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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Online Access: | https://doi.org/10.1140/epjc/s10052-021-09212-7 |
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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 |
work_keys_str_mv |
AT prabaladhikari quarkpionandaxialcondensatesinthreeflavorfiniteisospinchiralperturbationtheory AT jensoandersen quarkpionandaxialcondensatesinthreeflavorfiniteisospinchiralperturbationtheory AT martinamojahed quarkpionandaxialcondensatesinthreeflavorfiniteisospinchiralperturbationtheory |
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