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    Observing the exponential growth of the eigenmodes in the absence of coalescence for a non-Hermitian circuit with an unavoidable inductor dissipation

    Jiaming Zhang1,2, Wenxuan Song1,2, Hanhao Li1,2, Zhiye Kuang1,2, Zhihua Xiong1,2, Longwen Zhou3,4,5, Jie Liu6,7,*, and Wen-Lei Zhao1,2,†

    • 1School of Science, Jiangxi University of Science and Technology, Ganzhou 341000, China
    • 2Key Laboratory of Low Dimensional Quantum Materials and Sensor Devices of Jiangxi Education Institutes, Ganzhou 341000, China
    • 3College of Physics and Optoelectronic Engineering, Ocean University of China, Qingdao 266100, China
    • 4Key Laboratory of Optics and Optoelectronics, Qingdao 266100, China
    • 5Engineering Research Center of Advanced Marine Physical Instruments and Equipment of MOE, Qingdao 266100, China
    • 6Graduate School of China Academy of Engineering Physics, Beijing 100193, China
    • 7CAPT, HEDPS, and IFSA Collaborative Innovation Center of the Ministry of Education, Peking University, Beijing 100871, China

    • *Contact author: jliu@gscaep.ac.cn
    • †Contact author: wlzhao@jxust.edu.cn

    Phys. Rev. A 112, 052211 – Published 13 November, 2025

    DOI: https://doi.org/10.1103/xlbc-w5ng

    Abstract

    We investigate, both experimentally and theoretically, the eigenmodes of an electronic circuit in which gain and loss RLC resonators are coupled through a capacitor. Due to the unavoidable magnetic loss in the inductors, we find that the eigenmode coalescence no longer emerges in contrast to the conventional non-Hermitian systems with spontaneous PT-symmetry breaking. In particular, we find a transition from exponential decay to exponential growth in the amplitude of the periodic voltage oscillations of the resonators. The transition occurs near the exceptional points of the non-Hermitian circuit without considering the dissipations in inductors. We introduce a small resistor two orders of magnitude smaller than that of the RLC resonators to mimic the energy dissipation in inductors and numerically solve the equivalent non-Hermitian Schrödinger equation. The numerical results can well reproduce experimental observations. Our above findings unambiguously indicate that the exponential growth behavior beyond the exceptional points is robust against some unavoidable dissipative perturbations.

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