包含胶子自耦合的QGP本征激发的非线性频移

用在电磁等离子体中广泛证明有效的导数展开法求解夸克胶子等离子体动力论方程,发现场方程的自作用项对夸克胶子等离子体的非Abelian激发的非线性频移具有非常重要的影响.求解到第三阶,得到了包含胶子自耦合作用的非线性频移的解析表达式,并给出了k=0模式的纯胶子气的非线性频移的数值解.     

产生在夸克–胶子等离子体中的中等质量双轻子的增强

基于一个相对论流体力学模型,在夸克–胶子等离子体中具有中等质量双轻子的产生被研究.由于相边对夸克–胶子等离子体系统演化的影响和产生在RHIC能量的夸克–胶子等离子体系统有高的初始温度,夸克相的贡献变得比强子相互作用的贡献重要得多,甚至能与本底相比较.它表明这样的增强是夸克–胶子等离子体形成的一种信号.     

QGP中胶子的经典输运方程

建立了夸克胶子等离子体中胶子的经典输运方程, 并讨论了它与胶子的量子输运方程以及它与夸克的经典输运方程之间的关系.     

化学非平衡夸克–胶子等离子体中的双轻子产生

研究了正在进行化学平衡的具有有限重子密度的夸克–胶子等离子体系统的演化和双轻子产生.结果发现由于夸克相的寿命随初始夸克化学势的增加而增加,以及其他一些因素,如较高的初始温度、较大的胶子密度和较大的胶子聚变和夸克湮没反应截面,导致热粲夸克对双轻子产生提供了占统治的贡献.这个效应造成中等质量双轻子的重大增强.     

超越阿贝尔优势近似和色等离子体的输运系数计算

给出了一种超越阿贝尔优势近似求解夸克胶子等离子体输运方程的方法，并用它计算了夸克、反夸克等离子体的输运系数，讨论了输运系数的非阿贝尔修正．     

洛伦兹规范条件下对单胶子夸克势的QCD非微扰修正形式

在洛伦兹规范条件下,导出了具有平移不变性的双胶子两点函数真空平均值.利用所获得的双胶子真空期待值,给出了对微扰单胶子交换夸克–夸克势、夸克–反夸克对湮没和夸克–反夸克对激发势的最低阶非微扰QCD修正形式.     

柱形夸克胶子等离子体的2π干涉学检测

在2п干涉学中,对不同的п源2п,关联函数可以是不同的. 如果在相对论重离子碰撞中出现柱形夸克胶子等离子体,п介子将从柱形夸克胶子等离子体表面发射,此时2п关联函数将出现一种特殊的振荡行为.这种振荡行为可以用来探明夸克胶子等离子体的存在性,同时也是相对论重离子碰撞中出现夸克胶子等离子体的一个信号.     

球形夸克-胶子等离子体演化源的π干涉学分析

本文对球形演化的夸克–胶子等离子体膨胀源进行了2π干涉学分析.夸克–胶子等离子体的演化由相对论流体力学和熵密度的物态方程描述,而2πHanbury-Brown-Twiss(HBT)关联函数由量子几率振幅的路径积分公式计算.研究结果表明,由2π干涉学得到的源的空间参量敏感地依赖于π介子发射源的相空间分布,源的膨胀速度导致HBT半径变小,并会改变HBT半径与冻结温度之间的关系.     

极端相对论性原子核碰撞产生的热夸克物质的特征轻子谱

基于相对论性流体力学,我们计算了在极端相对论性原子核碰撞中形成的高温高密夸克-胶子等离子体在衰变过程中产生的特征双轻子谱.我们不但考虑了物质的伴随横向膨胀的纵向膨胀,而且也首先在用相对论性流体力学方程描述膨胀过程时考虑了相变的影响.计算结果已预言,当夸克-胶子等离子体存在时展示的特征现象,从而为实验提供了理论依据.     

