Magnetic-field-induced topological phase transition in Fe-doped (Bi,Sb)Se heterostructures
arXiv:2002.09292 · doi:10.1103/PhysRevMaterials.4.044202
Abstract
Three-dimensional topological insulators (3D-TIs) possess a specific topological order of electronic bands, resulting in gapless surface states via bulk-edge correspondence. Exotic phenomena have been realized in ferromagnetic TIs, such as the quantum anomalous Hall (QAH) effect with a chiral edge conduction and a quantized value of the Hall resistance . Here, we report on the emergence of distinct topological phases in paramagnetic Fe-doped (Bi,Sb)Se heterostructures with varying structure architecture, doping, and magnetic and electric fields. Starting from a 3D-TI, a two-dimensional insulator appears at layer thicknesses below a critical value, which turns into an Anderson insulator for Fe concentrations sufficiently large to produce localization by magnetic disorder. With applying a magnetic field, a topological transition from the Anderson insulator to the QAH state occurs, which is driven by the formation of an exchange gap owing to a giant Zeeman splitting and reduced magnetic disorder. Topological phase diagram of (Bi,Sb)Se allows exploration of intricate interplay of topological protection, magnetic disorder, and exchange splitting.
arXiv comment31 pages, 4 figures and supplementary 30 pages, 11 figures
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