Relevance of the axial anomaly at the finite-temperature chiral transition in QCD

被引:85
|
作者
Pelissetto, Andrea [1 ,2 ]
Vicari, Ettore [3 ,4 ]
机构
[1] Univ Roma La Sapienza, Dipartimento Fis, I-00185 Rome, Italy
[2] Ist Nazl Fis Nucl, Sez Roma 1, I-00185 Rome, Italy
[3] Univ Pisa, Dipartimento Fis, I-56127 Pisa, Italy
[4] Ist Nazl Fis Nucl, Sez Pisa, I-56127 Pisa, Italy
来源
PHYSICAL REVIEW D | 2013年 / 88卷 / 10期
关键词
NONUNIVERSAL CRITICAL PHENOMENA; RENORMALIZATION-GROUP; CRITICAL EXPONENTS; SYMMETRY RESTORATION; PHASE-TRANSITIONS; SCALING FUNCTIONS; CRITICAL-BEHAVIOR; GAUGE-THEORIES; LATTICE QCD; LAMBDA LINE;
D O I
10.1103/PhysRevD.88.105018
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We investigate the nature of the finite-temperature chiral transition in QCD with two light flavors, in the case of an effective suppression of the U(1)(A) symmetry breaking induced by the axial anomaly, which implies the symmetry breaking U(2)(L) circle times U(2)(R) -> U(2)(V), instead of S(2)(L) circle times S(2)(R) -> S(2)(V). For this purpose, we perform a high-order field-theoretical perturbative study of the renormalization-group flow of the corresponding three-dimensional multiparameter Landau-Ginzburg-Wilson Phi(4) theory with the same symmetry-breaking pattern. We confirm the existence of a stable fixed point and determine its attraction domain in the space of the bare quartic parameters. Therefore, the chiral QCD transition might be continuous also if the U(1)(A) symmetry is effectively restored at T-c. However, the corresponding universality class differs from the O(4) vector universality class which would describe a continuous transition in the presence of a substantial U(1)(A) symmetry breaking at T-c. We estimate the critical exponents of the U(2)(L) circle times U(2)(R) -> U(2)(V) universality class by computing and analyzing the corresponding perturbative expansions. These results are important to discriminate among the different scenarios for the scaling behavior of QCD with two light flavors close to the chiral transition.
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页数:12
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