The Background Field Method as a Canonical Transformation
arXiv:1203.6637 · doi:10.1103/PhysRevD.85.121702
Abstract
We construct explicitly the canonical transformation that controls the full dependence (local and non-local) of the vertex functional of a Yang-Mills theory on a background field. After showing that the canonical transformation found is nothing but a direct field-theoretic generalization of the Lie transform of classical analytical mechanics, we comment on a number of possible applications, and in particular the non perturbative implementation of the background field method on the lattice, the background field formulation of the two particle irreducible formalism, and, finally, the formulation of the Schwinger-Dyson series in the presence of topologically non-trivial configurations.
11 pages, REVTeX. References added, some explanations extended. Final version to appear in the journal
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- Patterns of gauge symmetry in the background field method
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- High-energy QCD evolution from Slavnov-Taylor identity
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