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Competing magnetic interactions in a spin-12 square lattice: Hidden order in Sr2VO4

Bongjae Kim, Sergii Khmelevskyi, Peter Mohn, and Cesare Franchini
Phys. Rev. B 96, 180405(R) – Published 8 November 2017
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Abstract

With decreasing temperature, Sr2VO4 undergoes two structural phase transitions, tetragonal-to-orthorhombic-to-tetragonal, without long-range magnetic order. Recent experiments suggest that only at very low temperature, Sr2VO4 might enter a yet-unknown phase with long-range magnetic order, but without orthorhombic distortion. By combining relativistic density functional theory with an extended spin-1/2 compass-Heisenberg model, we find an antiferromagnetic single-stripe ground state with highly competing exchange interactions, involving a non-negligible interlayer coupling, which places the system at the crossover between the XY-model and Heisenberg-model regimes. Most strikingly, we find a strong two-site “spin-compass” exchange anisotropy which is relieved by the orthorhombic distortion induced by the spin stripe order. Based on these results, we discuss the origin of the hidden-order phase and the possible formation of a spin liquid at low temperatures.

  • Figure
  • Figure
  • Received 23 August 2017

DOI:https://doi.org/10.1103/PhysRevB.96.180405

©2017 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Bongjae Kim1, Sergii Khmelevskyi1,2, Peter Mohn2, and Cesare Franchini1

  • 1University of Vienna, Faculty of Physics and Center for Computational Materials Science, Vienna A-1090, Austria
  • 2Center for Computational Materials Science, Institute for Applied Physics, Vienna University of Technology, Wiedner Hauptstrasse 8 - 10, 1040 Vienna, Austria

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Issue

Vol. 96, Iss. 18 — 1 November 2017

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Images

  • Figure 1
    Figure 1

    (a) Sketch of the different magnetic orderings used to fit the Heisenberg spin Hamiltonian. Single stripe (ST), double stripe along [100] and [110] (DS10 and DS11), ferromagnetic (FM), staggered dimer (SD), Néel, and Parquet order. (b) Total energy as a function of U within DFT+U calculations. Inset: schematic description of the exchange interactions.

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  • Figure 2
    Figure 2

    (a) Schematic diagram showing the transition temperatures and structures. The system has a tetragonal structure with active anisotropic exchange interactions for T>Tc2, while for the orthorhombic structure for Tc2>T>Tc1, the anisotropy vanishes. Tetragonal symmetry is recovered below Tc1. Stripe order is shown with moments along (b) (100) and (c) (010), respectively. The squares denotes the unit cell used.

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