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 it 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
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