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arXiv 2001.10579cond-mat.mtrl-sci
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Observation of high-temperature quantum anomalous Hall regime in intrinsic MnBi$_2$Te$_4$/Bi$_2$Te$_3$ superlattice

Haiming Deng, Zhiyi Chen, Agnieszka Wolos, Marcin Konczykowski, Kamil Sobczak, Joanna Sitnicka, Irina V. Fedorchenko, Jolanta Borysiuk, Tristan Heider, Lukasz P… 展开作者

Haiming Deng, Zhiyi Chen, Agnieszka Wolos, Marcin Konczykowski, Kamil Sobczak, Joanna Sitnicka, Irina V. Fedorchenko, Jolanta Borysiuk, Tristan Heider, Lukasz Plucinski, Kyungwha Park, Alexandru B. Georgescu, Jennifer Cano, Lia Krusin-Elbaum

英文摘要:

The quantum anomalous Hall effect is a fundamental transport response of a topologically non-trivial system in zero magnetic field. Its physical origin relies on the intrinsically inverted electronic band structure and ferromagnetism, and its most consequential manifestation is the dissipation-free flow of chiral charge currents at the edges that can potentially transform future quantum electronics. Here we report a previously unknown Berry-curvature-driven anomalous Hall regime ('Q-window') at above-Kelvin temperatures in the magnetic topological bulk crystals where through growth Mn ions self-organize into a period-ordered MnBi$_2$Te$_4$/Bi$_2$Te$_3$ superlattice. Robust ferromagnetism of the MnBi$_2$Te$_4$ monolayers opens a large surface gap, and anomalous Hall conductance reaches an $e^2/h$ quantization plateau when the Fermi level is tuned into this gap within a Q-window in which the anomalous Hall conductance from the bulk is to a high precision zero. The quantization in this new regime is not obstructed by the bulk conduction channels and thus should be present in a broad family of topological magnets.

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