Lie algebra of a Lie group

The tangent space at the identity of a Lie group, equipped with the bracket induced by left-invariant vector fields.
Lie algebra of a Lie group

Let GG be a with identity element ee. Its Lie algebra is the real vector space

g=TeG. \mathfrak{g}=T_eG.

To define the Lie bracket on g\mathfrak{g}, use . For each XTeGX\in T_eG, there is a unique left-invariant X~\widetilde X on GG satisfying X~e=X\widetilde X_e=X, namely

X~g=(dLg)e(X). \widetilde X_g = (\mathrm{d}L_g)_e(X).

The bracket on g\mathfrak{g} is then defined by

[X,Y]:=[X~,Y~]e, [X,Y] := [\widetilde X,\widetilde Y]_e,

where [X~,Y~][\widetilde X,\widetilde Y] is the of vector fields on GG. This operation is bilinear, alternating, and satisfies the Jacobi identity, making g\mathfrak{g} into a Lie algebra in the usual algebraic sense.

Examples

  1. General linear group. For G=GL(n,R)G=\mathrm{GL}(n,\mathbb{R}), one has g=gl(n,R)\mathfrak{g}=\mathfrak{gl}(n,\mathbb{R}) (all n×nn\times n real matrices) with bracket [A,B]=ABBA[A,B]=AB-BA.
  2. Special orthogonal group. For G=SO(n)G=\mathrm{SO}(n), the Lie algebra is so(n)={Agl(n,R)A=A}\mathfrak{so}(n)=\{A\in\mathfrak{gl}(n,\mathbb{R})\mid A^\top=-A\} with the same commutator bracket.
  3. Abelian Lie groups. For G=RnG=\mathbb{R}^n under addition (or a torus TnT^n), the bracket on gRn\mathfrak{g}\cong\mathbb{R}^n is identically zero.