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Modular construction of special mixed quantum states
Authors:Email author" target="_blank">M?MichelEmail author  G?Mahler
Institution:(1) Institute of Theoretical Physics I, University of Stuttgart, Pfaffenwaldring 57, 7, 0550 Stuttgart, Germany
Abstract:For a homogeneous quantum network of N subsystems with n levels each we consider separable generalized Werner states. A generalized Werner state is defined as a mixture of the totally mixed state and an arbitrary pure state $\vert\psi\rangle$ : $\hat{p}_{Werner} = (1-\epsilon)\hat{1}+\epsilon\vert\psi\rangle\langle\psi\vert$ with a mixture coefficient $\epsilon$ . For this density operator $\hat{p}_{Werner}$ to be separable, $\epsilon$ will have an upper bound $\epsilon_{sep}\leq1$ . Below this bound one should alternatively be able to reproduce $\hat{p}_{Werner}$ by a mixture of entirely separable input-states. For this purpose we introduce a set of modules, each contributing elementary coherence properties with respect to a generalized coherence vector. Based on these there exists a general step-by-step mixing process for any $\epsilon_{mix}\leq\epsilon_{max}$ . For $\vert\psi\rangle$ being a cat-state it is possible to define an optimal process, which produces states right up to the separability boundary ( $\epsilon_{max} = \epsilon_{sep} $ ).Received: 3 December 2002, Published online: 29 July 2003PACS: 03.65.Ud Entanglement and quantum nonlocality (e.g. EPR paradox, Bellrsquos inequalities, GHZ states, etc.) - 03.67.-a Quantum information - 03.65.-w Quantum mechanics
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