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  • Letter

Long-range spin-orbital order in the spin-orbital SU(2)×SU(2)×U(1) model

Yang Liu, Z. Y. Xie, Hong-Gang Luo, and Jize Zhao
Phys. Rev. B 107, L041106 – Published 17 January 2023

Abstract

By using the tensor-network state algorithm, we study a spin-orbital model with SU(2)×SU(2)×U(1) symmetry on the triangular lattice. This model was proposed to describe some triangular d1 materials and was argued to host a spin-orbital liquid ground state. In our work the trial wave function of its ground state is approximated by an infinite projected entangled simplex state and optimized by the imaginary-time evolution. Contrary to the previous conjecture, we find that the two SU(2) symmetries are broken, resulting in a stripe spin-orbital order with the same magnitude m=0.085(10). This value is about half of that in the spin-1/2 triangular Heisenberg antiferromagnet. Our result demonstrates that although the long-sought spin-orbital liquid is absent in this model the spin-orbital order is significantly reduced due to the enhanced quantum fluctuation. This suggests that high-symmetry spin-orbital models are promising in searching for exotic states of matter in condensed-matter physics.

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  • Received 15 November 2022
  • Revised 4 January 2023
  • Accepted 6 January 2023

DOI:https://doi.org/10.1103/PhysRevB.107.L041106

©2023 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Yang Liu1,2, Z. Y. Xie3,*, Hong-Gang Luo1,2,4, and Jize Zhao1,2,†

  • 1School of Physical Science and Technology & Key Laboratory for Magnetism and Magnetic Materials of the MoE, Lanzhou University, Lanzhou 730000, China
  • 2Lanzhou Center for Theoretical Physics and Key Laboratory of Theoretical Physics of Gansu Province, Lanzhou University, Lanzhou 730000, China
  • 3Department of Physics, Renmin University of China, Beijing 100872, China
  • 4Beijing Computational Science Research Center, Beijing 100084, China

  • *qingtaoxie@ruc.edu.cn
  • zhaojz@lzu.edu.cn

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Issue

Vol. 107, Iss. 4 — 15 January 2023

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Images

  • Figure 1
    Figure 1

    Schematic diagram of the triangular lattice and the PESS wave function ansatz. The black filled circles () represent the lattice sites. The blue solid and dashed lines connecting two nearest-neighbor lattice sites are the bonds of the lattice, indicating two different interaction terms corresponding to Eqs. (1) and (2), respectively. The red open circles () sitting at the center of upward triangles represent the rank-3 simplex tensors S in the PESS wave function, and at each lattice site there is a projection tensor A. The physical indices σ and σ perpendicular to the plane are not shown here. The four rhombuses in green mark the 2×2, 4×2, 3×3, and 4×4 periodic clusters used in the trial wave functions.

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  • Figure 2
    Figure 2

    The energy per bond E obtained from the wave function ansatz with different clusters are shown as a function of 1/D.

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  • Figure 3
    Figure 3

    The magnitude of the spin-orbit order obtained with D ranging from 4 to 18. Various polynomial functions are used to fit the curve. The dashed line denotes a linear fitting. It is estimated that mX/Y=0.085(10) in the large-D limit.

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  • Figure 4
    Figure 4

    Degenerate stripe spin-orbital configurations for the ground state. The data are obtained with D=18 and χ=D2.

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  • Figure 5
    Figure 5

    mX is shown as a function of 1/χ for D=11,12,14, and 18.

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