Chiral condensate in hadronic matter

被引:21
作者
Jankowski, J. [1 ]
Blaschke, D. [1 ,2 ,3 ]
Spalinski, M. [4 ,5 ]
机构
[1] Univ Wroclaw, Inst Theoret Phys, PL-50204 Wroclaw, Poland
[2] Univ Bielefeld, Fak Phys, D-33615 Bielefeld, Germany
[3] Joint Inst Nucl Res, Bogoliubov Lab Theoret Phys, RU-141980 Dubna, Russia
[4] Natl Ctr Nucl Res, PL-00681 Warsaw, Poland
[5] Univ Bialystok, Dept Phys, PL-15424 Bialystok, Poland
来源
PHYSICAL REVIEW D | 2013年 / 87卷 / 10期
基金
俄罗斯基础研究基金会;
关键词
RESONANCE GAS; SYMMETRY-BREAKING; QUARK; LATTICE; MASS; SPECTRUM; BARYONS; MODEL;
D O I
10.1103/PhysRevD.87.105018
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
The finite temperature chiral condensate for 2 + 1 quark flavors is considered in the framework of the hadron resonance gas model. This requires some dynamical information, for which two models are employed: one based on the quark structure of hadrons combined with the Nambu-Jona-Lasinio approach to chiral symmetry breaking, and one originating from gauge/gravity duality. Using these insights, hadronic sigma terms are discussed in the context of recent first-principles results following from lattice QCD and chiral perturbation theory. For the condensate, in generic agreement with lattice data it is found that chiral symmetry restoration in the strange quark sector takes place at higher temperatures than in the light quark sector. The importance of this result for a recently proposed dynamical model of hadronic freeze-out in heavy ion collisions is outlined.
引用
收藏
页数:13
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