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This paper investigates the mathematical derivation of exponential decay in quantum systems, specifically proving how discrete spectral models converge to continuous limits where Fermi's golden rule applies. By analyzing Friedrichs Hamiltonians coupled to bosonic fields, it provides rigorous error estimates for survival probability under specific convergence conditions relevant to open quantum system theory.
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On the Emergence of Exponential Decay from Discrete Spectra for Friedrichs Hamiltonians

arXiv2 min read

arXiv:2607.29485v1 Announce Type: cross Abstract: We study a class of Friedrichs Hamiltonians, that is, operators describing an excited state coupled to a bath through a rank-one perturbation, in the case where the bath Hamiltonian has purely discrete spectrum. We consider sequences of such Hamiltonians for which the spectral measures associated to the coupling functions by the bath Hamiltonians converge weakly to a limiting measure that is absolutely continuous with a H\"older continuous density near the excited energy. Under this assumption, we show that the survival probability of the excited state decays in an approximately exponential manner on suitable time scales and under favourable conditions, with a decay rate given by Fermi's golden rule for the limiting measure. The error is estimated in terms of the coupling strength and the L\'evy distance between the discrete spectral measures and the limiting measure. As an application, we treat a two-level atom coupled to a massless bosonic field confined to a large cavity in the rotating-wave approximation.

Abstract:We study a class of Friedrichs Hamiltonians, that is, operators describing an excited state coupled to a bath through a rank-one perturbation, in the case where the bath Hamiltonian has purely discrete spectrum. We consider sequences of such Hamiltonians for which the spectral measures associated to the coupling functions by the bath Hamiltonians converge weakly to a limiting measure that is absolutely continuous with a Hölder continuous density near the excited energy. Under this assumption, we show that the survival probability of the excited state decays in an approximately exponential manner on suitable time scales and under favourable conditions, with a decay rate given by Fermi's golden rule for the limiting measure. The error is estimated in terms of the coupling strength and the Lévy distance between the discrete spectral measures and the limiting measure. As an application, we treat a two-level atom coupled to a massless bosonic field confined to a large cavity in the rotating-wave approximation.

arXiv:2607.29485 [math-ph]

(or arXiv:2607.29485v1 [math-ph] for this version)

https://doi.org/10.48550/arXiv.2607.29485 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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Full text under the publisher's open licence · 249 words

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