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Conformal invariance in gauge theories. II. Yang-Mills theory

Journal Article · · Theor. Math. Phys.; (United States)
DOI:https://doi.org/10.1007/BF01028890· OSTI ID:6639964
The results of Part 1 are generalized to the non-Abelian case. By analogy with conformal QED, in which interaction with a matter field is realized by means of a four-vector potential that transforms in accordance with a direct sum of two nonprincipal representations, the first step in the present paper is the construction of a new formulation of quantum electrodynamics, in which the four-vector potential is regarded as an independent variable. Although the potential as a whole transforms in accordance with a principal representation, the corresponding conformally invariant two-point functions have a nonzero transverse part, and the Lagrangian is nondegenerate. In the non-Abelian case, one manifestly conformally invariant gauge condition is found, and the corresponding functional determinant is calculated. It is shown that in the gauge-invariant sector this theory is equivalent to the ordinary theory with conformally noninvariant gauge condition. A local effective Lagrangian is constructed, the Faddeev-Popov ''ghost'' fields having in this case scale dimension zero. It is shown that this effective Lagrangian has a residual global supersymmetry of Becchi-Rouet-Stora type.
Research Organization:
Joint Inst. for Nuclear Research, Dubna
OSTI ID:
6639964
Journal Information:
Theor. Math. Phys.; (United States), Journal Name: Theor. Math. Phys.; (United States) Vol. 67:1; ISSN TMPHA
Country of Publication:
United States
Language:
English

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