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Peres, A.5
Wootters, W.K.6
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2
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2642621560
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for experimental realization, see D. Bouwmeester, J.-W. Pan, K. Mattle, M. Elbl, H. Weinfurter, and A. Zeilinger, Nature (London) 390, 575 (1997)
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Bouwmeester, D.1
Pan, J.-W.2
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Boschi, D.1
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Hardy, L.4
Popescu, S.5
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5
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85037190208
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T. Mor, e-print quant-ph/9608005.
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Mor, T.1
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4243445702
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see also
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C. H. Bennett, H. Bernstein, S. Popescu, and B. Schumacher, Phys. Rev. A 53, 2046 (1996);see also 6.
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Phys. Rev. A
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C. H. Bennett, G. Brassard, S. Popescu, B. Schumacher, J. Smolin, and W. K. Wootters, Phys. Rev. Lett. 76, 722 (1996).
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Bennett, C.H.1
Brassard, G.2
Popescu, S.3
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Wootters, W.K.6
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6144265213
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D. Deutsch, A. Ekert, R. Jozsa, C. Macchiavello, S. Popescu, and A. Sanpera, Phys. Rev. Lett. 77, 2818 (1996).
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Sanpera, A.6
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M. Żukowski, R. Horodecki, M. Horodecki, and P. Horodecki, Phys. Rev. A 58, 1694 (1998).
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Phys. Rev. A
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Żukowski, M.1
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Horodecki, P.4
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4243216277
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C. H. Bennett, D. P. DiVincenzo, J. Smolin, and W. K. Wootters, Phys. Rev. A 54, 3824 (1996).
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6844242534
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Phys. Rev. AB. Schumacher, 54, 2614 (1996)
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Schumacher, B.1
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0001521178
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Phys. Rev. AS. Lloyd, 55, 1613 (1997).
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Lloyd, S.1
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25
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85037235035
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Recall that the map (Formula presented) acting on spin-(Formula presented) states is called completely positive, if the map (Formula presented) acting on the states of the system of two particles, one of spin s and the other of spin (Formula presented), is positive for any second system spin (Formula presented). We also call (Formula presented) trace preserving if it preserves trace of all mapped matrices
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Recall that the map (Formula presented) acting on spin-(Formula presented) states is called completely positive, if the map (Formula presented) acting on the states of the system of two particles, one of spin s and the other of spin (Formula presented), is positive for any second system spin (Formula presented). We also call (Formula presented) trace preserving if it preserves trace of all mapped matrices.
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32
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85037184195
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A simpler example (for the 2×2 case) is given in T. Mor and P. Horodecki (unpublished)
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A simpler example (for the 2×2 case) is given in T. Mor and P. Horodecki (unpublished).
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33
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0000239556
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The states play an important role in the activation of bound entanglement; namely, in P. Horodecki, M. Horodecki, and R. Horodecki, Phys. Rev. Lett. 82, 1056 (1999), we have shown that they can be quasidistilled if supported by a large enough supply of bound entangled states.
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Phys. Rev. Lett.
, vol.82
, pp. 1056
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Horodecki, P.1
Horodecki, M.2
Horodecki, R.3
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