论文标题
QCD基态和单数Gluon提交的真正动力学和量规结构
True Dynamical and Gauge Structures of the QCD Ground State and the Singular Gluon Fileds
论文作者
论文摘要
我们令人信服地认为,QCD基态的真正动力学和仪表结构比其Lagrangian精确规格对称性的复杂得多。这些并发症的动态来源已被t ta tadpole/seagull术语鉴定出来,该术语称为质量间隙。它的真正动力作用隐藏在QCD的基础状态中,但它明确地存在于完整的gluon自我能源中。为了披露它的全gluon自我能源的横向条件之间的分裂及其减法对应物。给出了由于质量差距的全Gluon传播器的运动方程,该方程允许通过新引入的广义量规固定动力学和规格结构。一种新型的非扰动分析方法,也为QCD及其Groud状态开发了质量差距方法。我们已经发现了一个普通的,非扰动的单数解,用于在整个Gluon动量范围内有效的完整Gluon繁殖物,同时在所有其他可能的解决方案上以较大的距离占主导地位。它适合所有严重的红外奇异点,由于无质量的gluon模式的自我交往,它们可能出现在QCD基态。已经制定了相应的非替代红外重新规定计划。由此产生的全gluon传播器可防止胶子出现在物理状态(颜色粘合剂的限制)中。我们的方法还解释了渐近自由制度中的规模违规,以及为什么重夸克之间的潜力不断增加只是线性的。
We convincingly argue that the true dynamical and gauge structure of the QCD ground state is much more complicated than its Lagrangian exact gauge symmetry supposes to be. The dynamical source of these complications has been identified with the tadpole/seagull term, which renormalized version called, the mass gap. Its true dynamical role is hidden in the QCD ground state, but it is explicitly present in the full gluon self-energy. To disclose it the splintering between the transverse conditions for the full gluon self-energy and its subtracted counterpart has been derived. The equation of motion for the full gluon propagator on account of the mass gap was given, which allows to fix the dynamical and gauge structures by a newly-introduced generalized gauge. A novel non-perturbative analytical method, the mass gap approach was developed for QCD and its groud state as well. We have discovered a general, non-perturbative singular solution for the full gluon propagator valid in the whole gluon momentum range, while dominating at large distances over all the other possible solutions. It accommodates all the severe infrared singularities, which may appear in the QCD ground state due to the self-interaction of massless gluon modes. A corresponding non-pertubative multiplicative infrared renormalization program has been formulated. The resulting full gluon propagator prevents gluons to appear at large distances as physical states (confinement of color gluons). Our approach also explains the scale violation in the asymptotic freedom regime, and why the rising potential between heavy quarks is only linear one.