带护送概率的Tsallis统计中的强子横向动量分布

Alexandru S. Parvan
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引用次数: 0

摘要

摘要:本文推导了具有护航概率的Tsallis统计(Tsallis-3统计)框架下粒子的费米-狄拉克、玻色-爱因斯坦和麦克斯韦-玻尔兹曼统计的精确和近似强子横动量分布。得到了第0项近似中的经典和量子横向动量分布,以及在第0项近似中引入的因式分解近似中的量子横向动量分布。在Tsallis-3、Tsallis-2和$q$-对偶统计中,第0项近似和第0项近似的因式分解近似的横向动量分布相同。著名的经典现象学Tsallis分布与经典的Tsallis-3统计量的横动量分布在零项近似中完全吻合,该近似中系统在整个状态变量范围内的熵为零。然而,量子现象学的Tsallis分布与Tsallis-3统计量的精确或近似横向动量分布并不一致。应用精确的Tsallis-3经典分布和经典现象学的Tsallis分布来描述高能质子-质子碰撞产生的带电介子的实验光谱。这两种模型分布的参数$(T,q)$的值在整个能量范围内是不同的。因此,经典现象学的Tsallis分布对于Tsallis-3统计量的经典横向动量分布是一个不能令人满意的近似。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Hadron transverse momentum distributions in the Tsallis statistics with escort probabilities
Abstract The exact and approximate hadron transverse momentum distributions for the Fermi-Dirac, Bose-Einstein and Maxwell-Boltzmann statistics of particles in the framework of the Tsallis statistics with escort probabilities (the Tsallis-3 statistics) have been derived. The classical and quantum transverse momentum distributions in the zeroth term approximation and the quantum transverse momentum distributions in the factorization approximation introduced in the zeroth term approximation were found. The transverse momentum distributions in the zeroth term approximation and in the factorization approximation of the zeroth term approximation are the same in the Tsallis-3, Tsallis-2 and $q$-dual statistics. The well-known classical phenomenological Tsallis distribution exactly coincides with the classical transverse momentum distribution of the Tsallis-3 statistics in the zeroth term approximation for which the entropy of system is zero in the whole range of state variables. However, the quantum phenomenological Tsallis distribution does not coincide with either the exact or approximate transverse momentum distributions of the Tsallis-3 statistics. The exact Tsallis-3 classical distribution and the classical phenomenological Tsallis distribution were applied to describe the experimental spectra of the charged pions produced in the proton-proton collisions at high energies. The values of the parameters $(T,q)$ for both these model distributions differ in the whole energy range. Thus, the classical phenomenological Tsallis distribution is an unsatisfactory approximation for the exact classical transverse momentum distribution of the Tsallis-3 statistics.
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