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{{Multiple issues|{{expert-subject|date=October 2013|reason=There is no lead and it needs to be better organized.}}{{no footnotes|date=October 2013}}
In [[differential geometry]], a '''connection on an affine bundle''' is a specialisation to [[affine bundle]]s of the more general notion of a [[connection on a principal bundle]]. Let {{math|''Y'' → ''X''}} be an affine bundle modelled over a vector bundle {{math|{{overline|''Y''}} → ''X''}}. A [[connection (fibred manifold)|connection]] {{math|Γ}} on {{math|''Y'' → ''X''}} is called an '''affine connection''' if, as a section {{math|Γ : ''Y'' → J<sup>1</sup>''Y''}} of the [[jet bundle]] {{math|J<sup>1</sup>''Y'' → ''Y''}} of {{math|''Y''}}, it is an affine bundle morphism over {{math|''X''}}.
}}


Let {{math|''Y'' → ''X''}} be an [[affine bundle]] modelled over a vector bundle {{math|{{overline|''Y''}} → ''X''}}. A [[connection (fibred manifold)|connection]] {{math|Γ}} on {{math|''Y'' → ''X''}} is called the '''affine connection''' if it as a section {{math|Γ : ''Y'' → J<sup>1</sup>''Y''}} of the [[jet bundle]] {{math|J<sup>1</sup>''Y'' → ''Y''}} of {{math|''Y''}} is an affine bundle morphism over {{math|''X''}}. In particular, this is the case of an [[affine connection]] on the [[tangent bundle]] {{math|T''X''}} of a [[smooth manifold]] {{math|''X''}}.
The term "affine connection" as used in this article should not be confused with [[affine connection|its more common usage]], namely a connection on the [[tangent bundle]] {{math|T''X''}} of a [[smooth manifold]] {{math|''X''}}, though as discussed below, the latter can be considered as a special example of the former.


With respect to affine bundle coordinates {{math|(''x<sup>λ</sup>'', ''y<sup>i</sup>'')}} on {{math|''Y''}}, an affine connection {{math|Γ}} on {{math|''Y'' → ''X''}} is given by the [[connection (fibred manifold)|tangent-valued connection form]]
With respect to affine bundle coordinates {{math|(''x<sup>λ</sup>'', ''y<sup>i</sup>'')}} on {{math|''Y''}}, an affine connection {{math|Γ}} on {{math|''Y'' → ''X''}} is given by the [[connection (fibred manifold)|tangent-valued connection form]]
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: <math>\begin{align}\Gamma &=dx^\lambda\otimes \left(\partial_\lambda + \Gamma_\lambda^i\partial_i\right)\,, \\ \Gamma_\lambda^i&={{\Gamma_\lambda}^i}_j\left(x^\nu\right) y^j + \sigma_\lambda^i\left(x^\nu\right)\,. \end{align}</math>
: <math>\begin{align}\Gamma &=dx^\lambda\otimes \left(\partial_\lambda + \Gamma_\lambda^i\partial_i\right)\,, \\ \Gamma_\lambda^i&={{\Gamma_\lambda}^i}_j\left(x^\nu\right) y^j + \sigma_\lambda^i\left(x^\nu\right)\,. \end{align}</math>


An affine bundle is a fiber bundle with a [[affine group|general affine]] [[fiber bundle|structure group]] {{math|GA(''m'', ℝ)}} of affine transformations of its typical fiber {{math|''V''}} of dimension {{math|''m''}}. Therefore, an affine connection is associated to a [[connection (principal bundle)|principal connection]]. It always exists.
An affine bundle is a fiber bundle with a [[affine group|general affine]] [[fiber bundle|structure group]] {{math|GA(''m'', ℝ)}} of affine transformations of its typical fiber {{math|''V''}} of dimension {{math|''m''}}. Therefore, an affine connection is associated to a principal connection. It always exists.
   
   
For any affine connection {{math|Γ : ''Y'' → J<sup>1</sup>''Y''}}, the corresponding [[affine bundle|linear derivative]]  {{math|{{overline|Γ}} : {{overline|''Y''}} → J<sup>1</sup>{{overline|''Y''}}}} of an affine morphism {{math|Γ}} defines a unique [[connection (vector bundle)|linear connection]] on a vector bundle {{math|{{overline|''Y''}} → ''X''}}. With respect to linear bundle coordinates {{math|(''x<sup>λ</sup>'', {{overline|''y''}}<sup>''i''</sup>)}} on {{math|{{overline|''Y''}}}}, this connection reads
For any affine connection {{math|Γ : ''Y'' → J<sup>1</sup>''Y''}}, the corresponding [[affine bundle|linear derivative]]  {{math|{{overline|Γ}} : {{overline|''Y''}} → J<sup>1</sup>{{overline|''Y''}}}} of an affine morphism {{math|Γ}} defines a unique [[connection (vector bundle)|linear connection]] on a vector bundle {{math|{{overline|''Y''}} → ''X''}}. With respect to linear bundle coordinates {{math|(''x<sup>λ</sup>'', {{overline|''y''}}<sup>''i''</sup>)}} on {{math|{{overline|''Y''}}}}, this connection reads
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is the [[connection (fibred manifold)|torsion]] of {{math|Γ}} with respect to the basic soldering form {{math|''σ''}}.
is the [[connection (fibred manifold)|torsion]] of {{math|Γ}} with respect to the basic soldering form {{math|''σ''}}.


