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    Limitations of strong coupling in non-Markovian quantum thermometry

    Qing-Shou Tan1,*, Yang Liu1, Xulin Liu1, Hao Chen1, Xing Xiao2, and Wei Wu3

    • 1Key Laboratory of Hunan Province on Information Photonics and Freespace Optical Communication, College of Physics and Electronics, Hunan Institute of Science and Technology, Yueyang, Hunan 414000, China
    • 2School of Physics and Electronic Information, Gannan Normal University, Ganzhou, Jiangxi 341000, China
    • 3Key Laboratory of Theoretical Physics of Gansu Province and Lanzhou Center for Theoretical Physics, Lanzhou University, Lanzhou, Gansu 730000, China

    • *Contact author: qstan@hnist.edu.cn

    Phys. Rev. A 112, 042612 – Published 20 October, 2025

    DOI: https://doi.org/10.1103/t74h-c8kw

    Abstract

    We investigate quantum thermometry using a single-qubit probe embedded in a non-Markovian environment, employing the numerically exact hierarchical equations of motion (HEOM) to overcome the limitations of Born-Markov approximations. Through a systematic analysis of the dynamical and steady-state behavior of the quantum signal-to-noise ratio (QSNR) for temperature estimation, we identify several key findings that challenge the conventional expectation that strong coupling necessarily enhances thermometric performance. In nonequilibrium dynamical thermometry, weak system-environment coupling generally yields the optimal QSNR, whereas in the steady-state regime, strong coupling enhances sensitivity only in the ultralow-temperature limit, while weak coupling significantly improves precision at moderately low temperatures. To optimize performance across coupling regimes, we develop a hybrid computational framework that integrates HEOM with quantum-enhanced particle swarm optimization, enabling precise quantum dynamical control under varying coupling strengths. Our results reveal fundamental constraints and opportunities in quantum thermometry, offering practical strategies for the design of high-performance quantum thermometers operating in realistic open quantum systems.

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