Electronic Structure of Liquid Alkanes: A Representative Case of Liquid Hexanes and Cyclohexane Studied Using Polarization-Dependent Two-Photon Absorption Spectroscopy. Bhattacharyya, D., Zhang, Y., Elles, C. G., & Bradforth, S. E. The Journal of Physical Chemistry A, American Chemical Society (ACS), 2021. 
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Paper doi abstract bibtex Two-photon absorption (2PA) spectra of liquid cyclohexane and hexanes are reported for the energy range 6.4–8.5 eV (177–145 nm), providing detailed information about their electronic structures in bulk liquid. Using a broadband pump–probe fashion, we measured the continuous 2PA spectra by simultaneous absorption of a 266 nm (4.6 eV) pump photon and one UV–vis probe photon from the white-light continuum (1.8–3.9 eV). Theoretical one-photon absorption (1PA) and 2PA cross sections of isolated gas phase molecules are computed by the equation of motion coupled-cluster method with single and double substitutions (EOM-CCSD) to substantiate the assignment of the experimental spectra, and the natural transition orbital (NTO) analysis provides visualization of the participating orbitals in a transition. Our analysis suggests that upon solvation transitions at the lowest excitation energy involving promotion of electron to the 3s Rydberg orbitals are blue-shifted (∼0.55 eV for cyclohexane and ∼0.18 eV for hexanes) to a greater extent as compared to those involving other Rydberg orbitals, which is similar to the behavior observed for water and alcohols. All other transitions experience negligible (cyclohexane) or minor red-shift by ∼0.15-0.2 eV (hexane) upon solvation. In both alkanes, the spectra are entirely dominated by Rydberg transitions: the most intense bands in 1PA and 2PA spectra are due to the excitation of electrons to the Rydberg “p” and “d” type orbitals, respectively, although one transition terminating in the 3s Rydberg has significant 2PA strength. This work demonstrates that the gas phase electronic transition properties in alkanes are not significantly altered upon solvation. In addition, electronic structure calculations using an isolated-molecule framework appear to provide a reasonable starting point for a semiquantitative picture for spectral assignment and also to analyze the solvatochromic shifts for liquid phase absorption spectra.
@article{Bhattacharyya_2021,
doi = {10.1021/acs.jpca.1c06230},
url = {https://doi.org/10.1021%2Facs.jpca.1c06230},
year = 2021,
publisher = {American Chemical Society ({ACS})},
author = {Dhritiman Bhattacharyya and Yuyuan Zhang and Christopher G. Elles and Stephen E. Bradforth},
title = {Electronic Structure of Liquid Alkanes: A Representative Case of Liquid Hexanes and Cyclohexane Studied Using Polarization-Dependent Two-Photon Absorption Spectroscopy},
journal = {The Journal of Physical Chemistry A},
abstract = {Two-photon absorption (2PA) spectra of liquid cyclohexane and hexanes are reported for the energy range 6.4–8.5 eV (177–145 nm), providing detailed information about their electronic structures in bulk liquid. Using a broadband pump–probe fashion, we measured the continuous 2PA spectra by simultaneous absorption of a 266 nm (4.6 eV) pump photon and one UV–vis probe photon from the white-light continuum (1.8–3.9 eV). Theoretical one-photon absorption (1PA) and 2PA cross sections of isolated gas phase molecules are computed by the equation of motion coupled-cluster method with single and double substitutions (EOM-CCSD) to substantiate the assignment of the experimental spectra, and the natural transition orbital (NTO) analysis provides visualization of the participating orbitals in a transition. Our analysis suggests that upon solvation transitions at the lowest excitation energy involving promotion of electron to the 3s Rydberg orbitals are blue-shifted (∼0.55 eV for cyclohexane and ∼0.18 eV for hexanes) to a greater extent as compared to those involving other Rydberg orbitals, which is similar to the behavior observed for water and alcohols. All other transitions experience negligible (cyclohexane) or minor red-shift by ∼0.15-0.2 eV (hexane) upon solvation. In both alkanes, the spectra are entirely dominated by Rydberg transitions: the most intense bands in 1PA and 2PA spectra are due to the excitation of electrons to the Rydberg “p” and “d” type orbitals, respectively, although one transition terminating in the 3s Rydberg has significant 2PA strength. This work demonstrates that the gas phase electronic transition properties in alkanes are not significantly altered upon solvation. In addition, electronic structure calculations using an isolated-molecule framework appear to provide a reasonable starting point for a semiquantitative picture for spectral assignment and also to analyze the solvatochromic shifts for liquid phase absorption spectra.},
