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    Switchable valley-contrasting Berry curvature in two-dimensional valley-semi-half-metals

    Mu Tian1,2,3, Chaoxi Cui1,2,3, ZhenHua Li4, Zhi-Ming Yu1,2,3, and Run-Wu Zhang1,2,3,*

    • 1Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing Institute of Technology, Beijing 100081, China
    • 2Beijing Key Lab of Nanophotonics & Ultrafine Optoelectronic Systems, School of Physics, Beijing Institute of Technology, Beijing 100081, China
    • 3Beijing Institute of Technology, Zhuhai 519000, China
    • 4Lanzhou Center for Theoretical Physics, Key Laboratory of Quantum Theory and Applications of MOE, and Key Laboratory of Theoretical Physics of Gansu Province, Lanzhou University, Lanzhou 730000, China

    • *Contact author: zhangrunwu@bit.edu.cn

    Phys. Rev. B 112, 045144 – Published 24 July, 2025

    DOI: https://doi.org/10.1103/7wxx-nm37

    Abstract

    Generating and controlling valley-contrasting Berry curvature in two-dimensional (2D) hexagonal magnetic materials holds significant promise for advancements in spintronics and valleytronics. Here, we explore the interplay between valley index, magnetic ordering, and band topology in a single 2D semi-half-metallic system, introducing a critical state termed valley-semi-half-metal, which is crucial for realizing high Chern number quantum anomalous Hall (QAH) insulators. We identify the fluorinated 1T−CrS2 monolayer (1T−CrS2F2) as a promising material, exhibiting soft ferromagnetic characteristics ideal for achieving this 2D valley-semi-half-metallic state. Remarkably, the monolayer 1T−CrS2F2 can transition from a semi-half-metallic state to a high Chern number QAH insulator with opposite-chiral edge states through magnetization reversal. Additionally, the Janus 1T−CrS2FCl monolayer, which lacks inversion symmetry, enables gate-tunable, valley-contrasting QAH insulator phases with opposite Chern numbers upon reversing the magnetization. Our findings highlight a promising magnetic candidate for exploring valley and topological physics, offering an alternative approach for designing switchable QAH effects and paving the way for innovative topological quantum devices.

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