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Electron-Positron Annihilation Provides Evidence of Three Colors for Quarks

电子-正电子湮灭提供了夸克三种颜色的证据

One of the definitive experiments which supports the quark model is the high energy annihilation of electrons and positrons. The annihilation can produce muon-antimuon pairs or quark-antiquark pairs which in turn produce hadrons. The hadron events are evidence of quark production. The ratio of the number of hadron events to the number of muon events gives a measure of the number of "colors" of the quarks, and the evidence points to five quarks with three colors. With the more recent evidence for the top quark, these experiments provide support for the standard model of six quarks with three colors.

支持夸克模型的一个决定性实验是高能电子与正电子的湮灭。这种湮灭可以产生μ子-反μ子对或夸克-反夸克对,后者进一步产生强子。强子事件是夸克产生的证据。强子事件数与μ子事件数的比值可以衡量夸克的“颜色”数,证据表明有五种夸克,三种颜色。随着顶夸克的最新证据出现,这些实验为标准模型中六种夸克、三种颜色的理论提供了支持。

The models which are evoked to explain the experimental results illustrated below involve the calculated cross-sections for the scattering events. It is helpful that the same type of scattering events, e.g., electron-positron scattering, can yield either two muons (leptons) or a variety of hadron products, any one of which suggests the creation of quarks. The experimental handle is then the relative frequency of the hadron events compared to the muon events. The calculated ratio of the products of the scattering process is the ratio of the cross-sections, and the cross-section σ for each product is proportional to the square of its charge. Therefore the ratio of the products R depends upon the ratio of the squares of the electric charges of the products. The calculated ratio then depends upon the number of types of quark-antiquark pairs which can be produced. So it has the form

用于解释以下实验结果的模型涉及散射事件的计算截面。有助于注意到,同一种散射事件,例如电子-正电子散射,可以产生两种缪子(轻子)或多种强子产物,其中任何一种都暗示了夸克的产生。实验处理则是强子事件与缪子事件的相对频率。计算的散射过程产物比是截面比,每个产物的截面σ与其电荷的平方成正比。因此,产物比R取决于产物电荷平方的比值。计算的比值则取决于可以产生的夸克-反夸克对的种类数。因此,它具有以下形式:

If we use the five quarks which would be available in this energy regime assuming only one color, the u, d, s, c and b quarks, then we get

如果我们假设只有一种颜色,使用在此能量范围内可获得的五种夸克(u、d、s、c 和 b 夸克),则可以得到

which is obviously wrong compared to the experiment. But when we take into account the three colors, we obtain

这显然与实验结果不符。但当我们考虑三种颜色时,却得到了

This produces good agreement with the experimental observations over a wide range of energy when the quantum chromodynamic corrections are applied. Obviously, there is a great deal which is not being said here about the details of the calculations. But hopefully it can be seen that this kind of experimental evidence is a strong check on the standard quark model. It includes the model's charges of 2e/3 and e/3, the five types of quarks, and the three colors.

这在应用量子色动力学修正时,与广泛的能量范围内的实验观测结果相吻合。显然,这里没有详细说明计算的细节。但希望可以看出来,这种实验证据对标准夸克模型是一个强有力的检验。它包括了模型的电荷为2e/3和e/3,五种夸克类型以及三种颜色。
From Particle Data Group, "Review of Particle Properties", Phys. Rev. D45, 1 (1992).

The sixth quark is not seen because the energies used are not sufficient to produce the top-antitop quark pair.

第六种夸克无法被观测到,因为所使用的能量不足以产生顶夸克-反顶夸克对。
从粒子数据组,《粒子性质综述》,《物理》D45, 1 (1992)。
Index

Particle concepts

Reference
Rohlf
Ch. 18
索引 质点 概念 参考 Rohlf 第18章
 
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Jets Provide Evidence for Quark Confinement Models

喷注为夸克禁闭模型提供证据

Deep inelastic scattering experiments provided the evidence that the proton and neutron are made up of three more fundamental particles called quarks . One type of experiment in the proton-antiproton colliders produces jets of mesons which correlate with the models of quark confinement. As visualized in the bag model for quark confinement, an individual quark cannot be pulled free because the energy required to do it is much greater than the pair production energy of a quark-antiquark pair. If in a high energy collision, something scatters directly off one of the constituent quarks, it will give it a high energy. With an energy many times the pair production energy, it will create a jet of quark-antiquark pairs (mesons).

深度非弹性散射实验表明,质子和中子由三个更基本的粒子——夸克——组成。质子—反质子对撞的一类实验产生介子喷注,与夸克禁闭模型的预期相符。按夸克禁闭的袋模型,要把单个夸克拉成自由粒子,所需能量远高于产生夸克—反夸克对的阈值。如果高能碰撞中的粒子直接撞击强子的一个组分夸克,使其获得远高于成对产生阈值的能量,就会形成由夸克—反夸克对构成的介子喷注。
Index

Particle concepts

Reference
Rohlf
Ch. 18
索引 质点 概念 参考 Rohlf 第18章
 
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