Differences and similarities between fundamental and adjoint matters in SU(N) gauge theories

被引:28
|
作者
Kouno, Hiroaki [1 ]
Misumi, Tatsuhiro [2 ,3 ]
Kashiwa, Kouji [4 ]
Makiyama, Takahiro [1 ]
Sasaki, Takahiro [5 ]
Yahiro, Masanobu [5 ]
机构
[1] Saga Univ, Dept Phys, Saga 8408502, Japan
[2] Keio Univ, Dept Phys, Yokohama, Kanagawa 2238521, Japan
[3] Keio Univ, Res & Educ Ctr Nat Sci, Yokohama, Kanagawa 2238521, Japan
[4] Brookhaven Natl Lab, RIKEN BNL, Upton, NY 11973 USA
[5] Kyushu Univ, Dept Phys, Grad Sch Sci, Fukuoka 8128581, Japan
来源
PHYSICAL REVIEW D | 2013年 / 88卷 / 01期
关键词
CHIRAL-SYMMETRY RESTORATION; THERMODYNAMICS; BREAKING; PHASE; MODEL;
D O I
10.1103/PhysRevD.88.016002
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We investigate differences and similarities between fundamental fermions and adjoint fermions in SU(N) gauge theory. The gauge theory with fundamental fermions possesses Z(N) symmetry only in the limit of infinite fermion mass, whereas the gauge theory with adjoint fermions does have the symmetry for any fermion mass. The flavor-dependent twisted boundary condition (FTBC) is then imposed on fundamental fermions so that the theory with fundamental fermions can possess Z(N) symmetry for any fermion mass. We show similarities between FTBC fundamental fermions and adjoint fermions, using the Polyakov-loop extended Nambu-Jona-Lasinio (PNJL) model. In the mean-field level, the PNJL model with FTBC fundamental fermions has dynamics similar to the PNJL model with adjoint fermions for the confinement-deconfinement transition related to Z(N) symmetry. The chiral property is somewhat different between the two models, but there is a simple relation between chiral condensates in the two models. As an interesting high-energy phenomenon, a possibility of the gauge symmetry breaking is studied for FTBC fundamental fermions.
引用
收藏
页数:14
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