affine connection

In differential geometry, an affine connection is a geometric object on a smooth manifold which ''connects'' nearby tangent spaces, so it permits tangent vector fields to be differentiated as if they were functions on the manifold with values in a fixed vector space. Connections are among the simplest methods of defining differentiation of the sections of vector bundles.

The notion of an affine connection has its roots in 19th-century geometry and tensor calculus, but was not fully developed until the early 1920s, by Élie Cartan (as part of his general theory of connections) and Hermann Weyl (who used the notion as a part of his foundations for general relativity). The terminology is due to Cartan and has its origins in the identification of tangent spaces in Euclidean space by translation: the idea is that a choice of affine connection makes a manifold look infinitesimally like Euclidean space not just smoothly, but as an affine space.

On any manifold of positive dimension there are infinitely many affine connections. If the manifold is further endowed with a metric tensor then there is a natural choice of affine connection, called the Levi-Civita connection. The choice of an affine connection is equivalent to prescribing a way of differentiating vector fields which satisfies several reasonable properties (linearity and the Leibniz rule). This yields a possible definition of an affine connection as a covariant derivative or (linear) connection on the tangent bundle. A choice of affine connection is also equivalent to a notion of parallel transport, which is a method for transporting tangent vectors along curves. This also defines a parallel transport on the frame bundle. Infinitesimal parallel transport in the frame bundle yields another description of an affine connection, either as a Cartan connection for the affine group or as a principal connection on the frame bundle.

The main invariants of an affine connection are its torsion and its curvature. The torsion measures how closely the Lie bracket of vector fields can be recovered from the affine connection. Affine connections may also be used to define (affine) geodesics on a manifold, generalizing the ''straight lines'' of Euclidean space, although the geometry of those straight lines can be very different from usual Euclidean geometry; the main differences are encapsulated in the curvature of the connection.

Motivation and history

A smooth manifold is a mathematical object which looks locally like a smooth deformation of Euclidean space : for example a smooth curve or surface looks locally like a smooth deformation of a line or a plane. Smooth functions and vector fields can be defined on manifolds, just as they can on Euclidean space, and scalar functions on manifolds can be differentiated in a natural way. However, differentiation of vector fields is less straightforward: this is a simple matter in Euclidean space, because the tangent space of based vectors at a point can be identified naturally (by translation) with the tangent space at a nearby point . On a general manifold, there is no such natural identification between nearby tangent spaces, and so tangent vectors at nearby points cannot be compared in a well-defined way. The notion of an affine connection was introduced to remedy this problem by ''connecting'' nearby tangent spaces. The origins of this idea can be traced back to two main sources: surface theory and tensor calculus.

Motivation from surface theory

Consider a smooth surface in a 3-dimensional Euclidean space. Near any point, can be approximated by its tangent plane at that point, which is an affine subspace of Euclidean space. Differential geometers in the 19th century were interested in the notion of development in which one surface was ''rolled'' along another, without ''slipping'' or ''twisting''. In particular, the tangent plane to a point of can be rolled on : this should be easy to imagine when is a surface like the 2-sphere, which is the smooth boundary of a convex region. As the tangent plane is rolled on , the point of contact traces out a curve on . Conversely, given a curve on , the tangent plane can be rolled along that curve. This provides a way to identify the tangent planes at different points along the curve: in particular, a tangent vector in the tangent space at one point on the curve is identified with a unique tangent vector at any other point on the curve. These identifications are always given by affine transformations from one tangent plane to another.

This notion of parallel transport of tangent vectors, by affine transformations, along a curve has a characteristic feature: the point of contact of the tangent plane with the surface ''always moves'' with the curve under parallel translation (i.e., as the tangent plane is rolled along the surface, the point of contact moves). This generic condition is characteristic of Cartan connections. In more modern approaches, the point of contact is viewed as the ''origin'' in the tangent plane (which is then a vector space), and the movement of the origin is corrected by a translation, so that parallel transport is linear, rather than affine.

In the point of view of Cartan connections, however, the affine subspaces of Euclidean space are ''model'' surfaces — they are the simplest surfaces in Euclidean 3-space, and are homogeneous under the affine group of the plane — and every smooth surface has a unique model surface tangent to it at each point. These model surfaces are ''Klein geometries'' in the sense of Felix Klein's Erlangen programme. More generally, an -dimensional affine space is a Klein geometry for the affine group , the stabilizer of a point being the general linear group . An affine -manifold is then a manifold which looks infinitesimally like -dimensional affine space.

