Invariant differential form

A differential form preserved by pullback under a Lie group action.
Invariant differential form

Let GG act on a manifold MM by a .

A ωΩk(M)\omega\in \Omega^k(M) is GG-invariant if for every gGg\in G,

(Φg)ω=ω, (\Phi_g)^*\omega = \omega,

where Φg:MM\Phi_g:M\to M is the diffeomorphism xgxx\mapsto g\cdot x.

If GG is connected, this is equivalent to infinitesimal invariance: for every XX in the Lie algebra, the Lie derivative satisfies LXMω=0\mathcal{L}_{X_M}\omega=0, where XMX_M is the vector field generated by XX.

Invariant forms form a subcomplex of the de Rham complex: if ω\omega is invariant, then so is .

Examples

  1. Left-invariant forms on a Lie group. For M=GM=G with the left translation action, any left-invariant 1-form (and its wedge products) is GG-invariant.
  2. Volume on the sphere. The standard volume form on SnS^n is invariant under the natural SO(n+1)SO(n+1)-action.
  3. Basic forms are invariant. Any on a principal bundle is invariant under the principal right action by definition.