View source for Parallel transport

A topological or differential geometric construction generalizing the idea of parallel translation in affine spaces to general bundles. In contrast with the affine case, the result of parallel transport along a closed path may in general be nontrivial, leading thus to the notion of [[curvature]]. 

==Parallel transport (translation) in affine spaces==
If $A$ is an affine space associated with the vector space $V=\Bbbk^n$ (over the field $\Bbbk$, usually $\Bbbk=\R$), then $V$ acts on $A$ by parallel translations $\{t_w:w\in V\}$:  
$$
\forall x=(a_1,\dots,a_n)\in A^n,\ \forall w=(w_1,\dots,w_n)\in V\qquad  t_w x=(a_1+w_1,\dots,a_n+ w_n).
$$
This action induces the (almost trivial) action of parallel transport on tangent vectors. If $TA\simeq V\times A\simeq\Bbbk^{2n}=\{(v,a)\}$ is the tangent bundle, the collection of vectors $v$ attached to different points $a\in A$, then the parallel transport acts on $TA$ by its [[differential]],
$$
\forall v\in T_aA,\ \forall w\in V,\qquad \rd t_w(a)\cdot v=v\in T_{t_w(a)}=T_{a+w} A.
$$
Consequently, if $w_1,\dots,w_k\in V$ are vectors such that $w=w_1+\cdots+w_k=0$, then the action $t_{w_k}\circ\cdots\circ t_{w_1}:T_a A\to T_a A$ is the identity for any point $a$.

These trivial observations indicate some of the properties that will fail for general parallel transport.

{{anchor|flat}}
===Parallel transport on Lie groups===
The idea of parallel transport uses the Lie group structure on $\R^n$ but the commutativity in fact is not necessary. 

Let $G$ be a (finite-dimensional) Lie group with $\mathfrak g=T_e G$ the tangent space at the unity. For any element $g\in G$ denote by $r_g:G\to G$ the right action, $r_g(x)=x\cdot g$. This [[action of a group on a manifold|action]] is transitive and free by the smooth diffeomorphisms. The differential $\rd r_g:T_e G\to T_g G$ is a bijection of the tangent spaces, which allows to identify them. For any ordered tuple of elements $g_1,\dots,g_k\in G$ whose product is equal to $e$, $g_1\cdots g_k=e$, the composition $r_{g_k}\circ\cdots \circ r_{g_1}$ is the identical transformation and the corresponding self-map $T_x G\to T_x G$ the identity map.

The same obviously holds also for the left action $l_g:x\mapsto g\cdot x$ of $G$ on itself and for any free transitive action of $G$ on the corresponding [[homogeneous space]] $F$.

==Parallel transport in topological bundles and fibrations==

Let $\pi:E\to B$ be a topological [[bundle]] with a generic fiber $F$, with all three topological spaces eventually having some additional structures defined on them. Usually we will assume that $E,B,F$ are smooth (finite-dimensional) manifolds with $\pi$ a differentiable map of full rank, in which case $\pi$ is often called [[fibration]].

===Motivation===

===Formal definition===

A ''connection'' in the topological bundle is a correspondence which allows to associate with any simple path $\gamma:[0,1]\to B$ in the base a family of homeomorphisms $\tau_t^s:\pi^{-1}(\gamma(t))\to\pi^{-1}(\gamma(s))$ between the respective fibers $F_t=\pi^{-1}(\gamma(t))$ and $F_s=\pi^{-1}(\gamma(s))$ such that:
* $\tau_t^s\circ \tau_r^t=\tau_{r}^s$ for all values $r,t,s\in[0,1]$ in any order, $\tau_t^t\equiv\operatorname{id}$,
* the homeomorphisms $\tau_{t}^s$ continuously depend on $t,s\in[0,1]$,
* the homemorphisms $\tau_t^s$ preserve the additional structure<ref>E.g., if all fibers are linear or Euclidean spaces, then $\tau_t^s$ must be linear, resp., linear orthogonal operators.</ref> on the fibers, if any.

