Basic forms theorem

Characterizes which differential forms on a principal bundle descend to the base manifold.
Basic forms theorem

Let π:PM\pi:P\to M be a principal GG-bundle with right action Rg:PPR_g:P\to P. A differential form αΩk(P)\alpha \in \Omega^k(P) is called basic if it satisfies:

  1. GG-invariance: Rgα=αfor all gG. R_g^*\alpha = \alpha \quad \text{for all } g\in G.
  2. Horizontality: for every XgX\in \mathfrak{g}, letting X#X^\# denote the corresponding fundamental vertical vector field on PP, ιX#α=0. \iota_{X^\#}\alpha = 0.

Theorem (basic forms theorem)

A form αΩk(P)\alpha \in \Omega^k(P) is basic if and only if there exists a unique form βΩk(M)\beta \in \Omega^k(M) such that

πβ=α. \pi^*\beta = \alpha.

In other words, basic forms are exactly those that “descend” from PP to the base MM.

Why the conditions are exactly right (proof idea)

  • If α=πβ\alpha=\pi^*\beta, then α\alpha is automatically GG-invariant because πRg=π\pi\circ R_g=\pi, and α\alpha is horizontal because π(X#)=0\pi_*(X^\#)=0 for vertical vectors.
  • Conversely, if α\alpha is horizontal and invariant, choose a local section s:UPs:U\to P and define βU:=sα\beta_U := s^*\alpha. On overlaps UVU\cap V, two sections differ by a gauge transformation sV=sUgs_V = s_U \cdot g for a map g:UVGg:U\cap V\to G. Invariance and horizontality imply sUα=sVαs_U^*\alpha = s_V^*\alpha, so the βU\beta_U glue to a global β\beta with πβ=α\pi^*\beta=\alpha.

Example: characteristic forms

If ω\omega is a connection on PP with curvature Ω\Omega, then applying an Ad\mathrm{Ad}-invariant polynomial PP on g\mathfrak{g} produces a real-valued form P(Ω)P(\Omega) that is horizontal and GG-invariant, hence basic, so it descends to MM. Its closedness is proved using the .