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Volumn 62, Issue 5, 2000, Pages 052310-052311

Optimization of entanglement witnesses

Author keywords

[No Author keywords available]

Indexed keywords

ALGORITHMS; CORRELATION METHODS; DATA PROCESSING; ELECTRON ENERGY LEVELS; MATHEMATICAL OPERATORS; OPTIMIZATION;

EID: 0141782139     PISSN: 10502947     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevA.62.052310     Document Type: Article
Times cited : (696)

References (54)
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    • T A ≥ 0. The relation between separable and positive partial transpose operators was established in Refs. [10, 11]. All separable operators have a positive partial transposition. However, the converse is not true in general. That is, there are positive partial transpose operators which are nonseparable.
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    • B.
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    • T.
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    • -1 X is the projector in R(X). If X has no zero eigenvalue, the pseudoinverse coincides with the inverse operator.
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    • For more examples of PPTES's also see (a) Ref. [9]; (b) D. Bruß and A. Peres, Phys. Rev. A 61, 030301(R) (2000); (c) P. Horodecki and M. Lewenstein, e-print quant-ph/0001035; Phys. Rev. Lett, (to be published).
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    • For more examples of PPTES's also see (a) Ref. [9]; (b) D. Bruß and A. Peres, Phys. Rev. A 61, 030301(R) (2000); (c) P. Horodecki and M. Lewenstein, e-print quant-ph/0001035; Phys. Rev. Lett, (to be published).
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    • e-print quant-ph/0001035; to be published
    • For more examples of PPTES's also see (a) Ref. [9]; (b) D. Bruß and A. Peres, Phys. Rev. A 61, 030301(R) (2000); (c) P. Horodecki and M. Lewenstein, e-print quant-ph/0001035; Phys. Rev. Lett, (to be published).
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    • b, where the partial transposition is taken in that basis.
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    • note
    • These states can be prepared locally, and can be used to construct PPTES's by mixing them "weakly" with entangled states. This provides an interesting possibility of an experimental realization of PPTES's. This suggestion was formulated by A. Weinfurter.
  • 54


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