The connection form evaluates to the generating Lie algebra element on each fundamental vector field.
Let π:P→M be a principal G-bundle and let ω∈Ω1(P;g) be a connection 1-form.
For X∈g, the fundamental vector fieldX# is the vector field on P defined by
Xp#:=dtdt=0(p⋅exp(tX)).
The reproduction property is the requirement that
ω(X#)=Xfor all X∈g.
This condition says that ω restricts on each vertical space Vp=ker(dπp) to the canonical identification Vp≅g coming from the infinitesimal right action.
ExamplesOpen
Maurer–Cartan form on a Lie group. For the principal bundle G→{∗} (right action by multiplication), the left Maurer–Cartan form θ=g−1dg satisfies θ(X#)=X because g−1dtd(gexp(tX))∣0=X.
Trivial bundle U×G. With ω=Ad(g−1)A+g−1dg as in a standard trivialization, a purely vertical vector at (x,g) has the form (0,(Rg)∗X), and one checks ω(0,(Rg)∗X)=X.
The abelian case U(1). Identify u(1)≅iR. If ∂θ denotes the fundamental field for the standard U(1)-action, the reproduction property is ω(∂θ)=1 (after the usual identification of iR with R).
Definition. A (smooth) vector field on M is a smooth map X:M→TM such that π∘X=idM. Equivalently, X is a smooth section of the tangent bundle, assigning to each p∈M a tangent vector
Xp∈TpM
(where TpM is the tangent space at p) in a way that is smooth in local coordinates.
A vector field can also be viewed as a derivation on smooth functions: for each X and each f∈C∞(M), one obtains a smooth function X(f)∈C∞(M) defined by differentiating f in the direction X. Using the pairing between tangent and cotangent spaces (see the cotangent bundle), this can be written pointwise as