Variety of magnetic topological phases in the (MnBi\(_2\)Te\(_4\))(Bi\(_2\)Te\(_3\))\(_m\) family

• Published in: arXiv.org 2019-10
• Main Authors: Klimovskikh, I I, Otrokov, M M, Estyunin, D, Eremeev, S V, Filnov, S O, Koroleva, A, Shevchenko, E, Voroshnin, V, Rusinov, I P, Blanco-Rey, M, Hoffmann, M, Aliev, Z S, Babanly, M B, Amiraslanov, I R, Abdullayev, N A, Zverev, V N, Kimura, A, Tereshchenko, O E, Kokh, K A, Petaccia, L, G Di Santo, Ernst, A, Echenique, P M, Mamedov, N T, Shikin, A M, Chulkov, E V
• Format: Article
• Language: English
• Subjects: Antiferromagnetism; Bismuth; Critical temperature; Ferromagnetism; Heterostructures; Homology; Magnetic properties; Magnetism; Phases; Photoelectric emission; Quantum computing; Spintronics; Topological insulators; Topology
• ISSN: 2331-8422
• DOI: 10.48550/arxiv.1910.11653

Quantum states of matter combining non-trivial topology and magnetism attract a lot of attention nowadays; the special focus is on magnetic topological insulators (MTIs) featuring quantum anomalous Hall and axion insulator phases. Feasibility of many novel phenomena that \emph{intrinsic} magnetic TIs may host depends crucially on our ability to engineer and efficiently tune their electronic and magnetic structures. Here, using angle- and spin-resolved photoemission spectroscopy along with \emph{ab initio} calculations we report on a large family of intrinsic magnetic TIs in the homologous series of the van der Waals compounds (MnBi\(_2\)Te\(_4\))(Bi\(_2\)Te\(_3\))\(_m\) with \(m=0, ..., 6\). Magnetic, electronic and, consequently, topological properties of these materials depend strongly on the \(m\) value and are thus highly tunable. The antiferromagnetic (AFM) coupling between the neighboring Mn layers strongly weakens on moving from MnBi2Te4 (m=0) to MnBi4Te7 (m=1), changes to ferromagnetic (FM) one in MnBi6Te10 (m=2) and disappears with further increase in m. In this way, the AFM and FM TI states are respectively realized in the \(m=0,1\) and \(m=2\) cases, while for \(m \ge 3\) a novel and hitherto-unknown topologically-nontrivial phase arises, in which below the corresponding critical temperature the magnetizations of the non-interacting 2D ferromagnets, formed by the \MBT\, building blocks, are disordered along the third direction. The variety of intrinsic magnetic TI phases in (MnBi\(_2\)Te\(_4\))(Bi\(_2\)Te\(_3\))\(_m\) allows efficient engineering of functional van der Waals heterostructures for topological quantum computation, as well as antiferromagnetic and 2D spintronics.