在弛豫时间近似下QGP动力论方程中的分布函数

从有碰撞项的QGP动力论方程出发,在色涨落扰动下,利用弛豫时间近似,得到至二级修正的夸克和胶子分布函数,通过数值分析重点讨论了高温低密情况下QGP中成分粒子分布函数的特性,并且由分布函数得到净重子数密度和能量密度.     

QGP Kinetic Equations Beyond the Linear Response Theory

It is shown that the non-Abelian properties? of QGP can be got by studying the kinetic equations for QGP beyond the linear response theory. The non-Abelian interaction of the eigenmodes in QGP is found and two quantities describing the non-Abelian properties of QGP are given.     

Enhancement of Dileptons with Intermediate Masses Produced in QGP

The production of dileptons in the intermediate mass region in QGP has been studied on the basis of a relativistic hydrodynamic model. Due to the influence of the phase boundary on the evolution of the QGP system and the high initial temperature of the QGP produced at RHIC energies, the quark phase contribution is much more important than that from hadronic interactions and even comparable with that from background sources. It is shown that such an enhancement is a signature for the QGP formation.     

Photon polarization as a probe for quark–gluon plasma dynamics

Prospects of measuring polarized photons emitted from a quark–gluon plasma (QGP) are discussed. In particular, the detection of a possible quark spin polarization in a QGP using circularly polarized photons emitted from the plasma is studied. Photons leave the QGP without further interaction and thus provide a primary probe for quark polarization within the QGP. We find that photon polarization cannot solely arise due to a possible QGP momentum space anisotropy, but may be enhanced due to it. In particular, for oblate momentum distributions and high photon energies, quark polarization is efficiently transfered to photon polarization. The role of competing sources of polarized photons in heavy-ion collisions is discussed.     

Introduction to Quark-Gluon plasma

Study of Quark-Gluon plasma (QGP) has been a very active area of research in high energy physics since last four decades. This article gives an elementary introduction to QGP. It covers the motivation to study QGP, its abundance in nature, experimental status, production mechanism, signatures and modelling dynamics. We have discussed the medium effects in QGP in terms of response functions, heavy quark potential and Landau damping. Some other recent approaches are also discussed.     

Refractive index of light and the quark-gluon plasma

The refractive index (RI) of light propagating in a medium of quark-gluon plasma (QGP) is studied. The weakly coupled QGP is studied in the framework of hard-thermal-loop (HTL) perturbation theory, and the strongly coupled one is treated based on the holographic approach. In more realistic setups, the feasibility of observing the optical phenomenon related to the RI of QGP is also discussed.     

Quark gluon plasma

Recent trends in the research of quark gluon plasma (QGP) are surveyed and the current experimental and theoretical status regarding the properties and signals of QGP is reported. We hope that the experiments commencing at relativistic heavy-ion collider (RHIC) in 2000 will provide a glimpse of the QGP formation.     

Vector bosons in heavy-ion collisions at the LHC

Vector bosons become accessible experimental probes in heavy-ion collisions at the LHC. The capabilities of the LHC experiments to perform their measurement are outlined. The focus is given to their utility to study the possible formation and properties of the Quark Gluon Plasma (QGP) in the most central heavy-ion collisions. Their own sensitivity (if any) to the QGP is discussed. Their interest as references to observe multiple QGP sensitive probes is justified.     

欧洲核子研究中心发现新物质形态——夸克胶子等离子体存在的证据

介绍和评述了欧洲核子研究中心（CERN）的相对论重离子碰撞的重要实验结果及其物理解释。碰撞初期形成了高温高密系统。能量密度达到了产生夸克胶子等离子体（QGP）的阈值,低质量双轻子增长、J／ψ反常压低和奇异粒子增长等实验现象可以用形成了QGP来解释。但目前的实验还不足以证明已经产生了QGP。     

Quark—Gluon Plasma in Equilibrium State

The thermodynamic potential of quark-gluon plasma (QGP) in equilibrium state is calculated by finite temperature QCD. The pressure correction of QGP and the critical temperature correction of deconfinement phase transition of hadron are discussed.