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Volumn 57, Issue 3, 1998, Pages R1477-R1480

Optical simulation of quantum logic

Author keywords

[No Author keywords available]

Indexed keywords

ALGORITHMS; COMPUTER SIMULATION; INTERFEROMETERS; LIGHT POLARIZATION; LOGIC GATES; NONLINEAR OPTICS; OPTICAL BEAM SPLITTERS; OPTICAL DEVICES; OPTICAL KERR EFFECT; OPTICAL ROTATION; PHASE SHIFTERS; PHOTONS;

EID: 0032026235     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.57.R1477     Document Type: Article
Times cited : (334)

References (23)
  • 13
    • 84967846232 scopus 로고
    • Am. J. Phys.A. Zeilinger, 49, 882 (1981);
    • (1981) , vol.49 , pp. 882
    • Zeilinger, A.1
  • 14
    • 0038220551 scopus 로고
    • Am. J. Phys.Z. Y. Ou and L. Mandel, 57, 66 (1989).
    • (1989) , vol.57 , pp. 66
    • Ou, Z.Y.1    Mandel, L.2
  • 15
    • 85037196957 scopus 로고    scopus 로고
    • Here and below, it is understood that the path lengths are adjusted so that the difference between dynamical phases vanishes
    • Here and below, it is understood that the path lengths are adjusted so that the difference between dynamical phases vanishes.
  • 16
    • 85037232924 scopus 로고    scopus 로고
    • This teleportation circuit is equivalent to the one described in G. Brassard, S. L. Braunstein, and R. Cleve (unpublished)
    • This teleportation circuit is equivalent to the one described in G. Brassard, S. L. Braunstein, and R. Cleve (unpublished).
  • 18
    • 85037242270 scopus 로고    scopus 로고
    • For convenience, two realizations (B and (Formula presented)) of the Hadamard gate are used in Fig. 33, where (Formula presented) is obtained from B by interchanging the (Formula presented) and (Formula presented) output ports in Fig. 11(a)
    • For convenience, two realizations (B and (Formula presented)) of the Hadamard gate are used in Fig. 33, where (Formula presented) is obtained from B by interchanging the (Formula presented) and (Formula presented) output ports in Fig. 11(a).
  • 19
    • 85037244250 scopus 로고    scopus 로고
    • A polarizing beam splitter leaves a horizontally polarized photon (in polarization state |0〉) unchanged, while vertical polarization (state |1〉) is reflected
    • A polarizing beam splitter leaves a horizontally polarized photon (in polarization state |0〉) unchanged, while vertical polarization (state |1〉) is reflected.
  • 20
    • 85037210909 scopus 로고    scopus 로고
    • Phase shifts that occur after polarization transformations C (and which must therefore be independent of polarization) could be produced by a calibrated rotation of a thin glass plate
    • Phase shifts that occur after polarization transformations C (and which must therefore be independent of polarization) could be produced by a calibrated rotation of a thin glass plate.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.