Parallel transport on a manifold 
makes precise the idea of translating a vector
field 
along a differentiable curve
to attain a new vector field 
which is parallel to
.
More precisely, let 
be a smooth manifold with affine connection 
, let 
be a differentiable
curve from an interval 
into 
, and let 
be a vector
tangent to 
at 
for some 
.
A vector field 
along 
is the parallel transport of 
provided that 
and 
is covariantly constant,
meaning that
 |
(1)
|
for all 
,
where 
denotes the covariant derivative of 
along 
associated to 
.
A standard result in differential geometry is that, under the above hypotheses, parallel transports are unique.
In addition to the above definition, some literature defines parallel transport in a more function analytic way. Indeed, given an interval 
and a point 
, a parallel transport 
of 
along 
is nothing more than a linear transformation
 |
(2)
|
which maps 
to 
.
It is obvious that this transformation is invertible, its inverse being given simply
by parallel transport along the reversed portion of 
from 
to 
. The expression 
has added benefit, too, because despite being defined
intrinsically in terms of the affine connection 
on 
, it also provides a mechanism whereby one can recover
a manifold's affine connection given a collection 
of parallel vector fields along a curve 
. In particular, if 
and 
, then
 |
(3)
|
where 
is the desired vector field given by the connection 
and where 
.
