scholarly journals Bose–Einstein condensation temperature of finite systems

2018 ◽  
Vol 2018 (5) ◽  
pp. 053109 ◽  
Author(s):  
Mi Xie
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.


2000 ◽  
Vol 14 (17n18) ◽  
pp. 645-651 ◽  
Author(s):  
LAUREAN HOMORODEAN

The magnetic susceptibilities of the degenerate (below the Bose–Einstein condensation temperature) and nondegenerate ideal gases of nonrelativistic charged spinless bosons are presented. In both cases, the boson gas is diamagnetic. The magnetic susceptibility of the degenerate boson gas below the Bose–Einstein condensation temperature increases in modulus as the temperature increases. As expected, the magnetic susceptibility of the nondegenerate boson gas decreases in modulus with increasing temperature according to the Curie law in low magnetic fields.


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