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Orbital and magnetic ordering in the weak ferromagnet vanadium trifluoride VF3

Reinhard K. Kremer1,*, Florian Kraus2,†, Patrick Woidy2, Gwilherm Nénert3,‡,§, Christina Drahten4,∥,¶, and Bachir Ouladdiaf3,**

  • *Contact author: R.Kremer@fkf.mpg.de
  • †Contact author: f.kraus@uni-marburg.de
  • ‡Contact author: gwilherm.nenert@malvernpanalytical.com
  • §Present address: Malvern Panalytical B.V. Lelyweg 1, 7602 EA Almelo, The Netherlands.
  • ∥Contact author: christina.drahten@thermofisher.com
  • Present address: Thermo Fisher Scientific GmbH, Im Steingrund 4, 63303 Dreieich, Germany.
  • **Contact author: ouladdia@ill.fr

Phys. Rev. B 113, 054442 – Published 25 February, 2026

DOI: https://doi.org/10.1103/3gzm-yxfb

Abstract

We report on an investigation of the low-temperature structural, thermal, and magnetic properties of the binary trifluoride VF3 by temperature-dependent magnetization, heat capacity, electron paramagnetic resonance, and synchrotron powder and neutron powder diffraction measurements. At room temperature the crystal structure of VF3 features V3+ spin S = 1 regular triangular layers. At ∼120K VF3 undergoes a structural phase transition, and at ∼18K it undergoes an antiferromagnetic phase transition. The structural phase transition involves a minute orthorhombic distortion of the regular octahedral fluorine coordination shell of the trivalent V cations, effecting a distortion to the monoclinic crystal system. The magnetic phase transition generates a weak ferromagnet with V magnetic moments essentially confined to the trigonal planes of the room temperature structure described in the space group R−3c. The ordered magnetic moments of the V3+ cations amount to ≈1μB and is thus distinctly reduced from the spin-only magnetic moment of 2μB. This finding and the weak ferromagnetic moment are discussed in view of the low-symmetry structure and spin-orbit effects on the 3T1 cubic ground term of the V3+ d2 system.

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References (31)

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