Motivation from tensor calculus

The second motivation for affine connections comes from the notion of a covariant derivative of vector fields. Before the advent of coordinate-independent methods, it was necessary to work with vector fields by embedding their respective Euclidean vectors into an atlas. These components can be differentiated, but the derivatives do not transform in a manageable way under changes of coordinates. Correction terms were introduced by Elwin Bruno Christoffel (following ideas of Bernhard Riemann) in the 1870s so that the (corrected) derivative of one vector field along another transformed covariantly under coordinate transformations — these correction terms subsequently came to be known as Christoffel symbols.

This idea was developed into the theory of ''absolute differential calculus'' (now known as tensor calculus) by Gregorio Ricci-Curbastro and his student Tullio Levi-Civita between 1880 and the turn of the 20th century.

Tensor calculus really came to life, however, with the advent of Albert Einstein's theory of general relativity in 1915. A few years after this, Levi-Civita formalized the unique connection associated to a Riemannian metric, now known as the Levi-Civita connection. More general affine connections were then studied around 1920, by Hermann Weyl, who developed a detailed mathematical foundation for general relativity, and Élie Cartan,. who made the link with the geometrical ideas coming from surface theory.

Approaches

The complex history has led to the development of widely varying approaches to and generalizations of the affine connection concept.

The most popular approach is probably the definition motivated by covariant derivatives. On the one hand, the ideas of Weyl were taken up by physicists in the form of gauge theory and gauge covariant derivatives. On the other hand, the notion of covariant differentiation was abstracted by Jean-Louis Koszul, who defined (linear or Koszul) connections on vector bundles. In this language, an affine connection is simply a covariant derivative or (linear) connection on the tangent bundle.

However, this approach does not explain the geometry behind affine connections nor how they acquired their name. The term really has its origins in the identification of tangent spaces in Euclidean space by translation: this property means that Euclidean -space is an affine space. (Alternatively, Euclidean space is a principal homogeneous space or torsor under the group of translations, which is a subgroup of the affine group.) As mentioned in the introduction, there are several ways to make this precise: one uses the fact that an affine connection defines a notion of parallel transport of vector fields along a curve. This also defines a parallel transport on the frame bundle. Infinitesimal parallel transport in the frame bundle yields another description of an affine connection, either as a Cartan connection for the affine group or as a principal connection on the frame bundle.

Formal definition as a differential operator

Let be a smooth manifold and let be the space of vector fields on , that is, the space of smooth sections of the tangent bundle . Then an affine connection on is a bilinear map

: $\begin \Gamma(\mathrmM)\times \Gamma(\mathrmM) & \rightarrow \Gamma(\mathrmM)\\ (X,Y) & \mapsto \nabla_X Y\,,\end$
such that for all in the set of smooth functions on , written , and all vector fields on :
# , that is, is -''linear'' in the first variable;
# , where denotes the directional derivative; that is, satisfies ''Leibniz rule'' in the second variable.

Elementary properties

* It follows from property 1 above that the value of at a point depends only on the value of at and not on the value of on . It also follows from property 2 above that the value of at a point depends only on the value of on a neighbourhood of .
* If are affine connections then the value at of may be written where $\Gamma_x : \mathrm_xM \times \mathrm_xM \to \mathrm_xM$ is bilinear and depends smoothly on (i.e., it defines a smooth bundle homomorphism). Conversely if is an affine connection and is such a smooth bilinear bundle homomorphism (called a connection form on ) then is an affine connection.
* If is an open subset of , then the tangent bundle of is the trivial bundle . In this situation there is a canonical affine connection on : any vector field is given by a smooth function from to ; then is the vector field corresponding to the smooth function from to . Any other affine connection on may therefore be written , where is a connection form on .
* More generally, a local trivialization of the tangent bundle is a bundle isomorphism between the restriction of to an open subset of , and . The restriction of an affine connection to may then be written in the form where is a connection form on .

Parallel transport for affine connections

Comparison of tangent vectors at different points on a manifold is generally not a well-defined process. An affine connection provides one way to remedy this using the notion of parallel transport, and indeed this can be used to give a definition of an affine connection.

