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Volumn 79, Issue 3, 2009, Pages

Nonlinear dynamics of a cigar-shaped Bose-Einstein condensate in an optical cavity

Author keywords

[No Author keywords available]

Indexed keywords

DYNAMICS; STABILITY; STEAM CONDENSERS;

EID: 62849101856     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.79.033401     Document Type: Article
Times cited : (77)

References (42)
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    • Terms such as c1† c1† c0 c0 are energetically detuned, and thus play a relatively minor role if the chemical potential of the condensate is much smaller than the energy detuning, i.e., μ= (3gω/4) 2/3 4.
    • Terms such as c1† c1† c0 c0 are energetically detuned, and thus play a relatively minor role if the chemical potential of the condensate is much smaller than the energy detuning, i.e., μ= (3gω/4) 2/3 4.
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    • In one dimension, in contrast to that in three dimension, the weaker the harmonic potential, the better the Thomas-Fermi approximation.
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    • Actually, Fig. 3 may also be plotted with nst versus the maximal photon number nm = η∼ 2 / κ∼ 2. By definition in Eq. 12, Zs is a function of nst and so is Zs† H2 Zs, which we denote as f (nst). To the lowest order, f (nst) is linear in nst, f (nst) =β nst. From Eq. 10, we then have nm = nst [1+ (Δ∼ c′ +4Nβ nst) 2 / κ∼ 2], which can be mapped exactly to the input-output relation in the discussion of dispersive optical bistability; see 3rd ed. (Springer-Verlag, Berlin
    • Actually, Fig. 3 may also be plotted with nst versus the maximal photon number nm = η∼ 2 / κ∼ 2. By definition in Eq. 12, Zs is a function of nst and so is Zs† H2 Zs, which we denote as f (nst). To the lowest order, f (nst) is linear in nst, f (nst) =β nst. From Eq. 10, we then have nm = nst [1+ (Δ∼ c′ +4Nβ nst) 2 / κ∼ 2], which can be mapped exactly to the input-output relation in the discussion of dispersive optical bistability; see P. Meystre and M. Sargent III, Elements of Quantum Optics, 3rd ed. (Springer-Verlag, Berlin, 1999).
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.