродинамические свойства в терагерцевом диапазоне частот},\n\tvolume = {54},\n\turl = {http://journals.ioffe.ru/articles/623},\n\tabstract = {Методами субмиллиметровой и инфракрасной Фурье-спектроскопии исследована природа вклада, дополнительного к фононному, в диэлектрическую проницаемость керамик феррита висмута. Выявлено, что его численное значение зависит от морфологических особенностей образцов, а природа обусловлена наличием дефектов и межкристаллитных границ. Отмечено влияние структурно-фазовых особенностей керамик феррита висмута на частоты линий антиферромагнитного резонанса.},\n\tlanguage = {ru},\n\tnumber = {6},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Командин, Г. А. and Торгашев, В. И. and Волков, А. А. and Породинков, О. Е. and Пронин, А. А. and Исхакова, Л. Д. and Буш, А. А.},\n\tmonth = may,\n\tyear = {2012},\n\tpages = {1120--1127},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Методами субмиллиметровой и инфракрасной Фурье-спектроскопии исследована природа вклада, дополнительного к фононному, в диэлектрическую проницаемость керамик феррита висмута. Выявлено, что его численное значение зависит от морфологических особенностей образцов, а природа обусловлена наличием дефектов и межкристаллитных границ. Отмечено влияние структурно-фазовых особенностей керамик феррита висмута на частоты линий антиферромагнитного резонанса.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"--------etal-cocrtextrm2otextrm4-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/523\"\n     onclick=\"return trackOutboundLink('publications', 'click', '--------etal-cocrtextrm2otextrm4-2012', 'http://journals.ioffe.ru/articles/523', event);\">\n    Магнитный и диэлектрический отклик кобальт-хромовой шпинели CoCr$_{\\textrm{2}}$O$_{\\textrm{4}}$ в терагерцевой области частот.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Торгашев, В. И.; Прохоров, А. С.; Командин, Г. А.; Жукова, Е. С.; Анзин, В. Б.; Таланов, В. М.; Рабкин, Л. М.; Буш, А. А.; Dressel, M.;  and Горшунов, Б. П.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 54(2): 330–339. January 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/523\"\n     onclick=\"log_download('--------etal-cocrtextrm2otextrm4-2012', 'http://journals.ioffe.ru/articles/523', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Магнитный и диэлектрический отклик кобальт-хромовой шпинели CoCr$_{\\textrm{2}}$O$_{\\textrm{4}}$ в терагерцевой области частот [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/--------etal-cocrtextrm2otextrm4-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('--------etal-cocrtextrm2otextrm4-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2012-7,\n\ttitle = {Магнитный и диэлектрический отклик кобальт-хромовой шпинели {CoCr}$_{\\textrm{2}}${O}$_{\\textrm{4}}$ в терагерцевой области частот},\n\tvolume = {54},\n\turl = {http://journals.ioffe.ru/articles/523},\n\tabstract = {Методами субмиллиметровой спектроскопии и инфракрасной Фурье-спектроскопии исследована природа фононных и магнонных мод в мультиферроике CoCr2O4 со структурой кубической шпинели. Впервые измерена температурная эволюция обменного оптического магнона в ферримагнитной (TC=94 K) и двух низкосимметричных (TS{\\textasciitilde} 26 K, Tlock-in=14.5 K) фазах CoCr2O4 вплоть до T=5 K в нулевом магнитном поле. Показано, что зарегистрированный магнон не является ферримагнитным параметром порядка и, вероятнее всего, обусловлен прецессией спинов в подрешетках кобальта. В точках магнитных фазовых переходов осцилляторные параметры двух наиболее низкочастотных фононных мод проявляют аномальную температурную зависимость, что свидетельствует о значительном взаимодействии между магнитной и фононной подсистемами. На основании того, что параметр затухания фононной моды, обусловленной колебаниями тетраэдров CoO4, при переходе CoCr2O4 в состояние мультиферроика (T{\\textless}TS) увеличивается на 25\\%, сделано предположение о структурных изменениях в решетке с потерей пространственной центросимметричности среды.},\n\tlanguage = {ru},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Торгашев, В. И. and Прохоров, А. С. and Командин, Г. А. and Жукова, Е. С. and Анзин, В. Б. and Таланов, В. М. and Рабкин, Л. М. and Буш, А. А. and Dressel, M. and Горшунов, Б. П.},\n\tmonth = jan,\n\tyear = {2012},\n\tpages = {330--339},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Методами субмиллиметровой спектроскопии и инфракрасной Фурье-спектроскопии исследована природа фононных и магнонных мод в мультиферроике CoCr2O4 со структурой кубической шпинели. Впервые измерена температурная эволюция обменного оптического магнона в ферримагнитной (TC=94 K) и двух низкосимметричных (TS~ 26 K, Tlock-in=14.5 K) фазах CoCr2O4 вплоть до T=5 K в нулевом магнитном поле. Показано, что зарегистрированный магнон не является ферримагнитным параметром порядка и, вероятнее всего, обусловлен прецессией спинов в подрешетках кобальта. В точках магнитных фазовых переходов осцилляторные параметры двух наиболее низкочастотных фононных мод проявляют аномальную температурную зависимость, что свидетельствует о значительном взаимодействии между магнитной и фононной подсистемами. На основании того, что параметр затухания фононной моды, обусловленной колебаниями тетраэдров CoO4, при переходе CoCr2O4 в состояние мультиферроика (T\\textlessTS) увеличивается на 25%, сделано предположение о структурных изменениях в решетке с потерей пространственной центросимметричности среды.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"--------2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/840\"\n     onclick=\"return trackOutboundLink('publications', 'click', '--------2012', 'http://journals.ioffe.ru/articles/840', event);\">\n    Нелинейно-оптическая микроскопия и спектроскопия сегнетоэлектрических и мультиферроидных материалов.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Мишина, Е. Д.; Семин, С. В.; Швырков, К. В.; Кудрявцев, А. В.; Ильин, Н. А.; Шерстюк, Н. Э.;  and Мухортов, В. М.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 54(5): 836–841. April 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/840\"\n     onclick=\"log_download('--------2012', 'http://journals.ioffe.ru/articles/840', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Нелинейно-оптическая микроскопия и спектроскопия сегнетоэлектрических и мультиферроидных материалов [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/--------2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('--------2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{_-_2012,\n\ttitle = {Нелинейно-оптическая микроскопия и спектроскопия сегнетоэлектрических и мультиферроидных материалов},\n\tvolume = {54},\n\turl = {http://journals.ioffe.ru/articles/840},\n\tabstract = {Раcсмотрены особенности применения двухфотонной микроскопии и спектроскопии для исследования мультиферроидных и пьезоэлектрических наноразмерных структур. Для наноразмерных планарных мультислойных структур титанат бария-стронция/феррит висмута показано проявление в нелинейно-оптическом отклике локальных электроиндуцированного и магнитоиндуцированного вкладов в определенных спектральных диапазонах. Для пьезоэлектрических био-микротрубок пептидов показано, что максимальное значение интенсивности второй гармоники не меняется вдоль трубки, в то время как направление поляризации изменяется значительно.},\n\tlanguage = {ru},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Мишина, Е. Д. and Семин, С. В. and Швырков, К. В. and Кудрявцев, А. В. and Ильин, Н. А. and Шерстюк, Н. Э. and Мухортов, В. М.},\n\tmonth = apr,\n\tyear = {2012},\n\tpages = {836--841},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Раcсмотрены особенности применения двухфотонной микроскопии и спектроскопии для исследования мультиферроидных и пьезоэлектрических наноразмерных структур. Для наноразмерных планарных мультислойных структур титанат бария-стронция/феррит висмута показано проявление в нелинейно-оптическом отклике локальных электроиндуцированного и магнитоиндуцированного вкладов в определенных спектральных диапазонах. Для пьезоэлектрических био-микротрубок пептидов показано, что максимальное значение интенсивности второй гармоники не меняется вдоль трубки, в то время как направление поляризации изменяется значительно.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/859\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------2012', 'http://journals.ioffe.ru/articles/859', event);\">\n    Электропроводность и термо-э.д.с. кристаллов титаната свинца.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Гавриляченко, В. Г.; Семенчев, А. Ф.; Авакян, Е. И.; Панченко, Е. М.;  and Мартыщенко, А. В.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 54(5): 901–902. April 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/859\"\n     onclick=\"log_download('------2012', 'http://journals.ioffe.ru/articles/859', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Электропроводность и термо-э.д.с. кристаллов титаната свинца [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>1 download</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2012-8,\n\ttitle = {Электропроводность и термо-э.д.с. кристаллов титаната свинца},\n\tvolume = {54},\n\turl = {http://journals.ioffe.ru/articles/859},\n\tabstract = {Исследованы температурные зависимости коэффициента термо-э.д.с. alpha и удельной объемной электропроводности sigmaV в температурном интервале 400-550 K, где в кристаллах титаната свинца наблюдаются аномалии диэлектрической проницаемости varepsilon, не связанные с фазовым переходом. Установлено, что в указанном интервале температур alpha имеет максимум и во многих кристаллах меняет знак, при этом sigmaV снижается. Сделано предположение о том, что аномалии alpha и sigmaV, коррелирующие с аномалиями varepsilon, обусловлены термоактивацией ловушек электронов, что приводит к компенсации проводимости p-типа. Определены концентрация свободных носителей заряда и их дрейфовая подвижность в парафазе вблизи точки Кюри. Эти данные указывают на возможность полного внутреннего экранирования связанного заряда Ps.},\n\tlanguage = {ru},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Гавриляченко, В. Г. and Семенчев, А. Ф. and Авакян, Е. И. and Панченко, Е. М. and Мартыщенко, А. В.},\n\tmonth = apr,\n\tyear = {2012},\n\tpages = {901--902},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследованы температурные зависимости коэффициента термо-э.д.с. alpha и удельной объемной электропроводности sigmaV в температурном интервале 400-550 K, где в кристаллах титаната свинца наблюдаются аномалии диэлектрической проницаемости varepsilon, не связанные с фазовым переходом. Установлено, что в указанном интервале температур alpha имеет максимум и во многих кристаллах меняет знак, при этом sigmaV снижается. Сделано предположение о том, что аномалии alpha и sigmaV, коррелирующие с аномалиями varepsilon, обусловлены термоактивацией ловушек электронов, что приводит к компенсации проводимости p-типа. Определены концентрация свободных носителей заряда и их дрейфовая подвижность в парафазе вблизи точки Кюри. Эти данные указывают на возможность полного внутреннего экранирования связанного заряда Ps.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------labgeotextrm5labsiotextrm5-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/780\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------labgeotextrm5labsiotextrm5-2012', 'http://journals.ioffe.ru/articles/780', event);\">\n    Электродинамические характеристики стекол составов LaBGeO$_{\\textrm{5}}$ и LaBSiO$_{\\textrm{5}}$ в терагерцевом и ИК-диапазонах.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Командин, Г. А.; Сигаев, В. Н.; Торгашев, В. И.; Лотарев, С. В.; Породинков, О. Е.;  and Спектор, И. Е.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 54(11): 2058–2065. October 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/780\"\n     onclick=\"log_download('------labgeotextrm5labsiotextrm5-2012', 'http://journals.ioffe.ru/articles/780', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Электродинамические характеристики стекол составов LaBGeO$_{\\textrm{5}}$ и LaBSiO$_{\\textrm{5}}$ в терагерцевом и ИК-диапазонах [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------labgeotextrm5labsiotextrm5-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------labgeotextrm5labsiotextrm5-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2012-9,\n\ttitle = {Электродинамические характеристики стекол составов {LaBGeO}$_{\\textrm{5}}$ и {LaBSiO}$_{\\textrm{5}}$ в терагерцевом и ИК-диапазонах},\n\tvolume = {54},\n\turl = {http://journals.ioffe.ru/articles/780},\n\tabstract = {Сравниваются методы расчета функций диэлектрического отклика разупорядоченных веществ по пропусканию (субмиллиметровый диапазон) и отражению (ИК диапазон) на примере функциональных стекол LaBGeO5 и LaBSiO5 со структурой стиллвеллита. В рамках четырехпараметрической факторизованной модели дисперсии определены диэлектрические параметры стекол LaBGeO5 и LaBSiO5 и выполнено соотнесение спектральных полос с фрагментами структуры.},\n\tlanguage = {ru},\n\tnumber = {11},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Командин, Г. А. and Сигаев, В. Н. and Торгашев, В. И. and Лотарев, С. В. and Породинков, О. Е. and Спектор, И. Е.},\n\tmonth = oct,\n\tyear = {2012},\n\tpages = {2058--2065},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Сравниваются методы расчета функций диэлектрического отклика разупорядоченных веществ по пропусканию (субмиллиметровый диапазон) и отражению (ИК диапазон) на примере функциональных стекол LaBGeO5 и LaBSiO5 со структурой стиллвеллита. В рамках четырехпараметрической факторизованной модели дисперсии определены диэлектрические параметры стекол LaBGeO5 и LaBSiO5 и выполнено соотнесение спектральных полос с фрагментами структуры.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----ortega-kumar-katiyar-batiotextrm3basrtiotextrm3-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/878\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----ortega-kumar-katiyar-batiotextrm3basrtiotextrm3-2012', 'http://journals.ioffe.ru/articles/878', event);\">\n    Исследование сверхрешеток BaTiO$_{\\textrm{3}}$/(Ba,Sr)TiO$_{\\textrm{3}}$ методом дифракции рентгеновских лучей.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Маслова, О. А.; Захарченко, И. Н.; Бунина, О. А.; Юзюк, Ю. И.; Ortega, N.; Kumar, A.;  and Katiyar, R. S.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 54(5): 953–955. April 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/878\"\n     onclick=\"log_download('----ortega-kumar-katiyar-batiotextrm3basrtiotextrm3-2012', 'http://journals.ioffe.ru/articles/878', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Исследование сверхрешеток BaTiO$_{\\textrm{3}}$/(Ba,Sr)TiO$_{\\textrm{3}}$ методом дифракции рентгеновских лучей [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----ortega-kumar-katiyar-batiotextrm3basrtiotextrm3-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----ortega-kumar-katiyar-batiotextrm3basrtiotextrm3-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2012-10,\n\ttitle = {Исследование сверхрешеток {BaTiO}$_{\\textrm{3}}$/({Ba},{Sr}){TiO}$_{\\textrm{3}}$ методом дифракции рентгеновских лучей},\n\tvolume = {54},\n\turl = {http://journals.ioffe.ru/articles/878},\n\tabstract = {Методом дифракции рентгеновских лучей проведено исследование образцов сверхрешеток BaTiO3/ (Ba1-xSrx)TiO3 (ВТ/BST-x). Установлена полная параллельная ориентация всех пленок и подложки, определены периоды модуляции Lambda сверхрешеток, параметры ячейки, усредненной по периоду Lambda, и параметры отдельных компонент сверхрешеток.},\n\tlanguage = {ru},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Маслова, О. А. and Захарченко, И. Н. and Бунина, О. А. and Юзюк, Ю. И. and Ortega, N. and Kumar, A. and Katiyar, R. S.},\n\tmonth = apr,\n\tyear = {2012},\n\tpages = {953--955},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Методом дифракции рентгеновских лучей проведено исследование образцов сверхрешеток BaTiO3/ (Ba1-xSrx)TiO3 (ВТ/BST-x). Установлена полная параллельная ориентация всех пленок и подложки, определены периоды модуляции Lambda сверхрешеток, параметры ячейки, усредненной по периоду Lambda, и параметры отдельных компонент сверхрешеток.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----agau-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/10727\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----agau-2012', 'http://journals.ioffe.ru/articles/10727', event);\">\n    Магнетронное и импульсное лазерное напыление наночастиц и несплошных пленок Ag и Au и исследование их оптических свойств.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Лянгузов, Н. В.; Кайдашев, В. Е.; Широков, В. Б.;  and Кайдашев, Е. М.\n</span>\n\n  \n\n</span>\n\n  <i>Журнал технической физики</i>, 82(10): 90–95. September 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/10727\"\n     onclick=\"log_download('----agau-2012', 'http://journals.ioffe.ru/articles/10727', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Магнетронное и импульсное лазерное напыление наночастиц и несплошных пленок Ag и Au и исследование их оптических свойств [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----agau-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----agau-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2012-11,\n\ttitle = {Магнетронное и импульсное лазерное напыление наночастиц и несплошных пленок {Ag} и {Au} и исследование их оптических свойств},\n\tvolume = {82},\n\turl = {http://journals.ioffe.ru/articles/10727},\n\tabstract = {Исследованы различные режимы получения наночастиц Ag и Au методами магнетронного и импульсного лазерного напыления и особенности спектров поглощения, связанные с плазмонными резонансами. Для получения наночастиц серебра малых размеров (5-10 nm) с большой плотностью поверхностного распределения определен оптимальный режим получения: повышенное давление аргона (2.5·10-2 Torr) и малое напряжение разряда (100 V). Массивы наночастиц Au, полученные методом импульского лазерного напыления, проявляют более высокую однородность при напылении на подложки при температуре 200oC в вакууме, нежели при комнатной температуре в атмосфере аргона. Показано, что положение максимума плазмонного поглощения сдвигается в область меньших длин волн при снижении значения эквивалентной толщины пленок металлов и зависит не только от данного значения, но и от типа подложки, которая определяет морфологические характеристики массивов наночастиц.},\n\tlanguage = {ru},\n\tnumber = {10},\n\turldate = {2023-11-11},\n\tjournal = {Журнал технической физики},\n\tauthor = {Лянгузов, Н. В. and Кайдашев, В. Е. and Широков, В. Б. and Кайдашев, Е. М.},\n\tmonth = sep,\n\tyear = {2012},\n\tpages = {90--95},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследованы различные режимы получения наночастиц Ag и Au методами магнетронного и импульсного лазерного напыления и особенности спектров поглощения, связанные с плазмонными резонансами. Для получения наночастиц серебра малых размеров (5-10 nm) с большой плотностью поверхностного распределения определен оптимальный режим получения: повышенное давление аргона (2.5·10-2 Torr) и малое напряжение разряда (100 V). Массивы наночастиц Au, полученные методом импульского лазерного напыления, проявляют более высокую однородность при напылении на подложки при температуре 200oC в вакууме, нежели при комнатной температуре в атмосфере аргона. Показано, что положение максимума плазмонного поглощения сдвигается в область меньших длин волн при снижении значения эквивалентной толщины пленок металлов и зависит не только от данного значения, но и от типа подложки, которая определяет морфологические характеристики массивов наночастиц.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/850\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----2012', 'http://journals.ioffe.ru/articles/850', event);\">\n    Фазовые переходы в поляризованных гетерофазных системах на основе цирконата-титаната свинца.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Милов, Е. В.; Акбаева, Г. М.; Гавриляченко, В. Г.;  and Семенчев, А. Ф.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 54(5): 878–879. April 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/850\"\n     onclick=\"log_download('-----2012', 'http://journals.ioffe.ru/articles/850', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Фазовые переходы в поляризованных гетерофазных системах на основе цирконата-титаната свинца [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2012-12,\n\ttitle = {Фазовые переходы в поляризованных гетерофазных системах на основе цирконата-титаната свинца},\n\tvolume = {54},\n\turl = {http://journals.ioffe.ru/articles/850},\n\tabstract = {Исследованы зависимости токов деполяризации, определены фазовые превращения между фазами R3c, R3m, P4mm и Pm3m в образцах пятикомпонентной гетерофазной сегнетокерамики на основе цирконата-титаната свинца.},\n\tlanguage = {ru},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Милов, Е. В. and Акбаева, Г. М. and Гавриляченко, В. Г. and Семенчев, А. Ф.},\n\tmonth = apr,\n\tyear = {2012},\n\tpages = {878--879},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследованы зависимости токов деполяризации, определены фазовые превращения между фазами R3c, R3m, P4mm и Pm3m в образцах пятикомпонентной гетерофазной сегнетокерамики на основе цирконата-титаната свинца.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"bunina-zakharchenko-golovko-mukhortov-stryukov-yuzyuk-structuralpropertiesofcompositethinfilmsbifeotextrm3batextrm08srtextrm02tiotextrm3-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/00150193.2012.741920\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'bunina-zakharchenko-golovko-mukhortov-stryukov-yuzyuk-structuralpropertiesofcompositethinfilmsbifeotextrm3batextrm08srtextrm02tiotextrm3-2012', 'https://doi.org/10.1080/00150193.2012.741920', event);\">\n    Structural Properties of Composite Thin Films BiFeO$_{\\textrm{3}}$ - Ba$_{\\textrm{0.8}}$Sr$_{\\textrm{0.2}}$TiO$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Bunina, O. A.; Zakharchenko, I. N.; Golovko, Y. I.; Mukhortov, V. M.; Stryukov, D. V.;  and Yuzyuk, Y. I.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 439(1): 67–73. January 2012.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2012.741920</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/00150193.2012.741920\"\n     onclick=\"log_download('bunina-zakharchenko-golovko-mukhortov-stryukov-yuzyuk-structuralpropertiesofcompositethinfilmsbifeotextrm3batextrm08srtextrm02tiotextrm3-2012', 'https://doi.org/10.1080/00150193.2012.741920', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Structural Properties of Composite Thin Films BiFeO$_{\\textrm{3}}$ - Ba$_{\\textrm{0.8}}$Sr$_{\\textrm{0.2}}$TiO$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150193.2012.741920\"\n     onclick=\"log_download('bunina-zakharchenko-golovko-mukhortov-stryukov-yuzyuk-structuralpropertiesofcompositethinfilmsbifeotextrm3batextrm08srtextrm02tiotextrm3-2012', 'http://doi.org/10.1080/00150193.2012.741920', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/bunina-zakharchenko-golovko-mukhortov-stryukov-yuzyuk-structuralpropertiesofcompositethinfilmsbifeotextrm3batextrm08srtextrm02tiotextrm3-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('bunina-zakharchenko-golovko-mukhortov-stryukov-yuzyuk-structuralpropertiesofcompositethinfilmsbifeotextrm3batextrm08srtextrm02tiotextrm3-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{bunina_structural_2012,\n\ttitle = {Structural {Properties} of {Composite} {Thin} {Films} {BiFeO}$_{\\textrm{3}}$ - {Ba}$_{\\textrm{0.8}}${Sr}$_{\\textrm{0.2}}${TiO}$_{\\textrm{3}}$},\n\tvolume = {439},\n\tissn = {0015-0193},\n\turl = {https://doi.org/10.1080/00150193.2012.741920},\n\tdoi = {10.1080/00150193.2012.741920},\n\tabstract = {The results of X-ray diffraction study of a new promising magnetoelectric composite films with alternating layers of barium strontium titanate and bismuth ferrite with layer thicknesses d = 6–200 nm are presented. All films show epitaxial growth on the MgO single crystals substrates. The 00L profiles for thick layered films (d {\\textgreater} 15 nm) consist of the two reflections corresponding to the separate coherent scattering regions of composite layers. The XRD patterns of thin layered films testify the formation of superlattice. The mean microstrain and mean size of coherent scattering regions were determined using the Willamson-Hall approach.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Ferroelectrics},\n\tauthor = {Bunina, O. A. and Zakharchenko, I. N. and Golovko, Yu. I. and Mukhortov, V. M. and Stryukov, D. V. and Yuzyuk, Yu. I.},\n\tmonth = jan,\n\tyear = {2012},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/00150193.2012.741920},\n\tkeywords = {X-ray diffraction, superlattice, Thin films, magnetoelectric composite},\n\tpages = {67--73},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The results of X-ray diffraction study of a new promising magnetoelectric composite films with alternating layers of barium strontium titanate and bismuth ferrite with layer thicknesses d = 6–200 nm are presented. All films show epitaxial growth on the MgO single crystals substrates. The 00L profiles for thick layered films (d \\textgreater 15 nm) consist of the two reflections corresponding to the separate coherent scattering regions of composite layers. The XRD patterns of thin layered films testify the formation of superlattice. The mean microstrain and mean size of coherent scattering regions were determined using the Willamson-Hall approach.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"bush-shkuratov-kamentsev-prokhorov-zhukova-gorshunov-torgashev-ferroelectricityinspinelsolidsolutioncotextrm08nitextrm02crtextrm2otextrm4-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.85.214112\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'bush-shkuratov-kamentsev-prokhorov-zhukova-gorshunov-torgashev-ferroelectricityinspinelsolidsolutioncotextrm08nitextrm02crtextrm2otextrm4-2012', 'https://link.aps.org/doi/10.1103/PhysRevB.85.214112', event);\">\n    Ferroelectricity in spinel solid solution Co$_{\\textrm{0.8}}$Ni$_{\\textrm{0.2}}$Cr$_{\\textrm{2}}$O$_{\\textrm{4}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Bush, A. A.; Shkuratov, V. Y.; Kamentsev, K. E.; Prokhorov, A. S.; Zhukova, E. S.; Gorshunov, B. P.;  and Torgashev, V. I.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 85(21): 214112. June 2012.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.85.214112\"\n     onclick=\"log_download('bush-shkuratov-kamentsev-prokhorov-zhukova-gorshunov-torgashev-ferroelectricityinspinelsolidsolutioncotextrm08nitextrm02crtextrm2otextrm4-2012', 'https://link.aps.org/doi/10.1103/PhysRevB.85.214112', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Ferroelectricity in spinel solid solution Co$_{\\textrm{0.8}}$Ni$_{\\textrm{0.2}}$Cr$_{\\textrm{2}}$O$_{\\textrm{4}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.85.214112\"\n     onclick=\"log_download('bush-shkuratov-kamentsev-prokhorov-zhukova-gorshunov-torgashev-ferroelectricityinspinelsolidsolutioncotextrm08nitextrm02crtextrm2otextrm4-2012', 'http://doi.org/10.1103/PhysRevB.85.214112', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/bush-shkuratov-kamentsev-prokhorov-zhukova-gorshunov-torgashev-ferroelectricityinspinelsolidsolutioncotextrm08nitextrm02crtextrm2otextrm4-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('bush-shkuratov-kamentsev-prokhorov-zhukova-gorshunov-torgashev-ferroelectricityinspinelsolidsolutioncotextrm08nitextrm02crtextrm2otextrm4-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{bush_ferroelectricity_2012,\n\ttitle = {Ferroelectricity in spinel solid solution {Co}$_{\\textrm{0.8}}${Ni}$_{\\textrm{0.2}}${Cr}$_{\\textrm{2}}${O}$_{\\textrm{4}}$},\n\tvolume = {85},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.85.214112},\n\tdoi = {10.1103/PhysRevB.85.214112},\n\tabstract = {Temperature dependencies of dielectric permittivity and loss tangent (at frequencies 0.1–200 kHz) together with thermally stimulated depolarization currents, magnetization, and Mössbauer spectra of ceramic solid solutions Co1−xNixCr2O4 (x = 0, 0.2, 0.4, 0.6, 1.0) are studied at temperatures from 80 to 350 K. We find evidence of two reversible phase transitions located at T1 and T2 (220 and 245 K, respectively, for x = 0.2), of occurrence of pyroelectric properties below T2, as well as of a phase transition to magnetically ordered state of ferrimagnetic type (below 86 K for x = 0.2). The obtained results evidence that the compounds possess, additionally to magnetic, ferroelectric properties and are thus new members in the family of multiferroics.},\n\tnumber = {21},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Bush, A. A. and Shkuratov, V. Ya. and Kamentsev, K. E. and Prokhorov, A. S. and Zhukova, E. S. and Gorshunov, B. P. and Torgashev, V. I.},\n\tmonth = jun,\n\tyear = {2012},\n\tnote = {Publisher: American Physical Society},\n\tpages = {214112},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Temperature dependencies of dielectric permittivity and loss tangent (at frequencies 0.1–200 kHz) together with thermally stimulated depolarization currents, magnetization, and Mössbauer spectra of ceramic solid solutions Co1−xNixCr2O4 (x = 0, 0.2, 0.4, 0.6, 1.0) are studied at temperatures from 80 to 350 K. We find evidence of two reversible phase transitions located at T1 and T2 (220 and 245 K, respectively, for x = 0.2), of occurrence of pyroelectric properties below T2, as well as of a phase transition to magnetically ordered state of ferrimagnetic type (below 86 K for x = 0.2). The obtained results evidence that the compounds possess, additionally to magnetic, ferroelectric properties and are thus new members in the family of multiferroics.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"druzhinina-yuzyuk-raevski-marssi-laguta-raevskaya-ramanspectraofpbfetextrm05nbtextrm05otextrm3multiferroicsinglecrystalsandceramics-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/00150193.2012.747391\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'druzhinina-yuzyuk-raevski-marssi-laguta-raevskaya-ramanspectraofpbfetextrm05nbtextrm05otextrm3multiferroicsinglecrystalsandceramics-2012', 'https://doi.org/10.1080/00150193.2012.747391', event);\">\n    Raman Spectra of PbFe$_{\\textrm{0.5}}$Nb$_{\\textrm{0.5}}$O$_{\\textrm{3}}$Multiferroic Single Crystals and Ceramics.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Druzhinina, N. S.; Yuzyuk, Y. I.; Raevski, I. P.; Marssi, M. E.; Laguta, V. V.;  and Raevskaya, S. I.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 438(1): 107–114. January 2012.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150193.2012.747391</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/00150193.2012.747391\"\n     onclick=\"log_download('druzhinina-yuzyuk-raevski-marssi-laguta-raevskaya-ramanspectraofpbfetextrm05nbtextrm05otextrm3multiferroicsinglecrystalsandceramics-2012', 'https://doi.org/10.1080/00150193.2012.747391', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Raman Spectra of PbFe$_{\\textrm{0.5}}$Nb$_{\\textrm{0.5}}$O$_{\\textrm{3}}$Multiferroic Single Crystals and Ceramics [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150193.2012.747391\"\n     onclick=\"log_download('druzhinina-yuzyuk-raevski-marssi-laguta-raevskaya-ramanspectraofpbfetextrm05nbtextrm05otextrm3multiferroicsinglecrystalsandceramics-2012', 'http://doi.org/10.1080/00150193.2012.747391', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/druzhinina-yuzyuk-raevski-marssi-laguta-raevskaya-ramanspectraofpbfetextrm05nbtextrm05otextrm3multiferroicsinglecrystalsandceramics-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('druzhinina-yuzyuk-raevski-marssi-laguta-raevskaya-ramanspectraofpbfetextrm05nbtextrm05otextrm3multiferroicsinglecrystalsandceramics-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{druzhinina_raman_2012,\n\ttitle = {Raman {Spectra} of {PbFe}$_{\\textrm{0.5}}${Nb}$_{\\textrm{0.5}}${O}$_{\\textrm{3}}${Multiferroic} {Single} {Crystals} and {Ceramics}},\n\tvolume = {438},\n\tissn = {0015-0193},\n\turl = {https://doi.org/10.1080/00150193.2012.747391},\n\tdoi = {10.1080/00150193.2012.747391},\n\tabstract = {Room temperature Raman spectra of both PbFe0.5Nb0.5O3 (PFN) single crystal and ceramics were found to contain 14 bands, namely 64, 130, 200, 265, 427, 488, 560, 703, 785, 861, 971, 1123, 1236, and 1383 cm−1. For the first time distinct anomalies in the temperature dependences of frequency and/or full width at half maximum were observed for some lines in the Raman spectra of PFN single crystal at both antiferromagnetic (≈150 K) and ferroelectric (≈350 K) phase transitions.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Ferroelectrics},\n\tauthor = {Druzhinina, N. S. and Yuzyuk, Yu. I. and Raevski, I. P. and Marssi, M. El and Laguta, V. V. and Raevskaya, S. I.},\n\tmonth = jan,\n\tyear = {2012},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/00150193.2012.747391},\n\tkeywords = {phase transition, ferroelectric, lead iron niobate, multiferroic, Raman spectra},\n\tpages = {107--114},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Room temperature Raman spectra of both PbFe0.5Nb0.5O3 (PFN) single crystal and ceramics were found to contain 14 bands, namely 64, 130, 200, 265, 427, 488, 560, 703, 785, 861, 971, 1123, 1236, and 1383 cm−1. For the first time distinct anomalies in the temperature dependences of frequency and/or full width at half maximum were observed for some lines in the Raman spectra of PFN single crystal at both antiferromagnetic (≈150 K) and ferroelectric (≈350 K) phase transitions.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"ortega-kumar-yuzyuk-scott-katiyar-ferroelectricanddielectricpropertiesofbatiotextrm3batextrm030srtextrm070tiotextrm3superlattices-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/10584587.2012.673980\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'ortega-kumar-yuzyuk-scott-katiyar-ferroelectricanddielectricpropertiesofbatiotextrm3batextrm030srtextrm070tiotextrm3superlattices-2012', 'https://doi.org/10.1080/10584587.2012.673980', event);\">\n    Ferroelectric and Dielectric Properties of BaTiO$_{\\textrm{3}}$/Ba$_{\\textrm{0.30}}$Sr$_{\\textrm{0.70}}$TiO$_{\\textrm{3}}$ Superlattices.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Ortega, N.; Kumar, A.; Yuzyuk, Y. I.; Scott, J. F.;  and Katiyar, R.\n</span>\n\n  \n\n</span>\n\n  <i>Integrated Ferroelectrics</i>, 134(1): 139–145. January 2012.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/10584587.2012.673980</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/10584587.2012.673980\"\n     onclick=\"log_download('ortega-kumar-yuzyuk-scott-katiyar-ferroelectricanddielectricpropertiesofbatiotextrm3batextrm030srtextrm070tiotextrm3superlattices-2012', 'https://doi.org/10.1080/10584587.2012.673980', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Ferroelectric and Dielectric Properties of BaTiO$_{\\textrm{3}}$/Ba$_{\\textrm{0.30}}$Sr$_{\\textrm{0.70}}$TiO$_{\\textrm{3}}$ Superlattices [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/10584587.2012.673980\"\n     onclick=\"log_download('ortega-kumar-yuzyuk-scott-katiyar-ferroelectricanddielectricpropertiesofbatiotextrm3batextrm030srtextrm070tiotextrm3superlattices-2012', 'http://doi.org/10.1080/10584587.2012.673980', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/ortega-kumar-yuzyuk-scott-katiyar-ferroelectricanddielectricpropertiesofbatiotextrm3batextrm030srtextrm070tiotextrm3superlattices-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('ortega-kumar-yuzyuk-scott-katiyar-ferroelectricanddielectricpropertiesofbatiotextrm3batextrm030srtextrm070tiotextrm3superlattices-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{ortega_ferroelectric_2012,\n\ttitle = {Ferroelectric and {Dielectric} {Properties} of {BaTiO}$_{\\textrm{3}}$/{Ba}$_{\\textrm{0.30}}${Sr}$_{\\textrm{0.70}}${TiO}$_{\\textrm{3}}$ {Superlattices}},\n\tvolume = {134},\n\tissn = {1058-4587},\n\turl = {https://doi.org/10.1080/10584587.2012.673980},\n\tdoi = {10.1080/10584587.2012.673980},\n\tabstract = {BaTiO3/Ba0.30Sr0.70TiO3 (BT/BST3070) artificial superlattice (SL) was fabricated by pulsed laser deposition on La0.67Sr0.33MnO3 (LSMO) coated (001) MgO substrates. Satellite reflections in X-ray diffraction are used to calculate the periodicity of SL structure indicates a period ∼14 nm. Cross polarized Raman spectra show upward shift of the E(1TO) soft mode, this is markedly changed with respect to its parent BT layer thin film. The BT/BST3070 SL illustrates high dielectric constant (1100-1300) and low loss tangent ({\\textless}0.1) below to 104 Hz. Polarization and dielectric constant show strong switching behavior under applied external electric field with well saturated hysteresis loop and high dielectric tunability.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Integrated Ferroelectrics},\n\tauthor = {Ortega, N. and Kumar, Ashok and Yuzyuk, YU. I. and Scott, J. F. and Katiyar, Rams.},\n\tmonth = jan,\n\tyear = {2012},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/10584587.2012.673980},\n\tkeywords = {Superlattices, BT/BST, dielectric, ferroelectric, PLD},\n\tpages = {139--145},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  BaTiO3/Ba0.30Sr0.70TiO3 (BT/BST3070) artificial superlattice (SL) was fabricated by pulsed laser deposition on La0.67Sr0.33MnO3 (LSMO) coated (001) MgO substrates. Satellite reflections in X-ray diffraction are used to calculate the periodicity of SL structure indicates a period ∼14 nm. Cross polarized Raman spectra show upward shift of the E(1TO) soft mode, this is markedly changed with respect to its parent BT layer thin film. The BT/BST3070 SL illustrates high dielectric constant (1100-1300) and low loss tangent (\\textless0.1) below to 104 Hz. Polarization and dielectric constant show strong switching behavior under applied external electric field with well saturated hysteresis loop and high dielectric tunability.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shakhovoy-raevskaya-shakhovaya-suzdalev-raevski-yuzyuk-semenchev-elmarssi-ferroelectricqandantiferroelectricpphasescoexistenceandlocalphasetransitionsinoxygendeficientnanbtextrm3singlecrystalmicroramandielectricanddilatometricstudies-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/jrs.3140\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shakhovoy-raevskaya-shakhovaya-suzdalev-raevski-yuzyuk-semenchev-elmarssi-ferroelectricqandantiferroelectricpphasescoexistenceandlocalphasetransitionsinoxygendeficientnanbtextrm3singlecrystalmicroramandielectricanddilatometricstudies-2012', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/jrs.3140', event);\">\n    Ferroelectric Q and antiferroelectric P phases' coexistence and local phase transitions in oxygen-deficient NaNb$_{\\textrm{3}}$ single crystal: micro-Raman, dielectric and dilatometric studies.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shakhovoy, R. A.; Raevskaya, S. I.; Shakhovaya, L. A.; Suzdalev, D. V.; Raevski, I. P.; Yuzyuk, Y. I.; Semenchev, A. F.;  and El Marssi, M.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Raman Spectroscopy</i>, 43(8): 1141–1145.  2012.\n  <span class=\"note\">_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/jrs.3140</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/jrs.3140\"\n     onclick=\"log_download('shakhovoy-raevskaya-shakhovaya-suzdalev-raevski-yuzyuk-semenchev-elmarssi-ferroelectricqandantiferroelectricpphasescoexistenceandlocalphasetransitionsinoxygendeficientnanbtextrm3singlecrystalmicroramandielectricanddilatometricstudies-2012', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/jrs.3140', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Ferroelectric Q and antiferroelectric P phases&#x27; coexistence and local phase transitions in oxygen-deficient NaNb$_{\\textrm{3}}$ single crystal: micro-Raman, dielectric and dilatometric studies [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1002/jrs.3140\"\n     onclick=\"log_download('shakhovoy-raevskaya-shakhovaya-suzdalev-raevski-yuzyuk-semenchev-elmarssi-ferroelectricqandantiferroelectricpphasescoexistenceandlocalphasetransitionsinoxygendeficientnanbtextrm3singlecrystalmicroramandielectricanddilatometricstudies-2012', 'http://doi.org/10.1002/jrs.3140', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shakhovoy-raevskaya-shakhovaya-suzdalev-raevski-yuzyuk-semenchev-elmarssi-ferroelectricqandantiferroelectricpphasescoexistenceandlocalphasetransitionsinoxygendeficientnanbtextrm3singlecrystalmicroramandielectricanddilatometricstudies-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shakhovoy-raevskaya-shakhovaya-suzdalev-raevski-yuzyuk-semenchev-elmarssi-ferroelectricqandantiferroelectricpphasescoexistenceandlocalphasetransitionsinoxygendeficientnanbtextrm3singlecrystalmicroramandielectricanddilatometricstudies-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shakhovoy_ferroelectric_2012,\n\ttitle = {Ferroelectric {Q} and antiferroelectric {P} phases&#x27; coexistence and local phase transitions in oxygen-deficient {NaNb}$_{\\textrm{3}}$ single crystal: micro-{Raman}, dielectric and dilatometric studies},\n\tvolume = {43},\n\tcopyright = {Copyright © 2012 John Wiley \\&amp; Sons, Ltd.},\n\tissn = {1097-4555},\n\tshorttitle = {Ferroelectric {Q} and antiferroelectric {P} phases&#x27; coexistence and local phase transitions in oxygen-deficient {NaNbO3} single crystal},\n\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/jrs.3140},\n\tdoi = {10.1002/jrs.3140},\n\tabstract = {Micro-Raman studies of oxygen-deficient gray-colored NaNbO3 single crystals have shown that at room temperature both antiferroelectric P and ferroelectric Q phases are present simultaneously as separate regions tens of micrometers in size. Phase transitions in P and Q regions have been elucidated by dielectric, dilatometric and micro-Raman studies. For the first time, the sequence of phase transitions between antiferroelectric phase P and ferroelectric Q and N phases has been revealed. Copyright © 2012 John Wiley \\&amp; Sons, Ltd.},\n\tlanguage = {en},\n\tnumber = {8},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Raman Spectroscopy},\n\tauthor = {Shakhovoy, R. A. and Raevskaya, S. I. and Shakhovaya, L. A. and Suzdalev, D. V. and Raevski, I. P. and Yuzyuk, Yu. I. and Semenchev, A. F. and El Marssi, M.},\n\tyear = {2012},\n\tnote = {\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/jrs.3140},\n\tkeywords = {phase transition, ferroelectric, antiferroelectric, micro-Raman spectroscopy, sodium niobate},\n\tpages = {1141--1145},\n\tfile = {Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\HWT6QGGA\\\\jrs.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Micro-Raman studies of oxygen-deficient gray-colored NaNbO3 single crystals have shown that at room temperature both antiferroelectric P and ferroelectric Q phases are present simultaneously as separate regions tens of micrometers in size. Phase transitions in P and Q regions have been elucidated by dielectric, dilatometric and micro-Raman studies. For the first time, the sequence of phase transitions between antiferroelectric phase P and ferroelectric Q and N phases has been revealed. Copyright © 2012 John Wiley & Sons, Ltd.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/10726\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----2012', 'http://journals.ioffe.ru/articles/10726', event);\">\n    Усиление комбинационного рассеяния локализованными плазмонами в наночастицах серебра на поверхности наностержней оксида цинка.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Кайдашев, В. Е.; Лянгузов, Н. В.; Юзюк, Ю. И.;  and Кайдашев, Е. М.\n</span>\n\n  \n\n</span>\n\n  <i>Журнал технической физики</i>, 82(10): 85–89. September 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/10726\"\n     onclick=\"log_download('-----2012', 'http://journals.ioffe.ru/articles/10726', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Усиление комбинационного рассеяния локализованными плазмонами в наночастицах серебра на поверхности наностержней оксида цинка [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2012-13,\n\ttitle = {Усиление комбинационного рассеяния локализованными плазмонами в наночастицах серебра на поверхности наностержней оксида цинка},\n\tvolume = {82},\n\turl = {http://journals.ioffe.ru/articles/10726},\n\tabstract = {Исследованы особенности процесса магнетронного напыления наночастиц Ag на массивы наностержней ZnO. Боковые грани наностержней покрываются наночастицами с гораздо меньшей плотностью, нежели плоские поверхности при аналогичных временах напыления. Повышенная плотность частиц Ag наблюдается на ребрах боковых граней наностержней. Максимум плазмонного поглощения в синтезированных массивах наностержней, покрытых изолированными наночастицами Ag, лежит в диапазоне 450-500 nm. Возникновение локальных плазмонных возбуждений приводит к усилению интенсивности многофононных процессов с участием полярных мод ZnO в спектрах комбинационного рассеяния. С увеличением эквивалентной толщины пленок Ag возрастает сечение резонансного комбинационного рассеяния для обертонов фонона A1(LO).},\n\tlanguage = {ru},\n\tnumber = {10},\n\turldate = {2023-11-11},\n\tjournal = {Журнал технической физики},\n\tauthor = {Кайдашев, В. Е. and Лянгузов, Н. В. and Юзюк, Ю. И. and Кайдашев, Е. М.},\n\tmonth = sep,\n\tyear = {2012},\n\tpages = {85--89},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследованы особенности процесса магнетронного напыления наночастиц Ag на массивы наностержней ZnO. Боковые грани наностержней покрываются наночастицами с гораздо меньшей плотностью, нежели плоские поверхности при аналогичных временах напыления. Повышенная плотность частиц Ag наблюдается на ребрах боковых граней наностержней. Максимум плазмонного поглощения в синтезированных массивах наностержней, покрытых изолированными наночастицами Ag, лежит в диапазоне 450-500 nm. Возникновение локальных плазмонных возбуждений приводит к усилению интенсивности многофононных процессов с участием полярных мод ZnO в спектрах комбинационного рассеяния. С увеличением эквивалентной толщины пленок Ag возрастает сечение резонансного комбинационного рассеяния для обертонов фонона A1(LO).\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---batextrm08srtextrm02tiotextrm3-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/10654\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---batextrm08srtextrm02tiotextrm3-2012', 'http://journals.ioffe.ru/articles/10654', event);\">\n    Оптические свойства эпитаксиальных тонких пленок Ba$_{\\textrm{0.8}}$Sr$_{\\textrm{0.2}}$TiO$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Широков, В. Б.; Головко, Ю. И.;  and Мухортов, В. М.\n</span>\n\n  \n\n</span>\n\n  <i>Журнал технической физики</i>, 82(7): 79–84. June 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/10654\"\n     onclick=\"log_download('---batextrm08srtextrm02tiotextrm3-2012', 'http://journals.ioffe.ru/articles/10654', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Оптические свойства эпитаксиальных тонких пленок Ba$_{\\textrm{0.8}}$Sr$_{\\textrm{0.2}}$TiO$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---batextrm08srtextrm02tiotextrm3-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---batextrm08srtextrm02tiotextrm3-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2012-14,\n\ttitle = {Оптические свойства эпитаксиальных тонких пленок {Ba}$_{\\textrm{0.8}}${Sr}$_{\\textrm{0.2}}${TiO}$_{\\textrm{3}}$},\n\tvolume = {82},\n\turl = {http://journals.ioffe.ru/articles/10654},\n\tabstract = {Исследованы свойства наноразмерных пленок (Ba0.8,Sr0.2)TiO3 на монокристаллических подложках окиси магния. Пленки изготовлены по методу высокочастотного распыления при осаждении по слоевому механизму роста. Измерения параметров решетки выполнены с помощью методов рентгеновской дифракции. Пропускание пленок различной толщины исследовано в диапазоне длин волн 190-1100 nm. При анализе экспериментальных оптических характеристик для определения коэффициента преломления и поглощения в дисперсионной формуле использованы дополнительные, релаксационные слагаемые, отражающие конечное время жизни осциллятора, что позволило более точно провести аппроксимацию экспериментальных данных.},\n\tlanguage = {ru},\n\tnumber = {7},\n\turldate = {2023-11-11},\n\tjournal = {Журнал технической физики},\n\tauthor = {Широков, В. Б. and Головко, Ю. И. and Мухортов, В. М.},\n\tmonth = jun,\n\tyear = {2012},\n\tpages = {79--84},\n\tfile = {Журнал технической физики:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\8NHTT9Q2\\\\10654.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследованы свойства наноразмерных пленок (Ba0.8,Sr0.2)TiO3 на монокристаллических подложках окиси магния. Пленки изготовлены по методу высокочастотного распыления при осаждении по слоевому механизму роста. Измерения параметров решетки выполнены с помощью методов рентгеновской дифракции. Пропускание пленок различной толщины исследовано в диапазоне длин волн 190-1100 nm. При анализе экспериментальных оптических характеристик для определения коэффициента преломления и поглощения в дисперсионной формуле использованы дополнительные, релаксационные слагаемые, отражающие конечное время жизни осциллятора, что позволило более точно провести аппроксимацию экспериментальных данных.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"--------zno-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/10579\"\n     onclick=\"return trackOutboundLink('publications', 'click', '--------zno-2012', 'http://journals.ioffe.ru/articles/10579', event);\">\n    Использование различных катализаторов роста для лазерного напыления микро- и наностержней ZnO.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Лянгузов, Н. В.; Кайдашев, В. Е.; Захарченко, И. Н.; Куприна, Ю.; Бунина, О. А.; Юзюк, Ю. И.; Киселев, А. П.;  and Кайдашев, Е. М.\n</span>\n\n  \n\n</span>\n\n  <i>Журнал технической физики</i>, 82(4): 108–116. March 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/10579\"\n     onclick=\"log_download('--------zno-2012', 'http://journals.ioffe.ru/articles/10579', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Использование различных катализаторов роста для лазерного напыления микро- и наностержней ZnO [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/--------zno-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('--------zno-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2012-15,\n\ttitle = {Использование различных катализаторов роста для лазерного напыления микро- и наностержней {ZnO}},\n\tvolume = {82},\n\turl = {http://journals.ioffe.ru/articles/10579},\n\tabstract = {С помощью метода импульсного лазерного напыления получены микро- и наностержни ZnO с использованием различных катализаторов роста при температурах, близких к оптимальным для каждого типа катализатора. Сравнительный анализ оптических и структурных свойств полученных образцов показал, что при снижении температуры роста при использовании подложек Al2O3 (11-20) уменьшаются внутренние напряжения в стержнях, что приводит к улучшению структуры и оптических свойств. При использовании подложек GaN/Si такой эффект не наблюдается из-за сильных напряжений, вносимых разностью параметров решеток. При повышении температуры синтеза увеличиваются внутренние напряжения и концентрация точечных дефектов решетки, происходит релаксация правил отбора, и наблюдаются множественные обертоны фонона A1(LO). Получено качественное соответствие результатов расчетов деформаций кристаллической решетки, произведенных по параметру a элементарной ячейки и по сдвигу частоты фонона A1(LO). Исследование фотолюминесценции образцов показало, что снижение температуры синтеза уменьшает дефектность стержней ZnO и позволяет улучшить их оптические свойства для УФ-приложений.},\n\tlanguage = {ru},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Журнал технической физики},\n\tauthor = {Лянгузов, Н. В. and Кайдашев, В. Е. and Захарченко, И. Н. and Куприна, Ю.А. and Бунина, О. А. and Юзюк, Ю. И. and Киселев, А. П. and Кайдашев, Е. М.},\n\tmonth = mar,\n\tyear = {2012},\n\tpages = {108--116},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  С помощью метода импульсного лазерного напыления получены микро- и наностержни ZnO с использованием различных катализаторов роста при температурах, близких к оптимальным для каждого типа катализатора. Сравнительный анализ оптических и структурных свойств полученных образцов показал, что при снижении температуры роста при использовании подложек Al2O3 (11-20) уменьшаются внутренние напряжения в стержнях, что приводит к улучшению структуры и оптических свойств. При использовании подложек GaN/Si такой эффект не наблюдается из-за сильных напряжений, вносимых разностью параметров решеток. При повышении температуры синтеза увеличиваются внутренние напряжения и концентрация точечных дефектов решетки, происходит релаксация правил отбора, и наблюдаются множественные обертоны фонона A1(LO). Получено качественное соответствие результатов расчетов деформаций кристаллической решетки, произведенных по параметру a элементарной ячейки и по сдвигу частоты фонона A1(LO). Исследование фотолюминесценции образцов показало, что снижение температуры синтеза уменьшает дефектность стержней ZnO и позволяет улучшить их оптические свойства для УФ-приложений.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"bouyanfif-elmarssi-leme-lemarrec-karkut-dkhil-yuzyuk-acomparativeramanstudyof065pbmgtextrm13nbtextrm23otextrm3035pbtiotextrm3singlecrystalandthinfilm-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1140/epjb/e2011-20484-3\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'bouyanfif-elmarssi-leme-lemarrec-karkut-dkhil-yuzyuk-acomparativeramanstudyof065pbmgtextrm13nbtextrm23otextrm3035pbtiotextrm3singlecrystalandthinfilm-2012', 'https://doi.org/10.1140/epjb/e2011-20484-3', event);\">\n    A comparative Raman study of 0.65(PbMg$_{\\textrm{1/3}}$Nb$_{\\textrm{2/3}}$O$_{\\textrm{3}}$) -0.35(PbTiO$_{\\textrm{3}}$) single crystal and thin film.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Bouyanfif, H.; El Marssi, M.; Lemée, N.; Le Marrec, F.; Karkut, M. G.; Dkhil, B.;  and Yuzyuk, Y. I.\n</span>\n\n  \n\n</span>\n\n  <i>The European Physical Journal B</i>, 85(1): 35. January 2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1140/epjb/e2011-20484-3\"\n     onclick=\"log_download('bouyanfif-elmarssi-leme-lemarrec-karkut-dkhil-yuzyuk-acomparativeramanstudyof065pbmgtextrm13nbtextrm23otextrm3035pbtiotextrm3singlecrystalandthinfilm-2012', 'https://doi.org/10.1140/epjb/e2011-20484-3', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"A comparative Raman study of 0.65(PbMg$_{\\textrm{1/3}}$Nb$_{\\textrm{2/3}}$O$_{\\textrm{3}}$) -0.35(PbTiO$_{\\textrm{3}}$) single crystal and thin film [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1140/epjb/e2011-20484-3\"\n     onclick=\"log_download('bouyanfif-elmarssi-leme-lemarrec-karkut-dkhil-yuzyuk-acomparativeramanstudyof065pbmgtextrm13nbtextrm23otextrm3035pbtiotextrm3singlecrystalandthinfilm-2012', 'http://doi.org/10.1140/epjb/e2011-20484-3', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/bouyanfif-elmarssi-leme-lemarrec-karkut-dkhil-yuzyuk-acomparativeramanstudyof065pbmgtextrm13nbtextrm23otextrm3035pbtiotextrm3singlecrystalandthinfilm-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('bouyanfif-elmarssi-leme-lemarrec-karkut-dkhil-yuzyuk-acomparativeramanstudyof065pbmgtextrm13nbtextrm23otextrm3035pbtiotextrm3singlecrystalandthinfilm-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{bouyanfif_comparative_2012,\n\ttitle = {A comparative {Raman} study of 0.65({PbMg}$_{\\textrm{1/3}}${Nb}$_{\\textrm{2/3}}${O}$_{\\textrm{3}}$) -0.35({PbTiO}$_{\\textrm{3}}$) single crystal and thin film},\n\tvolume = {85},\n\tissn = {1434-6036},\n\turl = {https://doi.org/10.1140/epjb/e2011-20484-3},\n\tdoi = {10.1140/epjb/e2011-20484-3},\n\tabstract = {We report a comparative Raman study of 0.65(PbMg1/3Nb2/3O3)-0.35(PbTiO3) (PMN-0.35PT) single crystal and thin film. Raman spectra investigation indicates a change in bulk from the high temperature cubic to the tetragonal phase and then to the low temperature Mc monoclinic phase. The transition temperatures are in good agreement with the ones previously observed by dielectric measurements on the same sample. In contrast, we observe no phase transition to the monoclinic phase in the PMN-0.35PT 4000 Å thick film and only a cubic to tetragonal diffuse transition has been determined at high temperature. The enhanced stability of the tetragonal phase and the absence of low temperature monoclinic phase have been attributed to the in plane strain.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {The European Physical Journal B},\n\tauthor = {Bouyanfif, H. and El Marssi, M. and Lemée, N. and Le Marrec, F. and Karkut, M. G. and Dkhil, B. and Yuzyuk, Yu. I.},\n\tmonth = jan,\n\tyear = {2012},\n\tkeywords = {Solid State and Materials},\n\tpages = {35},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\ZDGC57TN\\\\Bouyanfif и др. - 2012 - A comparative Raman study of 0.65(PbMg13Nb23O3) .pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We report a comparative Raman study of 0.65(PbMg1/3Nb2/3O3)-0.35(PbTiO3) (PMN-0.35PT) single crystal and thin film. Raman spectra investigation indicates a change in bulk from the high temperature cubic to the tetragonal phase and then to the low temperature Mc monoclinic phase. The transition temperatures are in good agreement with the ones previously observed by dielectric measurements on the same sample. In contrast, we observe no phase transition to the monoclinic phase in the PMN-0.35PT 4000 Å thick film and only a cubic to tetragonal diffuse transition has been determined at high temperature. The enhanced stability of the tetragonal phase and the absence of low temperature monoclinic phase have been attributed to the in plane strain.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---bi44cdbi43sn-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=17845707\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---bi44cdbi43sn-2012', 'https://elibrary.ru/item.asp?id=17845707', event);\">\n    Структурные изменения в жидкотвердых сплавах Bi + 44% Cd и Bi + 43% Sn под действием постоянного электрического тока.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Афашоков, В. З.; Ахкубеков, А. А.;  and Кабиров, Ю. В.\n</span>\n\n  \n\n</span>\n\n  <i>Известия Российской Академии Наук. Серия Физическая</i>, 76(7): 851.  2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=17845707\"\n     onclick=\"log_download('---bi44cdbi43sn-2012', 'https://elibrary.ru/item.asp?id=17845707', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Структурные изменения в жидкотвердых сплавах Bi + 44% Cd и Bi + 43% Sn под действием постоянного электрического тока [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---bi44cdbi43sn-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---bi44cdbi43sn-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2012-16,\n\ttitle = {Структурные изменения в жидкотвердых сплавах {Bi} + 44\\% {Cd} и {Bi} + 43\\% {Sn} под действием постоянного электрического тока},\n\tvolume = {76},\n\tissn = {0367-6765},\n\turl = {https://elibrary.ru/item.asp?id=17845707},\n\tabstract = {Исследовано влияние постоянного электрического тока на параметры ячеек компонентов в жидкотвердых сплавах Bi + 44\\% Cd и Bi + 43\\% Sn. Обнаружено изменение параметров ячеек, связанное со структурными эффектами.},\n\tlanguage = {ru},\n\tnumber = {7},\n\turldate = {2023-11-11},\n\tjournal = {Известия Российской Академии Наук. Серия Физическая},\n\tauthor = {Афашоков, В. З. and Ахкубеков, А. А. and Кабиров, Ю. В.