Let be a manifold with an affine connection . Then a vector field is said to be parallel if in the sense that for any vector field , . Intuitively speaking, parallel vectors have ''all their derivatives equal to zero'' and are therefore in some sense ''constant''. By evaluating a parallel vector field at two points and , an identification between a tangent vector at and one at is obtained. Such tangent vectors are said to be parallel transports of each other.

Nonzero parallel vector fields do not, in general, exist, because the equation is a partial differential equation which is overdetermined: the integrability condition for this equation is the vanishing of the curvature of (see below). However, if this equation is restricted to a curve from to it becomes an ordinary differential equation. There is then a unique solution for any initial value of at .

More precisely, if a smooth curve parametrized by an interval and , where , then a vector field along (and in particular, the value of this vector field at ) is called the parallel transport of along if
#, for all
#.
Formally, the first condition means that is parallel with respect to the pullback connection on the pullback bundle . However, in a local trivialization it is a first-order system of linear ordinary differential equations, which has a unique solution for any initial condition given by the second condition (for instance, by the Picard–Lindelöf theorem).

Thus parallel transport provides a way of moving tangent vectors along a curve using the affine connection to keep them "pointing in the same direction" in an intuitive sense, and this provides a linear isomorphism between the tangent spaces at the two ends of the curve. The isomorphism obtained in this way will in general depend on the choice of the curve: if it does not, then parallel transport along every curve can be used to define parallel vector fields on , which can only happen if the curvature of is zero.

A linear isomorphism is determined by its action on an ordered basis or frame. Hence parallel transport can also be characterized as a way of transporting elements of the (tangent) frame bundle along a curve. In other words, the affine connection provides a lift of any curve in to a curve in .

Formal definition on the frame bundle

An affine connection may also be defined as a principal connection on the frame bundle or of a manifold . In more detail, is a smooth map from the tangent bundle of the frame bundle to the space of matrices (which is the Lie algebra of the Lie group of invertible matrices) satisfying two properties:
# is equivariant with respect to the action of on and ;
# for any in , where is the vector field on corresponding to .

Such a connection immediately defines a covariant derivative not only on the tangent bundle, but on vector bundles associated to any group representation of , including bundles of tensors and tensor densities. Conversely, an affine connection on the tangent bundle determines an affine connection on the frame bundle, for instance, by requiring that vanishes on tangent vectors to the lifts of curves to the frame bundle defined by parallel transport.

The frame bundle also comes equipped with a solder form which is horizontal in the sense that it vanishes on vertical vectors such as the point values of the vector fields : Indeed is defined first by projecting a tangent vector (to at a frame ) to , then by taking the components of this tangent vector on with respect to the frame . Note that is also -equivariant (where acts on by matrix multiplication).

The pair defines a bundle isomorphism of with the trivial bundle , where is the Cartesian product of and (viewed as the Lie algebra of the affine group, which is actually a semidirect product – see below).

Affine connections as Cartan connections

Affine connections can be defined within Cartan's general framework. In the modern approach, this is closely related to the definition of affine connections on the frame bundle. Indeed, in one formulation, a Cartan connection is an absolute parallelism of a principal bundle satisfying suitable properties. From this point of view the -valued one-form on the frame bundle (of an affine manifold) is a Cartan connection. However, Cartan's original approach was different from this in a number of ways:
* the concept of frame bundles or principal bundles did not exist;
* a connection was viewed in terms of parallel transport between infinitesimally nearby points;
* this parallel transport was affine, rather than linear;
* the objects being transported were not tangent vectors in the modern sense, but elements of an affine space with a marked point, which the Cartan connection ultimately ''identifies'' with the tangent space.

Explanations and historical intuition

The points just raised are easiest to explain in reverse, starting from the motivation provided by surface theory. In this situation, although the planes being rolled over the surface are tangent planes in a naive sense, the notion of a tangent space is really an infinitesimal notion, whereas the planes, as affine subspaces of , are infinite in extent. However these affine planes all have a marked point, the point of contact with the surface, and they are tangent to the surface at this point. The confusion therefore arises because an affine space with a marked point can be identified with its tangent space at that point. However, the parallel transport defined by rolling does not fix this origin: it is affine rather than linear; the linear parallel transport can be recovered by applying a translation.

