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Connections and Frame Bundle Reductions

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arxiv 2002.01410 v1 pith:OIW6ZVCB submitted 2020-02-04 math-ph gr-qcmath.MP

classification math-phgr-qcmath.MP
keywords bundleconnectionconnectionsframepreservingreductiongrouplinear
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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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  1. Nontrivial constitutive laws and unified structures in constrained BF theory

    hep-th 2025-04 conditional novelty 5.0 of 10

    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.

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