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      Device-independent entanglement quantification and related applications

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          Abstract

          We present a general method to quantify both bipartite and multipartite entanglement in a device-independent manner, meaning that we put a lower bound on the amount of entanglement present in a system based on observed data only but independently of any quantum description of the employed devices. Some of the bounds we obtain, such as for the Clauser-Horne-Shimony-Holt Bell inequality or the Svetlichny inequality, are shown to be tight. Besides, device-independent entanglement quantification can serve as a basis for numerous tasks. We show in particular that our method provides a rigorous way to construct dimension witnesses, gives new insights into the question whether bound entangled states can violate a Bell inequality, and can be used to construct device independent entanglement witnesses involving an arbitrary number of parties.

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          Most cited references14

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          A computable measure of entanglement

          , (2001)
          We present a measure of entanglement that can be computed effectively for any mixed state of an arbitrary bipartite system. We show that it does not increase under local manipulations of the system, and use it to obtain a bound on the teleportation capacity and on the distillable entanglement of mixed states.
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            Steering, Entanglement, Nonlocality, and the EPR Paradox

            The concept of steering was introduced by Schrodinger in 1935 as a generalization of the EPR paradox for arbitrary pure bipartite entangled states and arbitrary measurements by one party. Until now, it has never been rigorously defined, so it has not been known (for example) what mixed states are steerable (that is, can be used to exhibit steering). We provide an operational definition, from which we prove (by considering Werner states and Isotropic states) that steerable states are a strict subset of the entangled states, and a strict superset of the states that can exhibit Bell-nonlocality. For arbitrary bipartite Gaussian states we derive a linear matrix inequality that decides the question of steerability via Gaussian measurements, and we relate this to the original EPR paradox.
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              Quantum Cryptography with Orthogonal States?

              (2009)
              This is a Comment on Phys Rev Lett 75 (1995) 1239, by Goldenberg and Vaidman
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                Author and article information

                Journal
                06 February 2013
                2013-05-14
                Article
                10.1103/PhysRevLett.111.030501
                1302.1336
                0f78a179-7e11-4381-a7d1-ed7b40e712ed

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                Phys. Rev. Lett. 111, 030501 (2013)
                4 pages + appendix, resubmitted version
                quant-ph

                Quantum physics & Field theory
                Quantum physics & Field theory

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