In particular, let us consider the tangent bundle {{math|T''X''}} of a manifold {{math|''X''}} coordinated by {{math|(''x<sup>μ</sup>'', ''ẋ<sup>μ</sup>'')}}. There is the canonical soldering form
In particular, consider the tangent bundle {{math|T''X''}} of a manifold {{math|''X''}} coordinated by {{math|(''x<sup>μ</sup>'', ''ẋ<sup>μ</sup>'')}}. There is the canonical soldering form
:<math>\theta=dx^\mu\otimes \dot\partial_\mu </math>
:<math>\theta=dx^\mu\otimes \dot\partial_\mu </math>
on {{math|T''X''}} which coincides with the [[tautological one-form]]
on {{math|T''X''}} which coincides with the [[tautological one-form]]
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==References==
==References==
* {{cite book|first1=S. |last1=Kobayashi |first2=K. |last2=Nomizu |title=Foundations of Differential Geometry |volume=1–2 |publisher=Wiley-Interscience |date=1996 |isbn=0-471-15733-3}}
* {{cite book|authorlink=Gennadi Sardanashvily|last=Sardanashvily |first=G. |title=Advanced Differential Geometry for Theoreticians. Fiber bundles, jet manifolds and Lagrangian theory |publisher=Lambert Academic Publishing |date=2013 |isbn=978-3-659-37815-7 |arxiv=0908.1886|bibcode=2009arXiv0908.1886S }}
* {{cite book|authorlink=Gennadi Sardanashvily|last=Sardanashvily |first=G. |title=Advanced Differential Geometry for Theoreticians. Fiber bundles, jet manifolds and Lagrangian theory |publisher=Lambert Academic Publishing |date=2013 |isbn=978-3-659-37815-7 |arxiv=0908.1886|bibcode=2009arXiv0908.1886S }}



Latest revision as of 22:14, 29 September 2026

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 Template:Math be an affine bundle modelled over a vector bundle Template:Math. A connection Template:Math on Template:Math is called an affine connection if, as a section Template:Math of the jet bundle Template:Math of Template:Math, it is an affine bundle morphism over Template:Math.

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 Template:Math of a smooth manifold Template:Math, though as discussed below, the latter can be considered as a special example of the former.

With respect to affine bundle coordinates Template:Math on Template:Math, an affine connection Template:Math on Template:Math is given by the tangent-valued connection form

<math>\begin{align}\Gamma &=dx^\lambda\otimes \left(\partial_\lambda + \Gamma_\lambda^i\partial_i\right)\,, \\ \Gamma_\lambda^i&={{\Gamma_\lambda}^i}_j\left(x^\nu\right) y^j + \sigma_\lambda^i\left(x^\nu\right)\,. \end{align}</math>

An affine bundle is a fiber bundle with a general affine structure group Template:Math of affine transformations of its typical fiber Template:Math of dimension Template:Math. Therefore, an affine connection is associated to a principal connection. It always exists.

For any affine connection Template:Math, the corresponding linear derivative Template:Math of an affine morphism Template:Math defines a unique linear connection on a vector bundle Template:Math. With respect to linear bundle coordinates Template:Math on Template:Math, this connection reads

<math> \overline \Gamma=dx^\lambda\otimes\left(\partial_\lambda +{{\Gamma_\lambda}^i}_j\left(x^\nu\right) \overline y^j\overline\partial_i\right)\,.</math>

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

If Template:Math is a vector bundle, both an affine connection Template:Math and an associated linear connection Template:Math are connections on the same vector bundle Template:Math, and their difference is a basic soldering form on

<math>\sigma= \sigma_\lambda^i(x^\nu) dx^\lambda\otimes\partial_i \,.</math>

Thus, every affine connection on a vector bundle Template:Math is a sum of a linear connection and a basic soldering form on Template:Math.

Due to the canonical vertical splitting Template:Math, this soldering form is brought into a vector-valued form

<math>\sigma= \sigma_\lambda^i(x^\nu) dx^\lambda\otimes e_i </math>

where Template:Math is a fiber basis for Template:Math.

Given an affine connection Template:Math on a vector bundle Template:Math, let Template:Math and Template:Math be the curvatures of a connection Template:Math and the associated linear connection Template:Math, respectively. It is readily observed that Template:Math, where

<math>\begin{align}

T &=\tfrac12 T_{\lambda\mu}^i dx^\lambda\wedge dx^\mu\otimes \partial_i\,, \\ T_{\lambda \mu}^i &= \partial_\lambda\sigma_\mu^i - \partial_\mu\sigma_\lambda^i + \sigma_\lambda^h {{\Gamma_\mu}^i}_h - \sigma_\mu^h {{\Gamma_\lambda}^i}_h\,, \end{align}</math>

is the torsion of Template:Math with respect to the basic soldering form Template:Math.

In particular, consider the tangent bundle Template:Math of a manifold Template:Math coordinated by Template:Math. There is the canonical soldering form

<math>\theta=dx^\mu\otimes \dot\partial_\mu </math>

on Template:Math which coincides with the tautological one-form

<math>\theta_X=dx^\mu\otimes \partial_\mu</math>

on Template:Math due to the canonical vertical splitting Template:Math. Given an arbitrary linear connection Template:Math on Template:Math, the corresponding affine connection

<math>\begin{align}

A&=\Gamma +\theta\,, \\ A_\lambda^\mu&={{\Gamma_\lambda}^\mu}_\nu \dot x^\nu +\delta^\mu_\lambda\,, \end{align}</math>

on Template:Math is the Cartan connection. The torsion of the Cartan connection Template:Math with respect to the soldering form Template:Math coincides with the torsion of a linear connection Template:Math, and its curvature is a sum Template:Math of the curvature and the torsion of Template:Math.

See also

References

Template:Differential-geometry-stub