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Separable-entangled frontier in a bipartite harmonic system

机译:二次谐波系统中的可缠边界

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We consider a statistical mixture based on that of two identical harmonic oscillators which is characterized by four parameters, namely, the concentrations (x and y) of diagonal and nondiagonal bipartite states, and their associated thermal-like noises (T/α and T, respectively). The fully random mixture of two spins 1/2 as well as the Einstein-Podolsky-Rosen (EPR) state are recovered as particular instances. By using the conditional nonextensive entropy as introduced by Abe and Rajagopal, we calculate a bound for the separable-entangled frontier. Although this procedure is known to provide a necessary but in general not sufficient condition for separability, it does recover, in the particular case x = T = 0 ( α), the 1/3 exact result known as Peres' criterion. The x = 0 frontier remarkably resembles to the critical line associated with standard diluted ferromagnetism where the entangled region corresponds to the ordered one and the separable region to the paramagnetic one. The entangled region generically shrinks for increasing T or increasing α.
机译:我们考虑基于两个相同的谐振子的统计混合,其特征在于四个参数,即对角和非对角二分态的浓度(x和y)及其相关的类热噪声(T /α和T,分别)。作为特定实例,恢复了两个自旋1/2的完全随机混合物以及爱因斯坦-波多尔斯基-罗森(EPR)状态。通过使用由安倍晋三和拉贾戈帕尔引入的条件非广义熵,我们计算了可分离纠缠边界的界。尽管已知此过程为可分离性提供了必要的条件(但通常不是充分条件),但在特定情况下x = T = 0(α),它确实可以恢复1/3精确结果,即佩雷斯准则。 x = 0的边界显着类似于与标准稀释铁磁性相关的临界线,其中纠缠区域对应于有序区域,而可分离区域对应于顺磁性区域。纠缠区域通常会收缩以增加T或增加α。

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