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    Double Supersolid Phase in a Bosonic t−J−V Model with Rydberg Atoms

    Kuangjie Chen1,2, Yang Qi1,3, Zheng Yan4,5,*, and Xiaopeng Li1,2,6,3,†

    • 1State Key Laboratory of Surface Physics, Institute of Nanoelectronics and Quantum Computing, Department of Physics, Fudan University, Shanghai 200438, China
    • 2Shanghai Qizhi Institute and Shanghai Artificial Intelligence Laboratory, Xuhui District, Shanghai 200232, China
    • 3Hefei National Laboratory, Hefei 230088, China
    • 4Department of Physics, School of Science and Research Center for Industries of the Future, Westlake University, Hangzhou 310030, China
    • 5Institute of Natural Sciences, Westlake Institute for Advanced Study, Hangzhou 310024, China
    • 6Shanghai Research Center for Quantum Sciences, Shanghai 201315, China

    • *Contact author: zhengyan@westlake.edu.cn
    • †Contact author: xiaopeng_li@fudan.edu.cn

    Phys. Rev. Lett. 135, 266003 – Published 22 December, 2025

    DOI: https://doi.org/10.1103/fg7f-zvtt

    Abstract

    Recent advances in Rydberg tweezer arrays bring novel opportunities for programmable quantum simulations beyond previous capabilities. In this Letter, we investigate a bosonic t−J−V model currently realized with Rydberg atoms. Through large-scale quantum Monte Carlo simulations, we uncover an emergent double supersolid (DSS) phase with the coexistence of two superfluids and crystalline order. Tunable long-range tunneling and repulsive hole-hole interactions enable a rich phase diagram featuring a double superfluid phase, a DSS phase, and an antiferromagnetic insulator. Intriguingly, within the DSS regime we observe an unconventional thermal enhancement of crystalline order. Our results establish the bosonic t−J−V model as a promising and experimentally accessible platform for exploring exotic quantum phases in Rydberg atom arrays.

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