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Volumn 79, Issue 6, 2009, Pages

Combination of a magnetic Feshbach resonance and an optical bound-to-bound transition

Author keywords

[No Author keywords available]

Indexed keywords

BOUND-TO-BOUND TRANSITION; DETUNING; EXPERIMENTAL DATA; FESHBACH RESONANCES; HIGH-RESOLUTION SPECTROSCOPY; LASER INTENSITIES; LASER LIGHTS; LOSS RATES; MAGNETIC FESHBACH RESONANCES; MOLECULAR STATE; OPTICAL LATTICES; ORDER OF MAGNITUDE; THEORETICAL MODELS;

EID: 67549127238     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.79.062713     Document Type: Article
Times cited : (34)

References (37)
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    • Autler, S.H.1    Townes, C.H.2
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    • 19644401454 scopus 로고    scopus 로고
    • 10.1103/PhysRevA.70.031601
    • S. Dürr, T. Volz, and G. Rempe, Phys. Rev. A 70, 031601 (R) (2004). 10.1103/PhysRevA.70.031601
    • (2004) Phys. Rev. A , vol.70 , pp. 031601
    • Dürr, S.1    Volz, T.2    Rempe, G.3
  • 33
    • 67549125382 scopus 로고    scopus 로고
    • There is a correlation in the observed line strengths, insofar as almost every resonance with a strong bound-to-bound feature correlates with a fairly strong feature in the photoassociation spectrum. But this does not imply that these lines have a large β. Instead, Eq. 18 shows that ΩR alone (even for β=0) can create a strong loss feature for atoms in state |a illuminated with light resonant with the photoassociation transition as long as Δg is not too large.
    • There is a correlation in the observed line strengths, insofar as almost every resonance with a strong bound-to-bound feature correlates with a fairly strong feature in the photoassociation spectrum. But this does not imply that these lines have a large β. Instead, Eq. 18 shows that ΩR alone (even for β=0) can create a strong loss feature for atoms in state |a illuminated with light resonant with the photoassociation transition as long as Δg is not too large.
  • 37
    • 67549138004 scopus 로고    scopus 로고
    • Here we use a and K2 from Eqs. 15 18. We derived these equations assuming that the sample is Bose condensed which is not the case in a deep optical lattice. But a and K2 express only properties of two-body scattering processes. They are unaffected by the many-body state of the system.
    • Here we use a and K2 from Eqs. 15 18. We derived these equations assuming that the sample is Bose condensed which is not the case in a deep optical lattice. But a and K2 express only properties of two-body scattering processes. They are unaffected by the many-body state of the system.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.