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.
A Lie group is a group G equipped with the structure of a smooth manifold such that the group operations are smooth maps:
μ:G×G→G,μ(g,h)=gh,ι:G→G,ι(g)=g−1.
For each g∈G, the left translationLg(h)=gh and the right translationRg(h)=hg are diffeomorphisms of G, with inverses Lg−1 and Rg−1. The tangent space at the identity TeG carries a canonical Lie algebra structure, called the Lie algebra of G, and the exponential map relates this infinitesimal structure to local group behavior near e.
A Lie bracket on a real vector space g is a bilinear map
[,]:g×g→g
such that:
Alternating / skew-symmetry:[X,X]=0 for all X∈g (equivalently [X,Y]=−[Y,X]).
Jacobi identity: for all X,Y,Z∈g,
[X,[Y,Z]]+[Y,[Z,X]]+[Z,[X,Y]]=0.
In differential geometry, there is a canonical Lie bracket on the space of vector fields on a smooth manifoldM: for vector fields X,Y define [X,Y] by its action on smooth functions,
[X,Y](f):=X(Y(f))−Y(X(f)),f∈C∞(M).
This produces another vector field and turns the space of vector fields into a Lie algebra.
Using the standard identification of the Lie algebra of a Lie group with the tangent space at the identity, we view this as a linear map
dφeG:g→h.
Theorem (Lie algebra homomorphism induced by φ). Let φ:G→H be a Lie group homomorphism. Then the differential at the identity dφeG:g→h is a homomorphism of Lie algebras, meaning it preserves the Lie bracket:
It is also functorial: if ψ:H→K is another Lie group homomorphism, then
d(ψ∘φ)eG=dψeH∘dφeG.
Examples
Inclusion of a Lie subgroup. If i:H↪G is the inclusion of a Lie subgroup, then dieH:h→g is the natural inclusion of tangent spaces at the identity. Concretely, it identifies h as a Lie subalgebra of g.
Determinant on GL(n,R). The determinant is a Lie group homomorphism det:GL(n,R)→R×. Identifying gl(n,R)≅Mn(R), the induced map on Lie algebras is
d(det)I(A)=tr(A),
and more generally d(det)B(V)=det(B)tr(B−1V).
Covering map R→S1. The map φ:R→S1⊂C, φ(t)=eit, is a Lie group homomorphism (additive to multiplicative). Then dφ0:R→T1S1 sends a↦ia (since dtdeitt=0=i). Under the common identification T1S1≅R via a↦ia, this differential is the identity.
(Rn,+). For the additive Lie group, La(x)=a+x. The differential (dLa)x is the identity map on Rn for every x.
Matrix groups. If G⊆GL(n,R), then LA(B)=AB. Identifying TBG with an appropriate subspace of matrices, (dLA)B acts by left multiplication:
(dLA)B(V)=AV.
Circle group S1. Writing elements as complex numbers of unit modulus, Leiθ(eit)=ei(θ+t). Geometrically, left translation rotates the circle by angle θ.