Let GG be a with identity element ee. The Lie algebra of GG is the

g:=TeG.\mathfrak{g} := T_eG.
How the bracket is defined

Using Lg(h)=ghL_g(h)=gh, any XTeGX\in T_eG determines a unique X~\widetilde X by

X~g:=(dLg)e(X)TgG.\widetilde X_g := (dL_g)_e(X)\in T_gG.

Then the Lie bracket on g\mathfrak{g} is defined by

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

where [X~,Y~][\widetilde X,\widetilde Y] is the commutator of .

Properties
Exponential and one-parameter subgroups

The exp:gG\exp:\mathfrak{g}\to G satisfies that texp(tX)t\mapsto \exp(tX) is a for each XgX\in\mathfrak{g}, forming a central part of the .