Condensates and pressure of two-flavor chiral perturbation theory at nonzero isospin and temperature

Abstract We consider two-flavor chiral perturbation theory ( $$\chi $$ χ PT) at finite isospin chemical potential $$\mu _I$$ μ I and finite temperature T. We calculate the effective potential and the quark and pion condensates as functions of T and $$\mu _I$$ μ I to next-to-leading order in the low-...

Full description

Bibliographic Details
Main Authors: Prabal Adhikari, Jens O. Andersen, Martin A. Mojahed
Format: Article
Language:English
Published: SpringerOpen 2021-02-01
Series:European Physical Journal C: Particles and Fields
Online Access:https://doi.org/10.1140/epjc/s10052-021-08948-6
id doaj-d1d79724f32b4593923ddaf51669bbb0
record_format Article
spelling doaj-d1d79724f32b4593923ddaf51669bbb02021-02-21T12:43:36ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522021-02-0181211110.1140/epjc/s10052-021-08948-6Condensates and pressure of two-flavor chiral perturbation theory at nonzero isospin and temperaturePrabal Adhikari0Jens O. Andersen1Martin A. Mojahed2Physics Department, Faculty of Natural Sciences and Mathematics, St. Olaf CollegeDepartment of Physics, Norwegian University of Science and TechnologyDepartment of Physics, Norwegian University of Science and TechnologyAbstract We consider two-flavor chiral perturbation theory ( $$\chi $$ χ PT) at finite isospin chemical potential $$\mu _I$$ μ I and finite temperature T. We calculate the effective potential and the quark and pion condensates as functions of T and $$\mu _I$$ μ I to next-to-leading order in the low-energy expansion in the presence of a pionic source. We map out the phase diagram in the $$\mu _I$$ μ I –T plane. Numerically, we find that the transition to the pion-condensed phase is second order in the region of validity of $$\chi $$ χ PT, which is in agreement with model calculations and lattice simulations. Finally, we calculate the pressure to two-loop order in the symmetric phase for nonzero $$\mu _I$$ μ I and find that $$\chi $$ χ PT seems to be converging very well.https://doi.org/10.1140/epjc/s10052-021-08948-6
collection DOAJ
language English
format Article
sources DOAJ
author Prabal Adhikari
Jens O. Andersen
Martin A. Mojahed
spellingShingle Prabal Adhikari
Jens O. Andersen
Martin A. Mojahed
Condensates and pressure of two-flavor chiral perturbation theory at nonzero isospin and temperature
European Physical Journal C: Particles and Fields
author_facet Prabal Adhikari
Jens O. Andersen
Martin A. Mojahed
author_sort Prabal Adhikari
title Condensates and pressure of two-flavor chiral perturbation theory at nonzero isospin and temperature
title_short Condensates and pressure of two-flavor chiral perturbation theory at nonzero isospin and temperature
title_full Condensates and pressure of two-flavor chiral perturbation theory at nonzero isospin and temperature
title_fullStr Condensates and pressure of two-flavor chiral perturbation theory at nonzero isospin and temperature
title_full_unstemmed Condensates and pressure of two-flavor chiral perturbation theory at nonzero isospin and temperature
title_sort condensates and pressure of two-flavor chiral perturbation theory at nonzero isospin and temperature
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2021-02-01
description Abstract We consider two-flavor chiral perturbation theory ( $$\chi $$ χ PT) at finite isospin chemical potential $$\mu _I$$ μ I and finite temperature T. We calculate the effective potential and the quark and pion condensates as functions of T and $$\mu _I$$ μ I to next-to-leading order in the low-energy expansion in the presence of a pionic source. We map out the phase diagram in the $$\mu _I$$ μ I –T plane. Numerically, we find that the transition to the pion-condensed phase is second order in the region of validity of $$\chi $$ χ PT, which is in agreement with model calculations and lattice simulations. Finally, we calculate the pressure to two-loop order in the symmetric phase for nonzero $$\mu _I$$ μ I and find that $$\chi $$ χ PT seems to be converging very well.
url https://doi.org/10.1140/epjc/s10052-021-08948-6
work_keys_str_mv AT prabaladhikari condensatesandpressureoftwoflavorchiralperturbationtheoryatnonzeroisospinandtemperature
AT jensoandersen condensatesandpressureoftwoflavorchiralperturbationtheoryatnonzeroisospinandtemperature
AT martinamojahed condensatesandpressureoftwoflavorchiralperturbationtheoryatnonzeroisospinandtemperature
_version_ 1724257854652678144