Flatness implies holonomy depends only on homotopy class of loops

For a flat connection, holonomy around a loop depends only on the loop's based homotopy class.
Flatness implies holonomy depends only on homotopy class of loops

Let π:PM\pi:P\to M be a with a ω\omega. Fix a basepoint xMx\in M and a point pPxp\in P_x. For a piecewise smooth loop γ\gamma based at xx, horizontal lifting gives an element Holp(γ)G\mathrm{Hol}_{p}(\gamma)\in G, and the subgroup generated by such elements is the at pp. Let Ω\Omega denote the of ω\omega.

Proposition (homotopy invariance of holonomy under flatness)

If Ω=0\Omega=0, then for any two piecewise smooth loops γ0,γ1\gamma_0,\gamma_1 based at xx that are homotopic through based loops, one has

Holp(γ0)=Holp(γ1). \mathrm{Hol}_{p}(\gamma_0)=\mathrm{Hol}_{p}(\gamma_1).

Consequently, the assignment [γ]Holp(γ)[\gamma]\mapsto \mathrm{Hol}_{p}(\gamma) defines a group homomorphism

π1(M,x)G, \pi_1(M,x)\longrightarrow G,

and changing the choice of pPxp\in P_x conjugates this homomorphism by an element of GG.

This is the precise sense in which a flat connection has “holonomy depending only on homotopy class.”

Examples

  1. Trivial flat connection. On P=M×GP=M\times G with the zero connection, every loop has holonomy eGe\in G, so the induced homomorphism π1(M,x)G\pi_1(M,x)\to G is trivial.
  2. Flat U(1)U(1)-connections on S1S^1. For a connection with constant local 1-form A=λdθA=\lambda\,d\theta (in a global gauge), curvature is zero and holonomy sends the generator of π1(S1)Z\pi_1(S^1)\cong \mathbb Z to e2πiλU(1)e^{2\pi i\lambda}\in U(1); dependence is only on the winding number.
  3. Möbius bundle as O(1)O(1)-bundle. The Möbius line bundle corresponds to a principal O(1){±1}O(1)\cong\{\pm 1\}-bundle with a flat connection whose holonomy representation sends the generator of π1(S1)\pi_1(S^1) to 1-1.