Pressure-induced large increase of Curie temperature of the van der Waals ferromagnet VI3

J. Valenta, M. Kratochvílová, M. Míšek, K. Carva, J. Kaštil, P. Doležal, P. Opletal, P. Čermák, P. Proschek, K. Uhlířová, J. Prchal, M. J. Coak, S. Son, J-G. Park, and V. Sechovský
Phys. Rev. B 103, 054424 – Published 17 February 2021

Abstract

Evolution of magnetism in single crystals of the van der Waals compound VI3 in external pressure up to 7.3 GPa studied by measuring magnetization and ac magnetic susceptibility is reported. Four magnetic phase transitions, at T1=54.5K, T2=53K, TC=49.5K, and TFM=26K, respectively, have been observed at ambient pressure. The first two have been attributed to the onset of ferromagnetism in specific crystal-surface layers. The bulk ferromagnetism is characterized by the magnetic ordering transition at Curie temperature TC and the transition between two different ferromagnetic phases TFM, accompanied by a structure transition from monoclinic to triclinic symmetry upon cooling. The pressure effects on magnetic parameters were studied with three independent techniques. TC was found to be almost unaffected by pressures up to 0.6 GPa whereas TFM increases rapidly with increasing pressure and reaches TC at a triple point at ≈ 0.85 GPa. At higher pressures, only one magnetic phase transition is observed moving to higher temperatures with increasing pressure to reach 99 K at 7.3 GPa. In contrast, the low-temperature bulk magnetization is significantly reduced by applying pressure (by more than 50% at 2.5 GPa) suggesting a possible pressure-induced reduction of vanadium magnetic moment. First-principles calculations of VI3 under pressure allow us to ascribe the evolution of TC with pressure to the reduction of interplanar distance, including the observed slope change at 0.6 GPa. These calculations also describe the associated band gap closing, showing that with a modest compression the material would become metallic. Overall, the large pressure range covered corresponds to a significant change of interplanar interactions. The obtained data thus allow us to shed light on how does the transition between the three-dimensional (3D) and quasi-2D system affect magnetic interactions in the system.

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  • Received 20 October 2020
  • Revised 15 December 2020
  • Accepted 15 January 2021

DOI:https://doi.org/10.1103/PhysRevB.103.054424

©2021 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

J. Valenta1,2, M. Kratochvílová1, M. Míšek3, K. Carva1, J. Kaštil3, P. Doležal1, P. Opletal1, P. Čermák1, P. Proschek1, K. Uhlířová1, J. Prchal1, M. J. Coak4,5, S. Son6,7,8, J-G. Park6,7,8, and V. Sechovský1

  • 1Charles University, Faculty of Mathematics and Physics, Department of Condensed Matter Physics, Ke Karlovu 5, 121 16 Prague 2, Czech Republic
  • 2National Institute for Materials Science, Thermal Energy Materials Group, International Center for Materials Nanoarchitectonics (MANA), 1-2-1, Sengen, Tsukuba, Ibaraki 305-0047, Japan
  • 3Institute of Physics, Czech Academy of Sciences, Na Slovance 2, 182 21 Prague 8, Czech Republic
  • 4Department of Physics, University of Warwick, Gibbet Hill Road, Coventry CV4 7AL, United Kingdom
  • 5Cavendish Laboratory, University of Cambridge, J.J. Thomson Ave, Cambridge CB3 0HE, United Kingdom
  • 6Center for Quantum Materials, Seoul National University, Seoul 08826, Republic of Korea
  • 7Center for Correlated Electron Systems, Institute for Basic Science, Seoul 08826, Korea
  • 8Department of Physics and Astronomy, Seoul National University, Seoul 08826, Korea

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Issue

Vol. 103, Iss. 5 — 1 February 2021

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