Condensed Matter Physics, 2010, vol. 13, No. 2, p. 23003:1-10
DOI:10.5488/CMP.13.23003
Title: The second critical density and anisotropic
generalised condensation
Author(s):
 
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M. Beau
(Université de la Méditerranée and Centre de Physique
Théorique - UMR 6207, Luminy - Case 907, 13288 Marseille,
Cedex 09, France)
,
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V.A. Zagrebnov
(Université de la Méditerranée and Centre de Physique
Théorique - UMR 6207, Luminy - Case 907, 13288 Marseille,
Cedex 09, France) |
In this letter we discuss the relevance of the 3D
Perfect Bose gas (PBG) condensation in extremely elongated vessels
for the study of anisotropic condensate coherence and the
"quasi-condensate". To this end we analyze the case of
exponentially anisotropic (van den Berg) boxes, when there
are two critical densities ρc<ρm for a generalised Bose-Einstein Condensation
(BEC). Here ρc is the standard critical density for
the PBG. We consider three examples of anisotropic geometry: slabs,
squared beams and "cigars" to demonstrate that the
"quasi-condensate" which exists in domain
ρc<ρ<ρm is in fact the
van den Berg-Lewis-Pulé
generalised condensation (vdBLP-GC) of the type III with no
macroscopic occupation of any mode.
We show that for the slab geometry the second critical density
ρm is a threshold between
quasi-two-dimensional (quasi-2D) condensate and the
three dimensional (3D) regime when there is a
coexistence of the "quasi-condensate" with the standard one-mode
BEC.
On the other hand,
in the case of squared beams and "cigars" geometries, critical
density ρm separates quasi-1D and 3D
regimes. We calculate the value of the difference between
ρc, ρm (and between corresponding
critical temperatures Tm, Tc) to show
that the observed space anisotropy of the condensate coherence can
be described by a critical exponent γ(T) related to the
anisotropic ODLRO. We compare our calculations with physical results
for extremely elongated traps that manifest "quasi-condensate".
Key words: anisotropic generalized Bose-condensation, van den
Berg-Lewis-Pule condensation of type III, effect of exponential
anisotropy, the second critical point for the BEC
PACS: 05.30.Jp, 03.75.Hh, 67.40.-w
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