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Volumn 56, Issue 2, 1997, Pages 1205-1211

Determination of entangled quantum states of a trapped atom

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EID: 0001739379     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.56.1205     Document Type: Article
Times cited : (61)

References (47)
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    • PLRAAN
    • W. Vogel and R. L. de Matos Filho, Phys. Rev. A 52, 4214 (1995). For a treatment of the modifications due to the micromotion in a Paul trap see 24.PLRAAN
    • (1995) Phys. Rev. A , vol.52 , pp. 4214
    • Vogel, W.1    de Matos Filho, R.L.2
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    • PLRAAN
    • Phys. Rev. A 44, 6023 (1991); PLRAAN
    • (1991) Phys. Rev. A , vol.44 , pp. 6023
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    • W. Vogel and D.-G. Welsch, Lectures on Quantum Optics (Akademie Verlag/VCH Publishers, Berlin, 1994).
    • W. Vogel and D.-G. Welsch, Lectures on Quantum Optics (Akademie Verlag/VCH Publishers, Berlin, 1994).
  • 24
    • 8644273627 scopus 로고    scopus 로고
    • PLRAAN
    • Phys. Rev. A 54, 3322 (1996); PLRAAN
    • (1996) Phys. Rev. A , vol.54 , pp. 3322
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    • PHRVAO
    • For the representation of the quasidistributions underlying the method see also K. E. Cahill and R. J. Glauber, Phys. Rev. 177, 1882 (1969); PHRVAO
    • (1969) Phys. Rev. , vol.177 , pp. 1882
    • Cahill, K.E.1    Glauber, R.J.2
  • 45
    • 85037254868 scopus 로고    scopus 로고
    • For a Raman-type excitation the phase (Formula presented) is the difference phase of the two Raman beams and can be held very stable.
    • For a Raman-type excitation the phase (Formula presented) is the difference phase of the two Raman beams and can be held very stable.
  • 46
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    • PRLTAO
    • The selection of no-fluorescence trajectories has also been proposed for stochastic cooling; cf. J. Eschner, B. Appasamy, and P. E. Toschek, Phys. Rev. Lett. 74, 2435 (1995).PRLTAO
    • (1995) Phys. Rev. Lett. , vol.74 , pp. 2435
    • Eschner, J.1    Appasamy, B.2    Toschek, P.E.3


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.