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    Power-Law Scaling of Lasing-State Switching in Optical Microcavities

    Qi-Tao Cao1, Qing-Xin Ji1,*, Pei-Ji Zhang1, Chiao Wang1, H. T. Quan1, Pai Peng2, Wenjing Liu1, and Yun-Feng Xiao1,3,†

    • 1State Key Laboratory for Mesoscopic Physics, Frontiers Science Center for Nano-optoelectronics, New Cornerstone Science Laboratory, School of Physics, Peking University, 100871 Beijing, China
    • 2Department of Electrical Engineering and Computer Science, Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
    • 3Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan 030006, China

    • *Present address: T. J. Watson Laboratory of Applied Physics, California Institute of Technology, Pasadena, California, USA.
    • †Contact author: yfxiao@pku.edu.cn

    Phys. Rev. Lett. 136, 053803 – Published 5 February, 2026

    DOI: https://doi.org/10.1103/s2x6-5k55

    Abstract

    Driven-dissipative optical microcavities provide a versatile platform for exploring lasing dynamics far from equilibrium. While the Kibble-Zurek mechanism provides a framework for understanding non-equilibrium phase transitions, the critical dynamics associated with first-order phase transitions in microlasers, particularly as a non-Hermitian system, remains largely unexplored. Here we report the temporal critical behavior of lasing-state transitions in an ultrahigh-Q whispering-gallery microlaser. By dynamically ramping a non-Hermitian interferometric coupling, the laser switches between two nearly degenerate standing-wave supermodes with opposite parities. Using radio-frequency beat-note readout with high resolution, we directly capture the real-time switching process and measure the transition time as a function of the ramp speed. A power-law scaling is found with an exponent of ∼0.5, which also remains robust in coupled-cavity laser networks, setting a fundamental speed limit for microcavity laser state conversion.

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