},\n\tyear = {2012},\n\tpages = {851},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследовано влияние постоянного электрического тока на параметры ячеек компонентов в жидкотвердых сплавах Bi + 44% Cd и Bi + 43% Sn. Обнаружено изменение параметров ячеек, связанное со структурными эффектами.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://elibrary.ru/item.asp?id=18062877\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------2012', 'https://elibrary.ru/item.asp?id=18062877', event);\">\n    Динамика решетки эпитаксиальной пленки титаната бария-стронция во внешнем электрическом поле.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Анохин, А. С.; Головко, Ю. И.; Широков, В. Б.; Мухортов, В. М.;  and Юзюк, Ю. И.\n</span>\n\n  \n\n</span>\n\n  <i>Вестник Южного Научного Центра Ран</i>, 8(3): 22–31.  2012.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://elibrary.ru/item.asp?id=18062877\"\n     onclick=\"log_download('------2012', 'https://elibrary.ru/item.asp?id=18062877', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Динамика решетки эпитаксиальной пленки титаната бария-стронция во внешнем электрическом поле [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>1 download</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2012-17,\n\ttitle = {Динамика решетки эпитаксиальной пленки титаната бария-стронция во внешнем электрическом поле},\n\tvolume = {8},\n\tissn = {1813-4289},\n\turl = {https://elibrary.ru/item.asp?id=18062877},\n\tabstract = {Исследована динамика решетки тонкой гетероэпитаксиальной пленки (Ba0,8Sr0,2)TiO3 на кубиче- ской подложке MgO во внешнем электрическом поле. Приведено как феноменологическое описание поведения мягких мод на основе теории Ландау, так и подробный анализ данных комбинационного рассеяния света. Расщепление мягкой моды на компоненты и их частотная зависимость свидетель- ствуют о переходе в моноклинную фазу при приложении внешнего электрического поля в направле- нии, перпендикулярном спонтанной поляризации c-доменной пленки.},\n\tlanguage = {ru},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Вестник Южного Научного Центра Ран},\n\tauthor = {Анохин, А. С. and Головко, Ю. И. and Широков, В. Б. and Мухортов, В. М. and Юзюк, Ю. И.},\n\tyear = {2012},\n\tkeywords = {Мягкая Мода, Сегнетоэлектрические Тонкие Пленки, Сегнетоэлектричество, Спектры Комбинационного Рассеяния Света},\n\tpages = {22--31},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследована динамика решетки тонкой гетероэпитаксиальной пленки (Ba0,8Sr0,2)TiO3 на кубиче- ской подложке MgO во внешнем электрическом поле. Приведено как феноменологическое описание поведения мягких мод на основе теории Ландау, так и подробный анализ данных комбинационного рассеяния света. Расщепление мягкой моды на компоненты и их частотная зависимость свидетель- ствуют о переходе в моноклинную фазу при приложении внешнего электрического поля в направле- нии, перпендикулярном спонтанной поляризации c-доменной пленки.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"pronin-uhlarz-beyer-fischer-wosnitza-gorshunov-komandin-prokhorov-etal-btphasediagramofcocrtextrm2otextrm4inmagneticfieldsupto14t-2012\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.85.012101\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'pronin-uhlarz-beyer-fischer-wosnitza-gorshunov-komandin-prokhorov-etal-btphasediagramofcocrtextrm2otextrm4inmagneticfieldsupto14t-2012', 'https://link.aps.org/doi/10.1103/PhysRevB.85.012101', event);\">\n    B-T phase diagram of CoCr$_{\\textrm{2}}$O$_{\\textrm{4}}$ in magnetic fields up to 14 T.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Pronin, A. V.; Uhlarz, M.; Beyer, R.; Fischer, T.; Wosnitza, J.; Gorshunov, B. P.; Komandin, G. A.; Prokhorov, A. S.; Dressel, M.; Bush, A. A.;  and Torgashev, V. I.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 85(1): 012101. January 2012.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.85.012101\"\n     onclick=\"log_download('pronin-uhlarz-beyer-fischer-wosnitza-gorshunov-komandin-prokhorov-etal-btphasediagramofcocrtextrm2otextrm4inmagneticfieldsupto14t-2012', 'https://link.aps.org/doi/10.1103/PhysRevB.85.012101', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"B-T phase diagram of CoCr$_{\\textrm{2}}$O$_{\\textrm{4}}$ in magnetic fields up to 14 T [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.85.012101\"\n     onclick=\"log_download('pronin-uhlarz-beyer-fischer-wosnitza-gorshunov-komandin-prokhorov-etal-btphasediagramofcocrtextrm2otextrm4inmagneticfieldsupto14t-2012', 'http://doi.org/10.1103/PhysRevB.85.012101', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/pronin-uhlarz-beyer-fischer-wosnitza-gorshunov-komandin-prokhorov-etal-btphasediagramofcocrtextrm2otextrm4inmagneticfieldsupto14t-2012\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('pronin-uhlarz-beyer-fischer-wosnitza-gorshunov-komandin-prokhorov-etal-btphasediagramofcocrtextrm2otextrm4inmagneticfieldsupto14t-2012')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{pronin_b-t_2012,\n\ttitle = {B-{T} phase diagram of {CoCr}$_{\\textrm{2}}${O}$_{\\textrm{4}}$ in magnetic fields up to 14 {T}},\n\tvolume = {85},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.85.012101},\n\tdoi = {10.1103/PhysRevB.85.012101},\n\tabstract = {We have measured the magnetization and specific heat of multiferroic CoCr2O4 in magnetic fields up to 14 T. The high-field magnetization measurements indicate a new phase transition at T∗=5–6 K. The phase between T∗ and the lock-in transition at 15 K is characterized by magnetic irreversibility. At higher magnetic fields, the irreversibility increases. Specific-heat measurements confirm the transition at T∗, and also show irreversible behavior. We construct a field-temperature phase diagram of CoCr2O4.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Pronin, A. V. and Uhlarz, M. and Beyer, R. and Fischer, T. and Wosnitza, J. and Gorshunov, B. P. and Komandin, G. A. and Prokhorov, A. S. and Dressel, M. and Bush, A. A. and Torgashev, V. I.},\n\tmonth = jan,\n\tyear = {2012},\n\tnote = {Publisher: American Physical Society},\n\tpages = {012101},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\AZP2XD73\\\\Pronin и др. - 2012 - \\$B\\$-\\$T\\$ phase diagram of CoCr\\$ _ 2 \\$O\\$ _ 4 \\$ in .pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We have measured the magnetization and specific heat of multiferroic CoCr2O4 in magnetic fields up to 14 T. The high-field magnetization measurements indicate a new phase transition at T∗=5–6 K. The phase between T∗ and the lock-in transition at 15 K is characterized by magnetic irreversibility. At higher magnetic fields, the irreversibility increases. Specific-heat measurements confirm the transition at T∗, and also show irreversible behavior. We construct a field-temperature phase diagram of CoCr2O4.\n</div>\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2011\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2011')\"\n      onkeypress=\"toggleGroup('group_2011')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2011</span>\n      <span class=\"bibbase_group_count\">\n        \n        (15)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"-----2011\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://ivdon.ru/magazine/archive/n1y2012/684\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----2011', 'http://ivdon.ru/magazine/archive/n1y2012/684', event);\">\n    Селективный рост массивов наностержней гидротермальным методом на кремнии.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Ступко, М. Ю.; Лянгузов, Н. В.; Николаев, А. Л.;  and Кайдашев, Е. М.\n</span>\n\n  \n\n</span>\n\n  . December 2011.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://ivdon.ru/magazine/archive/n1y2012/684\"\n     onclick=\"log_download('-----2011', 'http://ivdon.ru/magazine/archive/n1y2012/684', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Селективный рост массивов наностержней гидротермальным методом на кремнии [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----2011\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----2011')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2011,\n\ttitle = {Селективный рост массивов наностержней гидротермальным методом на кремнии},\n\turl = {http://ivdon.ru/magazine/archive/n1y2012/684},\n\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tauthor = {Ступко, М. Ю. and Лянгузов, Н. В. and Николаев, А. Л. and Кайдашев, Е. М.},\n\tmonth = dec,\n\tyear = {2011},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Сетевой научный журнал «Инженерный вестник Дона»\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"--2011\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://ivdon.ru/magazine/archive/n1y2012/683/\"\n     onclick=\"return trackOutboundLink('publications', 'click', '--2011', 'http://ivdon.ru/magazine/archive/n1y2012/683/', event);\">\n    Исследование роста наностержней в методике карботермического синтеза на тонкопленочных подслоях.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Лянгузов, Н. В.\n</span>\n\n  \n\n</span>\n\n  . December 2011.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://ivdon.ru/magazine/archive/n1y2012/683/\"\n     onclick=\"log_download('--2011', 'http://ivdon.ru/magazine/archive/n1y2012/683/', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Исследование роста наностержней в методике карботермического синтеза на тонкопленочных подслоях [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/--2011\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('--2011')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2011-1,\n\ttitle = {Исследование роста наностержней в методике карботермического синтеза на тонкопленочных подслоях},\n\turl = {http://ivdon.ru/magazine/archive/n1y2012/683/},\n\tabstract = {Сетевой научный журнал «Инженерный вестник Дона»},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tauthor = {Лянгузов, Н. В.},\n\tmonth = dec,\n\tyear = {2011},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Сетевой научный журнал «Инженерный вестник Дона»\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"mirzakhanyan-manukyan-badalyan-khachatryan-maslova-yuzyuk-bugaev-sharoyan-ramanspectraofnickelcarbonnanocomposites-2011\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.spiedigitallibrary.org/conference-proceedings-of-spie/7998/79981B/Raman-spectra-of-nickel-carbon-nanocomposites/10.1117/12.890940.full\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'mirzakhanyan-manukyan-badalyan-khachatryan-maslova-yuzyuk-bugaev-sharoyan-ramanspectraofnickelcarbonnanocomposites-2011', 'https://www.spiedigitallibrary.org/conference-proceedings-of-spie/7998/79981B/Raman-spectra-of-nickel-carbon-nanocomposites/10.1117/12.890940.full', event);\">\n    Raman spectra of nickel-carbon nanocomposites.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Mirzakhanyan, A. A.; Manukyan, A. S.; Badalyan, G. R.; Khachatryan, T. K.; Maslova, O. A.; Yuzyuk, Y. I.; Bugaev, L. A.;  and Sharoyan, E. G.\n</span>\n\n  \n\n</span>\n\n  In <i>International Conference on Laser Physics 2010</i>, volume 7998, pages 346–349, March 2011. SPIE\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.spiedigitallibrary.org/conference-proceedings-of-spie/7998/79981B/Raman-spectra-of-nickel-carbon-nanocomposites/10.1117/12.890940.full\"\n     onclick=\"log_download('mirzakhanyan-manukyan-badalyan-khachatryan-maslova-yuzyuk-bugaev-sharoyan-ramanspectraofnickelcarbonnanocomposites-2011', 'https://www.spiedigitallibrary.org/conference-proceedings-of-spie/7998/79981B/Raman-spectra-of-nickel-carbon-nanocomposites/10.1117/12.890940.full', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Raman spectra of nickel-carbon nanocomposites [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1117/12.890940\"\n     onclick=\"log_download('mirzakhanyan-manukyan-badalyan-khachatryan-maslova-yuzyuk-bugaev-sharoyan-ramanspectraofnickelcarbonnanocomposites-2011', 'http://doi.org/10.1117/12.890940', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/mirzakhanyan-manukyan-badalyan-khachatryan-maslova-yuzyuk-bugaev-sharoyan-ramanspectraofnickelcarbonnanocomposites-2011\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('mirzakhanyan-manukyan-badalyan-khachatryan-maslova-yuzyuk-bugaev-sharoyan-ramanspectraofnickelcarbonnanocomposites-2011')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{mirzakhanyan_raman_2011,\n\ttitle = {Raman spectra of nickel-carbon nanocomposites},\n\tvolume = {7998},\n\turl = {https://www.spiedigitallibrary.org/conference-proceedings-of-spie/7998/79981B/Raman-spectra-of-nickel-carbon-nanocomposites/10.1117/12.890940.full},\n\tdoi = {10.1117/12.890940},\n\tabstract = {By using the solid-phase pyrolysis of phthalocyanines the nickel-carbon nanocomposites have been synthesized. The composition, structure, and morphology of samples were investigated by scanning electron microscopy and Raman spectroscopy. The first-order Raman shifts of prepared materials were measured with laser excitation at 514.5 nm in the frequency range from 900 to 2000 cm$^{\\textrm{-1}}$. It is shown that the degree of graphitization in nanocomposites essentially depends on the pyrolysis temperature. By analyzing the intensity ratio of Raman D- and G-bands the mean sizes of graphitic nanocrystallites in prepared samples were estimated.},\n\turldate = {2023-11-11},\n\tbooktitle = {International {Conference} on {Laser} {Physics} 2010},\n\tpublisher = {SPIE},\n\tauthor = {Mirzakhanyan, Armen A. and Manukyan, Aram S. and Badalyan, George R. and Khachatryan, Tatevik K. and Maslova, Olga A. and Yuzyuk, Yurii I. and Bugaev, Lusegen A. and Sharoyan, Eduard G.},\n\tmonth = mar,\n\tyear = {2011},\n\tpages = {346--349},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  By using the solid-phase pyrolysis of phthalocyanines the nickel-carbon nanocomposites have been synthesized. The composition, structure, and morphology of samples were investigated by scanning electron microscopy and Raman spectroscopy. The first-order Raman shifts of prepared materials were measured with laser excitation at 514.5 nm in the frequency range from 900 to 2000 cm$^{\\textrm{-1}}$. It is shown that the degree of graphitization in nanocomposites essentially depends on the pyrolysis temperature. By analyzing the intensity ratio of Raman D- and G-bands the mean sizes of graphitic nanocrystallites in prepared samples were estimated.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"levshov-than-arenal-popov-parret-paillet-jourdain-zahab-etal-experimentalevidenceofamechanicalcouplingbetweenlayersinanindividualdoublewalledcarbonnanotube-2011\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1021/nl2026234\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'levshov-than-arenal-popov-parret-paillet-jourdain-zahab-etal-experimentalevidenceofamechanicalcouplingbetweenlayersinanindividualdoublewalledcarbonnanotube-2011', 'https://doi.org/10.1021/nl2026234', event);\">\n    Experimental Evidence of a Mechanical Coupling between Layers in an Individual Double-Walled Carbon Nanotube.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Levshov, D.; Than, T. X.; Arenal, R.; Popov, V. N.; Parret, R.; Paillet, M.; Jourdain, V.; Zahab, A. A.; Michel, T.; Yuzyuk, Y. I.;  and Sauvajol, J.\n</span>\n\n  \n\n</span>\n\n  <i>Nano Letters</i>, 11(11): 4800–4804. November 2011.\n  <span class=\"note\">Publisher: American Chemical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1021/nl2026234\"\n     onclick=\"log_download('levshov-than-arenal-popov-parret-paillet-jourdain-zahab-etal-experimentalevidenceofamechanicalcouplingbetweenlayersinanindividualdoublewalledcarbonnanotube-2011', 'https://doi.org/10.1021/nl2026234', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Experimental Evidence of a Mechanical Coupling between Layers in an Individual Double-Walled Carbon Nanotube [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1021/nl2026234\"\n     onclick=\"log_download('levshov-than-arenal-popov-parret-paillet-jourdain-zahab-etal-experimentalevidenceofamechanicalcouplingbetweenlayersinanindividualdoublewalledcarbonnanotube-2011', 'http://doi.org/10.1021/nl2026234', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/levshov-than-arenal-popov-parret-paillet-jourdain-zahab-etal-experimentalevidenceofamechanicalcouplingbetweenlayersinanindividualdoublewalledcarbonnanotube-2011\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('levshov-than-arenal-popov-parret-paillet-jourdain-zahab-etal-experimentalevidenceofamechanicalcouplingbetweenlayersinanindividualdoublewalledcarbonnanotube-2011')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{levshov_experimental_2011,\n\ttitle = {Experimental {Evidence} of a {Mechanical} {Coupling} between {Layers} in an {Individual} {Double}-{Walled} {Carbon} {Nanotube}},\n\tvolume = {11},\n\tissn = {1530-6984},\n\turl = {https://doi.org/10.1021/nl2026234},\n\tdoi = {10.1021/nl2026234},\n\tabstract = {We perform transmission electron microscopy, electron diffraction, and Raman scattering experiments on an individual suspended double-walled carbon nanotube (DWCNT). The first two techniques allow the unambiguous determination of the DWCNT structure: (12,8)@(16,14). However, the low-frequency features in the Raman spectra cannot be connected to the derived layer diameters d by means of the 1/d power law, widely used for the diameter dependence of the radial-breathing mode of single-walled nanotubes. We discuss this disagreement in terms of mechanical coupling between the layers of the DWCNT, which results in collective vibrational modes. Theoretical predictions for the breathing-like modes of the DWCNT, originating from the radial-breathing modes of the layers, are in a very good agreement with the observed Raman spectra. Moreover, the mechanical coupling qualitatively explains the observation of Raman lines of breathing-like modes, whenever only one of the layers is in resonance with the laser energy.},\n\tnumber = {11},\n\turldate = {2023-11-11},\n\tjournal = {Nano Letters},\n\tauthor = {Levshov, D. and Than, T. X. and Arenal, R. and Popov, V. N. and Parret, R. and Paillet, M. and Jourdain, V. and Zahab, A. A. and Michel, T. and Yuzyuk, Yu. I. and Sauvajol, J.-L.},\n\tmonth = nov,\n\tyear = {2011},\n\tnote = {Publisher: American Chemical Society},\n\tpages = {4800--4804},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We perform transmission electron microscopy, electron diffraction, and Raman scattering experiments on an individual suspended double-walled carbon nanotube (DWCNT). The first two techniques allow the unambiguous determination of the DWCNT structure: (12,8)@(16,14). However, the low-frequency features in the Raman spectra cannot be connected to the derived layer diameters d by means of the 1/d power law, widely used for the diameter dependence of the radial-breathing mode of single-walled nanotubes. We discuss this disagreement in terms of mechanical coupling between the layers of the DWCNT, which results in collective vibrational modes. Theoretical predictions for the breathing-like modes of the DWCNT, originating from the radial-breathing modes of the layers, are in a very good agreement with the observed Raman spectra. Moreover, the mechanical coupling qualitatively explains the observation of Raman lines of breathing-like modes, whenever only one of the layers is in resonance with the laser energy.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"leontyev-belenov-guterman-haghiashtiani-shaganov-dkhil-catalyticactivityofcarbonsupportedptnanoelectrocatalystswhyreducingthesizeofptnanoparticlesisnotalwaysbeneficial-2011\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1021/jp1109477\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'leontyev-belenov-guterman-haghiashtiani-shaganov-dkhil-catalyticactivityofcarbonsupportedptnanoelectrocatalystswhyreducingthesizeofptnanoparticlesisnotalwaysbeneficial-2011', 'https://doi.org/10.1021/jp1109477', event);\">\n    Catalytic Activity of Carbon-Supported Pt Nanoelectrocatalysts. Why Reducing the Size of Pt Nanoparticles is Not Always Beneficial.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Leontyev, I. N.; Belenov, S. V.; Guterman, V. E.; Haghi-Ashtiani, P.; Shaganov, A. P.;  and Dkhil, B.\n</span>\n\n  \n\n</span>\n\n  <i>The Journal of Physical Chemistry C</i>, 115(13): 5429–5434. April 2011.\n  <span class=\"note\">Publisher: American Chemical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1021/jp1109477\"\n     onclick=\"log_download('leontyev-belenov-guterman-haghiashtiani-shaganov-dkhil-catalyticactivityofcarbonsupportedptnanoelectrocatalystswhyreducingthesizeofptnanoparticlesisnotalwaysbeneficial-2011', 'https://doi.org/10.1021/jp1109477', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Catalytic Activity of Carbon-Supported Pt Nanoelectrocatalysts. Why Reducing the Size of Pt Nanoparticles is Not Always Beneficial [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1021/jp1109477\"\n     onclick=\"log_download('leontyev-belenov-guterman-haghiashtiani-shaganov-dkhil-catalyticactivityofcarbonsupportedptnanoelectrocatalystswhyreducingthesizeofptnanoparticlesisnotalwaysbeneficial-2011', 'http://doi.org/10.1021/jp1109477', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/leontyev-belenov-guterman-haghiashtiani-shaganov-dkhil-catalyticactivityofcarbonsupportedptnanoelectrocatalystswhyreducingthesizeofptnanoparticlesisnotalwaysbeneficial-2011\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('leontyev-belenov-guterman-haghiashtiani-shaganov-dkhil-catalyticactivityofcarbonsupportedptnanoelectrocatalystswhyreducingthesizeofptnanoparticlesisnotalwaysbeneficial-2011')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{leontyev_catalytic_2011,\n\ttitle = {Catalytic {Activity} of {Carbon}-{Supported} {Pt} {Nanoelectrocatalysts}. {Why} {Reducing} the {Size} of {Pt} {Nanoparticles} is {Not} {Always} {Beneficial}},\n\tvolume = {115},\n\tissn = {1932-7447},\n\turl = {https://doi.org/10.1021/jp1109477},\n\tdoi = {10.1021/jp1109477},\n\tabstract = {Carbon-supported Pt catalysts prepared by the impregnation method in water−dimethyl sulfoxide (DMSO) solutions were investigated. Using X-ray diffraction (XRD) technique for estimation of the particle size and shapes, we show that morphology of the Pt/C catalysts depends strongly on the DMSO content in the solutions. The average particles size reduces and a shape of the Pt nanocrystals changes from a truncated octahedron to a cuboctahedron and eventually to a truncated cube with increasing DMSO concentration in the reaction mixture. Antibate effects of the size and shape cause nonmonotonic dependence of the catalytic activity for the oxygen reduction reaction (ORR) with electric current maximum at an average particle size of 2.7 nm.},\n\tnumber = {13},\n\turldate = {2023-11-11},\n\tjournal = {The Journal of Physical Chemistry C},\n\tauthor = {Leontyev, I. N. and Belenov, S. V. and Guterman, V. E. and Haghi-Ashtiani, P. and Shaganov, A. P. and Dkhil, B.},\n\tmonth = apr,\n\tyear = {2011},\n\tnote = {Publisher: American Chemical Society},\n\tpages = {5429--5434},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Carbon-supported Pt catalysts prepared by the impregnation method in water−dimethyl sulfoxide (DMSO) solutions were investigated. Using X-ray diffraction (XRD) technique for estimation of the particle size and shapes, we show that morphology of the Pt/C catalysts depends strongly on the DMSO content in the solutions. The average particles size reduces and a shape of the Pt nanocrystals changes from a truncated octahedron to a cuboctahedron and eventually to a truncated cube with increasing DMSO concentration in the reaction mixture. Antibate effects of the size and shape cause nonmonotonic dependence of the catalytic activity for the oxygen reduction reaction (ORR) with electric current maximum at an average particle size of 2.7 nm.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----batextrm08srtextrm02tiotextrm3mgo-2011\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.elibrary.ru/item.asp?id=16220258\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----batextrm08srtextrm02tiotextrm3mgo-2011', 'https://www.elibrary.ru/item.asp?id=16220258', event);\">\n    Наноразмерные сегнетоэлектрические пленки Ba$_{\\textrm{0.8}}$Sr$_{\\textrm{0.2}}$TiO$_{\\textrm{3}}$ на подложках MgO.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Жигалина, О. М.; Мухортов, В. М.; Головко, Ю. И.; Чувилин, A. Л.;  and Кускова, А. Н.\n</span>\n\n  \n\n</span>\n\n  <i>Наукоемкие Технологии</i>, 12(5): 23–25.  2011.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.elibrary.ru/item.asp?id=16220258\"\n     onclick=\"log_download('-----batextrm08srtextrm02tiotextrm3mgo-2011', 'https://www.elibrary.ru/item.asp?id=16220258', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Наноразмерные сегнетоэлектрические пленки Ba$_{\\textrm{0.8}}$Sr$_{\\textrm{0.2}}$TiO$_{\\textrm{3}}$ на подложках MgO [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----batextrm08srtextrm02tiotextrm3mgo-2011\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----batextrm08srtextrm02tiotextrm3mgo-2011')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2011-2,\n\ttitle = {Наноразмерные сегнетоэлектрические пленки {Ba}$_{\\textrm{0.8}}${Sr}$_{\\textrm{0.2}}${TiO}$_{\\textrm{3}}$ на подложках {MgO}},\n\tvolume = {12},\n\tissn = {1999-8465},\n\turl = {https://www.elibrary.ru/item.asp?id=16220258},\n\tabstract = {Методом просвечивающей электронной микроскопии высокого разрешения проведены исследования и анализ дефектной микроструктуры монокристаллических сегнетоэлектрических наноразмерных пленок Ba0.8Sr0.2TiO3, выращенных методом магнетронного распыления мишени на подложках MgO. Выявлено в пленке наличие дислокаций с векторами Бюргерса {\\textless}100{\\textgreater}и 1/2{\\textless}110{\\textgreater} и границы блоков.},\n\tlanguage = {ru},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Наукоемкие Технологии},\n\tauthor = {Жигалина, О. М. and Мухортов, В. М. and Головко, Ю. И. and Чувилин, A. Л. and Кускова, А. Н.},\n\tyear = {2011},\n\tkeywords = {Тонкие Сегнетоэлектрические Пленки, Электронная Микроскопия Высокого Разрешения},\n\tpages = {23--25},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Методом просвечивающей электронной микроскопии высокого разрешения проведены исследования и анализ дефектной микроструктуры монокристаллических сегнетоэлектрических наноразмерных пленок Ba0.8Sr0.2TiO3, выращенных методом магнетронного распыления мишени на подложках MgO. Выявлено в пленке наличие дислокаций с векторами Бюргерса \\textless100\\textgreaterи 1/2\\textless110\\textgreater и границы блоков.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"ortega-kumar-maslova-yuzyuk-scott-katiyar-effectofperiodicityandcompositioninartificialbatiotextrm3basrtiotextrm3superlattices-2011\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.83.144108\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'ortega-kumar-maslova-yuzyuk-scott-katiyar-effectofperiodicityandcompositioninartificialbatiotextrm3basrtiotextrm3superlattices-2011', 'https://link.aps.org/doi/10.1103/PhysRevB.83.144108', event);\">\n    Effect of periodicity and composition in artificial BaTiO$_{\\textrm{3}}$/(Ba,Sr)TiO$_{\\textrm{3}}$ superlattices.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Ortega, N.; Kumar, A.; Maslova, O. A.; Yuzyuk, Y. I.; Scott, J. F.;  and Katiyar, R. S.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 83(14): 144108. April 2011.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.83.144108\"\n     onclick=\"log_download('ortega-kumar-maslova-yuzyuk-scott-katiyar-effectofperiodicityandcompositioninartificialbatiotextrm3basrtiotextrm3superlattices-2011', 'https://link.aps.org/doi/10.1103/PhysRevB.83.144108', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Effect of periodicity and composition in artificial BaTiO$_{\\textrm{3}}$/(Ba,Sr)TiO$_{\\textrm{3}}$ superlattices [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.83.144108\"\n     onclick=\"log_download('ortega-kumar-maslova-yuzyuk-scott-katiyar-effectofperiodicityandcompositioninartificialbatiotextrm3basrtiotextrm3superlattices-2011', 'http://doi.org/10.1103/PhysRevB.83.144108', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/ortega-kumar-maslova-yuzyuk-scott-katiyar-effectofperiodicityandcompositioninartificialbatiotextrm3basrtiotextrm3superlattices-2011\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('ortega-kumar-maslova-yuzyuk-scott-katiyar-effectofperiodicityandcompositioninartificialbatiotextrm3basrtiotextrm3superlattices-2011')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{ortega_effect_2011,\n\ttitle = {Effect of periodicity and composition in artificial {BaTiO}$_{\\textrm{3}}$/({Ba},{Sr}){TiO}$_{\\textrm{3}}$ superlattices},\n\tvolume = {83},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.83.144108},\n\tdoi = {10.1103/PhysRevB.83.144108},\n\tabstract = {We have prepared two series of BaTiO3/SrTiO3 (BT/ST) superlattices (SLs). In the first set, the modulation period (Λ) was varied from 136 to 16 Å, whereas in the second set ST was replaced with Ba(1−x)SrxTiO3 (BST) (0{\\textless}x{\\textless}1) with constant periodicity of ∼ 136 Å. A total stack height of 10 000 Å (1 μm) was maintained for both systems. The compositional changes give large spectral changes at x = 40\\% where the lowest E mode in BT/BST SL becomes underdamped. X-ray-diffraction patterns and surface topography of the modulated period revealed a Stranski-Krastanov growth mechanism. The upward frequency shift of the E(1TO) in SLs with decrease in Λ or Ba concentration in the BST layer was attributed to the in-plane compressive stress induced by the lattice mismatch of the constituent layers. [N.B., here the notation E(1TO) or A1(2TO) simply designates the vibrational mode of E or A1 symmetry, with 1TO or 2TO designating the transverse optical branch that is lowest, 1, or second lowest, 2, in energy.] In the low-frequency region, the folded acoustic phonon doublets were observed. Since the low-frequency out-of-plane dielectric constant is directly related to the E(1TO) soft mode frequency, strain engineering in artificial SLs allowed us to modify their dielectric properties by varying either the Ba/Sr in BST sublayer concentration or the modulation periodicity in the superlattices.},\n\tnumber = {14},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Ortega, N. and Kumar, A. and Maslova, O. A. and Yuzyuk, Yu. I. and Scott, J. F. and Katiyar, R. S.},\n\tmonth = apr,\n\tyear = {2011},\n\tnote = {Publisher: American Physical Society},\n\tpages = {144108},\n\tfile = {Принятая версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\56AU3DQI\\\\Ortega и др. - 2011 - Effect of periodicity and composition in artificia.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We have prepared two series of BaTiO3/SrTiO3 (BT/ST) superlattices (SLs). In the first set, the modulation period (Λ) was varied from 136 to 16 Å, whereas in the second set ST was replaced with Ba(1−x)SrxTiO3 (BST) (0\\textlessx\\textless1) with constant periodicity of ∼ 136 Å. A total stack height of 10 000 Å (1 μm) was maintained for both systems. The compositional changes give large spectral changes at x = 40% where the lowest E mode in BT/BST SL becomes underdamped. X-ray-diffraction patterns and surface topography of the modulated period revealed a Stranski-Krastanov growth mechanism. The upward frequency shift of the E(1TO) in SLs with decrease in Λ or Ba concentration in the BST layer was attributed to the in-plane compressive stress induced by the lattice mismatch of the constituent layers. [N.B., here the notation E(1TO) or A1(2TO) simply designates the vibrational mode of E or A1 symmetry, with 1TO or 2TO designating the transverse optical branch that is lowest, 1, or second lowest, 2, in energy.] In the low-frequency region, the folded acoustic phonon doublets were observed. Since the low-frequency out-of-plane dielectric constant is directly related to the E(1TO) soft mode frequency, strain engineering in artificial SLs allowed us to modify their dielectric properties by varying either the Ba/Sr in BST sublayer concentration or the modulation periodicity in the superlattices.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"anokhin-yuzyuk-golovko-mukhortov-elmarssi-electricfieldinducedmonoclinicphaseinbasrtiotextrm3thinfilm-2011\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.3573516\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'anokhin-yuzyuk-golovko-mukhortov-elmarssi-electricfieldinducedmonoclinicphaseinbasrtiotextrm3thinfilm-2011', 'https://doi.org/10.1063/1.3573516', event);\">\n    Electric-field-induced monoclinic phase in (Ba,Sr)TiO$_{\\textrm{3}}$ thin film.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Anokhin, A. S.; Yuzyuk, Y. I.; Golovko, Y. I.; Mukhortov, V. M.;  and El Marssi, M.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Applied Physics</i>, 109(7): 074111. April 2011.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.3573516\"\n     onclick=\"log_download('anokhin-yuzyuk-golovko-mukhortov-elmarssi-electricfieldinducedmonoclinicphaseinbasrtiotextrm3thinfilm-2011', 'https://doi.org/10.1063/1.3573516', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Electric-field-induced monoclinic phase in (Ba,Sr)TiO$_{\\textrm{3}}$ thin film [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.3573516\"\n     onclick=\"log_download('anokhin-yuzyuk-golovko-mukhortov-elmarssi-electricfieldinducedmonoclinicphaseinbasrtiotextrm3thinfilm-2011', 'http://doi.org/10.1063/1.3573516', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/anokhin-yuzyuk-golovko-mukhortov-elmarssi-electricfieldinducedmonoclinicphaseinbasrtiotextrm3thinfilm-2011\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('anokhin-yuzyuk-golovko-mukhortov-elmarssi-electricfieldinducedmonoclinicphaseinbasrtiotextrm3thinfilm-2011')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{anokhin_electric-field-induced_2011,\n\ttitle = {Electric-field-induced monoclinic phase in ({Ba},{Sr}){TiO}$_{\\textrm{3}}$ thin film},\n\tvolume = {109},\n\tissn = {0021-8979},\n\turl = {https://doi.org/10.1063/1.3573516},\n\tdoi = {10.1063/1.3573516},\n\tabstract = {We have studied electric-field-induced symmetry lowering in the tetragonal (001)-oriented heteroepitaxial (Ba0.8Sr0.2)TiO3 thin film deposited on (001)MgO substrate. Polarized micro-Raman spectra were recorded from the film area in between two planar electrodes deposited on the film surface. Presence of c domains with polarization normal to the substrate was confirmed from polarized Raman study under zero field, while splitting and hardening of the E(TO) soft mode and polarization changes in the Raman spectra suggest monoclinic symmetry under external electric field.},\n\tnumber = {7},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Applied Physics},\n\tauthor = {Anokhin, A. S. and Yuzyuk, Yu. I. and Golovko, Yu. I. and Mukhortov, V. M. and El Marssi, M.},\n\tmonth = apr,\n\tyear = {2011},\n\tpages = {074111},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\R9PF7M4M\\\\Anokhin и др. - 2011 - Electric-field-induced monoclinic phase in (Ba,Sr).pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We have studied electric-field-induced symmetry lowering in the tetragonal (001)-oriented heteroepitaxial (Ba0.8Sr0.2)TiO3 thin film deposited on (001)MgO substrate. Polarized micro-Raman spectra were recorded from the film area in between two planar electrodes deposited on the film surface. Presence of c domains with polarization normal to the substrate was confirmed from polarized Raman study under zero field, while splitting and hardening of the E(TO) soft mode and polarization changes in the Raman spectra suggest monoclinic symmetry under external electric field.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"leontyev-yuzyuk-janolin-elmarssi-chernyshov-dmitriev-golovko-mukhortov-etal-orthorhombicpolarnddopedbifeotextrm3thinfilmonmgosubstrate-2011\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/0953-8984/23/33/332201\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'leontyev-yuzyuk-janolin-elmarssi-chernyshov-dmitriev-golovko-mukhortov-etal-orthorhombicpolarnddopedbifeotextrm3thinfilmonmgosubstrate-2011', 'https://dx.doi.org/10.1088/0953-8984/23/33/332201', event);\">\n    Orthorhombic polar Nd-doped BiFeO$_{\\textrm{3}}$ thin film on MgO substrate.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Leontyev, I. N.; Yuzyuk, Y. I.; Janolin, P.; El-Marssi, M.; Chernyshov, D.; Dmitriev, V.; Golovko, Y. I.; Mukhortov, V. M.;  and Dkhil, B.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics: Condensed Matter</i>, 23(33): 332201. July 2011.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/0953-8984/23/33/332201\"\n     onclick=\"log_download('leontyev-yuzyuk-janolin-elmarssi-chernyshov-dmitriev-golovko-mukhortov-etal-orthorhombicpolarnddopedbifeotextrm3thinfilmonmgosubstrate-2011', 'https://dx.doi.org/10.1088/0953-8984/23/33/332201', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Orthorhombic polar Nd-doped BiFeO$_{\\textrm{3}}$ thin film on MgO substrate [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/0953-8984/23/33/332201\"\n     onclick=\"log_download('leontyev-yuzyuk-janolin-elmarssi-chernyshov-dmitriev-golovko-mukhortov-etal-orthorhombicpolarnddopedbifeotextrm3thinfilmonmgosubstrate-2011', 'http://doi.org/10.1088/0953-8984/23/33/332201', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/leontyev-yuzyuk-janolin-elmarssi-chernyshov-dmitriev-golovko-mukhortov-etal-orthorhombicpolarnddopedbifeotextrm3thinfilmonmgosubstrate-2011\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('leontyev-yuzyuk-janolin-elmarssi-chernyshov-dmitriev-golovko-mukhortov-etal-orthorhombicpolarnddopedbifeotextrm3thinfilmonmgosubstrate-2011')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{leontyev_orthorhombic_2011,\n\ttitle = {Orthorhombic polar {Nd}-doped {BiFeO}$_{\\textrm{3}}$ thin film on {MgO} substrate},\n\tvolume = {23},\n\tissn = {0953-8984},\n\turl = {https://dx.doi.org/10.1088/0953-8984/23/33/332201},\n\tdoi = {10.1088/0953-8984/23/33/332201},\n\tabstract = {A Nd-doped BiFeO3 thin film deposited on MgO substrate was studied by synchrotron diffraction. The ferroelectric nature of the film is proven by in-plane remanent polarization measurement. The highest possible symmetry of the film is determined to be orthorhombic, within the Fm2m space group. Such a structure is rotated by 45° with respect to the substrate and is consistent with tilts of oxygen octahedra doubling the unit cell. This polar structure presents a rather unusual strain-accommodation mechanism.},\n\tlanguage = {en},\n\tnumber = {33},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics: Condensed Matter},\n\tauthor = {Leontyev, I. N. and Yuzyuk, Yu I. and Janolin, P.-E. and El-Marssi, M. and Chernyshov, D. and Dmitriev, V. and Golovko, Yu I. and Mukhortov, V. M. and Dkhil, B.},\n\tmonth = jul,\n\tyear = {2011},\n\tpages = {332201},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A Nd-doped BiFeO3 thin film deposited on MgO substrate was studied by synchrotron diffraction. The ferroelectric nature of the film is proven by in-plane remanent polarization measurement. The highest possible symmetry of the film is determined to be orthorhombic, within the Fm2m space group. Such a structure is rotated by 45° with respect to the substrate and is consistent with tilts of oxygen octahedra doubling the unit cell. This polar structure presents a rather unusual strain-accommodation mechanism.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-------bifeotextrm3ymnotextrm3-2011\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/1518\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-------bifeotextrm3ymnotextrm3-2011', 'http://journals.ioffe.ru/articles/1518', event);\">\n    Особенности структурных состояний в твердых растворах BiFeO$_{\\textrm{3}}$-YMnO$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Назаренко, А. В.; Разумная, А. Г.; Куприянов, М. Ф.; Кабиров, Ю. В.; Рудская, А. Г.; Тесленко, П. Ю.;  and Кофанова, Н. Б.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 53(8): 1523–1525. July 2011.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/1518\"\n     onclick=\"log_download('-------bifeotextrm3ymnotextrm3-2011', 'http://journals.ioffe.ru/articles/1518', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Особенности структурных состояний в твердых растворах BiFeO$_{\\textrm{3}}$-YMnO$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-------bifeotextrm3ymnotextrm3-2011\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-------bifeotextrm3ymnotextrm3-2011')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2011-3,\n\ttitle = {Особенности структурных состояний в твердых растворах {BiFeO}$_{\\textrm{3}}$-{YMnO}$_{\\textrm{3}}$},\n\tvolume = {53},\n\turl = {http://journals.ioffe.ru/articles/1518},\n\tabstract = {Обнаружено, что в твердых растворах (1-x)BiFeO3-xYMnO3 наблюдается следующая последовательность изменений фаз с увеличением x: R3c-{\\textgreater} Pbnm-{\\textgreater} C2-{\\textgreater} Pnma-{\\textgreater} P63cm. Установлено, что фазы Pbnm и Pnma различаются ориентацией атомных смещений и могут иметь антисегнетоэлектрические свойства. Работа поддержана грантом РФФИ N 10-03-00189-a. А.Г. Разумная благодарит Фонд содействия развитию малых форм предприятий в научно-технической сфере по программе У.М.Н.И.К. N 10170.},\n\tlanguage = {ru},\n\tnumber = {8},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Назаренко, А. В. and Разумная, А. Г. and Куприянов, М. Ф. and Кабиров, Ю. В. and Рудская, А. Г. and Тесленко, П. Ю. and Кофанова, Н. Б.},\n\tmonth = jul,\n\tyear = {2011},\n\tpages = {1523--1525},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Обнаружено, что в твердых растворах (1-x)BiFeO3-xYMnO3 наблюдается следующая последовательность изменений фаз с увеличением x: R3c-\\textgreater Pbnm-\\textgreater C2-\\textgreater Pnma-\\textgreater P63cm. Установлено, что фазы Pbnm и Pnma различаются ориентацией атомных смещений и могут иметь антисегнетоэлектрические свойства. Работа поддержана грантом РФФИ N 10-03-00189-a. А.Г. Разумная благодарит Фонд содействия развитию малых форм предприятий в научно-технической сфере по программе У.М.Н.И.К. N 10170.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----wang--2011\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/1557\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----wang--2011', 'http://journals.ioffe.ru/articles/1557', event);\">\n    Спектры комбинационного рассеяния поликристаллических нанотрубок титаната висмута.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Анохин, А. С.; Лянгузов, Н. В.; Рошаль, С. Б.; Юзюк, Ю. И.;  and Wang, W.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 53(9): 1768–1772. September 2011.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/1557\"\n     onclick=\"log_download('----wang--2011', 'http://journals.ioffe.ru/articles/1557', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Спектры комбинационного рассеяния поликристаллических нанотрубок титаната висмута [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----wang--2011\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----wang--2011')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2011-4,\n\ttitle = {Спектры комбинационного рассеяния поликристаллических нанотрубок титаната висмута},\n\tvolume = {53},\n\turl = {http://journals.ioffe.ru/articles/1557},\n\tabstract = {Исследованы спектры комбинационного рассеяния света нанотрубок титаната висмута Bi4Ti3O12 синтезированных темплатным методом на мембранах Al2O3. Полученные образцы представляли собой массив ориентированных нанотрубок со сросшимися гладкими стенками длиной около 50 mum. Толщина стенок нанотрубок варьировалась от 20 до 50 nm, а внутренний диаметр составлял около 200 nm. В спектрах комбинационного рассеяния света нанотрубок наблюдалось уширение линий, соответствующих валентным и деформационным колебаниям TiO6 октаэдров, а в низкочастотной области спектра, соответствующей колебаниям ионов Bi относительно кислородных октаэдров, наблюдалась трансформация, обусловленная сильными механическими напряжениями, возникающими при формировании нанотрубок.},\n\tlanguage = {ru},\n\tnumber = {9},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Анохин, А. С. and Лянгузов, Н. В. and Рошаль, С. Б. and Юзюк, Ю. И. and Wang, Wen},\n\tmonth = sep,\n\tyear = {2011},\n\tpages = {1768--1772},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследованы спектры комбинационного рассеяния света нанотрубок титаната висмута Bi4Ti3O12 синтезированных темплатным методом на мембранах Al2O3. Полученные образцы представляли собой массив ориентированных нанотрубок со сросшимися гладкими стенками длиной около 50 mum. Толщина стенок нанотрубок варьировалась от 20 до 50 nm, а внутренний диаметр составлял около 200 nm. В спектрах комбинационного рассеяния света нанотрубок наблюдалось уширение линий, соответствующих валентным и деформационным колебаниям TiO6 октаэдров, а в низкочастотной области спектра, соответствующей колебаниям ионов Bi относительно кислородных октаэдров, наблюдалась трансформация, обусловленная сильными механическими напряжениями, возникающими при формировании нанотрубок.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"--------etal-pbtextrm2scnbotextrm6-2011\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/14334\"\n     onclick=\"return trackOutboundLink('publications', 'click', '--------etal-pbtextrm2scnbotextrm6-2011', 'http://journals.ioffe.ru/articles/14334', event);\">\n    Формирование физических свойств релаксорного сегнетоэлектрика Pb$_{\\textrm{2}}$ScNbO$_{\\textrm{6}}$ методом механоактивации.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Убушаева, Э. Н.; Лихушина, Е. В.; Абдулвахидов, К. Г.; Витченко, М. А.; Абулвахидов, Б. К.; Широков, В. Б.; Лянгузов, Н. В.; Юзюк, Ю. И.; Кайдашев, Е. М.;  and Мардасова, И. В.\n</span>\n\n  \n\n</span>\n\n  <i>Письма в ЖТФ</i>, 37(20): 23–30. September 2011.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/14334\"\n     onclick=\"log_download('--------etal-pbtextrm2scnbotextrm6-2011', 'http://journals.ioffe.ru/articles/14334', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Формирование физических свойств релаксорного сегнетоэлектрика Pb$_{\\textrm{2}}$ScNbO$_{\\textrm{6}}$ методом механоактивации [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/--------etal-pbtextrm2scnbotextrm6-2011\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('--------etal-pbtextrm2scnbotextrm6-2011')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2011-5,\n\ttitle = {Формирование физических свойств релаксорного сегнетоэлектрика {Pb}$_{\\textrm{2}}${ScNbO}$_{\\textrm{6}}$ методом механоактивации},\n\tvolume = {37},\n\turl = {http://journals.ioffe.ru/articles/14334},\n\tabstract = {Изучен релаксорный сегнетоэлектрик Pb2ScNbO6 (PSN), полученный твердофазным методом, спеканию которого предшествовала обработка при комнатной температуре синтезированного порошка PSN в наковальнях Бриджмена силовым воздействием в сочетании со сдвиговой деформацией. Показано, что при интенсивных силовых воздействиях в сочетании со сдвиговой деформацией в PSN развиваются динамические рекристаллизационные процессы, вносящие существенный вклад в формирование физических свойств керамики.},\n\tlanguage = {ru},\n\tnumber = {20},\n\turldate = {2023-11-11},\n\tjournal = {Письма в ЖТФ},\n\tauthor = {Убушаева, Э. Н. and Лихушина, Е. В. and Абдулвахидов, К. Г. and Витченко, М. А. and Абулвахидов, Б. К. and Широков, В. Б. and Лянгузов, Н. В. and Юзюк, Ю. И. and Кайдашев, Е. М. and Мардасова, И. В.},\n\tmonth = sep,\n\tyear = {2011},\n\tpages = {23--30},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Изучен релаксорный сегнетоэлектрик Pb2ScNbO6 (PSN), полученный твердофазным методом, спеканию которого предшествовала обработка при комнатной температуре синтезированного порошка PSN в наковальнях Бриджмена силовым воздействием в сочетании со сдвиговой деформацией. Показано, что при интенсивных силовых воздействиях в сочетании со сдвиговой деформацией в PSN развиваются динамические рекристаллизационные процессы, вносящие существенный вклад в формирование физических свойств керамики.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----zno-2011\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/12488\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----zno-2011', 'http://journals.ioffe.ru/articles/12488', event);\">\n    Исследование влияния толщины медного катализатора и пленочного подслоя на морфологию наностержней ZnO.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Лянгузов, Н. В.; Кайдашев, В. Е.; Кайдашев, Е. М.;  and Абдулвахидов, К. Г.\n</span>\n\n  \n\n</span>\n\n  <i>Письма в ЖТФ</i>, 37(5): 1–8. February 2011.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/12488\"\n     onclick=\"log_download('----zno-2011', 'http://journals.ioffe.ru/articles/12488', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Исследование влияния толщины медного катализатора и пленочного подслоя на морфологию наностержней ZnO [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----zno-2011\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----zno-2011')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2011-6,\n\ttitle = {Исследование влияния толщины медного катализатора и пленочного подслоя на морфологию наностержней {ZnO}},\n\tvolume = {37},\n\turl = {http://journals.ioffe.ru/articles/12488},\n\tabstract = {Исследовано влияние толщины пленочного подслоя ZnO, а также толщины пленок катализатора роста (Cu) на морфологию наностержней ZnO, выращенных на подложках a-Al2O3(11-20) карботермическим методом. Увеличение толщины пленки Cu приводит к увеличению диаметров, высоты и поверхностной плотности наностержней. Увеличение толщины пленочного подслоя ZnO приводит к возрастанию среднего диаметра и уменьшению длины и поверхностной плотности наностержней. Проведены исследования по влиянию температуры на процесс термического развала сверхтонких пленок меди, нанесенынх на подложки a-Al2O3. Исследованы фотолюминесцентные свойства массивов наностержней при высоких уровнях оптической накачки. Повышение плотности мощности накачки до 250-280 kW/cm2 приводит к сверхлюминесценции наностержней.},\n\tlanguage = {ru},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Письма в ЖТФ},\n\tauthor = {Лянгузов, Н. В. and Кайдашев, В. Е. and Кайдашев, Е. М. and Абдулвахидов, К. Г.},\n\tmonth = feb,\n\tyear = {2011},\n\tpages = {1--8},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследовано влияние толщины пленочного подслоя ZnO, а также толщины пленок катализатора роста (Cu) на морфологию наностержней ZnO, выращенных на подложках a-Al2O3(11-20) карботермическим методом. Увеличение толщины пленки Cu приводит к увеличению диаметров, высоты и поверхностной плотности наностержней. Увеличение толщины пленочного подслоя ZnO приводит к возрастанию среднего диаметра и уменьшению длины и поверхностной плотности наностержней. Проведены исследования по влиянию температуры на процесс термического развала сверхтонких пленок меди, нанесенынх на подложки a-Al2O3. Исследованы фотолюминесцентные свойства массивов наностержней при высоких уровнях оптической накачки. Повышение плотности мощности накачки до 250-280 kW/cm2 приводит к сверхлюминесценции наностержней.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-------2011\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/12492\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-------2011', 'http://journals.ioffe.ru/articles/12492', event);\">\n    Поверхностные акустические волны в тонких пленках титаната бария-стронция на подложках из оксида магния.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Мухортов, В. М.; Бирюков, С. В.; Головко, Ю. И.; Карапетьян, Г. Я.; Масычев, С. И.;  and Мухортов, В.\n</span>\n\n  \n\n</span>\n\n  <i>Письма в ЖТФ</i>, 37(5): 31–37. February 2011.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/12492\"\n     onclick=\"log_download('-------2011', 'http://journals.ioffe.ru/articles/12492', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Поверхностные акустические волны в тонких пленках титаната бария-стронция на подложках из оксида магния [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-------2011\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-------2011')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2011-7,\n\ttitle = {Поверхностные акустические волны в тонких пленках титаната бария-стронция на подложках из оксида магния},\n\tvolume = {37},\n\turl = {http://journals.ioffe.ru/articles/12492},\n\tabstract = {Установлено, что при использовании в устройстве на поверхностных акустических волнах в качестве активного элемента тонкой пленки титаната бария-стронция на подложке из оксида магния можно вдвое повысить рабочую частоту преобразователя за счет формирования в пленке периодической доменной структуры. Показано, что в тонкой сегнетоэлектрической пленке при стандартной структуре электродов эффективно возбуждается вторая гармоника поверхностной акустической волны. Путем изменения внешнего поляризующего напряжения на электродах пленки можно создавать преобразователи с электрически регулируемым коэффициентом электромеханической связи.},\n\tlanguage = {ru},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Письма в ЖТФ},\n\tauthor = {Мухортов, В. М. and Бирюков, С. В. and Головко, Ю. И. and Карапетьян, Г. Я. and Масычев, С. И. and Мухортов, В.М.},\n\tmonth = feb,\n\tyear = {2011},\n\tpages = {31--37},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Установлено, что при использовании в устройстве на поверхностных акустических волнах в качестве активного элемента тонкой пленки титаната бария-стронция на подложке из оксида магния можно вдвое повысить рабочую частоту преобразователя за счет формирования в пленке периодической доменной структуры. Показано, что в тонкой сегнетоэлектрической пленке при стандартной структуре электродов эффективно возбуждается вторая гармоника поверхностной акустической волны. Путем изменения внешнего поляризующего напряжения на электродах пленки можно создавать преобразователи с электрически регулируемым коэффициентом электромеханической связи.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----2011\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/10392\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----2011', 'http://journals.ioffe.ru/articles/10392', event);\">\n    Поляризация тонких пленок титаната бария-стронция при действии внешнего электрического поля.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Широков, В. Б.; Бирюков, С. В.; Мухортов, В. М.;  and Юзюк, Ю. И.\n</span>\n\n  \n\n</span>\n\n  <i>Журнал технической физики</i>, 81(8): 115–120. July 2011.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/10392\"\n     onclick=\"log_download('-----2011', 'http://journals.ioffe.ru/articles/10392', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Поляризация тонких пленок титаната бария-стронция при действии внешнего электрического поля [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----2011\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----2011')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2011-8,\n\ttitle = {Поляризация тонких пленок титаната бария-стронция при действии внешнего электрического поля},\n\tvolume = {81},\n\turl = {http://journals.ioffe.ru/articles/10392},\n\tabstract = {В рамках простой феноменологической модели описано поведение поляризации тонкой пленки Ba0.8Sr0.2TiO3 во внешнем электрическом поле при планарной геометрии электродов. Для согласования с экспериментальными данными введено &quot;поле Ван-дер-Ваальса&quot; Ez, формируемое подложкой в направлении нормали к плоскости пленки. Оценка величины поля дает значение Ez=1.1· 108 V/m. Проанализирована фазовая диаграмма пленки Ba0.8Sr0.2TiO3 в плоскости Ez - misfit strain при комнатной температуре},\n\tlanguage = {ru},\n\tnumber = {8},\n\turldate = {2023-11-11},\n\tjournal = {Журнал технической физики},\n\tauthor = {Широков, В. Б. and Бирюков, С. В. and Мухортов, В. М. and Юзюк, Ю. И.},\n\tmonth = jul,\n\tyear = {2011},\n\tpages = {115--120},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  В рамках простой феноменологической модели описано поведение поляризации тонкой пленки Ba0.8Sr0.2TiO3 во внешнем электрическом поле при планарной геометрии электродов. Для согласования с экспериментальными данными введено \"поле Ван-дер-Ваальса\" Ez, формируемое подложкой в направлении нормали к плоскости пленки. Оценка величины поля дает значение Ez=1.1· 108 V/m. Проанализирована фазовая диаграмма пленки Ba0.8Sr0.2TiO3 в плоскости Ez - misfit strain при комнатной температуре\n</div>\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2010\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2010')\"\n      onkeypress=\"toggleGroup('group_2010')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2010</span>\n      <span class=\"bibbase_group_count\">\n        \n        (17)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"ishioka-petek-kaydashev-kaidashev-misochko-coherentopticalphononsofznoundernearresonantphotoexcitation-2010\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/0953-8984/22/46/465803\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'ishioka-petek-kaydashev-kaidashev-misochko-coherentopticalphononsofznoundernearresonantphotoexcitation-2010', 'https://dx.doi.org/10.1088/0953-8984/22/46/465803', event);\">\n    Coherent optical phonons of ZnO under near resonant photoexcitation.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Ishioka, K.; Petek, H.; Kaydashev, V. E.; Kaidashev, E. M.;  and Misochko, O. V.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics: Condensed Matter</i>, 22(46): 465803. November 2010.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/0953-8984/22/46/465803\"\n     onclick=\"log_download('ishioka-petek-kaydashev-kaidashev-misochko-coherentopticalphononsofznoundernearresonantphotoexcitation-2010', 'https://dx.doi.org/10.1088/0953-8984/22/46/465803', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Coherent optical phonons of ZnO under near resonant photoexcitation [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/0953-8984/22/46/465803\"\n     onclick=\"log_download('ishioka-petek-kaydashev-kaidashev-misochko-coherentopticalphononsofznoundernearresonantphotoexcitation-2010', 'http://doi.org/10.1088/0953-8984/22/46/465803', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/ishioka-petek-kaydashev-kaidashev-misochko-coherentopticalphononsofznoundernearresonantphotoexcitation-2010\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('ishioka-petek-kaydashev-kaidashev-misochko-coherentopticalphononsofznoundernearresonantphotoexcitation-2010')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{ishioka_coherent_2010,\n\ttitle = {Coherent optical phonons of {ZnO} under near resonant photoexcitation},\n\tvolume = {22},\n\tissn = {0953-8984},\n\turl = {https://dx.doi.org/10.1088/0953-8984/22/46/465803},\n\tdoi = {10.1088/0953-8984/22/46/465803},\n\tabstract = {Ultrafast electron–phonon coupling dynamics in ZnO are investigated by degenerate pump–probe reflectivity measurements using near resonant 400 nm light. Because of the below-gap excitation, photocarriers are excited primarily from deep levels of intrinsic point defects. At least six coherent phonon modes, including two E2 modes and their combination, longitudinal optical (LO) mode and its overtone (2LO), are observed. Unlike the previous resonant Raman studies using 325 nm light, the intensity of the polar LO phonons is only moderately enhanced by the Fröhlich interaction. The non-polar E2 phonons decay considerably faster than under visible excitation, indicative of strong deformation potential interaction with photocarriers. The overdamped oscillation centered at around 20 THz is tentatively attributed to the upper branch of the plasmon–phonon coupled mode. The pump-polarization dependence of the phonon amplitudes is consistent with the impulsive Raman generation.