Let GG be a . In this convention, a is a π:P→M\pi:P\to M equipped with a right smooth action

R:P×G→P,(p,g)↦p⋅g,R: P\times G\to P,\qquad (p,g)\mapsto p\cdot g,

which is free and transitive on each fiber, with M≅P/GM\cong P/G.

Consequences for formulas

All equivariance conditions are written with respect to this right action. In particular, for a 11-form ω∈Ω1(P;g)\omega\in\Omega^1(P;\mathfrak g) and g∈Gg\in G, the convention is

(Rg)∗ω=Ad(g−1) ω,(R_g)^*\omega=\mathrm{Ad}(g^{-1})\,\omega,

and the induced vertical identification uses fundamental vector fields defined from the right action (see ).

This convention fixes the sign choices appearing in curvature and covariant differentiation identities.

Examples
  1. Frame bundle. For a rank-nn vector bundle E→ME\to M, the frame bundle P=Fr⁡(E)P=\operatorname{Fr}(E) carries a natural right GL⁡(n,R)\operatorname{GL}(n,\mathbb R)-action by postcomposition: (u,g)↦u∘g(u,g)\mapsto u\circ g.
  1. Transition functions from local sections. If si,sj:U→Ps_i,s_j:U\to P are local sections, the transition map gij:U→Gg_{ij}:U\to G is defined by sj=si⋅gijs_j=s_i\cdot g_{ij}.
  1. Gauge transformations. A gauge transformation Φ:P→P\Phi:P\to P satisfies Φ(p⋅g)=Φ(p)⋅g\Phi(p\cdot g)=\Phi(p)\cdot g.