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Volumn 62, Issue 4, 2000, Pages 8-

Quantum communication with correlated nonclassical states

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EID: 85037256660     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.62.042311     Document Type: Article
Times cited : (91)

References (59)
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    • A. S. ParkinsH. J. Kimble available as e-print quant-ph/9904062; and submitted, 1999, e-print quant-ph/9909021.
    • (1999)
    • Parkins, A.S.1    Kimble, H.J.2
  • 34
    • 85037201855 scopus 로고    scopus 로고
    • United States Patent No. 5 339 182, Method and Apparatus for Quantum Communication Employing Nonclassical Correlations of Quadrature-Phase Amplitudes, issued 1994, H. J. Kimble, Z. Y. Ou, and S. F. Pereira
    • United States Patent No. 5 339 182, Method and Apparatus for Quantum Communication Employing Nonclassical Correlations of Quadrature-Phase Amplitudes, issued 1994, H. J. Kimble, Z. Y. Ou, and S. F. Pereira.
  • 40
    • 85037199903 scopus 로고    scopus 로고
    • M. Hillery, e-print quant-ph/9909006.
    • Hillery, M.1
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    • T. C. Ralph, e-print quant-ph/9907073.
    • Ralph, T.C.1
  • 42
    • 85037199052 scopus 로고    scopus 로고
    • M. D. Reid, e-print quant-ph/9909030.
    • Reid, M.D.1
  • 43
    • 0033617575 scopus 로고    scopus 로고
    • For a recent review of security proofs in quantum cryptography, see C. H. Bennett and P. W. Shor, Science 284, 747 (1999).
    • (1999) Science , vol.284 , pp. 747
    • Bennett, C.H.1    Shor, P.W.2
  • 45
    • 85037195745 scopus 로고    scopus 로고
    • D. Mayers, e-print quant-ph/9802025.
    • Mayers, D.1
  • 47
    • 0003904245 scopus 로고
    • J. Dalibard, J. M. Raimond, J. Zinn Justin, Elsevier, Amsterdam
    • H. J. Kimble, in Fundamental Systems in Quantum Optics, edited by J. Dalibard, J. M. Raimond, and J. Zinn Justin (Elsevier, Amsterdam, 1992), p. 545ff.
    • (1992) Fundamental Systems in Quantum Optics
    • Kimble, H.J.1
  • 54
    • 85037182817 scopus 로고    scopus 로고
    • Figs. 22 and 33, (Formula presented) (2.8 dB above) due to a slight imbalance (0.1 dB) between the (Formula presented) detectors and to a small contribution (0.1 dB) from detector thermal noise
    • In Figs. 22 and 33, (Formula presented) (2.8 dB above) due to a slight imbalance (0.1 dB) between the (Formula presented) detectors and to a small contribution (0.1 dB) from detector thermal noise.


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