2002/12/31 by M. Loewe, C. Villavicencio · 8 citations
Physics and Astronomy · #High-Energy Particle Collisions Research #Isospin #Nuclear physics #Particle physics theoretical and experimental studies #Physics #Pion #Quantum Chromodynamics and Particle Interactions #Thermal #Thermodynamics #hep-ph
paper · pdf · doi:10.1103/physrevd.67.074034
published as Phys.Rev. D67 (2003) 074034 · 13 pages, 5 figures
arxiv created 2003/01/21 · openalex publication_date 2003/04/29 · arxiv updated 2009/11/30 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
The density corrections, in terms of the isospin chemical potential \ensuremathμI, to the mass of the pions are studied in the framework of the SU(2) low-energy effective chiral Lagrangian. The pion decay constant f_\ensuremathπ(T,\ensuremathμI) is also analyzed. As a function of temperature for \ensuremathμI=0, the mass remains quite stable, starting to grow for very high values of T, confirming previous results. However, there are interesting corrections to the mass when both effects (temperature and chemical potential) are simultaneously present. At zero temperature the \ensuremathπ^\ifmmode±\else\textpm\fi should condensate when \ensuremathμI=\ensuremath∓m_\ensuremathπ. This is no longer valid at finite T. The mass of \ensuremathπ0 acquires also a nontrivial dependence on \ensuremathμI due to the finite temperature.