摘要
在坐标表象中由Bargmann Wigner方程导出了便于求解的高自旋场方程 。
From the Bargmann Wigner equation in coordinate representation, a convenient form of field equations for arbitrary spin, which are similar to the Rarita Schwinger equations for arbitrary half integral spin, is derived rigorously. The method used here is to expand the completely symmetric multispinor field with symmetric matrices and a tensor or tensor spinor field. Meanwhile, the Lagrangian functions for fields with arbitrary integral and half integral spin are given respectively.
出处
《高能物理与核物理》
EI
CSCD
北大核心
2001年第11期1058-1064,共7页
High Energy Physics and Nuclear Physics
基金
国家自然科学基金 (1 994 70 0 1
1 9775 94 4和 1 9991 4 80 )
高等学校博士学科点专项基金 (970 3 5 80 7)
北京正负电子对撞机国家实验室
兰州重离子加速器国家实验室原子核理论研究中心
安徽省教育厅自然科学基金 (99JL0 0 71 )资助~~