Trends of electronic and magnetic properties of transition-metal impurities in Sb$_{\mathrm{2}}$Te$_{\mathrm{3}}$ topological insulator.

ORAL

Abstract

The interaction between topological insulator (TI) surface states and magnetic order is crucial for future applications in spintronics and for the realization of novel quantum phenomena such as the quantum anomalous Hall effect (QAHE). Despite experimental progress in measuring the signatures of the QAHE in thin films of magnetically-doped TIs, the fate of the topological surface states, i.e. the presence or absence of a gap upon magnetic doping [1] as well as the nature of magnetic interactions in these systems [2] are under debate. Motivated by on-going experiments, we have systematically investigated the electronic structure and the magnetic anisotropy of transition-metal doped Sb$_{\mathrm{2}}$Te$_{\mathrm{3}}$ for both bulk and surface doping, using first-principles calculations based on density functional theory. In addition to magnetization-dependent gap, magnetic dopants introduce impurity states in the gap, whose detailed electronic and magnetic structure depends on the specific character of the dopant. We use these results to identify the conditions for the realization of a robust QAHE. [1] Sessi et al., Nat. Comm. 7, 12027 (2016); [2] Grauer et al., Phys. Rev. B 92, 201304 (2015).

Authors

  • C. M. Canali

    Linnaeus University, Department of Physics and Electrical Engineering, Linnaeus University, 391 82 Kalmar, Sweden, Department of Physics and Electrical Engineering, Linnaeus University, SE-391 82 Kalmar, Sweden

  • Anna Pertsova

    Nordita, KTH Royal Institute of Technology and Stockholm University

  • Fhokrul Islam

    Linnaeus University, Department of Physics and Electrical Engineering, Linnaeus University, 391 82 Kalmar, Sweden

  • Alexander Balatsky

    Nordita, KTH Royal Institute of Technology, Stockholm University and Los Alamos National Laboratory, Nordita, KTH Royal Institute of Technology and Stockholm University; Institute for Materials Science, Los Alamos National Laboratory, USA, Nordita, Center for Quantum Materials, KTH Royal Institute of Technology and Stockholm University, Stockholm, Sweden, Nordita, KTH Royal Institute of Technology and Stockholm University; Institute for Materials Science, Los Alamos National Laboratory, Los Alamos National Laboratory, NORDITA, Institute for Materials Science, Los Alamos National Laboratory, USA; Nordita, KTH Royal Institute of Technology and Stockholm University, Sweden, Nordita, Center for Quantum Materials, KTH Royal Institute of Technology and Stockholm University, Roslagstullsbacken 23, SE-106 91 Stockholm, Sweden, Nordita, Center for Quantum Materials, Stockholm University and KTH, Stockholm and Institute for Materials Science, LANL, Los Alamos, USA