Parallelizable manifold

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In mathematics, a differentiable manifold of dimension n is called parallelizable

on the manifold, such that at every point of the
tangent vectors
provide a
basis of the tangent space
at . Equivalently, the has a global section on

A particular choice of such a basis of vector fields on is called a parallelization (or an absolute parallelism) of .

Examples

  • An example with is the circle: we can take V1 to be the unit tangent vector field, say pointing in the anti-clockwise direction. The torus of dimension is also parallelizable, as can be seen by expressing it as a cartesian product of circles. For example, take and construct a torus from a square of graph paper with opposite edges glued together, to get an idea of the two tangent directions at each point. More generally, every Lie group G is parallelizable, since a basis for the tangent space at the identity element can be moved around by the action of the translation group of G on G (every translation is a diffeomorphism and therefore these translations induce linear isomorphisms between tangent spaces of points in G).
  • A classical problem was to determine which of the
    normed division algebras of the real numbers, complex numbers, quaternions, and octonions, which allows one to construct a parallelism for each. Proving that other spheres are not parallelizable is more difficult, and requires algebraic topology
    .
  • The product of parallelizable manifolds is parallelizable.
  • Every orientable closed three-dimensional manifold is parallelizable.[3]

Remarks

See also

Notes

  1. ^ Bishop, Richard L.; Goldberg, Samuel I. (1968), Tensor Analysis on Manifolds, New York: Macmillan, p. 160
  2. .
  3. ^ Milnor, John W. (1958), Differentiable manifolds which are homotopy spheres (PDF)

References