Horizontal lift of a vector field

The unique horizontal vector field on the total space that projects to a given vector field on the base.
Horizontal lift of a vector field

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

Let XX be a on MM. Since dπe:HeETπ(e)Md\pi_e:H_eE\to T_{\pi(e)}M is an isomorphism for each ee, one can lift XX pointwise and obtain a vector field on EE.

Definition. The horizontal lift of XX is the unique vector field XhX^{\mathrm h} on EE such that:

  1. Xh(e)HeEX^{\mathrm h}(e)\in H_eE for every eEe\in E, and
  2. dπe(Xh(e))=X(π(e))d\pi_e(X^{\mathrm h}(e)) = X(\pi(e)) for every eEe\in E.

Equivalently, Xh(e)X^{\mathrm h}(e) is the Xπ(e)X_{\pi(e)} at ee, for each ee.

Examples

  1. Product bundle. On E=M×FE=M\times F with product horizontals, the horizontal lift of XX is (X,0)(X,0): it differentiates in the base direction and does nothing in the fiber direction.
  2. Horizontal lift on a principal bundle. Given a principal connection on PMP\to M, the lift XhX^{\mathrm h} is the unique GG-equivariant vector field on PP that is everywhere horizontal and π\pi-related to XX.
  3. Lift to the tangent bundle. For an affine connection on TMMTM\to M, the horizontal lift of XX is a vector field on TMTM describing infinitesimal parallel translation of tangent vectors along the flow of XX.