Understanding of QCD at high density from Z3-symmetric QCD-like theory
Understanding of QCD at high density from Z3-symmetric QCD-like theory
复制标题
从 Z3 对称 QCD 类理论理解高密度 QCD
DOI:
10.1103/physrevd.93.056009
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发表时间:
2015
期刊:
影响因子:
--
通讯作者:
Masanobu Yahiro
中科院分区:
文献类型:
--
作者:
Hiroaki Kouno;Kouji Kashiwa;Junichi Takahashi;Tatsuhiro Misumi;Masanobu Yahiro
We investigate QCD at largeby using-symmetricgauge theory, whereis the quark-number chemical potential andis temperature. We impose the flavor-dependent twist boundary condition on quarks in QCD. This QCD-like theory has the twist angleas a parameter, and agrees with QCD whenand becomes symmetric when. For both QCD and the-symmetricgauge theory, the phase diagram is drawn in–plane with the Polyakov-loop extended Nambu–Jona-Lasinio model. In the-symmetricgauge theory, the Polyakov loopis zero in the confined phase appearing atand. The perfectly confined phase never coexists with the color superconducting (CSC) phase, since finite diquark condensate in the CSC phase breakssymmetry and then makesfinite. When, the CSC phase is more stable than the perfectly confined phase at. Meanwhile, the chiral symmetry can be broken in the perfectly confined phase, since the chiral condensate isinvariant. Consequently, the perfectly confined phase is divided into the perfectly confined phase without chiral symmetry restoration in a region ofandand the perfectly confined phase with chiral symmetry restoration in a region ofand. At low temperature, the basic phase structure of-symmetric QCD-like theory remains in QCD. Properties of the sign problem in-symmetric theory are also discussed. We discuss a numerical framework to evaluate observables atfrom those at.