QCD at finite isospin density: Chiral perturbation theory confronts lattice data

We consider the thermodynamics of three-flavor QCD in the pion-condensed phase at nonzero isospin chemical potential (μI) and vanishing temperature using chiral perturbation theory in the isospin limit. The transition from the vacuum phase to a superfluid phase with a Bose-Einstein condensate of cha...

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Main Authors: Prabal Adhikari, Jens O. Andersen
Format: Article
Language:English
Published: Elsevier 2020-05-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269320301568
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spelling doaj-b95f493838064572944e3c4e4b03e7992020-11-25T03:02:18ZengElsevierPhysics Letters B0370-26932020-05-01804QCD at finite isospin density: Chiral perturbation theory confronts lattice dataPrabal Adhikari0Jens O. Andersen1Wellesley College, Department of Physics, 106 Central Street, Wellesley, MA 02481, United States; Department of Physics, Norwegian University of Science and Technology, Høgskoleringen 5, N-7491 Trondheim, NorwayDepartment of Physics, Norwegian University of Science and Technology, Høgskoleringen 5, N-7491 Trondheim, Norway; Niels Bohr International Academy, Blegdamsvej 17, DK-2100 Copenhan, Denmark; Corresponding author at: Department of Physics, Norwegian University of Science and Technology, Høgskoleringen 5, N-7491 Trondheim, Norway.We consider the thermodynamics of three-flavor QCD in the pion-condensed phase at nonzero isospin chemical potential (μI) and vanishing temperature using chiral perturbation theory in the isospin limit. The transition from the vacuum phase to a superfluid phase with a Bose-Einstein condensate of charged pions is shown to be second order and takes place at μI=mπ. We calculate the pressure, isospin density, and energy density to next-to-leading order in the low-energy expansion. Our results are compared with recent high-precision lattice simulations as well as previously obtained results in two-flavor chiral perturbation theory. The agreement between the lattice results and the predictions from three-flavor chiral perturbation theory is very good for μI<200 MeV. For larger values of μI, the agreement between lattice data and the two-flavor predictions is surprisingly good and better than with the three-flavor predictions. Finally, in the limit ms≫mu=md, we show that the three-flavor observables reduce to the two-flavor observables with renormalized parameters. The disagreement between the results for two-flavor and three-flavor χPT can largely be explained by the differences in the measured low-energy constants. Keywords: Chiral perturbation theory, Finite isospin, QCDhttp://www.sciencedirect.com/science/article/pii/S0370269320301568
collection DOAJ
language English
format Article
sources DOAJ
author Prabal Adhikari
Jens O. Andersen
spellingShingle Prabal Adhikari
Jens O. Andersen
QCD at finite isospin density: Chiral perturbation theory confronts lattice data
Physics Letters B
author_facet Prabal Adhikari
Jens O. Andersen
author_sort Prabal Adhikari
title QCD at finite isospin density: Chiral perturbation theory confronts lattice data
title_short QCD at finite isospin density: Chiral perturbation theory confronts lattice data
title_full QCD at finite isospin density: Chiral perturbation theory confronts lattice data
title_fullStr QCD at finite isospin density: Chiral perturbation theory confronts lattice data
title_full_unstemmed QCD at finite isospin density: Chiral perturbation theory confronts lattice data
title_sort qcd at finite isospin density: chiral perturbation theory confronts lattice data
publisher Elsevier
series Physics Letters B
issn 0370-2693
publishDate 2020-05-01
description We consider the thermodynamics of three-flavor QCD in the pion-condensed phase at nonzero isospin chemical potential (μI) and vanishing temperature using chiral perturbation theory in the isospin limit. The transition from the vacuum phase to a superfluid phase with a Bose-Einstein condensate of charged pions is shown to be second order and takes place at μI=mπ. We calculate the pressure, isospin density, and energy density to next-to-leading order in the low-energy expansion. Our results are compared with recent high-precision lattice simulations as well as previously obtained results in two-flavor chiral perturbation theory. The agreement between the lattice results and the predictions from three-flavor chiral perturbation theory is very good for μI<200 MeV. For larger values of μI, the agreement between lattice data and the two-flavor predictions is surprisingly good and better than with the three-flavor predictions. Finally, in the limit ms≫mu=md, we show that the three-flavor observables reduce to the two-flavor observables with renormalized parameters. The disagreement between the results for two-flavor and three-flavor χPT can largely be explained by the differences in the measured low-energy constants. Keywords: Chiral perturbation theory, Finite isospin, QCD
url http://www.sciencedirect.com/science/article/pii/S0370269320301568
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