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Subband Structure of a Two-Dimensional Electron Gas Formed at the Polar Surface of the Strong Spin-Orbit Perovskite KTaO3

P. D. C. King, R. H. He, T. Eknapakul, P. Buaphet, S.-K. Mo, Y. Kaneko, S. Harashima, Y. Hikita, M. S. Bahramy, C. Bell, Z. Hussain, Y. Tokura, Z.-X. Shen, H. Y. Hwang, F. Baumberger, and W. Meevasana
Phys. Rev. Lett. 108, 117602 – Published 14 March 2012

Abstract

We demonstrate the formation of a two-dimensional electron gas (2DEG) at the (100) surface of the 5d transition-metal oxide KTaO3. From angle-resolved photoemission, we find that quantum confinement lifts the orbital degeneracy of the bulk band structure and leads to a 2DEG composed of ladders of subband states of both light and heavy carriers. Despite the strong spin-orbit coupling, our measurements provide a direct upper bound for the potential Rashba spin splitting of only Δk0.02Å1 at the Fermi level. The polar nature of the KTaO3(100) surface appears to help mediate the formation of the 2DEG as compared to nonpolar SrTiO3(100).

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  • Received 31 August 2011

DOI:https://doi.org/10.1103/PhysRevLett.108.117602

© 2012 American Physical Society

Authors & Affiliations

P. D. C. King1, R. H. He2, T. Eknapakul3, P. Buaphet3, S.-K. Mo2, Y. Kaneko4, S. Harashima5, Y. Hikita6,7, M. S. Bahramy8, C. Bell6,7, Z. Hussain2, Y. Tokura4,5,8, Z.-X. Shen6,7, H. Y. Hwang6,7,8, F. Baumberger1,*, and W. Meevasana3,9,†

  • 1SUPA, School of Physics and Astronomy, University of St. Andrews, St. Andrews, Fife KY16 9SS, United Kingdom
  • 2Advanced Light Source, Lawrence Berkeley National Lab, Berkeley, California 94720, USA
  • 3School of Physics, Suranaree University of Technology and Synchrotron Light Research Institute, Nakhon Ratchasima, 30000, Thailand
  • 4Multiferroics Project, ERATO, JST, Tokyo 113-8656, Japan
  • 5Department of Applied Physics, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan
  • 6Departments of Physics and Applied Physics, Stanford University, California 94305, USA
  • 7Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, California 94025, USA
  • 8Correlated Electron Research Group (CERG), RIKEN-ASI, Wako 351-0918, Japan
  • 9Thailand Center of Excellence in Physics, CHE, Bangkok, 10400, Thailand

  • *Corresponding author. fb40@st-andrews.ac.uk
  • Corresponding author. worawat@g.sut.ac.th

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Issue

Vol. 108, Iss. 11 — 16 March 2012

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Images

  • Figure 1
    Figure 1
    (a),(b) ARPES measurements of the ΓX dispersion of surface 2DEG states in KTaO3, measured using p- and s-polarized 55 eV synchrotron light around the Γ11 and Γ10 points, respectively. A schematic representation of the measured band structure is shown in the insets. (c),(d) Equivalent measurements of the Fermi surface.Reuse & Permissions
  • Figure 2
    Figure 2
    (a) Irradiation dose dependence of the Fermi wave vector of the deepest dxy-type band of surface 2DEGs formed in SrTiO3 and KTaO3 upon exposure to intense UV light, normalized to their saturation values. A low-energy electron diffraction image of KTaO3, taken after UV light exposure, is shown in the inset. (b) O 2p valence bands of KTaO3 after small and heavier irradiation doses, with the near-EF emission magnified in the inset.Reuse & Permissions
  • Figure 3
    Figure 3
    Local-density approximation (LDA) calculations of the bulk electronic structure and orbital character of KTaO3 (a) excluding and (b) including spin-orbit coupling. (c) Comparison of measured dispersions to model tight-binding calculations of a surface 2DEG in SrTiO3. (d) Equivalent calculations for a KTaO3 2DEG, including the strong spin-orbit coupling. The colored lines give a schematic decomposition of its orbital makeup. (e) Comparison of the KTaO3 calculations to the experimental data from Figs. 1a, 1b.Reuse & Permissions
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