Abstracting this idea, an affine manifold should therefore be an -manifold with an affine space , of dimension , ''attached'' to each at a marked point , together with a method for transporting elements of these affine spaces along any curve in . This method is required to satisfy several properties:
# for any two points on , parallel transport is an affine transformation from to ;
# parallel transport is defined infinitesimally in the sense that it is differentiable at any point on and depends only on the tangent vector to at that point;
# the derivative of the parallel transport at determines a linear isomorphism from to .

These last two points are quite hard to make precise, so affine connections are more often defined infinitesimally. To motivate this, it suffices to consider how affine frames of reference transform infinitesimally with respect to parallel transport. (This is the origin of Cartan's method of moving frames.) An affine frame at a point consists of a list , where and the form a basis of . The affine connection is then given symbolically by a first order differential system

:$(*) \begin \mathrm &= \theta^1\mathbf_1 + \cdots + \theta^n\mathbf_n \\ \mathrm\mathbf_i &= \omega^1_i\mathbf_1 + \cdots + \omega^n_i\mathbf_n \end \quad i=1,2,\ldots,n$

defined by a collection of one-forms . Geometrically, an affine frame undergoes a displacement travelling along a curve from to given (approximately, or infinitesimally) by

:$\begin p(\gamma(t+\delta t)) - p(\gamma(t)) &= \left(\theta^1\left(\gamma'(t)\right)\mathbf_1 + \cdots + \theta^n\left(\gamma'(t)\right)\mathbf_n\right)\mathrm \delta t \\ \mathbf_i(\gamma(t+\delta t)) - \mathbf_i(\gamma(t)) &= \left(\omega^1_i\left(\gamma'(t)\right)\mathbf_1 + \cdots + \omega^n_i\left(\gamma'(t)\right) \mathbf_n\right)\delta t\,. \end$

Furthermore, the affine spaces are required to be tangent to in the informal sense that the displacement of along can be identified (approximately or infinitesimally) with the tangent vector to at (which is the infinitesimal displacement of ). Since
:$a_x (\gamma(t + \delta t)) - a_x (\gamma(t)) = \theta\left(\gamma'(t)\right) \delta t \,,$
where is defined by , this identification is given by , so the requirement is that should be a linear isomorphism at each point.

The tangential affine space is thus identified intuitively with an ''infinitesimal affine neighborhood'' of .

The modern point of view makes all this intuition more precise using principal bundles (the essential idea is to replace a frame or a ''variable'' frame by the space of all frames and functions on this space). It also draws on the inspiration of Felix Klein's Erlangen programme, in which a ''geometry'' is defined to be a homogeneous space. Affine space is a geometry in this sense, and is equipped with a ''flat'' Cartan connection. Thus a general affine manifold is viewed as ''curved'' deformation of the flat model geometry of affine space.

Affine space as the flat model geometry

Definition of an affine space

Informally, an affine space is a vector space without a fixed choice of origin. It describes the geometry of points and free vectors in space. As a consequence of the lack of origin, points in affine space cannot be added together as this requires a choice of origin with which to form the parallelogram law for vector addition. However, a vector may be added to a point by placing the initial point of the vector at and then transporting to the terminal point. The operation thus described is the translation of along . In technical terms, affine -space is a set equipped with a free transitive action of the vector group on it through this operation of translation of points: is thus a principal homogeneous space for the vector group .

The general linear group is the group of transformations of which preserve the ''linear structure'' of in the sense that . By analogy, the affine group is the group of transformations of preserving the ''affine structure''. Thus must ''preserve translations'' in the sense that

:$\varphi(p+v)=\varphi(p)+T(v)$

where is a general linear transformation. The map sending to is a group homomorphism. Its kernel is the group of translations . The stabilizer of any point in can thus be identified with using this projection: this realises the affine group as a semidirect product of and , and affine space as the homogeneous space .

Affine frames and the flat affine connection

An ''affine frame'' for consists of a point and a basis of the vector space . The general linear group acts freely on the set of all affine frames by fixing and transforming the basis in the usual way, and the map sending an affine frame to is the quotient map. Thus is a principal -bundle over . The action of extends naturally to a free transitive action of the affine group on , so that is an -torsor, and the choice of a reference frame identifies with the principal bundle .

