胶子的极化态与ξ(2230)的胶子球解释

本文讨论了当胶子只有横极化分量时对ξ(2230)胶子球解释的影响.     

Pomeron的结构和胶球的强生机制

首先强调了在高能强作用软(高强软)过程,特别是在强子散射总截面中,单由Pomeron(IP)交换就渐进地饱和了幺正性条件这件事的重要性.结合对Landshoff和Nachtmann的IP场论模型适当修改,提出了最大非微扰强作用反应假说.与此相关,认为IP由这种反应中得出的一对共轭色八重态胶团组成.通过对修改后的q-q弹性振幅虚部图形的物理内涵的考察,一方面预言了高强软过程中会产生组分胶子,胶球态是由两个对撞的组分胶子熔合所形成.另一方面,通过这里的色胶团单圈图与Gell-mann-Zweig的介子散射时夸克图的对应,论证了IP与胶球态之间存在着Regge极点型的二元性关系.     

坡密子和胶子球

讨论了高能强子 -强子散射过程中的坡密子以及坡密子的 QCD内容 .认为坡密子有可能就是具有量子数 IG=0 + ,JPC=2 + +的张量胶子球 ξ( 2 2 30 ) .用雷其化胶子球模型计算了高能质子 -质子散射截面和坡密子 -核子的耦合参数 β.理论结果与实验的要求一致. The pomeron in high energy hadron hadron scattering as well as the QCD nature of the pomeron are discussed. We claimed that the pomeron may be the tenser glueball ξ(2 230) with quantum number I G =0 +, J PC =2 ++ . Under this reggeized glueball model the cross section of high energy proton proton scattering and the coupling parameter of the pomeron nucleon, β , are calculated. The theoretical results of the present model are in good agreement with experimental data.     

ξ(2230)的胶子球解释

本文讨论了ξ(2230)作为胶子球解释的可能性.螺旋性振幅之比x和y的理论值与实验值的比较表明,ξ(2230)不可能是一个纯的2⁺⁺S波(或D波)的胶子球,但可能是一个4⁺⁺D波胶子球.     

关于软坡密子的张量胶子球的内涵

通过把坡密子的轨迹跟观察到的量子数I^GJ^PC=0⁺2⁺⁺的同位旋标量的张量介子联系起来的关系,研究了坡密子的胶子球内涵.这些介子中有四个满足坡密子的自旋和质量的关系.这些坡密子的后选者可能是混合态.其中,f₂(2220)有极大的胶子球分量.讨论了关于这个介子宽度的实验争论,预言了它的理论下限,也阐明了在pp实验研究中观察不到f₂(2220)原因.     

关于软坡密子可能的胶子球本质(英文)

通过把坡密子与观察到的量子数为 IGJPC=0+2++的同位旋张量介子联系起来的思想, 研究了坡密子的胶子内涵。 有4个由胶子组成的这样的介子都满足坡密子自旋与质量的关系。 这些坡密子的候选者可能是混杂态。 它们其中之一 f2(2 220)介子可能包含着最大的胶子球成分。 阐明了实验上还不清楚的关于这个介子宽度的问题, 并给出了它的理论下限。 也说明为什么这个介子没有在p实验中发现的原因。 We study the gluonic content of the Pomeron through relating the Pomeron trajectory to the observed IGJPC=0+2++ isoscalar tensor mesons. Four of these mesons satisfy the spin mass relation of the Pomeron. These Pomeronian candidates may be hybrid states. One of them, the f2(2 220) meson, can have a predominant glueball component. We address the unsettled experimental situation about the width of this meson and give a theoretical lower bound for it. We also show why this meson has not been seen in p experiments.     

Υ的三胶子碎裂

至今,只有Lund模型能定性说明Υ三胶子碎裂的高重子产额,却没有一个模型能定量解释ARGUS组的精密测量结果.本文把我们成功解释了e⁺e^－→qq→2jet的夸克产生律与组合律,取代Lund弦碎裂模型,直接用到Υ→3g的色弦上.发现不附加任何参数,即与ARGUS的结果符合得很好.     

双胶子交换模型中J/ψ的衍射产生

利用双胶子交换模型并结合重夸克偶素的色八重态产生机制,计算了π与p碰撞过程中J/ψ的衍射产生总截面.结果发现:随着质心系能量的增加,J/ψ衍射产生的总截面逐渐增大;并且,不同的π介子中的胶子分布函数给出的总截面偏离也逐渐加大.计算结果与未来的实验数据比较,可以检验π介子中的胶子分布函数及双胶子交换模型.     

φ Electro-production in Pomeron Exchange Model

Based on the Pomeron exchange model, elastic production of φ meson in electron-proton interaction is investigated with both linear and non-linear Pomeron trajectories. The numerical calculations of the differential cross section for e p → e‘ p φ are performed. The theoretical predictions show that the dependence of the differentialcross section on virtual photon virtuality, Q2, is of moderation, the change of the energy scale parameter so causes moderate effect on the differential cross section, and the linear trajectory is a good approximation to non-linearity of the Pomeron trajectory, in particular, at small momentum transfer region | t |≤ 0.2 GeV2.     

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.     

