Left-Invariant Vector Field

A vector field on a Lie group that is unchanged by all left translations.
Left-Invariant Vector Field

Let GG be a . A XX on GG is left-invariant if for every gGg\in G,

(Lg)X=X, (L_g)_*X = X,

where LgL_g is and (Lg)(L_g)_* denotes the pushforward on vector fields.

Equivalently, for all g,hGg,h\in G,

Xgh=(dLg)h(Xh). X_{gh} = (dL_g)_h(X_h).

Determined by the value at the identity

A left-invariant vector field is completely determined by its value XeTeGX_e\in T_eG. Conversely, every vTeGv\in T_eG defines a unique left-invariant vector field by

Xg:=(dLg)e(v). X_g := (dL_g)_e(v).

Thus the space of left-invariant vector fields is naturally identified with the g=TeG\mathfrak{g}=T_eG.

Lie bracket compatibility

If X~,Y~\widetilde X,\widetilde Y are left-invariant, then so is [X~,Y~][\widetilde X,\widetilde Y], and

[X~,Y~]e=[Xe,Ye] [\widetilde X,\widetilde Y]_e = [X_e,Y_e]

defines the on g\mathfrak{g}.

Flows of left-invariant vector fields yield and are closely related to the .