The homeomorphism $\tau_\gamma=\tau_0^1:F_a\to F_b$, $a=\gamma(0)$, $b=\gamma(1)$, is called the ''parallel transport along the path $\gamma$''. By the natural extension, it is defined for closed paths $\gamma$ beginning and ending at any point $a$ as a self-map of the fiber $F_a$.

===Parallel transport for coverings: covering homotopy===

===Smooth connections on fibrations===
In the case where $\pi$ is a smooth bundle (''fibration''), it is natural to require that connections are differentiable maps between the fibers, differentiably depending also on the "transport time". This leads to the infinitesimal (tangent) construction known as the [[Ehresmann connection]].

====Covariant derivation via connection==== 
Let $\pi$ be a fibration and $s:B\to E$ a ''smooth [[section]]'', a differentiable map selecting a point $z=s(a)$ in each fiber $F_a$. A connection on the bundle $E$ allows to differentiate $s$ along a smooth path $\gamma:(\R^1,0)\to (B,a)$, with the derivative (at the initial point $a$) being a "vertical" vector tangent to the fiber $F_a$ at the point $z=s(a)\in E$.

The construction goes as follows: for every $t\in (\R^1,0)$ the parallel transport map $\tau_t^0=(\tau_0^t)^{-1}$ maps the point $s(\gamma(t))\in F_{\gamma(t)}$ back into the fiber $F_a=F_{\gamma(0)}$, defining thus a continuous curve
$$
(\R^1,0)\owns t\mapsto f(t)=\tau_t^0(s(\gamma(t))\in F_a.\tag{TC}
$$
If the section and the transport curve $\gamma$ are smooth (the condition that should be verified in the local trivializing charts), then the curve $t\mapsto f(t)$ is a smooth parametrized curve in the fiber $F_a$ which has a well-defined velocity vector $w\in T_z F\subseteq T_z E$, $z=f(0)=s(a)$.  

Linearization (computing the differentials) of all maps occurring in (TC) provides the linear relationships between the vectors $u=\dot \gamma(0)\in T_a B$, its image $v=\rd s(a) u$ and its "vertical projection" $w\in T_z F\subset T_z F$, $z=s(a)$. Thus the parallel transport in the tangential (linear) approximation provides us with the ''splitting'' of the space $T_z E$, the linear projection<ref>It should be stressed that the linear projection $P_z$ of a tangent space onto its subspace is not a differential of any suitable smooth map.</ref> $P_z:T_z E\to T_z F$ on the vertical subspace $T_z F$, the kernel of $\rd \pi(z):T_z E\to T_a B$. 

The directional derivative of a section $s(\cdot)$ along a curve $\gamma$ tangent to the vector $u=\dot\gamma(a)$ at the point $a$ of the base is therefore the vector $w=P_z\cdot\rd s(a)\cdot\dot\gamma(a)$, with the operators $\{P_z:T_zE\to \operatorname{Ker}\rd\pi(z)\}$ giving the complete infinitesimal description of the connection.

In practice instead of the family of operators $\{P_z\}$ one uses the [[distribution of tangent subspaces|distribution of their null spaces]], a sub-bundle $\Gamma\subset TE$ of the total bundle. Subspaces $\{\Gamma_z\subseteq T_z E\}$ from this distribution are referred to as [[horizontal distribution|horizontal subspaces]] should be ''complementary'' to the vertical subspaces $\{V_z=T_z E\}$ tangent to the fibers of the projection $\pi$. This means that  $\dim\Gamma=\dim B$ and the differential $\rd \pi$ restricted on these subspaces is invertible.



====Ehresmann connection====
The Ehresmann connection on the fiber bundle $\pi:E\to B$ is a [[horizontal distribution]] $\Gamma\subset TE$ complementary (transversal) to the ''vertical''<ref>Note that the vertical distribution is [[integrability|integrable]] ([[involutive distribution|involutive]]), while the integrability of $\Gamma$ is not postulated.</ref> distribution $V=\operatorname{Ker}\rd \pi\subset TE$.

