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arXiv 1003.4755quant-ph
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纠缠的几何度量与Schmidt分解

Geometric measures of entanglement and the Schmidt decomposition

M. E. Carrington, R. Kobes, G. Kunstatter, D. Ostapchuk, G. Passante

摘要:

在标准几何方法中,纯态的纠缠是$\sin^2θ$,其中$θ$是纠缠态与归一化量子比特态的乘积的最接近的可分离态之间的角度。我们在这里考虑一个概括的概念,考虑可分离的国家,包括产品的非正常化状态的不同尺寸。目标纠缠态和最近的非归一化产物态之间的距离可以解释为目标态纠缠的度量。最接近的产品状态和它的范数的组件有一个解释,分别在施密特分解的状态向量中产生的约化密度矩阵的特征向量和特征值。对于目标状态具有很大对称度的几种情况,我们解析地求解方程组,并特别关注量子位数很大的极限。

英文摘要:

In the standard geometric approach, the entanglement of a pure state is $\sin^2θ$, where $θ$ is the angle between the entangled state and the closest separable state of products of normalised qubit states. We consider here a generalisation of this notion by considering separable states that consist of products of unnormalised states of different dimension. The distance between the target entangled state and the closest unnormalised product state can be interpreted as a measure of the entanglement of the target state. The components of the closest product state and its norm have an interpretation in terms of, respectively, the eigenvectors and eigenvalues of the reduced density matrices arising in the Schmidt decomposition of the state vector. For several cases where the target state has a large degree of symmetry, we solve the system of equations analytically, and look specifically at the limit where the number of qubits is large.

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