Bose-Einstein condensation and chiral phase transition in linear sigma model
arXiv:hep-th/0501226 · doi:10.1088/0954-3899/31/5/015
Abstract
With the linear sigma model, we have studied Bose-Einstein condensation and the chiral phase transition in the chiral limit for an interacting pion system. A phase diagram including these two phenomena is presented. It is found that the phase plane has been divided into three areas: the Bose-Einstein condensation area, the chiral symmetry broken phase area and the chiral symmetry restored phase area. Bose-Einstein condensation can happen either from the chiral symmetry broken phase or from the restored phase. We show that the onset of the chiral phase transition is restricted in the area where there is no Bose-Einstein condensation.
13 pages, 7 figures
Cited by in corpus (7)
- The Linear Sigma Model and the formation of a charged pion condensate in the presence of an external magnetic field
- The linear sigma model at a finite isospin chemical potential
- Bose-Einstein condensation in linear sigma model at Hartree and large N approximation
- Chiral phase transition in the linear sigma model within Hartree factorization in the Tsallis nonextensive statistics
- The baryon mass calculation in the chiral soliton model at finite temperature and density
- Studying the baryon properties through chiral soliton model at finite temperature and denstity
- Mean-field approximation for the chiral soliton in a chiral phase transition