Journal
PHYSICAL REVIEW A
Volume 105, Issue 6, Pages -Publisher
AMER PHYSICAL SOC
DOI: 10.1103/PhysRevA.105.062207
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Funding
- Leverhulme Quantum Biology Doctoral Training Centre at the University of Surrey - Leverhulme Trust training center [DS-2017-079]
- EPSRC (United Kingdom) Strategic Equipment [EP/L02263X/1, EP/M008576/1]
- EPSRC (United Kingdom) [EP/M027791/1]
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This study explores the dynamics of coupled atomic two-level systems within a generic bosonic reservoir. In the regime where many atoms are identically coupled to a single reservoir, interesting effects are identified, such as the strong impact of the initial configuration of atomic excited-state amplitudes on the system dynamics, which can even sever the system from its environment. Additionally, it is found that steady-state amplitudes of the excited states become independent of the specific structure of the bosonic reservoirs considered.
We explore the dynamics of N coupled atomic two-level systems embedded within a generic bosonic reservoir under specific system symmetries. In the regime of many atoms identically coupled to a single reservoir, we identify remarkable effects, notably that the initial configuration of the atomic excited-state amplitudes strongly impacts the dynamics of the system and can even fully sever the system from its environment. Additionally, we find that steady-state amplitudes of the excited states become independent of the specific structure of the bosonic reservoirs considered. The framework introduced is deployed to model a structured photonic reservoir associated with a photonic crystal, where it recaptures previous theoretical and experimental results for the superradiance rates even within the single-excitation regime. For the photonic band-gap system, our formalism predicts the generation of pairwise entanglement between initially uncorrelated atomic systems. Furthermore, it suggests that???with respect to a non-Markovian metric???the non-Markovianity of the aggregated many-atom system is modulated by the total number of atoms. This is due to a stark interplay between the Lamb shifting of the atomic transition energies due to their varying number and the increased number of atomic systems with resonant transition energies.
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