# Ehresmann connection

In differential geometry, an **Ehresmann connection** (after the French mathematician Charles Ehresmann who first formalized this concept) is a version of the notion of a connection, which makes sense on any smooth fibre bundle. In particular, it does not rely on the possible vector bundle structure of the underlying fibre bundle, but nevertheless, linear connections may be viewed as a special case. Another important special case of Ehresmann connections are principal connections on principal bundles, which are required to be equivariant in the principal Lie group action.

## Introduction

A covariant derivative in differential geometry is a linear differential operator which takes the directional derivative of a section of a vector bundle in a covariant manner. It also allows one to formulate a notion of a parallel section of a bundle in the direction of a vector: a section *s* is parallel along a vector *X* if ∇_{X}*s* = 0. So a covariant derivative provides at least two things: a differential operator, *and* a notion of what it means to be parallel in each direction. An **Ehresmann connection** drops the differential operator completely and defines a connection axiomatically in terms of the sections parallel in each direction Template:Harv. Specifically, an Ehresmann connection singles out a vector subspace of each tangent space to the total space of the fibre bundle, called the *horizontal space*. A section *s* is then horizontal (i.e., parallel) in the direction *X* if d*s*(*X*) lies in a horizontal space. Here we are regarding *s* as a function *s* : *M* → *E* from the base *M* to the fibre bundle *E*, so that d*s* : *TM* → *s*TE* is then the pushforward of tangent vectors. The horizontal spaces together form a vector subbundle of *TE*.

This has the immediate benefit of being definable on a much broader class of structures than mere vector bundles. In particular, it is well-defined on a general fibre bundle. Furthermore, many of the features of the covariant derivative still remain: parallel transport, curvature, and holonomy.

The missing ingredient of the connection, apart from linearity, is *covariance*. With the classical covariant derivatives, covariance is an *a posteriori* feature of the derivative. In their construction one specifies the transformation law of the Christoffel symbols – which is not covariant – and then general covariance of the *derivative* follows as a result. For an Ehresmann connection, it is possible to impose a generalized covariance principle from the beginning by introducing a Lie group acting on the fibres of the fibre bundle. The appropriate condition is to require that the horizontal spaces be, in a certain sense, equivariant with respect to the group action.

The final finishing touch for an Ehresmann connection is that it can be represented as a differential form, in much the same way as the case of a connection form. If the group acts on the fibres and the connection is equivariant, then the form will also be equivariant. Furthermore, the connection form allows for a definition of curvature as a curvature form as well.

## Formal definition

Let *π*: *E* → *M* be a smooth fiber bundle.^{[1]} Let *V* = ker (d*π* : *TE* → *π***TM*) be the **vertical bundle** consisting of the vectors "tangent to the fibres" of *E*, i.e. the fibre of *V* at *e* ∈ *E* is *V*_{e} =*T*_{e}(*E*_{π(e)}). This subbundle of *TE* is canonically defined while the being tangent to the base space *M* is not (of course, this dissymmetry comes from the very definition of a fibre bundle, which "only has one projection" *π*: *E* → *M* while a product *E*=*M* × *F* would have two)

### Definition via horizontal subspaces

An **Ehresmann connection** on *E* is a smooth subbundle *H* of *TE*, called the **horizontal bundle** of the connection, which is complementary to *V*, in the sense that it defines a direct sum decomposition *TE* = *H*⊕*V* Template:Harv. In more detail, the horizontal bundle has the following properties.

- For each point
*e*∈*E*,*H*_{e}is a vector subspace of the tangent space*T*_{e}*E*to*E*at*e*, called the*horizontal subspace*of the connection at*e*. *H*_{e}depends smoothly on*e*.- For each
*e*∈*E*,*H*_{e}∩*V*_{e}= {0}. - Any tangent vector in
*T*_{e}*E*(for any*e*∈*E*) is the sum of a horizontal and vertical component, so that*T*_{e}*E*=*H*_{e}+*V*_{e}.

In more sophisticated terms, such an assignment of horizontal spaces satisfying these properties corresponds precisely to a smooth section of the jet bundle *J*^{1}*E* → *E*.

### Definition via a connection form

Equivalently, let *v* be the projection onto the vertical bundle *V* along *H* (so that *H* = ker *v*). This is determined by the above *direct sum* decomposition of *TE* into horizontal and vertical parts and is sometimes called the connection form of the Ehresmann connection. Thus *v* is a vector bundle homomorphism from *TE* to itself with the following properties (of projections in general):

*v*^{2}=*v*;*v*is the identity on*V=Image (v)*.

Conversely, if *v* is a vector bundle endomorphism of *TE* satisfying these two properties, then *H* = ker *v* is the horizontal subbundle of an Ehresmann connection.

Finally, note that *v*, being a linear mapping of each tangent space into itself, may also be regarded as a *TE*-valued 1-form on *E*. This will be a useful perspective in sections to come.