bibbase_note = {<img src="https://pubs.acs.org/cms/10.1021/acs.jpca.1c06230/asset/images/medium/jp1c06230_0009.gif">}
}
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Using a broadband pump–probe fashion, we measured the continuous 2PA spectra by simultaneous absorption of a 266 nm (4.6 eV) pump photon and one UV–vis probe photon from the white-light continuum (1.8–3.9 eV). Theoretical one-photon absorption (1PA) and 2PA cross sections of isolated gas phase molecules are computed by the equation of motion coupled-cluster method with single and double substitutions (EOM-CCSD) to substantiate the assignment of the experimental spectra, and the natural transition orbital (NTO) analysis provides visualization of the participating orbitals in a transition. Our analysis suggests that upon solvation transitions at the lowest excitation energy involving promotion of electron to the 3s Rydberg orbitals are blue-shifted (∼0.55 eV for cyclohexane and ∼0.18 eV for hexanes) to a greater extent as compared to those involving other Rydberg orbitals, which is similar to the behavior observed for water and alcohols. All other transitions experience negligible (cyclohexane) or minor red-shift by ∼0.15-0.2 eV (hexane) upon solvation. In both alkanes, the spectra are entirely dominated by Rydberg transitions: the most intense bands in 1PA and 2PA spectra are due to the excitation of electrons to the Rydberg “p” and “d” type orbitals, respectively, although one transition terminating in the 3s Rydberg has significant 2PA strength. This work demonstrates that the gas phase electronic transition properties in alkanes are not significantly altered upon solvation. In addition, electronic structure calculations using an isolated-molecule framework appear to provide a reasonable starting point for a semiquantitative picture for spectral assignment and also to analyze the solvatochromic shifts for liquid phase absorption spectra.","bibbase_note":"<img src=\"https://pubs.acs.org/cms/10.1021/acs.jpca.1c06230/asset/images/medium/jp1c06230_0009.gif\">","bibtex":"@article{Bhattacharyya_2021,\n\tdoi = {10.1021/acs.jpca.1c06230},\n\turl = {https://doi.org/10.1021%2Facs.jpca.1c06230},\n\tyear = 2021,\n\tpublisher = {American Chemical Society ({ACS})},\n\tauthor = {Dhritiman Bhattacharyya and Yuyuan Zhang and Christopher G. Elles and Stephen E. Bradforth},\n\ttitle = {Electronic Structure of Liquid Alkanes: A Representative Case of Liquid Hexanes and Cyclohexane Studied Using Polarization-Dependent Two-Photon Absorption Spectroscopy},\n\tjournal = {The Journal of Physical Chemistry A},\n\tabstract = {Two-photon absorption (2PA) spectra of liquid cyclohexane and hexanes are reported for the energy range 6.4–8.5 eV (177–145 nm), providing detailed information about their electronic structures in bulk liquid. Using a broadband pump–probe fashion, we measured the continuous 2PA spectra by simultaneous absorption of a 266 nm (4.6 eV) pump photon and one UV–vis probe photon from the white-light continuum (1.8–3.9 eV). Theoretical one-photon absorption (1PA) and 2PA cross sections of isolated gas phase molecules are computed by the equation of motion coupled-cluster method with single and double substitutions (EOM-CCSD) to substantiate the assignment of the experimental spectra, and the natural transition orbital (NTO) analysis provides visualization of the participating orbitals in a transition. Our analysis suggests that upon solvation transitions at the lowest excitation energy involving promotion of electron to the 3s Rydberg orbitals are blue-shifted (∼0.55 eV for cyclohexane and ∼0.18 eV for hexanes) to a greater extent as compared to those involving other Rydberg orbitals, which is similar to the behavior observed for water and alcohols. All other transitions experience negligible (cyclohexane) or minor red-shift by ∼0.15-0.2 eV (hexane) upon solvation. In both alkanes, the spectra are entirely dominated by Rydberg transitions: the most intense bands in 1PA and 2PA spectra are due to the excitation of electrons to the Rydberg “p” and “d” type orbitals, respectively, although one transition terminating in the 3s Rydberg has significant 2PA strength. This work demonstrates that the gas phase electronic transition properties in alkanes are not significantly altered upon solvation. In addition, electronic structure calculations using an isolated-molecule framework appear to provide a reasonable starting point for a semiquantitative picture for spectral assignment and also to analyze the solvatochromic shifts for liquid phase absorption spectra.},\n\tbibbase_note = {<img src=\"https://pubs.acs.org/cms/10.1021/acs.jpca.1c06230/asset/images/medium/jp1c06230_0009.gif\">}\n\n}","author_short":["Bhattacharyya, D.","Zhang, Y.","Elles, C. G.","Bradforth, S. 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