Dynamics of entangled states in squeezed reservoirs

TL;DR

This paper explores how entangled states of two cavities evolve in squeezed reservoirs, revealing that entanglement transfer and dynamics depend on the matching of initial correlations to the reservoir's quantum squeezing properties.

Contribution

It demonstrates the crucial role of quantum squeezing correlations in entanglement dynamics and distinguishes quantum from classical squeezing effects in cavity-reservoir interactions.

Findings

Entanglement transfer depends on correlation matching.

Quantum squeezing leads to unique transient entanglement features.

Entanglement recurrence occurs with a common quantum squeezed reservoir.

Abstract

Dynamics of entangled states of two independent single-mode cavities in squeezed reservoirs is investigated in the context of matching of the correlations contained in the entangled states to those contained in the squeezed reservoir. We illustrate our considerations by examining the time evolution of entanglement of single and double excitation NOON and EPR states. A comparison is made when each cavity is coupled to own reservoir or both cavities are coupled to a common reservoir. It is shown that the evolution of the initial entanglement and transfer of entanglement from the squeezed reservoir to the cavity modes depend crucially on the matching of the initial correlations to that contained in the squeezed reservoir. In particular, it is found that initially entangled modes with correlations different from the reservoir correlations prevent the transfer of the correlations from the squeezed field to the modes. In addition, we find that the transient entanglement exhibits several features unique to quantum nature of squeezing. In particular, we show that in the case of separate squeezed reservoirs a variation of the decay time of the initial entanglement with the squeezing phase is unique to quantum squeezing. In the case of a common reservoir a recurrence of entanglement occurs and we find that this feature also results from the reservoir correlations unique to quantum squeezing. There is no revival of entanglement when the modes interact with a classically squeezed field.