### Parallel transport via horizontal lifts

An Ehresmann connection also prescribes a manner for lifting curves from the base manifold *M* into the total space of the fibre bundle *E* so that the tangents to the curve are horizontal.^{[2]} These **horizontal lifts** are a direct analogue of parallel transport for other versions of the connection formalism.

Specifically, suppose that *γ*(*t*) is a smooth curve in *M* through the point *x* = *γ*(0). Let *e* ∈ *E*_{x} be a point in the fibre over *x*. A **lift** of *γ* through *e* is a curve in the total space *E* such that

A lift is **horizontal** if, in addition, every tangent of the curve lies in the horizontal subbundle of *TE*:

It can be shown using the rank-nullity theorem applied to *π* and *v* that each vector *X*∈*T*_{x}*M* has a unique horizontal lift to a vector . In particular, the tangent field to *γ* generates a horizontal vector field in the total space of the pullback bundle *γ***E*. By the Picard–Lindelöf theorem, this vector field is integrable. Thus, for any curve *γ* and point *e* over *x* = *γ*(0), there exists a *unique horizontal lift* of *γ* through *e* for small time *t*.

Note that, for general Ehresmann connections, the horizontal lift is path-dependent. When two smooth curves in *M*, coinciding at *γ*_{1}(0) = *γ*_{2}(0) = *x*_{0} and also intersecting at another point *x*_{1} ∈ *M*, are lifted horizontally to *E* through the same *e* ∈ *π*^{−1}(*x*_{0}), they will generally pass through different points of *π*^{−1}(*x*_{1}). This has important consequences for the differential geometry of fibre bundles: the space of sections of *H* is not a Lie subalgebra of the space of vector fields on *E*, because it is not (in general) closed under the Lie bracket of vector fields. This failure of closure under Lie bracket is measured by the *curvature*.

## Properties

### Curvature

Let *v* be an Ehresmann connection. Then the curvature of *v* is given by^{[3]}

where [-,-] denotes the Frölicher-Nijenhuis bracket of *v* ∈ Ω^{1}(*E*,*TE*) with itself. Thus *R* ∈ Ω^{2}(*E*,*TE*) is the two-form on *E* with values in *TE* defined by

or, in other terms,

where *X* = *X*_{H} + *X*_{V} denotes the direct sum decomposition into *H* and *V* components, respectively. From this last expression for the curvature, it is seen to vanish identically if, and only if, the horizontal subbundle is Frobenius integrable. Thus the curvature is the integrability condition for the horizontal subbundle to yield transverse sections of the fibre bundle *E* → *M*.

The curvature of an Ehresmann connection also satisfies a version of the Bianchi identity:

where again [-,-] is the Frölicher-Nijenhuis bracket of v ∈ Ω^{1}(*E*,*TE*) and *R* ∈ Ω^{2}(*E*,*TE*).

### Completeness

An Ehresmann connection allows curves to have unique horizontal lifts locally. For a **complete** Ehresmann connection, a curve can be horizontally lifted over its entire domain.

### Holonomy

Flatness of the connection corresponds locally to the Frobenius integrability of the horizontal spaces. At the other extreme, non-vanishing curvature implies the presence of holonomy of the connection.^{[4]}

## Special cases

### Principal bundles and principal connections

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Suppose that *E* is a smooth principal *G*-bundle over *M*. Then an Ehresmann connection *H* on *E* is said to be a **principal (Ehresmann) connection**^{[5]} if it is invariant with respect to the *G* action on *E* in the sense that

- for any
*e*∈*E*and*g*∈*G*; here denotes the differential of the right action of*g*on*E*at*e*.

The one-parameter subgroups of *G* act vertically on *E*. The differential of this action allows one to identify the subspace with the Lie algebra **g** of group *G*, say by map . The connection form *v* of the Ehresmann connection may then be viewed as a 1-form *ω* on *E* with values in **g** defined by *ω*(*X*)=*ι*(*v*(*X*)).

Thus reinterpreted, the connection form *ω* satisfies the following two properties:

- It transforms equivariantly under the
*G*action: for all*h*∈*G*, where*R*_{h}^{*}is the pullback under the right action and*Ad*is the adjoint representation of*G*on its Lie algebra. - It maps vertical vector fields to their associated elements of the Lie algebra:
*ω*(*X*)=*ι*(*X*) for all*X*∈*V*.

Conversely, it can be shown that such a **g**-valued 1-form on a principal bundle generates a horizontal distribution satisfying the aforementioned properties.

Given a local trivialization one can reduce *ω* to the horizontal vector fields (in this trivialization). It defines a 1-form *ω' * on *B* via pullback. The form *ω'* determines *ω* completely, but it depends on the choice of trivialization. (This form is often also called a **connection form** and denoted simply by *ω*.)

### Vector bundles and covariant derivatives

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Suppose that *E* is a smooth vector bundle over *M*. Then an Ehresmann connection *H* on *E* is said to be a **linear (Ehresmann) connection** if *H*_{e} depends linearly on *e* ∈ *E*_{x} for each *x* ∈ *M*. To make this precise, let *S*_{λ} denote scalar multiplication by *λ* on *E*, and let denote addition.

