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Anticollinear order and degeneracy lifting in square lattice antiferromagnet LaSrCrO4

Jing Zhou1,2, Guy Quirion3, Jeffrey A. Quilliam4, Huibo Cao5, Feng Ye5, Matthew B. Stone5, Qing Huang6, Haidong Zhou6, Jinguang Cheng1 et al.

Xiaojian Bai7,*, Martin Mourigal7, Yuan Wan1,2,8,†, and Zhiling Dun1,7,‡

  • 1Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
  • 2University of the Chinese Academy of Sciences, Beijing 100049, China
  • 3Department of Physics and Physical Oceanography, Memorial University of Newfoundland, St. John's, Canada A1B 3X7
  • 4Institute Quantique, Départment de Physique, and RQMP, Université de Sherbrooke, Sherbrooke, Québec, Canada J1K 2R1
  • 5Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 6Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA
  • 7School of Physics, Georgia Institute of Technology, Atlanta, Georgia 30332, USA
  • 8Songshan Lake Materials Laboratory, Dongguan, Guangdong 523808, China

  • *Present address: Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, TN 37831, USA.
  • †yuan.wan@iphy.ac.cn
  • ‡dun@iphy.ac.cn

Phys. Rev. B 105, L180411 – Published 23 May, 2022

DOI: https://doi.org/10.1103/PhysRevB.105.L180411

Abstract

We report the static and dynamic magnetic properties of LaSrCrO4, a seemingly canonical spin-3/2 square-lattice antiferromagnet that exhibits frustration between magnetic layers—owing to their AB stacking—and offers a rare testbed to investigate accidental-degeneracy lifting in magnetism. Neutron diffraction experiments on single-crystal samples uncover a remarkable anticollinear magnetic order below TN = 170 K characterized by a Néel arrangement of the spins within each layer and an orthogonal arrangement between adjacent layers. To understand the origin of this unusual magnetic structure, we analyze the spin-wave excitation spectrum by means of inelastic neutron scattering and bulk measurements. A spectral gap of 0.5 meV, along with a spin-flop transition at 3.2 T, reflect the energy scale associated with the degeneracy-lifting. A minimal model to explain these observations requires both a positive biquadratic interlayer exchange and dipolar interactions, both of which are on the order of 10−4 meV, only a few parts per million of the dominant exchange interaction J1≈11 meV. These results provide direct evidence for the selection of a noncollinear magnetic structure by the combined effect of two distinct degeneracy lifting interactions.

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