Let π:P→M\pi:P\to M be a equipped with a ω\omega, and let H:=ker⁡ω⊂TPH:=\ker\omega\subset TP be its .

A smooth curve γ~:I→P\widetilde\gamma:I\to P is horizontal if ω(γ~˙(t))=0\omega(\dot{\widetilde\gamma}(t))=0 for all t∈It\in I (equivalently, γ~˙(t)∈Hγ~(t)\dot{\widetilde\gamma}(t)\in H_{\widetilde\gamma(t)}).

Theorem (horizontal lifting). Let γ:I→M\gamma:I\to M be a smooth curve and fix t0∈It_0\in I and p0∈Pp_0\in P with π(p0)=γ(t0)\pi(p_0)=\gamma(t_0). Then there exists a unique horizontal curve γ~:I→P\widetilde\gamma:I\to P such that

π∘γ~=γ,γ~(t0)=p0.\pi\circ \widetilde\gamma = \gamma,\qquad \widetilde\gamma(t_0)=p_0.

This construction is the input for defining on principal and associated bundles.

Equivalent characterizations

Equivalently, γ~\widetilde\gamma is the unique solution to the first-order ODE requiring that dπ(γ~˙)=γ˙d\pi(\dot{\widetilde\gamma})=\dot\gamma and γ~˙\dot{\widetilde\gamma} lies in the horizontal subspace.

Examples
  1. If P=M×GP=M\times G is trivial and ω\omega is given by a local gauge potential AA on MM, then the horizontal lift equation becomes an ODE for a curve in GG driven by A(γ˙)A(\dot\gamma).
  2. For the orthonormal frame bundle of a with Levi-Civita connection, horizontal lifts are precisely parallel frames along γ\gamma.
  3. If γ\gamma is constant, the unique horizontal lift with initial value p0p_0 is the constant curve at p0p_0.