Topologically massive gauge theories (Reprinted from Annals of Physics, vol 140, pg 372-411, 1982)

被引:329
作者
Deser, S [1 ]
Jackiw, R
Templeton, S
机构
[1] Brandeis Univ, Dept Phys, Waltham, MA 02254 USA
[2] MIT, Ctr Theoret Phys, Nucl Sci Lab, Cambridge, MA 02139 USA
[3] MIT, Dept Phys, Cambridge, MA 02139 USA
关键词
D O I
10.1006/aphy.2000.6013
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
Gauge vector and gravity models are studied in three-dimensional space-time, where novel. gauge invariant, P and T odd terms of topological origin give rise to masses For the gauge fields. In the vector case. the massless Maxwell excitation, which is spinless, becomes massive with spin 1. When interacting with fermions. the quantum theory is infrared and ultraviolet finite in perturbation theory. Fur non-Abelian models, topological considerations lead to a quantization condition on the dimensionless coupling constant-mass ratio. Ordinary Einstein gravity is trivial, but when augmented by our mass term, it acquires a propagating, massive? spin 2 mode. This theory is ghost-fret and causal, although of third-derivative order. Quantum calculations are presented in both the Abelian and non-Abelian vector models, to exhibit some of the delicate aspects of infrared behavior. and regularization dependence. (C) 1982 Academic Press.
引用
收藏
页码:409 / 449
页数:41
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