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Topological Hall effect in the antiferromagnetic Dirac semimetal EuAgAs

Antu Laha1,*, Ratnadwip Singha2,†, Sougata Mardanya1, Bahadur Singh3,‡, Amit Agarwal1, Prabhat Mandal2, and Z. Hossain1,§

  • 1Department of Physics, Indian Institute of Technology, Kanpur 208016, India
  • 2Saha Institute of Nuclear Physics, HBNI, 1/AF Bidhannagar, Calcutta 700 064, India
  • 3Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Mumbai 400005, India

  • *antuiitk2012@gmail.com
  • †Present address: Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA.
  • ‡bahadur.singh@tifr.res.in
  • §zakir@iitk.ac.in

Phys. Rev. B 103, L241112 – Published 21 June, 2021

DOI: https://doi.org/10.1103/PhysRevB.103.L241112

Abstract

The nontrivial magnetic texture in real space gives rise to the intriguing phenomenon of the topological Hall effect (THE), which is relatively less explored in topological semimetals. Here, we report a large THE in the antiferromagnetic (AFM) state in single crystals of EuAgAs, an AFM Dirac semimetal. EuAgAs hosts an AFM ground state below TN=12 K with a weak ferromagnetic component. The in-plane isothermal magnetization below TN exhibits a weak metamagnetic transition. We also observe chiral anomaly induced positive longitudinal magnetoconductivity, which indicates a Weyl fermion state under an applied magnetic field. The first-principles calculations reveal that EuAgAs is an AFM Dirac semimetal with a pair of Dirac cones, and therefore a Weyl semimetallic state can be realized under time-reversal symmetry breaking via an applied magnetic field. Our study establishes that EuAgAs is a system for exploiting the interplay of band topology and the topology of the magnetic texture.

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