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1
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85037192944
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D.N. Klyshko, Photons and Nonlinear Optics (Gordon and Breach, New York, 1988)
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D.N. Klyshko, Photons and Nonlinear Optics (Gordon and Breach, New York, 1988).
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4
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85037200789
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Y.H. Shih and C.O. Alley, in Proceedings of the 2nd International Symposium Foundation of Quantum Mechanics, Tokyo, 1986, edited by M. Namiki et al. (Physical Society of Japan, Tokyo, 1987);
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Y.H. Shih and C.O. Alley, in Proceedings of the 2nd International Symposium Foundation of Quantum Mechanics, Tokyo, 1986, edited by M. Namiki et al. (Physical Society of Japan, Tokyo, 1987)
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5
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15044361457
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Phys. Rev. Lett. 61, 2921 (1988).
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(1988)
Phys. Rev. Lett.
, vol.61
, pp. 2921
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8
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0001154787
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M.H. Rubin, D.N. Klyshko, Y.H. Shih, and A.V. Sergienko, Phys. Rev. A 50, 5122 (1994).
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(1994)
Phys. Rev. A
, vol.50
, pp. 5122
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Rubin, M.H.1
Klyshko, D.N.2
Shih, Y.H.3
Sergienko, A.V.4
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13
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85037248663
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collinear type-I SPDC, the SPDC ring overlaps with the pump beam. In this case, however, photon pair cannot be spatially separated unless they have different wavelengths
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In collinear type-I SPDC, the SPDC ring overlaps with the pump beam. In this case, however, photon pair cannot be spatially separated unless they have different wavelengths.
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16
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0000369884
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C.H. Monken, P.H. Souto Ribeiro, and S. P’adua, Phys. Rev. A 57, R2267 (1998). The result reported in this paper is, in fact, an application of two-photon geometrical optics reported in Ref. 12.
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(1998)
Phys. Rev. A
, vol.57
, pp. R2267
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Monken, C.H.1
Souto Ribeiro, P.H.2
P’adua, S.3
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19
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85037240374
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Ref. 13, the authors report the coincidence/single ratio of (Formula presented) without using interference filters. With beamlike type-II SPDC, some sort of spectral filtering is necessary because dual wavelengths exist at (Formula presented) emission angles
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In Ref. 13, the authors report the coincidence/single ratio of (Formula presented) without using interference filters. With beamlike type-II SPDC, some sort of spectral filtering is necessary because dual wavelengths exist at (Formula presented) emission angles.
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28
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85037220554
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Polarization-entangled state generation scheme shown in Fig. 22, in fact, generates post-selected polarization-entangled states, i.e., the amplitudes (both photons leaving the beamsplitter via the same output port) that do not contribute to a coincidence count are ignored
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Polarization-entangled state generation scheme shown in Fig. 22, in fact, generates post-selected polarization-entangled states, i.e., the amplitudes (both photons leaving the beamsplitter via the same output port) that do not contribute to a coincidence count are ignored.
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