| Autor: |
Otrokov, Mikhail M., Klimovskikh, Ilya I., Bentmann, Hendrik, Zeugner, Alexander, Aliev, Ziya S., Gass, Sebastian, Wolter, Anja U. B., Koroleva, Alexandra V., Estyunin, Dmitry, Shikin, Alexander M., Blanco-Rey, María, Hoffmann, Martin, Vyazovskaya, Alexandra Yu., Eremeev, Sergey V., Koroteev, Yury M., Amiraslanov, Imamaddin R., Babanly, Mahammad B., Mamedov, Nazim T., Abdullayev, Nadir A., Zverev, Vladimir N., Büchner, Bernd, Schwier, Eike F., Kumar, Shiv, Kimura, Akio, Petaccia, Luca, Di Santo, Giovanni, Vidal, Raphael C., Schatz, Sonja, Kißner, Katharina, Min, Chul-Hee, Moser, Simon K., Peixoto, Thiago R. F., Reinert, Friedrich, Ernst, Arthur, Echenique, Pedro M., Isaeva, Anna, Chulkov, Evgueni V. |
| Rok vydání: |
2018 |
| Předmět: |
|
| Zdroj: |
Nature 576, 416-422 (2019) |
| Druh dokumentu: |
Working Paper |
| DOI: |
10.1038/s41586-019-1840-9 |
| Popis: |
Despite immense advances in the field of topological materials, the antiferromagnetic topological insulator (AFMTI) state, predicted in 2010, has been resisting experimental observation up to now. Here, using density functional theory and Monte Carlo method we predict and by means of structural, transport, magnetic, and angle-resolved photoemission spectroscopy measurements confirm for the first time realization of the AFMTI 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, $S=\Theta T_{1/2}$, which gives rise to the $Z_2$ topological classification of AFM insulators, $Z_2$ being equal to 1 for this material. The $S$-breaking (0001) surface of MnBi$_2$Te$_4$ features a giant bandgap in the topological surface state thus representing an ideal platform for the observation of such long-sought phenomena as the quantized magnetoelectric coupling and intrinsic axion insulator state. |
| Databáze: |
arXiv |
| Externí odkaz: |
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