메뉴 건너뛰기




Volumn 66, Issue 5, 2002, Pages 6-

Effect of cold collisions on spin coherence and resonance shifts in a magnetically trapped ultracold gas

Author keywords

[No Author keywords available]

Indexed keywords


EID: 84876773880     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.66.053616     Document Type: Article
Times cited : (7)

References (24)
  • 11
    • 85037246208 scopus 로고    scopus 로고
    • N.F. Ramsey, Molecular Beams (Clarendon Press, Oxford, 1956)
    • N.F. Ramsey, Molecular Beams (Clarendon Press, Oxford, 1956).
  • 13
    • 85037205935 scopus 로고    scopus 로고
    • At (Formula presented) (Formula presented) so interrogation times of 20 ms are acceptable
    • At (Formula presented) (Formula presented) so interrogation times of 20 ms are acceptable.
  • 14
    • 85037185194 scopus 로고    scopus 로고
    • Where (Formula presented) and (Formula presented) 9
    • Where (Formula presented) and (Formula presented) 9.
  • 19
    • 85037243355 scopus 로고    scopus 로고
    • The Thomas-Fermi radius (and to a lesser extent the critical temperature) are of course interaction dependent, and therefore using measurements of these quantities to calibrate densities in order to characterize interaction strengths is somewhat circular. Our directly measured value of (Formula presented) on the other hand, is based predominantly on measured spatial extent of the cloud and on an absolute determination of the absorption depth, and therefore it is only weakly model dependent. We quote the “worst-case corrected value” of (Formula presented) in order to put a reasonable limit on the size of possible systematic errors, and not because we feel it is the preferred value
    • The Thomas-Fermi radius (and to a lesser extent the critical temperature) are of course interaction dependent, and therefore using measurements of these quantities to calibrate densities in order to characterize interaction strengths is somewhat circular. Our directly measured value of (Formula presented) on the other hand, is based predominantly on measured spatial extent of the cloud and on an absolute determination of the absorption depth, and therefore it is only weakly model dependent. We quote the “worst-case corrected value” of (Formula presented) in order to put a reasonable limit on the size of possible systematic errors, and not because we feel it is the preferred value.
  • 21
    • 85037198160 scopus 로고    scopus 로고
    • When we changed the length of the first Ramsey pulse, the second pulse length was also changed such that the two pulses combined to form a (Formula presented) pulse, which gives us the maximum signal to noise
    • When we changed the length of the first Ramsey pulse, the second pulse length was also changed such that the two pulses combined to form a (Formula presented) pulse, which gives us the maximum signal to noise.
  • 22
    • 85037236400 scopus 로고    scopus 로고
    • The quoted chirp limit of (Formula presented) includes a correction to account for a small frequency change associated with decay of total atom number during the measurement time. For each data set the number decay was found by allowing an exponential decay in the fit of the Ramsey fringes (not to be confused with the decay in Ramsey fringe contrast associated with decoherence), resulting in a correction amounting to (Formula presented) on average
    • The quoted chirp limit of (Formula presented) includes a correction to account for a small frequency change associated with decay of total atom number during the measurement time. For each data set the number decay was found by allowing an exponential decay in the fit of the Ramsey fringes (not to be confused with the decay in Ramsey fringe contrast associated with decoherence), resulting in a correction amounting to (Formula presented) on average.
  • 23
    • 85037243008 scopus 로고    scopus 로고
    • Fitting the decay of the integrated transverse magnetization to (Formula presented) the same functional form as we fit to the actual experimental data, gives values typically within 5%, and at worst 12%, of the (Formula presented) time
    • Fitting the decay of the integrated transverse magnetization to (Formula presented) the same functional form as we fit to the actual experimental data, gives values typically within 5%, and at worst 12%, of the (Formula presented) time.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.