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    Probing the non-Hermitian skin effect via the cavity transmission spectrum

    Yu-Bo Liang1,*, Chenyang Wang1,*, Zi-Jian Lin1, Ge Song2, Jabir Hakami3,†, Jingping Xu1,‡, and Ya-Ping Yang1,§

    • 1MOE Key Laboratory of Artificial Microstructure Materials, School of Physical Science and Engineering, Tongji University, Shanghai 200092, China
    • 2College of Information Technology, Shanghai Ocean University, Shanghai 201306, China
    • 3Department of Physical Sciences, Physics Division, College of Science, Jazan University, Jazan 45142, Saudi Arabia

    • *These authors contributed equally to this work.
    • †Contact author: j.hakami@jazanu.edu.sa
    • ‡Contact author: xx_jj_pp@tongji.edu.cn
    • §Contact author: yang_yaping@tongji.edu.cn

    Phys. Rev. A 112, 063705 – Published 5 December, 2025

    DOI: https://doi.org/10.1103/ppfg-2r57

    Abstract

    In recent years, the study of non-Hermitian systems has attracted significant attention, particularly for their unique topological phenomena such as the non-Hermitian skin effect (NHSE). Here we investigate the NHSE in a non-Hermitian Su-Schrieffer-Heeger atomic chain and its coupling with a cavity mode, focusing on how NHSE modifies the cavity's transmission spectrum. We theoretically model the atomic chain which possesses a specific symmetry under open boundary conditions. Our results show that the eigenstates localize at the chain edges for certain parameters, indicating the existence of the NHSE. This effect produces distinct peaks in the cavity transmission spectrum at frequencies corresponding to eigenstates in the nontrivial phase; these peaks vanish in the trivial phase. By tuning atomic gain and loss, we identify sharp spectral minima at the topological phase transition point, which enables precise detection of the transition. These results demonstrate that the cavity transmission spectrum serves as a sensitive probe for non-Hermitian topological effects, offering a scalable experimental framework to explore the NHSE without calculating topological invariants.

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