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Teoreticheskaya i Matematicheskaya Fizika, 1986, Volume 67, Number 1, Pages 76–88
(Mi tmf4922)
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This article is cited in 1 scientific paper (total in 1 paper)
Conformal invariance in gauge theories II. Yang–Mills theory
R. P. Zaikov
Abstract:
The results of Part I are generalized to the non-Abelian ease. 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 eleetrodynamics, 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.
Received: 14.02.1983 Revised: 10.04.1985
Citation:
R. P. Zaikov, “Conformal invariance in gauge theories II. Yang–Mills theory”, TMF, 67:1 (1986), 76–88; Theoret. and Math. Phys., 67:1 (1986), 368–375
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https://www.mathnet.ru/eng/tmf4922 https://www.mathnet.ru/eng/tmf/v67/i1/p76
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Abstract page: | 326 | Full-text PDF : | 153 | References: | 59 | First page: | 1 |
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