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    Ground state phase diagram and Haldane-like symmetry-protected phase in the S=12 Heisenberg model on the two-dimensional square-hexagon-octagon lattice

    Yumeng Luo, Yuehong Li, Mengfan Jiang, Muwei Wu, Jian-Jian Yang, Dao-Xin Yao*, and Han-Qing Wu†

    • Center for Neutron Science and Technology, Guangdong Provincial Key Laboratory of Magnetoelectric Physics and Devices, State Key Laboratory of Optoelectronic Materials and Technologies, School of Physics, Sun Yat-sen University, Guangzhou 510275, China

    • *Contact author: yaodaox@mail.sysu.edu.cn
    • †Contact author: wuhanq3@mail.sysu.edu.cn

    Phys. Rev. B 113, 045103 – Published 2 January, 2026

    DOI: https://doi.org/10.1103/ycsq-w3fr

    Abstract

    Using stochastic series expansion quantum Monte Carlo and density matrix renormalization group methods, we investigate the ground-state phase diagram of the S=1/2 Heisenberg model on the two-dimensional square-hexagon-octagon (SHO) lattice. The model incorporates nearest-neighbor interactions J1 (intrahexagon interaction) and J2 (interhexagon), as well as a selected third-neighbor interaction J3 along the x direction. We identify five distinct phases in the parameter regime 0<λ1=J2/J1<4,0<λ2=J3/J1<4: a Néel antiferromagentic phase, two dimer phases (orthogonal and ladder staggered dimers), a hexagon singlet phase, and notably a Haldane-like symmetry-protected topological (SPT) phase. The topological nature of the Haldane-like phase is confirmed by the degeneracy of the ground-state energy under open boundary conditions and the twofold degeneracy of the entanglement spectrum. Phase boundaries are accurately determined using finite-size scaling of the spin stiffness and Binder cumulant. Data collapse analysis reveals that all transitions from nonmagnetic phases to the antiferromagnetic phase belong to the three-dimensional O(3) Heisenberg universality class. In addition, we investigate the robustness of the SPT phase to other interactions, such as those that could arise in experimental materials. Our work establishes a comprehensive theoretical framework for understanding magnetic and topological phases on the SHO lattice.

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