Lie groups

Definition and some properties

A Lie group is a manifold G together with two smooth operations satisfying the group definition.

Some interesting elementary properties:
Proposition
The identity component G0 of a Lie group G is a closed normal subgroup.
Proof
First, a connected component is always closed. And it is a submanifold.

Second, given g,hG, g can be seen as an homeomorphism

GG

by left multiplication. But since h and e are in the same connected component, gh and g are in the same component (and the same that e). Therefore, ghG0, and it is a subgroup.
Also, given gG0, the map G0G given by

hg1h

is a homeomorphism, so since g and e are in the same connected component e and g1 are in the same component. In conclusion, G0 is a subgroup.
And finally, since the map

ϕg:hghg1

is an homeomorphism of G into G, and eG0ϕg(G0), then ϕg(G0)=G0, so G0 is normal.

Two key results for the classification of Lie groups are:
Proposition
Every Lie group has connected components diffeomorphic to the normal subgroup of the identity component.

Proposition
Every connected Lie group G has a simply connected universal covering group G (see section covering group).

The following is a general result used in the context of covering groups:
Proposition
Let G be a connected Lie group and N a discrete normal subgroup of G. Then N is contained in the center Z(G).

Proof
Let gN and consider the map

Fg:GN

such that Fg(h)=h1gh. Since Fg is continuous and G is connected, the image is connected, and since N is discrete, im(Fg)={g}.

And so gh=hg for every hG.

Lie algebra and Lie groups correspondence

For gG we define:

Lg:xgx

and

Rg:xxg

called left and right multiplication respectively.
A vector field in G is left-invariant if d(Lg)p(X(p))=X(gp). That is to say: X(g)=d(Lg)e(X(e)) for all g, and being e the identity of G. Left invariant vector fields are closed under the Lie bracket, so they constitute a Lie algebra gTeG.

We have that:
Theorem(Lie's third theorem). Every finite-dimensional real Lie algebra is the Lie algebra of some simply connected Lie group.

And it can be shown that if two simply connected Lie groups have the same Lie algebra, they are isomorphic.

Given two groups with isomorphic Lie algebras you can only infer that they are isomorphic in some neighborhood of identity. Moreover, they would have the same universal covering group, so both are quotient of the same group by a discrete subgroup.

Proposition. A connected Lie group is abelian if and only if the Lie algebra is abelian (see this).

Proposition. A connected, one-dimensional Lie group G is isomorphic to R or S1 (see this).

Corollary. Every connected 1-dimensional Lie group is commutative.

Parallelizable manifolds

A Lie group is a parallelizable manifold. The tangent spaces at different points can be identified using left translations, so we have TGG×TeG. This is related to the Maurer-Cartan form.

Examples

K={(cosθsinθsinθcosθ)},A={(r001/r):r>0},N={(1x01)}

It can be shown that every element of SL(2) split as product of the elements of these groups. That is,

SL(2)=KAN

This is called Iwasawa decomposition. From here can be concluded that SL(2) is homeomorphic to the interior of a solid torus. See Decomposing SL(2,R) in Calibre.