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具有耦合纹理的蜂窝晶格上的拓扑磁振子模式

Topological magnon modes on honeycomb lattice with coupling textures.

作者信息

Huang Hong, Kariyado Toshikaze, Hu Xiao

机构信息

International Center for Materials Nanoarchitectonics (WPI-MANA), National Institute for Materials Science, Tsukuba 305-0044, Japan.

Graduate School of Science and Technology, University of Tsukuba, Tsukuba 305-8571, Japan.

出版信息

Sci Rep. 2022 Apr 15;12(1):6257. doi: 10.1038/s41598-022-10189-w.

DOI:10.1038/s41598-022-10189-w
PMID:35428809
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9012859/
Abstract

Topological magnon modes are expected to be useful for novel applications such as robust information propagation, since they are immune to backscattering and robust against disorder. Although there are several theoretical proposals for topological magnon modes and growing experimental efforts for realizing them by now, it is still desirable to add complementary insights on this important phenomenon. Here, we propose a new scheme to achieve topological magnon where only nearest-neighbour exchange couplings on honeycomb lattice are necessary. In both ferromagnets and antiferromagnets, tuning exchange couplings between and inside hexagonal unit cells induces a topological state accompanied by a band inversion between p-orbital and d-orbital like magnon modes. Topological magnon modes appear at the interface between a topological domain and a trivial domain with magnon currents, which counterpropagate depending on pseudospins originated from orbital angular momenta of magnon modes. This mimics the spin-momentum locking phenomenon in the quantum spin Hall effect.

摘要

拓扑磁振子模式有望用于诸如稳健信息传播等新型应用,因为它们对背散射免疫且对无序具有鲁棒性。尽管目前已有若干关于拓扑磁振子模式的理论提议以及为实现它们而不断增加的实验努力,但仍希望能对这一重要现象增添补充性见解。在此,我们提出一种新方案来实现拓扑磁振子,其中仅需蜂窝晶格上的最近邻交换耦合。在铁磁体和反铁磁体中,调节六边形晶胞之间以及内部的交换耦合会诱导出一种拓扑态,伴随有类似磁振子模式的p轨道和d轨道之间的能带反转。拓扑磁振子模式出现在拓扑畴和平凡畴之间的界面处,并带有磁振子电流,这些电流根据源自磁振子模式轨道角动量的赝自旋反向传播。这模仿了量子自旋霍尔效应中的自旋 - 动量锁定现象。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dc86/9012859/3598ba2c7034/41598_2022_10189_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dc86/9012859/4a7eb90d986d/41598_2022_10189_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dc86/9012859/39e0cdb9a0d6/41598_2022_10189_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dc86/9012859/1d2d0241a809/41598_2022_10189_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dc86/9012859/325df172c4de/41598_2022_10189_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dc86/9012859/1ff251865f94/41598_2022_10189_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dc86/9012859/943f8d784cf0/41598_2022_10189_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dc86/9012859/5b5725422848/41598_2022_10189_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dc86/9012859/3598ba2c7034/41598_2022_10189_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dc86/9012859/4a7eb90d986d/41598_2022_10189_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dc86/9012859/39e0cdb9a0d6/41598_2022_10189_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dc86/9012859/1d2d0241a809/41598_2022_10189_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dc86/9012859/325df172c4de/41598_2022_10189_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dc86/9012859/1ff251865f94/41598_2022_10189_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dc86/9012859/943f8d784cf0/41598_2022_10189_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dc86/9012859/5b5725422848/41598_2022_10189_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dc86/9012859/3598ba2c7034/41598_2022_10189_Fig8_HTML.jpg

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