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Since *E* is a vector bundle, its vertical bundle *V* is isomorphic to *π***E*. Therefore if *s* is a section of *E*, then
*v*(d*s*):*TM*→*s***V*=*s***π***E*=*E*. The fact that the Ehresmann connection is linear implies that this is a vector bundle homomorphism, and is therefore given by a section ∇*s* of the vector bundle Hom(*TM*,*E*), called the covariant derivative of *s*.

Conversely a covariant derivative *∇* on a vector bundle defines a linear Ehresmann connection by defining *H*_{e}, for *e* ∈ *E* with *x*=*π*(*e*), to be the image d*s*_{x}(*T*_{x}*M*) where *s* is a section of *E* with *s(x)*=*e* and *∇ _{}*Xs

*=0 for all*X

*∈*T

*xM*

_{}*.*

Note that (for historical reasons) the term *linear* when applied to connections, is sometimes used (like the word *affine* – see Affine connection) to refer to connections defined on the tangent bundle or frame bundle.

### Associated bundles

An Ehresmann connection on a fibre bundle (endowed with a structure group) sometimes gives rise to an Ehresmann connection on an associated bundle. For instance, a (linear) connection in a vector bundle *E*, thought of giving a parallelism of *E* as above, induces a connection on the associated bundle of frames P*E* of *E*. Conversely, a connection in P*E* gives rise to a (linear) connection in *E* provided that the connection in P*E* is equivariant with respect to the action of the general linear group on the frames (and thus a principal connection). It is *not always* possible for an Ehresmann connection to induce, in a natural way, a connection on an associated bundle. For example, a non-equivariant Ehresmann connection on a bundle of frames of a vector bundle may not induce a connection on the vector bundle.

Suppose that *E* is an associated bundle of *P*, so that *E* = *P* ×_{G} *F*. A ** G-connection** on

*E*is an Ehresmann connection such that the parallel transport map τ :

*F*

_{x}→

*F*

_{x′}is given by a

*G*-transformation of the fibres (over sufficiently nearby points

*x*and

*x*′ in

*M*joined by a curve).

^{[6]}

Given a principal connection on *P*, one obtains a *G*-connection on the associated fibre bundle *E* = *P* ×_{G} *F* via pullback.

Conversely, given a *G*-connection on *E* it is possible to recover the principal connection on the associated principal bundle *P*. To recover this principal connection, one introduces the notion of a *frame* on the typical fibre *F*. Since *G* is a finite-dimensional^{[7]} Lie group acting effectively on *F*, there must exist a finite configuration of points (*y*_{1},...,*y*_{m}) within *F* such that the *G*-orbit *R* = {(*gy*_{1},...,*gy*_{m}) | *g* ∈ *G*} is a principal homogeneous space of *G*. One can think of *R* as giving a generalization of the notion of a frame for the *G*-action on *F*. Note that, since *R* is a principal homogeneous space for *G*, the fibre bundle *E*(*R*) associated to *E* with typical fibre *R* is (equivalent to) the principal bundle associated to *E*. But it is also a subbundle of the *m*-fold product bundle of *E* with itself. The distribution of horizontal spaces on *E* induces a distribution of spaces on this product bundle. Since the parallel transport maps associated to the connection are *G*-maps, they preserve the subspace *E*(*R*), and so the *G*-connection descends to a principal *G*-connection on *E*(*R*).

In summary, there is a one-to-one correspondence (up to equivalence) between the descents of principal connections to associated fibre bundles, and *G*-connections on associated fibre bundles. For this reason, in the category of fibre bundles with a structure group *G*, the principal connection contains all relevant information for *G*-connections on the associated bundles. Hence, unless there is an overriding reason to consider connections on associated bundles (as there is, for instance, in the case of Cartan connections) one usually works directly with the principal connection.

## Notes

- ↑ These considerations apply equally well to the more general situation in which
*π*:*E*→*M*is a surjective submersion: i.e.,*E*is a fibred manifold over*M*. In an alternative generalization, due to Template:Harv and Template:Harv,*E*and*M*are permitted to be Banach manifolds, with*E*a fibre bundle over*M*as above. - ↑ See Template:Harv and Template:Harv
- ↑ Template:Harv
- ↑ Holonomy for Ehresmann connections in fibre bundles is sometimes called the
**Ehresmann-Reeb holonomy**or**leaf holonomy**in reference to the first detailed study using Ehresmann connections to study foliations in Template:Harv - ↑ Template:Harvnb Volume 1.
- ↑ See also Lumiste (2001),
*Connections on a manifold*. - ↑ For convenience, we assume that
*G*is finite-dimensional, although this assumption can safely be dropped with minor modifications.

## References

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## Further reading

- Raoul Bott (1970) "Topological obstruction to integrability",
*Proc. Symp. Pure Math.*,**16**Amer. Math. Soc., Providence, RI.