Thermal properties of $$\pi $$ π and $$\rho $$ ρ meson
Abstract We computed the pole masses and decay constants of $$\pi $$ π and $$\rho $$ ρ meson at finite temperature in the framework of Dyson–Schwinger equations and Bethe–Salpeter equations approach. Below transition temperature, pion pole mass increases monotonously, while $$\rho $$ ρ meson seems t...
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2020-12-01
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Series: | European Physical Journal C: Particles and Fields |
Online Access: | https://doi.org/10.1140/epjc/s10052-020-08766-2 |
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doaj-517ed9ab76d14f7989e72a7c4ac1c9982020-12-27T12:18:43ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522020-12-0180121910.1140/epjc/s10052-020-08766-2Thermal properties of $$\pi $$ π and $$\rho $$ ρ mesonFei Gao0Minghui Ding1Institut für Theoretische Physik, Universität HeidelbergEuropean Centre for Theoretical Studies in Nuclear Physics and Related Areas (ECT*) and Fondazione Bruno KesslerAbstract We computed the pole masses and decay constants of $$\pi $$ π and $$\rho $$ ρ meson at finite temperature in the framework of Dyson–Schwinger equations and Bethe–Salpeter equations approach. Below transition temperature, pion pole mass increases monotonously, while $$\rho $$ ρ meson seems to be temperature independent. Above transition temperature, pion mass approaches the free field limit of screening mass $$\sim 2\pi T$$ ∼ 2 π T , whereas $$\rho $$ ρ meson is about twice as large as that limit. Pion and the longitudinal projection of $$\rho $$ ρ meson decay constants have similar behaviour as the order parameter of chiral symmetry, whereas the transverse projection of $$\rho $$ ρ meson decay constant rises monotonously as temperature increases. The inflection point of decay constant and the chiral susceptibility get the same phase transition temperature. Though there is no access to the thermal width of mesons within this scheme, it is discussed by analyzing the Gell-Mann-Oakes-Renner (GMOR) relation in medium. These thermal properties of hadron observables will help us understand the QCD phases at finite temperature and can be employed to improve the experimental data analysis and heavy ion collision simulations.https://doi.org/10.1140/epjc/s10052-020-08766-2 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Fei Gao Minghui Ding |
spellingShingle |
Fei Gao Minghui Ding Thermal properties of $$\pi $$ π and $$\rho $$ ρ meson European Physical Journal C: Particles and Fields |
author_facet |
Fei Gao Minghui Ding |
author_sort |
Fei Gao |
title |
Thermal properties of $$\pi $$ π and $$\rho $$ ρ meson |
title_short |
Thermal properties of $$\pi $$ π and $$\rho $$ ρ meson |
title_full |
Thermal properties of $$\pi $$ π and $$\rho $$ ρ meson |
title_fullStr |
Thermal properties of $$\pi $$ π and $$\rho $$ ρ meson |
title_full_unstemmed |
Thermal properties of $$\pi $$ π and $$\rho $$ ρ meson |
title_sort |
thermal properties of $$\pi $$ π and $$\rho $$ ρ meson |
publisher |
SpringerOpen |
series |
European Physical Journal C: Particles and Fields |
issn |
1434-6044 1434-6052 |
publishDate |
2020-12-01 |
description |
Abstract We computed the pole masses and decay constants of $$\pi $$ π and $$\rho $$ ρ meson at finite temperature in the framework of Dyson–Schwinger equations and Bethe–Salpeter equations approach. Below transition temperature, pion pole mass increases monotonously, while $$\rho $$ ρ meson seems to be temperature independent. Above transition temperature, pion mass approaches the free field limit of screening mass $$\sim 2\pi T$$ ∼ 2 π T , whereas $$\rho $$ ρ meson is about twice as large as that limit. Pion and the longitudinal projection of $$\rho $$ ρ meson decay constants have similar behaviour as the order parameter of chiral symmetry, whereas the transverse projection of $$\rho $$ ρ meson decay constant rises monotonously as temperature increases. The inflection point of decay constant and the chiral susceptibility get the same phase transition temperature. Though there is no access to the thermal width of mesons within this scheme, it is discussed by analyzing the Gell-Mann-Oakes-Renner (GMOR) relation in medium. These thermal properties of hadron observables will help us understand the QCD phases at finite temperature and can be employed to improve the experimental data analysis and heavy ion collision simulations. |
url |
https://doi.org/10.1140/epjc/s10052-020-08766-2 |
work_keys_str_mv |
AT feigao thermalpropertiesofpipandrhormeson AT minghuiding thermalpropertiesofpipandrhormeson |
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