},\n\tlanguage = {en},\n\tnumber = {46},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics: Condensed Matter},\n\tauthor = {Ishioka, K. and Petek, H. and Kaydashev, V. E. and Kaidashev, E. M. and Misochko, O. V.},\n\tmonth = nov,\n\tyear = {2010},\n\tpages = {465803},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Ultrafast electron–phonon coupling dynamics in ZnO are investigated by degenerate pump–probe reflectivity measurements using near resonant 400 nm light. Because of the below-gap excitation, photocarriers are excited primarily from deep levels of intrinsic point defects. At least six coherent phonon modes, including two E2 modes and their combination, longitudinal optical (LO) mode and its overtone (2LO), are observed. Unlike the previous resonant Raman studies using 325 nm light, the intensity of the polar LO phonons is only moderately enhanced by the Fröhlich interaction. The non-polar E2 phonons decay considerably faster than under visible excitation, indicative of strong deformation potential interaction with photocarriers. The overdamped oscillation centered at around 20 THz is tentatively attributed to the upper branch of the plasmon–phonon coupled mode. The pump-polarization dependence of the phonon amplitudes is consistent with the impulsive Raman generation.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"monnier-rochal-parmeggiani-lorman-longrangeproteincouplingmediatedbycriticallowenergymodesoftubularlipidmembranes-2010\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevLett.105.028102\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'monnier-rochal-parmeggiani-lorman-longrangeproteincouplingmediatedbycriticallowenergymodesoftubularlipidmembranes-2010', 'https://link.aps.org/doi/10.1103/PhysRevLett.105.028102', event);\">\n    Long-Range Protein Coupling Mediated by Critical Low-Energy Modes of Tubular Lipid Membranes.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Monnier, S.; Rochal, S. B.; Parmeggiani, A.;  and Lorman, V. L.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review Letters</i>, 105(2): 028102. July 2010.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevLett.105.028102\"\n     onclick=\"log_download('monnier-rochal-parmeggiani-lorman-longrangeproteincouplingmediatedbycriticallowenergymodesoftubularlipidmembranes-2010', 'https://link.aps.org/doi/10.1103/PhysRevLett.105.028102', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Long-Range Protein Coupling Mediated by Critical Low-Energy Modes of Tubular Lipid Membranes [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevLett.105.028102\"\n     onclick=\"log_download('monnier-rochal-parmeggiani-lorman-longrangeproteincouplingmediatedbycriticallowenergymodesoftubularlipidmembranes-2010', 'http://doi.org/10.1103/PhysRevLett.105.028102', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/monnier-rochal-parmeggiani-lorman-longrangeproteincouplingmediatedbycriticallowenergymodesoftubularlipidmembranes-2010\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('monnier-rochal-parmeggiani-lorman-longrangeproteincouplingmediatedbycriticallowenergymodesoftubularlipidmembranes-2010')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{monnier_long-range_2010,\n\ttitle = {Long-{Range} {Protein} {Coupling} {Mediated} by {Critical} {Low}-{Energy} {Modes} of {Tubular} {Lipid} {Membranes}},\n\tvolume = {105},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevLett.105.028102},\n\tdoi = {10.1103/PhysRevLett.105.028102},\n\tabstract = {We develop a theory of a resonant effect in protein-membrane coupling taking place in the vicinity of instabilities in tubular lipid membranes (TLMs) under longitudinal force and pressure difference constraints. Two critical low-energy modes defining the stability domain boundaries are found. We show that these modes mediate long-range TLM-protein coupling and interactions between absorbed proteins. Besides, TLM mechanical instabilities strongly influence protein desorption and protein cluster nucleation on TLMs. Model predictions can be tested over a large spectrum of mechanochemical conditions.},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review Letters},\n\tauthor = {Monnier, Sylvain and Rochal, Sergei B. and Parmeggiani, Andrea and Lorman, Vladimir L.},\n\tmonth = jul,\n\tyear = {2010},\n\tnote = {Publisher: American Physical Society},\n\tpages = {028102},\n\tfile = {APS Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\22HMBNIH\\\\PhysRevLett.105.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We develop a theory of a resonant effect in protein-membrane coupling taking place in the vicinity of instabilities in tubular lipid membranes (TLMs) under longitudinal force and pressure difference constraints. Two critical low-energy modes defining the stability domain boundaries are found. We show that these modes mediate long-range TLM-protein coupling and interactions between absorbed proteins. Besides, TLM mechanical instabilities strongly influence protein desorption and protein cluster nucleation on TLMs. Model predictions can be tested over a large spectrum of mechanochemical conditions.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------2010\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.elibrary.ru/item.asp?id=15271362\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------2010', 'https://www.elibrary.ru/item.asp?id=15271362', event);\">\n    Спектры комбинационного рассеяния углеродного наноматериала \"Таунит\".\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Маслова, О. А.; Михейкин, А. С.; Леонтьев, И. Н.; Юзюк, Ю. И.;  and Ткачев, А. Г.\n</span>\n\n  \n\n</span>\n\n  <i>Российские Нанотехнологии</i>, 5(9-10): 89–93.  2010.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.elibrary.ru/item.asp?id=15271362\"\n     onclick=\"log_download('------2010', 'https://www.elibrary.ru/item.asp?id=15271362', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Спектры комбинационного рассеяния углеродного наноматериала &quot;Таунит&quot; [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------2010\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------2010')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2010,\n\ttitle = {Спектры комбинационного рассеяния углеродного наноматериала &quot;Таунит&quot;},\n\tvolume = {5},\n\tissn = {1992-7223, 1993-4068},\n\turl = {https://www.elibrary.ru/item.asp?id=15271362},\n\tabstract = {Изучены спектры комбинационного рассеяния света (КРС) образцов углеродного наноматериала (УНМ) «Таунит», отожженных при различных температурах. Кроме того, исследовалось влияние наночастиц катализатора Pt с размерами 3-6 нм на спектры КРС УНМ «Таунит». Было обнаружено, что «Таунит» относится к углеродным материалам с нарушенной степенью организации, однако с ростом температуры отжига наблюдалось упорядочение его кристаллической структуры. Показано, что осаждение частиц платинового катализатора на поверхность УНМ «Таунит» приводит к увеличению интенсивности дефектной полосы в спектрах КРС из-за появления некоторого количества дефектов кристаллической решеткиRaman spectra of carbonaceous nanomaterial (CNM) «Taunit» samples annealed at different temperatures were studied. Also influence Pt-catalyst nanoparticles with the size distribution 3-6 nm on the Raman spectra of CNM «Taunit» was studied. It was found that «Taunit» belonged to poorly organized CNM but the its crystalline structure ordering was observed with increasing of annealing temperature. It is shown that Pt-catalyst precipitation on the surface of CNM «Taunit» leads to increasing of the defect band intensity due to appearance of some crystal lattice defects.},\n\tlanguage = {ru},\n\tnumber = {9-10},\n\turldate = {2023-11-11},\n\tjournal = {Российские Нанотехнологии},\n\tauthor = {Маслова, О. А. and Михейкин, А. С. and Леонтьев, И. Н. and Юзюк, Ю. И. and Ткачев, А. Г.},\n\tyear = {2010},\n\tpages = {89--93},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Изучены спектры комбинационного рассеяния света (КРС) образцов углеродного наноматериала (УНМ) «Таунит», отожженных при различных температурах. Кроме того, исследовалось влияние наночастиц катализатора Pt с размерами 3-6 нм на спектры КРС УНМ «Таунит». Было обнаружено, что «Таунит» относится к углеродным материалам с нарушенной степенью организации, однако с ростом температуры отжига наблюдалось упорядочение его кристаллической структуры. Показано, что осаждение частиц платинового катализатора на поверхность УНМ «Таунит» приводит к увеличению интенсивности дефектной полосы в спектрах КРС из-за появления некоторого количества дефектов кристаллической решеткиRaman spectra of carbonaceous nanomaterial (CNM) «Taunit» samples annealed at different temperatures were studied. Also influence Pt-catalyst nanoparticles with the size distribution 3-6 nm on the Raman spectra of CNM «Taunit» was studied. It was found that «Taunit» belonged to poorly organized CNM but the its crystalline structure ordering was observed with increasing of annealing temperature. It is shown that Pt-catalyst precipitation on the surface of CNM «Taunit» leads to increasing of the defect band intensity due to appearance of some crystal lattice defects.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"leontyev-guterman-pakhomova-timoshenko-avguterman-zakharchenko-petin-dkhil-xrdandelectrochemicalinvestigationofparticlesizeeffectsinplatinumcobaltcathodeelectrocatalystsforoxygenreduction-2010\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0925838810008091\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'leontyev-guterman-pakhomova-timoshenko-avguterman-zakharchenko-petin-dkhil-xrdandelectrochemicalinvestigationofparticlesizeeffectsinplatinumcobaltcathodeelectrocatalystsforoxygenreduction-2010', 'https://www.sciencedirect.com/science/article/pii/S0925838810008091', event);\">\n    XRD and electrochemical investigation of particle size effects in platinum-cobalt cathode electrocatalysts for oxygen reduction.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Leontyev, I. N.; Guterman, V. E.; Pakhomova, E. B.; Timoshenko, P. E.; A.V.Guterman; Zakharchenko, I. N.; Petin, G. P.;  and Dkhil, B.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Alloys and Compounds</i>, 500(2): 241–246. June 2010.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0925838810008091\"\n     onclick=\"log_download('leontyev-guterman-pakhomova-timoshenko-avguterman-zakharchenko-petin-dkhil-xrdandelectrochemicalinvestigationofparticlesizeeffectsinplatinumcobaltcathodeelectrocatalystsforoxygenreduction-2010', 'https://www.sciencedirect.com/science/article/pii/S0925838810008091', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"XRD and electrochemical investigation of particle size effects in platinum-cobalt cathode electrocatalysts for oxygen reduction [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.jallcom.2010.04.018\"\n     onclick=\"log_download('leontyev-guterman-pakhomova-timoshenko-avguterman-zakharchenko-petin-dkhil-xrdandelectrochemicalinvestigationofparticlesizeeffectsinplatinumcobaltcathodeelectrocatalystsforoxygenreduction-2010', 'http://doi.org/10.1016/j.jallcom.2010.04.018', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/leontyev-guterman-pakhomova-timoshenko-avguterman-zakharchenko-petin-dkhil-xrdandelectrochemicalinvestigationofparticlesizeeffectsinplatinumcobaltcathodeelectrocatalystsforoxygenreduction-2010\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('leontyev-guterman-pakhomova-timoshenko-avguterman-zakharchenko-petin-dkhil-xrdandelectrochemicalinvestigationofparticlesizeeffectsinplatinumcobaltcathodeelectrocatalystsforoxygenreduction-2010')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{leontyev_xrd_2010,\n\ttitle = {{XRD} and electrochemical investigation of particle size effects in platinum-cobalt cathode electrocatalysts for oxygen reduction},\n\tvolume = {500},\n\tissn = {0925-8388},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0925838810008091},\n\tdoi = {10.1016/j.jallcom.2010.04.018},\n\tabstract = {Pt-Co/C electrocatalysts with Pt loadings close to 30wt.\\% prepared by the impregnation method in water–ethylene glycol solutions were investigated by X-ray diffraction and correlated with electrochemical measurements. We show that composition of the binary solvent controls the average particle size and its distribution. The unit cell parameter of the Pt3Co alloy decreases nonlinearly with decreasing particle size. The ORR activity of the prepared Pt-Co/C catalysts in H2SO4 solution enhances with decreasing particle size and unit cell parameter as well as with narrowing of the particle size distribution. Corrosion treatment of the synthesized Pt-Co/C materials brings about an increase of ca. 1nm in the average grain size accompanied by broadening of the grain size distribution and a decrease in the Co content. All of the synthesized Pt-Co/C materials show higher ORR activities compared with commercial Pt/C electrocatalysts.},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Alloys and Compounds},\n\tauthor = {Leontyev, I. N. and Guterman, V. E. and Pakhomova, E. B. and Timoshenko, P. E. and {A.V.Guterman} and Zakharchenko, I. N. and Petin, G. P. and Dkhil, B.},\n\tmonth = jun,\n\tyear = {2010},\n\tkeywords = {Grain size distribution, Electrocatalysis, Oxygen reduction reaction (ORR), Platinum alloy, X-ray diffraction (XRD)},\n\tpages = {241--246},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\RVNSSP3Z\\\\Leontyev и др. - 2010 - XRD and electrochemical investigation of particle .pdf:application/pdf;ScienceDirect Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\VESEAEDH\\\\S0925838810008091.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Pt-Co/C electrocatalysts with Pt loadings close to 30wt.% prepared by the impregnation method in water–ethylene glycol solutions were investigated by X-ray diffraction and correlated with electrochemical measurements. We show that composition of the binary solvent controls the average particle size and its distribution. The unit cell parameter of the Pt3Co alloy decreases nonlinearly with decreasing particle size. The ORR activity of the prepared Pt-Co/C catalysts in H2SO4 solution enhances with decreasing particle size and unit cell parameter as well as with narrowing of the particle size distribution. Corrosion treatment of the synthesized Pt-Co/C materials brings about an increase of ca. 1nm in the average grain size accompanied by broadening of the grain size distribution and a decrease in the Co content. All of the synthesized Pt-Co/C materials show higher ORR activities compared with commercial Pt/C electrocatalysts.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"lorenz-rahm-cao-zigaprez-kaidashev-zhakarov-wagner-nobis-etal-selforganizedgrowthofznobasednanoandmicrostructures-2010\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.200945514\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'lorenz-rahm-cao-zigaprez-kaidashev-zhakarov-wagner-nobis-etal-selforganizedgrowthofznobasednanoandmicrostructures-2010', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.200945514', event);\">\n    Self-organized growth of ZnO-based nano- and microstructures.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Lorenz, M.; Rahm, A.; Cao, B.; Zúñiga-Pérez, J.; Kaidashev, E. M.; Zhakarov, N.; Wagner, G.; Nobis, T.; Czekalla, C.; Zimmermann, G.;  and Grundmann, M.\n</span>\n\n  \n\n</span>\n\n  <i>physica status solidi (b)</i>, 247(6): 1265–1281.  2010.\n  <span class=\"note\">_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.200945514</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.200945514\"\n     onclick=\"log_download('lorenz-rahm-cao-zigaprez-kaidashev-zhakarov-wagner-nobis-etal-selforganizedgrowthofznobasednanoandmicrostructures-2010', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.200945514', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Self-organized growth of ZnO-based nano- and microstructures [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1002/pssb.200945514\"\n     onclick=\"log_download('lorenz-rahm-cao-zigaprez-kaidashev-zhakarov-wagner-nobis-etal-selforganizedgrowthofznobasednanoandmicrostructures-2010', 'http://doi.org/10.1002/pssb.200945514', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/lorenz-rahm-cao-zigaprez-kaidashev-zhakarov-wagner-nobis-etal-selforganizedgrowthofznobasednanoandmicrostructures-2010\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('lorenz-rahm-cao-zigaprez-kaidashev-zhakarov-wagner-nobis-etal-selforganizedgrowthofznobasednanoandmicrostructures-2010')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{lorenz_self-organized_2010,\n\ttitle = {Self-organized growth of {ZnO}-based nano- and microstructures},\n\tvolume = {247},\n\tcopyright = {Copyright © 2010 WILEY-VCH Verlag GmbH \\&amp; Co. KGaA, Weinheim},\n\tissn = {1521-3951},\n\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.200945514},\n\tdoi = {10.1002/pssb.200945514},\n\tabstract = {ZnO-based nano- and micro-structures with controlled orientation, size, and lateral density were grown by specially designed two-step pulsed laser deposition and direct carbothermal growth, respectively. Different substrate orientations and nucleation layers allow well-defined tuning of growth direction and lateral arrangement of the wires. As a result, axial MgZnOZnO nano quantum dots and homogeneous radial nano core-shell quantum well structures are demonstrated. Donor and acceptor doping of nano- and microwires influence considerably both electrical characteristics as well as morphology including branching. Field effect transistors with n- and p-type wire channel and nanowire p–n junctions seem to prove a reproducible p-type conductivity of phosphorous-doped ZnO wires. Single ZnO wire (309 nm thick, 3.99 µm high) grown on pyramidal base with controlled lateral density by tuning the ZnO template layer in a two-step PLD process.},\n\tlanguage = {en},\n\tnumber = {6},\n\turldate = {2023-11-11},\n\tjournal = {physica status solidi (b)},\n\tauthor = {Lorenz, Michael and Rahm, Andreas and Cao, Bingqiang and Zúñiga-Pérez, Jesús and Kaidashev, Evgeni M. and Zhakarov, Nikolai and Wagner, Gerald and Nobis, Thomas and Czekalla, Christian and Zimmermann, Gregor and Grundmann, Marius},\n\tyear = {2010},\n\tnote = {\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.200945514},\n\tkeywords = {72.80.Ey, 73.21.Fg, 78.67.Bf, 81.05.Dz, 81.16.Dn, 81.16.Mk},\n\tpages = {1265--1281},\n\tfile = {Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\6WSS5J7I\\\\pssb.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  ZnO-based nano- and micro-structures with controlled orientation, size, and lateral density were grown by specially designed two-step pulsed laser deposition and direct carbothermal growth, respectively. Different substrate orientations and nucleation layers allow well-defined tuning of growth direction and lateral arrangement of the wires. As a result, axial MgZnOZnO nano quantum dots and homogeneous radial nano core-shell quantum well structures are demonstrated. Donor and acceptor doping of nano- and microwires influence considerably both electrical characteristics as well as morphology including branching. Field effect transistors with n- and p-type wire channel and nanowire p–n junctions seem to prove a reproducible p-type conductivity of phosphorous-doped ZnO wires. Single ZnO wire (309 nm thick, 3.99 µm high) grown on pyramidal base with controlled lateral density by tuning the ZnO template layer in a two-step PLD process.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------2010\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/1291\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------2010', 'http://journals.ioffe.ru/articles/1291', event);\">\n    Структура и фазовые переходы твердых растворов цирконата-гафната свинца.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Кабиров, Ю. В.; Куприянов, М. Ф.; Петрович, Э. В.; Дуймакаев, Ш. И.;  and Пономоренко, В. О.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 53(1): 110–113. December 2010.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/1291\"\n     onclick=\"log_download('------2010', 'http://journals.ioffe.ru/articles/1291', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Структура и фазовые переходы твердых растворов цирконата-гафната свинца [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------2010\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------2010')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2010-1,\n\ttitle = {Структура и фазовые переходы твердых растворов цирконата-гафната свинца},\n\tvolume = {53},\n\turl = {http://journals.ioffe.ru/articles/1291},\n\tabstract = {Методом твердофазного синтеза из простых оксидов приготовлены твердые растворы двух антисегнетоэлектриков - цирконата и гафната свинца PbZr1-xHfxO3, x=0, 0.3, 0.5, 0.7, 1. Элементный состав образцов и их структура изучены методами рентгенофлуоресцентного анализа и рентгеновской дифракции. Определены фазовые изменения твердых растворов в области температур 20{\\textless}t{\\textless}300oC. Работа поддержана грантом РФФИ N 10-03-00189-a.},\n\tlanguage = {ru},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Кабиров, Ю. В. and Куприянов, М. Ф. and Петрович, Э. В. and Дуймакаев, Ш. И. and Пономоренко, В. О.},\n\tmonth = dec,\n\tyear = {2010},\n\tpages = {110--113},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Методом твердофазного синтеза из простых оксидов приготовлены твердые растворы двух антисегнетоэлектриков - цирконата и гафната свинца PbZr1-xHfxO3, x=0, 0.3, 0.5, 0.7, 1. Элементный состав образцов и их структура изучены методами рентгенофлуоресцентного анализа и рентгеновской дифракции. Определены фазовые изменения твердых растворов в области температур 20\\textlesst\\textless300oC. Работа поддержана грантом РФФИ N 10-03-00189-a.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"--------2010\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/1900\"\n     onclick=\"return trackOutboundLink('publications', 'click', '--------2010', 'https://journals.ioffe.ru/articles/1900', event);\">\n    Структура и динамика решетки гетероструктур на основе феррита висмута и титаната бария-стронция на подложке оксида магния.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Головко, Ю. И.; Мухортов, В. М.; Бунина, О. А.; Захарченко, И. Н.; Анохин, А. С.; Широков, В. Б.;  and Юзюк, Ю. И.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 52(7): 1336–1341. June 2010.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/1900\"\n     onclick=\"log_download('--------2010', 'https://journals.ioffe.ru/articles/1900', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Структура и динамика решетки гетероструктур на основе феррита висмута и титаната бария-стронция на подложке оксида магния [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/--------2010\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('--------2010')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2010-2,\n\ttitle = {Структура и динамика решетки гетероструктур на основе феррита висмута и титаната бария-стронция на подложке оксида магния},\n\tvolume = {52},\n\turl = {https://journals.ioffe.ru/articles/1900},\n\tabstract = {Пленки феррита висмута, легированные неодимом, получены на монокристаллических подложках MgO с эпитаксиальным тонким (1-2 nm) подслоем титаната бария-стронция методом высокочастотного распыления керамических мишеней при повышенном парциальном давлении кислорода при температурах ниже температур сегнетоэлектрического и магнитного переходов. Методами дифракции рентгеновских лучей и спектроскопии комбинационного рассеяния света установлено, что в этих пленках феррита висмута реализуется новая фаза, которая не наблюдается в объемных образцах. Симметрия такой фазы моноклинная, элементарная ячейка содержит две формульные единицы, а вектор спонтанной поляризации отклоняется от направления [111]cub и может иметь различные компоненты вдоль осей x, y и z.},\n\tlanguage = {ru},\n\tnumber = {7},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Головко, Ю. И. and Мухортов, В. М. and Бунина, О. А. and Захарченко, И. Н. and Анохин, А. С. and Широков, В. Б. and Юзюк, Ю. И.},\n\tmonth = jun,\n\tyear = {2010},\n\tpages = {1336--1341},\n\tfile = {Физика твердого тела:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\3AQF2CGA\\\\1900.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Пленки феррита висмута, легированные неодимом, получены на монокристаллических подложках MgO с эпитаксиальным тонким (1-2 nm) подслоем титаната бария-стронция методом высокочастотного распыления керамических мишеней при повышенном парциальном давлении кислорода при температурах ниже температур сегнетоэлектрического и магнитного переходов. Методами дифракции рентгеновских лучей и спектроскопии комбинационного рассеяния света установлено, что в этих пленках феррита висмута реализуется новая фаза, которая не наблюдается в объемных образцах. Симметрия такой фазы моноклинная, элементарная ячейка содержит две формульные единицы, а вектор спонтанной поляризации отклоняется от направления [111]cub и может иметь различные компоненты вдоль осей x, y и z.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----2010\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/1789\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----2010', 'http://journals.ioffe.ru/articles/1789', event);\">\n    Тонкие сегнетоэлектрические пленки: получение и перспективы интеграции.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Сигов, А. С.; Мишина, Е. Д.;  and Мухортов, В. М.\n</span>\n\n  \n\n</span>\n\n  <i>Тонкие сегнетоэлектрические пленки: получение и перспективы интеграции</i>, 52(4): 709–717. March 2010.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/1789\"\n     onclick=\"log_download('----2010', 'http://journals.ioffe.ru/articles/1789', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Тонкие сегнетоэлектрические пленки: получение и перспективы интеграции [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----2010\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>1 download</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----2010')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2010-3,\n\ttitle = {Тонкие сегнетоэлектрические пленки: получение и перспективы интеграции},\n\tvolume = {52},\n\turl = {http://journals.ioffe.ru/articles/1789},\n\tabstract = {ассматриваются свойства тонких пленок (Ba,Sr)TiO3 и BiFeO3 и наноструктур на их основе. Пленки изготавливаются методом высокочастотного распыления в атмосфере кислорода с повышенным давлением, наноструктуры - методом фокусированного ионного травления; электрическое поле прикладывается в планарной структуре встречно-штыревых электродов. Исследуются структура, диэлектрические, электро-оптические и нелинейно-оптические свойства полученных образцов в широком диапазоне толщин и частот электрического поля. Показана высокая эффективность планарного переключения и его влияния на оптические свойства полученных структур. Наноструктурирование позволяет изменять диэлектрические и оптические свойства исследуемых материалов и таким образом увеличивать диапазон переключения функциональных параметров.},\n\tlanguage = {ru},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Тонкие сегнетоэлектрические пленки: получение и перспективы интеграции},\n\tauthor = {Сигов, А. С. and Мишина, Е. Д. and Мухортов, В. М.},\n\tmonth = mar,\n\tyear = {2010},\n\tpages = {709--717},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  ассматриваются свойства тонких пленок (Ba,Sr)TiO3 и BiFeO3 и наноструктур на их основе. Пленки изготавливаются методом высокочастотного распыления в атмосфере кислорода с повышенным давлением, наноструктуры - методом фокусированного ионного травления; электрическое поле прикладывается в планарной структуре встречно-штыревых электродов. Исследуются структура, диэлектрические, электро-оптические и нелинейно-оптические свойства полученных образцов в широком диапазоне толщин и частот электрического поля. Показана высокая эффективность планарного переключения и его влияния на оптические свойства полученных структур. Наноструктурирование позволяет изменять диэлектрические и оптические свойства исследуемых материалов и таким образом увеличивать диапазон переключения функциональных параметров.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------bitextrm098ndtextrm002feotextrm3-2010\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/1956\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------bitextrm098ndtextrm002feotextrm3-2010', 'http://journals.ioffe.ru/articles/1956', event);\">\n    Диэлектрические спектры тонких пленок мультиферроика Bi$_{\\textrm{0.98}}$Nd$_{\\textrm{0.02}}$FeO$_{\\textrm{3}}$ в терагерцевом диапазоне частот.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Командин, Г. А.; Торгашев, В. И.; Волков, А. А.; Породинков, О. Е.; Спектор, И. Е.;  and Мухортов, В. М.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 52(9): 1717–1723. September 2010.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/1956\"\n     onclick=\"log_download('------bitextrm098ndtextrm002feotextrm3-2010', 'http://journals.ioffe.ru/articles/1956', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Диэлектрические спектры тонких пленок мультиферроика Bi$_{\\textrm{0.98}}$Nd$_{\\textrm{0.02}}$FeO$_{\\textrm{3}}$ в терагерцевом диапазоне частот [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------bitextrm098ndtextrm002feotextrm3-2010\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------bitextrm098ndtextrm002feotextrm3-2010')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2010-4,\n\ttitle = {Диэлектрические спектры тонких пленок мультиферроика {Bi}$_{\\textrm{0.98}}${Nd}$_{\\textrm{0.02}}${FeO}$_{\\textrm{3}}$ в терагерцевом диапазоне частот},\n\tvolume = {52},\n\turl = {http://journals.ioffe.ru/articles/1956},\n\tabstract = {етодами субмиллиметровой спектроскопии на основе ламп обратной волны (ЛОВ) и инфракрасной Фурье-спектроскопии в диапазоне частот 8-1000 cm-1 при комнатной температуре измерены спектры пропускания и отражения тонких пленок мультиферроика Bi0.98Nd0.02FeO3 на подложках монокристаллического MgO. В рамках модели слоистой среды рассчитаны спектры комплексной диэлектрической проницаемости пленок. Обнаружены мощный рост потерь в области 30 cm-1 при уменьшении толщины пленок и обусловленное им пятикратное увеличение статической диэлектрической проницаемости (до 500 в пленке толщиной 32 nm). Явление обсуждается в рамках феноменологической теории фазовых переходов.},\n\tlanguage = {ru},\n\tnumber = {9},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Командин, Г. А. and Торгашев, В. И. and Волков, А. А. and Породинков, О. Е. and Спектор, И. Е. and Мухортов, В. М.},\n\tmonth = sep,\n\tyear = {2010},\n\tpages = {1717--1723},\n\tfile = {Физика твердого тела:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\NZQTPGVK\\\\1956.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  етодами субмиллиметровой спектроскопии на основе ламп обратной волны (ЛОВ) и инфракрасной Фурье-спектроскопии в диапазоне частот 8-1000 cm-1 при комнатной температуре измерены спектры пропускания и отражения тонких пленок мультиферроика Bi0.98Nd0.02FeO3 на подложках монокристаллического MgO. В рамках модели слоистой среды рассчитаны спектры комплексной диэлектрической проницаемости пленок. Обнаружены мощный рост потерь в области 30 cm-1 при уменьшении толщины пленок и обусловленное им пятикратное увеличение статической диэлектрической проницаемости (до 500 в пленке толщиной 32 nm). Явление обсуждается в рамках феноменологической теории фазовых переходов.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----2010\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.elibrary.ru/item.asp?id=15249715\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----2010', 'https://www.elibrary.ru/item.asp?id=15249715', event);\">\n    Спектры комбинационного рассеяния пленки титаната бария-стронция в электрических полях.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Анохин, А. С.; Юзюк, Ю. И.; Головко, Ю. И.;  and Мухортов, В. М.\n</span>\n\n  \n\n</span>\n\n  <i>Известия Российской Академии Наук. Серия Физическая</i>, 74(9): 1282–1284.  2010.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.elibrary.ru/item.asp?id=15249715\"\n     onclick=\"log_download('-----2010', 'https://www.elibrary.ru/item.asp?id=15249715', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Спектры комбинационного рассеяния пленки титаната бария-стронция в электрических полях [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----2010\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----2010')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2010-5,\n\ttitle = {Спектры комбинационного рассеяния пленки титаната бария-стронция в электрических полях},\n\tvolume = {74},\n\tissn = {0367-6765},\n\turl = {https://www.elibrary.ru/item.asp?id=15249715},\n\tabstract = {Исследованы поляризованные спектры комбинационного рассеяния гетероэпитаксиальной пленки титаната бария–стронция на подложке MgO во внешнем электрическом поле, приложенном перпендикулярно направлению спонтанной поляризации. Частичная деполяризация, наблюдающаяся в спектрах, свидетельствует об индуцированном полем понижении симметрии кристаллической решетки.},\n\tlanguage = {ru},\n\tnumber = {9},\n\turldate = {2023-11-11},\n\tjournal = {Известия Российской Академии Наук. Серия Физическая},\n\tauthor = {Анохин, А. С. and Юзюк, Ю. И. and Головко, Ю. И. and Мухортов, В. М.},\n\tyear = {2010},\n\tkeywords = {⛔ No DOI found},\n\tpages = {1282--1284},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследованы поляризованные спектры комбинационного рассеяния гетероэпитаксиальной пленки титаната бария–стронция на подложке MgO во внешнем электрическом поле, приложенном перпендикулярно направлению спонтанной поляризации. Частичная деполяризация, наблюдающаяся в спектрах, свидетельствует об индуцированном полем понижении симметрии кристаллической решетки.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----bifeotextrm3nd-2010\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.elibrary.ru/item.asp?id=15142299\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----bifeotextrm3nd-2010', 'https://www.elibrary.ru/item.asp?id=15142299', event);\">\n    Сегнетоэлектрические тонкие пленки BiFeO$_{\\textrm{3}}$ с орторомбической структурой допированного Nd.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Леонтьев, И. Н.; Анохин, А. С.; Юзюк, Ю. И.; Головко, Ю. И.;  and Мухортов, В. М.\n</span>\n\n  \n\n</span>\n\n  <i>Известия Российской Академии Наук. Серия Физическая</i>, 74(8): 1163–1165.  2010.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.elibrary.ru/item.asp?id=15142299\"\n     onclick=\"log_download('-----bifeotextrm3nd-2010', 'https://www.elibrary.ru/item.asp?id=15142299', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Сегнетоэлектрические тонкие пленки BiFeO$_{\\textrm{3}}$ с орторомбической структурой допированного Nd [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----bifeotextrm3nd-2010\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----bifeotextrm3nd-2010')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2010-6,\n\ttitle = {Сегнетоэлектрические тонкие пленки {BiFeO}$_{\\textrm{3}}$ с орторомбической структурой допированного {Nd}},\n\tvolume = {74},\n\tissn = {0367-6765},\n\turl = {https://www.elibrary.ru/item.asp?id=15142299},\n\tabstract = {Методами дифракции рентгеновских лучей и рамановской спектроскопии определена орторомбическая симметрия (Fmm2, a = 7.914 A, b = 7.913 A и c = 7.937 A) эпитаксиальных пленок феррита висмута, допированного Nd, на подложках MgO.},\n\tlanguage = {ru},\n\tnumber = {8},\n\turldate = {2023-11-11},\n\tjournal = {Известия Российской Академии Наук. Серия Физическая},\n\tauthor = {Леонтьев, И. Н. and Анохин, А. С. and Юзюк, Ю. И. and Головко, Ю. И. and Мухортов, В. М.},\n\tyear = {2010},\n\tkeywords = {⛔ No DOI found},\n\tpages = {1163--1165},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Методами дифракции рентгеновских лучей и рамановской спектроскопии определена орторомбическая симметрия (Fmm2, a = 7.914 A, b = 7.913 A и c = 7.937 A) эпитаксиальных пленок феррита висмута, допированного Nd, на подложках MgO.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-------2010\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/9945\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-------2010', 'http://journals.ioffe.ru/articles/9945', event);\">\n    Влияние внутренних деформационных полей на управляемость наноразмерных сегнетоэлектрических пленок в планарном конденсаторе.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Мухортов, В. М.; Головко, Ю. И.; Маматов, А. А.; Жигалина, О. М.; Кускова, А. Н.;  and Чувилин, A. Л.\n</span>\n\n  \n\n</span>\n\n  <i>Журнал технической физики</i>, 80(3): 77–82. February 2010.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/9945\"\n     onclick=\"log_download('-------2010', 'http://journals.ioffe.ru/articles/9945', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Влияние внутренних деформационных полей на управляемость наноразмерных сегнетоэлектрических пленок в планарном конденсаторе [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-------2010\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-------2010')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2010-7,\n\ttitle = {Влияние внутренних деформационных полей на управляемость наноразмерных сегнетоэлектрических пленок в планарном конденсаторе},\n\tvolume = {80},\n\turl = {http://journals.ioffe.ru/articles/9945},\n\tabstract = {Рентгенодифракционными методами и просвечивающей электронной спектроскопией высокого разрешения исследованы наноразмерные сегнетоэлектрические гетероэпитаксиальные пленки Ba0.8Sr0.2TiO3, выращенные по слоевому механизму роста на подложках (100) MgO. Установлено, что при изменении толщины пленок релаксация напряжений происходит посредством образования дислокаций нсоответствия на границе раздела между пленкой и подложкой. Существует критическая толщина ({\\textasciitilde}40 nm) пленок, ниже которой в пленках имеют место напряжения растяжения, а выше - напряжения сжатия. Приведены примеры влияния напряжений на диэлектрические характеристики пленок.},\n\tlanguage = {ru},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Журнал технической физики},\n\tauthor = {Мухортов, В. М. and Головко, Ю. И. and Маматов, А. А. and Жигалина, О. М. and Кускова, А. Н. and Чувилин, A. Л.},\n\tmonth = feb,\n\tyear = {2010},\n\tpages = {77--82},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Рентгенодифракционными методами и просвечивающей электронной спектроскопией высокого разрешения исследованы наноразмерные сегнетоэлектрические гетероэпитаксиальные пленки Ba0.8Sr0.2TiO3, выращенные по слоевому механизму роста на подложках (100) MgO. Установлено, что при изменении толщины пленок релаксация напряжений происходит посредством образования дислокаций нсоответствия на границе раздела между пленкой и подложкой. Существует критическая толщина (~40 nm) пленок, ниже которой в пленках имеют место напряжения растяжения, а выше - напряжения сжатия. Приведены примеры влияния напряжений на диэлектрические характеристики пленок.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"--------pbfetextrm05nbtextrm05otextrm3-2010\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/10151\"\n     onclick=\"return trackOutboundLink('publications', 'click', '--------pbfetextrm05nbtextrm05otextrm3-2010', 'http://journals.ioffe.ru/articles/10151', event);\">\n    Наноструктурированный мультиферроик PbFe$_{\\textrm{0.5}}$Nb$_{\\textrm{0.5}}$O$_{\\textrm{3}}$ и его физические свойства.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Убушаева, Э. Н.; Абдулвахидов, К. Г.; Мардасова, И. В.; Абулвахидов, Б. К.; Витченко, М. А.; Амиров, А. А.; Батдалов, А. Б.;  and Гамзатов, А. Г.\n</span>\n\n  \n\n</span>\n\n  <i>Журнал технической физики</i>, 80(11): 49–52. October 2010.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/10151\"\n     onclick=\"log_download('--------pbfetextrm05nbtextrm05otextrm3-2010', 'http://journals.ioffe.ru/articles/10151', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Наноструктурированный мультиферроик PbFe$_{\\textrm{0.5}}$Nb$_{\\textrm{0.5}}$O$_{\\textrm{3}}$ и его физические свойства [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/--------pbfetextrm05nbtextrm05otextrm3-2010\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('--------pbfetextrm05nbtextrm05otextrm3-2010')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2010-8,\n\ttitle = {Наноструктурированный мультиферроик {PbFe}$_{\\textrm{0.5}}${Nb}$_{\\textrm{0.5}}${O}$_{\\textrm{3}}$ и его физические свойства},\n\tvolume = {80},\n\turl = {http://journals.ioffe.ru/articles/10151},\n\tabstract = {Изучен поликристаллический мультиферроик PbFe0.5Nb0.5O3 (PEN), полученный твердофазным методом, спеканию которого предшествовала обработка при комнатной температуре синтезированного порошка PFN в наковальнях Бриджмена силовым воздействием в сочетании со сдвиговой деформацией (СВСД). Проведен сравнительный анализ электрофизических свойств и структурных параметров рабочих и эталонного образцов. Показано, что, начиная с величины СВСД, равной 200 MPa, доминирующую роль в формировании физических свойств играют точечные дефекты.},\n\tlanguage = {ru},\n\tnumber = {11},\n\turldate = {2023-11-11},\n\tjournal = {Журнал технической физики},\n\tauthor = {Убушаева, Э. Н. and Абдулвахидов, К. Г. and Мардасова, И. В. and Абулвахидов, Б. К. and Витченко, М. А. and Амиров, А. А. and Батдалов, А. Б. and Гамзатов, А. Г.},\n\tmonth = oct,\n\tyear = {2010},\n\tpages = {49--52},\n\tfile = {Журнал технической физики:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\26FX65HJ\\\\10151.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Изучен поликристаллический мультиферроик PbFe0.5Nb0.5O3 (PEN), полученный твердофазным методом, спеканию которого предшествовала обработка при комнатной температуре синтезированного порошка PFN в наковальнях Бриджмена силовым воздействием в сочетании со сдвиговой деформацией (СВСД). Проведен сравнительный анализ электрофизических свойств и структурных параметров рабочих и эталонного образцов. Показано, что, начиная с величины СВСД, равной 200 MPa, доминирующую роль в формировании физических свойств играют точечные дефекты.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"yuzyuk-shakhovoy-raevskaya-raevski-elmarssi-karkut-simon-ferroelectricqphaseinananbotextrm3epitaxialthinfilm-2010\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.3437090\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'yuzyuk-shakhovoy-raevskaya-raevski-elmarssi-karkut-simon-ferroelectricqphaseinananbotextrm3epitaxialthinfilm-2010', 'https://doi.org/10.1063/1.3437090', event);\">\n    Ferroelectric Q-phase in a NaNbO$_{\\textrm{3}}$ epitaxial thin film.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Yuzyuk, Y. I.; Shakhovoy, R. A.; Raevskaya, S. I.; Raevski, I. P.; El Marssi, M.; Karkut, M. G.;  and Simon, P.\n</span>\n\n  \n\n</span>\n\n  <i>Applied Physics Letters</i>, 96(22): 222904. June 2010.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.3437090\"\n     onclick=\"log_download('yuzyuk-shakhovoy-raevskaya-raevski-elmarssi-karkut-simon-ferroelectricqphaseinananbotextrm3epitaxialthinfilm-2010', 'https://doi.org/10.1063/1.3437090', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Ferroelectric Q-phase in a NaNbO$_{\\textrm{3}}$ epitaxial thin film [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.3437090\"\n     onclick=\"log_download('yuzyuk-shakhovoy-raevskaya-raevski-elmarssi-karkut-simon-ferroelectricqphaseinananbotextrm3epitaxialthinfilm-2010', 'http://doi.org/10.1063/1.3437090', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/yuzyuk-shakhovoy-raevskaya-raevski-elmarssi-karkut-simon-ferroelectricqphaseinananbotextrm3epitaxialthinfilm-2010\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('yuzyuk-shakhovoy-raevskaya-raevski-elmarssi-karkut-simon-ferroelectricqphaseinananbotextrm3epitaxialthinfilm-2010')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{yuzyuk_ferroelectric_2010,\n\ttitle = {Ferroelectric {Q}-phase in a {NaNbO}$_{\\textrm{3}}$ epitaxial thin film},\n\tvolume = {96},\n\tissn = {0003-6951},\n\turl = {https://doi.org/10.1063/1.3437090},\n\tdoi = {10.1063/1.3437090},\n\tabstract = {Epitaxial NaNbO3 thin films have been grown by pulsed laser deposition on cubic (00l) MgO substrate with epitaxial (La0.5Sr0.5)CoO3 buffer layer. Micro-Raman spectroscopy studies revealed that the ferroelectric Q phase (Pmc21, Z=4) is stable in a 250-nm-thick film in contrast to the antiferroelectric phase P (Pbma, Z=8) known to exist in the bulk single crystals and ceramics of undoped stoichiometric NaNbO3. Temperature-dependent Raman spectra indicate that the Q phase is stable over a wide temperature range (at least from 80 to 600 K), while the low-temperature ferroelectric rhombohedral phase N, typical for NaNbO3 single crystals, is not observed.},\n\tnumber = {22},\n\turldate = {2023-11-11},\n\tjournal = {Applied Physics Letters},\n\tauthor = {Yuzyuk, Yu. I. and Shakhovoy, R. A. and Raevskaya, S. I. and Raevski, I. P. and El Marssi, M. and Karkut, M. G. and Simon, P.},\n\tmonth = jun,\n\tyear = {2010},\n\tpages = {222904},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Epitaxial NaNbO3 thin films have been grown by pulsed laser deposition on cubic (00l) MgO substrate with epitaxial (La0.5Sr0.5)CoO3 buffer layer. Micro-Raman spectroscopy studies revealed that the ferroelectric Q phase (Pmc21, Z=4) is stable in a 250-nm-thick film in contrast to the antiferroelectric phase P (Pbma, Z=8) known to exist in the bulk single crystals and ceramics of undoped stoichiometric NaNbO3. Temperature-dependent Raman spectra indicate that the Q phase is stable over a wide temperature range (at least from 80 to 600 K), while the low-temperature ferroelectric rhombohedral phase N, typical for NaNbO3 single crystals, is not observed.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"elmarssi-gagou-belhadi-deguerville-yuzyuk-raevski-ferroelectricbatiotextrm3bazrotextrm3superlatticesxraydiffractionramanspectroscopyandpolarizationhysteresisloops-2010\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.3496620\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'elmarssi-gagou-belhadi-deguerville-yuzyuk-raevski-ferroelectricbatiotextrm3bazrotextrm3superlatticesxraydiffractionramanspectroscopyandpolarizationhysteresisloops-2010', 'https://doi.org/10.1063/1.3496620', event);\">\n    Ferroelectric BaTiO$_{\\textrm{3}}$/BaZrO$_{\\textrm{3}}$ superlattices: X-ray diffraction, Raman spectroscopy, and polarization hysteresis loops.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  El Marssi, M.; Gagou, Y.; Belhadi, J.; De Guerville, F.; Yuzyuk, Y. I.;  and Raevski, I. P.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Applied Physics</i>, 108(8): 084104. October 2010.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.3496620\"\n     onclick=\"log_download('elmarssi-gagou-belhadi-deguerville-yuzyuk-raevski-ferroelectricbatiotextrm3bazrotextrm3superlatticesxraydiffractionramanspectroscopyandpolarizationhysteresisloops-2010', 'https://doi.org/10.1063/1.3496620', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Ferroelectric BaTiO$_{\\textrm{3}}$/BaZrO$_{\\textrm{3}}$ superlattices: X-ray diffraction, Raman spectroscopy, and polarization hysteresis loops [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.3496620\"\n     onclick=\"log_download('elmarssi-gagou-belhadi-deguerville-yuzyuk-raevski-ferroelectricbatiotextrm3bazrotextrm3superlatticesxraydiffractionramanspectroscopyandpolarizationhysteresisloops-2010', 'http://doi.org/10.1063/1.3496620', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/elmarssi-gagou-belhadi-deguerville-yuzyuk-raevski-ferroelectricbatiotextrm3bazrotextrm3superlatticesxraydiffractionramanspectroscopyandpolarizationhysteresisloops-2010\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('elmarssi-gagou-belhadi-deguerville-yuzyuk-raevski-ferroelectricbatiotextrm3bazrotextrm3superlatticesxraydiffractionramanspectroscopyandpolarizationhysteresisloops-2010')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{el_marssi_ferroelectric_2010,\n\ttitle = {Ferroelectric {BaTiO}$_{\\textrm{3}}$/{BaZrO}$_{\\textrm{3}}$ superlattices: {X}-ray diffraction, {Raman} spectroscopy, and polarization hysteresis loops},\n\tvolume = {108},\n\tissn = {0021-8979},\n\tshorttitle = {Ferroelectric {BaTiO3}/{BaZrO3} superlattices},\n\turl = {https://doi.org/10.1063/1.3496620},\n\tdoi = {10.1063/1.3496620},\n\tabstract = {Artificial superlattices (SLs) consisting of ferroelectric BaTiO3 (BT) and paraelectric BaZrO3 (BZ) have been growth by a pulsed laser deposition technique. The epitaxial BT and BZ layers with a periodicity from 16 Å to 1056 Å were sequentially deposited on (001) MgO substrate buffered with an oxide conducting layer of La1/2Sr1/2CoO3. The out-of-plane lattice parameters of the SLs constituents were determined by modeling of the x-ray diffractograms. The results indicate that the polar c-axis of the BT layers lies in the plane of the substrate and BZ layers exhibit enhanced tetragonal distortion which is induced by the mismatch between the alternating BZ and BT layers. The Raman data reinforces this interpretation and suggest a monoclinic phase in BT layers and polar phase in BZ layers. The Raman spectra give evidence of coupling between the constituent layers and a narrowing of the Raman peaks is attributed to a reduction in the disorder of the Ti4+ ions due to the epitaxial strain. This strain is responsible for the upward frequency shift in the soft modes, especially, the E(1TO) mode, which is markedly altered with respect to its analogs in BT-bulk crystal and BT thin film. Ferroelectric hysteresis loops measurements, confirmed the x-ray diffraction and Raman results, and revealed a clear ferroelectric behavior for the constrained SLs (32 Å≤Λ≤256 Å) while a weak ferroelectricity is observed for the large periods (Λ=500 Å and 1056 Å). This is attributed to the strain-induced ferroelectricity in BZ layers for the constrained SLs.},\n\tnumber = {8},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Applied Physics},\n\tauthor = {El Marssi, M. and Gagou, Y. and Belhadi, J. and De Guerville, F. and Yuzyuk, Yu. I. and Raevski, I. P.},\n\tmonth = oct,\n\tyear = {2010},\n\tpages = {084104},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Artificial superlattices (SLs) consisting of ferroelectric BaTiO3 (BT) and paraelectric BaZrO3 (BZ) have been growth by a pulsed laser deposition technique. The epitaxial BT and BZ layers with a periodicity from 16 Å to 1056 Å were sequentially deposited on (001) MgO substrate buffered with an oxide conducting layer of La1/2Sr1/2CoO3. The out-of-plane lattice parameters of the SLs constituents were determined by modeling of the x-ray diffractograms. The results indicate that the polar c-axis of the BT layers lies in the plane of the substrate and BZ layers exhibit enhanced tetragonal distortion which is induced by the mismatch between the alternating BZ and BT layers. The Raman data reinforces this interpretation and suggest a monoclinic phase in BT layers and polar phase in BZ layers. The Raman spectra give evidence of coupling between the constituent layers and a narrowing of the Raman peaks is attributed to a reduction in the disorder of the Ti4+ ions due to the epitaxial strain. This strain is responsible for the upward frequency shift in the soft modes, especially, the E(1TO) mode, which is markedly altered with respect to its analogs in BT-bulk crystal and BT thin film. Ferroelectric hysteresis loops measurements, confirmed the x-ray diffraction and Raman results, and revealed a clear ferroelectric behavior for the constrained SLs (32 Å≤Λ≤256 Å) while a weak ferroelectricity is observed for the large periods (Λ=500 Å and 1056 Å). This is attributed to the strain-induced ferroelectricity in BZ layers for the constrained SLs.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"leontyev-fesenko-leontyev-dkhil-ferroelectricbatiotextrm3singlecrystalundersuperstrongelectricfieldsupto55mvmacomparativeexperimentalandtheoreticalstudy-2010\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.3386537\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'leontyev-fesenko-leontyev-dkhil-ferroelectricbatiotextrm3singlecrystalundersuperstrongelectricfieldsupto55mvmacomparativeexperimentalandtheoreticalstudy-2010', 'https://doi.org/10.1063/1.3386537', event);\">\n    Ferroelectric BaTiO$_{\\textrm{3}}$ single crystal under superstrong electric fields up to 55 MV/m: A comparative experimental and theoretical study.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Leontyev, I. N.; Fesenko, O. E.; Leontyev, N. G.;  and Dkhil, B.\n</span>\n\n  \n\n</span>\n\n  <i>Applied Physics Letters</i>, 96(14): 142904. April 2010.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.3386537\"\n     onclick=\"log_download('leontyev-fesenko-leontyev-dkhil-ferroelectricbatiotextrm3singlecrystalundersuperstrongelectricfieldsupto55mvmacomparativeexperimentalandtheoreticalstudy-2010', 'https://doi.org/10.1063/1.3386537', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Ferroelectric BaTiO$_{\\textrm{3}}$ single crystal under superstrong electric fields up to 55 MV/m: A comparative experimental and theoretical study [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.3386537\"\n     onclick=\"log_download('leontyev-fesenko-leontyev-dkhil-ferroelectricbatiotextrm3singlecrystalundersuperstrongelectricfieldsupto55mvmacomparativeexperimentalandtheoreticalstudy-2010', 'http://doi.org/10.1063/1.3386537', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/leontyev-fesenko-leontyev-dkhil-ferroelectricbatiotextrm3singlecrystalundersuperstrongelectricfieldsupto55mvmacomparativeexperimentalandtheoreticalstudy-2010\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('leontyev-fesenko-leontyev-dkhil-ferroelectricbatiotextrm3singlecrystalundersuperstrongelectricfieldsupto55mvmacomparativeexperimentalandtheoreticalstudy-2010')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{leontyev_ferroelectric_2010,\n\ttitle = {Ferroelectric {BaTiO}$_{\\textrm{3}}$ single crystal under superstrong electric fields up to 55 {MV}/m: {A} comparative experimental and theoretical study},\n\tvolume = {96},\n\tissn = {0003-6951},\n\tshorttitle = {Ferroelectric {BaTiO3} single crystal under superstrong electric fields up to 55 {MV}/m},\n\turl = {https://doi.org/10.1063/1.3386537},\n\tdoi = {10.1063/1.3386537},\n\tabstract = {We investigated the effect of huge electric field up to E=55 MV/m on tetragonal ferroelectric phase of BaTiO3 single crystal. Both lattice parameters and the dielectric susceptibility along the polar axis were determined. The induced polarization shows a continuous increase up to 20\\% of the spontaneous polarization. The longitudinal d33 and transverse d31 piezoelectric coefficients were also determined. The experimental data are described by a phenomenological approach. Interestingly, an intermediate critical electric field value of E∼25 MV/m was evidenced suggesting that the physics below and above this value are different.},\n\tnumber = {14},\n\turldate = {2023-11-11},\n\tjournal = {Applied Physics Letters},\n\tauthor = {Leontyev, I. N. and Fesenko, O. E. and Leontyev, N. G. and Dkhil, B.},\n\tmonth = apr,\n\tyear = {2010},\n\tpages = {142904},\n\tfile = {Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\ZP8445SF\\\\Ferroelectric-BaTiO3-single-crystal-under.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We investigated the effect of huge electric field up to E=55 MV/m on tetragonal ferroelectric phase of BaTiO3 single crystal. Both lattice parameters and the dielectric susceptibility along the polar axis were determined. The induced polarization shows a continuous increase up to 20% of the spontaneous polarization. The longitudinal d33 and transverse d31 piezoelectric coefficients were also determined. The experimental data are described by a phenomenological approach. Interestingly, an intermediate critical electric field value of E∼25 MV/m was evidenced suggesting that the physics below and above this value are different.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----pbsctextrm05tatextrm05otextrm3-2010\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://journals.ioffe.ru/articles/9965\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----pbsctextrm05tatextrm05otextrm3-2010', 'http://journals.ioffe.ru/articles/9965', event);\">\n    Фазовые переходы в PbSc$_{\\textrm{0.5}}$Ta$_{\\textrm{0.5}}$O$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Абдулвахидов, К. Г.; Мардасова, И. В.; Мясникова, Т. П.; Витченко, М. А.;  and Ошаева, Э. Н.\n</span>\n\n  \n\n</span>\n\n  <i>Журнал технической физики</i>, 80(4): 81–83. March 2010.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://journals.ioffe.ru/articles/9965\"\n     onclick=\"log_download('-----pbsctextrm05tatextrm05otextrm3-2010', 'http://journals.ioffe.ru/articles/9965', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Фазовые переходы в PbSc$_{\\textrm{0.5}}$Ta$_{\\textrm{0.5}}$O$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----pbsctextrm05tatextrm05otextrm3-2010\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----pbsctextrm05tatextrm05otextrm3-2010')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2010-9,\n\ttitle = {Фазовые переходы в {PbSc}$_{\\textrm{0.5}}${Ta}$_{\\textrm{0.5}}${O}$_{\\textrm{3}}$},\n\tvolume = {80},\n\turl = {http://journals.ioffe.ru/articles/9965},\n\tabstract = {Рентгенодифрактометрическим, электрофизическими и оптическими методами изучены разупорядоченные и частично упорядоченные сегнетоэлектрические монокристаллы PbSc0.5Ta0.5O3 в широком интервале значений температуры. В низкотемпературной области при T=-40oC обнаружен фазовый переход, который подтверждается как электрофизическими, так и рентгенодифрактометрическим методами.},\n\tlanguage = {ru},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Журнал технической физики},\n\tauthor = {Абдулвахидов, К. Г. and Мардасова, И. В. and Мясникова, Т. П. and Витченко, М. А. and Ошаева, Э. Н.},\n\tmonth = mar,\n\tyear = {2010},\n\tpages = {81--83},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Рентгенодифрактометрическим, электрофизическими и оптическими методами изучены разупорядоченные и частично упорядоченные сегнетоэлектрические монокристаллы PbSc0.5Ta0.5O3 в широком интервале значений температуры. В низкотемпературной области при T=-40oC обнаружен фазовый переход, который подтверждается как электрофизическими, так и рентгенодифрактометрическим методами.\n</div>\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2009\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2009')\"\n      onkeypress=\"toggleGroup('group_2009')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2009</span>\n      <span class=\"bibbase_group_count\">\n        \n        (12)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"timoshenko-babicheva-ivanov-zubkov-impedanceofthemicrostriplineformagnetostaticbackwardvolumewaves-2009\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1007/s11141-010-9197-9\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'timoshenko-babicheva-ivanov-zubkov-impedanceofthemicrostriplineformagnetostaticbackwardvolumewaves-2009', 'https://doi.org/10.1007/s11141-010-9197-9', event);\">\n    Impedance of the microstrip line for magnetostatic backward volume waves.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Timoshenko, P. E.; Babicheva, E. R.; Ivanov, V. N.;  and Zubkov, V. I.