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Connections give rise to parallel transport along a curve on a manifold. A connection also leads to invariants of curvature (see also curvature tensor and curvature form), and the so-called torsion. General conceptThe general concept can be summarized as follows: given a fiber bundle <math>\eta:E\to B<math> the tangent space at any point of E has canonical "vertical" subspace, the subspace tangent to the fiber. The connection fixes a choice of "horizontal" subspace at each point of E so that the tangent space of E is a direct sum of vertical and horizontal subspaces. Usually more requirements are imposed on the choice of "horizontal" subspaces, but they depend on the type of the bundle. Given a <math>B'\to B<math> the induced bundle has an induced connection. If <math>B'=I<math> is a segment then connection on B gives a trivialization on the induced bundle over I, i.e. a choice of smooth one-parameter family of isomorphisms between the fibers over I. This family is called parallel displacement along the curve <math>I\to B <math> and it gives an equivalent description of connection (which in case of Levi-Civita connection on a Riemannian manifold is called parallel transport). There are many ways to describe connection, in one particular approach, a connection can be locally described as a matrix of 1-forms which is the multiplant of the difference between the covariant derivative and the ordinary partial derivative in a coordinate chart. That is, partial derivatives are not an intrinsic notion on a manifold: a connection 'fixes up' the concept and permits discussion in geometric terms. Possible approachesThere are quite a number of possible approaches to the connection concept. They include the following:
The connections referred to above are linear or affine connections. There is also a concept of projective connection; the most commonly-met form of this is the Schwarzian derivative in complex analysis. See also: Gauss-Manin connection |
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