Chern-Simons Perturbation Theory

dc.creatorAxelrod, Scott
dc.creatorSinger, I. M.
dc.date1991-10-20
dc.date.accessioned2026-07-07T09:13:55Z
dc.date.available2026-07-07T09:13:55Z
dc.descriptionWe study the perturbation theory for three dimensional Chern--Simons quantum field theory on a general compact three manifold without boundary. We show that after a simple change of variables, the action obtained by BRS gauge fixing in the Lorentz gauge has a superspace formulation. The basic properties of the propagator and the Feynman rules are written in a precise manner in the language of differential forms. Using the explicit description of the propagator singularities, we prove that the theory is finite. Finally the anomalous metric dependence of the $2$-loop partition function on the Riemannian metric (which was introduced to define the gauge fixing) can be cancelled by a local counterterm as in the $1$-loop case. In fact, the counterterm is equal to the Chern--Simons action of the metric connection, normalized precisely as one would expect based on the framing dependence of Witten's exact solution.
dc.description36 pages. Invited talk at the XXth Conference on Differential Geometric Methods in Physics, New York, June 1991
dc.identifierhttps://arxiv.org/abs/hep-th/9110056
dc.identifierhttp://arxiv.org/abs/hep-th/9110056
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/152492
dc.subjectHigh Energy Physics - Theory
dc.subjectDifferential Geometry
dc.subjectQuantum Algebra
dc.titleChern-Simons Perturbation Theory
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