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Theoretical modeling demonstrates accurate multi-time correlation functions in strongly coupled spin-boson models, highlighting expanded reach for analytical open quantum system equations.
While the quantum regression theorem (QRT) is the standard tool for computing multi-time correlation functions in open quantum systems, it relies on system–bath separability and an environment that remains in equilibrium, assumptions that are violated once dynamical correlations develop. Using the projection operator formalism, we derive an extension to the QRT that explicitly incorporates these correlation-induced corrections, enabling us to capture multi-time correlation functions in non-Markovian regimes. We apply this framework to the variational polaron master equation for the spin–boson model in ohmic and super-ohmic regimes, where the polaron transformation mixes system–bath degrees of freedom to produce a non-thermal effective environment. Benchmarking against numerically exact tensor-network simulations, we demonstrate quantitative agreement for single- and two-time observables, including linear-response spectra, even at strong coupling. Our approach broadens the reach of analytic master equations to multi-time observables in strong-coupling and non-Markovian regimes, where environmental memory effects and system–bath correlations are crucial.
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Bundgaard-Nielsen et al. (2026) studied this question.
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