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    Spontaneous continuous-symmetry breaking and tower of states in a comb chain

    Jingya Wang1,2,3, Zenan Liu2,3, Bin-Bin Mao4, Xu Tian2,3, Zijian Xiong5,*, Zhe Wang2,3,†, and Zheng Yan2,3

    • 1State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai 200438, China
    • 2Department of Physics, School of Science and Research Center for Industries of the Future, Westlake University, Hangzhou 310030, China
    • 3Institute of Natural Sciences, Westlake Institute for Advanced Study, Hangzhou 310024, China
    • 4School of Foundational Education, University of Health and Rehabilitation Sciences, Qingdao 266000, China
    • 5College of Physics and Electronic Engineering, Chongqing Normal University, Chongqing 401331, China

    • *Contact author: xiongzjsysu@hotmail.com
    • †Contact author: wangzhe90@westlake.edu.cn

    Phys. Rev. B 113, 174405 – Published 13 May, 2026

    DOI: https://doi.org/10.1103/mj51-1vgz

    Abstract

    Based on the study of a one-dimensional (1D) antiferromagnetic Heisenberg model on a comb lattice, in this work, we identify an example of spontaneous continuous symmetry breaking in a 1D system with short-range interactions. When a symmetry-preserving relevant perturbation is applied to the system, we find that this model can always be described by the Marshall-Lieb-Mattis (MLM) theorem. The Shen-Qiu-Tian theorem establishes a direct connection between the MLM theorem (in the case of bipartite lattices with unequal numbers of sites in the two sublattices) and the breaking of continuous symmetry. Moreover, although authors of previous studies have suggested that the presence of a tower of states (TOS) serves as an important numerical diagnostic of the tendency of a system toward spontaneous symmetry breaking, these investigations have primarily focused on two-dimensional systems. In 1D systems, however, the presence of long-range order does not automatically imply the emergence of a TOS. Here, we observe the existence of a TOS in a 1D realistic ferrimagnetic lattice system with short-range interactions.

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