\n</span>\n\n  \n\n</span>\n\n  <i>Radiophysics and Quantum Electronics</i>, 52(12): 892–899. December 2009.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1007/s11141-010-9197-9\"\n     onclick=\"log_download('timoshenko-babicheva-ivanov-zubkov-impedanceofthemicrostriplineformagnetostaticbackwardvolumewaves-2009', 'https://doi.org/10.1007/s11141-010-9197-9', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Impedance of the microstrip line for magnetostatic backward volume waves [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1007/s11141-010-9197-9\"\n     onclick=\"log_download('timoshenko-babicheva-ivanov-zubkov-impedanceofthemicrostriplineformagnetostaticbackwardvolumewaves-2009', 'http://doi.org/10.1007/s11141-010-9197-9', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/timoshenko-babicheva-ivanov-zubkov-impedanceofthemicrostriplineformagnetostaticbackwardvolumewaves-2009\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('timoshenko-babicheva-ivanov-zubkov-impedanceofthemicrostriplineformagnetostaticbackwardvolumewaves-2009')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{timoshenko_impedance_2009,\n\ttitle = {Impedance of the microstrip line for magnetostatic backward volume waves},\n\tvolume = {52},\n\tissn = {1573-9120},\n\turl = {https://doi.org/10.1007/s11141-010-9197-9},\n\tdoi = {10.1007/s11141-010-9197-9},\n\tabstract = {We study excitation of magnetostatic backward volume waves on the microstrip line. The relation between the current density in the line and the normal component of the magnetic induction is found. The impedance of the line per unit length, i.e., its reactance and radiation resistance per unit length, is represented as a functional of the current density. The dependence of the operating-wave radiation resistance on the transverse size of the line and the width of the dielectric gap is studied. The radiation resistances of multistrip array and meander-type converters of magnetostatic backward volume waves are calculated},\n\tlanguage = {en},\n\tnumber = {12},\n\turldate = {2023-11-11},\n\tjournal = {Radiophysics and Quantum Electronics},\n\tauthor = {Timoshenko, P. E. and Babicheva, E. R. and Ivanov, V. N. and Zubkov, V. I.},\n\tmonth = dec,\n\tyear = {2009},\n\tkeywords = {Ferrite, Frequency Dependence, Radiation Resistance, Side Lobe, Unit Length},\n\tpages = {892--899},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We study excitation of magnetostatic backward volume waves on the microstrip line. The relation between the current density in the line and the normal component of the magnetic induction is found. The impedance of the line per unit length, i.e., its reactance and radiation resistance per unit length, is represented as a functional of the current density. The dependence of the operating-wave radiation resistance on the transverse size of the line and the width of the dielectric gap is studied. The radiation resistances of multistrip array and meander-type converters of magnetostatic backward volume waves are calculated\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"rochal-lorman-theoryofareconstructivestructuraltransformationincapsidsoficosahedralviruses-2009\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevE.80.051905\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'rochal-lorman-theoryofareconstructivestructuraltransformationincapsidsoficosahedralviruses-2009', 'https://link.aps.org/doi/10.1103/PhysRevE.80.051905', event);\">\n    Theory of a reconstructive structural transformation in capsids of icosahedral viruses.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Rochal, S. B.;  and Lorman, V. L.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review E</i>, 80(5): 051905. November 2009.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevE.80.051905\"\n     onclick=\"log_download('rochal-lorman-theoryofareconstructivestructuraltransformationincapsidsoficosahedralviruses-2009', 'https://link.aps.org/doi/10.1103/PhysRevE.80.051905', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Theory of a reconstructive structural transformation in capsids of icosahedral viruses [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevE.80.051905\"\n     onclick=\"log_download('rochal-lorman-theoryofareconstructivestructuraltransformationincapsidsoficosahedralviruses-2009', 'http://doi.org/10.1103/PhysRevE.80.051905', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/rochal-lorman-theoryofareconstructivestructuraltransformationincapsidsoficosahedralviruses-2009\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('rochal-lorman-theoryofareconstructivestructuraltransformationincapsidsoficosahedralviruses-2009')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{rochal_theory_2009,\n\ttitle = {Theory of a reconstructive structural transformation in capsids of icosahedral viruses},\n\tvolume = {80},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevE.80.051905},\n\tdoi = {10.1103/PhysRevE.80.051905},\n\tabstract = {A theory of a reconstructive structural transformation in icosahedral capsid shells is developed for a whole family of virulent human viruses. It is shown that the reversible rearrangement of proteins during the virus maturation transformation is driven by the variation in the wave number l associated with the protein density distribution function. The collective displacement field of protein centers from their positions in the initial (procapsid) and the final (capsid) two-dimensional icosahderal structures is derived. The amplitude of the displacement field is shown to be small and it minimizes the calculated free energy of the transformation. The theory allows us to propose a continuous thermodynamical mechanism of the reconstructive procapsid-to-capsid transformation. In the frame of the density-wave approach, we also propose to take an equivalent plane-wave vector as a common structural feature for different icosahedral capsid shells formed by the same proteins. Using these characteristics, we explain the relation between the radii of the procapsid and capsid shells and generalize it to the case of the viral capsid polymorphism.},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review E},\n\tauthor = {Rochal, S. B. and Lorman, V. L.},\n\tmonth = nov,\n\tyear = {2009},\n\tnote = {Publisher: American Physical Society},\n\tpages = {051905},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A theory of a reconstructive structural transformation in icosahedral capsid shells is developed for a whole family of virulent human viruses. It is shown that the reversible rearrangement of proteins during the virus maturation transformation is driven by the variation in the wave number l associated with the protein density distribution function. The collective displacement field of protein centers from their positions in the initial (procapsid) and the final (capsid) two-dimensional icosahderal structures is derived. The amplitude of the displacement field is shown to be small and it minimizes the calculated free energy of the transformation. The theory allows us to propose a continuous thermodynamical mechanism of the reconstructive procapsid-to-capsid transformation. In the frame of the density-wave approach, we also propose to take an equivalent plane-wave vector as a common structural feature for different icosahedral capsid shells formed by the same proteins. Using these characteristics, we explain the relation between the radii of the procapsid and capsid shells and generalize it to the case of the viral capsid polymorphism.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"leontyev-chernyshov-guterman-pakhomova-guterman-particlesizeeffectincarbonsupportedptcoalloyelectrocatalystspreparedbytheborohydridemethodxrdcharacterization-2009\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0926860X08007874\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'leontyev-chernyshov-guterman-pakhomova-guterman-particlesizeeffectincarbonsupportedptcoalloyelectrocatalystspreparedbytheborohydridemethodxrdcharacterization-2009', 'https://www.sciencedirect.com/science/article/pii/S0926860X08007874', event);\">\n    Particle size effect in carbon supported Pt–Co alloy electrocatalysts prepared by the borohydride method: XRD characterization.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Leontyev, I. N.; Chernyshov, D. Y.; Guterman, V. E.; Pakhomova, E. V.;  and Guterman, A. V.\n</span>\n\n  \n\n</span>\n\n  <i>Applied Catalysis A: General</i>, 357(1): 1–4. March 2009.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0926860X08007874\"\n     onclick=\"log_download('leontyev-chernyshov-guterman-pakhomova-guterman-particlesizeeffectincarbonsupportedptcoalloyelectrocatalystspreparedbytheborohydridemethodxrdcharacterization-2009', 'https://www.sciencedirect.com/science/article/pii/S0926860X08007874', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Particle size effect in carbon supported Pt–Co alloy electrocatalysts prepared by the borohydride method: XRD characterization [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.apcata.2008.12.023\"\n     onclick=\"log_download('leontyev-chernyshov-guterman-pakhomova-guterman-particlesizeeffectincarbonsupportedptcoalloyelectrocatalystspreparedbytheborohydridemethodxrdcharacterization-2009', 'http://doi.org/10.1016/j.apcata.2008.12.023', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/leontyev-chernyshov-guterman-pakhomova-guterman-particlesizeeffectincarbonsupportedptcoalloyelectrocatalystspreparedbytheborohydridemethodxrdcharacterization-2009\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('leontyev-chernyshov-guterman-pakhomova-guterman-particlesizeeffectincarbonsupportedptcoalloyelectrocatalystspreparedbytheborohydridemethodxrdcharacterization-2009')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{leontyev_particle_2009,\n\ttitle = {Particle size effect in carbon supported {Pt}–{Co} alloy electrocatalysts prepared by the borohydride method: {XRD} characterization},\n\tvolume = {357},\n\tissn = {0926-860X},\n\tshorttitle = {Particle size effect in carbon supported {Pt}–{Co} alloy electrocatalysts prepared by the borohydride method},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0926860X08007874},\n\tdoi = {10.1016/j.apcata.2008.12.023},\n\tabstract = {Pt3Co/C electrocatalysts prepared by wet synthesis method from water–ethylene glycol solutions of Pt and Co precursors were investigated by X-ray diffraction in conjunction with electrochemical measurements. It was shown that varying the binary solvent composition is an effective means of control over the average nanoparticle size and the grain size distribution. It was found that unit cell parameter of the Pt3Co/C electrocatalysts decreases nonlinearly with decreasing particle size. The activity of the prepared Pt3Co/C catalysts for the oxygen reduction reaction (ORR) in H2SO4 solution enhances with decrease in the particle size, the unit cell parameter, and the dispersion of the grain size distribution. All samples studied show higher catalytic activities in comparison with the commercial Pt/C materials.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Applied Catalysis A: General},\n\tauthor = {Leontyev, I. N. and Chernyshov, D. Yu. and Guterman, V. E. and Pakhomova, E. V. and Guterman, A. V.},\n\tmonth = mar,\n\tyear = {2009},\n\tkeywords = {X-ray diffraction, Grain size distribution, Oxygen reduction, Pt–Co alloy, Size effects},\n\tpages = {1--4},\n\tfile = {ScienceDirect Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\356CZ2CX\\\\S0926860X08007874.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Pt3Co/C electrocatalysts prepared by wet synthesis method from water–ethylene glycol solutions of Pt and Co precursors were investigated by X-ray diffraction in conjunction with electrochemical measurements. It was shown that varying the binary solvent composition is an effective means of control over the average nanoparticle size and the grain size distribution. It was found that unit cell parameter of the Pt3Co/C electrocatalysts decreases nonlinearly with decreasing particle size. The activity of the prepared Pt3Co/C catalysts for the oxygen reduction reaction (ORR) in H2SO4 solution enhances with decrease in the particle size, the unit cell parameter, and the dispersion of the grain size distribution. All samples studied show higher catalytic activities in comparison with the commercial Pt/C materials.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"martinandmari-maury-rousset-sahuquet-mennessier-rochal-lorman-mangeat-etal-topologicalcontroloflifeanddeathinnonproliferativeepithelia-2009\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.plos.org/plosone/article?id=10.1371/journal.pone.0004202\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'martinandmari-maury-rousset-sahuquet-mennessier-rochal-lorman-mangeat-etal-topologicalcontroloflifeanddeathinnonproliferativeepithelia-2009', 'https://journals.plos.org/plosone/article?id=10.1371/journal.pone.0004202', event);\">\n    Topological Control of Life and Death in Non-Proliferative Epithelia.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Martinand-Mari, C.; Maury, B.; Rousset, F.; Sahuquet, A.; Mennessier, G.; Rochal, S.; Lorman, V.; Mangeat, P.;  and Baghdiguian, S.\n</span>\n\n  \n\n</span>\n\n  <i>PLOS ONE</i>, 4(1): e4202.  2009.\n  <span class=\"note\">Publisher: Public Library of Science</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.plos.org/plosone/article?id=10.1371/journal.pone.0004202\"\n     onclick=\"log_download('martinandmari-maury-rousset-sahuquet-mennessier-rochal-lorman-mangeat-etal-topologicalcontroloflifeanddeathinnonproliferativeepithelia-2009', 'https://journals.plos.org/plosone/article?id=10.1371/journal.pone.0004202', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Topological Control of Life and Death in Non-Proliferative Epithelia [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1371/journal.pone.0004202\"\n     onclick=\"log_download('martinandmari-maury-rousset-sahuquet-mennessier-rochal-lorman-mangeat-etal-topologicalcontroloflifeanddeathinnonproliferativeepithelia-2009', 'http://doi.org/10.1371/journal.pone.0004202', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/martinandmari-maury-rousset-sahuquet-mennessier-rochal-lorman-mangeat-etal-topologicalcontroloflifeanddeathinnonproliferativeepithelia-2009\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('martinandmari-maury-rousset-sahuquet-mennessier-rochal-lorman-mangeat-etal-topologicalcontroloflifeanddeathinnonproliferativeepithelia-2009')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{martinand-mari_topological_2009,\n\ttitle = {Topological {Control} of {Life} and {Death} in {Non}-{Proliferative} {Epithelia}},\n\tvolume = {4},\n\tissn = {1932-6203},\n\turl = {https://journals.plos.org/plosone/article?id=10.1371/journal.pone.0004202},\n\tdoi = {10.1371/journal.pone.0004202},\n\tabstract = {Programmed cell death is one of the most fascinating demonstrations of the plasticity of biological systems. It is classically described to act upstream of and govern major developmental patterning processes (e.g. inter-digitations in vertebrates, ommatidia in Drosophila). We show here the first evidence that massive apoptosis can also be controlled and coordinated by a pre-established pattern of a specific ‘master cell’ population. This new concept is supported by the development and validation of an original model of cell patterning. Ciona intestinalis eggs are surrounded by a three-layered follicular organization composed of 60 elongated floating extensions made of as many outer and inner cells, and indirectly spread through an extracellular matrix over 1200 test cells. Experimental and selective ablation of outer and inner cells results in the abrogation of apoptosis in respective remaining neighbouring test cells. In addition incubation of outer/inner follicular cell-depleted eggs with a soluble extract of apoptotic outer/inner cells partially restores apoptosis to apoptotic-defective test cells. The 60 inner follicular cells were thus identified as ‘apoptotic master’ cells which collectively are induction sites for programmed cell death of the underlying test cells. The position of apoptotic master cells is controlled by topological constraints exhibiting a tetrahedral symmetry, and each cell spreads over and can control the destiny of 20 smaller test cells, which leads to optimized apoptosis signalling.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {PLOS ONE},\n\tauthor = {Martinand-Mari, Camille and Maury, Benoit and Rousset, François and Sahuquet, Alain and Mennessier, Gérard and Rochal, Sergei and Lorman, Vladimir and Mangeat, Paul and Baghdiguian, Stephen},\n\tyear = {2009},\n\tnote = {Publisher: Public Library of Science},\n\tkeywords = {Apoptosis, Apoptotic signaling cascade, Chorion, Ciona intestinalis, Eggs, Fertilization, Ova, Symmetry},\n\tpages = {e4202},\n\tfile = {Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\U26F6JVM\\\\Martinand-Mari и др. - 2009 - Topological Control of Life and Death in Non-Proli.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Programmed cell death is one of the most fascinating demonstrations of the plasticity of biological systems. It is classically described to act upstream of and govern major developmental patterning processes (e.g. inter-digitations in vertebrates, ommatidia in Drosophila). We show here the first evidence that massive apoptosis can also be controlled and coordinated by a pre-established pattern of a specific ‘master cell’ population. This new concept is supported by the development and validation of an original model of cell patterning. Ciona intestinalis eggs are surrounded by a three-layered follicular organization composed of 60 elongated floating extensions made of as many outer and inner cells, and indirectly spread through an extracellular matrix over 1200 test cells. Experimental and selective ablation of outer and inner cells results in the abrogation of apoptosis in respective remaining neighbouring test cells. In addition incubation of outer/inner follicular cell-depleted eggs with a soluble extract of apoptotic outer/inner cells partially restores apoptosis to apoptotic-defective test cells. The 60 inner follicular cells were thus identified as ‘apoptotic master’ cells which collectively are induction sites for programmed cell death of the underlying test cells. The position of apoptotic master cells is controlled by topological constraints exhibiting a tetrahedral symmetry, and each cell spreads over and can control the destiny of 20 smaller test cells, which leads to optimized apoptosis signalling.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"ankiewicz-gehlhoff-martins-pereira-pereira-hoffmann-kaidashev-rahm-etal-magneticandstructuralpropertiesoftransitionmetaldopedzincoxidenanostructures-2009\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.200880581\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'ankiewicz-gehlhoff-martins-pereira-pereira-hoffmann-kaidashev-rahm-etal-magneticandstructuralpropertiesoftransitionmetaldopedzincoxidenanostructures-2009', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.200880581', event);\">\n    Magnetic and structural properties of transition metal doped zinc-oxide nanostructures.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Ankiewicz, A. O.; Gehlhoff, W.; Martins, J. S.; Pereira, Â. S.; Pereira, S.; Hoffmann, A.; Kaidashev, E. M.; Rahm, A.; Lorenz, M.; Grundmann, M.; Carmo, M. C.; Trindade, T.;  and Sobolev, N. A.\n</span>\n\n  \n\n</span>\n\n  <i>physica status solidi (b)</i>, 246(4): 766–770.  2009.\n  <span class=\"note\">_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.200880581</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.200880581\"\n     onclick=\"log_download('ankiewicz-gehlhoff-martins-pereira-pereira-hoffmann-kaidashev-rahm-etal-magneticandstructuralpropertiesoftransitionmetaldopedzincoxidenanostructures-2009', 'https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.200880581', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Magnetic and structural properties of transition metal doped zinc-oxide nanostructures [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1002/pssb.200880581\"\n     onclick=\"log_download('ankiewicz-gehlhoff-martins-pereira-pereira-hoffmann-kaidashev-rahm-etal-magneticandstructuralpropertiesoftransitionmetaldopedzincoxidenanostructures-2009', 'http://doi.org/10.1002/pssb.200880581', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/ankiewicz-gehlhoff-martins-pereira-pereira-hoffmann-kaidashev-rahm-etal-magneticandstructuralpropertiesoftransitionmetaldopedzincoxidenanostructures-2009\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('ankiewicz-gehlhoff-martins-pereira-pereira-hoffmann-kaidashev-rahm-etal-magneticandstructuralpropertiesoftransitionmetaldopedzincoxidenanostructures-2009')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{ankiewicz_magnetic_2009,\n\ttitle = {Magnetic and structural properties of transition metal doped zinc-oxide nanostructures},\n\tvolume = {246},\n\tcopyright = {Copyright © 2009 WILEY-VCH Verlag GmbH \\&amp; Co. KGaA, Weinheim},\n\tissn = {1521-3951},\n\turl = {https://onlinelibrary.wiley.com/doi/abs/10.1002/pssb.200880581},\n\tdoi = {10.1002/pssb.200880581},\n\tabstract = {We report on the magnetic and structural properties of two types of nanostructures doped with Co or Mn, namely, ZnO nanowires and colloidal ZnO nanocrystals. Electron paramagnetic resonance (EPR) spectra have been measured and analysed to extract information on the incorporation of the ions in the lattice. A detailed analysis by means of simulations of the experimental EPR spectra confirms that the transition metal (TM) ions were mainly incorporated as TM2+, occupying the Zn2+ sites in the wurtzite structure of ZnO. Furthermore, for both types of nanostructures, the EPR spectra are composed of more than one signal, revealing locally distorted environments or core-shell structures, proved by surface modifications via inorganic coatings. (© 2009 WILEY-VCH Verlag GmbH \\&amp; Co. KGaA, Weinheim)},\n\tlanguage = {en},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {physica status solidi (b)},\n\tauthor = {Ankiewicz, Amélia O. and Gehlhoff, Wolfgang and Martins, Joana S. and Pereira, Ângela S. and Pereira, Sérgio and Hoffmann, Axel and Kaidashev, Evgeni M. and Rahm, Andreas and Lorenz, Michael and Grundmann, Marius and Carmo, Maria C. and Trindade, Tito and Sobolev, Nikolai A.},\n\tyear = {2009},\n\tnote = {\\_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb.200880581},\n\tkeywords = {61.72.Vv, 68.65.La, 75.50.Pp, 76.30.Fc, 81.07.Bc},\n\tpages = {766--770},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We report on the magnetic and structural properties of two types of nanostructures doped with Co or Mn, namely, ZnO nanowires and colloidal ZnO nanocrystals. Electron paramagnetic resonance (EPR) spectra have been measured and analysed to extract information on the incorporation of the ions in the lattice. A detailed analysis by means of simulations of the experimental EPR spectra confirms that the transition metal (TM) ions were mainly incorporated as TM2+, occupying the Zn2+ sites in the wurtzite structure of ZnO. Furthermore, for both types of nanostructures, the EPR spectra are composed of more than one signal, revealing locally distorted environments or core-shell structures, proved by surface modifications via inorganic coatings. (© 2009 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---origin-2009\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://urss.ru/cgi-bin/db.pl?lang=Ru&amp;blang=ru&amp;page=Book&amp;id=81481&amp;list=Found\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---origin-2009', 'https://urss.ru/cgi-bin/db.pl?lang=Ru&amp;blang=ru&amp;page=Book&amp;id=81481&amp;list=Found', event);\">\n    Обработка и визуализация данных физических экспериментов с помощью пакета Origin.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Исакова О.П.; Тарасевич Ю.Ю.;  and Юзюк Ю.И.\n</span>\n\n  \n\n</span>\n\n   2009.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://urss.ru/cgi-bin/db.pl?lang=Ru&amp;blang=ru&amp;page=Book&amp;id=81481&amp;list=Found\"\n     onclick=\"log_download('---origin-2009', 'https://urss.ru/cgi-bin/db.pl?lang=Ru&amp;blang=ru&amp;page=Book&amp;id=81481&amp;list=Found', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Обработка и визуализация данных физических экспериментов с помощью пакета Origin [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---origin-2009\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---origin-2009')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@book{___2009,\n\ttitle = {Обработка и визуализация данных физических экспериментов с помощью пакета {Origin}},\n\tisbn = {978-5-397-00183-0},\n\turl = {https://urss.ru/cgi-bin/db.pl?lang=Ru&amp;blang=ru&amp;page=Book&amp;id=81481&amp;list=Found},\n\tabstract = {Настоящее учебно-методическое пособие на конкретных примерах учит приемам обработки спектров с помощью пакета Origin. Рассматриваются типичные задачи, наиболее часто встречающиеся на практике.\n\nПособие может использоваться при изучении дисциплин общего и специального физического практикума студентами направлений &quot;Нанотехнология&quot;, &quot;Физика&quot; и других физических направлений и специальностей. Оно будет полезно всем, кому по роду своей деятельности приходится иметь дело с анализом спектров.},\n\tauthor = {{Исакова О.П.} and {Тарасевич Ю.Ю.} and {Юзюк Ю.И.}},\n\tyear = {2009},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Настоящее учебно-методическое пособие на конкретных примерах учит приемам обработки спектров с помощью пакета Origin. Рассматриваются типичные задачи, наиболее часто встречающиеся на практике. Пособие может использоваться при изучении дисциплин общего и специального физического практикума студентами направлений \"Нанотехнология\", \"Физика\" и других физических направлений и специальностей. Оно будет полезно всем, кому по роду своей деятельности приходится иметь дело с анализом спектров.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----basrtiotextrm3-2009\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/2288\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----basrtiotextrm3-2009', 'https://journals.ioffe.ru/articles/2288', event);\">\n    Терагерцевые диэлектрические спектры тонких пленок (Ba,Sr)TiO$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Командин, Г. А.; Волков, А. А.; Спектор, И. Е.; Воротилов, К. А.;  and Мухортов, В. М.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 51(7): 1280–1283. June 2009.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/2288\"\n     onclick=\"log_download('-----basrtiotextrm3-2009', 'https://journals.ioffe.ru/articles/2288', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Терагерцевые диэлектрические спектры тонких пленок (Ba,Sr)TiO$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----basrtiotextrm3-2009\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----basrtiotextrm3-2009')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2009,\n\ttitle = {Терагерцевые диэлектрические спектры тонких пленок ({Ba},{Sr}){TiO}$_{\\textrm{3}}$},\n\tvolume = {51},\n\turl = {https://journals.ioffe.ru/articles/2288},\n\tabstract = {Измерены спектры отражения и пропускания пленок Ba0.7Sr0.3TiO3 с толщинами 36 и 800 mum на подложке из MgO на частотах 8-1000 cm-1 при комнатной температуре. Методом моделирования извлечены диэлектрические параметры материала пленок. Найдена зависимость диэлектрической проницаемости от толщины пленки. Выявлено сильное влияние спектра поглощения излучения в подложке на расчетные диэлектрические спектры материала пленки. Показана необходимость учета при моделировании подфононных диэлектрических потерь в подложке.},\n\tlanguage = {ru},\n\tnumber = {7},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Командин, Г. А. and Волков, А. А. and Спектор, И. Е. and Воротилов, К. А. and Мухортов, В. М.},\n\tmonth = jun,\n\tyear = {2009},\n\tpages = {1280--1283},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Измерены спектры отражения и пропускания пленок Ba0.7Sr0.3TiO3 с толщинами 36 и 800 mum на подложке из MgO на частотах 8-1000 cm-1 при комнатной температуре. Методом моделирования извлечены диэлектрические параметры материала пленок. Найдена зависимость диэлектрической проницаемости от толщины пленки. Выявлено сильное влияние спектра поглощения излучения в подложке на расчетные диэлектрические спектры материала пленки. Показана необходимость учета при моделировании подфононных диэлектрических потерь в подложке.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---srtiotextrm3-2009\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/2235\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---srtiotextrm3-2009', 'https://journals.ioffe.ru/articles/2235', event);\">\n    Феноменологическое описание тонких пленок SrTiO$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Широков, В. Б.; Юзюк, Ю. И.;  and Леманов, В. В.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 51(5): 972–978. April 2009.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/2235\"\n     onclick=\"log_download('---srtiotextrm3-2009', 'https://journals.ioffe.ru/articles/2235', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Феноменологическое описание тонких пленок SrTiO$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---srtiotextrm3-2009\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---srtiotextrm3-2009')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2009-1,\n\ttitle = {Феноменологическое описание тонких пленок {SrTiO}$_{\\textrm{3}}$},\n\tvolume = {51},\n\turl = {https://journals.ioffe.ru/articles/2235},\n\tabstract = {Проведено вычисление констант феноменологического потенциала SrTiO3 с учетом последних экспериментальных данных. По сравнению с ранее приведенными значениями константы alpha11,alpha12,t44 изменены более чем на порядок. Рассчитаны фазовые T-P-диаграммы при действии одноосных - [001] и [110] - нагрузок. Построена фазовая диаграмма температура-деформация (misfit strain) тонкой пленки SrTiO3, на которой чисто сегнетоэлектрические фазы существуют при низких температурах.},\n\tlanguage = {ru},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Широков, В. Б. and Юзюк, Ю. И. and Леманов, В. В.},\n\tmonth = apr,\n\tyear = {2009},\n\tpages = {972--978},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Проведено вычисление констант феноменологического потенциала SrTiO3 с учетом последних экспериментальных данных. По сравнению с ранее приведенными значениями константы alpha11,alpha12,t44 изменены более чем на порядок. Рассчитаны фазовые T-P-диаграммы при действии одноосных - [001] и [110] - нагрузок. Построена фазовая диаграмма температура-деформация (misfit strain) тонкой пленки SrTiO3, на которой чисто сегнетоэлектрические фазы существуют при низких температурах.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-yuzyuk-dkhil-lemanov-phenomenologicaltheoryofphasetransitionsinepitaxialbatextrmxsrtextrm1xtiotextrm3thinfilms-2009\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.79.144118\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-yuzyuk-dkhil-lemanov-phenomenologicaltheoryofphasetransitionsinepitaxialbatextrmxsrtextrm1xtiotextrm3thinfilms-2009', 'https://link.aps.org/doi/10.1103/PhysRevB.79.144118', event);\">\n    Phenomenological theory of phase transitions in epitaxial Ba$_{\\textrm{x}}$Sr$_{\\textrm{1-x}}$TiO$_{\\textrm{3}}$ thin films.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.; Yuzyuk, Y. I.; Dkhil, B.;  and Lemanov, V. V.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 79(14): 144118. April 2009.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.79.144118\"\n     onclick=\"log_download('shirokov-yuzyuk-dkhil-lemanov-phenomenologicaltheoryofphasetransitionsinepitaxialbatextrmxsrtextrm1xtiotextrm3thinfilms-2009', 'https://link.aps.org/doi/10.1103/PhysRevB.79.144118', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Phenomenological theory of phase transitions in epitaxial Ba$_{\\textrm{x}}$Sr$_{\\textrm{1-x}}$TiO$_{\\textrm{3}}$ thin films [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.79.144118\"\n     onclick=\"log_download('shirokov-yuzyuk-dkhil-lemanov-phenomenologicaltheoryofphasetransitionsinepitaxialbatextrmxsrtextrm1xtiotextrm3thinfilms-2009', 'http://doi.org/10.1103/PhysRevB.79.144118', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-yuzyuk-dkhil-lemanov-phenomenologicaltheoryofphasetransitionsinepitaxialbatextrmxsrtextrm1xtiotextrm3thinfilms-2009\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-yuzyuk-dkhil-lemanov-phenomenologicaltheoryofphasetransitionsinepitaxialbatextrmxsrtextrm1xtiotextrm3thinfilms-2009')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_phenomenological_2009,\n\ttitle = {Phenomenological theory of phase transitions in epitaxial {Ba}$_{\\textrm{x}}${Sr}$_{\\textrm{1-x}}${TiO}$_{\\textrm{3}}$ thin films},\n\tvolume = {79},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.79.144118},\n\tdoi = {10.1103/PhysRevB.79.144118},\n\tabstract = {A phenomenological thermodynamic theory of BaxSr1−xTiO3 (BST-x) thin films epitaxially grown on cubic substrates is developed using the Landau-Devonshire approach. The eighth-order thermodynamic potential for BaTiO3 (BT) single crystal and modified fourth-order potential for SrTiO3 single crystal were used as starting potentials for the end members of the solid solution with the aim to develop potential of BST-x solid solution valid at high temperatures. Several coefficients of these potentials for BT were changed to obtain reasonable agreement between theory and experimental phase diagram for BST-x (x{\\textgreater}0.2) solid solutions. For low Ba content we constructed the specific phase diagram where five phases converge at the multiphase point (TN2=48 K, x=0.029) and all transitions are of the second order. The “concentration-misfit strain” phase diagrams for BST-x thin films at room temperature and “temperature-misfit strain” phase diagrams for particular concentrations are constructed and discussed. Near TN2 coupling between polarization and structural order parameter in the epitaxial film is modified considerably and large number of new phases not present in the bulk materials appear on the phase diagram.},\n\tnumber = {14},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Shirokov, V. B. and Yuzyuk, Yu. I. and Dkhil, B. and Lemanov, V. V.},\n\tmonth = apr,\n\tyear = {2009},\n\tnote = {Publisher: American Physical Society},\n\tpages = {144118},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\56FT9N2S\\\\Shirokov и др. - 2009 - Phenomenological theory of phase transitions in ep.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A phenomenological thermodynamic theory of BaxSr1−xTiO3 (BST-x) thin films epitaxially grown on cubic substrates is developed using the Landau-Devonshire approach. The eighth-order thermodynamic potential for BaTiO3 (BT) single crystal and modified fourth-order potential for SrTiO3 single crystal were used as starting potentials for the end members of the solid solution with the aim to develop potential of BST-x solid solution valid at high temperatures. Several coefficients of these potentials for BT were changed to obtain reasonable agreement between theory and experimental phase diagram for BST-x (x\\textgreater0.2) solid solutions. For low Ba content we constructed the specific phase diagram where five phases converge at the multiphase point (TN2=48 K, x=0.029) and all transitions are of the second order. The “concentration-misfit strain” phase diagrams for BST-x thin films at room temperature and “temperature-misfit strain” phase diagrams for particular concentrations are constructed and discussed. Near TN2 coupling between polarization and structural order parameter in the epitaxial film is modified considerably and large number of new phases not present in the bulk materials appear on the phase diagram.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"--peres-monteiro-correira-sobolev-zno-2009\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/9840\"\n     onclick=\"return trackOutboundLink('publications', 'click', '--peres-monteiro-correira-sobolev-zno-2009', 'https://journals.ioffe.ru/articles/9840', event);\">\n    Оптические и структурные свойства наностержней ZnO, полученных методом импульсного лазерного напыления без катализатора.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Кайдашев, В. Е.; Кайдашев, Е. М.; Peres, M.; Monteiro, T.; Correira, M. R.;  and Sobolev, N. A.\n</span>\n\n  \n\n</span>\n\n  <i>Журнал технической физики</i>, 79(11): 45–49. October 2009.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/9840\"\n     onclick=\"log_download('--peres-monteiro-correira-sobolev-zno-2009', 'https://journals.ioffe.ru/articles/9840', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Оптические и структурные свойства наностержней ZnO, полученных методом импульсного лазерного напыления без катализатора [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/--peres-monteiro-correira-sobolev-zno-2009\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('--peres-monteiro-correira-sobolev-zno-2009')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2009-2,\n\ttitle = {Оптические и структурные свойства наностержней {ZnO}, полученных методом импульсного лазерного напыления без катализатора},\n\tvolume = {79},\n\turl = {https://journals.ioffe.ru/articles/9840},\n\tabstract = {Методом импульсного лазерного напыления без использования катализатора на сапфире получены наностержни ZnO диаметром менее 10 nm. Исследованы структурные особенности наностержней методом комбинационного рассеяния при возбуждении в видимом и УФ-диапазонах. Изучены температурные зависимости экситонных спектров, а также поведение зеленой люминесценции в диапазоне 10-280 K. Интенсивность люминесценции полученных наностержней ZnO в экситонной области превышала зеленую люминесценцию в 7.8 раза при комнатной температуре.},\n\tlanguage = {ru},\n\tnumber = {11},\n\turldate = {2023-11-11},\n\tjournal = {Журнал технической физики},\n\tauthor = {Кайдашев, В. Е. and Кайдашев, Е. М. and Peres, M. and Monteiro, T. and Correira, M. R. and Sobolev, N. A.},\n\tmonth = oct,\n\tyear = {2009},\n\tpages = {45--49},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Методом импульсного лазерного напыления без использования катализатора на сапфире получены наностержни ZnO диаметром менее 10 nm. Исследованы структурные особенности наностержней методом комбинационного рассеяния при возбуждении в видимом и УФ-диапазонах. Изучены температурные зависимости экситонных спектров, а также поведение зеленой люминесценции в диапазоне 10-280 K. Интенсивность люминесценции полученных наностержней ZnO в экситонной области превышала зеленую люминесценцию в 7.8 раза при комнатной температуре.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------2009\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/9770\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------2009', 'https://journals.ioffe.ru/articles/9770', event);\">\n    Исследование пьезоактивности тонких пленок цирконата-титаната свинца.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Бирюков, С. В.; Головко, Ю. И.; Масычев, С. И.; Мухортов, В. М.;  and Шелепо, А. П.\n</span>\n\n  \n\n</span>\n\n  <i>Журнал технической физики</i>, 79(8): 90–92. July 2009.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/9770\"\n     onclick=\"log_download('------2009', 'https://journals.ioffe.ru/articles/9770', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Исследование пьезоактивности тонких пленок цирконата-титаната свинца [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------2009\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------2009')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2009-3,\n\ttitle = {Исследование пьезоактивности тонких пленок цирконата-титаната свинца},\n\tvolume = {79},\n\turl = {https://journals.ioffe.ru/articles/9770},\n\tabstract = {зучены особенности проявления пьезоактивности тонких сегнетоэлектрических пленок цирконата-титаната свинца, полученных высокочастотным катодным распылением мишеней стехиометрического состава. Установлено, что пленки обладают естественной униполярностью. Обсуждаются возможные причины этого явления. Экспериментально построено семейство петель пьезоэлектрического гистерезиса при различных значениях частоты и напряженности внешнего смещающего поля. Полученные зависимости сравниваются с классическими петлями диэлектрического гистерезиса},\n\tnumber = {8},\n\turldate = {2023-11-11},\n\tjournal = {Журнал технической физики},\n\tauthor = {Бирюков, С. В. and Головко, Ю. И. and Масычев, С. И. and Мухортов, В. М. and Шелепо, А. П.},\n\tmonth = jul,\n\tyear = {2009},\n\tpages = {90--92},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  зучены особенности проявления пьезоактивности тонких сегнетоэлектрических пленок цирконата-титаната свинца, полученных высокочастотным катодным распылением мишеней стехиометрического состава. Установлено, что пленки обладают естественной униполярностью. Обсуждаются возможные причины этого явления. Экспериментально построено семейство петель пьезоэлектрического гистерезиса при различных значениях частоты и напряженности внешнего смещающего поля. Полученные зависимости сравниваются с классическими петлями диэлектрического гистерезиса\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----2009\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://ufn.ru/ru/articles/2009/8/k/\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----2009', 'https://ufn.ru/ru/articles/2009/8/k/', event);\">\n    Гетероэпитаксиальные плёнки мультиферроика феррита висмута, допированного неодимом.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Мухортов, В. М.; Головко, Ю. И.;  and Юзюк, Ю. И.\n</span>\n\n  \n\n</span>\n\n  <i>Успехи физических наук</i>, 179(8): 909–913. August 2009.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://ufn.ru/ru/articles/2009/8/k/\"\n     onclick=\"log_download('----2009', 'https://ufn.ru/ru/articles/2009/8/k/', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Гетероэпитаксиальные плёнки мультиферроика феррита висмута, допированного неодимом [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----2009\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----2009')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2009-4,\n\ttitle = {Гетероэпитаксиальные плёнки мультиферроика феррита висмута, допированного неодимом},\n\tvolume = {179},\n\tissn = {0042-1294},\n\turl = {https://ufn.ru/ru/articles/2009/8/k/},\n\tabstract = {Гетероэпитаксиальные плёнки мультиферроика феррита висмута, допированного неодимом, Мухортов В.М., Головко Ю.И., Юзюк Ю.И.},\n\tlanguage = {ru},\n\tnumber = {8},\n\turldate = {2023-11-11},\n\tjournal = {Успехи физических наук},\n\tauthor = {Мухортов, В. М. and Головко, Ю. И. and Юзюк, Ю. И.},\n\tmonth = aug,\n\tyear = {2009},\n\tkeywords = {⛔ No DOI found},\n\tpages = {909--913},\n\tfile = {Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\2X6KHVNX\\\\Мухортов и др. - 2009 - Гетероэпитаксиальные плёнки мультиферроика феррита.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Гетероэпитаксиальные плёнки мультиферроика феррита висмута, допированного неодимом, Мухортов В.М., Головко Ю.И., Юзюк Ю.И.\n</div>\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2008\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2008')\"\n      onkeypress=\"toggleGroup('group_2008')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2008</span>\n      <span class=\"bibbase_group_count\">\n        \n        (14)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"czekalla-guinard-hanisch-cao-kaidashev-boukos-travlos-renard-etal-spatialfluctuationsofopticalemissionfromsingleznomgznonanowirequantumwells-2008\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/0957-4484/19/11/115202\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'czekalla-guinard-hanisch-cao-kaidashev-boukos-travlos-renard-etal-spatialfluctuationsofopticalemissionfromsingleznomgznonanowirequantumwells-2008', 'https://dx.doi.org/10.1088/0957-4484/19/11/115202', event);\">\n    Spatial fluctuations of optical emission from single ZnO/MgZnO nanowire quantum wells.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Czekalla, C.; Guinard, J.; Hanisch, C.; Cao, B. Q.; Kaidashev, E. M.; Boukos, N.; Travlos, A.; Renard, J.; Gayral, B.; Dang, D. L. S.; Lorenz, M.;  and Grundmann, M.\n</span>\n\n  \n\n</span>\n\n  <i>Nanotechnology</i>, 19(11): 115202. February 2008.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/0957-4484/19/11/115202\"\n     onclick=\"log_download('czekalla-guinard-hanisch-cao-kaidashev-boukos-travlos-renard-etal-spatialfluctuationsofopticalemissionfromsingleznomgznonanowirequantumwells-2008', 'https://dx.doi.org/10.1088/0957-4484/19/11/115202', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Spatial fluctuations of optical emission from single ZnO/MgZnO nanowire quantum wells [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/0957-4484/19/11/115202\"\n     onclick=\"log_download('czekalla-guinard-hanisch-cao-kaidashev-boukos-travlos-renard-etal-spatialfluctuationsofopticalemissionfromsingleznomgznonanowirequantumwells-2008', 'http://doi.org/10.1088/0957-4484/19/11/115202', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/czekalla-guinard-hanisch-cao-kaidashev-boukos-travlos-renard-etal-spatialfluctuationsofopticalemissionfromsingleznomgznonanowirequantumwells-2008\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('czekalla-guinard-hanisch-cao-kaidashev-boukos-travlos-renard-etal-spatialfluctuationsofopticalemissionfromsingleznomgznonanowirequantumwells-2008')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{czekalla_spatial_2008,\n\ttitle = {Spatial fluctuations of optical emission from single {ZnO}/{MgZnO} nanowire quantum wells},\n\tvolume = {19},\n\tissn = {0957-4484},\n\turl = {https://dx.doi.org/10.1088/0957-4484/19/11/115202},\n\tdoi = {10.1088/0957-4484/19/11/115202},\n\tabstract = {MgZnO/ZnO quantum wells on top of ZnO nanowires were grown by pulsed laser deposition. Ensembles of spatially fluctuating and narrow cathodoluminescence peaks with single widths down to 1 meV were found at the spectral position of the quantum well emission at 4 K. In addition, the number of these narrow QW peaks increases with increasing excitation power in micro-photoluminescence, thus pointing to quantum-dot-like emission centers. Indeed, laterally strained areas of about 5 nm diameter were identified at the quantum well positions on top of the nanowires by high-resolution transmission electron microscopy.},\n\tlanguage = {en},\n\tnumber = {11},\n\turldate = {2023-11-11},\n\tjournal = {Nanotechnology},\n\tauthor = {Czekalla, C. and Guinard, J. and Hanisch, C. and Cao, B. Q. and Kaidashev, E. M. and Boukos, N. and Travlos, A. and Renard, J. and Gayral, B. and Dang, D. Le Si and Lorenz, M. and Grundmann, M.},\n\tmonth = feb,\n\tyear = {2008},\n\tpages = {115202},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  MgZnO/ZnO quantum wells on top of ZnO nanowires were grown by pulsed laser deposition. Ensembles of spatially fluctuating and narrow cathodoluminescence peaks with single widths down to 1 meV were found at the spectral position of the quantum well emission at 4 K. In addition, the number of these narrow QW peaks increases with increasing excitation power in micro-photoluminescence, thus pointing to quantum-dot-like emission centers. Indeed, laterally strained areas of about 5 nm diameter were identified at the quantum well positions on top of the nanowires by high-resolution transmission electron microscopy.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kaidashev-lorenz-lenzner-ramm-nobis-grundmann-zakharov-kozakov-etal-structureandopticalpropertiesofznonanowiresfabricatedbypulsedlaserdepositionongansi111filmswiththeuseofauandniocatalysts-2008\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://link.springer.com/10.3103/S1062873808080315\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kaidashev-lorenz-lenzner-ramm-nobis-grundmann-zakharov-kozakov-etal-structureandopticalpropertiesofznonanowiresfabricatedbypulsedlaserdepositionongansi111filmswiththeuseofauandniocatalysts-2008', 'http://link.springer.com/10.3103/S1062873808080315', event);\">\n    Structure and optical properties of ZnO nanowires fabricated by pulsed laser deposition on GaN/Si(111) films with the use of Au and NiO catalysts.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kaidashev, E. M.; Lorenz, M.; Lenzner, J.; Ramm, A.; Nobis, T.; Grundmann, M.; Zakharov, N.; Kozakov, A. T.; Shevtsova, S. I.; Abdulvakhidov, K. G.;  and Kaidashev, V. E.\n</span>\n\n  \n\n</span>\n\n  <i>Bulletin of the Russian Academy of Sciences: Physics</i>, 72(8): 1129–1131. August 2008.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://link.springer.com/10.3103/S1062873808080315\"\n     onclick=\"log_download('kaidashev-lorenz-lenzner-ramm-nobis-grundmann-zakharov-kozakov-etal-structureandopticalpropertiesofznonanowiresfabricatedbypulsedlaserdepositionongansi111filmswiththeuseofauandniocatalysts-2008', 'http://link.springer.com/10.3103/S1062873808080315', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Structure and optical properties of ZnO nanowires fabricated by pulsed laser deposition on GaN/Si(111) films with the use of Au and NiO catalysts [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3103/S1062873808080315\"\n     onclick=\"log_download('kaidashev-lorenz-lenzner-ramm-nobis-grundmann-zakharov-kozakov-etal-structureandopticalpropertiesofznonanowiresfabricatedbypulsedlaserdepositionongansi111filmswiththeuseofauandniocatalysts-2008', 'http://doi.org/10.3103/S1062873808080315', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kaidashev-lorenz-lenzner-ramm-nobis-grundmann-zakharov-kozakov-etal-structureandopticalpropertiesofznonanowiresfabricatedbypulsedlaserdepositionongansi111filmswiththeuseofauandniocatalysts-2008\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kaidashev-lorenz-lenzner-ramm-nobis-grundmann-zakharov-kozakov-etal-structureandopticalpropertiesofznonanowiresfabricatedbypulsedlaserdepositionongansi111filmswiththeuseofauandniocatalysts-2008')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kaidashev_structure_2008,\n\ttitle = {Structure and optical properties of {ZnO} nanowires fabricated by pulsed laser deposition on {GaN}/{Si}(111) films with the use of {Au} and {NiO} catalysts},\n\tvolume = {72},\n\tissn = {1062-8738, 1934-9432},\n\turl = {http://link.springer.com/10.3103/S1062873808080315},\n\tdoi = {10.3103/S1062873808080315},\n\tlanguage = {en},\n\tnumber = {8},\n\turldate = {2023-11-11},\n\tjournal = {Bulletin of the Russian Academy of Sciences: Physics},\n\tauthor = {Kaidashev, E. M. and Lorenz, M. and Lenzner, J. and Ramm, A. and Nobis, T. and Grundmann, M. and Zakharov, N. and Kozakov, A. T. and Shevtsova, S. I. and Abdulvakhidov, K. G. and Kaidashev, V. E.},\n\tmonth = aug,\n\tyear = {2008},\n\tpages = {1129--1131},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\TPG4HECU\\\\Kaidashev и др. - 2008 - Structure and optical properties of ZnO nanowires .pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"schmidtgrund-rheinlnder-kaidashev-lorenz-grundmann-fritsch-schubert-schmidt-etal-vacuumultravioletdielectricfunctionandbandstructureofzno-2008\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://www.jkps.or.kr/journal/DOIx.php?id=10.3938/jkps.53.88\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'schmidtgrund-rheinlnder-kaidashev-lorenz-grundmann-fritsch-schubert-schmidt-etal-vacuumultravioletdielectricfunctionandbandstructureofzno-2008', 'http://www.jkps.or.kr/journal/DOIx.php?id=10.3938/jkps.53.88', event);\">\n    Vacuum Ultraviolet Dielectric Function and Band Structure of ZnO.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Schmidt-Grund, R.; Rheinländer, B.; Kaidashev, E. M.; Lorenz, M.; Grundmann, M.; Fritsch, D.; Schubert, M. M.; Schmidt, H.;  and Herzinger, C. M.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of the Korean Physical Society</i>, 53(1): 88–93. July 2008.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://www.jkps.or.kr/journal/DOIx.php?id=10.3938/jkps.53.88\"\n     onclick=\"log_download('schmidtgrund-rheinlnder-kaidashev-lorenz-grundmann-fritsch-schubert-schmidt-etal-vacuumultravioletdielectricfunctionandbandstructureofzno-2008', 'http://www.jkps.or.kr/journal/DOIx.php?id=10.3938/jkps.53.88', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Vacuum Ultraviolet Dielectric Function and Band Structure of ZnO [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.3938/jkps.53.88\"\n     onclick=\"log_download('schmidtgrund-rheinlnder-kaidashev-lorenz-grundmann-fritsch-schubert-schmidt-etal-vacuumultravioletdielectricfunctionandbandstructureofzno-2008', 'http://doi.org/10.3938/jkps.53.88', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/schmidtgrund-rheinlnder-kaidashev-lorenz-grundmann-fritsch-schubert-schmidt-etal-vacuumultravioletdielectricfunctionandbandstructureofzno-2008\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('schmidtgrund-rheinlnder-kaidashev-lorenz-grundmann-fritsch-schubert-schmidt-etal-vacuumultravioletdielectricfunctionandbandstructureofzno-2008')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{schmidt-grund_vacuum_2008,\n\ttitle = {Vacuum {Ultraviolet} {Dielectric} {Function} and {Band} {Structure} of {ZnO}},\n\tvolume = {53},\n\tissn = {0374-4884},\n\turl = {http://www.jkps.or.kr/journal/DOIx.php?id=10.3938/jkps.53.88},\n\tdoi = {10.3938/jkps.53.88},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Journal of the Korean Physical Society},\n\tauthor = {Schmidt-Grund, Rüdiger and Rheinländer, Bernd and Kaidashev, Evgeni M. and Lorenz, Michael and Grundmann, Marius and Fritsch, Daniel and Schubert, Mathias M. and Schmidt, Heidemarie and Herzinger, Craig M.},\n\tmonth = jul,\n\tyear = {2008},\n\tpages = {88--93},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"grundmann-rahm-nobis-lorenz-czekalla-kaidashev-lenzner-boukos-etal-growthandcharacterizationofznonanoandmicrostructures-2008\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/B9780080463254000098\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'grundmann-rahm-nobis-lorenz-czekalla-kaidashev-lenzner-boukos-etal-growthandcharacterizationofznonanoandmicrostructures-2008', 'https://linkinghub.elsevier.com/retrieve/pii/B9780080463254000098', event);\">\n    Growth and Characterization of ZnO Nano- and Microstructures.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Grundmann, M.; Rahm, A.; Nobis, T.; Lorenz, M.; Czekalla, C.; Kaidashev, E. M.; Lenzner, J.; Boukos, N.;  and Travlos, A.\n</span>\n\n  \n\n</span>\n\n  In <i>Handbook of Self Assembled Semiconductor Nanostructures for Novel Devices in Photonics and Electronics</i>, pages 293–323. Elsevier,  2008.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://linkinghub.elsevier.com/retrieve/pii/B9780080463254000098\"\n     onclick=\"log_download('grundmann-rahm-nobis-lorenz-czekalla-kaidashev-lenzner-boukos-etal-growthandcharacterizationofznonanoandmicrostructures-2008', 'https://linkinghub.elsevier.com/retrieve/pii/B9780080463254000098', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Growth and Characterization of ZnO Nano- and Microstructures [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/B978-0-08-046325-4.00009-8\"\n     onclick=\"log_download('grundmann-rahm-nobis-lorenz-czekalla-kaidashev-lenzner-boukos-etal-growthandcharacterizationofznonanoandmicrostructures-2008', 'http://doi.org/10.1016/B978-0-08-046325-4.00009-8', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/grundmann-rahm-nobis-lorenz-czekalla-kaidashev-lenzner-boukos-etal-growthandcharacterizationofznonanoandmicrostructures-2008\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('grundmann-rahm-nobis-lorenz-czekalla-kaidashev-lenzner-boukos-etal-growthandcharacterizationofznonanoandmicrostructures-2008')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@incollection{grundmann_growth_2008,\n\ttitle = {Growth and {Characterization} of {ZnO} {Nano}- and {Microstructures}},\n\tisbn = {978-0-08-046325-4},\n\turl = {https://linkinghub.elsevier.com/retrieve/pii/B9780080463254000098},\n\tlanguage = {en},\n\turldate = {2023-11-11},\n\tbooktitle = {Handbook of {Self} {Assembled} {Semiconductor} {Nanostructures} for {Novel} {Devices} in {Photonics} and {Electronics}},\n\tpublisher = {Elsevier},\n\tauthor = {Grundmann, Marius and Rahm, Andreas and Nobis, Thomas and Lorenz, Michael and Czekalla, Christian and Kaidashev, Evgeni M. and Lenzner, Jörg and Boukos, Nikos and Travlos, Anastasios},\n\tyear = {2008},\n\tdoi = {10.1016/B978-0-08-046325-4.00009-8},\n\tpages = {293--323},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----2008\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  Введение в химию и физику наноструктур и наноструктурированных материалов.\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Таланов В.М.; Ерейская Г.П.;  and Юзюк Ю.И.\n</span>\n\n  \n\n</span>\n\n  Москва: Академия Естествознания,  2008.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----2008\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----2008')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@book{___2008,\n\ttitle = {Введение в химию и физику наноструктур и наноструктурированных материалов},\n\tisbn = {978-5-91327-029-0},\n\tpublisher = {Москва: Академия Естествознания},\n\tauthor = {{Таланов В.М.} and {Ерейская Г.П.} and {Юзюк Ю.И.}},\n\tyear = {2008},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----simon-pbtextrm1xcatextrmxtiotextrm3040textlessxtextless062-2008\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/2094\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----simon-pbtextrm1xcatextrmxtiotextrm3040textlessxtextless062-2008', 'https://journals.ioffe.ru/articles/2094', event);\">\n    Микрорамановский отклик и осцилляторные параметры фононов в твердых растворах Pb$_{\\textrm{1-x}}$Ca$_{\\textrm{x}}$TiO$_{\\textrm{3}}$ (0.40\\textlessx\\textless0.62).\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Чабанюк, А. Н.; Торгашев, В. И.; Юзюк, Ю. И.; Леманов, В. В.;  and Simon, P.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 51(1): 155–163. December 2008.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/2094\"\n     onclick=\"log_download('----simon-pbtextrm1xcatextrmxtiotextrm3040textlessxtextless062-2008', 'https://journals.ioffe.ru/articles/2094', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Микрорамановский отклик и осцилляторные параметры фононов в твердых растворах Pb$_{\\textrm{1-x}}$Ca$_{\\textrm{x}}$TiO$_{\\textrm{3}}$ (0.40\\textlessx\\textless0.62) [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----simon-pbtextrm1xcatextrmxtiotextrm3040textlessxtextless062-2008\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----simon-pbtextrm1xcatextrmxtiotextrm3040textlessxtextless062-2008')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2008,\n\ttitle = {Микрорамановский отклик и осцилляторные параметры фононов в твердых растворах {Pb}$_{\\textrm{1-x}}${Ca}$_{\\textrm{x}}${TiO}$_{\\textrm{3}}$ (0.40{\\textless}x{\\textless}0.62)},\n\tvolume = {51},\n\turl = {https://journals.ioffe.ru/articles/2094},\n\tabstract = {Посредством температурных (295{\\textless}T{\\textless}650 K) исследований поляризованных спектров комбинационного рассеяния света в области частот 10{\\textless}nu{\\textless}1200 cm-1 на монокристаллическом образце твердого раствора Pb0.54Ca0.46TiO3 установлено существование по крейней мере одной особой температурной точки (Tc{\\textasciitilde}392 K), в которой наблюдаются заметные аномалии осцилляторных параметров фононных мод. Аналогичные явления имеют место в растворах с 0.4{\\textless}x{\\textless}0.5. Резкий рост интенсивности спектральных линий, соответствующих волнам поляризации, при температурах сразу ниже Tc позволяет сделать вывод о трансформации Pb1-xCaxTiO3 (0.4{\\textless}x{\\textless}0.5) в полярное состояние, которое отсутствует в системе при концентрациях x{\\textgreater}0.5.