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Volumn 82, Issue 3, 2010, Pages

Phase fluctuations in anisotropic Bose-Einstein condensates: From cigars to rings

Author keywords

[No Author keywords available]

Indexed keywords

BOSE-EINSTEIN CONDENSATES; GEOMETRIC LENGTH; PHASE FLUCTUATION; QUANTUM FLUCTUATION; RING GEOMETRY; THERMAL PHASE; TRAP GEOMETRIES; ULTRACOLD ATOMS; ZERO TEMPERATURES;

EID: 77957147153     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.82.033607     Document Type: Article
Times cited : (26)

References (30)
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    • The experimental setup will be discussed in detail elsewhere.
    • The experimental setup will be discussed in detail elsewhere.
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    • The parameter η is similar to the parameter ζ defined for Eq. (5), but includes only the transverse dimensions in the rescaling, whereas ζ includes all three dimensions, in analogy to Ref. [2].
    • The parameter η is similar to the parameter ζ defined for Eq. (5), but includes only the transverse dimensions in the rescaling, whereas ζ includes all three dimensions, in analogy to Ref. [2].
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    • The Bogoliubov spectrum crosses from a linear spectrum over to a quadratic spectrum at the inverse healing length. This motivates the choice of the healing length as a short-range cutoff. This short-range cutoff also appears in the long-range behavior of the correlation function, as the smallest "unit" of the spatial variables, which is characteristic for low-dimenionsal systems.
    • The Bogoliubov spectrum crosses from a linear spectrum over to a quadratic spectrum at the inverse healing length. This motivates the choice of the healing length as a short-range cutoff. This short-range cutoff also appears in the long-range behavior of the correlation function, as the smallest "unit" of the spatial variables, which is characteristic for low-dimenionsal systems.


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