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Volumn 81, Issue 5, 2010, Pages

Particle number fluctuations in a cloven trapped Bose gas at finite temperature

Author keywords

[No Author keywords available]

Indexed keywords

ANALYTICAL SOLUTIONS; ATOM NUMBERS; BOSE GAS; CLASSICAL FIELDS; CRITICAL TEMPERATURES; FINITE TEMPERATURES; HIGH TEMPERATURE; INTERFERENCE EFFECTS; LARGE SYSTEM SIZE; NONINTERACTING ATOMS; PARTICLE NUMBERS; THOMAS-FERMI; THREE DIMENSIONS;

EID: 77953210983     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.81.053623     Document Type: Article
Times cited : (15)

References (33)
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    • ′). Using polar coordinates we obtain I = 1 2 √ α β arctan β - α 2 √ α β. For β > α this is also I = 1 √ α β [π 4 - 1 2 arctan 2 √ α β β - α] = 1 √ α β [π 4 - arctan √ α β].
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    • -1η=j(1/ εj)[(|vj|uj)(\uj|,vj|)+(|uj*|vj*)(vj*|,j*|)] with η=(100-1), see, e.g., Ref. [22].
    • -1η=j(1/ εj)[(|vj|uj)(\uj|,vj|)+(|uj*|vj*)(vj*|,j*|)] with η=(100-1), see, e.g., Ref. [22].


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