},\n\tlanguage = {ru},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Чабанюк, А. Н. and Торгашев, В. И. and Юзюк, Ю. И. and Леманов, В. В. and Simon, P.},\n\tmonth = dec,\n\tyear = {2008},\n\tpages = {155--163},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Посредством температурных (295\\textlessT\\textless650 K) исследований поляризованных спектров комбинационного рассеяния света в области частот 10\\textlessnu\\textless1200 cm-1 на монокристаллическом образце твердого раствора Pb0.54Ca0.46TiO3 установлено существование по крейней мере одной особой температурной точки (Tc~392 K), в которой наблюдаются заметные аномалии осцилляторных параметров фононных мод. Аналогичные явления имеют место в растворах с 0.4\\textlessx\\textless0.5. Резкий рост интенсивности спектральных линий, соответствующих волнам поляризации, при температурах сразу ниже Tc позволяет сделать вывод о трансформации Pb1-xCaxTiO3 (0.4\\textlessx\\textless0.5) в полярное состояние, которое отсутствует в системе при концентрациях x\\textgreater0.5.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"--dkhil--batiotextrm3-2008\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/2648\"\n     onclick=\"return trackOutboundLink('publications', 'click', '--dkhil--batiotextrm3-2008', 'https://journals.ioffe.ru/articles/2648', event);\">\n    Феноменологическое описание фазовых переходов в тонких пленках BaTiO$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Широков, В. Б.; Юзюк, Ю. И.; Dkhil, B.;  and Леманов, В. В.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 50(5): 889–896.  2008.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/2648\"\n     onclick=\"log_download('--dkhil--batiotextrm3-2008', 'https://journals.ioffe.ru/articles/2648', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Феноменологическое описание фазовых переходов в тонких пленках BaTiO$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/--dkhil--batiotextrm3-2008\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('--dkhil--batiotextrm3-2008')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2008-1,\n\ttitle = {Феноменологическое описание фазовых переходов в тонких пленках {BaTiO}$_{\\textrm{3}}$},\n\tvolume = {50},\n\turl = {https://journals.ioffe.ru/articles/2648},\n\tabstract = {Проведено феноменологическое описание фазовых переходов в тонких эпитаксиальных пленках BaTiO3 на основе потенциалов Ландау шестой и восьмой степеней. Обнаружена зависимость вида фазовой диаграммы от величины электрострикционного коэффициента Q12. Для разных значений коэффициента Q12, известных из литературы, приведены качественно различные фазовые диаграммы. Определена зависимость деформации несоответствия (misfit strain) пленки от степени тетрагональности пленки при комнатной температуре, что позволяет определить термодинамический путь на фазовой диаграмме для конкретной пленки. Построены зависимости спонтанной поляризации и диэлектрической проницаемости пленки от деформации несоответствия при комнатной температуре.},\n\tlanguage = {ru},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Широков, В. Б. and Юзюк, Ю. И. and Dkhil, B. and Леманов, В. В.},\n\tyear = {2008},\n\tpages = {889--896},\n\tfile = {Физика твердого тела:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\BKW4NGEV\\\\2648.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Проведено феноменологическое описание фазовых переходов в тонких эпитаксиальных пленках BaTiO3 на основе потенциалов Ландау шестой и восьмой степеней. Обнаружена зависимость вида фазовой диаграммы от величины электрострикционного коэффициента Q12. Для разных значений коэффициента Q12, известных из литературы, приведены качественно различные фазовые диаграммы. Определена зависимость деформации несоответствия (misfit strain) пленки от степени тетрагональности пленки при комнатной температуре, что позволяет определить термодинамический путь на фазовой диаграмме для конкретной пленки. Построены зависимости спонтанной поляризации и диэлектрической проницаемости пленки от деформации несоответствия при комнатной температуре.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----2008\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://naukarus.com/fazovye-perehody-v-nanorazmernyh-epitaksialnyh-segnetoelektricheskih-plenkah-titanata-bariya-strontsiya\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----2008', 'http://naukarus.com/fazovye-perehody-v-nanorazmernyh-epitaksialnyh-segnetoelektricheskih-plenkah-titanata-bariya-strontsiya', event);\">\n    Фазовые переходы в наноразмерных эпитаксиальных сегнетоэлектрических пленках титаната бария-стронция.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Головко, Ю. И.; Маматов, А. А.;  and Мухортов, В. М.\n</span>\n\n  \n\n</span>\n\n  <i>Вестник Южного научного центра РАН</i>, 4(2).  2008.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://naukarus.com/fazovye-perehody-v-nanorazmernyh-epitaksialnyh-segnetoelektricheskih-plenkah-titanata-bariya-strontsiya\"\n     onclick=\"log_download('----2008', 'http://naukarus.com/fazovye-perehody-v-nanorazmernyh-epitaksialnyh-segnetoelektricheskih-plenkah-titanata-bariya-strontsiya', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Фазовые переходы в наноразмерных эпитаксиальных сегнетоэлектрических пленках титаната бария-стронция [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----2008\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----2008')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2008-2,\n\ttitle = {Фазовые переходы в наноразмерных эпитаксиальных сегнетоэлектрических пленках титаната бария-стронция},\n\tvolume = {4},\n\tissn = {1813-4289},\n\turl = {http://naukarus.com/fazovye-perehody-v-nanorazmernyh-epitaksialnyh-segnetoelektricheskih-plenkah-titanata-bariya-strontsiya},\n\tabstract = {С использованием дифракции рентгеновского излучения исследованы температурные зависимости параметров решетки в нормальном и тангенциальном к подложке направлении эиитакси-альных пленок титаната бария-стронция разной толщины (от 6 до 980 нм), выращенных по слоевому механизму высокочастотным катодным распылением при повышенном давлении кислорода. Выявлена критическая толщина пленок (-50 нм), ниже которой в пленках существуют сжимающие напряжения, а выше - растягивающие напряжения. Во всем интервале толщин при изменении температуры от 780 до 100 К в пленках наблюдаются два размытых структурных фазовых перехода второго рода.},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Вестник Южного научного центра РАН},\n\tauthor = {Головко, Ю. И. and Маматов, А. А. and Мухортов, В. М.},\n\tyear = {2008},\n\tkeywords = {⛔ No DOI found},\n\tfile = {Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\PWGKVDJ4\\\\fazovye-perehody-v-nanorazmernyh-epitaksialnyh-segnetoelektricheskih-plenkah-titanata-bariya-st.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  С использованием дифракции рентгеновского излучения исследованы температурные зависимости параметров решетки в нормальном и тангенциальном к подложке направлении эиитакси-альных пленок титаната бария-стронция разной толщины (от 6 до 980 нм), выращенных по слоевому механизму высокочастотным катодным распылением при повышенном давлении кислорода. Выявлена критическая толщина пленок (-50 нм), ниже которой в пленках существуют сжимающие напряжения, а выше - растягивающие напряжения. Во всем интервале толщин при изменении температуры от 780 до 100 К в пленках наблюдаются два размытых структурных фазовых перехода второго рода.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---janolin-dkhil--2008\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/2579\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---janolin-dkhil--2008', 'https://journals.ioffe.ru/articles/2579', event);\">\n    Структурные фазовые переходы в наноразмерных сегнетоэлектрических пленках титаната бария–стронция.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Головко, Ю. И.; Мухортов, В. М.; Юзюк, Ю. И.; Janolin, P. E.;  and Dkhil, B.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 50(3): 467–471.  2008.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/2579\"\n     onclick=\"log_download('---janolin-dkhil--2008', 'https://journals.ioffe.ru/articles/2579', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Структурные фазовые переходы в наноразмерных сегнетоэлектрических пленках титаната бария–стронция [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---janolin-dkhil--2008\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---janolin-dkhil--2008')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2008-3,\n\ttitle = {Структурные фазовые переходы в наноразмерных сегнетоэлектрических пленках титаната бария--стронция},\n\tvolume = {50},\n\turl = {https://journals.ioffe.ru/articles/2579},\n\tabstract = {С использованием метода дифракции рентгеновского излучения исследованы температурные зависимости параметров решетки в нормальном и тангенциальном к подложке направлениях эпитаксиальных пленок титаната бария-стронция разной толщины (от 6 до 960 nm), выращенных по слоевому механизму высокочастотным катодным распылением при повышенном давлении кислорода. Выявлена критическая толщина пленок ({\\textasciitilde}50 nm), ниже которой в пленках существуют сжимающие, а выше - растягивающие напряжения. Во всем интервале толщин при изменении температуры от 780 до 100 K в пленках наблюдаются два размытых структурных фазовых перехода второго рода. При растягивающих напряжениях переходы могут соответствовать переходам из тетрагональной параэлектрической фазы в aa-фазу и далее в r-фазу, в то время как при сжимающих напряжениях переходы происходят из тетрагональной параэлектрической фазы в сегнетоэлектрическую c-фазу, а при дальнейшем понижении температуры - в r-фазу. Работа проводилась при финансовой поддержке Российского фонда фундаментальных исследований (гранты N 05-02-17191 и 06-02-16271). PACS: 77.80.-e, 64.70.Nd, 77.55.+f},\n\tlanguage = {ru},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Головко, Ю. И. and Мухортов, В. М. and Юзюк, Ю. И. and Janolin, P. E. and Dkhil, B.},\n\tyear = {2008},\n\tpages = {467--471},\n\tfile = {Физика твердого тела:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\GRNCX2XX\\\\2579.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  С использованием метода дифракции рентгеновского излучения исследованы температурные зависимости параметров решетки в нормальном и тангенциальном к подложке направлениях эпитаксиальных пленок титаната бария-стронция разной толщины (от 6 до 960 nm), выращенных по слоевому механизму высокочастотным катодным распылением при повышенном давлении кислорода. Выявлена критическая толщина пленок (~50 nm), ниже которой в пленках существуют сжимающие, а выше - растягивающие напряжения. Во всем интервале толщин при изменении температуры от 780 до 100 K в пленках наблюдаются два размытых структурных фазовых перехода второго рода. При растягивающих напряжениях переходы могут соответствовать переходам из тетрагональной параэлектрической фазы в aa-фазу и далее в r-фазу, в то время как при сжимающих напряжениях переходы происходят из тетрагональной параэлектрической фазы в сегнетоэлектрическую c-фазу, а при дальнейшем понижении температуры - в r-фазу. Работа проводилась при финансовой поддержке Российского фонда фундаментальных исследований (гранты N 05-02-17191 и 06-02-16271). PACS: 77.80.-e, 64.70.Nd, 77.55.+f\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----sauvajol-pbtextrmxsrtextrm1textrmtextrmxtiotextrm3-2008\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.elibrary.ru/item.asp?id=9934183\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----sauvajol-pbtextrmxsrtextrm1textrmtextrmxtiotextrm3-2008', 'https://www.elibrary.ru/item.asp?id=9934183', event);\">\n    Особенности рамановских спектров и фазовых состояний в твердых растворах Pb$_{\\textrm{x}}$Sr$_{\\textrm{1}}$ $_{\\textrm{-}}$ $_{\\textrm{x}}$TiO$_{\\textrm{3}}$ с низким содержанием свинца.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Торгашев, В. И.; Чабанюк, А. Н.; Юзюк, Ю. И.; Леманов, В. В.;  and Sauvajol, J. L.\n</span>\n\n  \n\n</span>\n\n  <i>Известия Российской Академии Наук. Серия Физическая</i>, 72(4): 569–571.  2008.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.elibrary.ru/item.asp?id=9934183\"\n     onclick=\"log_download('----sauvajol-pbtextrmxsrtextrm1textrmtextrmxtiotextrm3-2008', 'https://www.elibrary.ru/item.asp?id=9934183', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Особенности рамановских спектров и фазовых состояний в твердых растворах Pb$_{\\textrm{x}}$Sr$_{\\textrm{1}}$ $_{\\textrm{-}}$ $_{\\textrm{x}}$TiO$_{\\textrm{3}}$ с низким содержанием свинца [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----sauvajol-pbtextrmxsrtextrm1textrmtextrmxtiotextrm3-2008\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----sauvajol-pbtextrmxsrtextrm1textrmtextrmxtiotextrm3-2008')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2008-4,\n\ttitle = {Особенности рамановских спектров и фазовых состояний в твердых растворах {Pb}$_{\\textrm{x}}${Sr}$_{\\textrm{1}}$ $_{\\textrm{-}}$ $_{\\textrm{x}}${TiO}$_{\\textrm{3}}$ с низким содержанием свинца},\n\tvolume = {72},\n\tissn = {0367-6765},\n\turl = {https://www.elibrary.ru/item.asp?id=9934183},\n\tabstract = {Приведены результаты исследований микрорамановского спектрального отклика в твердых растворах PbxSr1 - xTiO3 (x = 0.005, 0.01, 0.02, 0.03, 0.04) в диапазоне частот 15–1200 см-1 при нескольких температурах между 10 и 300 К. Проведенное исследование позволило сделать вывод, что в твердых растворах PST область концентраций с x {\\textless} 0.04 скорее всего следует рассматривать как гетерофазную.},\n\tlanguage = {ru},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Известия Российской Академии Наук. Серия Физическая},\n\tauthor = {Торгашев, В. И. and Чабанюк, А. Н. and Юзюк, Ю. И. and Леманов, В. В. and Sauvajol, J. L.},\n\tyear = {2008},\n\tkeywords = {⛔ No DOI found},\n\tpages = {569--571},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Приведены результаты исследований микрорамановского спектрального отклика в твердых растворах PbxSr1 - xTiO3 (x = 0.005, 0.01, 0.02, 0.03, 0.04) в диапазоне частот 15–1200 см-1 при нескольких температурах между 10 и 300 К. Проведенное исследование позволило сделать вывод, что в твердых растворах PST область концентраций с x \\textless 0.04 скорее всего следует рассматривать как гетерофазную.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---------2008\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/9548\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---------2008', 'https://journals.ioffe.ru/articles/9548', event);\">\n    Диэлектрические свойства пленок титаната бария-стронция нанометровой толщины.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Мигунов, С. Н.; Волков, А. А.; Командин, Г. А.; Лобанов, А. Н.; Горшунов, Б. П.; Головко, Ю. И.; Мухортов, В. М.;  and Юзюк, Ю. И.\n</span>\n\n  \n\n</span>\n\n  <i>Журнал технической физики</i>, 78(11): 99–103.  2008.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/9548\"\n     onclick=\"log_download('---------2008', 'https://journals.ioffe.ru/articles/9548', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Диэлектрические свойства пленок титаната бария-стронция нанометровой толщины [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---------2008\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---------2008')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2008-5,\n\ttitle = {Диэлектрические свойства пленок титаната бария-стронция нанометровой толщины},\n\tvolume = {78},\n\turl = {https://journals.ioffe.ru/articles/9548},\n\tabstract = {Методами субмиллиметровой и инфракрасной спектроскопии в области частот 10{\\textless}nu{\\textless}3000 cm-1 впервые измерены спектры отражения R(nu) и пропускания T(nu) гетероэпитаксиальных пленок титаната бария-стронция различной толщины на подложках MgO. Путем моделирования экспериментальных спектров френелевскими формулами для слоистых сред определены спектры комплексной диэлектрической проницаемости varepsilon*(nu)=varepsilon&#x27;(nu)+ivarepsilon&#x27;&#x27;(nu) пленок. Показано, что при уменьшении толщины до 10 nm в пленках возникают растягивающие напряжения в направлении, параллельном плоскости подложки, вызывающие возрастание в несколько раз диэлектрического вклада низкочастотной мягкой моды. PACS: 77.22.Ch, 77.22.Gm, 78.20.Ci, 71.28.+d},\n\tlanguage = {ru},\n\tnumber = {11},\n\turldate = {2023-11-11},\n\tjournal = {Журнал технической физики},\n\tauthor = {Мигунов, С. Н. and Волков, А. А. and Командин, Г. А. and Лобанов, А. Н. and Горшунов, Б. П. and Головко, Ю. И. and Мухортов, В. М. and Юзюк, Ю. И.},\n\tyear = {2008},\n\tpages = {99--103},\n\tfile = {Журнал технической физики:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\WZE458EK\\\\9548.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Методами субмиллиметровой и инфракрасной спектроскопии в области частот 10\\textlessnu\\textless3000 cm-1 впервые измерены спектры отражения R(nu) и пропускания T(nu) гетероэпитаксиальных пленок титаната бария-стронция различной толщины на подложках MgO. Путем моделирования экспериментальных спектров френелевскими формулами для слоистых сред определены спектры комплексной диэлектрической проницаемости varepsilon*(nu)=varepsilon'(nu)+ivarepsilon''(nu) пленок. Показано, что при уменьшении толщины до 10 nm в пленках возникают растягивающие напряжения в направлении, параллельном плоскости подложки, вызывающие возрастание в несколько раз диэлектрического вклада низкочастотной мягкой моды. PACS: 77.22.Ch, 77.22.Gm, 78.20.Ci, 71.28.+d\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-------2008\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.elibrary.ru/item.asp?id=9955581\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-------2008', 'https://www.elibrary.ru/item.asp?id=9955581', event);\">\n    Внутренние напряжения и деформационный фазовый переход в наноразмерных пленках титаната бария-стронция.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Мухортов, В. М.; Головко, Ю. И.; Юзюк, Ю. И.; Латуш, Л. Т.; Жигалина, О. М.;  and Кускова, А. Н.\n</span>\n\n  \n\n</span>\n\n  <i>Кристаллография</i>, 53(3): 536–542.  2008.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.elibrary.ru/item.asp?id=9955581\"\n     onclick=\"log_download('-------2008', 'https://www.elibrary.ru/item.asp?id=9955581', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Внутренние напряжения и деформационный фазовый переход в наноразмерных пленках титаната бария-стронция [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-------2008\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-------2008')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2008-6,\n\ttitle = {Внутренние напряжения и деформационный фазовый переход в наноразмерных пленках титаната бария-стронция},\n\tvolume = {53},\n\tissn = {0023-4761},\n\turl = {https://www.elibrary.ru/item.asp?id=9955581},\n\tabstract = {Установлено, что при изменении толщины гетероэпитаксиальных пленок Ba0.8Sr0.2TiO3, выращенных по слоевому механизму роста на подложках (100) MgO, существует критическая толщина пленок ( 50 нм), характерная тем, что внутренние деформационные поля в пленках толщиной ниже критической существенно меньше, чем в пленках толщиной выше критической. При толщине ниже критической имеют место напряжения растяжения, а при больших толщинах – напряжения сжатия. Существование критической толщины подтверждено рентгеноструктурными данными и рамановской спектроскопией.},\n\tlanguage = {ru},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Кристаллография},\n\tauthor = {Мухортов, В. М. and Головко, Ю. И. and Юзюк, Ю. И. and Латуш, Л. Т. and Жигалина, О. М. and Кускова, А. Н.},\n\tyear = {2008},\n\tkeywords = {⛔ No DOI found},\n\tpages = {536--542},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Установлено, что при изменении толщины гетероэпитаксиальных пленок Ba0.8Sr0.2TiO3, выращенных по слоевому механизму роста на подложках (100) MgO, существует критическая толщина пленок ( 50 нм), характерная тем, что внутренние деформационные поля в пленках толщиной ниже критической существенно меньше, чем в пленках толщиной выше критической. При толщине ниже критической имеют место напряжения растяжения, а при больших толщинах – напряжения сжатия. Существование критической толщины подтверждено рентгеноструктурными данными и рамановской спектроскопией.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---2008\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://rusneb.ru/catalog/000199_000009_004241648/\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---2008', 'https://rusneb.ru/catalog/000199_000009_004241648/', event);\">\n    Гетероструктуры на основе наноразмерных сегнетоэлектрических пленок: получение, свойства и применение.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Мухортов, В. М.;  and Юзюк, Ю. И.\n</span>\n\n  \n\n</span>\n\n   2008.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://rusneb.ru/catalog/000199_000009_004241648/\"\n     onclick=\"log_download('---2008', 'https://rusneb.ru/catalog/000199_000009_004241648/', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Гетероструктуры на основе наноразмерных сегнетоэлектрических пленок: получение, свойства и применение [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---2008\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---2008')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@book{__2008-7,\n\ttitle = {Гетероструктуры на основе наноразмерных сегнетоэлектрических пленок: получение, свойства и применение},\n\tisbn = {978-5-902982-42-5},\n\tshorttitle = {Гетероструктуры на основе наноразмерных сегнетоэлектрических пленок},\n\turl = {https://rusneb.ru/catalog/000199_000009_004241648/},\n\tabstract = {«Гетероструктуры на основе наноразмерных сегнетоэлектрических пленок: получение, свойства и применение» (978-5-902982-42-5 (в пер.)) — Мухортов, Владимир Михайлович, 221, [1] с.. Издано: (2008). ✔Читать онлайн. ✔Адрес библиотеки с ближайшим печатным изданием ➤ RusNeb.ru.},\n\tlanguage = {ru},\n\turldate = {2023-11-11},\n\tauthor = {Мухортов, В. М. and Юзюк, Ю. И.},\n\tyear = {2008},\n\tfile = {Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\VMDT5IMU\\\\000199_000009_004241648.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  «Гетероструктуры на основе наноразмерных сегнетоэлектрических пленок: получение, свойства и применение» (978-5-902982-42-5 (в пер.)) — Мухортов, Владимир Михайлович, 221, [1] с.. Издано: (2008). ✔Читать онлайн. ✔Адрес библиотеки с ближайшим печатным изданием ➤ RusNeb.ru.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"k-lorenz-lenzner-ramm-nobis-grundmann-zakharov--etal-znogansi111aunio-2008\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.elibrary.ru/item.asp?id=11036052\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'k-lorenz-lenzner-ramm-nobis-grundmann-zakharov--etal-znogansi111aunio-2008', 'https://www.elibrary.ru/item.asp?id=11036052', event);\">\n    СТРУКТУРА И ОПТИЧЕСКИЕ СВОЙСТВА ZnO-НАНОКРИСТАЛЛОВ, ПОЛУЧЕННЫХ МЕТОДОМ ИМПУЛЬСНОГО ЛАЗЕРНОГО НАПЫЛЕНИЯ НА ПЛЕНКАХ GaN/Si(111) С ИСПОЛЬЗОВАНИЕМ Au- И NiO-КАТАЛИЗАТОРОВ.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kайдашев, E. M.; Lorenz, M.; Lenzner, J.; Ramm, A.; Nobis, T.; Grundmann, M.; Zakharov, N.; Козаков, А. Т.; Шевцова, С. И.; Абдулвахидов, К. Г.;  and Кайдашев, В. Е.\n</span>\n\n  \n\n</span>\n\n  <i>Известия Российской Академии Наук. Серия Физическая</i>, 72(8): 1195–1197.  2008.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.elibrary.ru/item.asp?id=11036052\"\n     onclick=\"log_download('k-lorenz-lenzner-ramm-nobis-grundmann-zakharov--etal-znogansi111aunio-2008', 'https://www.elibrary.ru/item.asp?id=11036052', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"СТРУКТУРА И ОПТИЧЕСКИЕ СВОЙСТВА ZnO-НАНОКРИСТАЛЛОВ, ПОЛУЧЕННЫХ МЕТОДОМ ИМПУЛЬСНОГО ЛАЗЕРНОГО НАПЫЛЕНИЯ НА ПЛЕНКАХ GaN/Si(111) С ИСПОЛЬЗОВАНИЕМ Au- И NiO-КАТАЛИЗАТОРОВ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/k-lorenz-lenzner-ramm-nobis-grundmann-zakharov--etal-znogansi111aunio-2008\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('k-lorenz-lenzner-ramm-nobis-grundmann-zakharov--etal-znogansi111aunio-2008')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{k__2008,\n\ttitle = {{СТРУКТУРА} И ОПТИЧЕСКИЕ СВОЙСТВА {ZnO}-НАНОКРИСТАЛЛОВ, ПОЛУЧЕННЫХ МЕТОДОМ ИМПУЛЬСНОГО ЛАЗЕРНОГО НАПЫЛЕНИЯ НА ПЛЕНКАХ {GaN}/{Si}(111) С ИСПОЛЬЗОВАНИЕМ {Au}- И {NiO}-КАТАЛИЗАТОРОВ},\n\tvolume = {72},\n\tissn = {0367-6765},\n\turl = {https://www.elibrary.ru/item.asp?id=11036052},\n\tabstract = {Исследован рост ZnO-нанокристаллов на пленочном подслое GaN/Si(111) методом импульсного лазерного напыления при высоком давлении аргона с использованием Au- и NiO-катализаторов. Использование низкотемпературного NiO-катализатора позволяет снизить оптимальную температуру роста с 900°C (в случае Au-катализатора) до T = 570°C и вырастить высокоориентированные в направлении оси c решетки ZnO-нанокристаллов диаметром 20 нм полностью свободных от дислокаций.},\n\tlanguage = {ru},\n\tnumber = {8},\n\turldate = {2023-11-11},\n\tjournal = {Известия Российской Академии Наук. Серия Физическая},\n\tauthor = {Kайдашев, E. M. and Lorenz, M. and Lenzner, J. and Ramm, A. and Nobis, T. and Grundmann, M. and Zakharov, N. and Козаков, А. Т. and Шевцова, С. И. and Абдулвахидов, К. Г. and Кайдашев, В. Е.},\n\tyear = {2008},\n\tkeywords = {⛔ No DOI found},\n\tpages = {1195--1197},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследован рост ZnO-нанокристаллов на пленочном подслое GaN/Si(111) методом импульсного лазерного напыления при высоком давлении аргона с использованием Au- и NiO-катализаторов. Использование низкотемпературного NiO-катализатора позволяет снизить оптимальную температуру роста с 900°C (в случае Au-катализатора) до T = 570°C и вырастить высокоориентированные в направлении оси c решетки ZnO-нанокристаллов диаметром 20 нм полностью свободных от дислокаций.\n</div>\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2007\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2007')\"\n      onkeypress=\"toggleGroup('group_2007')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2007</span>\n      <span class=\"bibbase_group_count\">\n        \n        (11)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"wang-novelnanostructuresofznofornanoscalephotonicsoptoelectronicspiezoelectricityandsensing-2007\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://link.springer.com/10.1007/s00339-007-3942-8\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'wang-novelnanostructuresofznofornanoscalephotonicsoptoelectronicspiezoelectricityandsensing-2007', 'http://link.springer.com/10.1007/s00339-007-3942-8', event);\">\n    Novel nanostructures of ZnO for nanoscale photonics, optoelectronics, piezoelectricity, and sensing.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Wang, Z.\n</span>\n\n  \n\n</span>\n\n  <i>Applied Physics A</i>, 88(1): 7–15. May 2007.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://link.springer.com/10.1007/s00339-007-3942-8\"\n     onclick=\"log_download('wang-novelnanostructuresofznofornanoscalephotonicsoptoelectronicspiezoelectricityandsensing-2007', 'http://link.springer.com/10.1007/s00339-007-3942-8', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Novel nanostructures of ZnO for nanoscale photonics, optoelectronics, piezoelectricity, and sensing [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1007/s00339-007-3942-8\"\n     onclick=\"log_download('wang-novelnanostructuresofznofornanoscalephotonicsoptoelectronicspiezoelectricityandsensing-2007', 'http://doi.org/10.1007/s00339-007-3942-8', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/wang-novelnanostructuresofznofornanoscalephotonicsoptoelectronicspiezoelectricityandsensing-2007\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('wang-novelnanostructuresofznofornanoscalephotonicsoptoelectronicspiezoelectricityandsensing-2007')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{wang_novel_2007,\n\ttitle = {Novel nanostructures of {ZnO} for nanoscale photonics, optoelectronics, piezoelectricity, and sensing},\n\tvolume = {88},\n\tissn = {0947-8396, 1432-0630},\n\turl = {http://link.springer.com/10.1007/s00339-007-3942-8},\n\tdoi = {10.1007/s00339-007-3942-8},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Applied Physics A},\n\tauthor = {Wang, Z.L.},\n\tmonth = may,\n\tyear = {2007},\n\tpages = {7--15},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"mishina-zaitsev-ilyin-sherstyuk-sigov-golovko-muhortov-kolesnikov-etal-switchablenonlinearmetalloferroelectricphotoniccrystals-2007\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.2762284\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'mishina-zaitsev-ilyin-sherstyuk-sigov-golovko-muhortov-kolesnikov-etal-switchablenonlinearmetalloferroelectricphotoniccrystals-2007', 'https://doi.org/10.1063/1.2762284', event);\">\n    Switchable nonlinear metalloferroelectric photonic crystals.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Mishina, E.; Zaitsev, A.; Ilyin, N.; Sherstyuk, N.; Sigov, A.; Golovko, Y.; Muhortov, V.; Kolesnikov, A.; Lozovik, Y.; Yemtsova, M.;  and Rasing, T.\n</span>\n\n  \n\n</span>\n\n  <i>Applied Physics Letters</i>, 91(4): 041107. July 2007.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.2762284\"\n     onclick=\"log_download('mishina-zaitsev-ilyin-sherstyuk-sigov-golovko-muhortov-kolesnikov-etal-switchablenonlinearmetalloferroelectricphotoniccrystals-2007', 'https://doi.org/10.1063/1.2762284', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Switchable nonlinear metalloferroelectric photonic crystals [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.2762284\"\n     onclick=\"log_download('mishina-zaitsev-ilyin-sherstyuk-sigov-golovko-muhortov-kolesnikov-etal-switchablenonlinearmetalloferroelectricphotoniccrystals-2007', 'http://doi.org/10.1063/1.2762284', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/mishina-zaitsev-ilyin-sherstyuk-sigov-golovko-muhortov-kolesnikov-etal-switchablenonlinearmetalloferroelectricphotoniccrystals-2007\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('mishina-zaitsev-ilyin-sherstyuk-sigov-golovko-muhortov-kolesnikov-etal-switchablenonlinearmetalloferroelectricphotoniccrystals-2007')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{mishina_switchable_2007,\n\ttitle = {Switchable nonlinear metalloferroelectric photonic crystals},\n\tvolume = {91},\n\tissn = {0003-6951},\n\turl = {https://doi.org/10.1063/1.2762284},\n\tdoi = {10.1063/1.2762284},\n\tabstract = {Two types of low-voltage electroswitchable nonlinear photonic crystals were fabricated providing spatial-frequency control of second harmonic generation radiation of visible light. A two-dimensional photonic crystal was fabricated by focused ion beam etching of a ferroelectric BaSrTiO3 thin film and switched by an electric field applied by an interdigital electrode system, which simultaneously acted as a one-dimensional photonic crystal. The fabricated device operated at a second harmonic wavelength around 400nm with an efficiency incomparably higher than in the case of linear optics.},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Applied Physics Letters},\n\tauthor = {Mishina, E. and Zaitsev, A. and Ilyin, N. and Sherstyuk, N. and Sigov, A. and Golovko, Yu. and Muhortov, V. and Kolesnikov, A. and Lozovik, Yu. and Yemtsova, M. and Rasing, Th.},\n\tmonth = jul,\n\tyear = {2007},\n\tpages = {041107},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\UJII4ECH\\\\Mishina и др. - 2007 - Switchable nonlinear metalloferroelectric photonic.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Two types of low-voltage electroswitchable nonlinear photonic crystals were fabricated providing spatial-frequency control of second harmonic generation radiation of visible light. A two-dimensional photonic crystal was fabricated by focused ion beam etching of a ferroelectric BaSrTiO3 thin film and switched by an electric field applied by an interdigital electrode system, which simultaneously acted as a one-dimensional photonic crystal. The fabricated device operated at a second harmonic wavelength around 400nm with an efficiency incomparably higher than in the case of linear optics.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------2007\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://naukarus.com/fazovraschatel-na-schelevoy-linii-nagruzhennoy-varaktorami-na-osnove-nanorazmernyh-plenok-titanata-bariya-strontsiya\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------2007', 'http://naukarus.com/fazovraschatel-na-schelevoy-linii-nagruzhennoy-varaktorami-na-osnove-nanorazmernyh-plenok-titanata-bariya-strontsiya', event);\">\n    Фазовращатель на щелевой линии, нагруженный варакторами на основе наноразмерных пленок титаната бария-стронция.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Головко, Ю. И.; Масычев, С. И.; Мухортов, В.; Мухортов, В. М.;  and Чуб, А. В.\n</span>\n\n  \n\n</span>\n\n  <i>Радиотехника и электроника</i>, 52(11).  2007.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://naukarus.com/fazovraschatel-na-schelevoy-linii-nagruzhennoy-varaktorami-na-osnove-nanorazmernyh-plenok-titanata-bariya-strontsiya\"\n     onclick=\"log_download('------2007', 'http://naukarus.com/fazovraschatel-na-schelevoy-linii-nagruzhennoy-varaktorami-na-osnove-nanorazmernyh-plenok-titanata-bariya-strontsiya', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Фазовращатель на щелевой линии, нагруженный варакторами на основе наноразмерных пленок титаната бария-стронция [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------2007\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------2007')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2007,\n\ttitle = {Фазовращатель на щелевой линии, нагруженный варакторами на основе наноразмерных пленок титаната бария-стронция},\n\tvolume = {52},\n\tissn = {0033-8494},\n\turl = {http://naukarus.com/fazovraschatel-na-schelevoy-linii-nagruzhennoy-varaktorami-na-osnove-nanorazmernyh-plenok-titanata-bariya-strontsiya},\n\tabstract = {Реализован монолитный фазовращатель на щелевой линии передачи, периодически нагруженной сегнетоэлектрическими варакторами на основе наноразмерных пленок Bа0.8Sr0.2TiO3. Установлено, что при уменьшении толщины наноразмерной сегнетоэлектрической пленки, на основе которой реализованы варакторы, от 36 до 18 нм коэффициент качества фазовращателя в полосе частот от 12 до 13.5 ГГц возрастает более чем в два раза.},\n\tlanguage = {ru},\n\tnumber = {11},\n\turldate = {2023-11-11},\n\tjournal = {Радиотехника и электроника},\n\tauthor = {Головко, Ю. И. and Масычев, С. И. and Мухортов, Вас.М. and Мухортов, Вл. М. and Чуб, А. В.},\n\tyear = {2007},\n\tkeywords = {⛔ No DOI found},\n\tfile = {Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\NC57SS3Z\\\\fazovraschatel-na-schelevoy-linii-nagruzhennoy-varaktorami-na-osnove-nanorazmernyh-plenok-titan.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Реализован монолитный фазовращатель на щелевой линии передачи, периодически нагруженной сегнетоэлектрическими варакторами на основе наноразмерных пленок Bа0.8Sr0.2TiO3. Установлено, что при уменьшении толщины наноразмерной сегнетоэлектрической пленки, на основе которой реализованы варакторы, от 36 до 18 нм коэффициент качества фазовращателя в полосе частот от 12 до 13.5 ГГц возрастает более чем в два раза.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"katiyar-yuzyuk-stressmanipulationinferroelectricthinfilmsandsuperlattices-2007\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0924203107000537\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'katiyar-yuzyuk-stressmanipulationinferroelectricthinfilmsandsuperlattices-2007', 'https://www.sciencedirect.com/science/article/pii/S0924203107000537', event);\">\n    Stress manipulation in ferroelectric thin films and superlattices.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Katiyar, R. S.;  and Yuzyuk, Y. I.\n</span>\n\n  \n\n</span>\n\n  <i>Vibrational Spectroscopy</i>, 45(2): 108–111. November 2007.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0924203107000537\"\n     onclick=\"log_download('katiyar-yuzyuk-stressmanipulationinferroelectricthinfilmsandsuperlattices-2007', 'https://www.sciencedirect.com/science/article/pii/S0924203107000537', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Stress manipulation in ferroelectric thin films and superlattices [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.vibspec.2007.05.004\"\n     onclick=\"log_download('katiyar-yuzyuk-stressmanipulationinferroelectricthinfilmsandsuperlattices-2007', 'http://doi.org/10.1016/j.vibspec.2007.05.004', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/katiyar-yuzyuk-stressmanipulationinferroelectricthinfilmsandsuperlattices-2007\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('katiyar-yuzyuk-stressmanipulationinferroelectricthinfilmsandsuperlattices-2007')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{katiyar_stress_2007,\n\tseries = {Raman {Spectroscopy} {Workshop} 2006},\n\ttitle = {Stress manipulation in ferroelectric thin films and superlattices},\n\tvolume = {45},\n\tissn = {0924-2031},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0924203107000537},\n\tdoi = {10.1016/j.vibspec.2007.05.004},\n\tabstract = {The integration of ferroelectric oxides into microelectronic devices requires a better understanding of stress and size effects onto ferroelectric properties of epitaxial thin films and superlattices which are generally imposed by the underlying substrate due to misfits in their lattice parameters and their thermal expansion coefficients. We have utilized polarized micro-Raman spectroscopy to investigate such stress effects in epitaxially grown Ba0.7Sr0.3TiO3 (BST-0.3) thin films and BaTiO3/SrTiO3 (BT/ST) superlattices with different periodicities as a function of temperature. In BST-0.3 films, the mismatch of the thermal expansion coefficients of the film and the substrate induces significant two-dimensional (2D) clamping and governs the domain structure formation. Moreover, the 2D stresses increase the Curie temperature remarkably and even change the phase-transition sequence in thin films, creating new phases, which were never observed in bulk materials. It is shown that in the epitaxial BST-0.3 films and BT/ST superlattices the E(TO) soft mode is very sensitive internal probe of 2D clamping and can be used for precise characterization.},\n\tlanguage = {en},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Vibrational Spectroscopy},\n\tauthor = {Katiyar, R. S. and Yuzyuk, Yu. I.},\n\tmonth = nov,\n\tyear = {2007},\n\tkeywords = {Ferroelectrics, Raman spectroscopy, Superlattices},\n\tpages = {108--111},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The integration of ferroelectric oxides into microelectronic devices requires a better understanding of stress and size effects onto ferroelectric properties of epitaxial thin films and superlattices which are generally imposed by the underlying substrate due to misfits in their lattice parameters and their thermal expansion coefficients. We have utilized polarized micro-Raman spectroscopy to investigate such stress effects in epitaxially grown Ba0.7Sr0.3TiO3 (BST-0.3) thin films and BaTiO3/SrTiO3 (BT/ST) superlattices with different periodicities as a function of temperature. In BST-0.3 films, the mismatch of the thermal expansion coefficients of the film and the substrate induces significant two-dimensional (2D) clamping and governs the domain structure formation. Moreover, the 2D stresses increase the Curie temperature remarkably and even change the phase-transition sequence in thin films, creating new phases, which were never observed in bulk materials. It is shown that in the epitaxial BST-0.3 films and BT/ST superlattices the E(TO) soft mode is very sensitive internal probe of 2D clamping and can be used for precise characterization.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"mishina-sherstyuk-golovko-muhortov-sigov-polarizationswitchinginferroelectricthinfilmsstudiedbyopticalsecondharmonicgeneration-2007\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/10584580701746913\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'mishina-sherstyuk-golovko-muhortov-sigov-polarizationswitchinginferroelectricthinfilmsstudiedbyopticalsecondharmonicgeneration-2007', 'https://doi.org/10.1080/10584580701746913', event);\">\n    Polarization Switching in Ferroelectric Thin Films Studied by Optical Second Harmonic Generation.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Mishina, E.; Sherstyuk, N.; Golovko, Y.; Muhortov, V.;  and Sigov, A.\n</span>\n\n  \n\n</span>\n\n  <i>Integrated Ferroelectrics</i>, 92(1): 65–76. December 2007.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/10584580701746913</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/10584580701746913\"\n     onclick=\"log_download('mishina-sherstyuk-golovko-muhortov-sigov-polarizationswitchinginferroelectricthinfilmsstudiedbyopticalsecondharmonicgeneration-2007', 'https://doi.org/10.1080/10584580701746913', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Polarization Switching in Ferroelectric Thin Films Studied by Optical Second Harmonic Generation [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/10584580701746913\"\n     onclick=\"log_download('mishina-sherstyuk-golovko-muhortov-sigov-polarizationswitchinginferroelectricthinfilmsstudiedbyopticalsecondharmonicgeneration-2007', 'http://doi.org/10.1080/10584580701746913', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/mishina-sherstyuk-golovko-muhortov-sigov-polarizationswitchinginferroelectricthinfilmsstudiedbyopticalsecondharmonicgeneration-2007\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('mishina-sherstyuk-golovko-muhortov-sigov-polarizationswitchinginferroelectricthinfilmsstudiedbyopticalsecondharmonicgeneration-2007')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{mishina_polarization_2007,\n\ttitle = {Polarization {Switching} in {Ferroelectric} {Thin} {Films} {Studied} by {Optical} {Second} {Harmonic} {Generation}},\n\tvolume = {92},\n\tissn = {1058-4587},\n\turl = {https://doi.org/10.1080/10584580701746913},\n\tdoi = {10.1080/10584580701746913},\n\tabstract = {Domain configuration during polarization switching in ferroelectric thin films was studied by optical second harmonic generation on different time scales: quasistatic (0.1 Hz), low-frequency (0.1–1 kHz) and fast (0.1 GHz). It is shown that within the electric pulses of several tenth of nanoseconds domain configuration may be different from the equilibrium.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Integrated Ferroelectrics},\n\tauthor = {Mishina, Elena and Sherstyuk, Nataliya and Golovko, Yurii and Muhortov, Vladimir and Sigov, Alexandr},\n\tmonth = dec,\n\tyear = {2007},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/10584580701746913},\n\tpages = {65--76},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Domain configuration during polarization switching in ferroelectric thin films was studied by optical second harmonic generation on different time scales: quasistatic (0.1 Hz), low-frequency (0.1–1 kHz) and fast (0.1 GHz). It is shown that within the electric pulses of several tenth of nanoseconds domain configuration may be different from the equilibrium.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"shirokov-yuzyuk-dkhil-lemanov-phenomenologicaltheoryofphasetransitionsinepitaxialbatiotextrm3thinfilms-2007\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.75.224116\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'shirokov-yuzyuk-dkhil-lemanov-phenomenologicaltheoryofphasetransitionsinepitaxialbatiotextrm3thinfilms-2007', 'https://link.aps.org/doi/10.1103/PhysRevB.75.224116', event);\">\n    Phenomenological theory of phase transitions in epitaxial BaTiO$_{\\textrm{3}}$ thin films.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Shirokov, V. B.; Yuzyuk, Y. I.; Dkhil, B.;  and Lemanov, V. V.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 75(22): 224116. June 2007.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.75.224116\"\n     onclick=\"log_download('shirokov-yuzyuk-dkhil-lemanov-phenomenologicaltheoryofphasetransitionsinepitaxialbatiotextrm3thinfilms-2007', 'https://link.aps.org/doi/10.1103/PhysRevB.75.224116', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Phenomenological theory of phase transitions in epitaxial BaTiO$_{\\textrm{3}}$ thin films [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.75.224116\"\n     onclick=\"log_download('shirokov-yuzyuk-dkhil-lemanov-phenomenologicaltheoryofphasetransitionsinepitaxialbatiotextrm3thinfilms-2007', 'http://doi.org/10.1103/PhysRevB.75.224116', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/shirokov-yuzyuk-dkhil-lemanov-phenomenologicaltheoryofphasetransitionsinepitaxialbatiotextrm3thinfilms-2007\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('shirokov-yuzyuk-dkhil-lemanov-phenomenologicaltheoryofphasetransitionsinepitaxialbatiotextrm3thinfilms-2007')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{shirokov_phenomenological_2007,\n\ttitle = {Phenomenological theory of phase transitions in epitaxial {BaTiO}$_{\\textrm{3}}$ thin films},\n\tvolume = {75},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.75.224116},\n\tdoi = {10.1103/PhysRevB.75.224116},\n\tabstract = {We develop a phenomenological thermodynamic theory of ferroelectric BaTiO3 (BT) thin films epitaxially grown on cubic substrates using the Landau-Devonshire eight-order potential. The constructed “misfit-temperature” phase diagram is asymmetrical. We found that the overall view of the phase diagram depends on the values of compliances used in calculations and we provide two qualitatively different diagrams. A thermodynamic path for BT film grown onto a particular substrate can be found using a plot of the room-temperature tetragonal distortion (c−a)∕a as a function of misfit strain.},\n\tlanguage = {en},\n\tnumber = {22},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Shirokov, V. B. and Yuzyuk, Yu. I. and Dkhil, B. and Lemanov, V. V.},\n\tmonth = jun,\n\tyear = {2007},\n\tnote = {Publisher: American Physical Society},\n\tpages = {224116},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We develop a phenomenological thermodynamic theory of ferroelectric BaTiO3 (BT) thin films epitaxially grown on cubic substrates using the Landau-Devonshire eight-order potential. The constructed “misfit-temperature” phase diagram is asymmetrical. We found that the overall view of the phase diagram depends on the values of compliances used in calculations and we provide two qualitatively different diagrams. A thermodynamic path for BT film grown onto a particular substrate can be found using a plot of the room-temperature tetragonal distortion (c−a)∕a as a function of misfit strain.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"ankiewicz-carmo-sobolev-gehlhoff-kaidashev-rahm-lorenz-grundmann-electronparamagneticresonanceintransitionmetaldopedznonanowires-2007\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.2402095\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'ankiewicz-carmo-sobolev-gehlhoff-kaidashev-rahm-lorenz-grundmann-electronparamagneticresonanceintransitionmetaldopedznonanowires-2007', 'https://doi.org/10.1063/1.2402095', event);\">\n    Electron paramagnetic resonance in transition metal-doped ZnO nanowires.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Ankiewicz, A. O.; Carmo, M. C.; Sobolev, N. A.; Gehlhoff, W.; Kaidashev, E. M.; Rahm, A.; Lorenz, M.;  and Grundmann, M.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Applied Physics</i>, 101(2): 024324. January 2007.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.2402095\"\n     onclick=\"log_download('ankiewicz-carmo-sobolev-gehlhoff-kaidashev-rahm-lorenz-grundmann-electronparamagneticresonanceintransitionmetaldopedznonanowires-2007', 'https://doi.org/10.1063/1.2402095', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Electron paramagnetic resonance in transition metal-doped ZnO nanowires [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.2402095\"\n     onclick=\"log_download('ankiewicz-carmo-sobolev-gehlhoff-kaidashev-rahm-lorenz-grundmann-electronparamagneticresonanceintransitionmetaldopedznonanowires-2007', 'http://doi.org/10.1063/1.2402095', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/ankiewicz-carmo-sobolev-gehlhoff-kaidashev-rahm-lorenz-grundmann-electronparamagneticresonanceintransitionmetaldopedznonanowires-2007\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('ankiewicz-carmo-sobolev-gehlhoff-kaidashev-rahm-lorenz-grundmann-electronparamagneticresonanceintransitionmetaldopedznonanowires-2007')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{ankiewicz_electron_2007,\n\ttitle = {Electron paramagnetic resonance in transition metal-doped {ZnO} nanowires},\n\tvolume = {101},\n\tissn = {0021-8979},\n\turl = {https://doi.org/10.1063/1.2402095},\n\tdoi = {10.1063/1.2402095},\n\tabstract = {The wide-band-gap zinc oxide-based diluted magnetic semiconductors currently attract considerable attention due to their possible use in spintronic devices. In this work, we studied ZnO nanowire samples synthesized on 10×10 mm2 a-plane sapphire substrates by high-pressure pulsed laser deposition. The samples were characterized by scanning electron microscopy (SEM) and electron paramagnetic resonance (EPR) in the X-band (≃9.3 GHz) from T=4 to 300 K. According to the SEM pictures, the nanowires exhibit a length of about 1 μm and are aligned perpendicular to the substrate surface. The structures have a hexagonal cross section and their diameter ranges from 60 nm up to 150 nm. For the lowest nominal concentrations of xMn=3 at. \\% and xCo=5 at. \\%, we detect the anisotropic EPR spectra of isolated Mn2+ (3d5, S6) and Co2+ (3d7, F4), respectively, on Zn sites. The detection of the well-resolved anisotropic spectra proves a coherent crystallographic orientation of the nanowires. The linewidth was larger than the best values reported in the literature. Nevertheless, it was possible to identify two different components, A and B, of the reported spectra. From the temperature dependence of the EPR intensity, we found that both components exhibit paramagnetic behavior and are present in a concentration ratio of NB∕NA=1.4. In the case of the Mn-doped ZnO wires, the linewidth increases with increasing Mn concentration due to the dipole-dipole interaction of the paramagnetic ions. At the highest used nominal concentration, xMn=10 at. \\%, an additional broad single line is observed.},\n\tlanguage = {en},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Applied Physics},\n\tauthor = {Ankiewicz, A. O. and Carmo, M. C. and Sobolev, N. A. and Gehlhoff, W. and Kaidashev, E. M. and Rahm, A. and Lorenz, M. and Grundmann, M.},\n\tmonth = jan,\n\tyear = {2007},\n\tpages = {024324},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The wide-band-gap zinc oxide-based diluted magnetic semiconductors currently attract considerable attention due to their possible use in spintronic devices. In this work, we studied ZnO nanowire samples synthesized on 10×10 mm2 a-plane sapphire substrates by high-pressure pulsed laser deposition. The samples were characterized by scanning electron microscopy (SEM) and electron paramagnetic resonance (EPR) in the X-band (≃9.3 GHz) from T=4 to 300 K. According to the SEM pictures, the nanowires exhibit a length of about 1 μm and are aligned perpendicular to the substrate surface. The structures have a hexagonal cross section and their diameter ranges from 60 nm up to 150 nm. For the lowest nominal concentrations of xMn=3 at. % and xCo=5 at. %, we detect the anisotropic EPR spectra of isolated Mn2+ (3d5, S6) and Co2+ (3d7, F4), respectively, on Zn sites. The detection of the well-resolved anisotropic spectra proves a coherent crystallographic orientation of the nanowires. The linewidth was larger than the best values reported in the literature. Nevertheless, it was possible to identify two different components, A and B, of the reported spectra. From the temperature dependence of the EPR intensity, we found that both components exhibit paramagnetic behavior and are present in a concentration ratio of NB∕NA=1.4. In the case of the Mn-doped ZnO wires, the linewidth increases with increasing Mn concentration due to the dipole-dipole interaction of the paramagnetic ions. At the highest used nominal concentration, xMn=10 at. %, an additional broad single line is observed.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-------2007\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/9249\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-------2007', 'https://journals.ioffe.ru/articles/9249', event);\">\n    Геометрические эффекты в наноразмерных эпитаксиальных пленках титаната бария-стронция.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Мухортов, В. М.; Колесников, В. В.; Головко, Ю. И.; Бирюков, С. В.; Маматов, А. А.;  and Юзюк, Ю. И.\n</span>\n\n  \n\n</span>\n\n  <i>Журнал технической физики</i>, 77(10): 97–102.  2007.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/9249\"\n     onclick=\"log_download('-------2007', 'https://journals.ioffe.ru/articles/9249', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Геометрические эффекты в наноразмерных эпитаксиальных пленках титаната бария-стронция [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-------2007\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-------2007')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2007-1,\n\ttitle = {Геометрические эффекты в наноразмерных эпитаксиальных пленках титаната бария-стронция},\n\tvolume = {77},\n\turl = {https://journals.ioffe.ru/articles/9249},\n\tabstract = {Исследованы наноразмерные (6−950 nm) эпитаксиальные пленки Ba0.8Sr0.2TiO3 на (001) MgO с целью\nизучения влияния толщины пленки на особенности проявления сегнетоэлектрических свойств. Данные\nкомбинационного рассеяния света и рентгеновской дифрактометрии показывают, что при толщине пленки\n∼ 70 nm происходит структурный фазовый переход, при котором резко изменяются параметры решетки\nпленки.\nСпектры комбинационного рассеяния света наноразмерных пленок подтвердили наличие в них сегне тоэлектрического состояния и изменение симметрии при переходе пленок через критическую толщину,\nчто проявилось в резком смещении пиков, соответствующих A1 (TO) и E (TO) компонентам мягкой\nмоды. В области толщины пленок {\\textless} 100 nm в зависимости диэлектрической проницаемости от толщины\nпоявляются два максимума при толщине ∼ 18 и ∼ 36 nm. Диэлектрическая нелинейность в области первого\nмаксимума существенно больше, чем в области второго.},\n\tlanguage = {ru},\n\tnumber = {10},\n\turldate = {2023-11-11},\n\tjournal = {Журнал технической физики},\n\tauthor = {Мухортов, В. М. and Колесников, В. В. and Головко, Ю. И. and Бирюков, С. В. and Маматов, А. А. and Юзюк, Ю. И.},\n\tyear = {2007},\n\tkeywords = {⛔ No DOI found},\n\tpages = {97--102},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Исследованы наноразмерные (6−950 nm) эпитаксиальные пленки Ba0.8Sr0.2TiO3 на (001) MgO с целью изучения влияния толщины пленки на особенности проявления сегнетоэлектрических свойств. Данные комбинационного рассеяния света и рентгеновской дифрактометрии показывают, что при толщине пленки ∼ 70 nm происходит структурный фазовый переход, при котором резко изменяются параметры решетки пленки. Спектры комбинационного рассеяния света наноразмерных пленок подтвердили наличие в них сегне тоэлектрического состояния и изменение симметрии при переходе пленок через критическую толщину, что проявилось в резком смещении пиков, соответствующих A1 (TO) и E (TO) компонентам мягкой моды. В области толщины пленок \\textless 100 nm в зависимости диэлектрической проницаемости от толщины появляются два максимума при толщине ∼ 18 и ∼ 36 nm. Диэлектрическая нелинейность в области первого максимума существенно больше, чем в области второго.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------simon--2007\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/3167\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------simon--2007', 'https://journals.ioffe.ru/articles/3167', event);\">\n    Влияние механизма роста и термоупругих напряжений на динамику кристаллической решетки гетероэпитаксиальных пленок титаната бария-стронция.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Юзюк, Ю. И.; Захарченко, И. Н.; Алёшин, В. А.; Леонтьев, И. Н.; Рабкин, Л. М.; Мухортов, В. М.;  and Simon, P.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 49(9): 1676–1682.  2007.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/3167\"\n     onclick=\"log_download('------simon--2007', 'https://journals.ioffe.ru/articles/3167', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Влияние механизма роста и термоупругих напряжений на динамику кристаллической решетки гетероэпитаксиальных пленок титаната бария-стронция [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------simon--2007\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------simon--2007')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2007-2,\n\ttitle = {Влияние механизма роста и термоупругих напряжений на динамику кристаллической решетки гетероэпитаксиальных пленок титаната бария-стронция},\n\tvolume = {49},\n\turl = {https://journals.ioffe.ru/articles/3167},\n\tlanguage = {ru},\n\tnumber = {9},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Юзюк, Ю. И. and Захарченко, И. Н. and Алёшин, В. А. and Леонтьев, И. Н. and Рабкин, Л. М. and Мухортов, В. М. and Simon, P.},\n\tyear = {2007},\n\tkeywords = {⛔ No DOI found},\n\tpages = {1676--1682},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-------bifeotextrm3-2007\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.elibrary.ru/item.asp?id=11693334\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-------bifeotextrm3-2007', 'https://www.elibrary.ru/item.asp?id=11693334', event);\">\n    Магнитоэлектрические и нелинейно-оптические свойства пленок BiFeO$_{\\textrm{3}}$, допированных неодимом.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Кузнецов, М. А.; Мишина, Е. Д.; Морозов, А. И.; Сигов, А. С.; Головко, Ю. И.; Мухортов, В. М.;  and Мошняга, В. Т.\n</span>\n\n  \n\n</span>\n\n  <i>Нано- И Микросистемная Техника</i>, (12): 20–22.  2007.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.elibrary.ru/item.asp?id=11693334\"\n     onclick=\"log_download('-------bifeotextrm3-2007', 'https://www.elibrary.ru/item.asp?id=11693334', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Магнитоэлектрические и нелинейно-оптические свойства пленок BiFeO$_{\\textrm{3}}$, допированных неодимом [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-------bifeotextrm3-2007\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-------bifeotextrm3-2007')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2007-3,\n\ttitle = {Магнитоэлектрические и нелинейно-оптические свойства пленок {BiFeO}$_{\\textrm{3}}$, допированных неодимом},\n\tissn = {1813-8586},\n\turl = {https://www.elibrary.ru/item.asp?id=11693334},\n\tabstract = {Методом магнетронного распыления получены мо-нокристаллические и поликристаллические пленки фер-рита висмута. Показано, что монокристаллические пленки обладают высокими значениями остаточной по-ляризации и намагниченности насыщения. Наличие маг-нитоэлектрического взаимодействия подтверждено нели-нейно-оптическими измерениями.