中国物理B ›› 2024, Vol. 33 ›› Issue (12): 127503-127503.doi: 10.1088/1674-1056/ad7af7

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Valley modulation and topological phase transition in staggered kagome ferromagnets

Yuheng Xing(邢玉恒), Wenjuan Qiu(邱文娟), Xinxing Wu(吴新星)†, and Yue Tan(谭悦)‡   

  1. Department of Physics, School of Mathematics and Physics, Yancheng Institute of Technology, Yancheng 224051, China
  • 收稿日期:2024-06-17 修回日期:2024-08-31 接受日期:2024-09-14 发布日期:2024-11-12
  • 通讯作者: Xinxing Wu, Yue Tan E-mail:wuxinxing@ycit.edu.cn;tanyue@ycit.edu.cn
  • 基金资助:
    We acknowledge support from the Funding for School-level Research Projects of Yancheng Institute of Technology (Grant Nos. xjr2020038, xjr2022039, and xjr2022040).

Valley modulation and topological phase transition in staggered kagome ferromagnets

Yuheng Xing(邢玉恒), Wenjuan Qiu(邱文娟), Xinxing Wu(吴新星)†, and Yue Tan(谭悦)‡   

  1. Department of Physics, School of Mathematics and Physics, Yancheng Institute of Technology, Yancheng 224051, China
  • Received:2024-06-17 Revised:2024-08-31 Accepted:2024-09-14 Published:2024-11-12
  • Contact: Xinxing Wu, Yue Tan E-mail:wuxinxing@ycit.edu.cn;tanyue@ycit.edu.cn
  • Supported by:
    We acknowledge support from the Funding for School-level Research Projects of Yancheng Institute of Technology (Grant Nos. xjr2020038, xjr2022039, and xjr2022040).

摘要: Owing to their charge-free property, magnons are highly promising for achieving dissipationless transport without Joule heating, and are thus potentially applicable to energy-efficient devices. Here, we investigate valley magnons and associated valley modulations in a kagome ferromagnetic lattice with staggered exchange interaction and Dzyaloshinskii-Moriya interaction. The staggered exchange interaction breaks the spatial inversion symmetry, leading to a valley magnon Hall effect. With nonzero Dzyaloshinskii-Moriya interaction in a staggered kagome lattice, the magnon Hall effect can be observed from only one valley. Moreover, reversing the Dzyaloshinskii-Moriya interaction ($D\to -D$) and exchanging $J_{1}$ and $J_{2}$ ($J_{1} \leftrightarrow J_{2}$) can also regulate the position of the unequal valleys. With increasing Dzyaloshinskii-Moriya interaction, a series of topological phase transitions appear when two bands come to touch and split at the valleys. The valley Hall effect and topological phase transitions observed in kagome magnon lattices can be realized in thin films of insulating ferromagnets such as Lu$_{2}$V$_{2}$O$_{7}$, and will extend the basis for magnonics applications in the future.

关键词: valley modulation, Dzyaloshinskii-Moriya interaction, staggered kagome ferromagnets, topological phase transitions, magnon Hall effect

Abstract: Owing to their charge-free property, magnons are highly promising for achieving dissipationless transport without Joule heating, and are thus potentially applicable to energy-efficient devices. Here, we investigate valley magnons and associated valley modulations in a kagome ferromagnetic lattice with staggered exchange interaction and Dzyaloshinskii-Moriya interaction. The staggered exchange interaction breaks the spatial inversion symmetry, leading to a valley magnon Hall effect. With nonzero Dzyaloshinskii-Moriya interaction in a staggered kagome lattice, the magnon Hall effect can be observed from only one valley. Moreover, reversing the Dzyaloshinskii-Moriya interaction ($D\to -D$) and exchanging $J_{1}$ and $J_{2}$ ($J_{1} \leftrightarrow J_{2}$) can also regulate the position of the unequal valleys. With increasing Dzyaloshinskii-Moriya interaction, a series of topological phase transitions appear when two bands come to touch and split at the valleys. The valley Hall effect and topological phase transitions observed in kagome magnon lattices can be realized in thin films of insulating ferromagnets such as Lu$_{2}$V$_{2}$O$_{7}$, and will extend the basis for magnonics applications in the future.

Key words: valley modulation, Dzyaloshinskii-Moriya interaction, staggered kagome ferromagnets, topological phase transitions, magnon Hall effect

中图分类号:  (Spin waves)

  • 75.30.Ds
75.47.-m (Magnetotransport phenomena; materials for magnetotransport) 75.70.Ak (Magnetic properties of monolayers and thin films) 85.75.-d (Magnetoelectronics; spintronics: devices exploiting spin polarized transport or integrated magnetic fields)