二部纠缠非线性相干态的量子不和谐

E. Castro, A. Zambrano, C. Ladera, R. Gómez
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引用次数: 1

摘要

量子不和谐测量的是在多方系统中局部不可访问的成对互信息的比例。非零量子纠缠虽然保证了二部量子系统中量子相关的存在,但零纠缠并不能保证不存在量子相关,因此非零量子不和谐具有有趣而重要的应用。另一方面,许多量子光学系统可以被描述为变形量子振子。在这项工作中,我们研究了二部纠缠非线性相干态的量子不和谐,在所谓的f-变形相干态代数的背景下。为了计算量子不和谐,我们考虑了基于二部纠缠f形变相干态的准Werner混合态。导出了两种不同非线性变形相干态的量子不谐的显式解析表达式。前者将得到的形变相干态作为湮灭变形算子的本征态,后者是利用形变位移算子得到的本征态。当非线性变形函数分别与Gilmore-Perelomov或Barut-Girardello表示中的SU(1,1)相干态相关联时,我们比较了这些态的量子不和谐。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Quantum discord of bipartite entangled non-linear coherent states
Quantum discord measures the fraction of the pair-wise mutual information that is locally inaccessible in a multipartite system. Nonzero quantum discord has interesting and significant applications because although non-zero entanglement guarantees the existence of quantum correlation in a bipartite quantum system, zero entanglement does not guarantee the absence of a quantum correlation. On the other hand, many quantum optics systems can be described as deformed quantum oscillators. In this work, we investigate the quantum discord of bipartite entangled nonlinear coherent states, in the context of the so-called f-deformed coherent states algebra. To calculate the quantum discord, we consider quasi- Werner mixed states bases on bipartite entangled f-deformed coherent states. Two explicit analytic expressions are derived for the quantum discord of two different nonlinear deformed coherent states. The first one considers deformed coherent states obtained as eigenstates of the annihilation deformed operator, and the second one is obtained by using a deformed displacement operator. We compare the quantum discord of those states, when the nonlinear deformation function is either associated with the SU(1,1) coherent states in the Gilmore-Perelomov or Barut-Girardello representations, respectively.
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