Integrable horizontal distribution

A horizontal distribution closed under Lie brackets, equivalently tangent to a foliation transverse to the fibers.
Integrable horizontal distribution

Let π:EM\pi:E\to M be a surjective submersion and let HTEH\subset TE be a .

Definition. The horizontal distribution HH is integrable if it is involutive: for any smooth vector fields X,YX,Y on EE taking values in HH (i.e. horizontal vector fields), their [X,Y][X,Y] also takes values in HH.

By the Frobenius theorem, integrability is equivalent to the existence of a foliation of EE by immersed submanifolds whose tangent spaces equal HH. For a horizontal distribution, such leaves are automatically transverse to the fibers, so locally each leaf projects diffeomorphically onto an open subset of MM. In many geometric settings, non-integrability is measured by an appropriate notion of (the “vertical part” of brackets of horizontal fields).

Examples

  1. Product horizontals are integrable. On E=M×FE=M\times F with H(x,f)=TxM{0}H_{(x,f)}=T_xM\oplus\{0\}, the horizontal leaves are the slices M×{f}M\times\{f\}, so HH is integrable.
  2. Flat principal connection gives integrable horizontals. On a principal bundle with a flat connection, the horizontal distribution is involutive; locally, horizontal leaves provide local “parallel” sections.
  3. Non-example from curvature. For the Levi-Civita connection on the frame bundle of a curved Riemannian manifold (e.g. the round sphere), the induced horizontal distribution is typically not integrable; horizontal loops can produce nontrivial holonomy.