Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Chapman & Hall/CRC eBooks

Bose-Einstein condensation of ideal Bose gases under external conditions

Published Dec 13, 2001• 0 citations
Publisher
DOI
10.1201/9781420035469.ch9

Related papers

Necessary and sufficient condition for the occurrence of Bose-Einstein condensation in ideal gases

G.S. Rosa

•Jan 1, 1975•0 citations

Multi-step Bose–Einstein condensation of trapped ideal Bose gases

Wenji Deng

arXiv:cond-mat/9809232•Physics Letters A•Sep 1, 1999•4 citations

Bose-Einstein condensation of ideal Bose gases under external conditions

Klaus Kirsten

This chapter focuses on the applications involving finite temperature theories. Technically, the grand canonical partition function is easiest to handle and in general it is the one used for the analysis of the thermodynamical properties. In fact, for properties like the energy and the specific heat of the gas this is justified because in the thermodynamical limit the different ensembles are known to give the same answer. The chapter uses the grand canonical ensemble to obtain properties like critical temperature, energy and specific heat. It summarizes the grand canonical description of ideal Bose gases trapped by magnetic fields and describes the formulation of Bose-Einstein condensation as a symmetry-breaking phenomenon.

Chapman & Hall/CRC eBooks•Dec 13, 2001•0 citations

Bose-Einstein condensation under external conditions

Klaus Kirsten, David J. Toms

arXiv:cond-mat/9804218•Physics Letters A•Jun 1, 1998•42 citations

On the Bose-Einstein condensation of an ideal gas

Lawrence J. Landau, Ivan F. Wilde

Communications in Mathematical Physics•Feb 1, 1979•75 citations

Producing Condition on Bose-Einstein Condensation of Any Dimensional Ideal Bose System

Wu Bo

According to generic relation between particle's energy and momentum,we adopt the common procedure of quanta statistics which firstly work out the grand partition function,the critical temperature and producing condition of any dimensional ideal Bose system.With no external potential and in the thermodynamics condition,it is shown that the producing condition of any dimensional ideal Bose-Einstein Condensation only lies on the size relation between space dimensionality of particle and momentum's index in energy expression,which is a universal conclusion.For it,we can explain no Bose-Einstein Condensation with no external potential and under low dimensional spaces.

Journal of Chongqing University of Science and Technology•Jan 1, 2012•0 citations
This chapter focuses on the applications involving finite temperature theories. Technically, the grand canonical partition function is easiest to handle and in general it is the one used for the analysis of the thermodynamical properties. In fact, for properties like the energy and the specific heat of the gas this is justified because in the thermodynamical limit the different ensembles are known to give the same answer. The chapter uses the grand canonical ensemble to obtain properties like critical temperature, energy and specific heat. It summarizes the grand canonical description of ideal Bose gases trapped by magnetic fields and describes the formulation of Bose-Einstein condensation as a symmetry-breaking phenomenon.
According to generic relation between particle's energy and momentum,we adopt the common procedure of quanta statistics which firstly work out the grand partition function,the critical temperature and producing condition of any dimensional ideal Bose system.With no external potential and in the thermodynamics condition,it is shown that the producing condition of any dimensional ideal Bose-Einstein Condensation only lies on the size relation between space dimensionality of particle and momentum's index in energy expression,which is a universal conclusion.For it,we can explain no Bose-Einstein Condensation with no external potential and under low dimensional spaces.