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Prediction and observation of the first antiferromagnetic topological insulator
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abstract
Magnetic topological insulators (MTIs) are narrow gap semiconductor materials that combine non-trivial band topology and magnetic order. Unlike their nonmagnetic counterparts, MTIs may have some of the surfaces gapped due to breaking the time-reversal symmetry, which enables a number of exotic phenomena having potential applications in spintronics. So far, MTIs have only been created by means of doping nonmagnetic TIs with 3d transition metal elements, however, such an approach leads to strongly inhomogeneous magnetic and electronic properties of these materials, restricting the observation of important effects to very low temperatures. Finding intrinsic MTI, i.e. a stoichiometric well-ordered magnetic compound, could be an ideal solution to these problems, but no such material was observed to date. Here, using density functional theory we predict and further confirm by means of structural, transport, magnetic, angle- and spin-resolved photoemission spectroscopy measurements the realization of the antiferromagnetic (AFM) TI phase, that is hosted by the van der Waals layered compound MnBi$_2$Te$_4$. An interlayer AFM ordering makes MnBi$_2$Te$_4$ invariant with respect to the combination of the time-reversal ($\Theta$) and primitive-lattice translation ($T_{1/2}$) symmetries, $S = \Theta T_{1/2}$, giving rise to the $Z_2$ topological classification of AFM insulators. We find $Z_2 = 1$ for MnBi$_2$Te$_4$, which confirms its topologically nontrivial nature. The $S$-breaking (0001) surface of MnBi$_2$Te$_4$ exhibits a giant bandgap in the topological surface state as evidenced by ab initio calculations and photoemission measurements. These results culminate almost a decade-long search of an AFMTI, predicted in 2010. Furthermore, MnBi$_2$Te$_4$ is the first intrinsic magnetic TI realized experimentally.
Forward citations
Cited by 4 Pith papers
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Berry Curvature Engineering by Gating Two-Dimensional Antiferromagnets
An out-of-plane electric field breaks PT symmetry in even-layer MnBi2Te4 and drives a topological phase transition to a Chern insulator with Chern number 3, enabling an electric-field-controlled anomalous Hall switch.
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Competing magnetic interactions in the antiferromagnetic topological insulator MnBi$_{2}$Te$_{4}$
Spin-wave measurements show that MnBi2Te4 has frustrated intralayer magnetic exchange close to the classical limit for ferromagnetism.
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Exchange Bias and Quantum Anomalous Hall Effect in the MnBi2Te4-CrI3 Heterostructure
DFT calculations predict that CrI3 proximity induces a 40 meV exchange bias in MnBi2Te4 films, enabling zero-field QAH states with Chern numbers 1 and 3.
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Flat Chern Band From Twisted Bilayer MnBi$_2$Te$_4$
A twisted bilayer of MnBi2Te4 is predicted to host an isolated flat Chern band at about one degree twist, offering a time-reversal-broken moire platform for correlated topological states.
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