High-pressure effects on structural, magnetic, and vibrational properties of van der Waals antiferromagnet MnPS3

D. P. Kozlenko, O. N. Lis, N. T. Dang, M. Coak, J.-G. Park, E. V. Lukin, S. E. Kichanov, N. O. Golosova, I. Yu. Zel, and B. N. Savenko
Phys. Rev. Materials 8, 024402 – Published 6 February 2024

Abstract

The crystal structure, vibrational spectra, and magnetic structure of quasi-two-dimensional layered van der Waals material MnPS3 were studied using x-ray diffraction and Raman spectroscopy at high pressures up to 28 GPa, and neutron diffraction up to 3.6 GPa, respectively. A structural phase transition between two monoclinic modifications of the same C2/m symmetry was observed, evolving gradually in the pressure range of about 1–6 GPa. The transition is accompanied by abrupt shortening of lattice parameters, significant reduction of the monoclinic distortion, and anomalies in the pressure behavior of several Raman-mode frequencies. No more structural phase transitions were revealed in the studied pressure range. The antiferromagnetic (AFM) state with a propagation vector k = (0, 0, 0) remains stable in ambient pressure and high-pressure structural phases of MnPS3 at least up to 3.6 GPa. The Néel temperature increases noticeably with a pressure coefficient of dTN/dP=6.7 K/GPa, leading to modification of the dominant first-neighbor magnetic interaction exchange parameter with a relevant coefficient dJ1/dP0.6 meV/GPa. This observation is in contrast to the pressure behavior of FePS3, demonstrating modification of the AFM state from 2D-like to 3D-like at the similar pressure-induced structural phase transition. The different pressure response of the magnetic states of MnPS3 and FePS3 is analyzed in terms of competing in-plane and interplane magnetic interactions.

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  • Received 17 November 2023
  • Accepted 9 January 2024

DOI:https://doi.org/10.1103/PhysRevMaterials.8.024402

©2024 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

D. P. Kozlenko1,*, O. N. Lis1,2, N. T. Dang3,4, M. Coak5,6,7, J.-G. Park6,7,8, E. V. Lukin1, S. E. Kichanov1, N. O. Golosova1, I. Yu. Zel1, and B. N. Savenko1

  • 1Frank Laboratory of Neutron Physics, JINR, 141980 Dubna, Moscow Region, Russian Federation
  • 2Kazan Federal University, 420008, Kazan, Russian Federation
  • 3Institute of Research and Development, Duy Tan University, 550000 Danang, Vietnam
  • 4Faculty of Environmental and Natural Sciences, Duy Tan University, 550000 Danang, Vietnam
  • 5School of Physics and Astronomy, University of Birmingham, Edgbaston, Birmingham B15 2TT, United Kingdom
  • 6Center for Correlated Electron Systems, Institute for Basic Science, Seoul 08826, Republic of Korea
  • 7Department of Physics and Astronomy, Seoul National University, Seoul 08826, Republic of Korea
  • 8Center for Quantum Materials, Seoul National University, Seoul 08826, Republic of Korea

  • *denk@nf.jinr.ru

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Vol. 8, Iss. 2 — February 2024

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