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note
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In Sections 3-6 of this paper, where we focus on time-bin entanglement, we call "pulse" each pulse that enters the non-linear crystal; therefore, one qubit is created by two pulses. In reference [6], we had used "pulse" to describe each pulse produced by the pump laser, each such process creating a qubit. So "per pulse" in reference [6] is equivalent to "per qubit" here
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note
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This efficiency factor takes into account the losses on the lines, the quantum efficiency η of the detector, and the amplitude of each monochromatic field component (whose weak ν-dependance has been omitted)
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3442883654
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J.D. Franson, Phys. Rev. Lett. 62, 2205 (1989); reviewed in: M.O. Scully, M.S. Zubairy, Quantum Optics (Cambridge Univ. Press, 1997), p. 597
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Franson, J.D.1
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3442883654
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Cambridge Univ. Press
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J.D. Franson, Phys. Rev. Lett. 62, 2205 (1989); reviewed in: M.O. Scully, M.S. Zubairy, Quantum Optics (Cambridge Univ. Press, 1997), p. 597
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Scully, M.O.1
Zubairy, M.S.2
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85118959691
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note
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A,B). Consequently, we set θ = εω with ω the central frequency of the photon
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c
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The data obtained in the early experiment (full squares in Fig. 4) are more noisy than the new ones (open circles) because the crystal that we used in 2001 was less efficient and because in the meantime we have improved the techniques to stabilize the interferometers
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preprint arXiv: quant-ph/0408030
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H.S. Eisenberg, G. Khoury, G. Durkin, C. Simon, D. Bouwmeester, preprint arXiv: quant-ph/0408030
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Eisenberg, H.S.1
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