Localization of two-dimensional electron gas in LaAlO3/SrTiO3 heterostructures. Hernandez, T., Bark, C. W., Felker, D. A., Eom, C. B., & Rzchowski, M. S. PHYSICAL REVIEW B, APR 18, 2012. doi abstract bibtex We report strong localization of two-dimensional electron gas in LaAlO3/SrTiO3 epitaxial thin-film heterostructures grown on (LaAlO3)(0.3)-(Sr2AlTaO3)(0.7) substrates by using pulsed laser deposition with in situ reflection high-energy electron diffraction. Using longitudinal and transverse magnetotransport measurements, we have determined that disorder at the interface influences the conduction behavior, and that increasing the carrier concentration by growing at lower oxygen partial pressure changes the conduction from strongly localized at low carrier concentration to metallic at higher carrier concentration, with indications of weak localization. We interpret this behavior in terms of a changing occupation of Ti 3d bands near the interface, each with a different spatial extent and susceptibility to localization by disorder, and differences in carrier confinement due to misfit strain and point defects.
@article{ ISI:000302960500001,
Author = {Hernandez, T. and Bark, C. W. and Felker, D. A. and Eom, C. B. and
Rzchowski, M. S.},
Title = {{Localization of two-dimensional electron gas in LaAlO3/SrTiO3
heterostructures}},
Journal = {{PHYSICAL REVIEW B}},
Year = {{2012}},
Volume = {{85}},
Number = {{16}},
Month = {{APR 18}},
Abstract = {{We report strong localization of two-dimensional electron gas in
LaAlO3/SrTiO3 epitaxial thin-film heterostructures grown on
(LaAlO3)(0.3)-(Sr2AlTaO3)(0.7) substrates by using pulsed laser
deposition with in situ reflection high-energy electron diffraction.
Using longitudinal and transverse magnetotransport measurements, we have
determined that disorder at the interface influences the conduction
behavior, and that increasing the carrier concentration by growing at
lower oxygen partial pressure changes the conduction from strongly
localized at low carrier concentration to metallic at higher carrier
concentration, with indications of weak localization. We interpret this
behavior in terms of a changing occupation of Ti 3d bands near the
interface, each with a different spatial extent and susceptibility to
localization by disorder, and differences in carrier confinement due to
misfit strain and point defects.}},
DOI = {{10.1103/PhysRevB.85.161407}},
Article-Number = {{161407}},
ISSN = {{1098-0121}},
ResearcherID-Numbers = {{Bark, Chung Wung/B-9534-2014
Eom, Chang-Beom/I-5567-2014}},
ORCID-Numbers = {{Bark, Chung Wung/0000-0002-9394-4240
}},
Unique-ID = {{ISI:000302960500001}},
}
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