摘要
在假定有质量的组分胶子是介子的构成子之一的基础上, 根据 Lorentz 群与 S U( Nc) 色群的分析,构造了基态 J P= 1- 介子的波函数, 分析了基态1- 介子中 ρ±、κ±、ρ0 、ω和 ф介子的磁矩与自旋结构(即夸克、反夸克与组分胶子对介子自旋的贡献).得到了关于 ρ±、κ± 介子的磁矩和自旋朗德因子gs 的限制条件以及关于基态1- 介子各组成子(夸克、反夸克或组分胶子)所携带的介子自旋的份额r 的限制条件,
The non\|perturbative effect of gluons in a bound state is assumed to be simulated by the massive constituent gluons, and then the general wave functions of the usual J P=1 - mesons are constructed to be a superposition of a qq state and qqg state through an analysis of the Lorentz\|group and the SU (N c ) color group representations. Based on this, the magnetic moments as well as the spin structure (i.e. the contributions of quark, antiquark and gluon to the spin of a meson) of ρ ±、κ *± 、ρ 0、 ω and ф mesons are investigated. A constraint condition for the spin Lande g\|factor of the charged 1 - mesons is obtained, and furthermore, a constraint condition for the magnitudes of the contributions of the valence quark, antiquark and the constituent gluon to the spin of a vector meson is then derived on the same basis. The effect of the constituent gluon on the meson spin is found to be significant.
出处
《武汉大学学报(自然科学版)》
CSCD
1999年第3期321-324,共4页
Journal of Wuhan University(Natural Science Edition)
关键词
组分胶子
自旋结构
磁矩
介子
胶子
自由度
constituent gluon
mesonic spin structure
mesonic magnetic moment