Bi-invariant differential form

A differential form on a Lie group invariant under both left and right translations.
Bi-invariant differential form

Let GG be a . For gGg\in G, write LgL_g and RgR_g for and .

Definition. A differential kk-form ωΩk(G)\omega\in \Omega^k(G) is bi-invariant if

Lgω=ωandRgω=ωfor all gG. L_g^*\omega=\omega \quad\text{and}\quad R_g^*\omega=\omega \qquad \text{for all } g\in G.

Equivalently, ω\omega is both and .

Characterization (connected case). If GG is connected, a left-invariant form is determined by its value at the identity ee, i.e. by an alternating multilinear map ωe:kgk\omega_e:\wedge^k\mathfrak{g}\to \Bbbk. Such a form is bi-invariant if and only if ωe\omega_e is invariant under the :

ωe(AdgX1,,AdgXk)=ωe(X1,,Xk)for all gG. \omega_e(\mathrm{Ad}_g X_1,\dots,\mathrm{Ad}_g X_k)=\omega_e(X_1,\dots,X_k)\quad\text{for all }g\in G.

Motivation. Bi-invariant forms capture intrinsic geometry on GG compatible with both left and right symmetries. For example, a determines a bi-invariant volume form, and Ad-invariant forms on g\mathfrak{g} are the starting point for Chern–Weil constructions on homogeneous spaces.