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    Exact treatment of the memory kernel under time-dependent system-environment coupling via a train of delta distributions

    Yuta Uenaga1,*, Kensuke Gallock-Yoshimura1,2,†, and Takano Taira1,3,‡

    • 1Department of Physics, Kyushu University, 744 Motooka, Nishi-Ku, Fukuoka 819-0395, Japan
    • 2Department of Information and Communication Engineering, Graduate School of Information Science and Technology, The University of Tokyo, 7–3–1 Hongo, Bunkyo-ku, Tokyo 113–8656, Japan
    • 3Institute of Industrial Science, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8574, Japan

    • *Contact author: uenaga.yuta.617@s.kyushu-u.ac.jp
    • †Contact author: gallockyoshimura@biom.t.u-tokyo.ac.jp
    • ‡Contact author: taira.takano.292@m.kyushu-u.ac.jp

    Phys. Rev. A 113, 012224 – Published 26 January, 2026

    DOI: https://doi.org/10.1103/t9wh-k9pz

    Abstract

    Memory effects in a quantum system coupled to an environment are one of the central features in the theory of open quantum systems. The dynamics of such quantum systems are typically governed by an equation of motion with a time-convolution integral of the memory kernel. However, solving such integrodifferential equations is challenging, especially when the memory kernel is nonstationary (not time-translation invariant). In this paper, we analytically and nonperturbatively solve such integrodifferential equations with a nonstationary memory kernel by employing a train of Dirac-delta switchings. We then apply this method to the damped Jaynes-Cummings model and the damped harmonic oscillator model to demonstrate that (i) our solution asymptotes to the well-known exact solution in the continuum limit and that (ii) our method also enables us to visualize the memory effect in the environment.

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