线性自对偶约束理论的一种推广形式及其量子化  

Extension of the Linear Self-Dual Constraint Theory and Its Quantization

作　　者：缪炎刚[1] 

机构地区：[1]兰州大学物理系,730000

出　　处：《高能物理与核物理》1993年第7期626-630,共5页High Energy Physics and Nuclear Physics

摘　　要：本文推广了线性自对偶约束理论,使其包含以拉氏乘子场为宗量的一个任意势函数,通过分析该系统的约束代数,证明了只有当势函数为二次形时,这个模型才给出自对偶场的Floreanini-Jackiw理论,并且当势函数为一种正幂次函数时,该模型可以给出一个自由标量场理论。We extend the self-dual field theory with a linear self-dual constraint to include an arbitrary potential of the Lagrange multiplier field. We show that this theory coincides with the Floreanini-Jackiw's formalism only for a quadratic potential, and the free scalar field theory for the potentials of the Lagrange multiplier to finite and positive power.

关 键 词：自对偶约束 对偶 约束 量子化 

分 类 号：O413.3[理学—理论物理]