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Gaussian measures of entanglement versus negativities: Ordering of two-mode Gaussian states

机译:纠缠与负性的高斯度量:双模高斯态的阶

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We study the entanglement of general (pure or mixed) two-mode Gaussian states of continuous-variable systems by comparing the two available classes of computable measures of entanglement: entropy-inspired Gaussian convex-roof measures and positive partial transposition-inspired measures (negativity and logarithmic negativity). We first review the formalism of Gaussian measures of entanglement, adopting the framework introduced in M. M. Wolf , Phys. Rev. A 69, 052320 (2004), where the Gaussian entanglement of formation was defined. We compute explicitly Gaussian measures of entanglement for two important families of nonsymmetric two-mode Gaussian state: namely, the states of extremal (maximal and minimal) negativities at fixed global and local purities, introduced in G. Adesso , Phys. Rev. Lett. 92, 087901 (2004). This analysis allows us to compare the different orderings induced on the set of entangled two-mode Gaussian states by the negativities and by the Gaussian measures of entanglement. We find that in a certain range of values of the global and local purities (characterizing the covariance matrix of the corresponding extremal states), states of minimum negativity can have more Gaussian entanglement of formation than states of maximum negativity. Consequently, Gaussian measures and negativities are definitely inequivalent measures of entanglement on nonsymmetric two-mode Gaussian states, even when restricted to a class of extremal states. On the other hand, the two families of entanglement measures are completely equivalent on symmetric states, for which the Gaussian entanglement of formation coincides with the true entanglement of formation. Finally, we show that the inequivalence between the two families of continuous-variable entanglement measures is somehow limited. Namely, we rigorously prove that, at fixed negativities, the Gaussian measures of entanglement are bounded from below. Moreover, we provide some strong evidence suggesting that they are as well bounded from above.
机译:通过比较两种可用的纠缠可计算量度,我们研究了连续变量系统的一般(纯或混合)双模高斯状态的纠缠:熵激发的高斯凸屋顶量度和正部分换位激发的量度(负性)和对数负数)。我们首先采用M.M. Wolf,Phys。 Rev.A 69,052320(2004),其中定义了高斯形成的纠缠。我们显式地计算了两个重要的非对称双模高斯状态族的纠缠的高斯测度:即在固定的全局和局部纯度下的极值(最大和最小)负性状态,引入G. Adesso,Phys。牧师92,087901(2004)。该分析使我们能够比较由负性和高斯纠缠度对在纠缠双模高斯状态集上诱导的不同顺序。我们发现,在全局纯度和局部纯度的特定范围内(表征相应极值状态的协方差矩阵),最小消极状态比最大消极状态具有更多的高斯缠结。因此,即使限于一类极值态,高斯测度和负性也绝对是非对称双模高斯态纠缠的不等价测度。另一方面,纠缠度的两个族在对称态上完全相等,为此,高斯形成的纠缠与真实的形成的纠缠重合。最后,我们表明连续可变纠缠测度的两个族之间的不等式在某种程度上受到限制。即,我们严格证明,在固定负数下,高斯缠结量度是从下面限制的。此外,我们提供了一些有力的证据,表明它们也从上面受到限制。

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