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Switch metastable dynamics in many-body open quantum systems
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Abstract
Stochastic switching is a central phenomenon in dissipative many-body systems, offering a key probe of metastability across classical and quantum regimes. Here, we unravel the connection between switching dynamics and quantum metastability through the lens of spectral decomposition, quantum-jump simulations, and the large deviation principles. By establishing a direct correspondence between classical fixed points and quantum metastable states, we distinguish the trajectory-level noise-induced metastability from the spectrum-level deterministic metastability in a Markovian open quantum system with bistability. The Liouvillian gap, the steady-state occupation ratio, and the observed switching rates of the metastable states all exhibit exponential scaling with system size, giving rise to a quantum analogue of Arrhenius law, with the inverse system size serving as an effective temperature. These results provide a unified picture of quantum bistability and clarify the relaxation processes of strongly interacting, dissipative quantum systems far from the thermodynamic limit.
Oxford University Press (OUP)
Title: Switch metastable dynamics in many-body open quantum systems
Description:
Abstract
Stochastic switching is a central phenomenon in dissipative many-body systems, offering a key probe of metastability across classical and quantum regimes.
Here, we unravel the connection between switching dynamics and quantum metastability through the lens of spectral decomposition, quantum-jump simulations, and the large deviation principles.
By establishing a direct correspondence between classical fixed points and quantum metastable states, we distinguish the trajectory-level noise-induced metastability from the spectrum-level deterministic metastability in a Markovian open quantum system with bistability.
The Liouvillian gap, the steady-state occupation ratio, and the observed switching rates of the metastable states all exhibit exponential scaling with system size, giving rise to a quantum analogue of Arrhenius law, with the inverse system size serving as an effective temperature.
These results provide a unified picture of quantum bistability and clarify the relaxation processes of strongly interacting, dissipative quantum systems far from the thermodynamic limit.
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