Holonomy element from parallel transport around a loop

Definition of the holonomy element in G obtained by transporting a point around a based loop.
Holonomy element from parallel transport around a loop

Let π:PM\pi:P\to M be a with ω\omega. Fix a basepoint xMx\in M and a point pPxp\in P_x. Let γ:[0,1]M\gamma:[0,1]\to M be a loop based at xx, meaning γ(0)=γ(1)=x\gamma(0)=\gamma(1)=x.

Using , pp is carried to another point in the same fiber:

PTγω(p)Px. \mathrm{PT}^\omega_\gamma(p)\in P_x.

Because PxP_x is a right GG-torsor, there is a unique element hγ(p)Gh_\gamma(p)\in G such that

PTγω(p)=phγ(p). \mathrm{PT}^\omega_\gamma(p)=p\cdot h_\gamma(p).

This element is the holonomy element of ω\omega along γ\gamma based at pp.

Changing the basepoint in the fiber conjugates the element: if p=pgp'=p\cdot g, then

hγ(p)=g1hγ(p)g. h_\gamma(p') = g^{-1}\,h_\gamma(p)\,g.

Thus the subgroup {hγ(p)}\{h_\gamma(p)\} depends on pp, but its conjugacy class depends only on xx and defines the at xx.

Examples

  1. If ω\omega is flat and MM is simply connected, then hγ(p)=eh_\gamma(p)=e for all loops, so the holonomy group is trivial.
  2. On the Levi-Civita connection of the round 2-sphere, transporting a tangent frame around a latitude circle yields a nontrivial rotation, giving a nontrivial holonomy element.
  3. For an abelian structure group GG, the conjugation ambiguity disappears, so hγ(p)h_\gamma(p) is independent of the choice of pPxp\in P_x.