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    Scale-invariant-like states and conformal-invariant states in the vicinity of the ferromagnetic SU(3) point in the spin-1 bilinear-biquadratic model

    Qian-Qian Shi1,*, Murray T. Batchelor1,2,†, and Huan-Qiang Zhou1,‡

    • *Contact author: shiqianqian@cqu.edu.cn
    • †Contact author: murray.batchelor@anu.edu.au
    • ‡Contact author: hqzhou@cqu.edu.cn

    Phys. Rev. B 114, 134409 – Published 8 September, 2026

    DOI: https://doi.org/10.1103/1464-5mdp

    Abstract

    Using exact diagonalization and variational tensor network methods, we study ground states near the ferromagnetic SU(3) point at θ=5π/4 in the spin-1 bilinear-biquadratic model from a finite-size approach. In particular, two types of scale-invariant states, scale-invariant states with type-B Goldstone modes and conformal-invariant states, are involved. Universal finite-size entanglement entropy scaling for the two distinct types of scale-invariant states, which exhibit boundary dependence in conformal-invariant states and boundary independence arising from emergent lattice-permutation symmetry in scale-invariant states with type-B Goldstone modes, enable a clarification of the physics in the vicinity of the ferromagnetic SU(3) point. According to the results from exact diagonalization with system size up to L=16, entanglement entropy in the vicinity of the point θ=5π/4 presents a universal finite-size scaling for scale-invariant states with two type-B Goldstone modes to high precision, independent of the boundary conditions, as a result of an emergent lattice-permutation symmetry in the scale-invariant states. Meanwhile, from both an exact diagonalization method and a variational tensor network method, a unique “conformal-invariant point” is identified near θ=5π/4 with central charge c=2 under both periodic and open boundary conditions, moving toward the point θ=5π/4 as L increases, suggesting a direct ferromagnetic-to-dimerized phase transition in the thermodynamic limit. The fractal nature at the SU(3) point is confirmed indirectly by the nearby scale-invariant-like states, following the spontaneous breaking of SU(3) symmetry to SU(2)×U(1) symmetry, resulting in two type-B Goldstone modes. Such scale-invariant-like states in the vicinity of points relating to type-B Goldstone modes may exist more generally in other models, offering an indirect approach to detecting type-B Goldstone modes.

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