Quark, pion and axial condensates in three-flavor finite isospin chiral perturbation theory

Abstract We calculate the light-quark condensate, the strange-quark condensate, the pion condensate, and the axial condensate in three-flavor chiral perturbation theory ( $$\chi $$ χ PT) in the presence of an isospin chemical potential at next-to-leading order at zero temperature. It is shown that t...

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Main Authors: Prabal Adhikari, Jens O. Andersen, Martin A. Mojahed
Format: Article
Language:English
Published: SpringerOpen 2021-05-01
Series:European Physical Journal C: Particles and Fields
Online Access:https://doi.org/10.1140/epjc/s10052-021-09212-7
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spelling doaj-a7918c8147ee45d1a4c3943570b9b34b2021-05-30T11:45:03ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522021-05-0181511210.1140/epjc/s10052-021-09212-7Quark, pion and axial condensates in three-flavor finite isospin chiral perturbation theoryPrabal 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 calculate the light-quark condensate, the strange-quark condensate, the pion condensate, and the axial condensate in three-flavor chiral perturbation theory ( $$\chi $$ χ PT) in the presence of an isospin chemical potential at next-to-leading order at zero temperature. It is shown that the three-flavor $$\chi $$ χ PT effective potential and condensates can be mapped onto two-flavor $$\chi $$ χ PT ones by integrating out mesons with strange-quark content (kaons and eta), with renormalized couplings. We compare the results for the light-quark and pion condensates at finite pseudoscalar source with ( $$2+1$$ 2 + 1 )-flavor lattice QCD, and we also compare the axial condensate at zero pseudoscalar and axial sources with lattice QCD data. We find that the light-quark, pion, and axial condensates are in very good agreement with lattice data. There is an overall improvement by including NLO effects.https://doi.org/10.1140/epjc/s10052-021-09212-7
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
Quark, pion and axial condensates in three-flavor finite isospin chiral perturbation theory
European Physical Journal C: Particles and Fields
author_facet Prabal Adhikari
Jens O. Andersen
Martin A. Mojahed
author_sort Prabal Adhikari
title Quark, pion and axial condensates in three-flavor finite isospin chiral perturbation theory
title_short Quark, pion and axial condensates in three-flavor finite isospin chiral perturbation theory
title_full Quark, pion and axial condensates in three-flavor finite isospin chiral perturbation theory
title_fullStr Quark, pion and axial condensates in three-flavor finite isospin chiral perturbation theory
title_full_unstemmed Quark, pion and axial condensates in three-flavor finite isospin chiral perturbation theory
title_sort quark, pion and axial condensates in three-flavor finite isospin chiral perturbation theory
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2021-05-01
description Abstract We calculate the light-quark condensate, the strange-quark condensate, the pion condensate, and the axial condensate in three-flavor chiral perturbation theory ( $$\chi $$ χ PT) in the presence of an isospin chemical potential at next-to-leading order at zero temperature. It is shown that the three-flavor $$\chi $$ χ PT effective potential and condensates can be mapped onto two-flavor $$\chi $$ χ PT ones by integrating out mesons with strange-quark content (kaons and eta), with renormalized couplings. We compare the results for the light-quark and pion condensates at finite pseudoscalar source with ( $$2+1$$ 2 + 1 )-flavor lattice QCD, and we also compare the axial condensate at zero pseudoscalar and axial sources with lattice QCD data. We find that the light-quark, pion, and axial condensates are in very good agreement with lattice data. There is an overall improvement by including NLO effects.
url https://doi.org/10.1140/epjc/s10052-021-09212-7
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AT jensoandersen quarkpionandaxialcondensatesinthreeflavorfiniteisospinchiralperturbationtheory
AT martinamojahed quarkpionandaxialcondensatesinthreeflavorfiniteisospinchiralperturbationtheory
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