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Volumn 82, Issue 4, 2010, Pages

Single Cs atoms as collisional probes in a large Rb magneto-optical trap

Author keywords

[No Author keywords available]

Indexed keywords

COHERENT PROBE; COLLISION PARAMETER; FLUORESCENCE DYNAMICS; INDUCED LOSS; INTERSPECIES COLLISIONS; MAGNETOOPTICAL TRAPS; NEUTRAL ATOMS; QUANTUM SYSTEM; STEADY STATE;

EID: 78650955179     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.82.042722     Document Type: Article
Times cited : (20)

References (26)
  • 8
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    • PRLTAO 0031-9007 10.1103/PhysRevLett.63.957
    • A. Gallagher and D. E. Pritchard, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.63.957 63, 957 (1989).
    • (1989) Phys. Rev. Lett. , vol.63 , pp. 957
    • Gallagher, A.1    Pritchard, D.E.2
  • 11
    • 78650962762 scopus 로고    scopus 로고
    • It has been pointed out that the heteronuclear loss rates are not reciprocal, i.e., one cannot a priori assume βi,j′=βj,i′.
    • It has been pointed out that the heteronuclear loss rates are not reciprocal, i.e., one cannot a priori assume β i, j ′ = β j, i ′.
  • 17
    • 78650933950 scopus 로고    scopus 로고
    • The Geiger mode can be used only for photon rates which are smaller than the inverse dead time of 1/35 ns of the APD. Considering the corresponding detection setups the count rates of Rb and Cs are 108/s and 105/s, respectively, thus only allowing to operate the Cs APD in the Geiger mode.
    • The Geiger mode can be used only for photon rates which are smaller than the inverse dead time of 1/35 ns of the APD. Considering the corresponding detection setups the count rates of Rb and Cs are 10 8 /s and 10 5 /s, respectively, thus only allowing to operate the Cs APD in the Geiger mode.
  • 18
    • 78650960240 scopus 로고    scopus 로고
    • For Rb atom numbers less than 700 the statistics is much less, and we average over about 50 traces only. However, this does not influence the analysis of the Rb-Cs interaction parameter, because this is based only on data sets with Rb atom numbers larger than or equal to 1000.
    • For Rb atom numbers less than 700 the statistics is much less, and we average over about 50 traces only. However, this does not influence the analysis of the Rb-Cs interaction parameter, because this is based only on data sets with Rb atom numbers larger than or equal to 1000.
  • 19
    • 78650929574 scopus 로고    scopus 로고
    • While in steady state the histograms are expected to follow a Poissonian distribution, we find that also for non-steady-state conditions our data are very well described by a Poissonian. For simplicity we therefore fit a Poissonian distribution to the data and extract its mean atom number which is shifted toward smaller values for an increasing number of Rb atoms.
    • While in steady state the histograms are expected to follow a Poissonian distribution, we find that also for non-steady-state conditions our data are very well described by a Poissonian. For simplicity we therefore fit a Poissonian distribution to the data and extract its mean atom number which is shifted toward smaller values for an increasing number of Rb atoms.
  • 21
    • 42549143701 scopus 로고    scopus 로고
    • JPAPEH 0953-4075 10.1088/0953-4075/41/3/035303
    • M. L. Harris, P. Tierney, and S. L. Cornish, J. Phys. B JPAPEH 0953-4075 10.1088/0953-4075/41/3/035303 41, 035303 (2008).
    • (2008) J. Phys. B , vol.41 , pp. 035303
    • Harris, M.L.1    Tierney, P.2    Cornish, S.L.3
  • 22
    • 49249091667 scopus 로고    scopus 로고
    • PLRAAN 1050-2947 10.1103/PhysRevA.78.023610
    • H. T. Ng and S. Bose, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.78. 023610 78, 023610 (2008).
    • (2008) Phys. Rev. A , vol.78 , pp. 023610
    • Ng, H.T.1    Bose, S.2
  • 23
    • 33744819428 scopus 로고    scopus 로고
    • NJOPFM 1367-2630 10.1088/1367-2630/8/6/087
    • M. Bruderer and D. Jaksch, New J. Phys. NJOPFM 1367-2630 10.1088/1367-2630/8/6/087 8, 87 (2006).
    • (2006) New J. Phys. , vol.8 , pp. 87
    • Bruderer, M.1    Jaksch, D.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.