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This research presents a novel time-local master equation for open quantum systems driven by periodic forces, effectively capturing strong non-Markovian memory effects without resorting to the Markov approximation. By leveraging Floquet theory combined with projection operator techniques, the study identifies quasienergy-induced mechanisms that create decoherence-protected subspaces in driven dissipative environments. These findings advance theoretical frameworks essential for controlling quantum coherence and noise resilience in future fault-tolerant quantum processors.
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Floquet time-convolutionless master equation for non-Markovian driven quantum systems

arXiv2 min read

arXiv:2607.24406v1 Announce Type: new Abstract: We study the dynamics of open quantum systems driven by an external time-periodic force. Combining Floquet theory and the time-convolutionless projection operator technique we derive a time-local quantum master equation which exactly takes into account the periodic driving, while treating the system-environment interaction within second order in the coupling strength without performing the Markov approximation. The resulting equation of motion for the reduced density matrix is called Floquet time-convolutionless master equation. Employing the example of the driven spin-boson system, we demonstrate that this master equation is capable of describing strong non-Markovian effects, while yielding the Floquet-Lindblad master equation in the Markovian limit. A characteristic feature of memory effects in such driven dissipative systems is the emergence of sharp peaks of the trace-distance based non-Markovianity measure as a function of the driving amplitude, which can be traced back to quasienergy crossings leading to almost decoherence-protected subspaces through a quasienergy-induced dissipative decoupling mechanism.

Abstract:We study the dynamics of open quantum systems driven by an external time-periodic force. Combining Floquet theory and the time-convolutionless projection operator technique we derive a time-local quantum master equation which exactly takes into account the periodic driving, while treating the system-environment interaction within second order in the coupling strength without performing the Markov approximation. The resulting equation of motion for the reduced density matrix is called Floquet time-convolutionless master equation. Employing the example of the driven spin-boson system, we demonstrate that this master equation is capable of describing strong non-Markovian effects, while yielding the Floquet-Lindblad master equation in the Markovian limit. A characteristic feature of memory effects in such driven dissipative systems is the emergence of sharp peaks of the trace-distance based non-Markovianity measure as a function of the driving amplitude, which can be traced back to quasienergy crossings leading to almost decoherence-protected subspaces through a quasienergy-induced dissipative decoupling mechanism.

arXiv:2607.24406 [quant-ph]

(or arXiv:2607.24406v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2607.24406 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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Full text under the publisher's open licence · 242 words

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