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Entanglement Dynamics and Spin Squeezing of The non-linear Tavis-Cummings model mediated by a Nonlinear Binomial Field

机译:非线性系统的纠缠动力学与自旋压缩   由非线性二项式场介导的Tavis-Cummings模型

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摘要

We show that spin squeezing implies entanglement for quantumtripartite-state, where the subsystem of the bipartite-state is identical. Westudy the relation between spin squeezing parameters and entanglement throughthe quantum entropy of a system starts initially in a pure state when thecavity is binomial. We show that spin squeezing can be a convenient tool togive some insight into the subsystems entanglement dynamics when the bipartitesubsystem interacts simultaneously with the cavity field subsystem, speciallywhen the interaction occurs off-resonantly without and with a nonlinear mediumcontained in the cavity field subsystem. We illustrate that, in case of largeoff-resonance interaction, spin squeezing clarifies the properties ofentanglement almost with full success. However, it is not a general rule whenthe cavity is assumed to be filled with a non-linear medium. In this case, weillustrate that the insight into entanglement dynamics becomes more clearly incase of a weak nonlinear medium than in strong nonlinear medium. In parallel,the role of the phase space distribution in quantifying entanglement is alsostudied. The numerical results of Husimi $Q$-function show that the integerstrength of the nonlinear medium produces Schr\"{o}dinger cat states which isnecessary for quantum entanglement.
机译:我们表明自旋压缩意味着量子三方态的纠缠,其中两方态的子系统是相同的。检验当腔为二项式时,自旋压缩参数与通过系统量子熵的纠缠之间的关系最初从纯态开始。我们表明,自旋压缩可以成为一种方便的工具,以便在二分子系统与腔场子系统同时相互作用时,特别是当相互作用不谐振地在腔场子系统中包含和不包含非线性介质的情况下发生时,子系统的纠缠动力学有一些见解。我们说明,在大共振共振的情况下,自旋压缩几乎完全成功地阐明了纠缠的性质。然而,当空腔被非线性介质填充时,这不是一般规则。在这种情况下,我们说明,在弱非线性介质的情况下,与在强非线性介质中相比,对纠缠动力学的了解变得更加清晰。同时,研究了相空间分布在量化纠缠中的作用。 Husimi $ Q $函数的数值结果表明,非线性介质的整数强度产生Schr \“ {o} dinger猫态,这是量子纠缠所必需的。

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  • 作者

    Ateto, M. S.;

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  • 年度 2010
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  • 原文格式 PDF
  • 正文语种 {"code":"en","name":"English","id":9}
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