2014
DOI: 10.1103/physrevc.89.064905
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Isospin-symmetry breaking and baryon-isospin correlations from the Polyakov–Nambu–Jona-Lasinio model

Abstract: We present a study of the 1+1 flavor system of strongly interacting matter in terms of the Polyakov−Nambu−Jona-Lasinio model. We find that though the small isospin symmetry breaking brought in through unequal light quark masses is too small to affect the thermodynamics of the system in general, it may have significant effect in baryon-isospin correlations and have a measurable impact in heavy-ion collision experiments. PACS numbers: 12.38.Aw, 12.38.Mh, I. INTRODUCTIONSignatures of phases of matter with deconf… Show more

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Cited by 24 publications
(17 citation statements)
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“…On the contrary to what happens at finite baryonic density, systems with finite isospin density does not suffer with the sign problem and hence are easily accessible to lattice QCD based calculations. Initial results of lattice QCD at finite temperature and isospin density appeared in early 2000's [6,7] and they were also investigated by other available techniques, such as chiral perturbation theory (χPT) [8][9][10][11][12][13][14][15][16][17], Hard Thermal Loop perturbation theory (HTLPt) [18], Nambu-Jona-Lasinio (NJL) model [19][20][21][22][23][24][25][26][27][28][29][30][31][32][33][34][35] and its Polyakov loop extended version PNJL [36,37], quark meson model (QMM) [38][39][40][41] and the results were largely in qualitative agreement. However, all of the early lattice QCD calculations have been done considering unphysical pion masses and/or an unphysical flavour content.…”
Section: Introductionmentioning
confidence: 99%
“…On the contrary to what happens at finite baryonic density, systems with finite isospin density does not suffer with the sign problem and hence are easily accessible to lattice QCD based calculations. Initial results of lattice QCD at finite temperature and isospin density appeared in early 2000's [6,7] and they were also investigated by other available techniques, such as chiral perturbation theory (χPT) [8][9][10][11][12][13][14][15][16][17], Hard Thermal Loop perturbation theory (HTLPt) [18], Nambu-Jona-Lasinio (NJL) model [19][20][21][22][23][24][25][26][27][28][29][30][31][32][33][34][35] and its Polyakov loop extended version PNJL [36,37], quark meson model (QMM) [38][39][40][41] and the results were largely in qualitative agreement. However, all of the early lattice QCD calculations have been done considering unphysical pion masses and/or an unphysical flavour content.…”
Section: Introductionmentioning
confidence: 99%
“…In ref. [56] it was shown that though in general a small amount of mass difference between the two light quarks does not affect the thermodynamics of the system much, it might have a significant effect on baryon-isospin correlations. Studies of various thermodynamic quantities and fluctuation and correlations of conserved charges incorporating finite volume effects have been reported in ref.…”
Section: Introductionmentioning
confidence: 99%
“…From this one is able to undestand the presence of m 2 scaling for some correlators. The detail analysis is shown in [9].…”
Section: Off-diagonalmentioning
confidence: 99%