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Volumn 80, Issue 3, 2009, Pages

Density ripples in expanding low-dimensional gases as a probe of correlations

Author keywords

[No Author keywords available]

Indexed keywords

ANALYTICAL EXPRESSIONS; ANALYTICAL RELATIONS; BALLISTIC EXPANSION; BEREZINSKII-KOSTERLITZ-THOULESS TRANSITION; BKT TRANSITION; BOSE GAS; CONFINED SYSTEMS; CORRELATION FUNCTION; DENSITY FLUCTUATION; FIRST-ORDER; QUANTUM FLUCTUATION; SELF-SIMILAR; SHAPE-CONTROLLED; TRANSVERSE CONFINEMENT; TWO-POINT; ULTRA-COLD;

EID: 70249151041     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.80.033604     Document Type: Article
Times cited : (121)

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    • Note an extra factor 1 2 in front of the mass in Eq. 16, in contrast to Eq. 10.
    • Note an extra factor 1 2 in front of the mass in Eq. 16, in contrast to Eq. 10.
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    • One should note that, strictly speaking, | ρ (q) | 2 does not have to be positive since it is not an expectation value of a positive operator. According to our definition [Eq. 22] square of the operator dxexp (iqx) ψ † (x,t) ψ (x,t) differs from L | ρ (q) | 2 by a term which arises due to normal ordering present in the definition of g2 (x;t).
    • One should note that, strictly speaking, | ρ (q) | 2 does not have to be positive since it is not an expectation value of a positive operator. According to our definition [Eq. 22] square of the operator dxexp (iqx) ψ † (x,t) ψ (x,t) differs from L | ρ (q) | 2 by a term which arises due to normal ordering present in the definition of g2 (x;t).
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    • Constant -1 in Eq. 52 is included for the convenience to make the integrand vanish at ry →, and its contribution disappears after integration over rx.
    • Constant -1 in Eq. 52 is included for the convenience to make the integrand vanish at ry →, and its contribution disappears after integration over rx.
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