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Electronic Structure of Oxide Interfaces: A Comparative Analysis of GdTiO3/SrTiO3 and LaAlO3/SrTiO3 Interfaces

机译:氧化物界面的电子结构:GdTiO3 / SrTiO3和LaAlO3 / SrTiO3界面的比较分析

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摘要

Emergent phases in the two-dimensional electron gas (2DEG) formed at the interface between two insulating oxides have attracted great attention in the past decade. We present ab-initio electronic structure calculations for the interface between a Mott insulator GdTiO3 (GTO) and a band insulator SrTiO3 (STO) and compare our results with those for the widely studied LaAlO3/SrTiO3 (LAO/STO) interface between two band insulators. Our GTO/STO results are in excellent agreement with experiments, but qualitatively different from LAO/STO. We find an interface carrier density of 0.5 e/Ti, independent of GTO thickness in both superlattice and thin film geometries, in contrast to LAO/STO. The superlattice geometry in LAO/STO offers qualitatively the same result as in GTO/STO. On the other hand, for a thin film geometry, the interface carrier density builds up only beyond a threshold thickness of LAO. The positive charge at the vacuum surface that compensates the 2DEG at the interface also exhibits distinct behaviors in the two systems. The compensating positive charge at the exposed surface of GTO charge disproportionates due to correlation effect making the surface insulating as opposed to that in LAO which remains metallic within band theory and presumably becomes insulating due to surface disorder or surface reconstruction.
机译:在过去的十年中,在两种绝缘氧化物之间的界面处形成的二维电子气(2DEG)中的新兴相引起了极大的关注。我们介绍了莫特绝缘子GdTiO3(GTO)和带状绝缘子SrTiO3(STO)之间的界面的从头算电子结构计算,并将我们的结果与两个带状绝缘子之间广泛研究的LaAlO3 / SrTiO3(LAO / STO)界面的结果进行了比较。我们的GTO / STO结果与实验非常吻合,但在质量上与LAO / STO不同。我们发现,与LAO / STO相比,在超晶格和薄膜几何中,界面载流子密度为0.5 e - / Ti,与GTO厚度无关。 LAO / STO中的超晶格几何定性提供与GTO / STO中相同的结果。另一方面,对于薄膜几何形状,仅在超过LAO的阈值厚度时才建立界面载流子密度。真空表面上的正电荷在界面处补偿了2DEG,在两个系统中也表现出不同的行为。 GTO电荷暴露表面的补偿正电荷由于相关效应而使表面绝缘,这与带理论中保持金属状态的LAO中的绝缘效应相反,并且可能由于表面无序或表面重构而绝缘。

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