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F. De Martini, Phys. Rev. Lett. 81, 2842 (1998); Phys. Lett. A 250, 15 (1998). In the present paper a non conditional experiment is reported, where the R-amplified ebit is post-selected by NEIF against the squeezed- vacuum noise.
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Phys. Rev. Lett.
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De Martini, F.1
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F. De Martini, Phys. Rev. Lett. 81, 2842 (1998); Phys. Lett. A 250, 15 (1998). In the present paper a non conditional experiment is reported, where the R-amplified ebit is post-selected by NEIF against the squeezed-vacuum noise.
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The virtual absence of decoherence in the QIOPA is discussed in [8, 9]
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F. De Martini, V. Mussi, and F. Bovino, Optics Comm. 179, 581 (2000). The virtual absence of decoherence in the QIOPA is discussed in [8, 9].
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G. Di Giuseppe, F. De Martini, D. Boschi, and S. Branca, in: Quantum Interferometry, F. De Martini, G. Denardo, and Y. Shih (eds.), VCH, Berlin 1996. See also: Fortschritte der Physik 46, 643 (1998).
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D. Boschi, S. Branca, F. De Martini, L. Hardy, and S. Popescu, Phys. Rev. Lett. 80, 1121 (1998). The parity-selectivity of the present system is indeed formally related to the Bell-state selectivity within the above QST scheme.
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D. Walls and G. Milburn, Quantum Optics, Springer, New York 1994. Note that in general, the adoption of different φ's of the λ/4 plate and of an optional π-analyzer, all possible 2-particle entangled states, with any parity could be generated by this procedure starting from any L-generated |Φ′〉.
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W. L. Munro and M. D. Reid, Quantum Opt. 6, 1 (1994); W. L. Munro, M. D. Reid and F. De Martini, in preparation.
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