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Volumn 58, Issue 5, 1998, Pages 3953-3962

Atom cooling and trapping by disorder

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EID: 0000428493     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.58.3953     Document Type: Article
Times cited : (89)

References (28)
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    • North-Holland, Amsterdam
    • P. Beckmann, in Progress in Optics VI, edited by E. Wolf (North-Holland, Amsterdam, 1967), pp. 55–69.
    • (1967) Progress in Optics VI , pp. 55-69
    • Beckmann, P.1
  • 4
    • 77956965782 scopus 로고
    • North-Holland, Amsterdam
    • J. C. Dainty, in Progress in Optics XIV, edited by E. Wolf (North-Holland, Amsterdam, 1977), pp. 1–46.
    • (1977) Progress in Optics XIV , pp. 1-46
    • Dainty, J.C.1
  • 5
    • 85037242344 scopus 로고    scopus 로고
    • Waves Random Media 7, 283 (1997), special issue on wave scattering from rough surfaces and related phenomena, edited by A. A. Maradudin and M. Nieto-Vesperinas; 8, 1 (1998)
    • Waves Random Media 7, 283 (1997), special issue on wave scattering from rough surfaces and related phenomena, edited by A. A. Maradudin and M. Nieto-Vesperinas;8, 1 (1998).
  • 9
    • 85037191730 scopus 로고    scopus 로고
    • G. Grynberg and C. Triché, in Coherent and Collective Interactions of Particles and Radiation Beams, Proceedings of the International School of Physics “Enrico Fermi,” Course CXXXI, Varenna, 1995, edited by A. Aspect, W. Barletta, and R. Bonifacio (ETS Editrice, Pisa, 1996), p. 243
    • G. Grynberg and C. Triché, in Coherent and Collective Interactions of Particles and Radiation Beams, Proceedings of the International School of Physics “Enrico Fermi,” Course CXXXI, Varenna, 1995, edited by A. Aspect, W. Barletta, and R. Bonifacio (ETS Editrice, Pisa, 1996), p. 243.
  • 17
    • 0028494203 scopus 로고
    • OPLEDP
    • In the different context of magneto-optical traps other schemes to achieve 3D cooling and trapping by only two laser beams have been suggested and experimentally demonstrated; see, e.g., C. Chesman et al, Opt. Lett. 19, 1237 (1994).OPLEDP
    • (1994) Opt. Lett. , vol.19 , pp. 1237
    • Chesman, C.1
  • 25
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    • Note that this approximation is justified only in the regime of a friction force linear in velocity, i.e., well below the capture range of the Sisyphus cooling [Eq. (28)]. For very light atoms, where the capture range is rather small, the cooling of hot atoms is much less efficient, and thus the spatial diffusion can be much larger than the value given by Eq. (32)
    • Note that this approximation is justified only in the regime of a friction force linear in velocity, i.e., well below the capture range of the Sisyphus cooling [Eq. (28)]. For very light atoms, where the capture range is rather small, the cooling of hot atoms is much less efficient, and thus the spatial diffusion can be much larger than the value given by Eq. (32).
  • 26
    • 85037226755 scopus 로고    scopus 로고
    • Although we focused this paper on the case of the (Formula presented) configuration, we also made some calculations for the (Formula presented) case. In that situation a Sisyphus cooling occurs in the transverse plane because of the phase and intensity variations of the speckle field. However, the temperature is generally higher than the one found in the (Formula presented) configuration
    • Although we focused this paper on the case of the (Formula presented) configuration, we also made some calculations for the (Formula presented) case. In that situation a Sisyphus cooling occurs in the transverse plane because of the phase and intensity variations of the speckle field. However, the temperature is generally higher than the one found in the (Formula presented) configuration.


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