On there is a collection of functions defined by

:$\pi(p;\mathbf_1, \dots ,\mathbf_n) = p$

(as before) and

:$\varepsilon_i(p;\mathbf_1,\dots , \mathbf_n) = \mathbf_i\,.$

After choosing a basepoint for , these are all functions with values in , so it is possible to take their exterior derivatives to obtain differential 1-forms with values in . Since the functions yield a basis for at each point of , these 1-forms must be expressible as sums of the form

:$\begin \mathrm\pi &= \theta^1\varepsilon_1+\cdots+\theta^n\varepsilon_n\\ \mathrm\varepsilon_i &= \omega^1_i\varepsilon_1+\cdots+\omega^n_i\varepsilon_n \end$

for some collection of real-valued one-forms on . This system of one-forms on the principal bundle defines the affine connection on .

Taking the exterior derivative a second time, and using the fact that as well as the linear independence of the , the following relations are obtained:

:$\begin \mathrm\theta^j - \sum_i\omega^j_i\wedge\theta^i &=0\\ \mathrm\omega^j_i - \sum_k \omega^j_k\wedge\omega^k_i &=0\,. \end$

These are the Maurer–Cartan equations for the Lie group (identified with by the choice of a reference frame). Furthermore:
* the Pfaffian system (for all ) is integrable, and its integral manifolds are the fibres of the principal bundle .
* the Pfaffian system (for all ) is also integrable, and its integral manifolds define parallel transport in .

Thus the forms define a flat principal connection on .

For a strict comparison with the motivation, one should actually define parallel transport in a principal -bundle over . This can be done by pulling back by the smooth map defined by translation. Then the composite is a principal -bundle over , and the forms pull back to give a flat principal -connection on this bundle.

General affine geometries: formal definitions

An affine space, as with essentially any smooth Klein geometry, is a manifold equipped with a flat Cartan connection. More general affine manifolds or affine geometries are obtained easily by dropping the flatness condition expressed by the Maurer-Cartan equations. There are several ways to approach the definition and two will be given. Both definitions are facilitated by the realisation that 1-forms in the flat model fit together to give a 1-form with values in the Lie algebra of the affine group .

In these definitions, is a smooth -manifold and is an affine space of the same dimension.

Definition via absolute parallelism

Let be a manifold, and a principal -bundle over . Then an affine connection is a 1-form on with values in satisfying the following properties
# is equivariant with respect to the action of on and ;
# for all in the Lie algebra of all matrices;
# is a linear isomorphism of each tangent space of with .
The last condition means that is an absolute parallelism on , i.e., it identifies the tangent bundle of with a trivial bundle (in this case ). The pair defines the structure of an affine geometry on , making it into an affine manifold.

The affine Lie algebra splits as a semidirect product of and and so may be written as a pair where takes values in and takes values in . Conditions 1 and 2 are equivalent to being a principal -connection and being a horizontal equivariant 1-form, which induces a bundle homomorphism from to the associated bundle . Condition 3 is equivalent to the fact that this bundle homomorphism is an isomorphism. (However, this decomposition is a consequence of the rather special structure of the affine group.) Since is the frame bundle of , it follows that provides a bundle isomorphism between and the frame bundle of ; this recovers the definition of an affine connection as a principal -connection on .

The 1-forms arising in the flat model are just the components of and .

Definition as a principal affine connection

An affine connection on is a principal -bundle over , together with a principal -subbundle of and a principal -connection (a 1-form on with values in ) which satisfies the following (generic) ''Cartan condition''. The component of pullback of to is a horizontal equivariant 1-form and so defines a bundle homomorphism from to : this is required to be an isomorphism.

Relation to the motivation

Since acts on , there is, associated to the principal bundle , a bundle , which is a fiber bundle over whose fiber at in is an affine space . A section of (defining a marked point in for each ) determines a principal -subbundle of (as the bundle of stabilizers of these marked points) and vice versa. The principal connection defines an Ehresmann connection on this bundle, hence a notion of parallel transport. The Cartan condition ensures that the distinguished section always moves under parallel transport.

Further properties

Curvature and torsion

Curvature and torsion are the main invariants of an affine connection. As there are many equivalent ways to define the notion of an affine connection, so there are many different ways to define curvature and torsion.

