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...
Main Authors: | , |
---|---|
Format: | Article |
Language: | English |
Published: |
Elsevier
2020-05-01
|
Series: | Physics Letters B |
Online Access: | http://www.sciencedirect.com/science/article/pii/S0370269320301568 |
id |
doaj-b95f493838064572944e3c4e4b03e799 |
---|---|
record_format |
Article |
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 |
work_keys_str_mv |
AT prabaladhikari qcdatfiniteisospindensitychiralperturbationtheoryconfrontslatticedata AT jensoandersen qcdatfiniteisospindensitychiralperturbationtheoryconfrontslatticedata |
_version_ |
1724690339549151232 |