Lie algebras

Idea

When a Lie group G acts on a manifold, it is interesting to study its infinitesimal generators, that is, the tangent vectors at the identity eG. They correspond to vector fields at the manifold and they are called the fundamental vector field X associated to Xg.

This is related to the Lie algebra action and the Maurer-Cartan form.

When two Lie groups share the same Lie algebra they are locally the same. See relation SO(3) and SU(2) for an important example.

Definition and remarks

Definition (abstract)
A Lie algebra is a vector space g together with a bilinear operation

[,]:g×gg

obeying the following identities

Bilinearity makes equivalent alternativity and anticommutativity:

[x,y]=[y,x]

On the other hand, Jacobi identity is better understood as saying that [,z] are derivations of the Lie algebra.

On an associative algebra A over a field F with multiplication (x,y)xy, a Lie bracket may be defined by the commutator [x,y]=xyyx.
With this bracket, A is a Lie algebra. The associative algebra A is called an enveloping algebra of the Lie algebra (A,[,]). Every Lie algebra can be embedded into one in such a way that it arises from an associative algebra in this fashion; see universal enveloping algebra.

In abstract, a Lie algebra is a vector space (finite or infinite dimensional). See about solvable algebras and solvable structures to understand things about the finite dimensional and infinite dimensional cases.

Examples:


Important cases: solvable Lie algebras, simple Lie algebras,...