Let π:P→M\pi:P\to M be a with Lie algebra g\mathfrak{g}. The is the vector bundle

ad(P)≔P×Adg  →  M,\mathrm{ad}(P)\coloneqq P\times_{\mathrm{Ad}} \mathfrak{g}\;\to\;M,

associated to the adjoint action of GG on g\mathfrak{g}.

A on PP induces a connection ∇\nabla on ad(P)\mathrm{ad}(P) (equivalently, it induces the operator on tensorial forms described by ). The covariant exterior derivative

d∇:Ωk(M;ad(P))→Ωk+1(M;ad(P))d_\nabla:\Omega^k(M;\mathrm{ad}(P))\to \Omega^{k+1}(M;\mathrm{ad}(P))

is the of ∇\nabla, defined by the Koszul formula: for α∈Ωk(M;ad(P))\alpha\in \Omega^k(M;\mathrm{ad}(P)) and vector fields X0,…,XkX_0,\dots,X_k,

(d∇α)(X0,…,Xk)=∑i=0k(−1)i ∇Xi(α(X0,…,Xi^,…,Xk))+∑0≤i<j≤k(−1)i+j α([Xi,Xj],X0,…,Xi^,…,Xj^,…,Xk),\begin{aligned} (d_\nabla \alpha)(X_0,\dots,X_k) &= \sum_{i=0}^k (-1)^i\,\nabla_{X_i}\bigl(\alpha(X_0,\dots,\widehat{X_i},\dots,X_k)\bigr) \\ &\quad + \sum_{0\le i<j\le k} (-1)^{i+j}\,\alpha([X_i,X_j],X_0,\dots,\widehat{X_i},\dots,\widehat{X_j},\dots,X_k), \end{aligned}

where the bracket is the of vector fields on MM.

Locally, if A∈Ω1(U;g)A\in \Omega^1(U;\mathfrak{g}) is a local connection form and we identify ad(P)∣U≅U×g\mathrm{ad}(P)|_U\cong U\times \mathfrak{g}, then for α∈Ωk(U;g)\alpha\in \Omega^k(U;\mathfrak{g}),

d∇α=dα+[A∧α],d_\nabla \alpha = d\alpha + [A\wedge \alpha],

with dd the .

Examples
  1. Sections of ad(P)\mathrm{ad}(P) (degree 0). For ϕ∈Ω0(M;ad(P))\phi\in \Omega^0(M;\mathrm{ad}(P)), locally ϕ:U→g\phi:U\to\mathfrak{g}, one has
    d∇ϕ=dϕ+[A,ϕ],d_\nabla \phi = d\phi + [A,\phi],
    which is the usual covariant derivative in the adjoint representation.
  1. Bianchi identity on the base. Let F∈Ω2(U;g)F\in \Omega^2(U;\mathfrak{g}) be the local curvature 2-form. Then
    d∇F=0d_\nabla F = 0
    is the Bianchi identity written as a covariant closure condition.
  1. Abelian structure group. If GG is abelian, then [A∧α]=0[A\wedge \alpha]=0 for all α\alpha, so d∇d_\nabla reduces to the ordinary exterior derivative on g\mathfrak{g}-valued forms.