Parallelization (mathematics)
In mathematics, a parallelization[1] of a manifold of dimension n is a set of n global linearly independent vector fields.
Formal definition
Given a manifold of dimension n, a parallelization of
is a set
of n vector fields defined on all of
such that for every
the set
is a basis of
, where
denotes the fiber over
of the tangent vector bundle
.
A manifold is called parallelizable whenever admits a parallelization.
Examples
- Every Lie group is a parallelizable manifold.
- The product of parallelizable manifolds is parallelizable.
- Every affine space, considered as manifold, is parallelizable.
Properties
Proposition. A manifold is parallelizable iff there is a diffeomorphism
such that the first projection of
is
and for each
the second factor—restricted to
—is a linear map
.
In other words, is parallelizable if and only if
is a trivial bundle. For example suppose that
is an open subset of
, i.e., an open submanifold of
. Then
is equal to
, and
is clearly parallelizable.[2]
See also
- Chart (topology)
- Differentiable manifold
- Frame bundle
- Orthonormal frame bundle
- Principal bundle
- Connection (mathematics)
- G-structure
- Web (differential geometry)
Notes
- ↑ Bishop & Goldberg (1968), p. 160
- ↑ Milnor & Stasheff (1974), p. 15.
References
- Bishop, R.L.; Goldberg, S.I. (1968), Tensor Analysis on Manifolds (First Dover 1980 ed.), The Macmillan Company, ISBN 0-486-64039-6
- Milnor, J.W.; Stasheff, J.D. (1974), Characteristic Classes, Princeton University Press