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Limit of the electrostatic doping in two-dimensional electron gases of LaXO(3)(X = Al, Ti)/SrTiO(3)

In LaTiO(3)/SrTiO(3) and LaAlO(3)/SrTiO(3) heterostructures, the bending of the SrTiO(3) conduction band at the interface forms a quantum well that contains a superconducting two-dimensional electron gas (2-DEG). Its carrier density and electronic properties, such as superconductivity and Rashba spi...

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Detalles Bibliográficos
Autores principales: Biscaras, J., Hurand, S., Feuillet-Palma, C., Rastogi, A., Budhani, R. C., Reyren, N., Lesne, E., Lesueur, J., Bergeal, N.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2014
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4209450/
https://www.ncbi.nlm.nih.gov/pubmed/25346028
http://dx.doi.org/10.1038/srep06788
Descripción
Sumario:In LaTiO(3)/SrTiO(3) and LaAlO(3)/SrTiO(3) heterostructures, the bending of the SrTiO(3) conduction band at the interface forms a quantum well that contains a superconducting two-dimensional electron gas (2-DEG). Its carrier density and electronic properties, such as superconductivity and Rashba spin-orbit coupling can be controlled by electrostatic gating. In this article we show that the Fermi energy lies intrinsically near the top of the quantum well. Beyond a filling threshold, electrons added by electrostatic gating escape from the well, hence limiting the possibility to reach a highly-doped regime. This leads to an irreversible doping regime where all the electronic properties of the 2-DEG, such as its resistivity and its superconducting transition temperature, saturate. The escape mechanism can be described by the simple analytical model we propose.