Let π:P→M\pi:P\to M be a with GG, and let ρ:G→GL(V)\rho:G\to \mathrm{GL}(V) be a on a vector space VV.

Form the E:=P×GVE := P\times_G V (using the ).

Assume PP is equipped with a (equivalently, a ω\omega on PP). Let H⊂TPH\subset TP denote the associated .

Construction (horizontal differentiation)

A s∈Γ(E)s\in\Gamma(E) can be represented by a smooth ρ\rho-equivariant map f:P→Vf:P\to V satisfying

f(p⋅g)=ρ(g−1) f(p).f(p\cdot g)=\rho(g^{-1})\,f(p).

Given a vector field XX on MM and a point x∈Mx\in M, pick p∈Pxp\in P_x and let X~p∈Hp\widetilde{X}_p\in H_p be the of XxX_x at pp. Define

(∇Xs)(x):=[ p,  dfp(X~p) ]∈Ex.(\nabla_X s)(x) := [\,p,\; df_p(\widetilde{X}_p)\,]\in E_x.

Why this is well-defined

  • If pp is replaced by p⋅gp\cdot g, then X~p⋅g=(dRg)p(X~p)\widetilde{X}_{p\cdot g} = (dR_g)_p(\widetilde{X}_p) because the horizontal distribution is GG-invariant.
  • Using the equivariance f(p⋅g)=ρ(g−1)f(p)f(p\cdot g)=\rho(g^{-1})f(p) and differentiating along a horizontal direction shows that dfp⋅g(X~p⋅g)df_{p\cdot g}(\widetilde{X}_{p\cdot g}) represents the same element of the fiber quotient P×GVP\times_G V.

The operator s↦∇ss\mapsto \nabla s is a EE, and it satisfies the Leibniz rule (see ). In particular, this construction is the section-level version of .

Local formula

Choose a local section s0:U→Ps_0:U\to P. Writing a section of EE as s(x)=[s0(x),v(x)]s(x)=[s_0(x),v(x)] with v:U→Vv:U\to V, let

A:=s0∗ω∈Ω1(U;g)A := s_0^*\omega \in \Omega^1(U;\mathfrak g)

be the . Let ρ∗:g→End(V)\rho_*:\mathfrak g\to \mathrm{End}(V) be the induced Lie algebra representation (obtained by differentiating ρ\rho, as in ). Then locally,

∇v=dv+ρ∗(A) v.\nabla v = dv + \rho_*(A)\,v.
Examples
  1. Trivial bundle with a matrix-valued potential. For P=U×GP=U\times G and E=U×VE=U\times V, a choice of A∈Ω1(U;g)A\in\Omega^1(U;\mathfrak g) produces
    ∇=d+ρ∗(A).\nabla = d + \rho_*(A).
    If A=0A=0 this reduces to the ordinary derivative and corresponds to the .
  1. Adjoint bundle. Take V=gV=\mathfrak g with ρ=Ad\rho=\mathrm{Ad}. Then EE is the Ad(P)\mathrm{Ad}(P). In a local trivialization with local connection form AA, the induced covariant derivative on a section ϕ\phi of Ad(P)\mathrm{Ad}(P) has the familiar form
    ∇ϕ=dϕ+[A,ϕ],\nabla \phi = d\phi + [A,\phi],
    which underlies the .
  1. Tangent bundle from the frame bundle. Let P=Fr(TM)P=\mathrm{Fr}(TM) be the and let V=RnV=\mathbb R^n with the standard representation of GL(n,R)\mathrm{GL}(n,\mathbb R). Then TM≅P×GL(n)RnTM\cong P\times_{\mathrm{GL}(n)}\mathbb R^n, and a principal connection on PP induces the usual covariant derivative on vector fields. In the Riemannian case, choosing the orthonormal frame bundle and its connection recovers the .