Gluonic Origin and Glueball Nature of Pomeron

The Pomeron-nucleon coupling vertex is theoretically derived from the fundamental theory of strong interaction QCD. The empirical vertex βγ^μF1 （t） used commonly in diffractive processes with a coupling strength β = 6.0 GeV^-1 is initially obtained from QCD theoretically. Our study not only reproduces the Pomeron-nucleon coupling from QCD but also clearly shows the gluonlc origin and glueball nature of Pomeron, which is a longstanding puzzle. From this investigation, we claim that Pomeron can be regarded as a Reggeized tensor glueball ζ（2230） with quantum numbers of I^GJ^PC = 0＋2＋＋. Since the tensor glueball ζ（2230） lies on the Pomeron trajectory αp（t = Mζ^2） = 2, the longstanding puzzle that no physical particle lies on the Pomeron trajectory, αp（t） = 1.08 ＋ 0.20 GeV^-2 .t, seems to be solved.     

在量子色动力学中坡密子与核子的耦合

用强相互作用的基本理论量子色动力学推导出了坡密子与核子的耦合顶点, 得到了在绕射过程的研究中广泛应用的, 耦合强度,β=6.0GeV^—1,的经验的耦合顶点,βγ^μF¹(t). 本研究也清楚地表明了坡密子的胶子起源和胶子球的粒子性本质, 这是一个长期没有解决的问题. 结合我们以前的研究结果, 我们认为坡密子可能是一个在雷其轨迹,α(t)=1.08+0.20GeV^－2t,上, 具有量子数,I^G J^PC = 0⁺2⁺⁺,的雷其化的张量胶子球. 所以在雷其轨迹没有物理粒子的困难似乎得到了解决.     

关于软玻密子的结构

本文修改了Landshoff-Nachtmann的软玻密子(Pomeron P)场论模型.从强子组分夸克具有结构的观点出发,根据高能强作用软过程中的最大非微扰强作用反应假定,提出了有关软P新的结构图像.对撞强子中的一对组分夸克被分解为裸夸克和一系列非微扰胶子(和夸克对).与此相应,软P的结构是由胶子形成的一系列切割梯形图之和所代表.在系统能量s很大而动量转移|t|很小的多重雷吉(Regge)运动学区间,并在保留lns的领头阶近似下,计算了这组切割梯形图之和所对应的散射振幅和总截面.它们的表达式出现了对s的Regge型幂次因子,得出了软P轨迹的简洁表达式.简单说明了按本文提出的方案可以讨论那些相关的强作用过程.     

Reggeon, Pomeron and Glueball, Odderon-Hadron-Hadron Interaction at High Energies - From Regge Theory to Quantum Chromodynamics

Based on analysis of scattering matrix S, and its properties such as analyticity, unitarity, Lorentz invariance, and crossing symmetry relation, the Regge theory was proposed to describe hadron-hadron scattering at high energies before the advent of QCD, and correspondingly a Reggeon concept was born as a mediator of strongly interaction. This theory serves as a successful approach and has explained a great number of experimental data successfully, which proves that the Regge theory can be regarded as a basic theory of hadron interaction at high energies and its validity in many applications. However, as new experimental data come out, we have some difficulties in explaining the data. The new experimental total cross section violates the predictions of Regge theory, which shows that Regge formalism is limited in its applications to high energy data. To understand new experimental measurements, a new exchange theory was consequently born and its mediator is called Pomeron, which has vacuum quantum numbers. The new theory named as Pomeron exchange theory which reproduces the new experimental data of diffractive processes successfully. There are two exchange mediators： Reggeon and Pomeron. Reggeon exchange theory can only produce data at the relatively lower energy region, while Pomeron exchange theory fits the data only at higher-energy region, separately. In order to explain the data in the whole energy region, we propose a Reggeon-Pomeron model to describe high-energy hadron- hadron scattering and other diffractive processes. Although the Reggeon-Pomeron model is successful in describing high-energy hadron-hadron interaction in the whole energy region, it is a phenomenological model. After the advent of QCD, people try to reveal the mystery of the phenomenological theory from QCD since hadron-hadron processes is a strong interaction, which is believed to be described by QCD. According to this point of view, we study the QCD nature of Reggeon and Pomeron. We claim that the Reggeon exchange is an exchange of mult     

Gluonic Origin and Glueball Nature of Pomeron

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Coupling Vertex of the Pomeron to Nucleon in QCD

The coupling vertex of the Pomeron to nucleon is derived from QCD. A γμ coupling vertex and coupling strength of β＝ 6.0 GeV-1, which has been used commonly as a free parameter in literature, are obtained. The result leads a support to the belief that the Pomeron could be a tensor glueball ξ(2230) with quantum numbers of IGJPC ＝ 0+2++ in nature.     

关于P的结构模型(部分子分布)的检验

用不同的P部分子模型计算了高能P+P(P)对撞中双重P交换对J/ψ产生过程的贡献.对以胶子为主的Ingelman-Schlein模型,高能时截面随能量s以Ins或In²S平稳增加.在TeV能区σ(S)～10²—10³nb.对于认为P类似于C=+1同位旋标量光子的Donnachie-Landshoff模型,截面随行为复杂些,而σ(S)值仅为1—3nb,比前者小2—3个量级.因此如果认为两模型采用的参数值可靠,则此过程是检验它们的有效方法.文章就此作了质疑式的简短讨论.