LIQUID HELIUM AND THE PROPERTIES OF FINITE BOSE–EINSTEIN ASSEMBLIES

1966 ◽  
Vol 44 (1) ◽  
pp. 27-43 ◽  
Author(s):  
D. F. Goble ◽  
L. E. H. Trainor

In order to explain certain properties of thin helium films, Ziman has proposed an ideal gas model in which the bulk liquid is treated as a collection of independent, Bose–Einstein assemblies each a few hundred angstroms in extent. In this paper, an extensive numerical study is made of the thermodynamic properties of such finite assemblies. In particular, the specific heats of thin films have been calculated on the basis of the model and the results compared with the experimental data of Frederikse. It is found that the model predicts a shift of the specific-heat maxima to higher temperatures as the film thickness is decreased, rather than to lower temperatures as required by the observations on actual helium films. The nature of the Bose–Einstein condensation in finite assemblies is discussed in some detail and some general conclusions are drawn concerning Ziman's model.

2018 ◽  
Vol 182 ◽  
pp. 02066
Author(s):  
Evgeni E. Kolomeitsev ◽  
Maxim E. Borisov ◽  
Dmitry N. Voskresensky

We consider a non-ideal hot pion gas with the dynamically fixed number of particles in the model with the λφ4 interaction. The effective Lagrangian for the description of such a system is obtained by dropping the terms responsible for the change of the total particle number. Within the self-consistent Hartree approximation, we compute the effective pion mass, thermodynamic characteristics of the system and identify a critical point of the induced Bose-Einstein condensation when the pion chemical potential reaches the value of the effective pion mass. The normalized variance, skewness, and kurtosis of the particle number distributions are calculated. We demonstrate that all these characteristics remain finite at the critical point of the Bose-Einstein condensation. This is due to the non-perturbative account of the interaction and is in contrast to the ideal-gas case.


1967 ◽  
Vol 35 (12) ◽  
pp. 1154-1158 ◽  
Author(s):  
A. Casher ◽  
M. Revzen

2000 ◽  
Vol 14 (04) ◽  
pp. 405-409 ◽  
Author(s):  
LUCA SALASNICH

We discuss the Bose–Einstein condensation (BEC) for an ideal gas of bosons in the framework of Tsallis's nonextensive statistical mechanics. We study the corrections to the st and ard BEC formulas due to a weak nonextensivity of the system. In particular, we consider three cases in the D-dimensional space: the homogeneous gas, the gas in a harmonic trap and the relativistic homogenous gas. The results show that small deviations from the extensive Bose statistics produce remarkably large changes in the BEC transition temperature.


JETP Letters ◽  
1997 ◽  
Vol 66 (8) ◽  
pp. 598-604
Author(s):  
V. A. Alekseev ◽  
V. V. Klimov ◽  
D. D. Krylova

2001 ◽  
Vol 15 (09) ◽  
pp. 1253-1256 ◽  
Author(s):  
LUCA SALASNICH

In a recent paper1 we discussed the Bose–Einstein condensation (BEC) in the framework of Tsallis's nonextensive statistical mechanics. In particular, we studied an ideal gas of bosons in a confining harmonic potential. In this memoir we generalize our previous analysis by investigating an ideal Bose gas in a generic power-law external potential. We derive analytical formulas for the energy of the system, the BEC transition temperature and the condensed fraction.


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