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Dynamics of different entanglement measures of two three-level atoms interacting nonlinearly with a single-mode field

机译:两个三能级原子不同纠缠度量的动力学   与单模场非线性地相互作用

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摘要

In this paper, we present a model which exhibits two identical $\Xi$-typethree-level atoms interacting with a single-mode field with $k$-photontransition in an optical cavity enclosed by a Kerr medium. Considering fullnonlinear formalism, it is assumed that the single-mode field, atom-fieldcoupling and Kerr medium are all $f$-deformed. By using the adiabaticelimination method, it is shown that, the Hamiltonian of the considered systemcan be reduced to an effective Hamiltonian with two two-level atoms and$f$-deformed Stark shift. In spite of the fact that, the system seems to becomplicated, under initial conditions which may be prepared for the atoms(coherent superposition of their ground and upper states) and the field(coherent state), the explicit form of the state vector of the entire system isanalytically obtained. Then, the entanglement dynamics between differentsubsystems (i.e. "field-two atoms", "atom-(field+atom)" and "atom-atom") areevaluated through appropriate measures like von Neumann entropy, tangle andconcurrence. In addition, the effects of intensity-dependent coupling, deformedKerr medium, detuning parameter, deformed Stark shift and multi-photon processon the considered entanglement measures are numerically analyzed, in detail. Itis shown that the degree of entanglement between subsystems can be controlledby selecting the evolved parameters, suitably. Briefly, the Kerr medium highlydecreases the amount of different considered measures of entanglement,especially for two-photon transition. This destructive effect preserves evenwhen all other parameters are present, too. Furthermore, we find that theso-called entanglement sudden death and birth can occur in the atom-atomentanglement.
机译:在本文中,我们提出了一个模型,该模型展示了两个相同的$ \ Xi $型三能级原子与被Kerr介质包围的光学腔中的$ k $-光子跃迁相互作用的单模场。考虑到完全非线性形式主义,假设单模场,原子场耦合和Kerr介质都是$ f $变形的。通过使用绝热消除方法,可以看出,所考虑系统的哈密顿量可以简化为具有两个二能级原子和$ f $变形的斯塔克位移的有效哈密顿量。尽管存在这样的事实,但该系统似乎很复杂,在可能为原子(基态和上态的相干叠加)和场(相干态)准备的初始条件下,状态向量的显式形式为整个系统可以通过解析获得。然后,通过诸如冯·诺依曼熵,纠缠和并发性的适当措施来评估不同子系统(即“场-两个原子”,“原子-(场+原子)”和“原子-原子”)之间的纠缠动力学。此外,还详细分析了强度依赖性耦合,变形的Kerr介质,失谐参数,变形的Stark位移和多光子过程对所考虑的纠缠措施的影响。结果表明,可以通过适当选择演化参数来控制子系统之间的缠结程度。简而言之,Kerr介质极大地减少了各种考虑的纠缠量,尤其是对于两个光子跃迁。即使所有其他参数都存在,这种破坏性的效果也会保留。此外,我们发现原子缠结中可能发生所谓的纠缠猝死。

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