Changing the gravitational constitutive law in BF theory does not force any change in the internal gauge-theory constitutive law, because no canonical map connects the two sectors.
Connections and Frame Bundle Reductions
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abstract
In general relativity, the gravitational potential is represented by the Levi-Civita connection, the only symmetric connection preserving the metric. On a differentiable manifold, a metric identifies with an orthogonal structure, defined as a Lorentz reduction of the frame bundle. The Levi-Civita connection appears as the only symmetric connection preserving the reduction. This paper presents generalization of this process to other aproaches of gravitation: Weyl structure with Weyl connections, teleparallel structures with Weitzenbock connections, unimodular structure, similarly appear as frame bundle reductions, with preserving connections. To each subgroup H of the linear group GL correspond reduced structures, or H-structures. They are subbundles of the frame bundle (with GL as principal group), with H as principal group. A linear connection in a manifold M is a principal connection on the frame bundle. Given a reduction, the corresponding preserving connections on M are the linear connections which preserve it. I also show that the time gauge used in the 3+1 formalism for general relativity similarly appears as the result of a bundle reduction.
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Nontrivial constitutive laws and unified structures in constrained BF theory
Changing the gravitational constitutive law in BF theory does not force any change in the internal gauge-theory constitutive law, because no canonical map connects the two sectors.