},\n\tlanguage = {ru},\n\tnumber = {12},\n\turldate = {2023-11-11},\n\tjournal = {Нано- И Микросистемная Техника},\n\tauthor = {Кузнецов, М. А. and Мишина, Е. Д. and Морозов, А. И. and Сигов, А. С. and Головко, Ю. И. and Мухортов, В. М. and Мошняга, В. Т.},\n\tyear = {2007},\n\tkeywords = {⛔ No DOI found},\n\tpages = {20--22},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Методом магнетронного распыления получены мо-нокристаллические и поликристаллические пленки фер-рита висмута. Показано, что монокристаллические пленки обладают высокими значениями остаточной по-ляризации и намагниченности насыщения. Наличие маг-нитоэлектрического взаимодействия подтверждено нели-нейно-оптическими измерениями.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"yuzyuk-simon-zakharchenko-alyoshin-leontyev-mukhortov-stressalterationinheteroepitaxialbasrtiotextrm3001mgothinfilmsviagrowthmechanism-2007\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://dx.doi.org/10.1088/0022-3727/40/14/025\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'yuzyuk-simon-zakharchenko-alyoshin-leontyev-mukhortov-stressalterationinheteroepitaxialbasrtiotextrm3001mgothinfilmsviagrowthmechanism-2007', 'https://dx.doi.org/10.1088/0022-3727/40/14/025', event);\">\n    Stress alteration in heteroepitaxial (Ba,Sr)TiO$_{\\textrm{3}}$/(001) MgO thin films via growth mechanism.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Yuzyuk, Y. I.; Simon, P.; Zakharchenko, I. N.; Alyoshin, V. A.; Leontyev, I. N.;  and Mukhortov, V. M.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Physics D: Applied Physics</i>, 40(14): 4271. June 2007.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://dx.doi.org/10.1088/0022-3727/40/14/025\"\n     onclick=\"log_download('yuzyuk-simon-zakharchenko-alyoshin-leontyev-mukhortov-stressalterationinheteroepitaxialbasrtiotextrm3001mgothinfilmsviagrowthmechanism-2007', 'https://dx.doi.org/10.1088/0022-3727/40/14/025', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Stress alteration in heteroepitaxial (Ba,Sr)TiO$_{\\textrm{3}}$/(001) MgO thin films via growth mechanism [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1088/0022-3727/40/14/025\"\n     onclick=\"log_download('yuzyuk-simon-zakharchenko-alyoshin-leontyev-mukhortov-stressalterationinheteroepitaxialbasrtiotextrm3001mgothinfilmsviagrowthmechanism-2007', 'http://doi.org/10.1088/0022-3727/40/14/025', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/yuzyuk-simon-zakharchenko-alyoshin-leontyev-mukhortov-stressalterationinheteroepitaxialbasrtiotextrm3001mgothinfilmsviagrowthmechanism-2007\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('yuzyuk-simon-zakharchenko-alyoshin-leontyev-mukhortov-stressalterationinheteroepitaxialbasrtiotextrm3001mgothinfilmsviagrowthmechanism-2007')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{yuzyuk_stress_2007,\n\ttitle = {Stress alteration in heteroepitaxial ({Ba},{Sr}){TiO}$_{\\textrm{3}}$/(001) {MgO} thin films via growth mechanism},\n\tvolume = {40},\n\tissn = {0022-3727},\n\turl = {https://dx.doi.org/10.1088/0022-3727/40/14/025},\n\tdoi = {10.1088/0022-3727/40/14/025},\n\tabstract = {We have studied stress effects in heteroepitaxial (Ba0.7Sr0.3)TiO3 thin films deposited by rf sputtering on (0 0 1) MgO substrates. By varying the deposition conditions, three-dimensional (3D) nucleation growth and layer-by-layer growth mechanisms were realized. X-ray diffraction (XRD) measurements revealed that tetragonal distortion and Curie temperature (Tc) depend on the growth mechanism. The frequency of the E(TO) soft mode in the polarized Raman spectra correlated with the value of two-dimensional stress, determined from XRD experiments. Temperature-dependent lattice parameters and Raman spectra revealed an upward shift of the Curie temperature. Two-dimensional compressive stress was found to be larger in the film grown by the 3D nucleation mechanism.},\n\tlanguage = {en},\n\tnumber = {14},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Physics D: Applied Physics},\n\tauthor = {Yuzyuk, Yu I. and Simon, P. and Zakharchenko, I. N. and Alyoshin, V. A. and Leontyev, I. N. and Mukhortov, V. M.},\n\tmonth = jun,\n\tyear = {2007},\n\tpages = {4271},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We have studied stress effects in heteroepitaxial (Ba0.7Sr0.3)TiO3 thin films deposited by rf sputtering on (0 0 1) MgO substrates. By varying the deposition conditions, three-dimensional (3D) nucleation growth and layer-by-layer growth mechanisms were realized. X-ray diffraction (XRD) measurements revealed that tetragonal distortion and Curie temperature (Tc) depend on the growth mechanism. The frequency of the E(TO) soft mode in the polarized Raman spectra correlated with the value of two-dimensional stress, determined from XRD experiments. Temperature-dependent lattice parameters and Raman spectra revealed an upward shift of the Curie temperature. Two-dimensional compressive stress was found to be larger in the film grown by the 3D nucleation mechanism.\n</div>\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2006\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2006')\"\n      onkeypress=\"toggleGroup('group_2006')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2006</span>\n      <span class=\"bibbase_group_count\">\n        \n        (7)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"rahm-kaidashev-schmidt-diaconu-pppl-bttcher-meinecke-butz-etal-growthandcharacterizationofmnandcodopedznonanowires-2006\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1007/s00604-006-0602-1\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'rahm-kaidashev-schmidt-diaconu-pppl-bttcher-meinecke-butz-etal-growthandcharacterizationofmnandcodopedznonanowires-2006', 'https://doi.org/10.1007/s00604-006-0602-1', event);\">\n    Growth and characterization of Mn- and Co-doped ZnO nanowires.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Rahm, A.; Kaidashev, E. M.; Schmidt, H.; Diaconu, M.; Pöppl, A.; Böttcher, R.; Meinecke, C.; Butz, T.; Lorenz, M.;  and Grundmann, M.\n</span>\n\n  \n\n</span>\n\n  <i>Microchimica Acta</i>, 156(1): 21–25. November 2006.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1007/s00604-006-0602-1\"\n     onclick=\"log_download('rahm-kaidashev-schmidt-diaconu-pppl-bttcher-meinecke-butz-etal-growthandcharacterizationofmnandcodopedznonanowires-2006', 'https://doi.org/10.1007/s00604-006-0602-1', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Growth and characterization of Mn- and Co-doped ZnO nanowires [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1007/s00604-006-0602-1\"\n     onclick=\"log_download('rahm-kaidashev-schmidt-diaconu-pppl-bttcher-meinecke-butz-etal-growthandcharacterizationofmnandcodopedznonanowires-2006', 'http://doi.org/10.1007/s00604-006-0602-1', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/rahm-kaidashev-schmidt-diaconu-pppl-bttcher-meinecke-butz-etal-growthandcharacterizationofmnandcodopedznonanowires-2006\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('rahm-kaidashev-schmidt-diaconu-pppl-bttcher-meinecke-butz-etal-growthandcharacterizationofmnandcodopedznonanowires-2006')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{rahm_growth_2006,\n\ttitle = {Growth and characterization of {Mn}- and {Co}-doped {ZnO} nanowires},\n\tvolume = {156},\n\tissn = {1436-5073},\n\turl = {https://doi.org/10.1007/s00604-006-0602-1},\n\tdoi = {10.1007/s00604-006-0602-1},\n\tabstract = {We report on the high-pressure pulsed laser deposition growth of zinc oxide nanowires containing about 0.2 at.\\% Co and 0.5 at.\\% Mn by NiO and Au catalyst. Scanning electron microscopy and X-ray diffraction measurements revealed arrays of parallel-standing nanowires with hexagonal cross section and uniform in-plane epitaxial relations without rotational domains. Elemental analysis was carried out using particle induced X-ray emission and Q-band electron spin resonance. The valence of the incorporated Mn was determined to be 2+. Atomic and magnetic force microscopy measurements indicate that Mn is incorporated preferentially at the nanowire boundaries.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Microchimica Acta},\n\tauthor = {Rahm, Andreas and Kaidashev, Evgeni M. and Schmidt, Heidemarie and Diaconu, Mariana and Pöppl, Andreas and Böttcher, Rolf and Meinecke, Christoph and Butz, Tilman and Lorenz, Michael and Grundmann, Marius},\n\tmonth = nov,\n\tyear = {2006},\n\tkeywords = {Key words: Zinc oxide; pulsed laser deposition; nanowire; transition metal.},\n\tpages = {21--25},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We report on the high-pressure pulsed laser deposition growth of zinc oxide nanowires containing about 0.2 at.% Co and 0.5 at.% Mn by NiO and Au catalyst. Scanning electron microscopy and X-ray diffraction measurements revealed arrays of parallel-standing nanowires with hexagonal cross section and uniform in-plane epitaxial relations without rotational domains. Elemental analysis was carried out using particle induced X-ray emission and Q-band electron spin resonance. The valence of the incorporated Mn was determined to be 2+. Atomic and magnetic force microscopy measurements indicate that Mn is incorporated preferentially at the nanowire boundaries.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----2006\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://cyberleninka.ru/article/n/novyy-datchik-dinamicheskoy-deformatsii-na-osnove-tonkih-piezoelektricheskih-plenok-poluchennyh-ionnoplazmennym-napyleniem\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----2006', 'https://cyberleninka.ru/article/n/novyy-datchik-dinamicheskoy-deformatsii-na-osnove-tonkih-piezoelektricheskih-plenok-poluchennyh-ionnoplazmennym-napyleniem', event);\">\n    Новый датчик динамической деформации на основе тонких пьезоэлектрических пленок, полученных ионноплазменным напылением.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Мухортов, В. М.; Мухортов, В.;  and Бирюков, С. В.\n</span>\n\n  \n\n</span>\n\n  <i>Известия Южного федерального университета. Технические науки</i>, 58(3): 221–227.  2006.\n  <span class=\"note\">Number: 3 Place: Россия, Ростов-на-Дону Publisher: Федеральное государственное автономное образовательное учреждение высшего образования «Южный федеральный университет»</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://cyberleninka.ru/article/n/novyy-datchik-dinamicheskoy-deformatsii-na-osnove-tonkih-piezoelektricheskih-plenok-poluchennyh-ionnoplazmennym-napyleniem\"\n     onclick=\"log_download('----2006', 'https://cyberleninka.ru/article/n/novyy-datchik-dinamicheskoy-deformatsii-na-osnove-tonkih-piezoelektricheskih-plenok-poluchennyh-ionnoplazmennym-napyleniem', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Новый датчик динамической деформации на основе тонких пьезоэлектрических пленок, полученных ионноплазменным напылением [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----2006\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----2006')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2006,\n\ttitle = {Новый датчик динамической деформации на основе тонких пьезоэлектрических пленок, полученных ионноплазменным напылением},\n\tvolume = {58},\n\tissn = {1999-9429},\n\turl = {https://cyberleninka.ru/article/n/novyy-datchik-dinamicheskoy-deformatsii-na-osnove-tonkih-piezoelektricheskih-plenok-poluchennyh-ionnoplazmennym-napyleniem},\n\tlanguage = {ru},\n\tnumber = {3},\n\turldate = {2023-11-11},\n\tjournal = {Известия Южного федерального университета. Технические науки},\n\tauthor = {Мухортов, Вл. М. and Мухортов, Вас.М. and Бирюков, С. В.},\n\tyear = {2006},\n\tnote = {Number: 3\nPlace: Россия, Ростов-на-Дону\nPublisher: Федеральное государственное автономное образовательное учреждение высшего образования «Южный федеральный университет»},\n\tkeywords = {⛔ No DOI found},\n\tpages = {221--227},\n\tfile = {Full Text PDF:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\D4V7B898\\\\В.м и др. - 2006 - Новый датчик динамической деформации на основе тон.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"deguerville-elmarssi-raevski-karkut-yuzyuk-softmodedynamicsandthereductionoftitextrm4disorderinferroelectricrelaxorsuperlatticesbatiotextrm3batitextrm068zrtextrm032otextrm3-2006\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.74.064107\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'deguerville-elmarssi-raevski-karkut-yuzyuk-softmodedynamicsandthereductionoftitextrm4disorderinferroelectricrelaxorsuperlatticesbatiotextrm3batitextrm068zrtextrm032otextrm3-2006', 'https://link.aps.org/doi/10.1103/PhysRevB.74.064107', event);\">\n    Soft mode dynamics and the reduction of Ti$^{\\textrm{4+}}$ disorder in ferroelectric∕relaxor superlattices BaTiO$_{\\textrm{3}}$ / BaTi$_{\\textrm{0.68}}$Zr$_{\\textrm{0.32}}$O$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  De Guerville, F.; El Marssi, M.; Raevski, I. P.; Karkut, M. G.;  and Yuzyuk, Y. I.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 74(6): 064107. August 2006.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.74.064107\"\n     onclick=\"log_download('deguerville-elmarssi-raevski-karkut-yuzyuk-softmodedynamicsandthereductionoftitextrm4disorderinferroelectricrelaxorsuperlatticesbatiotextrm3batitextrm068zrtextrm032otextrm3-2006', 'https://link.aps.org/doi/10.1103/PhysRevB.74.064107', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Soft mode dynamics and the reduction of Ti$^{\\textrm{4+}}$ disorder in ferroelectric∕relaxor superlattices BaTiO$_{\\textrm{3}}$ / BaTi$_{\\textrm{0.68}}$Zr$_{\\textrm{0.32}}$O$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.74.064107\"\n     onclick=\"log_download('deguerville-elmarssi-raevski-karkut-yuzyuk-softmodedynamicsandthereductionoftitextrm4disorderinferroelectricrelaxorsuperlatticesbatiotextrm3batitextrm068zrtextrm032otextrm3-2006', 'http://doi.org/10.1103/PhysRevB.74.064107', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/deguerville-elmarssi-raevski-karkut-yuzyuk-softmodedynamicsandthereductionoftitextrm4disorderinferroelectricrelaxorsuperlatticesbatiotextrm3batitextrm068zrtextrm032otextrm3-2006\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('deguerville-elmarssi-raevski-karkut-yuzyuk-softmodedynamicsandthereductionoftitextrm4disorderinferroelectricrelaxorsuperlatticesbatiotextrm3batitextrm068zrtextrm032otextrm3-2006')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{de_guerville_soft_2006,\n\ttitle = {Soft mode dynamics and the reduction of {Ti}$^{\\textrm{4+}}$ disorder in ferroelectric∕relaxor superlattices {BaTiO}$_{\\textrm{3}}$ / {BaTi}$_{\\textrm{0.68}}${Zr}$_{\\textrm{0.32}}${O}$_{\\textrm{3}}$},\n\tvolume = {74},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.74.064107},\n\tdoi = {10.1103/PhysRevB.74.064107},\n\tabstract = {We used pulsed laser deposition to grow a series of [BaTiO3]Λ∕2/[BaTi0.68Zr0.32O3]Λ∕2 (BTZ∕BT) superlattices (SL’s) with a modulation period Λ that varies between 16Å⩽Λ⩽1008Å; the total thickness is kept constant at about 4000Å. We determine the out-of-plane lattice parameters of the SL constituents by modeling the x-ray diffractograms of the SL’s. The results indicate that the polar c axis of the BT layers lies in the plane of the film. The Raman data reinforces this interpretation. The Raman spectra of SL’s give evidence of coupling between BT and BTZ layers and a narrowing of the Raman peaks suggest a reduction of the disorder of the Ti4+ ions due to the strain. This strain resulting from the lattice mismatch between the constituent layers is responsible for the upward frequency shift of the soft modes, especially the E(1TO) mode, which is markedly altered with respect to its analogs in BT-bulk crystals and BT film. This soft-mode behavior as a function of Λ indicates that the crystal structure of all SL’s is more rigid than in BTZ and BT single thin films.},\n\tlanguage = {en},\n\tnumber = {6},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {De Guerville, F. and El Marssi, M. and Raevski, I. P. and Karkut, M. G. and Yuzyuk, Yu. I.},\n\tmonth = aug,\n\tyear = {2006},\n\tnote = {Publisher: American Physical Society},\n\tpages = {064107},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We used pulsed laser deposition to grow a series of [BaTiO3]Λ∕2/[BaTi0.68Zr0.32O3]Λ∕2 (BTZ∕BT) superlattices (SL’s) with a modulation period Λ that varies between 16Å⩽Λ⩽1008Å; the total thickness is kept constant at about 4000Å. We determine the out-of-plane lattice parameters of the SL constituents by modeling the x-ray diffractograms of the SL’s. The results indicate that the polar c axis of the BT layers lies in the plane of the film. The Raman data reinforces this interpretation. The Raman spectra of SL’s give evidence of coupling between BT and BTZ layers and a narrowing of the Raman peaks suggest a reduction of the disorder of the Ti4+ ions due to the strain. This strain resulting from the lattice mismatch between the constituent layers is responsible for the upward frequency shift of the soft modes, especially the E(1TO) mode, which is markedly altered with respect to its analogs in BT-bulk crystals and BT film. This soft-mode behavior as a function of Λ indicates that the crystal structure of all SL’s is more rigid than in BTZ and BT single thin films.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"gupta-bhattacharya-yuzuk-sreenivas-katiyar-opticalphononmodesinznonanorodsonsipreparedbypulsedlaserdeposition-2006\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0022024805011619\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'gupta-bhattacharya-yuzuk-sreenivas-katiyar-opticalphononmodesinznonanorodsonsipreparedbypulsedlaserdeposition-2006', 'https://www.sciencedirect.com/science/article/pii/S0022024805011619', event);\">\n    Optical phonon modes in ZnO nanorods on Si prepared by pulsed laser deposition.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Gupta, V.; Bhattacharya, P.; Yuzuk, Y. I.; Sreenivas, K.;  and Katiyar, R. S.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Crystal Growth</i>, 287(1): 39–43. January 2006.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0022024805011619\"\n     onclick=\"log_download('gupta-bhattacharya-yuzuk-sreenivas-katiyar-opticalphononmodesinznonanorodsonsipreparedbypulsedlaserdeposition-2006', 'https://www.sciencedirect.com/science/article/pii/S0022024805011619', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Optical phonon modes in ZnO nanorods on Si prepared by pulsed laser deposition [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.jcrysgro.2005.10.039\"\n     onclick=\"log_download('gupta-bhattacharya-yuzuk-sreenivas-katiyar-opticalphononmodesinznonanorodsonsipreparedbypulsedlaserdeposition-2006', 'http://doi.org/10.1016/j.jcrysgro.2005.10.039', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/gupta-bhattacharya-yuzuk-sreenivas-katiyar-opticalphononmodesinznonanorodsonsipreparedbypulsedlaserdeposition-2006\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('gupta-bhattacharya-yuzuk-sreenivas-katiyar-opticalphononmodesinznonanorodsonsipreparedbypulsedlaserdeposition-2006')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{gupta_optical_2006,\n\tseries = {Proceedings of the {International} {Conference} on {Materials} for {Advanced} {Technologies} ({ICMAT} 2005) {Symposium} {N}},\n\ttitle = {Optical phonon modes in {ZnO} nanorods on {Si} prepared by pulsed laser deposition},\n\tvolume = {287},\n\tissn = {0022-0248},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0022024805011619},\n\tdoi = {10.1016/j.jcrysgro.2005.10.039},\n\tabstract = {An array of vertically aligned c-axis-oriented zinc oxide (ZnO) nanorods were fabricated at a low substrate temperature (500°C) without using any catalytic template on the Si substrate by pulsed laser deposition at a high pressure (1–5Torr). The successive deposition of ZnO nanoparticles one over the other during growth led to the formation of elongated and well-isolated nanorods with a diameter in the range 70–350nm and up to 14μm long. The influence of deposition parameters on the Raman phonon modes was investigated. The polarized Raman studies were carried out in the backward geometry with incident light (i) parallel and (ii) perpendicular to the nanorod length. The activation of lower and upper surface phonon modes were observed in the ZnO nanorods between the transverse optical (ωTO) and the longitudinal optical (ωLO) phonon frequencies. The lower surface mode observed at ∼475cm−1 is found to be predominant in the X(ZZ)X¯ configuration. The surface phonon modes were not found in the samples prepared at {\\textgreater}600°C due to the coalescence process resulting in a continuous film. The agreement of polarized Raman spectra with single crystal data indicates the growth of good quality ZnO nanorods, and allows direct integration on Si without introducing contamination at the interface due to any catalytic material.},\n\tlanguage = {en},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Crystal Growth},\n\tauthor = {Gupta, Vinay and Bhattacharya, P. and Yuzuk, Yu. I. and Sreenivas, K. and Katiyar, R. S.},\n\tmonth = jan,\n\tyear = {2006},\n\tkeywords = {A1. axis orientation, A1. Nanorods, A1. Raman scattering, A1. Surface phonon mode, A3. PLD, B2. Zinc oxide},\n\tpages = {39--43},\n\tfile = {ScienceDirect Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\HR85BTQK\\\\S0022024805011619.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  An array of vertically aligned c-axis-oriented zinc oxide (ZnO) nanorods were fabricated at a low substrate temperature (500°C) without using any catalytic template on the Si substrate by pulsed laser deposition at a high pressure (1–5Torr). The successive deposition of ZnO nanoparticles one over the other during growth led to the formation of elongated and well-isolated nanorods with a diameter in the range 70–350nm and up to 14μm long. The influence of deposition parameters on the Raman phonon modes was investigated. The polarized Raman studies were carried out in the backward geometry with incident light (i) parallel and (ii) perpendicular to the nanorod length. The activation of lower and upper surface phonon modes were observed in the ZnO nanorods between the transverse optical (ωTO) and the longitudinal optical (ωLO) phonon frequencies. The lower surface mode observed at ∼475cm−1 is found to be predominant in the X(ZZ)X¯ configuration. The surface phonon modes were not found in the samples prepared at \\textgreater600°C due to the coalescence process resulting in a continuous film. The agreement of polarized Raman spectra with single crystal data indicates the growth of good quality ZnO nanorods, and allows direct integration on Si without introducing contamination at the interface due to any catalytic material.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----pbtextrm1xcatextrmxtiotextrm3-2006\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/3406\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----pbtextrm1xcatextrmxtiotextrm3-2006', 'https://journals.ioffe.ru/articles/3406', event);\">\n    Ротационно-полярные структурные искажения в твердых растворах Pb$_{\\textrm{1-x}}$Ca$_{\\textrm{x}}$TiO$_{\\textrm{3}}$ на основе данных спектроскопии комбинационного рассеяния света.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Торгашев, В. И.; Юзюк, Ю. И.; Широков, В. Б.;  and Леманов, В. В.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 48(5): 864–873.  2006.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/3406\"\n     onclick=\"log_download('----pbtextrm1xcatextrmxtiotextrm3-2006', 'https://journals.ioffe.ru/articles/3406', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Ротационно-полярные структурные искажения в твердых растворах Pb$_{\\textrm{1-x}}$Ca$_{\\textrm{x}}$TiO$_{\\textrm{3}}$ на основе данных спектроскопии комбинационного рассеяния света [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----pbtextrm1xcatextrmxtiotextrm3-2006\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----pbtextrm1xcatextrmxtiotextrm3-2006')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{_-_2006,\n\ttitle = {Ротационно-полярные структурные искажения в твердых растворах {Pb}$_{\\textrm{1-x}}${Ca}$_{\\textrm{x}}${TiO}$_{\\textrm{3}}$ на основе данных спектроскопии комбинационного рассеяния света},\n\tvolume = {48},\n\turl = {https://journals.ioffe.ru/articles/3406},\n\tabstract = {При проведении высокотемпературных (290−560 K) исследований поляризованных спектров комбинаци онного рассеяния света в области частот 6 {\\textless}ν{\\textless} 1200 cm−1 на монокристаллическом образце твердого\nраствора Pb0.55Ca0.45TiO3 установлено существование трех особых температурных точек, по крайней мере\nв двух из которых происходят структурные фазовые переходы. В рамках теории Ландау фазовых переходов\nвторого рода обсуждается допустимая топология фазовых диаграмм, качественно верно отражающая\nэкспериментальную ситуацию.},\n\tlanguage = {ru},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Торгашев, В. И. and Юзюк, Ю. И. and Широков, В. Б. and Леманов, В. В.},\n\tyear = {2006},\n\tkeywords = {⛔ No DOI found},\n\tpages = {864--873},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  При проведении высокотемпературных (290−560 K) исследований поляризованных спектров комбинаци онного рассеяния света в области частот 6 \\textlessν\\textless 1200 cm−1 на монокристаллическом образце твердого раствора Pb0.55Ca0.45TiO3 установлено существование трех особых температурных точек, по крайней мере в двух из которых происходят структурные фазовые переходы. В рамках теории Ландау фазовых переходов второго рода обсуждается допустимая топология фазовых диаграмм, качественно верно отражающая экспериментальную ситуацию.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"---kuntscher-pbtextrm1xcatextrmxtiotextrm3-2006\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/3382\"\n     onclick=\"return trackOutboundLink('publications', 'click', '---kuntscher-pbtextrm1xcatextrmxtiotextrm3-2006', 'https://journals.ioffe.ru/articles/3382', event);\">\n    Концентрационный фазовый переход в твердых растворах Pb$_{\\textrm{1-x}}$Ca$_{\\textrm{x}}$TiO$_{\\textrm{3}}$ по данным спектроскопии комбинационного рассеяния света.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Торгашев, В. И.; Юзюк, Ю. И.; Леманов, В. В.;  and Kuntscher, C. A.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 48(4): 717–725.  2006.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/3382\"\n     onclick=\"log_download('---kuntscher-pbtextrm1xcatextrmxtiotextrm3-2006', 'https://journals.ioffe.ru/articles/3382', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Концентрационный фазовый переход в твердых растворах Pb$_{\\textrm{1-x}}$Ca$_{\\textrm{x}}$TiO$_{\\textrm{3}}$ по данным спектроскопии комбинационного рассеяния света [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/---kuntscher-pbtextrm1xcatextrmxtiotextrm3-2006\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('---kuntscher-pbtextrm1xcatextrmxtiotextrm3-2006')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2006-1,\n\ttitle = {Концентрационный фазовый переход в твердых растворах {Pb}$_{\\textrm{1-x}}${Ca}$_{\\textrm{x}}${TiO}$_{\\textrm{3}}$ по данным спектроскопии комбинационного рассеяния света},\n\tvolume = {48},\n\turl = {https://journals.ioffe.ru/articles/3382},\n\tabstract = {Впервые на монокристаллических образцах твердых перовскитных растворов Pb1−xCaxTiO3 (составы:\nx = 0, 0.03, 0.04, 0.15, 0.23, 0.28, 0.34, 0.38, 0.40, 0.45 и 0.50) получены поляризованные спектры\nкомбинационного рассеяния света и ИК отражения в области частот 6 {\\textless}ν{\\textless} 1200 cm−1 и температурах\n290–620 K. Основное внимание уделено низкочастотной динамике решетки, где установлено аномальное\nконцентрационное поведение фононного спектрального отклика при 0.38 {\\textless} x {\\textless} 0.40. При комнатной\nтемпературе в области x {\\textgreater} 0.40 в твердых растворах Pb1−xCaxTiO3 реализуется новое фазовое состояние,\nкоторое, вероятно, является полярным},\n\tlanguage = {ru},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Торгашев, В. И. and Юзюк, Ю. И. and Леманов, В. В. and Kuntscher, C. A.},\n\tyear = {2006},\n\tkeywords = {⛔ No DOI found},\n\tpages = {717--725},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Впервые на монокристаллических образцах твердых перовскитных растворов Pb1−xCaxTiO3 (составы: x = 0, 0.03, 0.04, 0.15, 0.23, 0.28, 0.34, 0.38, 0.40, 0.45 и 0.50) получены поляризованные спектры комбинационного рассеяния света и ИК отражения в области частот 6 \\textlessν\\textless 1200 cm−1 и температурах 290–620 K. Основное внимание уделено низкочастотной динамике решетки, где установлено аномальное концентрационное поведение фононного спектрального отклика при 0.38 \\textless x \\textless 0.40. При комнатной температуре в области x \\textgreater 0.40 в твердых растворах Pb1−xCaxTiO3 реализуется новое фазовое состояние, которое, вероятно, является полярным\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"----2006\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.elibrary.ru/item.asp?id=12884469\"\n     onclick=\"return trackOutboundLink('publications', 'click', '----2006', 'https://www.elibrary.ru/item.asp?id=12884469', event);\">\n    Конечно-элементное моделирование в динамических задачах для упругих решеток микро- и нанокристаллов из оксида цинка.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Еремеев, В. А.; Кайдашев, Е. М.;  and Соловьев, А. Н.\n</span>\n\n  \n\n</span>\n\n  <i>Вестник Южного Научного Центра Ран</i>, 2(1): 10–15.  2006.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.elibrary.ru/item.asp?id=12884469\"\n     onclick=\"log_download('----2006', 'https://www.elibrary.ru/item.asp?id=12884469', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Конечно-элементное моделирование в динамических задачах для упругих решеток микро- и нанокристаллов из оксида цинка [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/----2006\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('----2006')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{_-_2006-1,\n\ttitle = {Конечно-элементное моделирование в динамических задачах для упругих решеток микро- и нанокристаллов из оксида цинка},\n\tvolume = {2},\n\tissn = {1813-4289},\n\turl = {https://www.elibrary.ru/item.asp?id=12884469},\n\tabstract = {Представлены результаты конечно-элементного моделирования процессов деформирования решетки нано- и микрокристаллов из оксида цинка. В рамках плоской теории электроупругости рассмотрены свободные и вынужденные колебания, а также нестационарные задачи для решетки микро- или нанокристаллов из оксида цинка, расположенных на подложке сапфира. Определены собственные частоты для системы решетка кристаллов - подложка, показано, что по найденному спектру большой системы (решетка - подложка) и спектру подложки можно определить первые собственные частоты одного нанокристалла. Это позволяет по экспериментальным данным для больших систем определить собственные частоты нанообъекта, которые непосредственно трудно определить другим способом. Знание собственных частот позволяет, в частности, судить о механических свойствах нанокристалла. Обсуждается возможность использования решеток нанокристаллов в качестве элементов наносенсоров.},\n\tlanguage = {ru},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Вестник Южного Научного Центра Ран},\n\tauthor = {Еремеев, В. А. and Кайдашев, Е. М. and Соловьев, А. Н.},\n\tyear = {2006},\n\tkeywords = {⛔ No DOI found},\n\tpages = {10--15},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Представлены результаты конечно-элементного моделирования процессов деформирования решетки нано- и микрокристаллов из оксида цинка. В рамках плоской теории электроупругости рассмотрены свободные и вынужденные колебания, а также нестационарные задачи для решетки микро- или нанокристаллов из оксида цинка, расположенных на подложке сапфира. Определены собственные частоты для системы решетка кристаллов - подложка, показано, что по найденному спектру большой системы (решетка - подложка) и спектру подложки можно определить первые собственные частоты одного нанокристалла. Это позволяет по экспериментальным данным для больших систем определить собственные частоты нанообъекта, которые непосредственно трудно определить другим способом. Знание собственных частот позволяет, в частности, судить о механических свойствах нанокристалла. Обсуждается возможность использования решеток нанокристаллов в качестве элементов наносенсоров.\n</div>\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2005\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2005')\"\n      onkeypress=\"toggleGroup('group_2005')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2005</span>\n      <span class=\"bibbase_group_count\">\n        \n        (7)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"nobis-kaidashev-rahm-lorenz-grundmann-whisperinggallerymodesinhexagonalzincoxidemicroandnanocrystals-2005\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  Whispering Gallery Modes in Hexagonal Zinc Oxide Micro- and Nanocrystals.\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Nobis, T.; Kaidashev, E. M.; Rahm, A.; Lorenz, M.;  and Grundmann, M.\n</span>\n\n  \n\n</span>\n\n  In Nickel, N. H.;  and Terukov, E., editor(s), <i>Zinc Oxide — A Material for Micro- and Optoelectronic Applications</i>, of <i>NATO Science Series II: Mathematics, Physics and Chemistry</i>, pages 83–98, Dordrecht,  2005. Springer Netherlands\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n\n  \n  <a href=\"http://doi.org/10.1007/1-4020-3475-X_8\"\n     onclick=\"log_download('nobis-kaidashev-rahm-lorenz-grundmann-whisperinggallerymodesinhexagonalzincoxidemicroandnanocrystals-2005', 'http://doi.org/10.1007/1-4020-3475-X_8', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/nobis-kaidashev-rahm-lorenz-grundmann-whisperinggallerymodesinhexagonalzincoxidemicroandnanocrystals-2005\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('nobis-kaidashev-rahm-lorenz-grundmann-whisperinggallerymodesinhexagonalzincoxidemicroandnanocrystals-2005')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@inproceedings{nobis_whispering_2005,\n\taddress = {Dordrecht},\n\tseries = {{NATO} {Science} {Series} {II}: {Mathematics}, {Physics} and {Chemistry}},\n\ttitle = {Whispering {Gallery} {Modes} in {Hexagonal} {Zinc} {Oxide} {Micro}- and {Nanocrystals}},\n\tisbn = {978-1-4020-3475-6},\n\tdoi = {10.1007/1-4020-3475-X_8},\n\tabstract = {The resonator properties of zinc oxide (ZnO) micro- and nanocrystals grown by a novel high pressure pulsed laser deposition process have been investigated at room temperature by cathodoluminescence (CL), spatially resolved CL-imaging and polarization resolved micro-photoluminescence (μ-PL) within the visible spectral range. The spectra exhibit a series of comparatively sharp and almost equidistant resonance lines. Using a simple plane wave interference model and taking into account the spectral characteristic n(ω) of the refractive index of ZnO, we can unambiguously attribute those lines to whispering gallery modes (WGMs) of a two dimensional hexagonal resonator. The predicted resonator diameters agree well with the measured crystal sizes. Tapered, high aspect ratio ZnO nanoneedles furthermore allow systematic investigations of the WGMs as a function of cavity diameter D down to zero. Hence, the transition from a multi-mode to a single mode cavity is directly observed. μ-PL experiments demonstrate that the WGMs are mainly TM polarized.},\n\tlanguage = {en},\n\tbooktitle = {Zinc {Oxide} — {A} {Material} for {Micro}- and {Optoelectronic} {Applications}},\n\tpublisher = {Springer Netherlands},\n\tauthor = {Nobis, Thomas and Kaidashev, Evgeni M. and Rahm, Andreas and Lorenz, Michael and Grundmann, Marius},\n\teditor = {Nickel, Norbert H. and Terukov, Evgenii},\n\tyear = {2005},\n\tkeywords = {microcrystal, nanocavity, nanostructure, polarization, Whispering gallery modes},\n\tpages = {83--98},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The resonator properties of zinc oxide (ZnO) micro- and nanocrystals grown by a novel high pressure pulsed laser deposition process have been investigated at room temperature by cathodoluminescence (CL), spatially resolved CL-imaging and polarization resolved micro-photoluminescence (μ-PL) within the visible spectral range. The spectra exhibit a series of comparatively sharp and almost equidistant resonance lines. Using a simple plane wave interference model and taking into account the spectral characteristic n(ω) of the refractive index of ZnO, we can unambiguously attribute those lines to whispering gallery modes (WGMs) of a two dimensional hexagonal resonator. The predicted resonator diameters agree well with the measured crystal sizes. Tapered, high aspect ratio ZnO nanoneedles furthermore allow systematic investigations of the WGMs as a function of cavity diameter D down to zero. Hence, the transition from a multi-mode to a single mode cavity is directly observed. μ-PL experiments demonstrate that the WGMs are mainly TM polarized.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------2005\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/viewPDF/8639\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------2005', 'https://journals.ioffe.ru/articles/viewPDF/8639', event);\">\n    Особенности динамики переключения поляризации в тонких пленках цирконата–титаната–свинца.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Мухортов В.М.; Колесников В.В.; Головко Ю.И.; Мащенко А.И.;  and Бирюков С.В.\n</span>\n\n  \n\n</span>\n\n  <i>Журнал технической физики</i>, 75(5): 126–131.  2005.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/viewPDF/8639\"\n     onclick=\"log_download('------2005', 'https://journals.ioffe.ru/articles/viewPDF/8639', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Особенности динамики переключения поляризации в тонких пленках цирконата–титаната–свинца [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------2005\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------2005')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{___2005,\n\ttitle = {Особенности динамики переключения поляризации в тонких пленках цирконата–титаната–свинца},\n\tvolume = {75},\n\turl = {https://journals.ioffe.ru/articles/viewPDF/8639},\n\tnumber = {5},\n\tjournal = {Журнал технической физики},\n\tauthor = {{Мухортов В.М.} and {Колесников В.В.} and {Головко Ю.И.} and {Мащенко А.И.} and {Бирюков С.В.}},\n\tyear = {2005},\n\tkeywords = {⛔ No DOI found},\n\tpages = {126--131},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"------2005\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/3735\"\n     onclick=\"return trackOutboundLink('publications', 'click', '------2005', 'https://journals.ioffe.ru/articles/3735', event);\">\n    Спектры комбинационного рассеяния света титаната кадмия.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Торгашев, В. И.; Юзюк, Ю. И.; Широков, В. Б.; Леманов, В. В.;  and Спектор, И. Е.\n</span>\n\n  \n\n</span>\n\n  <i>Физика твердого тела</i>, 47(2): 324–333.  2005.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/3735\"\n     onclick=\"log_download('------2005', 'https://journals.ioffe.ru/articles/3735', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Спектры комбинационного рассеяния света титаната кадмия [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/------2005\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('------2005')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2005,\n\ttitle = {Спектры комбинационного рассеяния света титаната кадмия},\n\tvolume = {47},\n\turl = {https://journals.ioffe.ru/articles/3735},\n\tabstract = {Впервые получены поляризованные спектры комбинационного рассеяния света монокристаллических\nобразцов CdTiO3 в области частот 5 {\\textless}ν{\\textless} 1000 cm$^{\\textrm{−1}}$ при температурах 10−1200 K. Основное внима ние уделено низкочастотной области, где обнаружено аномальное температурное поведение нескольких\nфононных мод. Высокотемпературными исследованиями выявлено существование четырех фононов с характерным для мягких мод поведением. Эти фононы отнесены к модам, восстанавливающим кубическую симметрию решетки. Экстраполяции их температурных зависимостей позволили выдвинуть гипотезу о существовании цепочки из трех гипотетических высокотемпературных фазовых переходов, аналогичных тем, что наблюдаются собственно в перовските CaTiO3. При температурах ниже 78 K спектр комбинационного рассеяния обогащается новыми линиями, появление которых связано с полярными искажениями ячейки. На низких частотах обнаружено три линии с аномальным поведением осцилляторных параметров, которое характерно для мягких мод в сегнетоэлектрических фазах. Предполагается возможность существования нескольких разных полярных состояний при низких температурах.},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Физика твердого тела},\n\tauthor = {Торгашев, В. И. and Юзюк, Ю. И. and Широков, В. Б. and Леманов, В. В. and Спектор, И. Е.},\n\tyear = {2005},\n\tkeywords = {⛔ No DOI found},\n\tpages = {324--333},\n\tfile = {Физика твердого тела:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\9NBHHWBQ\\\\3735.html:text/html;Физика твердого тела.pdf:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\3H3Z7B97\\\\Физика твердого тела.pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Впервые получены поляризованные спектры комбинационного рассеяния света монокристаллических образцов CdTiO3 в области частот 5 \\textlessν\\textless 1000 cm$^{\\textrm{−1}}$ при температурах 10−1200 K. Основное внима ние уделено низкочастотной области, где обнаружено аномальное температурное поведение нескольких фононных мод. Высокотемпературными исследованиями выявлено существование четырех фононов с характерным для мягких мод поведением. Эти фононы отнесены к модам, восстанавливающим кубическую симметрию решетки. Экстраполяции их температурных зависимостей позволили выдвинуть гипотезу о существовании цепочки из трех гипотетических высокотемпературных фазовых переходов, аналогичных тем, что наблюдаются собственно в перовските CaTiO3. При температурах ниже 78 K спектр комбинационного рассеяния обогащается новыми линиями, появление которых связано с полярными искажениями ячейки. На низких частотах обнаружено три линии с аномальным поведением осцилляторных параметров, которое характерно для мягких мод в сегнетоэлектрических фазах. Предполагается возможность существования нескольких разных полярных состояний при низких температурах.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"-----2005\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://elibrary.lt/resursai/Uzsienio%20leidiniai/ioffe/pztf/2005/23/pztf_t31v23_12.pdf\"\n     onclick=\"return trackOutboundLink('publications', 'click', '-----2005', 'http://elibrary.lt/resursai/Uzsienio%20leidiniai/ioffe/pztf/2005/23/pztf_t31v23_12.pdf', event);\">\n    Формирование доменной структуры под действием деформационных полей в наноразмерных пленках титаната бария-стронция.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Мухортов, В. М.; Головко, Ю. И.; Колесников, В. В.;  and Бирюков, С. В.\n</span>\n\n  \n\n</span>\n\n  <i>Письма ЖТФ</i>, 31(23): 75–81.  2005.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://elibrary.lt/resursai/Uzsienio%20leidiniai/ioffe/pztf/2005/23/pztf_t31v23_12.pdf\"\n     onclick=\"log_download('-----2005', 'http://elibrary.lt/resursai/Uzsienio%20leidiniai/ioffe/pztf/2005/23/pztf_t31v23_12.pdf', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/pdf.svg\"\n\t     alt=\"Формирование доменной структуры под действием деформационных полей в наноразмерных пленках титаната бария-стронция [pdf]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/-----2005\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('-----2005')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{__2005-1,\n\ttitle = {Формирование доменной структуры под действием деформационных полей в наноразмерных пленках титаната бария-стронция},\n\tvolume = {31},\n\turl = {http://elibrary.lt/resursai/Uzsienio%20leidiniai/ioffe/pztf/2005/23/pztf_t31v23_12.pdf},\n\tnumber = {23},\n\turldate = {2023-11-11},\n\tjournal = {Письма ЖТФ},\n\tauthor = {Мухортов, В. М. and Головко, Ю. И. and Колесников, В. В. and Бирюков, С. В.},\n\tyear = {2005},\n\tkeywords = {⛔ No DOI found},\n\tpages = {75--81},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"lorenz-kaidashev-rahm-nobis-lenzner-wagner-spemann-hochmuth-etal-mgtextrmxzntextrm1xo0xtextless02nanowirearraysonsapphiregrownbyhighpressurepulsedlaserdeposition-2005\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.1898433\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'lorenz-kaidashev-rahm-nobis-lenzner-wagner-spemann-hochmuth-etal-mgtextrmxzntextrm1xo0xtextless02nanowirearraysonsapphiregrownbyhighpressurepulsedlaserdeposition-2005', 'https://doi.org/10.1063/1.1898433', event);\">\n    Mg$_{\\textrm{x}}$Zn$_{\\textrm{1−x}}$O(0⩽x\\textless0.2) nanowire arrays on sapphire grown by high-pressure pulsed-laser deposition.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Lorenz, M.; Kaidashev, E. M.; Rahm, A.; Nobis, T.; Lenzner, J.; Wagner, G.; Spemann, D.; Hochmuth, H.;  and Grundmann, M.\n</span>\n\n  \n\n</span>\n\n  <i>Applied Physics Letters</i>, 86(14): 143113. March 2005.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.1898433\"\n     onclick=\"log_download('lorenz-kaidashev-rahm-nobis-lenzner-wagner-spemann-hochmuth-etal-mgtextrmxzntextrm1xo0xtextless02nanowirearraysonsapphiregrownbyhighpressurepulsedlaserdeposition-2005', 'https://doi.org/10.1063/1.1898433', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Mg$_{\\textrm{x}}$Zn$_{\\textrm{1−x}}$O(0⩽x\\textless0.2) nanowire arrays on sapphire grown by high-pressure pulsed-laser deposition [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.1898433\"\n     onclick=\"log_download('lorenz-kaidashev-rahm-nobis-lenzner-wagner-spemann-hochmuth-etal-mgtextrmxzntextrm1xo0xtextless02nanowirearraysonsapphiregrownbyhighpressurepulsedlaserdeposition-2005', 'http://doi.org/10.1063/1.1898433', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/lorenz-kaidashev-rahm-nobis-lenzner-wagner-spemann-hochmuth-etal-mgtextrmxzntextrm1xo0xtextless02nanowirearraysonsapphiregrownbyhighpressurepulsedlaserdeposition-2005\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('lorenz-kaidashev-rahm-nobis-lenzner-wagner-spemann-hochmuth-etal-mgtextrmxzntextrm1xo0xtextless02nanowirearraysonsapphiregrownbyhighpressurepulsedlaserdeposition-2005')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{lorenz_mgxzn1xo0x02_2005,\n\ttitle = {Mg$_{\\textrm{x}}${Zn}$_{\\textrm{1−x}}${O}(0⩽x{\\textless}0.2) nanowire arrays on sapphire grown by high-pressure pulsed-laser deposition},\n\tvolume = {86},\n\tissn = {0003-6951},\n\turl = {https://doi.org/10.1063/1.1898433},\n\tdoi = {10.1063/1.1898433},\n\tabstract = {MgxZn1−xO nanowires with Mg-content x from 0 to 0.2 have been grown by high-pressure pulsed-laser deposition (PLD) on gold-covered sapphire single crystals. The PLD process allows for a unique wide-range control of morphology, diameter, and composition of the MgxZn1−xO nanowires. The diameter of single ZnO wires could be varied between about 50 and 3000 nm, and the Mg content x of MgxZn1−xO wire arrays was controlled via the PLD gas pressure. The microscopic homogeneity of Mg content is displayed by cathodoluminescence (CL) imaging of the excitonic peak energy. The fluctuation of CL peak energy between individual wires is about an order of magnitude smaller than the alloy broadening.},\n\tnumber = {14},\n\turldate = {2023-11-11},\n\tjournal = {Applied Physics Letters},\n\tauthor = {Lorenz, M. and Kaidashev, E. M. and Rahm, A. and Nobis, Th. and Lenzner, J. and Wagner, G. and Spemann, D. and Hochmuth, H. and Grundmann, M.},\n\tmonth = mar,\n\tyear = {2005},\n\tpages = {143113},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  MgxZn1−xO nanowires with Mg-content x from 0 to 0.2 have been grown by high-pressure pulsed-laser deposition (PLD) on gold-covered sapphire single crystals. The PLD process allows for a unique wide-range control of morphology, diameter, and composition of the MgxZn1−xO nanowires. The diameter of single ZnO wires could be varied between about 50 and 3000 nm, and the Mg content x of MgxZn1−xO wire arrays was controlled via the PLD gas pressure. The microscopic homogeneity of Mg content is displayed by cathodoluminescence (CL) imaging of the excitonic peak energy. The fluctuation of CL peak energy between individual wires is about an order of magnitude smaller than the alloy broadening.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"jain-yuzyuk-katiyar-somiya-bhalla-localsymmetrybreakinginpbtextrmxsrtextrm1xtiotextrm3ceramicsandcompositesstudiedbyramanspectroscopy-2005\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.1989434\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'jain-yuzyuk-katiyar-somiya-bhalla-localsymmetrybreakinginpbtextrmxsrtextrm1xtiotextrm3ceramicsandcompositesstudiedbyramanspectroscopy-2005', 'https://doi.org/10.1063/1.1989434', event);\">\n    Local symmetry breaking in Pb$_{\\textrm{x}}$Sr$_{\\textrm{1−x}}$TiO$_{\\textrm{3}}$ ceramics and composites studied by Raman spectroscopy.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Jain, M.; Yuzyuk, Y. I.; Katiyar, R. S.; Somiya, Y.;  and Bhalla, A. S.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Applied Physics</i>, 98(2): 024116. July 2005.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.1989434\"\n     onclick=\"log_download('jain-yuzyuk-katiyar-somiya-bhalla-localsymmetrybreakinginpbtextrmxsrtextrm1xtiotextrm3ceramicsandcompositesstudiedbyramanspectroscopy-2005', 'https://doi.org/10.1063/1.1989434', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Local symmetry breaking in Pb$_{\\textrm{x}}$Sr$_{\\textrm{1−x}}$TiO$_{\\textrm{3}}$ ceramics and composites studied by Raman spectroscopy [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.1989434\"\n     onclick=\"log_download('jain-yuzyuk-katiyar-somiya-bhalla-localsymmetrybreakinginpbtextrmxsrtextrm1xtiotextrm3ceramicsandcompositesstudiedbyramanspectroscopy-2005', 'http://doi.org/10.1063/1.1989434', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/jain-yuzyuk-katiyar-somiya-bhalla-localsymmetrybreakinginpbtextrmxsrtextrm1xtiotextrm3ceramicsandcompositesstudiedbyramanspectroscopy-2005\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('jain-yuzyuk-katiyar-somiya-bhalla-localsymmetrybreakinginpbtextrmxsrtextrm1xtiotextrm3ceramicsandcompositesstudiedbyramanspectroscopy-2005')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{jain_local_2005,\n\ttitle = {Local symmetry breaking in {Pb}$_{\\textrm{x}}${Sr}$_{\\textrm{1−x}}${TiO}$_{\\textrm{3}}$ ceramics and composites studied by {Raman} spectroscopy},\n\tvolume = {98},\n\tissn = {0021-8979},\n\turl = {https://doi.org/10.1063/1.1989434},\n\tdoi = {10.1063/1.1989434},\n\tabstract = {Local symmetry breaking in PbxSr1−xTiO3 (PST) solid solutions was revealed by Raman spectroscopy below and above the ferroelectric phase-transition temperature. In the paraelectric phase, local symmetry breaking associated with the polar clusters localized mostly at grain boundaries in ceramic samples leads to the activation of the polar modes far above the dielectric maximum. This effect was found remarkably enhanced in the PST:MgO composites due to the compositional inhomogeneity of the grain boundaries and the intergrain stresses in the composite. In the ferroelectric phase, the degeneracy of the E(TO1) soft mode was lifted due to translational symmetry breaking in the solid solutions with x=0.2 and 0.3, where the substitution of Sr by Pb replaces partially the ionic bonding between the A cations and the oxygens by a stronger covalent bonding.},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Applied Physics},\n\tauthor = {Jain, M. and Yuzyuk, Yu. I. and Katiyar, R. S. and Somiya, Y. and Bhalla, A. S.},\n\tmonth = jul,\n\tyear = {2005},\n\tpages = {024116},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Local symmetry breaking in PbxSr1−xTiO3 (PST) solid solutions was revealed by Raman spectroscopy below and above the ferroelectric phase-transition temperature. In the paraelectric phase, local symmetry breaking associated with the polar clusters localized mostly at grain boundaries in ceramic samples leads to the activation of the polar modes far above the dielectric maximum. This effect was found remarkably enhanced in the PST:MgO composites due to the compositional inhomogeneity of the grain boundaries and the intergrain stresses in the composite. In the ferroelectric phase, the degeneracy of the E(TO1) soft mode was lifted due to translational symmetry breaking in the solid solutions with x=0.2 and 0.3, where the substitution of Sr by Pb replaces partially the ionic bonding between the A cations and the oxygens by a stronger covalent bonding.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"katiyar-yuzyuk-das-bhattacharya-gupta-polarizedramanspectraofbatiotextrm3srtiotextrm3superlattices-2005\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1080/00150190500314833\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'katiyar-yuzyuk-das-bhattacharya-gupta-polarizedramanspectraofbatiotextrm3srtiotextrm3superlattices-2005', 'https://doi.org/10.1080/00150190500314833', event);\">\n    Polarized Raman Spectra of BaTiO$_{\\textrm{3}}$/SrTiO$_{\\textrm{3}}$ Superlattices.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Katiyar, R. S.; Yuzyuk†, Y. I.; Das, R. R.; Bhattacharya, P.;  and Gupta, V.\n</span>\n\n  \n\n</span>\n\n  <i>Ferroelectrics</i>, 329(1): 3–12. December 2005.\n  <span class=\"note\">Publisher: Taylor & Francis _eprint: https://doi.org/10.1080/00150190500314833</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1080/00150190500314833\"\n     onclick=\"log_download('katiyar-yuzyuk-das-bhattacharya-gupta-polarizedramanspectraofbatiotextrm3srtiotextrm3superlattices-2005', 'https://doi.org/10.1080/00150190500314833', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Polarized Raman Spectra of BaTiO$_{\\textrm{3}}$/SrTiO$_{\\textrm{3}}$ Superlattices [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1080/00150190500314833\"\n     onclick=\"log_download('katiyar-yuzyuk-das-bhattacharya-gupta-polarizedramanspectraofbatiotextrm3srtiotextrm3superlattices-2005', 'http://doi.org/10.1080/00150190500314833', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/katiyar-yuzyuk-das-bhattacharya-gupta-polarizedramanspectraofbatiotextrm3srtiotextrm3superlattices-2005\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('katiyar-yuzyuk-das-bhattacharya-gupta-polarizedramanspectraofbatiotextrm3srtiotextrm3superlattices-2005')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{katiyar_polarized_2005,\n\ttitle = {Polarized {Raman} {Spectra} of {BaTiO}$_{\\textrm{3}}$/{SrTiO}$_{\\textrm{3}}$ {Superlattices}},\n\tvolume = {329},\n\tissn = {0015-0193},\n\turl = {https://doi.org/10.1080/00150190500314833},\n\tdoi = {10.1080/00150190500314833},\n\tabstract = {BaTiO 3 /SrTiO 3 superlattices were grown on (001)MgO substrates by pulsed-laser-deposition technique. The thickness of each layer varied from 6 to 25 unit cells. Polarization-dependent Raman spectra confirmed tetragonal symmetry of the superlattices with the polar axis being normal to the layers. The observed optic modes in the superlattices showed intermediate frequencies between corresponding bulk BaTiO 3 and SrTiO 3 values, while the E(TO 1 ) soft mode exhibited upward shift due to significant two-dimensional clamping caused by the lattice mismatch of the constituting layers. The observed downward shift of the soft mode revealed relaxation of two-dimensional stresses with increasing the stacking periodicity of the superlattices. The excitation of folded transverse acoustic phonons in the Raman spectra due to the new periodicity of the Brillouin zone was revealed. The observed data are quantitatively explained by a folding of the corresponding acoustic branch. It is shown that micro-Raman spectroscopy provides determination of a spatial variation of the layer thickness in graded superlattices. On leave from the Faculty of Physics, Rostov State University, Rostov-on-Don, Russia},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Ferroelectrics},\n\tauthor = {Katiyar, Ram S. and Yuzyuk†, Yu. I. and Das, R. R. and Bhattacharya, P. and Gupta, V.},\n\tmonth = dec,\n\tyear = {2005},\n\tnote = {Publisher: Taylor \\&amp; Francis\n\\_eprint: https://doi.org/10.1080/00150190500314833},\n\tpages = {3--12},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  BaTiO 3 /SrTiO 3 superlattices were grown on (001)MgO substrates by pulsed-laser-deposition technique. The thickness of each layer varied from 6 to 25 unit cells. Polarization-dependent Raman spectra confirmed tetragonal symmetry of the superlattices with the polar axis being normal to the layers. The observed optic modes in the superlattices showed intermediate frequencies between corresponding bulk BaTiO 3 and SrTiO 3 values, while the E(TO 1 ) soft mode exhibited upward shift due to significant two-dimensional clamping caused by the lattice mismatch of the constituting layers. The observed downward shift of the soft mode revealed relaxation of two-dimensional stresses with increasing the stacking periodicity of the superlattices. The excitation of folded transverse acoustic phonons in the Raman spectra due to the new periodicity of the Brillouin zone was revealed. The observed data are quantitatively explained by a folding of the corresponding acoustic branch. It is shown that micro-Raman spectroscopy provides determination of a spatial variation of the layer thickness in graded superlattices. On leave from the Faculty of Physics, Rostov State University, Rostov-on-Don, Russia\n</div>\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2004\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2004')\"\n      onkeypress=\"toggleGroup('group_2004')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2004</span>\n      <span class=\"bibbase_group_count\">\n        \n        (11)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"nobis-kaidashev-rahm-lorenz-grundmann-whisperinggallerymodesinnanosizeddielectricresonatorswithhexagonalcrosssection-2004\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevLett.93.103903\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'nobis-kaidashev-rahm-lorenz-grundmann-whisperinggallerymodesinnanosizeddielectricresonatorswithhexagonalcrosssection-2004', 'https://link.aps.org/doi/10.1103/PhysRevLett.93.103903', event);\">\n    Whispering Gallery Modes in Nanosized Dielectric Resonators with Hexagonal Cross Section.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Nobis, T.; Kaidashev, E. M.; Rahm, A.; Lorenz, M.;  and Grundmann, M.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review Letters</i>, 93(10): 103903. September 2004.