scholarly journals Nonuniversal critical quantities from variational perturbation theory and their application to the Bose-Einstein condensation temperature shift

2004 ◽  
Vol 70 (4) ◽  
Author(s):  
Boris Kastening
2003 ◽  
Vol 17 (19) ◽  
pp. 1011-1020 ◽  
Author(s):  
H. Kleinert

Using variational perturbation theory, we calculate the shift in the critical temperature Tcup to five loops to lowest order in the scattering length a and find [Formula: see text], where n is the particle density. Our result is slightly lower than the latest Monte Carlo result (1.32±0.02) an1/3.


Symmetry ◽  
2019 ◽  
Vol 11 (5) ◽  
pp. 603 ◽  
Author(s):  
Vyacheslav I. Yukalov

Particle fluctuations in mesoscopic Bose systems of arbitrary spatial dimensionality are considered. Both ideal Bose gases and interacting Bose systems are studied in the regions above the Bose–Einstein condensation temperature T c , as well as below this temperature. The strength of particle fluctuations defines whether the system is stable or not. Stability conditions depend on the spatial dimensionality d and on the confining dimension D of the system. The consideration shows that mesoscopic systems, experiencing Bose–Einstein condensation, are stable when: (i) ideal Bose gas is confined in a rectangular box of spatial dimension d > 2 above T c and in a box of d > 4 below T c ; (ii) ideal Bose gas is confined in a power-law trap of a confining dimension D > 2 above T c and of a confining dimension D > 4 below T c ; (iii) the interacting Bose system is confined in a rectangular box of dimension d > 2 above T c , while below T c , particle interactions stabilize the Bose-condensed system, making it stable for d = 3 ; (iv) nonlocal interactions diminish the condensation temperature, as compared with the fluctuations in a system with contact interactions.


2001 ◽  
Vol 15 (25) ◽  
pp. 1147-1154 ◽  
Author(s):  
LAUREAN HOMORODEAN

We present the temperature dependences of the magnetic susceptibilities for degenerate (below the Bose–Einstein-condensation temperature) and nondegenerate ideal gases of relativistic charged spinless bosons. The nonrelativistic limits of these laws are also discussed. A comparison with the relativistic electron gas is made.


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