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Affine gauge theory : ウィキペディア英語版
Affine gauge theory
Affine gauge theory is classical gauge theory where gauge fields are affine connections on the tangent bundle over a smooth manifold X. For instance, these are gauge theory of dislocations in continuous media when X=\mathbb R^3, the generalization of metric-affine gravitation theory when X is a world manifold and, in particular, gauge theory of the fifth force.
==Affine tangent bundle==

Being a vector bundle, the tangent bundle TX of an n-dimensional manifold X admits a natural structure of an affine bundle ATX, called the ''affine tangent bundle'', possessing bundle atlases with affine transition functions. It is associated to a principal bundle AFX of affine frames in tangent space over X, whose structure group is a general affine group GA(n,\mathbb R).
The tangent bundle TX is associated to a principal linear frame bundle FX, whose structure group is a general linear group GL(n,\mathbb R). This is a subgroup of GA(n,\mathbb R) so that the latter is a semidirect product of GL(n,\mathbb R) and a group T^n of translations.
There is the canonical imbedding of FX to AFX onto a reduced principal subbundle which corresponds to the canonical structure of a vector bundle TX as the affine one.
Given linear bundle coordinates
: (x^\mu,\dot x^\mu), \qquad \dot x'^\mu=\frac\dot x^\nu, \qquad\qquad (1)
on the tangent bundle TX, the affine tangent bundle can be provided with affine bundle coordinates
: (x^\mu,\widetilde x^\mu=\dot x^\mu +a^\mu(x^\alpha)), \qquad \widetilde x'^\mu=\frac\widetilde x^\nu + b^\mu(x^\alpha). \qquad\qquad (2)
and, in particular, with the linear coordinates (1).

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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