In gravitation theory, a world manifold endowed with some Lorentzian pseudo-Riemannian metric and an associated space-time structure is a space-time. Gravitation theory is formulated as classical field theory on natural bundles over a world manifold.
A world manifold is a four-dimensional orientable real smooth manifold. It is assumed to be a Hausdorff and second countable topological space. Consequently, it is a locally compact space which is a union of a countable number of compact subsets, a separable space, a paracompact and completely regular space. Being paracompact, a world manifold admits a partition of unity by smooth functions. Paracompactness is an essential characteristic of a world manifold. It is necessary and sufficient in order that a world manifold admits a Riemannian metric and necessary for the existence of a pseudo-Riemannian metric. A world manifold is assumed to be connected and, consequently, it is arcwise connected.
The tangent bundle of a world manifold and the associated principal frame bundle of linear tangent frames in possess a general linear group structure group . A world manifold is said to be parallelizable if the tangent bundle and, accordingly, the frame bundle are trivial, i.e., there exists a global section (a frame field) of . It is essential that the tangent and associated bundles over a world manifold admit a bundle atlas of finite number of trivialization charts.
Tangent and frame bundles over a world manifold are natural bundles characterized by general covariant transformations. These transformations are gauge symmetries of gravitation theory on a world manifold.
By virtue of the well-known theorem on structure group reduction, a structure group of a frame bundle over a world manifold is always reducible to its maximal compact subgroup . The corresponding global section of the quotient bundle is a Riemannian metric on . Thus, a world manifold always admits a Riemannian metric which makes a metric topological space.
In accordance with the geometric Equivalence Principle, a world manifold possesses a Lorentzian structure, i.
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In quantum field theory, gauge gravitation theory is the effort to extend Yang–Mills theory, which provides a universal description of the fundamental interactions, to describe gravity. Gauge gravitation theory should not be confused with the similarly-named gauge theory gravity, which is a formulation of (classical) gravitation in the language of geometric algebra. Nor should it be confused with Kaluza–Klein theory, where the gauge fields are used to describe particle fields, but not gravity itself.