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Volumn 70, Issue 6, 2000, Pages 873-877

Efficient atomic beam splitters based on Talbot array illumination

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EID: 13444276407     PISSN: 09462171     EISSN: None     Source Type: Journal    
DOI: 10.1007/PL00021148     Document Type: Article
Times cited : (3)

References (64)
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    • Baldwin, K.G.H.1
  • 2
    • 0004241917 scopus 로고    scopus 로고
    • Academic Press, New York
    • Two recent overviews on atom interferometry are given in: Atom Interferometry, ed. by P.R. Berman (Academic Press, New York 1997);
    • (1997) Atom Interferometry
    • Berman, P.R.1
  • 23
    • 4244129112 scopus 로고    scopus 로고
    • Phys. Rev. Lett. 81, 5705 (1998)
    • (1998) Phys. Rev. Lett. , vol.81 , pp. 5705
  • 30
    • 0346478362 scopus 로고    scopus 로고
    • A Talbot interferometer based on light gratings is discussed in: B. Rohwedder, M.F. Santos: Phys. Rev. A 61, 023601 (2000)
    • (2000) Phys. Rev. A , vol.61 , pp. 023601
    • Rohwedder, B.1    Santos, M.F.2
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    • Phys. Rev. Lett. 56, 827 (1986);
    • (1986) Phys. Rev. Lett. , vol.56 , pp. 827
  • 41
    • 0031269950 scopus 로고    scopus 로고
    • A combination of the Raman and bichromatic beam splitting ideas has been proposed by E.A. Korsunsky, Y.B. Ovchinmkov: Opt. Commun. 143, 219 (1997)
    • (1997) Opt. Commun. , vol.143 , pp. 219
    • Korsunsky, E.A.1    Ovchinmkov, Y.B.2
  • 46
    • 0001517243 scopus 로고
    • For a concise introduction into the theory of thin atom-optical phase gratings made of light see, for instance, C. Henkel, J.-Y. Courtois, A. Aspect: J. Phys. (France) II 4, 1955 (1994)
    • (1994) J. Phys. (France) II , vol.4 , pp. 1955
    • Henkel, C.1    Courtois, J.-Y.2    Aspect, A.3
  • 47
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    • note
    • 2τ/Δ in order to correctly account for the Gaussian intensity profile of the laser beam producing the standing-wave of light [29]
  • 48
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    • ed. by E. Wolf North-Holland, Amsterdam
    • K. Patorski: In Progress in Optics, Vol. 27, ed. by E. Wolf (North-Holland, Amsterdam 1989)
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    • Patorski, K.1
  • 62
    • 24044521260 scopus 로고    scopus 로고
    • note
    • Equation (8) shows that for any Φ the atomic density at the D/4 plane fluctuates in the [0, 2] range. For |Φ|≤ π/2 only one maximum per grating period arises. Values above the critical parameter |Φ| = π/2 lead to additional maxima


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