The second critical density and anisotropic generalised condensation
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 a...
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Інститут фізики конденсованих систем НАН України
2010
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| Schriftenreihe: | Condensed Matter Physics |
| Online Zugang: | http://dspace.nbuv.gov.ua/handle/123456789/32089 |
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| Zitieren: | The second critical density and anisotropic generalised condensation / M. Beau, V.A. Zagrebnov // Condensed Matter Physics. — 2010. — Т. 13, № 2. — С. 23003: 1-10. — Бібліогр.: 23 назв. — англ. |
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irk-123456789-320892012-04-09T12:14:35Z The second critical density and anisotropic generalised condensation Beau, M. Zagrebnov, V.A. 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". 2010 Article The second critical density and anisotropic generalised condensation / M. Beau, V.A. Zagrebnov // Condensed Matter Physics. — 2010. — Т. 13, № 2. — С. 23003: 1-10. — Бібліогр.: 23 назв. — англ. 1607-324X PACS: 05.30.Jp, 03.75.Hh, 67.40.-w http://dspace.nbuv.gov.ua/handle/123456789/32089 en Condensed Matter Physics Інститут фізики конденсованих систем НАН України |
| institution |
Digital Library of Periodicals of National Academy of Sciences of Ukraine |
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DSpace DC |
| language |
English |
| description |
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". |
| format |
Article |
| author |
Beau, M. Zagrebnov, V.A. |
| spellingShingle |
Beau, M. Zagrebnov, V.A. The second critical density and anisotropic generalised condensation Condensed Matter Physics |
| author_facet |
Beau, M. Zagrebnov, V.A. |
| author_sort |
Beau, M. |
| title |
The second critical density and anisotropic generalised condensation |
| title_short |
The second critical density and anisotropic generalised condensation |
| title_full |
The second critical density and anisotropic generalised condensation |
| title_fullStr |
The second critical density and anisotropic generalised condensation |
| title_full_unstemmed |
The second critical density and anisotropic generalised condensation |
| title_sort |
second critical density and anisotropic generalised condensation |
| publisher |
Інститут фізики конденсованих систем НАН України |
| publishDate |
2010 |
| url |
http://dspace.nbuv.gov.ua/handle/123456789/32089 |
| citation_txt |
The second critical density and anisotropic generalised condensation / M. Beau, V.A. Zagrebnov // Condensed Matter Physics. — 2010. — Т. 13, № 2. — С. 23003: 1-10. — Бібліогр.: 23 назв. — англ. |
| series |
Condensed Matter Physics |
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| first_indexed |
2025-07-03T12:35:26Z |
| last_indexed |
2025-07-03T12:35:26Z |
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