SO(2,1) - Haar measure, exponential map

Click For Summary
SUMMARY

The discussion centers on the group SO(2,1) and its properties regarding the exponential map and Haar measure. It is established that the exponential map is surjective for the connected component SO^+(2,1), as referenced in Nishikawa's work. The Haar measure can be constructed using the Maurer-Cartan 1-form, which involves the Lie algebra's elements generating 1-parameter subgroups. Additionally, the group SO(2,1) is isomorphic to SL(2,ℝ), allowing for further geometric interpretations related to the hyperbolic plane.

PREREQUISITES
  • Understanding of Lie groups and Lie algebras
  • Familiarity with the exponential map in the context of differential geometry
  • Knowledge of Haar measure and its applications in group theory
  • Concept of path connectedness in topological spaces
NEXT STEPS
  • Study the properties of the Maurer-Cartan 1-form in Lie groups
  • Explore the implications of the exponential map in non-compact groups
  • Research the relationship between SO(2,1) and SL(2,ℝ) in detail
  • Investigate the topology of the unit tangent bundle of the hyperbolic plane
USEFUL FOR

Mathematicians, physicists, and students studying group theory, differential geometry, and the geometry of hyperbolic spaces.

Bobhawke
Messages
142
Reaction score
0
I wasn't quite sure where to put this, so here goes:

I am trying to find out some facts about the group SO(2,1). Specifically; Is the exponential map onto? If so, can the Haar measure be written in terms of the Lebesgue integral over a suitable subset of the Lie algebra? What is that subset?

If the exponential map isn't onto, then for what subset of the Lie algebra is it at least 1-1 (injective)?

I was hoping there would be a reference out there that explained these things, but have so far been unable to find it.

Thank you.
 
Physics news on Phys.org
SO(2,1) is not connected. There is a component that is connected to the identity, called ##SO^+(2,1)##, for which the exponential map is surjective. This is assumed in all of the physics literature on the Lorentz group, but I am at a loss to come up with a simple convincing proof at the moment. The surjectivity is claimed as a result of Nishikawa in prop 1.6 in http://www.heldermann-verlag.de/jlt/jlt07/DOKHOFPL.PDF.

Since the exponential map is surjective, you should be able to use the Maurer-Cartan 1-form ##\omega= g^{-1} dg## to build the Haar measure using the appropriate angle and real parameters.
 
Could you say something like: Each element of the Lie algebra generates a 1-parameter subgroup in the connected part of the group, and locally the basis elements of the Lie algebra take you in orthogonal directions. Therefore you can string together a series of curves which take you from the origin to any point which it is path connected?
 
Bobhawke said:
Could you say something like: Each element of the Lie algebra generates a 1-parameter subgroup in the connected part of the group, and locally the basis elements of the Lie algebra take you in orthogonal directions. Therefore you can string together a series of curves which take you from the origin to any point which it is path connected?

What you say is true for compact groups. It may also be true for the connected components of matrix groups. I'm not familiar enough with the esoteric details to say with 100% confidence. The counter-examples to surjectivity for matrix groups that I've found in the literature all seem to be related to disconnectedness. On the other hand I know that for diffeomorphism groups, the exponential map is not generally surjective, and this is directly related to noncompactness, rather than disconnectedness.

For SO(2,1) we have some extra tricks available, since it is isomorphic to ##SL(2,\mathbb{R})##. The connected component is ##PSL(2,\mathbb{R})=SL(2,\mathbb{R})/\{\pm I\}##. So we can use the fact that the geometry is that of the unit tangent bundle of the hyperbolic (upper-half) plane (see http://en.wikipedia.org/wiki/SL2(R)#Topology_and_universal_cover).
 

Similar threads

  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 4 ·
Replies
4
Views
610
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 3 ·
Replies
3
Views
959
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 4 ·
Replies
4
Views
4K
  • · Replies 12 ·
Replies
12
Views
2K
  • · Replies 3 ·
Replies
3
Views
4K