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    Simulating bulk gap in chiral projected entangled pair states

    Ji-Yao Chen1,*, Yi Tan2,*, Sylvain Capponi3, Didier Poilblanc3,4, Fei Ye2, and Jia-Wei Mei2,†

    • 1Center for Neutron Science and Technology, Guangdong Provincial Key Laboratory of Magnetoelectric Physics and Devices, School of Physics, Sun Yat-sen University, Guangzhou 510275, China
    • 2State Key Laboratory of Quantum Functional Materials, Department of Physics, and Guangdong Basic Research Center of Excellence for Quantum Science, Southern University of Science and Technology (SUSTech), Shenzhen 518055, China
    • 3Laboratoire de Physique Théorique, Université de Toulouse, CNRS, UPS, France
    • 4French-American Center for Theoretical Science, CNRS, KITP, Santa Barbara, California 93106-4030, USA

    • *These authors contributed equally to this work.
    • †Contact author: meijw@sustech.edu.cn

    Phys. Rev. B 113, 085130 – Published 18 February, 2026

    DOI: https://doi.org/10.1103/g8cb-fz29

    Abstract

    Projected entangled-pair states (PEPS) have proven effective in capturing chiral spin liquid ground states, yet the presence of long-range “gossamer” correlation tails raises concerns about their ability to accurately describe bulk gaps. Here, we address this challenge and demonstrate that PEPS can reliably characterize gapped bulk excitations in chiral topological phases. Using a variational principle for excited states within a local mode approximation, we establish that correlation functions decaying faster than r−2 are not necessarily related to gapless modes and thus long-range “gossamer” correlation tails in chiral PEPS do not contradict the presence of a bulk gap. This framework is validated in the spin-12 Kitaev model with a chiral term, where PEPS yields excitation gaps that agree well with exact solutions. Extending our approach to the Z3 Kitaev model, we present compelling evidence for its chiral ground state and accurately resolve its gapped excitations. These findings thus solidify PEPS as a powerful tool for studying both ground and excited states in chiral topological systems, thereby bridging a key gap in the understanding of their bulk properties.

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