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevLett.93.103903\"\n     onclick=\"log_download('nobis-kaidashev-rahm-lorenz-grundmann-whisperinggallerymodesinnanosizeddielectricresonatorswithhexagonalcrosssection-2004', 'https://link.aps.org/doi/10.1103/PhysRevLett.93.103903', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Whispering Gallery Modes in Nanosized Dielectric Resonators with Hexagonal Cross Section [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevLett.93.103903\"\n     onclick=\"log_download('nobis-kaidashev-rahm-lorenz-grundmann-whisperinggallerymodesinnanosizeddielectricresonatorswithhexagonalcrosssection-2004', 'http://doi.org/10.1103/PhysRevLett.93.103903', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/nobis-kaidashev-rahm-lorenz-grundmann-whisperinggallerymodesinnanosizeddielectricresonatorswithhexagonalcrosssection-2004\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('nobis-kaidashev-rahm-lorenz-grundmann-whisperinggallerymodesinnanosizeddielectricresonatorswithhexagonalcrosssection-2004')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{nobis_whispering_2004,\n\ttitle = {Whispering {Gallery} {Modes} in {Nanosized} {Dielectric} {Resonators} with {Hexagonal} {Cross} {Section}},\n\tvolume = {93},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevLett.93.103903},\n\tdoi = {10.1103/PhysRevLett.93.103903},\n\tabstract = {The size dependence of whispering gallery modes in dielectric resonators with hexagonal cross section has been observed within the visible spectral range for cavity diameters comparable to the light wavelength. As a model system single, tapered, high aspect ratio zinc oxide nanoneedles were analyzed. They enable systematic investigations as a function of the resonator diameter down to the nanometer regime. A simple plane wave interference model without free parameter describes the spectral positions and the linewidths of the modes in good agreement with the experiment.},\n\tnumber = {10},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review Letters},\n\tauthor = {Nobis, Thomas and Kaidashev, Evgeni M. and Rahm, Andreas and Lorenz, Michael and Grundmann, Marius},\n\tmonth = sep,\n\tyear = {2004},\n\tnote = {Publisher: American Physical Society},\n\tpages = {103903},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The size dependence of whispering gallery modes in dielectric resonators with hexagonal cross section has been observed within the visible spectral range for cavity diameters comparable to the light wavelength. As a model system single, tapered, high aspect ratio zinc oxide nanoneedles were analyzed. They enable systematic investigations as a function of the resonator diameter down to the nanometer regime. A simple plane wave interference model without free parameter describes the spectral positions and the linewidths of the modes in good agreement with the experiment.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"nobis-kaidashev-rahm-lorenz-lenzner-grundmann-spatiallyinhomogeneousimpuritydistributioninznomicropillars-2004\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1021/nl049889y\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'nobis-kaidashev-rahm-lorenz-lenzner-grundmann-spatiallyinhomogeneousimpuritydistributioninznomicropillars-2004', 'https://doi.org/10.1021/nl049889y', event);\">\n    Spatially Inhomogeneous Impurity Distribution in ZnO Micropillars.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Nobis, T.; Kaidashev, E. M.; Rahm, A.; Lorenz, M.; Lenzner, J.;  and Grundmann, M.\n</span>\n\n  \n\n</span>\n\n  <i>Nano Letters</i>, 4(5): 797–800. May 2004.\n  <span class=\"note\">Publisher: American Chemical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1021/nl049889y\"\n     onclick=\"log_download('nobis-kaidashev-rahm-lorenz-lenzner-grundmann-spatiallyinhomogeneousimpuritydistributioninznomicropillars-2004', 'https://doi.org/10.1021/nl049889y', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Spatially Inhomogeneous Impurity Distribution in ZnO Micropillars [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1021/nl049889y\"\n     onclick=\"log_download('nobis-kaidashev-rahm-lorenz-lenzner-grundmann-spatiallyinhomogeneousimpuritydistributioninznomicropillars-2004', 'http://doi.org/10.1021/nl049889y', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/nobis-kaidashev-rahm-lorenz-lenzner-grundmann-spatiallyinhomogeneousimpuritydistributioninznomicropillars-2004\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('nobis-kaidashev-rahm-lorenz-lenzner-grundmann-spatiallyinhomogeneousimpuritydistributioninznomicropillars-2004')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{nobis_spatially_2004,\n\ttitle = {Spatially {Inhomogeneous} {Impurity} {Distribution} in {ZnO} {Micropillars}},\n\tvolume = {4},\n\tissn = {1530-6984},\n\turl = {https://doi.org/10.1021/nl049889y},\n\tdoi = {10.1021/nl049889y},\n\tabstract = {Using ZnO a variety of micro- and nanostructures can be fabricated. We investigate hexagonal micropillars grown by high pressure pulsed laser deposition on sapphire with spatially and spectrally resolved cathodoluminescence. We demonstrate that the impurity and defect incorporation is strongly inhomogeneous, at least under the present growth conditions, dramatically influencing the optical properties.},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Nano Letters},\n\tauthor = {Nobis, Thomas and Kaidashev, Evgeni M. and Rahm, Andreas and Lorenz, Michael and Lenzner, Jörg and Grundmann, Marius},\n\tmonth = may,\n\tyear = {2004},\n\tnote = {Publisher: American Chemical Society},\n\tpages = {797--800},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Using ZnO a variety of micro- and nanostructures can be fabricated. We investigate hexagonal micropillars grown by high pressure pulsed laser deposition on sapphire with spatially and spectrally resolved cathodoluminescence. We demonstrate that the impurity and defect incorporation is strongly inhomogeneous, at least under the present growth conditions, dramatically influencing the optical properties.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"bundesmann-ashkenov-schubert-rahm-wenckstern-kaidashev-lorenz-grundmann-infrareddielectricfunctionsandcrystalorientationofaplaneznothinfilmsonrplanesapphiredeterminedbygeneralizedellipsometry-2004\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0040609003018285\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'bundesmann-ashkenov-schubert-rahm-wenckstern-kaidashev-lorenz-grundmann-infrareddielectricfunctionsandcrystalorientationofaplaneznothinfilmsonrplanesapphiredeterminedbygeneralizedellipsometry-2004', 'https://www.sciencedirect.com/science/article/pii/S0040609003018285', event);\">\n    Infrared dielectric functions and crystal orientation of a-plane ZnO thin films on r-plane sapphire determined by generalized ellipsometry.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Bundesmann, C.; Ashkenov, N.; Schubert, M.; Rahm, A.; Wenckstern, H. v.; Kaidashev, E. M.; Lorenz, M.;  and Grundmann, M.\n</span>\n\n  \n\n</span>\n\n  <i>Thin Solid Films</i>, 455-456: 161–166. May 2004.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0040609003018285\"\n     onclick=\"log_download('bundesmann-ashkenov-schubert-rahm-wenckstern-kaidashev-lorenz-grundmann-infrareddielectricfunctionsandcrystalorientationofaplaneznothinfilmsonrplanesapphiredeterminedbygeneralizedellipsometry-2004', 'https://www.sciencedirect.com/science/article/pii/S0040609003018285', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Infrared dielectric functions and crystal orientation of a-plane ZnO thin films on r-plane sapphire determined by generalized ellipsometry [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.tsf.2003.11.226\"\n     onclick=\"log_download('bundesmann-ashkenov-schubert-rahm-wenckstern-kaidashev-lorenz-grundmann-infrareddielectricfunctionsandcrystalorientationofaplaneznothinfilmsonrplanesapphiredeterminedbygeneralizedellipsometry-2004', 'http://doi.org/10.1016/j.tsf.2003.11.226', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/bundesmann-ashkenov-schubert-rahm-wenckstern-kaidashev-lorenz-grundmann-infrareddielectricfunctionsandcrystalorientationofaplaneznothinfilmsonrplanesapphiredeterminedbygeneralizedellipsometry-2004\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('bundesmann-ashkenov-schubert-rahm-wenckstern-kaidashev-lorenz-grundmann-infrareddielectricfunctionsandcrystalorientationofaplaneznothinfilmsonrplanesapphiredeterminedbygeneralizedellipsometry-2004')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{bundesmann_infrared_2004,\n\tseries = {The 3rd {International} {Conference} on {Spectroscopic} {Ellipsometry}},\n\ttitle = {Infrared dielectric functions and crystal orientation of a-plane {ZnO} thin films on r-plane sapphire determined by generalized ellipsometry},\n\tvolume = {455-456},\n\tissn = {0040-6090},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0040609003018285},\n\tdoi = {10.1016/j.tsf.2003.11.226},\n\tabstract = {Generalized infrared spectroscopic ellipsometry for wave numbers from 370 to 1200 cm−1 was applied to study the anisotropic dielectric response of wurtzite-type ZnO thin films grown on r-plane sapphire. Combined wavelength-by-wavelength analysis of data measured at multiple sample in-plane orientations allows for simultaneous extraction of the dielectric function (DF) tensor, the film thickness and the respective ZnO c-axis orientation, specifically in relation to the sapphire substrate. For anisotropic materials and use of generalized ellipsometry, the correlation problem between thickness and DF does not exist. Subsequent line shape analysis of ordinary and extraordinary DFs provides complete A1- and E1-symmetry longitudinal and transverse optical phonon-mode and broadening parameters, together with the static dielectric constants. The epitaxial relations from the ellipsometry data analysis are (11−20)ZnO∣∣(01−12)sapphire and [0001]ZnO∣∣[0−111]sapphire, which was confirmed by XRD measurements.},\n\turldate = {2023-11-11},\n\tjournal = {Thin Solid Films},\n\tauthor = {Bundesmann, C. and Ashkenov, N. and Schubert, M. and Rahm, A. and Wenckstern, H. v. and Kaidashev, E. M. and Lorenz, M. and Grundmann, M.},\n\tmonth = may,\n\tyear = {2004},\n\tkeywords = {-Plane ZnO, Epitaxial relation, Generalized infrared spectroscopic ellipsometry, Phonon modes},\n\tpages = {161--166},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Generalized infrared spectroscopic ellipsometry for wave numbers from 370 to 1200 cm−1 was applied to study the anisotropic dielectric response of wurtzite-type ZnO thin films grown on r-plane sapphire. Combined wavelength-by-wavelength analysis of data measured at multiple sample in-plane orientations allows for simultaneous extraction of the dielectric function (DF) tensor, the film thickness and the respective ZnO c-axis orientation, specifically in relation to the sapphire substrate. For anisotropic materials and use of generalized ellipsometry, the correlation problem between thickness and DF does not exist. Subsequent line shape analysis of ordinary and extraordinary DFs provides complete A1- and E1-symmetry longitudinal and transverse optical phonon-mode and broadening parameters, together with the static dielectric constants. The epitaxial relations from the ellipsometry data analysis are (11−20)ZnO∣∣(01−12)sapphire and [0001]ZnO∣∣[0−111]sapphire, which was confirmed by XRD measurements.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"das-yuzyuk-bhattacharya-gupta-katiyar-foldedacousticphononsandsoftmodedynamicsinbatiotextrm3srtiotextrm3superlattices-2004\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.69.132302\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'das-yuzyuk-bhattacharya-gupta-katiyar-foldedacousticphononsandsoftmodedynamicsinbatiotextrm3srtiotextrm3superlattices-2004', 'https://link.aps.org/doi/10.1103/PhysRevB.69.132302', event);\">\n    Folded acoustic phonons and soft mode dynamics in BaTiO$_{\\textrm{3}}$/SrTiO$_{\\textrm{3}}$ superlattices.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Das, R. R.; Yuzyuk, Y. I.; Bhattacharya, P.; Gupta, V.;  and Katiyar, R. S.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 69(13): 132302. April 2004.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.69.132302\"\n     onclick=\"log_download('das-yuzyuk-bhattacharya-gupta-katiyar-foldedacousticphononsandsoftmodedynamicsinbatiotextrm3srtiotextrm3superlattices-2004', 'https://link.aps.org/doi/10.1103/PhysRevB.69.132302', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Folded acoustic phonons and soft mode dynamics in BaTiO$_{\\textrm{3}}$/SrTiO$_{\\textrm{3}}$ superlattices [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.69.132302\"\n     onclick=\"log_download('das-yuzyuk-bhattacharya-gupta-katiyar-foldedacousticphononsandsoftmodedynamicsinbatiotextrm3srtiotextrm3superlattices-2004', 'http://doi.org/10.1103/PhysRevB.69.132302', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/das-yuzyuk-bhattacharya-gupta-katiyar-foldedacousticphononsandsoftmodedynamicsinbatiotextrm3srtiotextrm3superlattices-2004\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('das-yuzyuk-bhattacharya-gupta-katiyar-foldedacousticphononsandsoftmodedynamicsinbatiotextrm3srtiotextrm3superlattices-2004')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{das_folded_2004,\n\ttitle = {Folded acoustic phonons and soft mode dynamics in {BaTiO}$_{\\textrm{3}}$/{SrTiO}$_{\\textrm{3}}$ superlattices},\n\tvolume = {69},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.69.132302},\n\tdoi = {10.1103/PhysRevB.69.132302},\n\tabstract = {A series of BaTiO3/SrTiO3 superlattices with stacking periodicity of 6–10 unit cells were fabricated on (001)MgO substrates using pulsed-laser-deposition technique. Polarized Raman spectra revealed BaTiO3-like optical vibrations and confirmed tetragonal symmetry of the superlattices with the c axis being normal to the layers. Due to in-plane compressive stresses generated by the lattice mismatch of the constituting layers, the E(1TO) soft mode was underdamped and markedly shifted to higher frequencies with respect to its analogs in the bulk. The existence of perfect superlattice structure was evident from the observation of the folded acoustic phonons in Raman spectra. The frequencies of the folded phonons matched well with the calculated transverse-acoustic branches of the constituent materials. No phase transitions were revealed in the superlattices below room temperature, while phase transition to the paraelectric state is shifted up to 650–700 K and it is diffused.},\n\tnumber = {13},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Das, Rasmi R. and Yuzyuk, Yu. I. and Bhattacharya, P. and Gupta, V. and Katiyar, R. S.},\n\tmonth = apr,\n\tyear = {2004},\n\tnote = {Publisher: American Physical Society},\n\tpages = {132302},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A series of BaTiO3/SrTiO3 superlattices with stacking periodicity of 6–10 unit cells were fabricated on (001)MgO substrates using pulsed-laser-deposition technique. Polarized Raman spectra revealed BaTiO3-like optical vibrations and confirmed tetragonal symmetry of the superlattices with the c axis being normal to the layers. Due to in-plane compressive stresses generated by the lattice mismatch of the constituting layers, the E(1TO) soft mode was underdamped and markedly shifted to higher frequencies with respect to its analogs in the bulk. The existence of perfect superlattice structure was evident from the observation of the folded acoustic phonons in Raman spectra. The frequencies of the folded phonons matched well with the calculated transverse-acoustic branches of the constituent materials. No phase transitions were revealed in the superlattices below room temperature, while phase transition to the paraelectric state is shifted up to 650–700 K and it is diffused.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"gupta-bhattacharya-yuzyuk-katiyar-tomar-sreenivas-growthandcharacterizationofcaxisorientedlinbotextrm3filmonatransparentconductingalznointerlayeronsi-2004\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1557/JMR.2004.0322\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'gupta-bhattacharya-yuzyuk-katiyar-tomar-sreenivas-growthandcharacterizationofcaxisorientedlinbotextrm3filmonatransparentconductingalznointerlayeronsi-2004', 'https://doi.org/10.1557/JMR.2004.0322', event);\">\n    Growth and characterization of c-axis oriented LiNbO$_{\\textrm{3}}$ film on a transparent conducting Al:ZnO inter-layer on Si.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Gupta, V.; Bhattacharya, P.; Yuzyuk, Y. I.; Katiyar, R. S.; Tomar, M.;  and Sreenivas, K.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Materials Research</i>, 19(8): 2235–2239. August 2004.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1557/JMR.2004.0322\"\n     onclick=\"log_download('gupta-bhattacharya-yuzyuk-katiyar-tomar-sreenivas-growthandcharacterizationofcaxisorientedlinbotextrm3filmonatransparentconductingalznointerlayeronsi-2004', 'https://doi.org/10.1557/JMR.2004.0322', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Growth and characterization of c-axis oriented LiNbO$_{\\textrm{3}}$ film on a transparent conducting Al:ZnO inter-layer on Si [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1557/JMR.2004.0322\"\n     onclick=\"log_download('gupta-bhattacharya-yuzyuk-katiyar-tomar-sreenivas-growthandcharacterizationofcaxisorientedlinbotextrm3filmonatransparentconductingalznointerlayeronsi-2004', 'http://doi.org/10.1557/JMR.2004.0322', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/gupta-bhattacharya-yuzyuk-katiyar-tomar-sreenivas-growthandcharacterizationofcaxisorientedlinbotextrm3filmonatransparentconductingalznointerlayeronsi-2004\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('gupta-bhattacharya-yuzyuk-katiyar-tomar-sreenivas-growthandcharacterizationofcaxisorientedlinbotextrm3filmonatransparentconductingalznointerlayeronsi-2004')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{gupta_growth_2004,\n\ttitle = {Growth and characterization of c-axis oriented {LiNbO}$_{\\textrm{3}}$ film on a transparent conducting {Al}:{ZnO} inter-layer on {Si}},\n\tvolume = {19},\n\tissn = {2044-5326},\n\tshorttitle = {Growth and characterization of c-axis oriented {LiNbO3} film on a transparent conducting {Al}},\n\turl = {https://doi.org/10.1557/JMR.2004.0322},\n\tdoi = {10.1557/JMR.2004.0322},\n\tabstract = {C-axis oriented lithium niobate (LiNbO3) films were deposited by pulsed-laser deposition on silicon using a transparent conducting interlayer of aluminum (Al)-doped zinc oxide (ZnO). Only two x-ray diffraction reflections corresponding to (006) and (0012) planes of LiNbO3 were observed in the films deposited at a 100-mTorr oxygen pressure and a 450–500 °C substrate temperature. Presence of sharp modes corresponding to E(TO) and A(LO), and absence of any superfluous peaks mainly around 900–905 cm−1 in the Raman spectra confirmed the formation of textured LiNbO3 film. Measured value of direct current and alternate current (AC) conductivities and dielectric constant are 8.6 × 10-12 Ω−1cm-1, 1.16 × 10-6 Ω−1cm-1, and 29.3, respectively, at room temperature. Behavior of dielectric constant and AC conductivity with frequency and temperature are close to the reported single-crystal data.},\n\tlanguage = {en},\n\tnumber = {8},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Materials Research},\n\tauthor = {Gupta, Vinay and Bhattacharya, P. and Yuzyuk, Yu. I. and Katiyar, R. S. and Tomar, Monika and Sreenivas, K.},\n\tmonth = aug,\n\tyear = {2004},\n\tpages = {2235--2239},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  C-axis oriented lithium niobate (LiNbO3) films were deposited by pulsed-laser deposition on silicon using a transparent conducting interlayer of aluminum (Al)-doped zinc oxide (ZnO). Only two x-ray diffraction reflections corresponding to (006) and (0012) planes of LiNbO3 were observed in the films deposited at a 100-mTorr oxygen pressure and a 450–500 °C substrate temperature. Presence of sharp modes corresponding to E(TO) and A(LO), and absence of any superfluous peaks mainly around 900–905 cm−1 in the Raman spectra confirmed the formation of textured LiNbO3 film. Measured value of direct current and alternate current (AC) conductivities and dielectric constant are 8.6 × 10-12 Ω−1cm-1, 1.16 × 10-6 Ω−1cm-1, and 29.3, respectively, at room temperature. Behavior of dielectric constant and AC conductivity with frequency and temperature are close to the reported single-crystal data.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kholkin-bdikin-yuzyuk-almeida-chaves-calzada-mendiola-ramanscatteringinsolgelderivedpbtiotextrm3filmsmodifiedwithca-2004\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S025405840400029X\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kholkin-bdikin-yuzyuk-almeida-chaves-calzada-mendiola-ramanscatteringinsolgelderivedpbtiotextrm3filmsmodifiedwithca-2004', 'https://www.sciencedirect.com/science/article/pii/S025405840400029X', event);\">\n    Raman scattering in sol–gel derived PbTiO$_{\\textrm{3}}$ films modified with Ca.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kholkin, A. L; Bdikin, I; Yuzyuk, Y. I; Almeida, A; Chaves, M. R; Calzada, M. L;  and Mendiola, J\n</span>\n\n  \n\n</span>\n\n  <i>Materials Chemistry and Physics</i>, 85(1): 176–179. May 2004.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S025405840400029X\"\n     onclick=\"log_download('kholkin-bdikin-yuzyuk-almeida-chaves-calzada-mendiola-ramanscatteringinsolgelderivedpbtiotextrm3filmsmodifiedwithca-2004', 'https://www.sciencedirect.com/science/article/pii/S025405840400029X', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Raman scattering in sol–gel derived PbTiO$_{\\textrm{3}}$ films modified with Ca [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.matchemphys.2004.01.001\"\n     onclick=\"log_download('kholkin-bdikin-yuzyuk-almeida-chaves-calzada-mendiola-ramanscatteringinsolgelderivedpbtiotextrm3filmsmodifiedwithca-2004', 'http://doi.org/10.1016/j.matchemphys.2004.01.001', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kholkin-bdikin-yuzyuk-almeida-chaves-calzada-mendiola-ramanscatteringinsolgelderivedpbtiotextrm3filmsmodifiedwithca-2004\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kholkin-bdikin-yuzyuk-almeida-chaves-calzada-mendiola-ramanscatteringinsolgelderivedpbtiotextrm3filmsmodifiedwithca-2004')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kholkin_raman_2004,\n\ttitle = {Raman scattering in sol–gel derived {PbTiO}$_{\\textrm{3}}$ films modified with {Ca}},\n\tvolume = {85},\n\tissn = {0254-0584},\n\turl = {https://www.sciencedirect.com/science/article/pii/S025405840400029X},\n\tdoi = {10.1016/j.matchemphys.2004.01.001},\n\tabstract = {X-ray diffraction (XRD) and Raman scattering in sol–gel derived Pb1−xCaxTiO3 (PCT) thin films are studied as a function of Ca content x. It is found that Ca2+ addition to PbTiO3 films results in a gradual decrease of tetragonality of the perovskite lattice accompanied with a considerable modification of the Raman spectra. A significant difference in Raman spectra of PCT films and available reference data for single crystals (x=0) is explained in terms of the large internal stress, small grain size, and structural disorder produced by Ca2+ substitution. It is found that the shift of the frequency of ferroelectric soft mode correlates well with the variation of tetragonality for x≤xc=0.4. The concentration dependence of the shift is strongly non-linear being qualitatively different from that observed earlier in other A-site doped lead titanate-based systems. According to XRD data, the averaged crystal structure for xc≈0.4 appears as pseudo-cubic, while Raman scattering revealed short-range order tetragonal distortion. The structural characteristics of PCT films are linked to their electromechanical properties measured earlier by interferometric technique.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Materials Chemistry and Physics},\n\tauthor = {Kholkin, A. L and Bdikin, I and Yuzyuk, Yu. I and Almeida, A and Chaves, M. R and Calzada, M. L and Mendiola, J},\n\tmonth = may,\n\tyear = {2004},\n\tkeywords = {Ferroelectricity, Thin films, Raman spectroscopy and scattering, Sol–gel growth},\n\tpages = {176--179},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  X-ray diffraction (XRD) and Raman scattering in sol–gel derived Pb1−xCaxTiO3 (PCT) thin films are studied as a function of Ca content x. It is found that Ca2+ addition to PbTiO3 films results in a gradual decrease of tetragonality of the perovskite lattice accompanied with a considerable modification of the Raman spectra. A significant difference in Raman spectra of PCT films and available reference data for single crystals (x=0) is explained in terms of the large internal stress, small grain size, and structural disorder produced by Ca2+ substitution. It is found that the shift of the frequency of ferroelectric soft mode correlates well with the variation of tetragonality for x≤xc=0.4. The concentration dependence of the shift is strongly non-linear being qualitatively different from that observed earlier in other A-site doped lead titanate-based systems. According to XRD data, the averaged crystal structure for xc≈0.4 appears as pseudo-cubic, while Raman scattering revealed short-range order tetragonal distortion. The structural characteristics of PCT films are linked to their electromechanical properties measured earlier by interferometric technique.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"korolkov-kaidashev-abdulvakhidov-kupriyanov-nanodimensionaleffectsinthestructureofepitaxialybatextrm2cutextrm3otextrm7yfilms-2004\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/1.1666963\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'korolkov-kaidashev-abdulvakhidov-kupriyanov-nanodimensionaleffectsinthestructureofepitaxialybatextrm2cutextrm3otextrm7yfilms-2004', 'https://doi.org/10.1134/1.1666963', event);\">\n    Nanodimensional effects in the structure of epitaxial YBa$_{\\textrm{2}}$Cu$_{\\textrm{3}}$O$_{\\textrm{7-y}}$ films.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Korol’kov, D. S.; Kaidashev, E. M.; Abdulvakhidov, K. G.;  and Kupriyanov, M. F.\n</span>\n\n  \n\n</span>\n\n  <i>Technical Physics Letters</i>, 30(2): 135–137. February 2004.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/1.1666963\"\n     onclick=\"log_download('korolkov-kaidashev-abdulvakhidov-kupriyanov-nanodimensionaleffectsinthestructureofepitaxialybatextrm2cutextrm3otextrm7yfilms-2004', 'https://doi.org/10.1134/1.1666963', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Nanodimensional effects in the structure of epitaxial YBa$_{\\textrm{2}}$Cu$_{\\textrm{3}}$O$_{\\textrm{7-y}}$ films [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/1.1666963\"\n     onclick=\"log_download('korolkov-kaidashev-abdulvakhidov-kupriyanov-nanodimensionaleffectsinthestructureofepitaxialybatextrm2cutextrm3otextrm7yfilms-2004', 'http://doi.org/10.1134/1.1666963', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/korolkov-kaidashev-abdulvakhidov-kupriyanov-nanodimensionaleffectsinthestructureofepitaxialybatextrm2cutextrm3otextrm7yfilms-2004\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('korolkov-kaidashev-abdulvakhidov-kupriyanov-nanodimensionaleffectsinthestructureofepitaxialybatextrm2cutextrm3otextrm7yfilms-2004')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{korolkov_nanodimensional_2004,\n\ttitle = {Nanodimensional effects in the structure of epitaxial {YBa}$_{\\textrm{2}}${Cu}$_{\\textrm{3}}${O}$_{\\textrm{7-y}}$ films},\n\tvolume = {30},\n\tissn = {1090-6533},\n\turl = {https://doi.org/10.1134/1.1666963},\n\tdoi = {10.1134/1.1666963},\n\tabstract = {We have studied the structure of YBa2Cu3O7−y(YBCO) high-Tcsuperconductor films obtained by deposition for various times under otherwise identical conditions. Thin YBCO films prepared by the nonaxial laser shadow deposition technique are epitaxial and have microstrains below 1×10−3. The main factor determining variations of the unit cell parameter c in the films is the difference of the crystal block size 〈D〉 in the direction normal to the film surface, which reflects the nanodimensional effects known in oxides.},\n\tlanguage = {en},\n\tnumber = {2},\n\turldate = {2023-11-11},\n\tjournal = {Technical Physics Letters},\n\tauthor = {Korol’kov, D. S. and Kaidashev, E. M. and Abdulvakhidov, K. G. and Kupriyanov, M. F.},\n\tmonth = feb,\n\tyear = {2004},\n\tkeywords = {Block Size, Cell Parameter, Film Surface, Identical Condition, Oxide},\n\tpages = {135--137},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We have studied the structure of YBa2Cu3O7−y(YBCO) high-Tcsuperconductor films obtained by deposition for various times under otherwise identical conditions. Thin YBCO films prepared by the nonaxial laser shadow deposition technique are epitaxial and have microstrains below 1×10−3. The main factor determining variations of the unit cell parameter c in the films is the difference of the crystal block size 〈D〉 in the direction normal to the film surface, which reflects the nanodimensional effects known in oxides.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"prosandeev-cockayne-burton-kamba-petzelt-yuzyuk-katiyar-vakhrushev-latticedynamicsinpbmgtextrm13nbtextrm23otextrm3-2004\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.70.134110\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'prosandeev-cockayne-burton-kamba-petzelt-yuzyuk-katiyar-vakhrushev-latticedynamicsinpbmgtextrm13nbtextrm23otextrm3-2004', 'https://link.aps.org/doi/10.1103/PhysRevB.70.134110', event);\">\n    Lattice dynamics in PbMg$_{\\textrm{1/3}}$Nb$_{\\textrm{2/3}}$O$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Prosandeev, S. A.; Cockayne, E.; Burton, B. P.; Kamba, S.; Petzelt, J.; Yuzyuk, Y.; Katiyar, R. S.;  and Vakhrushev, S. B.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 70(13): 134110. October 2004.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.70.134110\"\n     onclick=\"log_download('prosandeev-cockayne-burton-kamba-petzelt-yuzyuk-katiyar-vakhrushev-latticedynamicsinpbmgtextrm13nbtextrm23otextrm3-2004', 'https://link.aps.org/doi/10.1103/PhysRevB.70.134110', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Lattice dynamics in PbMg$_{\\textrm{1/3}}$Nb$_{\\textrm{2/3}}$O$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.70.134110\"\n     onclick=\"log_download('prosandeev-cockayne-burton-kamba-petzelt-yuzyuk-katiyar-vakhrushev-latticedynamicsinpbmgtextrm13nbtextrm23otextrm3-2004', 'http://doi.org/10.1103/PhysRevB.70.134110', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/prosandeev-cockayne-burton-kamba-petzelt-yuzyuk-katiyar-vakhrushev-latticedynamicsinpbmgtextrm13nbtextrm23otextrm3-2004\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('prosandeev-cockayne-burton-kamba-petzelt-yuzyuk-katiyar-vakhrushev-latticedynamicsinpbmgtextrm13nbtextrm23otextrm3-2004')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{prosandeev_lattice_2004,\n\ttitle = {Lattice dynamics in {PbMg}$_{\\textrm{1/3}}${Nb}$_{\\textrm{2/3}}${O}$_{\\textrm{3}}$},\n\tvolume = {70},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.70.134110},\n\tdoi = {10.1103/PhysRevB.70.134110},\n\tabstract = {Lattice dynamics for five ordered PbMg1∕3Nb2∕3O3 supercells were calculated from first principles by the frozen phonon method. Maximal symmetries of all supercells are reduced by structural instabilities. Lattice modes corresponding to these instabilities, equilibrium ionic positions, and infrared reflectivity spectra were computed for all supercells. Results are compared with our experimental data for a chemically disordered PMN single crystal.},\n\tnumber = {13},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Prosandeev, S. A. and Cockayne, E. and Burton, B. P. and Kamba, S. and Petzelt, J. and Yuzyuk, Yu. and Katiyar, R. S. and Vakhrushev, S. B.},\n\tmonth = oct,\n\tyear = {2004},\n\tnote = {Publisher: American Physical Society},\n\tpages = {134110},\n\tfile = {Отправленная версия:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\GZG82Z22\\\\Prosandeev и др. - 2004 - Lattice dynamics in \\$ mathrm PbMg _ 1∕3 mathrm.pdf:application/pdf;APS Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\T9HNHJSG\\\\PhysRevB.70.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Lattice dynamics for five ordered PbMg1∕3Nb2∕3O3 supercells were calculated from first principles by the frozen phonon method. Maximal symmetries of all supercells are reduced by structural instabilities. Lattice modes corresponding to these instabilities, equilibrium ionic positions, and infrared reflectivity spectra were computed for all supercells. Results are compared with our experimental data for a chemically disordered PMN single crystal.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"schmidtgrund-schubert-rheinlnder-fritsch-schmidt-kaidashev-lorenz-herzinger-etal-uvvuvspectroscopicellipsometryofternarymgtextrmxzntextrm1xo0x053thinfilms-2004\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S004060900301856X\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'schmidtgrund-schubert-rheinlnder-fritsch-schmidt-kaidashev-lorenz-herzinger-etal-uvvuvspectroscopicellipsometryofternarymgtextrmxzntextrm1xo0x053thinfilms-2004', 'https://www.sciencedirect.com/science/article/pii/S004060900301856X', event);\">\n    UV–VUV spectroscopic ellipsometry of ternary Mg$_{\\textrm{x}}$Zn$_{\\textrm{1−x}}$O (0≤x≤0.53) thin films.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Schmidt-Grund, R.; Schubert, M.; Rheinländer, B.; Fritsch, D.; Schmidt, H.; Kaidashev, E. M.; Lorenz, M.; Herzinger, C. M.;  and Grundmann, M.\n</span>\n\n  \n\n</span>\n\n  <i>Thin Solid Films</i>, 455-456: 500–504. May 2004.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S004060900301856X\"\n     onclick=\"log_download('schmidtgrund-schubert-rheinlnder-fritsch-schmidt-kaidashev-lorenz-herzinger-etal-uvvuvspectroscopicellipsometryofternarymgtextrmxzntextrm1xo0x053thinfilms-2004', 'https://www.sciencedirect.com/science/article/pii/S004060900301856X', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"UV–VUV spectroscopic ellipsometry of ternary Mg$_{\\textrm{x}}$Zn$_{\\textrm{1−x}}$O (0≤x≤0.53) thin films [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.tsf.2003.11.249\"\n     onclick=\"log_download('schmidtgrund-schubert-rheinlnder-fritsch-schmidt-kaidashev-lorenz-herzinger-etal-uvvuvspectroscopicellipsometryofternarymgtextrmxzntextrm1xo0x053thinfilms-2004', 'http://doi.org/10.1016/j.tsf.2003.11.249', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/schmidtgrund-schubert-rheinlnder-fritsch-schmidt-kaidashev-lorenz-herzinger-etal-uvvuvspectroscopicellipsometryofternarymgtextrmxzntextrm1xo0x053thinfilms-2004\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('schmidtgrund-schubert-rheinlnder-fritsch-schmidt-kaidashev-lorenz-herzinger-etal-uvvuvspectroscopicellipsometryofternarymgtextrmxzntextrm1xo0x053thinfilms-2004')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{schmidt-grund_uvvuv_2004,\n\tseries = {The 3rd {International} {Conference} on {Spectroscopic} {Ellipsometry}},\n\ttitle = {{UV}–{VUV} spectroscopic ellipsometry of ternary {Mg}$_{\\textrm{x}}${Zn}$_{\\textrm{1−x}}${O} (0≤x≤0.53) thin films},\n\tvolume = {455-456},\n\tissn = {0040-6090},\n\turl = {https://www.sciencedirect.com/science/article/pii/S004060900301856X},\n\tdoi = {10.1016/j.tsf.2003.11.249},\n\tabstract = {The ordinary optical dielectric functions of pulsed-laser-deposition grown wurtzite c-plane MgxZn1−xO (0≤x≤0.53) thin films have been determined by using spectroscopic ellipsometry in the photon energy range from 4.5 to 9.5 eV. The dielectric functions reveal features which resemble those previously detected in uniaxial AlGaN and identified as E1- and E2-type band-to-band transitions with no remarkable dependence of the transition energy on Mg content x. The E1- and E2-type transitions for ZnO are compared with pseudopotential band-structure calculations.},\n\turldate = {2023-11-11},\n\tjournal = {Thin Solid Films},\n\tauthor = {Schmidt-Grund, R. and Schubert, M. and Rheinländer, B. and Fritsch, D. and Schmidt, H. and Kaidashev, E. M. and Lorenz, M. and Herzinger, C. M. and Grundmann, M.},\n\tmonth = may,\n\tyear = {2004},\n\tkeywords = {Optical properties, Dielectric function, Ellipsometry, MgZnO, Vacuum ultraviolet, Zinc oxide (ZnO), ZnMgO},\n\tpages = {500--504},\n\tfile = {ScienceDirect Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\E97NUBSQ\\\\S004060900301856X.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The ordinary optical dielectric functions of pulsed-laser-deposition grown wurtzite c-plane MgxZn1−xO (0≤x≤0.53) thin films have been determined by using spectroscopic ellipsometry in the photon energy range from 4.5 to 9.5 eV. The dielectric functions reveal features which resemble those previously detected in uniaxial AlGaN and identified as E1- and E2-type band-to-band transitions with no remarkable dependence of the transition energy on Mg content x. The E1- and E2-type transitions for ZnO are compared with pseudopotential band-structure calculations.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"spemann-kaidashev-lorenz-vogt-butz-ionbeamanalysisofepitaxialmgcdtextrmxzntextrm1xoandznolialgasbthinfilmsgrownoncplanesapphire-2004\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0168583X0400223X\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'spemann-kaidashev-lorenz-vogt-butz-ionbeamanalysisofepitaxialmgcdtextrmxzntextrm1xoandznolialgasbthinfilmsgrownoncplanesapphire-2004', 'https://www.sciencedirect.com/science/article/pii/S0168583X0400223X', event);\">\n    Ion beam analysis of epitaxial (Mg, Cd)$_{\\textrm{x}}$Zn$_{\\textrm{1−x}}$O and ZnO:(Li, Al, Ga, Sb) thin films grown on c-plane sapphire.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Spemann, D; Kaidashev, E. M; Lorenz, M; Vogt, J;  and Butz, T\n</span>\n\n  \n\n</span>\n\n  <i>Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms</i>, 219-220: 891–896. June 2004.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0168583X0400223X\"\n     onclick=\"log_download('spemann-kaidashev-lorenz-vogt-butz-ionbeamanalysisofepitaxialmgcdtextrmxzntextrm1xoandznolialgasbthinfilmsgrownoncplanesapphire-2004', 'https://www.sciencedirect.com/science/article/pii/S0168583X0400223X', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Ion beam analysis of epitaxial (Mg, Cd)$_{\\textrm{x}}$Zn$_{\\textrm{1−x}}$O and ZnO:(Li, Al, Ga, Sb) thin films grown on c-plane sapphire [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/j.nimb.2004.01.183\"\n     onclick=\"log_download('spemann-kaidashev-lorenz-vogt-butz-ionbeamanalysisofepitaxialmgcdtextrmxzntextrm1xoandznolialgasbthinfilmsgrownoncplanesapphire-2004', 'http://doi.org/10.1016/j.nimb.2004.01.183', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/spemann-kaidashev-lorenz-vogt-butz-ionbeamanalysisofepitaxialmgcdtextrmxzntextrm1xoandznolialgasbthinfilmsgrownoncplanesapphire-2004\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('spemann-kaidashev-lorenz-vogt-butz-ionbeamanalysisofepitaxialmgcdtextrmxzntextrm1xoandznolialgasbthinfilmsgrownoncplanesapphire-2004')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{spemann_ion_2004,\n\tseries = {Proceedings of the {Sixteenth} {International} {Conference} on {Ion} {Beam} {Analysis}},\n\ttitle = {Ion beam analysis of epitaxial ({Mg}, {Cd})$_{\\textrm{x}}${Zn}$_{\\textrm{1−x}}${O} and {ZnO}:({Li}, {Al}, {Ga}, {Sb}) thin films grown on c-plane sapphire},\n\tvolume = {219-220},\n\tissn = {0168-583X},\n\tshorttitle = {Ion beam analysis of epitaxial ({Mg}, {Cd}){xZn1}−{xO} and {ZnO}},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0168583X0400223X},\n\tdoi = {10.1016/j.nimb.2004.01.183},\n\tabstract = {In this study ZnO thin films, nominally undoped, doped with Li, Al, Ga and Sb and alloyed with Mg and Cd grown epitaxially on c-plane sapphire by pulsed laser deposition (PLD) were investigated. In order to correlate the optical and electrical properties, e.g. the band gap energy and carrier concentration, to the elemental composition, the films were analyzed by RBS, PIXE and PIGE using He+ and H+ ion beams. It was found that the element transfer from the PLD target to the film differs significantly for the individual doping and alloying elements, with concentration ratios between film and target ranging from ∼4\\% for Li and Cd to ∼400\\% for Ga. In general, the films exhibited a metal to oxygen ratio of 1:1, only the ZnO:Li films were slightly oxygen deficient. Furthermore, the crystalline quality of the films was investigated using ion channeling. The nominally undoped ZnO films which were deposited with low-temperature interlayers for lower lateral stress showed a normalized minimum RBS yield of χmin=3.3\\% under channeling conditions. Whereas the incorporation of isovalent alloying atoms into the ZnO films leads to a slight degradation of the crystalline quality only, doping degrades the crystalline quality remarkably, even at low dopant concentrations.},\n\turldate = {2023-11-11},\n\tjournal = {Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms},\n\tauthor = {Spemann, D and Kaidashev, E. M and Lorenz, M and Vogt, J and Butz, T},\n\tmonth = jun,\n\tyear = {2004},\n\tkeywords = {Elemental composition, Thin films, Zinc oxide, Crystalline quality},\n\tpages = {891--896},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  In this study ZnO thin films, nominally undoped, doped with Li, Al, Ga and Sb and alloyed with Mg and Cd grown epitaxially on c-plane sapphire by pulsed laser deposition (PLD) were investigated. In order to correlate the optical and electrical properties, e.g. the band gap energy and carrier concentration, to the elemental composition, the films were analyzed by RBS, PIXE and PIGE using He+ and H+ ion beams. It was found that the element transfer from the PLD target to the film differs significantly for the individual doping and alloying elements, with concentration ratios between film and target ranging from ∼4% for Li and Cd to ∼400% for Ga. In general, the films exhibited a metal to oxygen ratio of 1:1, only the ZnO:Li films were slightly oxygen deficient. Furthermore, the crystalline quality of the films was investigated using ion channeling. The nominally undoped ZnO films which were deposited with low-temperature interlayers for lower lateral stress showed a normalized minimum RBS yield of χmin=3.3% under channeling conditions. Whereas the incorporation of isovalent alloying atoms into the ZnO films leads to a slight degradation of the crystalline quality only, doping degrades the crystalline quality remarkably, even at low dopant concentrations.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"yuzyuk-gagarina-simon-reznitchenko-hennet-thiaudire-synchrotronxraydiffractionandramanscatteringinvestigationsoflitextrmxnatextrm1xnbotextrm3solidsolutionsevidenceoftherhombohedralphase-2004\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.69.144105\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'yuzyuk-gagarina-simon-reznitchenko-hennet-thiaudire-synchrotronxraydiffractionandramanscatteringinvestigationsoflitextrmxnatextrm1xnbotextrm3solidsolutionsevidenceoftherhombohedralphase-2004', 'https://link.aps.org/doi/10.1103/PhysRevB.69.144105', event);\">\n    Synchrotron x-ray diffraction and Raman scattering investigations of (Li$_{\\textrm{x}}$Na$_{\\textrm{1-x}}$)NbO$_{\\textrm{3}}$ solid solutions: Evidence of the rhombohedral phase.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Yuzyuk, Y. I.; Gagarina, E.; Simon, P.; Reznitchenko, L. A.; Hennet, L.;  and Thiaudière, D.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 69(14): 144105. April 2004.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.69.144105\"\n     onclick=\"log_download('yuzyuk-gagarina-simon-reznitchenko-hennet-thiaudire-synchrotronxraydiffractionandramanscatteringinvestigationsoflitextrmxnatextrm1xnbotextrm3solidsolutionsevidenceoftherhombohedralphase-2004', 'https://link.aps.org/doi/10.1103/PhysRevB.69.144105', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Synchrotron x-ray diffraction and Raman scattering investigations of (Li$_{\\textrm{x}}$Na$_{\\textrm{1-x}}$)NbO$_{\\textrm{3}}$ solid solutions: Evidence of the rhombohedral phase [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.69.144105\"\n     onclick=\"log_download('yuzyuk-gagarina-simon-reznitchenko-hennet-thiaudire-synchrotronxraydiffractionandramanscatteringinvestigationsoflitextrmxnatextrm1xnbotextrm3solidsolutionsevidenceoftherhombohedralphase-2004', 'http://doi.org/10.1103/PhysRevB.69.144105', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/yuzyuk-gagarina-simon-reznitchenko-hennet-thiaudire-synchrotronxraydiffractionandramanscatteringinvestigationsoflitextrmxnatextrm1xnbotextrm3solidsolutionsevidenceoftherhombohedralphase-2004\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('yuzyuk-gagarina-simon-reznitchenko-hennet-thiaudire-synchrotronxraydiffractionandramanscatteringinvestigationsoflitextrmxnatextrm1xnbotextrm3solidsolutionsevidenceoftherhombohedralphase-2004')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{yuzyuk_synchrotron_2004,\n\ttitle = {Synchrotron x-ray diffraction and {Raman} scattering investigations of ({Li}$_{\\textrm{x}}${Na}$_{\\textrm{1-x}}$){NbO}$_{\\textrm{3}}$ solid solutions: {Evidence} of the rhombohedral phase},\n\tvolume = {69},\n\tshorttitle = {Synchrotron x-ray diffraction and {Raman} scattering investigations of \\$(\\{{\\textbackslash}mathrm\\{{Li}\\}\\}\\_\\{x\\}\\{{\\textbackslash}mathrm\\{{Na}\\}\\}\\_\\{1{\\textbackslash}ensuremath\\{-\\}x\\})\\{{\\textbackslash}mathrm\\{{NbO}\\}\\}\\_\\{3\\}\\$ solid solutions},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.69.144105},\n\tdoi = {10.1103/PhysRevB.69.144105},\n\tabstract = {The (LixNa1−x)NbO3 perovskite solid solutions are investigated using synchrotron x-ray diffraction and Raman spectroscopy in order to clarify the structural changes in the concentration range 0{\\textless}{\\textasciitilde}x{\\textless}{\\textasciitilde}0.145 at room temperature. The orthorhombic antiferroelectric P phase (space group Pbma, Z=8) exists up to x=0.02 and in the concentration interval 0.02{\\textless}{\\textasciitilde}x{\\textless}{\\textasciitilde}0.03 we have confirmed a previously reported transition to the orthorhombic ferroelectric Q phase (space group P21ma, Z=4). It is found that the Q phase is stable up to x=0.145 but in the narrow concentration interval at x=0.12 the dominating (86.2\\%) rhombohedral N phase (space group R3c, Z=2) coexists with the minor (13.8\\%) Q phase at room temperature. The crystal structure of this rhombohedral N phase has been refined using Rietveld method. Detailed comparison with similar low-temperature phase of pure NaNbO3 showed that the NbO6 octahedra are slightly distorted in the solid solution with x=0.12 while they are rather regular in NaNbO3. Raman spectra showed drastic changes associated with the P−Q transition and revealed coexistence of the P and Q phases in the interval 0.02{\\textless}{\\textasciitilde}x{\\textless}{\\textasciitilde}0.03. Abrupt transformation of the Raman response and remarkable narrowing of the Nb-O stretching vibrations related to the existence of the rhombohedral N phase at x=0.12 were observed.},\n\tnumber = {14},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Yuzyuk, Yu. I. and Gagarina, E. and Simon, P. and Reznitchenko, L. A. and Hennet, L. and Thiaudière, D.},\n\tmonth = apr,\n\tyear = {2004},\n\tnote = {Publisher: American Physical Society},\n\tpages = {144105},\n\tfile = {APS Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\BS8JEKPQ\\\\PhysRevB.69.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The (LixNa1−x)NbO3 perovskite solid solutions are investigated using synchrotron x-ray diffraction and Raman spectroscopy in order to clarify the structural changes in the concentration range 0\\textless~x\\textless~0.145 at room temperature. The orthorhombic antiferroelectric P phase (space group Pbma, Z=8) exists up to x=0.02 and in the concentration interval 0.02\\textless~x\\textless~0.03 we have confirmed a previously reported transition to the orthorhombic ferroelectric Q phase (space group P21ma, Z=4). It is found that the Q phase is stable up to x=0.145 but in the narrow concentration interval at x=0.12 the dominating (86.2%) rhombohedral N phase (space group R3c, Z=2) coexists with the minor (13.8%) Q phase at room temperature. The crystal structure of this rhombohedral N phase has been refined using Rietveld method. Detailed comparison with similar low-temperature phase of pure NaNbO3 showed that the NbO6 octahedra are slightly distorted in the solid solution with x=0.12 while they are rather regular in NaNbO3. Raman spectra showed drastic changes associated with the P−Q transition and revealed coexistence of the P and Q phases in the interval 0.02\\textless~x\\textless~0.03. Abrupt transformation of the Raman response and remarkable narrowing of the Nb-O stretching vibrations related to the existence of the rhombohedral N phase at x=0.12 were observed.\n</div>\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2003\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2003')\"\n      onkeypress=\"toggleGroup('group_2003')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2003</span>\n      <span class=\"bibbase_group_count\">\n        \n        (9)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"vonwenckstern-kaidashev-lorenz-hochmuth-biehne-lenzner-gottschalch-pickenhain-etal-lateralhomogeneityofschottkycontactsonntypezno-2003\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.1638898\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'vonwenckstern-kaidashev-lorenz-hochmuth-biehne-lenzner-gottschalch-pickenhain-etal-lateralhomogeneityofschottkycontactsonntypezno-2003', 'https://doi.org/10.1063/1.1638898', event);\">\n    Lateral homogeneity of Schottky contacts on n-type ZnO.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  von Wenckstern, H.; Kaidashev, E. M.; Lorenz, M.; Hochmuth, H.; Biehne, G.; Lenzner, J.; Gottschalch, V.; Pickenhain, R.;  and Grundmann, M.\n</span>\n\n  \n\n</span>\n\n  <i>Applied Physics Letters</i>, 84(1): 79–81. December 2003.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.1638898\"\n     onclick=\"log_download('vonwenckstern-kaidashev-lorenz-hochmuth-biehne-lenzner-gottschalch-pickenhain-etal-lateralhomogeneityofschottkycontactsonntypezno-2003', 'https://doi.org/10.1063/1.1638898', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Lateral homogeneity of Schottky contacts on n-type ZnO [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.1638898\"\n     onclick=\"log_download('vonwenckstern-kaidashev-lorenz-hochmuth-biehne-lenzner-gottschalch-pickenhain-etal-lateralhomogeneityofschottkycontactsonntypezno-2003', 'http://doi.org/10.1063/1.1638898', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/vonwenckstern-kaidashev-lorenz-hochmuth-biehne-lenzner-gottschalch-pickenhain-etal-lateralhomogeneityofschottkycontactsonntypezno-2003\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('vonwenckstern-kaidashev-lorenz-hochmuth-biehne-lenzner-gottschalch-pickenhain-etal-lateralhomogeneityofschottkycontactsonntypezno-2003')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{von_wenckstern_lateral_2003,\n\ttitle = {Lateral homogeneity of {Schottky} contacts on n-type {ZnO}},\n\tvolume = {84},\n\tissn = {0003-6951},\n\turl = {https://doi.org/10.1063/1.1638898},\n\tdoi = {10.1063/1.1638898},\n\tabstract = {The electrical properties of Schottky contacts (SCs) produced ex situ on n-type ZnO single crystals and epitaxial thin films were investigated. Electron beam induced current imaging was used to study lateral variations of the current induced in the space charge region of the SC. Further, the effective barrier height was determined by current–voltage and capacitance–voltage measurements. Pd contacts prepared on ZnO thin films that had undergone treatment in a plasma-enhanced chemical vapor deposition with nitrous oxide (N2O) as ambient gas are laterally homogeneous with an effective barrier height of (600±30) meV.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Applied Physics Letters},\n\tauthor = {von Wenckstern, H. and Kaidashev, E. M. and Lorenz, M. and Hochmuth, H. and Biehne, G. and Lenzner, J. and Gottschalch, V. and Pickenhain, R. and Grundmann, M.},\n\tmonth = dec,\n\tyear = {2003},\n\tpages = {79--81},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The electrical properties of Schottky contacts (SCs) produced ex situ on n-type ZnO single crystals and epitaxial thin films were investigated. Electron beam induced current imaging was used to study lateral variations of the current induced in the space charge region of the SC. Further, the effective barrier height was determined by current–voltage and capacitance–voltage measurements. Pd contacts prepared on ZnO thin films that had undergone treatment in a plasma-enhanced chemical vapor deposition with nitrous oxide (N2O) as ambient gas are laterally homogeneous with an effective barrier height of (600±30) meV.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"bundesmann-ashkenov-schubert-spemann-butz-kaidashev-lorenz-grundmann-ramanscatteringinznothinfilmsdopedwithfesbalgaandli-2003\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.1609251\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'bundesmann-ashkenov-schubert-spemann-butz-kaidashev-lorenz-grundmann-ramanscatteringinznothinfilmsdopedwithfesbalgaandli-2003', 'https://doi.org/10.1063/1.1609251', event);\">\n    Raman scattering in ZnO thin films doped with Fe, Sb, Al, Ga, and Li.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Bundesmann, C.; Ashkenov, N.; Schubert, M.; Spemann, D.; Butz, T.; Kaidashev, E. M.; Lorenz, M.;  and Grundmann, M.\n</span>\n\n  \n\n</span>\n\n  <i>Applied Physics Letters</i>, 83(10): 1974–1976. September 2003.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.1609251\"\n     onclick=\"log_download('bundesmann-ashkenov-schubert-spemann-butz-kaidashev-lorenz-grundmann-ramanscatteringinznothinfilmsdopedwithfesbalgaandli-2003', 'https://doi.org/10.1063/1.1609251', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Raman scattering in ZnO thin films doped with Fe, Sb, Al, Ga, and Li [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.1609251\"\n     onclick=\"log_download('bundesmann-ashkenov-schubert-spemann-butz-kaidashev-lorenz-grundmann-ramanscatteringinznothinfilmsdopedwithfesbalgaandli-2003', 'http://doi.org/10.1063/1.1609251', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/bundesmann-ashkenov-schubert-spemann-butz-kaidashev-lorenz-grundmann-ramanscatteringinznothinfilmsdopedwithfesbalgaandli-2003\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('bundesmann-ashkenov-schubert-spemann-butz-kaidashev-lorenz-grundmann-ramanscatteringinznothinfilmsdopedwithfesbalgaandli-2003')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{bundesmann_raman_2003,\n\ttitle = {Raman scattering in {ZnO} thin films doped with {Fe}, {Sb}, {Al}, {Ga}, and {Li}},\n\tvolume = {83},\n\tissn = {0003-6951},\n\turl = {https://doi.org/10.1063/1.1609251},\n\tdoi = {10.1063/1.1609251},\n\tabstract = {Polarized micro-Raman measurements were performed to study the phonon modes of Fe, Sb, Al, Ga, and Li doped ZnO thin films, grown by pulsed-laser deposition on c-plane sapphire substrates. Additional modes at about 277, 511, 583, and 644 cm−1, recently assigned to N incorporation [A. Kaschner et al., Appl. Phys. Lett. 80, 1909 (2002)], were observed for Fe, Sb, and Al doped films, intentionally grown without N. The mode at 277 cm−1 occurs also for Ga doped films. These modes thus cannot be related directly to N incorporation. Instead, we suggest host lattice defects as their origin. Further additional modes at 531, 631, and 720 cm−1 seem specific for the Sb, Ga, and Fe dopants, respectively. Li doped ZnO did not reveal additional modes.},\n\tnumber = {10},\n\turldate = {2023-11-11},\n\tjournal = {Applied Physics Letters},\n\tauthor = {Bundesmann, C. and Ashkenov, N. and Schubert, M. and Spemann, D. and Butz, T. and Kaidashev, E. M. and Lorenz, M. and Grundmann, M.},\n\tmonth = sep,\n\tyear = {2003},\n\tpages = {1974--1976},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Polarized micro-Raman measurements were performed to study the phonon modes of Fe, Sb, Al, Ga, and Li doped ZnO thin films, grown by pulsed-laser deposition on c-plane sapphire substrates. Additional modes at about 277, 511, 583, and 644 cm−1, recently assigned to N incorporation [A. Kaschner et al., Appl. Phys. Lett. 80, 1909 (2002)], were observed for Fe, Sb, and Al doped films, intentionally grown without N. The mode at 277 cm−1 occurs also for Ga doped films. These modes thus cannot be related directly to N incorporation. Instead, we suggest host lattice defects as their origin. Further additional modes at 531, 631, and 720 cm−1 seem specific for the Sb, Ga, and Fe dopants, respectively. Li doped ZnO did not reveal additional modes.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"kaidashev-lorenz-vonwenckstern-rahm-semmelhack-han-benndorf-bundesmann-etal-highelectronmobilityofepitaxialznothinfilmsoncplanesapphiregrownbymultisteppulsedlaserdeposition-2003\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.1578694\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'kaidashev-lorenz-vonwenckstern-rahm-semmelhack-han-benndorf-bundesmann-etal-highelectronmobilityofepitaxialznothinfilmsoncplanesapphiregrownbymultisteppulsedlaserdeposition-2003', 'https://doi.org/10.1063/1.1578694', event);\">\n    High electron mobility of epitaxial ZnO thin films on c-plane sapphire grown by multistep pulsed-laser deposition.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Kaidashev, E. M.; Lorenz, M.; von Wenckstern, H.; Rahm, A.; Semmelhack, H.; Han, K.; Benndorf, G.; Bundesmann, C.; Hochmuth, H.;  and Grundmann, M.\n</span>\n\n  \n\n</span>\n\n  <i>Applied Physics Letters</i>, 82(22): 3901–3903. May 2003.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.1578694\"\n     onclick=\"log_download('kaidashev-lorenz-vonwenckstern-rahm-semmelhack-han-benndorf-bundesmann-etal-highelectronmobilityofepitaxialznothinfilmsoncplanesapphiregrownbymultisteppulsedlaserdeposition-2003', 'https://doi.org/10.1063/1.1578694', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"High electron mobility of epitaxial ZnO thin films on c-plane sapphire grown by multistep pulsed-laser deposition [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.1578694\"\n     onclick=\"log_download('kaidashev-lorenz-vonwenckstern-rahm-semmelhack-han-benndorf-bundesmann-etal-highelectronmobilityofepitaxialznothinfilmsoncplanesapphiregrownbymultisteppulsedlaserdeposition-2003', 'http://doi.org/10.1063/1.1578694', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/kaidashev-lorenz-vonwenckstern-rahm-semmelhack-han-benndorf-bundesmann-etal-highelectronmobilityofepitaxialznothinfilmsoncplanesapphiregrownbymultisteppulsedlaserdeposition-2003\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('kaidashev-lorenz-vonwenckstern-rahm-semmelhack-han-benndorf-bundesmann-etal-highelectronmobilityofepitaxialznothinfilmsoncplanesapphiregrownbymultisteppulsedlaserdeposition-2003')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{kaidashev_high_2003,\n\ttitle = {High electron mobility of epitaxial {ZnO} thin films on c-plane sapphire grown by multistep pulsed-laser deposition},\n\tvolume = {82},\n\tissn = {0003-6951},\n\turl = {https://doi.org/10.1063/1.1578694},\n\tdoi = {10.1063/1.1578694},\n\tabstract = {A multistep pulsed-laser deposition (PLD) process is presented for epitaxial, nominally undoped ZnO thin films of total thickness of 1 to 2 μm on c-plane sapphire substrates. We obtain reproducibly high electron mobilities from 115 up to 155 cm2/V s at 300 K in a narrow carrier concentration range from 2 to 5×1016 cm−3. The key issue of the multistep PLD process is the insertion of 30-nm-thin ZnO relaxation layers deposited at reduced substrate temperature. The high-mobility samples show atomically flat surface structure with grain size of about 0.5–1 μm, whereas the surfaces of low-mobility films consist of clearly resolved hexagonally faceted columnar grains of only 200-nm size, as shown by atomic force microscopy. Structurally optimized PLD ZnO thin films show narrow high-resolution x-ray diffraction peak widths of the ZnO(0002) ω- and 2Θ-scans as low as 151 and 43 arcsec, respectively, and narrow photoluminescence linewidths of donor-bound excitons of 1.7 meV at 2 K.