6533b7dcfe1ef96bd1272016

RESEARCH PRODUCT

Two-dimensional electron gas at the LaAlO$_3$/SrTiO$_3$ inteface with a potential barrier

Vladimir A. StephanovichVitalii K. DugaevJózef Barnaś

subject

Materials scienceCondensed matter physicsStrongly Correlated Electrons (cond-mat.str-el)Band gapGeneral Physics and AstronomyFOS: Physical sciences02 engineering and technologyElectronConductivity021001 nanoscience & nanotechnologyCritical value01 natural sciencesCondensed Matter - Strongly Correlated ElectronsTight binding0103 physical sciencesRectangular potential barrierCharge carrierPhysical and Theoretical Chemistry010306 general physics0210 nano-technologyElectronic band structure

description

We present a tight binding description of electronic properties of the interface between LaAlO$_3$ (LAO) and SrTiO$_3$ (STO). The description assumes LAO and STO perovskites as sets of atomic layers in the $x$-$y$ plane, which are weakly coupled by an interlayer hopping term along the $z$ axis. The interface is described by an additional potential, $U_0$, which simulates a planar defect. Physically, the interfacial potential can result from either a mechanical stress at the interface or other structural imperfections. We show that depending on the potential strength, charge carriers (electrons or holes) may form an energy band which is localized at the interface and is within the band gaps of the constituting materials (LAO and STO). Moreover, our description predicts a {\it valve effect} at a certain critical potential strength, $U_{0cr}$, when the interface potential works as a valve suppressing the interfacial conductivity. In other words, the interfacial electrons become dispersionless at $U_0= U_{0cr}$, and thus cannot propagate. This critical value separates the {\it quasielectron} ($U_0$ $U_{0cr}$) regimes of the interfacial conductivity.

https://dx.doi.org/10.48550/arxiv.1510.07575