The transfer of the quantum correlation from two-mode nonclassical state field to the supercurrents in two distant SQUID rings  

The transfer of the quantum correlation from two-mode nonclassical state field to the supercurrents in two distant SQUID rings

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作  者:彭朝辉 邹健 邵彬 

机构地区:[1]Department of Physics, Beijing .Institute of Technology, Beijing 100081, China [2]Department of Physics, Hunan University of Science and Technology, Xiangtan 411201, China

出  处:《Chinese Physics B》2007年第9期2569-2577,共9页中国物理B(英文版)

基  金:Project supported by the National Natural Science Foundation of China (Grant No 10374007).

摘  要:We have considered two distant mesoscopic superconducting quantum interference device (SQUID) rings A and B in the presence of two-mode nonclassical state fields and investigated the correlation of the supercurrents in the two rings using the normalized correlation function CAB. We show that when the parameter c~ is very small for the separable state with the density matrix ρ = {│α,-α) (α,-α│ + │-α, α) (-α, α│}/2 and entangled coherent state {(ECS) [u) = N1(│α, -α) + │-α, α)} fields, the dynamic behaviours of the normalized correlation function CAB are similar, but it is quite different for the entangled coherent state │u') = N2(│α,-α) - │-α, α)} field. When the parameter α is very large, the dynamic behaviours of CAB are almost the same for the separable state, entangled coherent state │u) and [u'〉 fields. For the two-mode squeezed vacuum state field the maximum of CAB increases monotonically with the squeezing parameter γ, and as γ→ ∞ , CAB→ 1. This means that the supercurrents in the two rings A and B are quantum mechanically correlated perfectly. It is concluded that not all the quantum correlations in the two-mode nonclassical state field can be transferred to the supercurrents; and the transfer depends on the state of the two-mode nonclassical state field prepared.We have considered two distant mesoscopic superconducting quantum interference device (SQUID) rings A and B in the presence of two-mode nonclassical state fields and investigated the correlation of the supercurrents in the two rings using the normalized correlation function CAB. We show that when the parameter c~ is very small for the separable state with the density matrix ρ = {│α,-α) (α,-α│ + │-α, α) (-α, α│}/2 and entangled coherent state {(ECS) [u) = N1(│α, -α) + │-α, α)} fields, the dynamic behaviours of the normalized correlation function CAB are similar, but it is quite different for the entangled coherent state │u') = N2(│α,-α) - │-α, α)} field. When the parameter α is very large, the dynamic behaviours of CAB are almost the same for the separable state, entangled coherent state │u) and [u'〉 fields. For the two-mode squeezed vacuum state field the maximum of CAB increases monotonically with the squeezing parameter γ, and as γ→ ∞ , CAB→ 1. This means that the supercurrents in the two rings A and B are quantum mechanically correlated perfectly. It is concluded that not all the quantum correlations in the two-mode nonclassical state field can be transferred to the supercurrents; and the transfer depends on the state of the two-mode nonclassical state field prepared.

关 键 词:SQUID normalized correlation function two-mode nonclassical state field 

分 类 号:O413[理学—理论物理]

 

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