Lie algebra bundle

In mathematics, a weak Lie algebra bundle

 \xi=(\xi, p, X, \theta)\,

is a vector bundle \xi\, over a base space X together with a morphism

 \theta : \xi \otimes \xi \rightarrow \xi

which induces a Lie algebra structure on each fibre  \xi_x\, .

A Lie algebra bundle  \xi=(\xi, p, X)\, is a vector bundle in which each fibre is a Lie algebra and for every x in X, there is an open set  U containing x, a Lie algebra L and a homeomorphism

 \phi:U\times L\to p^{-1}(U)\,

such that

 \phi_x:x\times L \rightarrow p^{-1}(x)\,

is a Lie algebra isomorphism.

Any Lie algebra bundle is a weak Lie algebra bundle, but the converse need not be true in general.

As an example of a weak Lie algebra bundle that is not a strong Lie algebra bundle, consider the total space \mathfrak{so}(3)\times\mathbb{R} over the real line \mathbb{R}. Let [.,.] denote the Lie bracket of \mathfrak{so}(3) and deform it by the real parameter as:

[X,Y]_x = x\cdot[X,Y]

for X,Y\in\mathfrak{so}(3) and x\in\mathbb{R}.

Lie's third theorem states that every bundle of Lie algebras can locally be integrated to a bundle of Lie groups. However globally the total space might fail to be Hausdorff.[1]

References

  1. A. Weinstein, A.C. da Silva: Geometric models for noncommutative algebras, 1999 Berkley LNM, online readable at , in particular chapter 16.3.

See also

This article is issued from Wikipedia - version of the Friday, March 25, 2016. The text is available under the Creative Commons Attribution/Share Alike but additional terms may apply for the media files.