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Magnetic structure of the topological semimetal YbMnSb2

Jian-Rui Soh1, Siobhan M. Tobin2, Hao Su3, Ivica Zivkovic1, Bachir Ouladdiaf4, Anne Stunault4, J. Alberto Rodríguez-Velamazán4, Ketty Beauvois4, Yanfeng Guo3 et al.

Andrew T. Boothroyd2

  • 1Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland
  • 2Department of Physics, University of Oxford, Clarendon Laboratory, Oxford OX1 3PU, United Kingdom
  • 3School of Physical Science and Technology, ShanghaiTech University, Shanghai 201210, China
  • 4Institut Laue-Langevin, 6 rue Jules Horowitz, BP 156, F-38042 Grenoble Cedex 9, France

Phys. Rev. B 104, L161103 – Published 5 October, 2021

DOI: https://doi.org/10.1103/PhysRevB.104.L161103

Abstract

The antiferromagnetic (AFM) semimetal YbMnSb2 has recently been identified as a candidate topological material, driven by time-reversal symmetry breaking. Depending on the ordered arrangement of Mn spins below the Néel temperature, TN=345K, the electronic bands near the Fermi energy can either have a Dirac node, a Weyl node, or a nodal line. We have investigated the ground state magnetic structure of YbMnSb2 using unpolarized and polarized single crystal neutron diffraction. We find that the Mn moments lie along the c axis of the P4/nmm space group and are arranged in a C-type AFM structure, which implies the existence of gapped Dirac nodes near the Fermi level. The results highlight how different magnetic structures can critically affect the topological nature of fermions in semimetals.

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