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

Pure and applied physics

Perturbation Theory at Finite Temperatures

Published Jan 1, 1961• 0 citations
Publisher
DOI
10.1016/b978-1-4832-3066-5.50011-1

Related papers

Perturbation Theory at Finite Temperatures

Wolfgang Nolting

Springer eBooks•Jan 1, 2018•0 citations

Perturbation Theory at Finite Temperatures

Wolfgang Nolting, William Dean Brewer

Springer eBooks•Jan 1, 2009•0 citations

Optimized Perturbation Theory: Finite Temperature Applications

Marcus Benghi Pinto

International Workshop on Relativistic Aspects of Nuclear Physics (RANP)•Sep 1, 2001•0 citations

Finite-temperature second-order many-body perturbation theory revisited

Robin Santra, J. Schirmer

arXiv:1609.00492•Chemical Physics•Aug 5, 2016•32 citations

Perturbation theory in the polaron model at finite temperature

N. N. Bologyubov, V. N. Plechko

Theoretical and Mathematical Physics•Dec 1, 1985•5 citations

Finite-size scaling and the role of the thermodynamic ensemble in the transition temperature of a dilute Bose gas

Erich J. Mueller, Gordon Baym, Markus Holzmann

We study the Bose-Einstein condensation phase transition in a weakly interacting gas through a perturbative analysis of finite systems. In both the grand canonical and the canonical ensembles, perturbation theory suffers from infrared divergences and cannot directly determine the transition temperature in the thermodynamic limit. However, in conjunction with finite-size scaling, perturbation theory provides a powerful calculation tool. Here we use this combination of perturbation theory and scaling to estimate a shift in the transition temperature in the canonical ensemble consistent with grand canonical calculations.

arXiv:cond-mat/0105359•Journal of Physics B Atomic Molecular and Optical Physics•Nov 23, 2001•14 citations
We study the Bose-Einstein condensation phase transition in a weakly interacting gas through a perturbative analysis of finite systems. In both the grand canonical and the canonical ensembles, perturbation theory suffers from infrared divergences and cannot directly determine the transition temperature in the thermodynamic limit. However, in conjunction with finite-size scaling, perturbation theory provides a powerful calculation tool. Here we use this combination of perturbation theory and scaling to estimate a shift in the transition temperature in the canonical ensemble consistent with grand canonical calculations.