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    Magnetic-field and strain engineering of transverse transport in altermagnetic topological materials

    Xiuxian Yang1, Xiaodong Zhou2,*, Jingming Shi1, Shifeng Qian3,†, Xiaotian Wang4,‡, Wenhong Wang5, and Yinwei Li1,§

    • 1Jiangsu Key Laboratory of Extreme Multi-Field Materials Physics, School of Physics and Electronic Engineering, Jiangsu Normal University, Xuzhou 221116, China
    • 2School of Physical Science and Technology, Tiangong University, Tianjin 300387, China
    • 3Anhui Province Key Laboratory for Control and Applications of Optoelectronic Information Materials, Department of Physics, Anhui Normal University, Anhui, Wuhu 241000, China
    • 4Institute for Superconducting and Electronic Materials, Faculty of Engineering and Information Sciences, University of Wollongong, Wollongong 2500, Australia
    • 5School of Electronic and Information Engineering, Tiangong University, Tianjin 300387, China

    • *Contact author: zhouxiaodong@tiangong.edu.cn
    • †Contact author: qiansf@ahnu.edu.cn
    • ‡Contact author: xiaotianw@uow.edu.au
    • §Contact author: yinwei_li@jsnu.edu.cn

    Phys. Rev. B 112, 214418 – Published 9 December, 2025

    DOI: https://doi.org/10.1103/1ffx-lv6y

    Abstract

    Here, we explore the role of inherent altermagnetic topology in transverse transport phenomena (such as crystal or anomalous Hall, Nernst, and thermal Hall effects) in several famous altermagnets, including tetragonal XV2Y2O (X=K,Rb,Cs; Y=S,Se,Te), RuO2, MnF2, as well as hexagonal CrSb and MnTe. Notably, in XV2Y2O, the first experimentally realized layered altermagnets, transverse transport is governed by altermagnetic pseudonodal surfaces, emphasizing the purely topological contributions to transverse transport. Interestingly, we demonstrate that strain engineering and magnetic field, two unique methods for selectively controlling crystal and anomalous transport, can substantially enhance the magnitude of these phenomena while preserving the alternating spin characteristics in both real and momentum space. Moreover, due to the spin symmetry breaking via shear strain, a new magnetic phase, fully compensated ferrimagnetism, with isotropic spin splitting, can be induced. Our findings provide effective strategies not only for manipulating transverse transport in altermagnets but also for controlling magnetic phase transitions, offering valuable insights for their potential applications in spintronics and spin caloritronics.

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