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    Scheme to Detect the Strong-to-Weak Symmetry Breaking via Randomized Measurements

    Ning Sun1, Pengfei Zhang1,2,3,4,*, and Lei Feng1,2,5,6,4,†

    • 1Department of Physics, Fudan University, Shanghai 200438, China
    • 2State Key Laboratory of Surface Physics, Fudan University, Shanghai 200438, China
    • 3Shanghai Qi Zhi Institute, AI Tower, Xuhui District, Shanghai 200232, China
    • 4Hefei National Laboratory, Hefei 230088, China
    • 5Institute for Nanoelectronic devices and Quantum computing, Fudan University, Shanghai 200438, China
    • 6Shanghai Key Laboratory of Metasurfaces for Light Manipulation, Shanghai 200433, China

    • *Contact author: PengfeiZhang.physics@gmail.com
    • †Contact author: leifeng@fudan.edu.cn

    Phys. Rev. Lett. 135, 090403 – Published 29 August, 2025

    DOI: https://doi.org/10.1103/7p5x-7yqb

    Abstract

    Symmetry breaking plays a central role in classifying the phases of quantum many-body systems. Recent developments have highlighted a novel symmetry-breaking pattern, in which the strong symmetry of a density matrix spontaneously breaks to the weak symmetry. This strong-to-weak symmetry breaking is typically detected using multireplica correlation functions, such as the Rényi-2 correlator. In this Letter, we propose a practical protocol for detecting strong-to-weak symmetry breaking in experiments using the randomized measurement toolbox. Our scheme involves collecting the results of random Pauli measurements for (i) the original quantum state and (ii) the quantum state after evolution with the charged operators. Based on the measurement results, with a large number of samples, we can obtain an unbiased estimate of the Rényi-2 correlator. With a small sample size, we can still provide an alternative approach to estimate the phase boundary to a decent accuracy. We perform numerical simulations of Ising chains with all-to-all decoherence as an exemplary demonstration. Our result opens the opportunity for the experimental studies of the novel quantum phases in mixed quantum states.

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