Probe-dependent Dirac-point gap in the gadolinium-doped thallium-based topological insulator TlBi0.9Gd0.1Se2

S. O. Filnov, I. I. Klimovskikh, D. A. Estyunin, A. V. Fedorov, V. Yu. Voroshnin, A. V. Koroleva, A. G. Rybkin, E. V. Shevchenko, Z. S. Aliev, M. B. Babanly, I. R. Amiraslanov, N. T. Mamedov, E. F. Schwier, K. Miyamoto, T. Okuda, S. Kumar, A. Kimura, V. M. Misheneva, A. M. Shikin, and E. V. Chulkov
Phys. Rev. B 102, 085149 – Published 26 August 2020
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Abstract

A tunable gap in the topological surface state is of great interest for novel spintronic devices and applications in quantum computing. Here, we study the surface electronic structure and magnetic properties of the Gd-doped topological insulator TlBi0.9Gd0.1Se2. Utilizing superconducting quantum interference device magnetometry, we show paramagnetic behavior down to 2 K. Combining spin- and angle-resolved photoemission spectroscopy with different polarizations of light, we demonstrate that the topological surface state is characterized by the Dirac cone with a helical spin structure and confirm its localization within the bulk band gap. By using different light sources in photoemission spectroscopy, various Dirac-point gap values were observed: 50 meV for hν=18eV and 20 meV for hν=6.3eV. Here, we discuss the gap observation by the angle-resolved photoemission spectroscopy method as a consequence of the scattering processes. Simulating the corresponding spectral function, we demonstrate that the asymmetric energy-distribution curve of the surface state leads to an overestimation of the corresponding gap value. We speculate that 20 meV in our case is a trustworthy value and attribute this gap to be originated by scattering both on magnetic and charge impurities provided by Gd atoms and surface defects. Given the complexity and importance of scattering processes in the topological surface state together with our observations of distinctive photoemission asymmetry, we believe our results are important for research of the massive Dirac fermions in novel quantum materials.

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  • Received 31 December 2019
  • Revised 11 June 2020
  • Accepted 27 July 2020

DOI:https://doi.org/10.1103/PhysRevB.102.085149

©2020 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

S. O. Filnov1,*, I. I. Klimovskikh1, D. A. Estyunin1, A. V. Fedorov2,3, V. Yu. Voroshnin3,1, A. V. Koroleva1, A. G. Rybkin1, E. V. Shevchenko1, Z. S. Aliev4,5, M. B. Babanly6,7, I. R. Amiraslanov5,7, N. T. Mamedov5, E. F. Schwier8, K. Miyamoto8, T. Okuda8, S. Kumar8, A. Kimura9,10, V. M. Misheneva1, A. M. Shikin1, and E. V. Chulkov11,12,1,13

  • 1Saint Petersburg State University, 198504 Saint Petersburg, Russia
  • 2IFW Dresden, Helmholtzstrasse 20, 01069 Dresden, Germany
  • 3Helmholtz-Zentrum Berlin fr Materialien und Energie, Albert-Einstein-Strasse 15, 12489 Berlin, Germany
  • 4Azerbaijan State Oil and Industry University, AZ 1010 Baku, Azerbaijan
  • 5Institute of Physics, Azerbaijan National Academy of Sciences, AZ 1143 Baku, Azerbaijan
  • 6Institute of Catalysis and Inorganic Chemistry, Azerbaijan National Academy of Science, AZ1143 Baku, Azerbaijan
  • 7Baku State University, AZ 1148 Baku, Azerbaijan
  • 8Hiroshima Synchrotron Radiation Center, Hiroshima University, 2-313 Kagamiyama, Higashi-Hiroshima, Hiroshima 739-0046, Japan
  • 9Department of Physical Sciences, Graduate School of Science, Hiroshima University, 1-3-1 Kagamiyama, Higashi-Hiroshima, Hiroshima 739-8526, Japan
  • 10Graduate School of Advanced Science and Engineering, Hiroshima University, 1-3-1 Kagamiyama, Higashi-Hiroshima 739-8526, Japan
  • 11Tomsk State University, 634050 Tomsk, Russia
  • 12Donostia International Physics Center (DIPC), 20018 San Sebastin/Donostia, Basque Country, Spain
  • 13Centro de Física de Materiales (CFM-MPC), Centro Mixto CSIC-UPV/EHU, 20080 San Sebastin/Donostia, Basque Country, Spain

  • *st040513@student.spbu.ru

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Issue

Vol. 102, Iss. 8 — 15 August 2020

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