메뉴 건너뛰기




Volumn 68, Issue 1, 2003, Pages 4-

Quantum interference with beamlike type-II spontaneous parametric down-conversion

Author keywords

[No Author keywords available]

Indexed keywords


EID: 85037204113     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.68.013804     Document Type: Article
Times cited : (11)

References (35)
  • 1
    • 85037192944 scopus 로고    scopus 로고
    • D.N. Klyshko, Photons and Nonlinear Optics (Gordon and Breach, New York, 1988)
    • D.N. Klyshko, Photons and Nonlinear Optics (Gordon and Breach, New York, 1988).
  • 4
    • 85037200789 scopus 로고    scopus 로고
    • 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);
    • 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)
  • 5
    • 15044361457 scopus 로고
    • Phys. Rev. Lett. 61, 2921 (1988).
    • (1988) Phys. Rev. Lett. , vol.61 , pp. 2921
  • 13
    • 85037248663 scopus 로고    scopus 로고
    • 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
    • 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.
  • 16
    • 0000369884 scopus 로고    scopus 로고
    • 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.
    • (1998) Phys. Rev. A , vol.57 , pp. R2267
    • Monken, C.H.1    Souto Ribeiro, P.H.2    P’adua, S.3
  • 19
    • 85037240374 scopus 로고    scopus 로고
    • 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
    • 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.
  • 28
    • 85037220554 scopus 로고    scopus 로고
    • 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
    • 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.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.