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Nonlinear dynamics of soft boson excitations in hot QCD plasma. 1. Plasmon-plasmon scattering

机译:QCD热等离子体中软玻色子激发的非线性动力学。 1.等离子体激元散射

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On the basis of the pure gauge sector of the Blaizot-lancu equation, we derive a kinetic equation of Boltzmann type, taking into account 2n + 2-colorless plasmon decay processes, n = 1, 2,.... Using the so-called Tsytovich correspondence principle, a direct connection between matrix elements of the plasmon decay processes and a certain effective current, generating these processes, is established. The procedure of calculating a matrix element for the simplest four-plasmon decay is considered comprehensively. The limiting value of, the plasmon occupation number (similar to1/g(2), where g is a strong coupling) wherein all plasmon decays with n greater than or equal to 1 contribute to the right-hand side of the Boltzmann equation, is defined. The iterative method of calculation of matrix elements for higher decay processes (n > 1) is proposed, and a problem of their gauge-invariance is discussed. We proceed from the general reasons the problem of extending the suggested approach to the case of color plasmons is considered. The explicit form of a linearized Boltzmann equation for color plasmons is written out, and it is shown that this equation covariantly conserves the color current, resulting from color-plasmon number density. (C) 2002 Elsevier Science (USA). [References: 36]
机译:基于Blaizot-lancu方程的纯规范扇区,我们考虑了2n + 2无色等离振子衰减过程,n = 1,2,...,推导了Boltzmann型动力学方程。称为Tsytovich对应原理,建立了等离激元衰变过程的矩阵元素与产生这些过程的一定有效电流之间的直接连接。全面考虑了计算最简单的四等离激元衰变的矩阵元素的过程。等离子激元占据数(类似于1 / g(2),其中g是强耦合)的极限值为其中n大于或等于1的所有等离子激元衰变都有助于玻尔兹曼方程的右侧。定义。提出了一种计算高衰减过程(n> 1)的矩阵元素的迭代方法,并讨论了其尺度不变性的问题。我们从一般原因出发,考虑将建议的方法扩展到彩色等离子体激元的情况。写下了线性等离激元的玻尔兹曼方程的显式形式,并且表明该方程协变地保存了由等离激元数密度引起的色电流。 (C)2002 Elsevier Science(美国)。 [参考:36]

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