},\n\tnumber = {22},\n\turldate = {2023-11-11},\n\tjournal = {Applied Physics Letters},\n\tauthor = {Kaidashev, E. M. and Lorenz, M. and von Wenckstern, H. and Rahm, A. and Semmelhack, H.-C. and Han, K.-H. and Benndorf, G. and Bundesmann, C. and Hochmuth, H. and Grundmann, M.},\n\tmonth = may,\n\tyear = {2003},\n\tpages = {3901--3903},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A multistep pulsed-laser deposition (PLD) process is presented for epitaxial, nominally undoped ZnO thin films of total thickness of 1 to 2 μm on c-plane sapphire substrates. We obtain reproducibly high electron mobilities from 115 up to 155 cm2/V s at 300 K in a narrow carrier concentration range from 2 to 5×1016 cm−3. The key issue of the multistep PLD process is the insertion of 30-nm-thin ZnO relaxation layers deposited at reduced substrate temperature. The high-mobility samples show atomically flat surface structure with grain size of about 0.5–1 μm, whereas the surfaces of low-mobility films consist of clearly resolved hexagonally faceted columnar grains of only 200-nm size, as shown by atomic force microscopy. Structurally optimized PLD ZnO thin films show narrow high-resolution x-ray diffraction peak widths of the ZnO(0002) ω- and 2Θ-scans as low as 151 and 43 arcsec, respectively, and narrow photoluminescence linewidths of donor-bound excitons of 1.7 meV at 2 K.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"lorenz-kaidashev-vonwenckstern-riede-bundesmann-spemann-benndorf-hochmuth-etal-opticalandelectricalpropertiesofepitaxialmgcdtextrmxzntextrm1xoznoandznogaalthinfilmsoncplanesapphiregrownbypulsedlaserdeposition-2003\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0038110103001989\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'lorenz-kaidashev-vonwenckstern-riede-bundesmann-spemann-benndorf-hochmuth-etal-opticalandelectricalpropertiesofepitaxialmgcdtextrmxzntextrm1xoznoandznogaalthinfilmsoncplanesapphiregrownbypulsedlaserdeposition-2003', 'https://www.sciencedirect.com/science/article/pii/S0038110103001989', event);\">\n    Optical and electrical properties of epitaxial (Mg,Cd)$_{\\textrm{x}}$Zn$_{\\textrm{1−x}}$O, ZnO, and ZnO:(Ga,Al) thin films on c-plane sapphire grown by pulsed laser deposition.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Lorenz, M.; Kaidashev, E. M.; von Wenckstern, H.; Riede, V.; Bundesmann, C.; Spemann, D.; Benndorf, G.; Hochmuth, H.; Rahm, A.; Semmelhack, H. -.;  and Grundmann, M.\n</span>\n\n  \n\n</span>\n\n  <i>Solid-State Electronics</i>, 47(12): 2205–2209. December 2003.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://www.sciencedirect.com/science/article/pii/S0038110103001989\"\n     onclick=\"log_download('lorenz-kaidashev-vonwenckstern-riede-bundesmann-spemann-benndorf-hochmuth-etal-opticalandelectricalpropertiesofepitaxialmgcdtextrmxzntextrm1xoznoandznogaalthinfilmsoncplanesapphiregrownbypulsedlaserdeposition-2003', 'https://www.sciencedirect.com/science/article/pii/S0038110103001989', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Optical and electrical properties of epitaxial (Mg,Cd)$_{\\textrm{x}}$Zn$_{\\textrm{1−x}}$O, ZnO, and ZnO:(Ga,Al) thin films on c-plane sapphire grown by pulsed laser deposition [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1016/S0038-1101(03)00198-9\"\n     onclick=\"log_download('lorenz-kaidashev-vonwenckstern-riede-bundesmann-spemann-benndorf-hochmuth-etal-opticalandelectricalpropertiesofepitaxialmgcdtextrmxzntextrm1xoznoandznogaalthinfilmsoncplanesapphiregrownbypulsedlaserdeposition-2003', 'http://doi.org/10.1016/S0038-1101(03)00198-9', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/lorenz-kaidashev-vonwenckstern-riede-bundesmann-spemann-benndorf-hochmuth-etal-opticalandelectricalpropertiesofepitaxialmgcdtextrmxzntextrm1xoznoandznogaalthinfilmsoncplanesapphiregrownbypulsedlaserdeposition-2003\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('lorenz-kaidashev-vonwenckstern-riede-bundesmann-spemann-benndorf-hochmuth-etal-opticalandelectricalpropertiesofepitaxialmgcdtextrmxzntextrm1xoznoandznogaalthinfilmsoncplanesapphiregrownbypulsedlaserdeposition-2003')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{lorenz_optical_2003,\n\tseries = {Proceedings of the 9th {International} {Workshop} on {Oxide} {Electronics}},\n\ttitle = {Optical and electrical properties of epitaxial ({Mg},{Cd})$_{\\textrm{x}}${Zn}$_{\\textrm{1−x}}${O}, {ZnO}, and {ZnO}:({Ga},{Al}) thin films on c-plane sapphire grown by pulsed laser deposition},\n\tvolume = {47},\n\tissn = {0038-1101},\n\tshorttitle = {Optical and electrical properties of epitaxial ({Mg},{Cd}){xZn1}−{xO}, {ZnO}, and {ZnO}},\n\turl = {https://www.sciencedirect.com/science/article/pii/S0038110103001989},\n\tdoi = {10.1016/S0038-1101(03)00198-9},\n\tabstract = {A consistent set of epitaxial, n-type conducting ZnO thin films, nominally undoped, doped with Ga or Al, or alloyed with Mg or Cd, was grown by pulsed laser deposition (PLD) on single-crystalline c-plane sapphire (0001) substrates, and characterized by Hall measurement, and UV/VIS optical transmission spectroscopy. The optical band gap of undoped ZnO films at nearly 3.28 eV was shifted by alloying with Mg up to 4.5 eV and by alloying with Cd down to 3.18 eV, dependent on the alloy composition. In addition, highly doped ZnO:Al films show a blue-shifted optical absorption edge due to filling of electronic states in the conduction band. The Hall transport data of the PLD (Mg,Zn,Cd)O:(Ga,Al) thin films span a carrier concentration range of six orders of magnitude from 3×1014 to 3×1020 cm−3, which corresponds to a resistivity from 5×10−4 to 3×103 Ωcm. Structurally optimized, nominally undoped ZnO films grown with ZnO nucleation and top layer reached an electron mobility of 155 cm2/Vs (300 K), which is among the largest values reported for heteroepitaxial ZnO thin films so far. Finally, we succeeded in combining the low resistivity of ZnO:Ga and the band gap shift of MgZnO in MgZnO:Ga thin films. This results demonstrate the unique tunability of the optical and electrical properties of the ZnO-based wide-band gap material for future electronic devices.},\n\tnumber = {12},\n\turldate = {2023-11-11},\n\tjournal = {Solid-State Electronics},\n\tauthor = {Lorenz, M. and Kaidashev, E. M. and von Wenckstern, H. and Riede, V. and Bundesmann, C. and Spemann, D. and Benndorf, G. and Hochmuth, H. and Rahm, A. and Semmelhack, H. -C. and Grundmann, M.},\n\tmonth = dec,\n\tyear = {2003},\n\tkeywords = {Electrical properties, Optical properties, Pulsed laser deposition, Thin films, Wide-band gap material, Zinc oxide},\n\tpages = {2205--2209},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  A consistent set of epitaxial, n-type conducting ZnO thin films, nominally undoped, doped with Ga or Al, or alloyed with Mg or Cd, was grown by pulsed laser deposition (PLD) on single-crystalline c-plane sapphire (0001) substrates, and characterized by Hall measurement, and UV/VIS optical transmission spectroscopy. The optical band gap of undoped ZnO films at nearly 3.28 eV was shifted by alloying with Mg up to 4.5 eV and by alloying with Cd down to 3.18 eV, dependent on the alloy composition. In addition, highly doped ZnO:Al films show a blue-shifted optical absorption edge due to filling of electronic states in the conduction band. The Hall transport data of the PLD (Mg,Zn,Cd)O:(Ga,Al) thin films span a carrier concentration range of six orders of magnitude from 3×1014 to 3×1020 cm−3, which corresponds to a resistivity from 5×10−4 to 3×103 Ωcm. Structurally optimized, nominally undoped ZnO films grown with ZnO nucleation and top layer reached an electron mobility of 155 cm2/Vs (300 K), which is among the largest values reported for heteroepitaxial ZnO thin films so far. Finally, we succeeded in combining the low resistivity of ZnO:Ga and the band gap shift of MgZnO in MgZnO:Ga thin films. This results demonstrate the unique tunability of the optical and electrical properties of the ZnO-based wide-band gap material for future electronic devices.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"misochko-kaidashev-georgiev-dekorsy-zakharchenko-atimeresolvedopticalstudyoftheparamagneticdielectricferromagneticmetaltransitioninlatextrm07catextrm03mnotextrm3-2003\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1134/1.1625069\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'misochko-kaidashev-georgiev-dekorsy-zakharchenko-atimeresolvedopticalstudyoftheparamagneticdielectricferromagneticmetaltransitioninlatextrm07catextrm03mnotextrm3-2003', 'https://doi.org/10.1134/1.1625069', event);\">\n    A time-resolved optical study of the paramagnetic dielectric-ferromagnetic metal transition in La$_{\\textrm{0.7}}$Ca$_{\\textrm{0.3}}$MnO$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Misochko, 1. O. V.; Kaidashev, E. M.; Georgiev, N.; Dekorsy, T.;  and Zakharchenko, I. N.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Experimental and Theoretical Physics</i>, 97(4): 788–793. October 2003.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1134/1.1625069\"\n     onclick=\"log_download('misochko-kaidashev-georgiev-dekorsy-zakharchenko-atimeresolvedopticalstudyoftheparamagneticdielectricferromagneticmetaltransitioninlatextrm07catextrm03mnotextrm3-2003', 'https://doi.org/10.1134/1.1625069', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"A time-resolved optical study of the paramagnetic dielectric-ferromagnetic metal transition in La$_{\\textrm{0.7}}$Ca$_{\\textrm{0.3}}$MnO$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1134/1.1625069\"\n     onclick=\"log_download('misochko-kaidashev-georgiev-dekorsy-zakharchenko-atimeresolvedopticalstudyoftheparamagneticdielectricferromagneticmetaltransitioninlatextrm07catextrm03mnotextrm3-2003', 'http://doi.org/10.1134/1.1625069', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/misochko-kaidashev-georgiev-dekorsy-zakharchenko-atimeresolvedopticalstudyoftheparamagneticdielectricferromagneticmetaltransitioninlatextrm07catextrm03mnotextrm3-2003\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('misochko-kaidashev-georgiev-dekorsy-zakharchenko-atimeresolvedopticalstudyoftheparamagneticdielectricferromagneticmetaltransitioninlatextrm07catextrm03mnotextrm3-2003')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{misochko_time-resolved_2003,\n\ttitle = {A time-resolved optical study of the paramagnetic dielectric-ferromagnetic metal transition in {La}$_{\\textrm{0.7}}${Ca}$_{\\textrm{0.3}}${MnO}$_{\\textrm{3}}$},\n\tvolume = {97},\n\tissn = {1090-6509},\n\turl = {https://doi.org/10.1134/1.1625069},\n\tdoi = {10.1134/1.1625069},\n\tabstract = {The relaxation dynamics of charge carriers in an epitaxial La0.7Ca0.3MnO3 film was studied by the light reflection method with a femtosecond time resolution in a wide temperature range. The relaxation of time-resolved photoinduced reflections was shown to be two-component in the whole temperature range including the paramagnetic dielectric-ferromagnetic metal transition at T ≈ 150–160 K. The fast relaxation component had a maximum lifetime (τ ∼ 500 ps) in the transition region, and its contribution to relaxation increased as temperature decreased. The lifetime of the slow component was minimum (τ ∼ 15 fs) in the transition region. In addition, fast oscillations assigned to coherent phonons appeared in photoinduced responses at T {\\textless} 200 K. The dephasing time of these oscillations increased as temperature decreased, whereas their frequency changed insignificantly.},\n\tlanguage = {en},\n\tnumber = {4},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Experimental and Theoretical Physics},\n\tauthor = {Misochko, 1. O. V. and Kaidashev, E. M. and Georgiev, N. and Dekorsy, T. and Zakharchenko, I. N.},\n\tmonth = oct,\n\tyear = {2003},\n\tkeywords = {Charge Carrier, Elementary Particle, Time Resolution, Transition Region, Wide Temperature Range},\n\tpages = {788--793},\n\tfile = {Полный текст:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\JRJUDEGD\\\\Misochko и др. - 2003 - A time-resolved optical study of the paramagnetic .pdf:application/pdf},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The relaxation dynamics of charge carriers in an epitaxial La0.7Ca0.3MnO3 film was studied by the light reflection method with a femtosecond time resolution in a wide temperature range. The relaxation of time-resolved photoinduced reflections was shown to be two-component in the whole temperature range including the paramagnetic dielectric-ferromagnetic metal transition at T ≈ 150–160 K. The fast relaxation component had a maximum lifetime (τ ∼ 500 ps) in the transition region, and its contribution to relaxation increased as temperature decreased. The lifetime of the slow component was minimum (τ ∼ 15 fs) in the transition region. In addition, fast oscillations assigned to coherent phonons appeared in photoinduced responses at T \\textless 200 K. The dephasing time of these oscillations increased as temperature decreased, whereas their frequency changed insignificantly.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"schmidt-rheinlnder-schubert-spemann-butz-lenzner-kaidashev-lorenz-etal-dielectricfunctions1to5evofwurtzitemgtextrmxzntextrm1xox029thinfilms-2003\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.1565185\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'schmidt-rheinlnder-schubert-spemann-butz-lenzner-kaidashev-lorenz-etal-dielectricfunctions1to5evofwurtzitemgtextrmxzntextrm1xox029thinfilms-2003', 'https://doi.org/10.1063/1.1565185', event);\">\n    Dielectric functions (1 to 5 eV) of wurtzite Mg$_{\\textrm{x}}$Zn$_{\\textrm{1−x}}$O (x⩽0.29) thin films.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Schmidt, R.; Rheinländer, B.; Schubert, M.; Spemann, D.; Butz, T.; Lenzner, J.; Kaidashev, E. M.; Lorenz, M.; Rahm, A.; Semmelhack, H. C.;  and Grundmann, M.\n</span>\n\n  \n\n</span>\n\n  <i>Applied Physics Letters</i>, 82(14): 2260–2262. April 2003.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.1565185\"\n     onclick=\"log_download('schmidt-rheinlnder-schubert-spemann-butz-lenzner-kaidashev-lorenz-etal-dielectricfunctions1to5evofwurtzitemgtextrmxzntextrm1xox029thinfilms-2003', 'https://doi.org/10.1063/1.1565185', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Dielectric functions (1 to 5 eV) of wurtzite Mg$_{\\textrm{x}}$Zn$_{\\textrm{1−x}}$O (x⩽0.29) thin films [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.1565185\"\n     onclick=\"log_download('schmidt-rheinlnder-schubert-spemann-butz-lenzner-kaidashev-lorenz-etal-dielectricfunctions1to5evofwurtzitemgtextrmxzntextrm1xox029thinfilms-2003', 'http://doi.org/10.1063/1.1565185', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/schmidt-rheinlnder-schubert-spemann-butz-lenzner-kaidashev-lorenz-etal-dielectricfunctions1to5evofwurtzitemgtextrmxzntextrm1xox029thinfilms-2003\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('schmidt-rheinlnder-schubert-spemann-butz-lenzner-kaidashev-lorenz-etal-dielectricfunctions1to5evofwurtzitemgtextrmxzntextrm1xox029thinfilms-2003')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{schmidt_dielectric_2003,\n\ttitle = {Dielectric functions (1 to 5 {eV}) of wurtzite {Mg}$_{\\textrm{x}}${Zn}$_{\\textrm{1−x}}${O} (x⩽0.29) thin films},\n\tvolume = {82},\n\tissn = {0003-6951},\n\turl = {https://doi.org/10.1063/1.1565185},\n\tdoi = {10.1063/1.1565185},\n\tabstract = {The optical dielectric functions for polarization perpendicular and parallel to the c-axis (optical axis) of pulsed-laser-deposition grown wurtzite MgxZn1−xO (0⩽x⩽0.29) thin films have been determined at room temperature using ellipsometry for photon energies from 1 to 5 eV. The dielectric functions reveal strong excitonic contributions for all Mg concentrations x. The band gap energies (E0A=3.369 eV for ZnO to 4.101 eV for x=0.29) show a remarkable blueshift. The exciton binding energy (61 meV for ZnO) decreases to approximately 50 meV for x≈0.17 and increases to approximately 58 meV for x=0.29. In contrast to ZnO, the MgxZn1−xO alloys are found uniaxial negative below the band gap energy, opposite to previously reported results.},\n\tnumber = {14},\n\turldate = {2023-11-11},\n\tjournal = {Applied Physics Letters},\n\tauthor = {Schmidt, R. and Rheinländer, B. and Schubert, M. and Spemann, D. and Butz, T. and Lenzner, J. and Kaidashev, E. M. and Lorenz, M. and Rahm, A. and Semmelhack, H. C. and Grundmann, M.},\n\tmonth = apr,\n\tyear = {2003},\n\tpages = {2260--2262},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The optical dielectric functions for polarization perpendicular and parallel to the c-axis (optical axis) of pulsed-laser-deposition grown wurtzite MgxZn1−xO (0⩽x⩽0.29) thin films have been determined at room temperature using ellipsometry for photon energies from 1 to 5 eV. The dielectric functions reveal strong excitonic contributions for all Mg concentrations x. The band gap energies (E0A=3.369 eV for ZnO to 4.101 eV for x=0.29) show a remarkable blueshift. The exciton binding energy (61 meV for ZnO) decreases to approximately 50 meV for x≈0.17 and increases to approximately 58 meV for x=0.29. In contrast to ZnO, the MgxZn1−xO alloys are found uniaxial negative below the band gap energy, opposite to previously reported results.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"yuzyuk-katiyar-alyoshin-zakharchenko-markov-sviridov-stressrelaxationinheteroepitaxialbasrtiotextrm3001mgothinfilmstudiedbymicroramanspectroscopy-2003\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.68.104104\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'yuzyuk-katiyar-alyoshin-zakharchenko-markov-sviridov-stressrelaxationinheteroepitaxialbasrtiotextrm3001mgothinfilmstudiedbymicroramanspectroscopy-2003', 'https://link.aps.org/doi/10.1103/PhysRevB.68.104104', event);\">\n    Stress relaxation in heteroepitaxial (Ba, Sr)TiO$_{\\textrm{3}}$/(001) MgO thin film studied by micro-Raman spectroscopy.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Yuzyuk, Y. I.; Katiyar, R. S.; Alyoshin, V. A.; Zakharchenko, I. N.; Markov, D. A.;  and Sviridov, E. V.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 68(10): 104104. September 2003.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.68.104104\"\n     onclick=\"log_download('yuzyuk-katiyar-alyoshin-zakharchenko-markov-sviridov-stressrelaxationinheteroepitaxialbasrtiotextrm3001mgothinfilmstudiedbymicroramanspectroscopy-2003', 'https://link.aps.org/doi/10.1103/PhysRevB.68.104104', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Stress relaxation in heteroepitaxial (Ba, Sr)TiO$_{\\textrm{3}}$/(001) MgO thin film studied by micro-Raman spectroscopy [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.68.104104\"\n     onclick=\"log_download('yuzyuk-katiyar-alyoshin-zakharchenko-markov-sviridov-stressrelaxationinheteroepitaxialbasrtiotextrm3001mgothinfilmstudiedbymicroramanspectroscopy-2003', 'http://doi.org/10.1103/PhysRevB.68.104104', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/yuzyuk-katiyar-alyoshin-zakharchenko-markov-sviridov-stressrelaxationinheteroepitaxialbasrtiotextrm3001mgothinfilmstudiedbymicroramanspectroscopy-2003\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('yuzyuk-katiyar-alyoshin-zakharchenko-markov-sviridov-stressrelaxationinheteroepitaxialbasrtiotextrm3001mgothinfilmstudiedbymicroramanspectroscopy-2003')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{yuzyuk_stress_2003,\n\ttitle = {Stress relaxation in heteroepitaxial ({Ba}, {Sr}){TiO}$_{\\textrm{3}}$/(001) {MgO} thin film studied by micro-{Raman} spectroscopy},\n\tvolume = {68},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.68.104104},\n\tdoi = {10.1103/PhysRevB.68.104104},\n\tabstract = {The evolution of stresses in a heteroepitaxial (Ba0.7Sr0.3)TiO3/(001)MgO thin film was studied by means of micro-Raman spectroscopy. A small part of the substrate was gradually dissolved, then partially unsupported and completely free-standing areas of the film were studied in a side-view backscattering geometry. The E(TO) soft mode was used to estimate local stresses in the thin film. Our experiments revealed stress relaxation and the gradient of the tetragonal distortion in the partially unsupported ferroelectric thin film. The length scale over which the stress relaxes in the heteroepitaxial film was estimated. The thermal strain arising mostly due to the difference between the thermal-expansion coefficients of the film and the substrate governs the domain structure and induces enhanced tetragonality in the film studied. We found that the partially unsupported thin film is polarization graded due to the stress gradient along the film-substrate interface.},\n\tnumber = {10},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Yuzyuk, Yu. I. and Katiyar, R. S. and Alyoshin, V. A. and Zakharchenko, I. N. and Markov, D. A. and Sviridov, E. V.},\n\tmonth = sep,\n\tyear = {2003},\n\tnote = {Publisher: American Physical Society},\n\tpages = {104104},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  The evolution of stresses in a heteroepitaxial (Ba0.7Sr0.3)TiO3/(001)MgO thin film was studied by means of micro-Raman spectroscopy. A small part of the substrate was gradually dissolved, then partially unsupported and completely free-standing areas of the film were studied in a side-view backscattering geometry. The E(TO) soft mode was used to estimate local stresses in the thin film. Our experiments revealed stress relaxation and the gradient of the tetragonal distortion in the partially unsupported ferroelectric thin film. The length scale over which the stress relaxes in the heteroepitaxial film was estimated. The thermal strain arising mostly due to the difference between the thermal-expansion coefficients of the film and the substrate governs the domain structure and induces enhanced tetragonality in the film studied. We found that the partially unsupported thin film is polarization graded due to the stress gradient along the film-substrate interface.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"yuzyuk-sauvajol-simon-lorman-alyoshin-zakharchenko-sviridov-phasetransitionsinbatextrm07srtextrm03tiotextrm3001mgothinfilmstudiedbyramanscattering-2003\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.1574173\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'yuzyuk-sauvajol-simon-lorman-alyoshin-zakharchenko-sviridov-phasetransitionsinbatextrm07srtextrm03tiotextrm3001mgothinfilmstudiedbyramanscattering-2003', 'https://doi.org/10.1063/1.1574173', event);\">\n    Phase transitions in (Ba$_{\\textrm{0.7}}$Sr$_{\\textrm{0.3}}$)TiO$_{\\textrm{3}}$/(001)MgO thin film studied by Raman scattering.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Yuzyuk, Y. I.; Sauvajol, J. L.; Simon, P.; Lorman, V. L.; Alyoshin, V. A.; Zakharchenko, I. N.;  and Sviridov, E. V.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Applied Physics</i>, 93(12): 9930–9937. May 2003.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.1574173\"\n     onclick=\"log_download('yuzyuk-sauvajol-simon-lorman-alyoshin-zakharchenko-sviridov-phasetransitionsinbatextrm07srtextrm03tiotextrm3001mgothinfilmstudiedbyramanscattering-2003', 'https://doi.org/10.1063/1.1574173', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Phase transitions in (Ba$_{\\textrm{0.7}}$Sr$_{\\textrm{0.3}}$)TiO$_{\\textrm{3}}$/(001)MgO thin film studied by Raman scattering [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.1574173\"\n     onclick=\"log_download('yuzyuk-sauvajol-simon-lorman-alyoshin-zakharchenko-sviridov-phasetransitionsinbatextrm07srtextrm03tiotextrm3001mgothinfilmstudiedbyramanscattering-2003', 'http://doi.org/10.1063/1.1574173', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/yuzyuk-sauvajol-simon-lorman-alyoshin-zakharchenko-sviridov-phasetransitionsinbatextrm07srtextrm03tiotextrm3001mgothinfilmstudiedbyramanscattering-2003\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('yuzyuk-sauvajol-simon-lorman-alyoshin-zakharchenko-sviridov-phasetransitionsinbatextrm07srtextrm03tiotextrm3001mgothinfilmstudiedbyramanscattering-2003')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{yuzyuk_phase_2003,\n\ttitle = {Phase transitions in ({Ba}$_{\\textrm{0.7}}${Sr}$_{\\textrm{0.3}}$){TiO}$_{\\textrm{3}}$/(001){MgO} thin film studied by {Raman} scattering},\n\tvolume = {93},\n\tissn = {0021-8979},\n\turl = {https://doi.org/10.1063/1.1574173},\n\tdoi = {10.1063/1.1574173},\n\tabstract = {Polarized Raman spectra of heteroepitaxial (Ba0.7Sr0.3)TiO3 thin film deposited on the (001)MgO substrate have been studied in the broad temperature range from 30 to 1300 K. Our results show that the ferroelectric–paraelectric phase transition is markedly shifted to higher temperatures with respect to the bulk ceramics of the same composition. Because of the two-dimensional compressive stresses imposed on the film by the substrate, the symmetry of the paraelectric phase is found to be tetragonal well above the Curie temperature. Near the deposition temperature (1173 K), the thermoelastic compressive stresses vanish and Raman response suggests nearly cubic symmetry. Raman measurements below room temperature show clearly that the phase transition to the rhombohedral phase is completely suppressed and only one phase transition from the tetragonal to the monoclinic phase is revealed at ∼150 K.},\n\tnumber = {12},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Applied Physics},\n\tauthor = {Yuzyuk, Yu. I. and Sauvajol, J. L. and Simon, P. and Lorman, V. L. and Alyoshin, V. A. and Zakharchenko, I. N. and Sviridov, E. V.},\n\tmonth = may,\n\tyear = {2003},\n\tpages = {9930--9937},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Polarized Raman spectra of heteroepitaxial (Ba0.7Sr0.3)TiO3 thin film deposited on the (001)MgO substrate have been studied in the broad temperature range from 30 to 1300 K. Our results show that the ferroelectric–paraelectric phase transition is markedly shifted to higher temperatures with respect to the bulk ceramics of the same composition. Because of the two-dimensional compressive stresses imposed on the film by the substrate, the symmetry of the paraelectric phase is found to be tetragonal well above the Curie temperature. Near the deposition temperature (1173 K), the thermoelastic compressive stresses vanish and Raman response suggests nearly cubic symmetry. Raman measurements below room temperature show clearly that the phase transition to the rhombohedral phase is completely suppressed and only one phase transition from the tetragonal to the monoclinic phase is revealed at ∼150 K.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"yuzyuk-simon-commentonstructuralorderingtransitionandrepulsionofthegiantlotosplittinginpolycrystallinebatextrmxsrtextrm1xtiotextrm3-2003\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.68.216101\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'yuzyuk-simon-commentonstructuralorderingtransitionandrepulsionofthegiantlotosplittinginpolycrystallinebatextrmxsrtextrm1xtiotextrm3-2003', 'https://link.aps.org/doi/10.1103/PhysRevB.68.216101', event);\">\n    Comment on ``Structural ordering transition and repulsion of the giant LO-TO splitting in polycrystalline Ba$_{\\textrm{x}}$Sr$_{\\textrm{1-x}}$TiO$_{\\textrm{3}}$.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Yuzyuk, Y. I.;  and Simon, P.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 68(21): 216101. December 2003.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.68.216101\"\n     onclick=\"log_download('yuzyuk-simon-commentonstructuralorderingtransitionandrepulsionofthegiantlotosplittinginpolycrystallinebatextrmxsrtextrm1xtiotextrm3-2003', 'https://link.aps.org/doi/10.1103/PhysRevB.68.216101', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Comment on &#x60;&#x60;Structural ordering transition and repulsion of the giant LO-TO splitting in polycrystalline Ba$_{\\textrm{x}}$Sr$_{\\textrm{1-x}}$TiO$_{\\textrm{3}}$ [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.68.216101\"\n     onclick=\"log_download('yuzyuk-simon-commentonstructuralorderingtransitionandrepulsionofthegiantlotosplittinginpolycrystallinebatextrmxsrtextrm1xtiotextrm3-2003', 'http://doi.org/10.1103/PhysRevB.68.216101', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/yuzyuk-simon-commentonstructuralorderingtransitionandrepulsionofthegiantlotosplittinginpolycrystallinebatextrmxsrtextrm1xtiotextrm3-2003\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('yuzyuk-simon-commentonstructuralorderingtransitionandrepulsionofthegiantlotosplittinginpolycrystallinebatextrmxsrtextrm1xtiotextrm3-2003')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{yuzyuk_comment_2003,\n\ttitle = {Comment on &#x60;&#x60;{Structural} ordering transition and repulsion of the giant {LO}-{TO} splitting in polycrystalline {Ba}$_{\\textrm{x}}${Sr}$_{\\textrm{1-x}}${TiO}$_{\\textrm{3}}$},\n\tvolume = {68},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.68.216101},\n\tdoi = {10.1103/PhysRevB.68.216101},\n\tabstract = {Recently, Kuo et al. [S.-Y. Kuo, W.-Y. Liao, and W.-F. Hsieh, Phys. Rev. B 64, 224103 (2001)] reported a new structural ordering in sol-gel derived polycrystalline BaxSr1−xTiO3 around x≈0.4–0.5 at room temperature. We show that unpolarized Raman data obtained in this work were analyzed incorrectly. As a consequence, conclusions derived from Raman-scattering experiments in the above paper are questionable.},\n\tnumber = {21},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Yuzyuk, Yu. I. and Simon, P.},\n\tmonth = dec,\n\tyear = {2003},\n\tnote = {Publisher: American Physical Society},\n\tpages = {216101},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Recently, Kuo et al. [S.-Y. Kuo, W.-Y. Liao, and W.-F. Hsieh, Phys. Rev. B 64, 224103 (2001)] reported a new structural ordering in sol-gel derived polycrystalline BaxSr1−xTiO3 around x≈0.4–0.5 at room temperature. We show that unpolarized Raman data obtained in this work were analyzed incorrectly. As a consequence, conclusions derived from Raman-scattering experiments in the above paper are questionable.\n</div>\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_2002\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_2002')\"\n      onkeypress=\"toggleGroup('group_2002')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>2002</span>\n      <span class=\"bibbase_group_count\">\n        \n        (4)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"ashkenov-mbenkum-bundesmann-riede-lorenz-spemann-kaidashev-kasic-etal-infrareddielectricfunctionsandphononmodesofhighqualityznofilms-2002\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.1526935\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'ashkenov-mbenkum-bundesmann-riede-lorenz-spemann-kaidashev-kasic-etal-infrareddielectricfunctionsandphononmodesofhighqualityznofilms-2002', 'https://doi.org/10.1063/1.1526935', event);\">\n    Infrared dielectric functions and phonon modes of high-quality ZnO films.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Ashkenov, N.; Mbenkum, B. N.; Bundesmann, C.; Riede, V.; Lorenz, M.; Spemann, D.; Kaidashev, E. M.; Kasic, A.; Schubert, M.; Grundmann, M.; Wagner, G.; Neumann, H.; Darakchieva, V.; Arwin, H.;  and Monemar, B.\n</span>\n\n  \n\n</span>\n\n  <i>Journal of Applied Physics</i>, 93(1): 126–133. December 2002.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.1526935\"\n     onclick=\"log_download('ashkenov-mbenkum-bundesmann-riede-lorenz-spemann-kaidashev-kasic-etal-infrareddielectricfunctionsandphononmodesofhighqualityznofilms-2002', 'https://doi.org/10.1063/1.1526935', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Infrared dielectric functions and phonon modes of high-quality ZnO films [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.1526935\"\n     onclick=\"log_download('ashkenov-mbenkum-bundesmann-riede-lorenz-spemann-kaidashev-kasic-etal-infrareddielectricfunctionsandphononmodesofhighqualityznofilms-2002', 'http://doi.org/10.1063/1.1526935', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/ashkenov-mbenkum-bundesmann-riede-lorenz-spemann-kaidashev-kasic-etal-infrareddielectricfunctionsandphononmodesofhighqualityznofilms-2002\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('ashkenov-mbenkum-bundesmann-riede-lorenz-spemann-kaidashev-kasic-etal-infrareddielectricfunctionsandphononmodesofhighqualityznofilms-2002')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{ashkenov_infrared_2002,\n\ttitle = {Infrared dielectric functions and phonon modes of high-quality {ZnO} films},\n\tvolume = {93},\n\tissn = {0021-8979},\n\turl = {https://doi.org/10.1063/1.1526935},\n\tdoi = {10.1063/1.1526935},\n\tabstract = {Infrared dielectric function spectra and phonon modes of high-quality, single crystalline, and highly resistive wurtzite ZnO films were obtained from infrared (300–1200 cm−1) spectroscopic ellipsometry and Raman scattering studies. The ZnO films were deposited by pulsed-laser deposition on c-plane sapphire substrates and investigated by high-resolution x-ray diffraction, high-resolution transmission electron microscopy, and Rutherford backscattering experiments. The crystal structure, phonon modes, and dielectric functions are compared to those obtained from a single-crystal ZnO bulk sample. The film ZnO phonon mode frequencies are highly consistent with those of the bulk material. A small redshift of the longitudinal optical phonon mode frequencies of the ZnO films with respect to the bulk material is observed. This is tentatively assigned to the existence of vacancy point defects within the films. Accurate long-wavelength dielectric constant limits of ZnO are obtained from the infrared ellipsometry analysis and compared with previously measured near-band-gap index-of-refraction data using the Lyddane–Sachs–Teller relation. The ZnO model dielectric function spectra will become useful for future infrared ellipsometry analysis of free-carrier parameters in complex ZnO-based heterostructures.},\n\tnumber = {1},\n\turldate = {2023-11-11},\n\tjournal = {Journal of Applied Physics},\n\tauthor = {Ashkenov, N. and Mbenkum, B. N. and Bundesmann, C. and Riede, V. and Lorenz, M. and Spemann, D. and Kaidashev, E. M. and Kasic, A. and Schubert, M. and Grundmann, M. and Wagner, G. and Neumann, H. and Darakchieva, V. and Arwin, H. and Monemar, B.},\n\tmonth = dec,\n\tyear = {2002},\n\tpages = {126--133},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Infrared dielectric function spectra and phonon modes of high-quality, single crystalline, and highly resistive wurtzite ZnO films were obtained from infrared (300–1200 cm−1) spectroscopic ellipsometry and Raman scattering studies. The ZnO films were deposited by pulsed-laser deposition on c-plane sapphire substrates and investigated by high-resolution x-ray diffraction, high-resolution transmission electron microscopy, and Rutherford backscattering experiments. The crystal structure, phonon modes, and dielectric functions are compared to those obtained from a single-crystal ZnO bulk sample. The film ZnO phonon mode frequencies are highly consistent with those of the bulk material. A small redshift of the longitudinal optical phonon mode frequencies of the ZnO films with respect to the bulk material is observed. This is tentatively assigned to the existence of vacancy point defects within the films. Accurate long-wavelength dielectric constant limits of ZnO are obtained from the infrared ellipsometry analysis and compared with previously measured near-band-gap index-of-refraction data using the Lyddane–Sachs–Teller relation. The ZnO model dielectric function spectra will become useful for future infrared ellipsometry analysis of free-carrier parameters in complex ZnO-based heterostructures.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"bundesmann-schubert-spemann-butz-lorenz-kaidashev-grundmann-ashkenov-etal-infrareddielectricfunctionsandphononmodesofwurtzitemgtextrmxzntextrm1xox02-2002\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://doi.org/10.1063/1.1509862\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'bundesmann-schubert-spemann-butz-lorenz-kaidashev-grundmann-ashkenov-etal-infrareddielectricfunctionsandphononmodesofwurtzitemgtextrmxzntextrm1xox02-2002', 'https://doi.org/10.1063/1.1509862', event);\">\n    Infrared dielectric functions and phonon modes of wurtzite Mg$_{\\textrm{x}}$Zn$_{\\textrm{1−x}}$O (x⩽0.2).\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Bundesmann, C.; Schubert, M.; Spemann, D.; Butz, T.; Lorenz, M.; Kaidashev, E. M.; Grundmann, M.; Ashkenov, N.; Neumann, H.;  and Wagner, G.\n</span>\n\n  \n\n</span>\n\n  <i>Applied Physics Letters</i>, 81(13): 2376–2378. September 2002.\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://doi.org/10.1063/1.1509862\"\n     onclick=\"log_download('bundesmann-schubert-spemann-butz-lorenz-kaidashev-grundmann-ashkenov-etal-infrareddielectricfunctionsandphononmodesofwurtzitemgtextrmxzntextrm1xox02-2002', 'https://doi.org/10.1063/1.1509862', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Infrared dielectric functions and phonon modes of wurtzite Mg$_{\\textrm{x}}$Zn$_{\\textrm{1−x}}$O (x⩽0.2) [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1063/1.1509862\"\n     onclick=\"log_download('bundesmann-schubert-spemann-butz-lorenz-kaidashev-grundmann-ashkenov-etal-infrareddielectricfunctionsandphononmodesofwurtzitemgtextrmxzntextrm1xox02-2002', 'http://doi.org/10.1063/1.1509862', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/bundesmann-schubert-spemann-butz-lorenz-kaidashev-grundmann-ashkenov-etal-infrareddielectricfunctionsandphononmodesofwurtzitemgtextrmxzntextrm1xox02-2002\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('bundesmann-schubert-spemann-butz-lorenz-kaidashev-grundmann-ashkenov-etal-infrareddielectricfunctionsandphononmodesofwurtzitemgtextrmxzntextrm1xox02-2002')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{bundesmann_infrared_2002,\n\ttitle = {Infrared dielectric functions and phonon modes of wurtzite {Mg}$_{\\textrm{x}}${Zn}$_{\\textrm{1−x}}${O} (x⩽0.2)},\n\tvolume = {81},\n\tissn = {0003-6951},\n\turl = {https://doi.org/10.1063/1.1509862},\n\tdoi = {10.1063/1.1509862},\n\tabstract = {Infrared dielectric function spectra and phonon modes with polarization parallel and perpendicular to the c axis of high quality, highly relaxed, and single crystalline wurtzite MgxZn1−xO films with 0⩽x⩽0.2 prepared by pulsed-laser deposition on c-plane sapphire substrates were obtained from infrared spectroscopic ellipsometry (380–1200 cm−1) and Raman scattering studies. A two-mode behavior is found for the modes with E1 symmetry, a lattice mode and an impurity-type mode are obtained for the A1 symmetry phonons. Model dielectric function spectra will become useful for future infrared ellipsometry analysis of complex MgxZn1−xO-based heterostructures.},\n\tnumber = {13},\n\turldate = {2023-11-11},\n\tjournal = {Applied Physics Letters},\n\tauthor = {Bundesmann, C. and Schubert, M. and Spemann, D. and Butz, T. and Lorenz, M. and Kaidashev, E. M. and Grundmann, M. and Ashkenov, N. and Neumann, H. and Wagner, G.},\n\tmonth = sep,\n\tyear = {2002},\n\tpages = {2376--2378},\n\tfile = {Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\MGX7XX67\\\\Infrared-dielectric-functions-and-phonon-modes-of.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  Infrared dielectric function spectra and phonon modes with polarization parallel and perpendicular to the c axis of high quality, highly relaxed, and single crystalline wurtzite MgxZn1−xO films with 0⩽x⩽0.2 prepared by pulsed-laser deposition on c-plane sapphire substrates were obtained from infrared spectroscopic ellipsometry (380–1200 cm−1) and Raman scattering studies. A two-mode behavior is found for the modes with E1 symmetry, a lattice mode and an impurity-type mode are obtained for the A1 symmetry phonons. Model dielectric function spectra will become useful for future infrared ellipsometry analysis of complex MgxZn1−xO-based heterostructures.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"yuzyuk-alyoshin-zakharchenko-sviridov-almeida-chaves-polarizationdependentramanspectraofheteroepitaxialbasrtiotextrm3001mgothinfilms-2002\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.65.134107\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'yuzyuk-alyoshin-zakharchenko-sviridov-almeida-chaves-polarizationdependentramanspectraofheteroepitaxialbasrtiotextrm3001mgothinfilms-2002', 'https://link.aps.org/doi/10.1103/PhysRevB.65.134107', event);\">\n    Polarization-dependent Raman spectra of heteroepitaxial (Ba, Sr)TiO$_{\\textrm{3}}$/(001) MgO thin films.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Yuzyuk, Y. I.; Alyoshin, V. A.; Zakharchenko, I. N.; Sviridov, E. V.; Almeida, A.;  and Chaves, M. R.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 65(13): 134107. March 2002.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.65.134107\"\n     onclick=\"log_download('yuzyuk-alyoshin-zakharchenko-sviridov-almeida-chaves-polarizationdependentramanspectraofheteroepitaxialbasrtiotextrm3001mgothinfilms-2002', 'https://link.aps.org/doi/10.1103/PhysRevB.65.134107', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Polarization-dependent Raman spectra of heteroepitaxial (Ba, Sr)TiO$_{\\textrm{3}}$/(001) MgO thin films [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.65.134107\"\n     onclick=\"log_download('yuzyuk-alyoshin-zakharchenko-sviridov-almeida-chaves-polarizationdependentramanspectraofheteroepitaxialbasrtiotextrm3001mgothinfilms-2002', 'http://doi.org/10.1103/PhysRevB.65.134107', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/yuzyuk-alyoshin-zakharchenko-sviridov-almeida-chaves-polarizationdependentramanspectraofheteroepitaxialbasrtiotextrm3001mgothinfilms-2002\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('yuzyuk-alyoshin-zakharchenko-sviridov-almeida-chaves-polarizationdependentramanspectraofheteroepitaxialbasrtiotextrm3001mgothinfilms-2002')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{yuzyuk_polarization-dependent_2002,\n\ttitle = {Polarization-dependent {Raman} spectra of heteroepitaxial ({Ba}, {Sr}){TiO}$_{\\textrm{3}}$/(001) {MgO} thin films},\n\tvolume = {65},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.65.134107},\n\tdoi = {10.1103/PhysRevB.65.134107},\n\tabstract = {We have studied the concentration dependence of the Raman spectra of heteroepitaxial (Ba1−xSrx)TiO3 (BST) (x=0, 0.15, 0.30, and 0.45) thin films deposited by rf sputtering on (001) MgO substrates. It is found that substitution of Ba by Sr leads to the distortions of the Ti-O bonds and causes the appearance of new bands in the Raman spectra near the bands corresponding to the Ti-O vibrations. The Sr incorporation induces relatively large shifts of the low-frequency Raman peaks attributed to ETO and A1TO components of the soft mode. The ETO soft mode in BST films becomes underdamped for x{\\textgreater}{\\textasciitilde}0.3 and is very sensitive to the two-dimensional compressive stresses.},\n\tnumber = {13},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Yuzyuk, Yu. I. and Alyoshin, V. A. and Zakharchenko, I. N. and Sviridov, E. V. and Almeida, A. and Chaves, M. R.},\n\tmonth = mar,\n\tyear = {2002},\n\tnote = {Publisher: American Physical Society},\n\tpages = {134107},\n\tfile = {APS Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\DIUXSDGU\\\\PhysRevB.65.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We have studied the concentration dependence of the Raman spectra of heteroepitaxial (Ba1−xSrx)TiO3 (BST) (x=0, 0.15, 0.30, and 0.45) thin films deposited by rf sputtering on (001) MgO substrates. It is found that substitution of Ba by Sr leads to the distortions of the Ti-O bonds and causes the appearance of new bands in the Raman spectra near the bands corresponding to the Ti-O vibrations. The Sr incorporation induces relatively large shifts of the low-frequency Raman peaks attributed to ETO and A1TO components of the soft mode. The ETO soft mode in BST films becomes underdamped for x\\textgreater~0.3 and is very sensitive to the two-dimensional compressive stresses.\n</div>\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"yuzyuk-simon-zakharchenko-alyoshin-sviridov-stresseffectontheferroelectrictoparaelectricphasetransitioninheteroepitaxialbasrtiotextrm3001mgothinfilmstudiedbyramanscatteringandxraydiffraction-2002\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.66.052103\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'yuzyuk-simon-zakharchenko-alyoshin-sviridov-stresseffectontheferroelectrictoparaelectricphasetransitioninheteroepitaxialbasrtiotextrm3001mgothinfilmstudiedbyramanscatteringandxraydiffraction-2002', 'https://link.aps.org/doi/10.1103/PhysRevB.66.052103', event);\">\n    Stress effect on the ferroelectric-to-paraelectric phase transition in heteroepitaxial (Ba, Sr)TiO$_{\\textrm{3}}$/(001) MgO thin film studied by Raman scattering and x-ray diffraction.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Yuzyuk, Y. I.; Simon, P.; Zakharchenko, I. N.; Alyoshin, V. A.;  and Sviridov, E. V.\n</span>\n\n  \n\n</span>\n\n  <i>Physical Review B</i>, 66(5): 052103. August 2002.\n  <span class=\"note\">Publisher: American Physical Society</span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://link.aps.org/doi/10.1103/PhysRevB.66.052103\"\n     onclick=\"log_download('yuzyuk-simon-zakharchenko-alyoshin-sviridov-stresseffectontheferroelectrictoparaelectricphasetransitioninheteroepitaxialbasrtiotextrm3001mgothinfilmstudiedbyramanscatteringandxraydiffraction-2002', 'https://link.aps.org/doi/10.1103/PhysRevB.66.052103', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Stress effect on the ferroelectric-to-paraelectric phase transition in heteroepitaxial (Ba, Sr)TiO$_{\\textrm{3}}$/(001) MgO thin film studied by Raman scattering and x-ray diffraction [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"http://doi.org/10.1103/PhysRevB.66.052103\"\n     onclick=\"log_download('yuzyuk-simon-zakharchenko-alyoshin-sviridov-stresseffectontheferroelectrictoparaelectricphasetransitioninheteroepitaxialbasrtiotextrm3001mgothinfilmstudiedbyramanscatteringandxraydiffraction-2002', 'http://doi.org/10.1103/PhysRevB.66.052103', event.ctrlKey)\"\n     class=\"bibbase doi link\">\n    <span>doi</span></a>\n  &nbsp;\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/yuzyuk-simon-zakharchenko-alyoshin-sviridov-stresseffectontheferroelectrictoparaelectricphasetransitioninheteroepitaxialbasrtiotextrm3001mgothinfilmstudiedbyramanscatteringandxraydiffraction-2002\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n  &nbsp;\n  <a class=\"bibbase_abstract_link bibbase link\"\n     href=\"#\"\n     onclick=\"showAbstract(event); return false;\">\n    abstract <i class=\"fa fa-caret-down\"></i></a>\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('yuzyuk-simon-zakharchenko-alyoshin-sviridov-stresseffectontheferroelectrictoparaelectricphasetransitioninheteroepitaxialbasrtiotextrm3001mgothinfilmstudiedbyramanscatteringandxraydiffraction-2002')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{yuzyuk_stress_2002,\n\ttitle = {Stress effect on the ferroelectric-to-paraelectric phase transition in heteroepitaxial ({Ba}, {Sr}){TiO}$_{\\textrm{3}}$/(001) {MgO} thin film studied by {Raman} scattering and x-ray diffraction},\n\tvolume = {66},\n\turl = {https://link.aps.org/doi/10.1103/PhysRevB.66.052103},\n\tdoi = {10.1103/PhysRevB.66.052103},\n\tabstract = {We report experimental evidence for the stress-induced tetragonal symmetry of the paraelectric phase in heteroepitaxial (Ba0.7Sr0.3)TiO3 thin film deposited on the (001)MgO substrate. Our Raman and x-ray-diffraction data evidently show that symmetry of the paraelectric phase is tetragonal well above the Curie temperature due to the two-dimensional compressive stresses imposed on the film by the substrate. On approaching the deposition temperature the thermoelastic compressive stresses vanish and Raman measurements revealed cubic symmetry of the paraelectric phase.},\n\tnumber = {5},\n\turldate = {2023-11-11},\n\tjournal = {Physical Review B},\n\tauthor = {Yuzyuk, Yu. I. and Simon, P. and Zakharchenko, I. N. and Alyoshin, V. A. and Sviridov, E. V.},\n\tmonth = aug,\n\tyear = {2002},\n\tnote = {Publisher: American Physical Society},\n\tpages = {052103},\n\tfile = {APS Snapshot:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\B9REP2NW\\\\PhysRevB.66.html:text/html},\n}\n\n</pre>\n</div>\n\n\n<div class=\"well well-small bibbase\" data-type=\"abstract\"\n     style=\"display:none\">\n  We report experimental evidence for the stress-induced tetragonal symmetry of the paraelectric phase in heteroepitaxial (Ba0.7Sr0.3)TiO3 thin film deposited on the (001)MgO substrate. Our Raman and x-ray-diffraction data evidently show that symmetry of the paraelectric phase is tetragonal well above the Curie temperature due to the two-dimensional compressive stresses imposed on the film by the substrate. On approaching the deposition temperature the thermoelastic compressive stresses vanish and Raman measurements revealed cubic symmetry of the paraelectric phase.\n</div>\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n  <div class=\"bibbase_group_whole\" id=\"group_undefined\">\n    <div class=\"bibbase_group\"\n      onclick=\"toggleGroup('group_undefined')\"\n      onkeypress=\"toggleGroup('group_undefined')\"\n      tabindex=\"0\">\n      <i class=\"fa fa-angle-down bibbase_group_head_icon\"></i>&nbsp;\n      <span>undefined</span>\n      <span class=\"bibbase_group_count\">\n        \n        (7)\n        \n      </span>\n    </div>\n    <div class=\"bibbase_group_body\">\n      \n  \n  <div class=\"bibbase_paper\" id=\"ru-ru-ru-ru-\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://findpatent.ru/patent/262/2629892.html\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'ru-ru-ru-ru-', 'https://findpatent.ru/patent/262/2629892.html', event);\">\n    Способ измерения физических величин с помощью датчиков на поверхностных акустических волнах.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  Минасян Тигран Арменович (RU); Кайдашев Евгений Михайлович (RU); Кайдашев Владимир Евгеньевич (RU);  and Карапетьян Геворк Яковлевич (RU)\n</span>\n\n  \n\n</span>\n\n   .<!-- NOTE FROM BIBBASE: This entry has an invalid bibtex entry type: patent. Therefore, we don't know how to render it properly. Please consider fixing this. -->\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://findpatent.ru/patent/262/2629892.html\"\n     onclick=\"log_download('ru-ru-ru-ru-', 'https://findpatent.ru/patent/262/2629892.html', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Способ измерения физических величин с помощью датчиков на поверхностных акустических волнах [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/ru-ru-ru-ru-\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('ru-ru-ru-ru-')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@patent{___ru__nodate,\n\ttitle = {Способ измерения физических величин с помощью датчиков на поверхностных акустических волнах},\n\turl = {https://findpatent.ru/patent/262/2629892.html},\n\tnumber = {RU 2629892},\n\tauthor = {{Минасян Тигран Арменович (RU)} and {Кайдашев Евгений Михайлович (RU)} and {Кайдашев Владимир Евгеньевич (RU)} and {Карапетьян Геворк Яковлевич (RU)}},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"anonymous-\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://www.maikonline.com/maik/showArticle.do?auid=VAH1QBBBMQ\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'anonymous-', 'http://www.maikonline.com/maik/showArticle.do?auid=VAH1QBBBMQ', event);\">\n    .\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  \n</span>\n\n  \n\n</span>\n\n   \n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://www.maikonline.com/maik/showArticle.do?auid=VAH1QBBBMQ\"\n     onclick=\"log_download('anonymous-', 'http://www.maikonline.com/maik/showArticle.do?auid=VAH1QBBBMQ', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\" [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/anonymous-\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>9 downloads</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('anonymous-')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@misc{noauthor_notitle_nodate,\n\turl = {http://www.maikonline.com/maik/showArticle.do?auid=VAH1QBBBMQ},\n\turldate = {2023-11-11},\n\tfile = {maikonline.com/maik/showArticle.do?auid=VAH1QBBBMQ:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\APT4EU54\\\\showArticle.html:text/html},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"anonymous-\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://www.maikonline.com/maik/showArticle.do?auid=VAH4QS914Q&amp;lang=ru\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'anonymous-', 'http://www.maikonline.com/maik/showArticle.do?auid=VAH4QS914Q&amp;lang=ru', event);\">\n    .\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  \n</span>\n\n  \n\n</span>\n\n   \n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://www.maikonline.com/maik/showArticle.do?auid=VAH4QS914Q&amp;lang=ru\"\n     onclick=\"log_download('anonymous-', 'http://www.maikonline.com/maik/showArticle.do?auid=VAH4QS914Q&amp;lang=ru', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\" [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/anonymous-\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>9 downloads</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('anonymous-')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@misc{noauthor_notitle_nodate-1,\n\turl = {http://www.maikonline.com/maik/showArticle.do?auid=VAH4QS914Q&amp;lang=ru},\n\turldate = {2023-11-11},\n\tfile = {maikonline.com/maik/showArticle.do?auid=VAH4QS914Q&amp;lang=ru:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\ZC6HN8U9\\\\showArticle.html:text/html},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"anonymous-\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://www.maikonline.com/maik/showArticle.do?auid=VAGWQ43GB0&amp;lang=ru\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'anonymous-', 'http://www.maikonline.com/maik/showArticle.do?auid=VAGWQ43GB0&amp;lang=ru', event);\">\n    .\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  \n</span>\n\n  \n\n</span>\n\n   \n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://www.maikonline.com/maik/showArticle.do?auid=VAGWQ43GB0&amp;lang=ru\"\n     onclick=\"log_download('anonymous-', 'http://www.maikonline.com/maik/showArticle.do?auid=VAGWQ43GB0&amp;lang=ru', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\" [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/anonymous-\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>9 downloads</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('anonymous-')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@misc{noauthor_notitle_nodate-2,\n\turl = {http://www.maikonline.com/maik/showArticle.do?auid=VAGWQ43GB0&amp;lang=ru},\n\turldate = {2023-11-11},\n\tfile = {maikonline.com/maik/showArticle.do?auid=VAGWQ43GB0&amp;lang=ru:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\22TTF2JJ\\\\showArticle.html:text/html},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"anonymous-\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"http://www.maikonline.com/maik/showArticle.do?auid=VAGZTLODNH\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'anonymous-', 'http://www.maikonline.com/maik/showArticle.do?auid=VAGZTLODNH', event);\">\n    .\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  \n</span>\n\n  \n\n</span>\n\n   \n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"http://www.maikonline.com/maik/showArticle.do?auid=VAGZTLODNH\"\n     onclick=\"log_download('anonymous-', 'http://www.maikonline.com/maik/showArticle.do?auid=VAGZTLODNH', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\" [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/anonymous-\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>9 downloads</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('anonymous-')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@misc{noauthor_notitle_nodate-3,\n\turl = {http://www.maikonline.com/maik/showArticle.do?auid=VAGZTLODNH},\n\turldate = {2023-11-11},\n\tfile = {maikonline.com/maik/showArticle.do?auid=VAGZTLODNH:C\\:\\\\Users\\\\aleks\\\\Zotero\\\\storage\\\\9FI6SVHU\\\\showArticle.html:text/html},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"anonymous-\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  <a href=\"https://journals.ioffe.ru/articles/3167\"\n     onclick=\"return trackOutboundLink('publications', 'click', 'anonymous-', 'https://journals.ioffe.ru/articles/3167', event);\">\n    Влияние механизма роста и термоупругих напряжений на динамику кристаллической решетки гетероэпитаксиальных пленок титаната бария–стронция.\n  </a>\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  \n</span>\n\n  \n\n</span>\n\n  .  .\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n  <a href=\"https://journals.ioffe.ru/articles/3167\"\n     onclick=\"log_download('anonymous-', 'https://journals.ioffe.ru/articles/3167', event.ctrlKey, event)\">\n    <img src=\"//bibbase.org/img/filetypes/link.svg\"\n\t     alt=\"Влияние механизма роста и термоупругих напряжений на динамику кристаллической решетки гетероэпитаксиальных пленок титаната бария–стронция [link]\"\n       title=\"Paper\"\n\t     class=\"bibbase_icon\"\n         ><span class=\"bibbase_icon_text\">Paper</span></a>\n  &nbsp;\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/anonymous-\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>9 downloads</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('anonymous-')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\">@article{noauthor__nodate,\n\ttitle = {Влияние механизма роста и термоупругих напряжений на динамику кристаллической решетки гетероэпитаксиальных пленок титаната бария--стронция},\n\turl = {https://journals.ioffe.ru/articles/3167},\n\turldate = {2023-11-11},\n}\n\n</pre>\n</div>\n\n\n\n</div>\n\n\n  <div class=\"bibbase_paper\" id=\"anonymous-\">\n  <span class=\"bibbase_paper_titleauthoryear\">\n\n  \n  <span class=\"bibbase_paper_title\">\n  \n  \n  \n  .\n  \n  \n  \n</span>\n\n  <span class=\"bibbase_paper_author\">\n  \n</span>\n\n  \n\n</span>\n\n  .  .\n  <span class=\"note\"></span>\n\n<span class=\"bibbase_note\"></span>\n\n<br class=\"bibbase_paper_content\"/>\n\n<span class=\"bibbase_paper_content dontprint\">\n\n  \n\n  \n\n  \n  <a href=\"//bibbase.org/network/publication/anonymous-\"\n     class=\"bibbase bibbase_page link\">link</a>\n  &nbsp;\n  \n\n  <a href=\"#\"\n     onclick=\"showBib(event); return false;\"\n     class=\"bibbase bibtex link\">bibtex\n    <i class=\"fa fa-caret-down\"></i></a>\n\n  \n\n  \n  &nbsp;\n  <span class=\"bibbase_stats_paper\" style=\"color: #777;\">\n    <span>9 downloads</span>\n  </span>\n  \n\n  <!-- <a class=\"bibbase read link hidden\" -->\n  <!--    href=\"javascript:toggleRead('anonymous-')\" -->\n  <!--    title=\"Marking this paper as read adds it to your library on BibBase.\" -->\n  <!--    > -->\n  <!--   <i class=\"fa fa-check\"></i>&nbsp; -->\n  <!--   <span>mark as read</span> -->\n  <!-- </a> -->\n\n  &nbsp;\n  \n  \n\n</span>\n\n<div class=\"well well-small bibbase\" data-type=\"bibtex\"\n     style=\"display:none\">\n  <pre style=\"white-space: pre-wrap;\"></pre>\n</div>\n\n\n\n</div>\n\n\n\n\n\n    </div>\n  </div>\n\n\n\n\n  </div>\n\n\n  <!-- Modal -->\n\n  <!-- <iframe id=\"bibbase_network_frame\" -->\n  <!--         src=\"//bibbase.org/network/control\" -->\n  <!--         style=\"display: none;\"> -->\n  <!-- </iframe> -->\n\n</div>\n"}; document.write(bibbase_data.data);