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Connection (affine bundle)

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In differential geometry, a connection on an affine bundle is a specialisation to affine bundles of the more general notion of a connection on a principal bundle. Let Y → X be an affine bundle modelled over a vector bundle Y → X. A connection Γ on Y → X is called an affine connection if, as a section Γ : Y → J1Y of the jet bundle J1Y → Y of Y, it is an affine bundle morphism over X.

The term "affine connection" as used in this article should not be confused with its more common usage, namely a connection on the tangent bundle TX of a smooth manifold X, though as discussed below, the latter can be considered as a special example of the former.

With respect to affine bundle coordinates (xλ, yi) on Y, an affine connection Γ on Y → X is given by the tangent-valued connection form

Γ=dxλ⊗(∂λ+Γλi∂i),Γλi=Γλij(xν)yj+σλi(xν).

An affine bundle is a fiber bundle with a general affine structure group GA(m, ℝ) of affine transformations of its typical fiber V of dimension m. Therefore, an affine connection is associated to a principal connection. It always exists.

For any affine connection Γ : Y → J1Y, the corresponding linear derivative Γ : Y → J1Y of an affine morphism Γ defines a unique linear connection on a vector bundle Y → X. With respect to linear bundle coordinates (xλ, yi) on Y, this connection reads

Γ‾=dxλ⊗(∂λ+Γλij(xν)y‾j∂‾i).

Since every vector bundle is an affine bundle, any linear connection on a vector bundle also is an affine connection.

If Y → X is a vector bundle, both an affine connection Γ and an associated linear connection Γ are connections on the same vector bundle Y → X, and their difference is a basic soldering form on

σ=σλi(xν)dxλ⊗∂i.

Thus, every affine connection on a vector bundle Y → X is a sum of a linear connection and a basic soldering form on Y → X.

Due to the canonical vertical splitting VY = Y × Y, this soldering form is brought into a vector-valued form

σ=σλi(xν)dxλ⊗ei

where ei is a fiber basis for Y.

Given an affine connection Γ on a vector bundle Y → X, let R and R be the curvatures of a connection Γ and the associated linear connection Γ, respectively. It is readily observed that R = R + T, where

T=12Tλμidxλ∧dxμ⊗∂i,Tλμi=∂λσμi−∂μσλi+σλhΓμih−σμhΓλih,

is the torsion of Γ with respect to the basic soldering form σ.

In particular, consider the tangent bundle TX of a manifold X coordinated by (xμ, ẋμ). There is the canonical soldering form

θ=dxμ⊗∂˙μ

on TX which coincides with the tautological one-form

θX=dxμ⊗∂μ

on X due to the canonical vertical splitting VTX = TX × TX. Given an arbitrary linear connection Γ on TX, the corresponding affine connection

A=Γ+θ,Aλμ=Γλμνx˙ν+δλμ,

on TX is the Cartan connection. The torsion of the Cartan connection A with respect to the soldering form θ coincides with the torsion of a linear connection Γ, and its curvature is a sum R + T of the curvature and the torsion of Γ.

See also

References

  • Sardanashvily, G. (2013). Advanced Differential Geometry for Theoreticians. Fiber bundles, jet manifolds and Lagrangian theory. Lambert Academic Publishing. arXiv:0908.1886. Bibcode:2009arXiv0908.1886S. ISBN 978-3-659-37815-7. Search this book on

Template:Differential-geometry-stub


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