Horizontal lift of a curve

A curve in the total space projecting to a base curve and whose velocity is everywhere horizontal.
Horizontal lift of a curve

Let π:EM\pi:E\to M be a surjective submersion equipped with an with horizontal subspaces HeETeEH_eE\subset T_eE.

Let γ:IM\gamma:I\to M be a from an interval IRI\subset\mathbb R, and fix t0It_0\in I and e0Ee_0\in E with π(e0)=γ(t0)\pi(e_0)=\gamma(t_0).

Definition. A horizontal lift of γ\gamma through e0e_0 is a curve γ~:JE\widetilde\gamma:J\to E defined on an interval JIJ\subset I containing t0t_0 such that:

  1. πγ~=γJ\pi\circ \widetilde\gamma=\gamma|_J, and
  2. γ~˙(t)Hγ~(t)E\dot{\widetilde\gamma}(t)\in H_{\widetilde\gamma(t)}E for all tJt\in J.

Standard existence/uniqueness results for ordinary differential equations imply: given an Ehresmann connection, such a lift exists and is unique on some (possibly smaller) interval around t0t_0, and extends uniquely to a maximal interval.

Horizontal lifts are the basic input for defining .

Examples

  1. Product bundle. In E=M×FE=M\times F with product horizontals, the horizontal lift through (γ(t0),f0)(\gamma(t_0),f_0) is γ~(t)=(γ(t),f0)\widetilde\gamma(t)=(\gamma(t),f_0): the fiber component stays constant.
  2. Principal bundle lift. On a principal bundle with connection, the horizontal lift of γ\gamma starting at p0Pγ(t0)p_0\in P_{\gamma(t_0)} is the unique path in PP projecting to γ\gamma whose tangent vectors lie in the connection’s horizontal spaces.
  3. Vector bundle interpretation. For a vector bundle with linear connection, a horizontal lift of γ\gamma in the total space corresponds to a vector-valued curve v(t)Eγ(t)v(t)\in E_{\gamma(t)} satisfying the parallel-transport ODE along γ\gamma (so that v(t)v(t) is a parallel section along the curve).