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This research investigates how collective effects in time-delayed waveguide QED setups induce non-Markovian behavior, challenging standard approximations used in quantum many-body systems. The findings reveal that memory impacts are state-dependent and become significant as emitter counts increase, offering critical insights for scaling up quantum devices. These results underscore the necessity of carefully evaluating Markov assumptions when designing large-scale quantum architectures.
Emergent non-Markovianity in time-delayed waveguide QED
arXiv:2608.26427v1 Announce Type: new Abstract: Quantum systems are invariably coupled to a surrounding environment. A common theoretical method to simplify the problem is to trace over the environment under a Markov approximation, which assumes that the environment holds no memory over the timescales that the system evolves under. In interacting many-body systems, it is often not trivial to extract which of the multiple collective timescales are relevant. We consider a time-delayed waveguide QED setup with a single excitation. By fixing the maximum propagation time and increasing the number of emitters, we show that, even for small delay times, collective effects are sufficient to cause non-Markovianity. The impact of memory is intrinsically state-dependent. For superradiant states, the relevant system timescale is the superradiant lifetime while the relevant bath timescale is the end-to-end delay time. For subradiant states, both timescales depend on the structure of the specific state. Our results demonstrate the importance of prudently making Markov approximations in quantum many-body systems, and highlight potential pitfalls to avoid in scaling up quantum devices to large system sizes.
Abstract:Quantum systems are invariably coupled to a surrounding environment. A common theoretical method to simplify the problem is to trace over the environment under a Markov approximation, which assumes that the environment holds no memory over the timescales that the system evolves under. In interacting many-body systems, it is often not trivial to extract which of the multiple collective timescales are relevant. We consider a time-delayed waveguide QED setup with a single excitation. By fixing the maximum propagation time and increasing the number of emitters, we show that, even for small delay times, collective effects are sufficient to cause non-Markovianity. The impact of memory is intrinsically state-dependent. For superradiant states, the relevant system timescale is the superradiant lifetime while the relevant bath timescale is the end-to-end delay time. For subradiant states, both timescales depend on the structure of the specific state. Our results demonstrate the importance of prudently making Markov approximations in quantum many-body systems, and highlight potential pitfalls to avoid in scaling up quantum devices to large system sizes.
Quantum Physics (quant-ph); Optics (physics.optics)
arXiv:2608.26427 [quant-ph]
(or arXiv:2608.26427v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2608.26427 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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