Let G be a Lie group
with identity element e, and let g=TeG be its Lie algebra
.
Definition (Lie group exponential).
For each X∈g, there exists a unique smooth group homomorphism
γX:(R,+)⟶Gsuch that γX(0)=e and γX′(0)=X (viewing X as a tangent vector in TeG). The exponential map of G is the smooth map
expG:g⟶G,expG(X)=γX(1).Equivalently, γX(t)=expG(tX) is the integral curve through e of the left-invariant vector field
determined by X, defined using left translations
.
Basic properties.
- expG(0)=e and (dexpG)0=idg.
- The curve t↦expG(tX) is a one-parameter subgroup: expG((s+t)X)=expG(sX)expG(tX).
- If X,Y∈g commute (i.e. [X,Y]=0 for the Lie bracket
), then expG(X+Y)=expG(X)expG(Y).
- If φ:G→H is a Lie group homomorphism
, then φ intertwines exponentials via the induced Lie algebra homomorphism
:
φ(expG(X))=expH(dφe(X)).
Examples
Additive group (Rn,+).
Here G=Rn is a Lie group under addition, g≅Rn, and the one-parameter subgroup with velocity X is γX(t)=tX. Thus expG(X)=X (the identity map).
Circle group S1⊂C.
With multiplication in C, G=S1 has Lie algebra g=T1S1=iR. The exponential map is the usual complex exponential restricted to iR:
expS1(iθ)=eiθ.Matrix Lie groups.
If G⊆GL(n,R) is a matrix Lie group, then g⊆Mn(R), and expG is given by the matrix exponential:
expG(A)=k=0∑∞k!Ak.For example, in SO(2) this recovers rotations, and in GL(n,R) it produces invertible matrices for all A.