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Composition dependence of bulk properties in the Co-intercalated transition metal dichalcogenide Co1/3TaS2

Pyeongjae Park1,2,3,*, Woonghee Cho1,2, Chaebin Kim1,2, Yeochan An1,2, Maxim Avdeev4,5, Kazuki Iida6, Ryoichi Kajimoto7, and Je-Geun Park1,2,8,†

  • 1Center for Quantum Materials, Seoul National University, Seoul 08826, Republic of Korea
  • 2Department of Physics and Astronomy, Seoul National University, Seoul 08826, Republic of Korea
  • 3Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 4Australian Nuclear Science and Technology Organization, Locked Bag 2001, Kirrawee DC, New South Wales 2232, Australia
  • 5School of Chemistry, The University of Sydney, Sydney, New South Wales 2006, Australia
  • 6Comprehensive Research Organization for Science and Society (CROSS), Tokai, Ibaraki 319-1106, Japan
  • 7Materials and Life Science Division, J-PARC Center, Tokai, Ibaraki 319-1195, Japan
  • 8Institute of Applied Physics, Seoul National University, Seoul 08826, Republic of Korea

  • *Corresponding author: parkp@ornl.gov
  • †Corresponding author: jgpark10@snu.ac.kr

Phys. Rev. B 109, L060403 – Published 6 February, 2024

DOI: https://doi.org/10.1103/PhysRevB.109.L060403

Abstract

Spontaneous Hall conductivity has recently been reported in the triangular lattice antiferromagnet Co1/3TaS2 under a zero magnetic field. This phenomenon originates from the distinctive noncoplanar triple-Q magnetic ground state, possessing uniform real-space Berry curvature characterized by scalar spin chirality. We investigated the physical properties of Co1/3TaS2 by judiciously controlling the composition, revealing a drastic change in its bulk properties, even by slight variations in cobalt composition, despite the same crystal structure. For 0.299≤x≤0.325, CoxTaS2 keeps all the characteristics of the ground state consistent with the previous studies—two antiferromagnetic phase transitions at TN1 and TN2 (<TN1), a large spontaneous Hall conductivity [σxy(H=0)], and a weak ferromagnetic moment along the c axis. However, samples with x≥0.330 exhibit distinct bulk properties, including the absence of both σxy(H=0) and the weak ferromagnetic moment. Our neutron diffraction data reveal that CoxTaS2 with x≥0.330 develops coplanar helical magnetic order with qm1=(1/3, 0, 0). This is entirely different from what has been seen in x≤0.325, explaining the observed composition dependence.

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