日本語フィールド
著者:河野宏明,三角樹弘,柏浩司,牧山隆洋,佐々木崇宏,八尋正信 読み: コウノ ヒロアキ,ミスミ タツヒロ,カシワ コウジ,マキヤマ タカヒロ,ササキ タカヒロ,ヤヒロ マサノブ題名:Differences and similarities between fundamental and adjoint matters in SU(N) gauge theory発表情報:Physical Review D88 (2013) 016002 巻: 88 号: 1 ページ: 016002-1-016002-14キーワード:量子色力学,クォーク,随伴表現,基本表現概要:We investigate differences and similarities between fundamental fermions and adjoint fermions in
$SU(N)$ gauge theory.
The gauge theory with fundamental fermions possesses $mathbb{Z}_{N}$ 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 $mathbb{Z}_N$ 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 $mathbb{Z}_N$ 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.抄録:We investigate differences and similarities between fundamental fermions and adjoint fermions in
$SU(N)$ gauge theory.
The gauge theory with fundamental fermions possesses $mathbb{Z}_{N}$ 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 $mathbb{Z}_N$ 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 $mathbb{Z}_N$ 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.英語フィールド
Author:Hiroaki Kouno, Tatsuhiro Misumi, Kouji Kashiwa, Takahiro Makiyama, Takahiro Sasaki, Masanobu YahiroTitle:Differences and similarities between fundamental and adjoint matters in SU(N) gauge theoryAnnouncement information:Physical Review D88 (2013) 016002 Vol: 88 Issue: 1 Page: 016002-1-016002-14Keyword:QCD, quark, adjoint representation, fundamental representationAn abstract:We investigate differences and similarities between fundamental fermions and adjoint fermions in
$SU(N)$ gauge theory.
The gauge theory with fundamental fermions possesses $mathbb{Z}_{N}$ 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 $mathbb{Z}_N$ 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 $mathbb{Z}_N$ 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.An abstract:We investigate differences and similarities between fundamental fermions and adjoint fermions in
$SU(N)$ gauge theory.
The gauge theory with fundamental fermions possesses $mathbb{Z}_{N}$ 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 $mathbb{Z}_N$ 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 $mathbb{Z}_N$ 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.