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Spatially Tunable High-density electron gas at the KTaO<sub>3</sub>/TbScO<sub>3 </sub> (001) interface

ORAL

Abstract

The interface between 3d and 5d polar oxides has potentials for thickness independent high-density electron gas that is highly tunable in terms of spatial localization, orbital distribution, and density, much of which are not available widely studied interface between polar-nonpolar oxide interfaces. As a model system for observing such behavior, we studied the (001) interface between polar KTaO3(KTO) and polar TbScO3 (TSO) and found a large density (> 1e/uc) two-dimensional electron gas (2DEG) spread across interface in both materials. While the electron gas density at the TSO side of the interface is small (<3% of total) and localized within the unit cell (less than half a nm), the concentration of electron gas in the KTO side of the interface is much larger (remaining ~97%), and the spread is much longer (at least 3 nm). An applied external voltage can tune the spatial location of electron gas across the interface. The metallic nature of KTO across the interface and eventual charge compensation may need a capping layer for experimental detection of 2DEG when the KTO thickness is less than two unit cells, similar to what is required for detecting hole gas at the surface of LAO/STO (001) heterostructure.

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Presenters

  • Tula Paudel

    Department of Physics, South Dakota School of Mines and Technology

Authors

  • Bhubnesh Lama

    Department of Physics, South Dakota School of Mines and Technology

  • Kitae Eom

    Materials Science and Engineering, University of Wisconsin-Madison, Department of Materials Science and Engineering, University of Wisconsin-Maddison, Department of Materials Science and Engineering, University of Wisconsin, Department of Materials Science Engineering, University of Wisconsin-Madison, Department of Materials Science and Engineering, University of Wisconsin-Madison,, University of Wisconsin, Material Science and Engineering, University of Wisconsin-Madison, University of Wisconsin-Madison, University of Wisconsin-Maddison

  • Jungwoo Lee

    Materials Science and Engineering, University of Wisconsin-Madison, University of Wisconsin, Madison, Department of Materials Science and Engineering, University of Wisconsin-Madison,, University of Wisconsin, University of Wisconsin-Madison, University of Wisconsin-Maddison, Department of Materials Science and Engineering, University of Wisconsin-Madison

  • Evgeny Y Tsymbal

    University of Nebraska - Lincoln, Department of Physics and Astronomy, Nebraska Center for Materials and Nanoscience, University of Nebraska, Lincoln, Department of Physics and Astronomy & Nebraska Center for Materials and Nanoscience, University of Nebraska - Lincoln

  • Chang-Beom Eom

    Materials Science and Engineering, University of Wisconsin-Madison, University of Wisconsin, Madison, Department of Materials Science and Engineering, University of Wisconsin-Maddison, Department of Materials Science and Engineering, University of Wisconsin, Department of Materials Science Engineering, University of Wisconsin-Madison, Department of Materials Science and Engineering, University of Wisconsin-Madison,, University of Wisconsin, Material Science and Engineering, University of Wisconsin-Madison, University of Wisconsin-Madison, University of Wisconsin-Maddison, University of Wisconsin - Madison, University of Wisconsin Madison, Department of Materials Science and Engineering, University of Wisconsin-Madison

  • Tula Paudel

    Department of Physics, South Dakota School of Mines and Technology