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双层共线反铁磁体中的磁振子弗洛凯量子自旋霍尔绝缘体

Magnonic Floquet Quantum Spin Hall Insulator in Bilayer Collinear Antiferromagnets.

作者信息

Owerre S A

机构信息

Perimeter Institute for Theoretical Physics, 31 Caroline St. N., Waterloo, Ontario, N2L 2Y5, Canada.

出版信息

Sci Rep. 2019 May 10;9(1):7197. doi: 10.1038/s41598-019-43702-9.

Abstract

We study irradiated two-dimensional insulating bilayer honeycomb ferromagnets and antiferromagnets coupled antiferromagnetically with a zero net magnetization. The former is realized in the recently synthesized bilayer honeycomb chromium triiodide CrI. In both systems, we show that circularly-polarized electric field breaks time-reversal symmetry and induces a dynamical Dzyaloshinskii-Moriya interaction in each honeycomb layer. However, the resulting bilayer antiferromagnetic system still preserves a combination of time-reversal and space-inversion ([Formula: see text]) symmetry. We show that the magnon topology of the bilayer antiferromagnetic system is characterized by a [Formula: see text] Floquet topological invariant. Therefore, the system realizes a magnonic Floquet quantum spin Hall insulator with spin filtered magnon edge states. This leads to a non-vanishing Floquet magnon spin Nernst effect, whereas the Floquet magnon thermal Hall effect vanishes due to [Formula: see text] symmetry. We study the rich [Formula: see text] Floquet topological magnon phase diagram of the system as a function of the light amplitudes and polarizations. We further discuss the great impact of the results on future experimental realizations.

摘要

我们研究了具有零净磁化强度且反铁磁耦合的二维绝缘双层蜂窝铁磁体和反铁磁体。前者在最近合成的双层蜂窝状三碘化铬(CrI)中得以实现。在这两个系统中,我们表明圆偏振电场打破了时间反演对称性,并在每个蜂窝层中诱导出动态的Dzyaloshinskii - Moriya相互作用。然而,由此产生的双层反铁磁系统仍然保留了时间反演和空间反演([公式:见原文])对称性的组合。我们表明,双层反铁磁系统的磁振子拓扑结构由一个[公式:见原文]弗洛凯拓扑不变量来表征。因此,该系统实现了具有自旋过滤磁振子边缘态的磁振子弗洛凯量子自旋霍尔绝缘体。这导致了非零的弗洛凯磁振子自旋能斯特效应,而弗洛凯磁振子热霍尔效应由于[公式:见原文]对称性而消失。我们研究了该系统丰富的[公式:见原文]弗洛凯拓扑磁振子相图作为光振幅和偏振的函数。我们进一步讨论了这些结果对未来实验实现的重大影响。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/41d0/6510812/fdc18171d705/41598_2019_43702_Fig1_HTML.jpg

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