From the Cartan connection point of view, the curvature is the failure of the affine connection to satisfy the Maurer–Cartan equation

:\mathrm\eta + \tfrac12 eta\wedge\eta= 0,

where the second term on the left hand side is the wedge product using the Lie bracket in to contract the values. By expanding into the pair and using the structure of the Lie algebra , this left hand side can be expanded into the two formulae

:$\mathrm\theta + \omega\wedge\theta \quad \text \quad \mathrm\omega + \omega\wedge\omega\,,$

where the wedge products are evaluated using matrix multiplication. The first expression is called the torsion of the connection, and the second is also called the curvature.

These expressions are differential 2-forms on the total space of a frame bundle. However, they are horizontal and equivariant, and hence define tensorial objects. These can be defined directly from the induced covariant derivative on as follows.

The torsion is given by the formula

:T^\nabla(X,Y) = \nabla_X Y - \nabla_Y X - ,Y

If the torsion vanishes, the connection is said to be ''torsion-free'' or ''symmetric''.

The curvature is given by the formula

:$R^\nabla_Z = \nabla_X\nabla_Y Z - \nabla_Y\nabla_X Z - \nabla_Z.$

Note that is the Lie bracket of vector fields

: ,Y\left(X^j \partial_j Y^i - Y^j \partial_j X^i\right)\partial_i

in Einstein notation. This is independent of coordinate system choice and

: $\partial_i = \left(\frac\right)_p\,,$

the tangent vector at point of the th coordinate curve. The are a natural basis for the tangent space at point , and the the corresponding coordinates for the vector field .

When both curvature and torsion vanish, the connection defines a pre-Lie algebra structure on the space of global sections of the tangent bundle.

The Levi-Civita connection

If is a Riemannian manifold then there is a unique affine connection on with the following two properties:
* the connection is torsion-free, i.e., is zero, so that ;
* parallel transport is an isometry, i.e., the inner products (defined using ) between tangent vectors are preserved.
This connection is called the Levi-Civita connection.

The term "symmetric" is often used instead of torsion-free for the first property. The second condition means that the connection is a metric connection in the sense that the Riemannian metric is parallel: . For a torsion-free connection, the condition is equivalent to the identity +
, "compatibility with the metric". In local coordinates the components of the form are called Christoffel symbols: because of the uniqueness of the Levi-Civita connection, there is a formula for these components in terms of the components of .

Geodesics

Since straight lines are a concept in affine geometry, affine connections define a generalized notion of (parametrized) straight lines on any affine manifold, called affine geodesics. Abstractly, a parametric curve is a straight line if its tangent vector remains parallel and equipollent with itself when it is transported along . From the linear point of view, an affine connection distinguishes the affine geodesics in the following way: a smooth curve is an affine geodesic if $\dot\gamma$ is parallel transported along , that is
:$\tau_t^s\dot\gamma(s) = \dot\gamma(t)$
where is the parallel transport map defining the connection.

In terms of the infinitesimal connection , the derivative of this equation implies
:$\nabla_\dot\gamma(t) = 0$
for all .

Conversely, any solution of this differential equation yields a curve whose tangent vector is parallel transported along the curve. For every and every , there exists a unique affine geodesic with and and where is the maximal open interval in , containing 0, on which the geodesic is defined. This follows from the Picard–Lindelöf theorem, and allows for the definition of an exponential map associated to the affine connection.

In particular, when is a ( pseudo-)Riemannian manifold and is the Levi-Civita connection, then the affine geodesics are the usual geodesics of Riemannian geometry and are the locally distance minimizing curves.

The geodesics defined here are sometimes called affinely parametrized, since a given straight line in determines a parametric curve through the line up to a choice of affine reparametrization , where and are constants. The tangent vector to an affine geodesic is parallel and equipollent along itself. An unparametrized geodesic, or one which is merely parallel along itself without necessarily being equipollent, need only satisfy

:$\nabla_\dot = k\dot$

for some function defined along . Unparametrized geodesics are often studied from the point of view of projective connections.

Development

An affine connection defines a notion of development of curves. Intuitively, development captures the notion that if is a curve in , then the affine tangent space at may be ''rolled'' along the curve. As it does so, the marked point of contact between the tangent space and the manifold traces out a curve in this affine space: the development of .

