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    Fermi surface reconstruction due to orthorhombic distortion in the Dirac semimetal YbMnSb2

    Dilip Bhoi1,*, Feng Ye2, Hanming Ma1, Xiaoling Shen1, Arvind Maurya3, Shusuke Kasamatsu4, Takahiro Misawa1, Kazuyoshi Yoshimi1, Taro Nakajima1 et al.

    Masaki Kondo1, Yuto Kinoshita1, Masashi Tokunaga1, Masaaki Matsuda2, and Yoshiya Uwatoko1

    • 1The Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan
    • 2Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
    • 3Department of Physics, School of Physical Sciences, Mizoram University, Aizawl 796 004, India
    • 4Academic Assembly (Faculty of Science), Yamagata University, Yamagata 990-8560, Japan

    • *Present address: Department of Engineering Science, University of Electro-Communications, Chofu, Tokyo 182-8585, Japan.

    Phys. Rev. B 111, 214115 – Published 20 June, 2025

    DOI: https://doi.org/10.1103/lk8w-7hkj

    Abstract

    A Dirac semimetal with magnetic atoms as constituents delivers an interesting platform to investigate the interplay of Fermi surface (FS) topology, electron correlation, and magnetism. One such family of semimetals is YbMnPn2 (Pn=Sb,Bi), which is being actively studied due to the intertwined spin and charge degrees of freedom. Here, we investigate the relationship between the magnetic/crystal structures and FS topology of YbMnSb2 using single crystal x-ray diffraction, neutron scattering, magnetic susceptibility, magnetotransport measurements, and complimentary density functional theory (DFT) calculations. Contrary to previous reports, the x-ray and neutron diffraction reveal that YbMnSb2 crystallizes in an orthorhombic Pnma structure with a notable antiphase displacement of the magnetic Mn ions that increases in magnitude upon cooling. As a result of this orthorhombicity, first-principles DFT calculation reveals a reduced Brillouin zone and more anisotropic FS of YbMnSb2 compared to YbMnBi2. Moreover, the hole-type carrier density drops by two orders of magnitude as YbMnSb2 orders antiferromagnetically, indicating band folding in a magnetic ordered state. In addition, the Landau level fan diagram yields a nontrivial nature of the Shubnikov–de Haas quantum oscillation frequency arising from the Dirac-like Fermi pocket. These results imply that YbMnSb2 is an ideal platform to explore the interplay of subtle lattice distortion, magnetic order, and topological transport arising from relativistic quasiparticles.

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