The Ehresmann connection defines the parallel transport along any ''smooth'' path $\gamma:[0,1]\to B$ in the base as follows. For any point $z\in E$ over the curve, $\pi(z)=\gamma(t)$, there is a unique "horizontal lift", the vector $v(z)\in\Gamma_z$, which "covers" the velocity vector $\dot\gamma(t)$, $\rd \pi(z)v(z)=\dot\gamma(t)$. The corresponding vector field is defined on the induced bundle $\gamma^*\pi$ over the segment $[0,1]$; by construction, the flow of this field commutes with the projection on the base, hence maps fibers to fibers and defines the family of transport maps $\tau_t^s$.

====Curvature and integrability====
The parallel transport between two fibers $F_0=\pi^{-1}(\gamma(0))$ and $F_1=\pi^{-1}(\gamma(1))$ defined by a horizontal distribution $\Gamma$ in general depends on the whole curve $\gamma$ and changes with the curve even if its endpoints remain fixed. 

The is one particular case when the parallel transport is (locally) independent of the path. Assume that the horizontal distribution is [[involutive distribution|involutive]] and by the [[Frobenius theorem]] it admits integral submanifolds through each point $z\in E$. By definition, these manifolds are transversal to the fibers and hence locally diffeomorphic to the base: each such manifold is the graph of a ''locally constant'' section $s$, whose graph is tangent to the distribution. If the generic fiber is compact, this implies that for any point $a\in B$ on the base, there exists a small neighborhood $U\owns a$ in $B$ such that each fiber $F_b=\pi^{-1}(b)$ is ''canonically diffeomorphic'' to $F_a$. The diffeomorphism maps every point $z\in F_a$ to the value $s_z(b)\in F_b$, where $s_z(\cdot)$ is the uniquely defined horizontal section of $\pi$ such that $s_z(a)=z$. In particular, the parallel transport of the fiber $F_a$ on itself is identical for any closed loop with $\gamma(0)=\gamma(1)=a$ (smooth or only continuous) which entirely belongs to $U$, $\gamma([0,1])\subset U$.


Connections with the property that the parallel translation along any sufficiently small (contractible) loop on the base is identical, are called [[locally flat connection]]s. The local flatness, however, does not guarantee that the parallel transport along a "large" (non-contractible) loop in the base will be identical. Ditto for ''singular connections'' exhibiting singularities on small subsets of the base.

==Connections on principal and vector bundles==

Non-involutive distributions produce parallel transport that is non-identical even for arbitrarily small simple closed loops: the deviation from the identity is generally referred to as the curvature of the connection. 

$\def\e{\varepsilon}$
To separate the contribution of different elements of the construction, consider two non-collinear vectors $u_1,u_2\in T_a B$ tangent to the base, and a small loop $\gamma_\e$ which (say, in a given chart $U$ on the base) corresponds to oriented boundary the parallelogram with the edges $\e u_1$ and $\e u_2$ for a sufficiently small real number $\e>0$. Although the loop $\gamma_\e$ is only piecewise-smooth, one can attempt to compute the corresponding parallel transport map $\tau_\e=\tau_{\gamma_\e}:F_a\to F_a$. An easy estimate made in the trivializing coordinates shows that if the generic fiber $F$ is compact, then $\tau_\e$ is a self-diffeomorphism of the fiber,  $O(\e^2)$-close to the identity.

In absence of another structure on the generic fiber $F$ it is difficult to say more, in particular to study how the properly normalized displacement $\lim_{\e\to0}\e^{-2}(\tau_\e(x)-x)$ depends on the point $x\in F_a$ and the two vectors $u_1,u_2$. However, for the special cases where the generic fiber is "flat" (a nicely parallelizable homogeneous space, see [[#flat|above]], e.g., for vector or principal G-bundles) the computation leads to the notion of the [[curvature tensor]], resp., [[curvature form]].


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