In formal terms, let be the linear parallel transport map associated to the affine connection. Then the development is the curve in starts off at 0 and is parallel to the tangent of for all time :
:$\dot_t = \tau_t^0\dot_t\,,\quad C_0 = 0.$

In particular, is a ''geodesic'' if and only if its development is an affinely parametrized straight line in .This treatment of development is from ; see section III.3 for a more geometrical treatment. See also for a thorough discussion of development in other geometrical situations.

Surface theory revisited

If is a surface in , it is easy to see that has a natural affine connection. From the linear connection point of view, the covariant derivative of a vector field is defined by differentiating the vector field, viewed as a map from to , and then projecting the result orthogonally back onto the tangent spaces of . It is easy to see that this affine connection is torsion-free. Furthermore, it is a metric connection with respect to the Riemannian metric on induced by the inner product on , hence it is the Levi-Civita connection of this metric.

Example: the unit sphere in Euclidean space

Let be the usual scalar product on , and let be the unit sphere. The tangent space to at a point is naturally identified with the vector subspace of consisting of all vectors orthogonal to . It follows that a vector field on can be seen as a map which satisfies

: $\langle Y_x, x\rangle = 0\,, \quad \forall x\in \mathbf^2.$

Denote as the differential (Jacobian matrix) of such a map. Then we have:

:Lemma. The formula
::$(\nabla_Z Y)_x = \mathrmY_x(Z_x) + \langle Z_x,Y_x\rangle x$
:defines an affine connection on with vanishing torsion.

:::Proof. It is straightforward to prove that satisfies the Leibniz identity and is linear in the first variable. So all that needs to be proved here is that the map above does indeed define a tangent vector field. That is, we need to prove that for all in
::::$\bigl\langle(\nabla_Z Y)_x,x\bigr\rangle = 0\,.\qquad \text$

:::Consider the map
::::$\begin f: \mathbf^2&\to \mathbf\\ x &\mapsto \langle Y_x, x\rangle\,.\end$

:::The map ''f'' is constant, hence its differential vanishes. In particular
::::$\mathrmf_x(Z_x) = \bigl\langle (\mathrm Y)_x(Z_x),x(\gamma'(t))\bigr\rangle + \langle Y_x, Z_x\rangle = 0\,.$

:::Equation 1 above follows. Q.E.D.

See also

*Atlas (topology)
*Connection (mathematics)
*Connection (fibred manifold)
* Connection (affine bundle)
*Differentiable manifold
*Differential geometry
* Introduction to the mathematics of general relativity
*Levi-Civita connection
* List of formulas in Riemannian geometry
*Riemannian geometry

Notes

Citations

References

*
*
*

Bibliography

Primary historical references

*
*
*
*
*
:: Cartan's treatment of affine connections as motivated by the study of relativity theory. Includes a detailed discussion of the physics of reference frames, and how the connection reflects the physical notion of transport along a worldline.
*
:: A more mathematically motivated account of affine connections.
* .
:: Affine connections from the point of view of Riemannian geometry. Robert Hermann's appendices discuss the motivation from surface theory, as well as the notion of affine connections in the modern sense of Koszul. He develops the basic properties of the differential operator ∇, and relates them to the classical affine connections in the sense of Cartan.
*

Secondary references

* .
:: This is the main reference for the technical details of the article. Volume 1, chapter III gives a detailed account of affine connections from the perspective of principal bundles on a manifold, parallel transport, development, geodesics, and associated differential operators. Volume 1 chapter VI gives an account of affine transformations, torsion, and the general theory of affine geodesy. Volume 2 gives a number of applications of affine connections to homogeneous spaces and complex manifolds, as well as to other assorted topics.
* .
* .
:: Two articles by Lumiste, giving precise conditions on parallel transport maps in order that they define affine connections. They also treat curvature, torsion, and other standard topics from a classical (non-principal bundle) perspective.
* .
:: This fills in some of the historical details, and provides a more reader-friendly elementary account of Cartan connections in general. Appendix A elucidates the relationship between the principal connection and absolute parallelism viewpoints. Appendix B bridges the gap between the classical "rolling" model of affine connections, and the modern one based on principal bundles and differential operators.

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Connection (mathematics)
Differential geometry
Maps of manifolds
Smooth functions

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