量子色动力学在有限温度密度区间的相结构(英文)  

QCD PHASE DIAGRAM AT HIGH TEMPERATURE AND DENSITY

作　　者：黄梅[1,2] 

机构地区：[1]中国科学院高能物理研究所,北京100049 [2]中国科学院大科学装置理论物理研究中心,北京100049

出　　处：《物理学进展》2010年第2期217-246,共30页Progress In Physics

基　　金：supported by CAS program"Outstanding young scientists abroad brought-in",CAS key project KJCX3-SYW-N2;NSFC10735040,NSFC10875134;the K.C.Wong Education Foundation, Hong Kong.

摘　　要：本文综述量子色动力学在有限温度密度区间的相结构,包括高密条件下的色超导态和在高温条件下相对论重离子碰撞实验中产生的强耦合夸克-胶子等离子体。我们简要地介绍在相对论重离子碰撞实验中发现强耦合夸克-胶子等离子体的历史,并且讨论用体粘滞系数与熵的比值确定QCD临界点的可能性。对于在高密区域的相结构,我们着重讨论错位配对情况下的非标准色超导态,解释无能隙色超导态的色磁不稳定性、Sarma不稳定性和Higgs不稳定性.This article reviews recent progress of QCD phase structure, including color superconductor at high baryon density and strongly interacting quark-gluon plasma （sQGP） at high temperature created through relativistic heavy ion collision. A brief overview is given on the discovery of sQGP at RHIC. The possibility of locating the critical end point （CEP） from the property of bulk viscosity over entropy density is discussed. For the phase structure at high baryon density, the status of the unconventional color superconducting phase with mismatched pairing is reviewed. The chromomagnetic instability, Sarma instability and Higgs instability in the gapless color superconducting phase are clarified.

关 键 词：强耦合夸克胶子等离子体 QCD临界点 无能隙色超导态 

分 类 号：O572.243[理学—粒子物理与原子核物理]