Curvature 2-form of a principal connection

A Lie-algebra-valued 2-form measuring the non-integrability of the horizontal distribution of a principal connection.
Curvature 2-form of a principal connection

Let π:PM\pi:P\to M be a principal GG-bundle with connection 1-form ωΩ1(P;g)\omega\in \Omega^1(P;\mathfrak{g}) (see ). The curvature 2-form is the g\mathfrak{g}-valued 2-form

Ω    dω  +  12[ωω]    Ω2(P;g), \Omega \;\coloneqq\; d\omega \;+\; \tfrac12[\omega\wedge \omega] \;\in\; \Omega^2(P;\mathfrak{g}),

where dd is the and [ωω][\omega\wedge\omega] is formed using the on g\mathfrak{g} together with the wedge product of 1-forms.

Key properties:

  • Ω\Omega is horizontal: Ω(X,)=0\Omega(X,\cdot)=0 whenever XX is vertical.
  • Ω\Omega is equivariant: RgΩ=Ad(g1)ΩR_g^*\Omega=\mathrm{Ad}(g^{-1})\Omega.

Consequently, Ω\Omega represents the of the underlying and can be viewed as an ad(P)\mathrm{ad}(P)-valued 2-form on MM after descending from PP.

One conceptual characterization: if X,YX,Y are vector fields on MM and XH,YHX^H,Y^H are their horizontal lifts to PP, then

Ω(XH,YH)=ω([XH,YH]), \Omega(X^H,Y^H) = -\,\omega([X^H,Y^H]),

so Ω\Omega measures the failure of horizontal lifts to close under brackets.

Examples

  1. Maurer–Cartan form is flat. On P=G{}P=G\to\{\ast\} with ω=θ=g1dg\omega=\theta=g^{-1}dg, the Maurer–Cartan equation says dθ+12[θθ]=0d\theta+\tfrac12[\theta\wedge\theta]=0. Hence Ω=0\Omega=0.

  2. Curvature in a trivialization. On U×GUU\times G\to U with ω=Ad(g1)A+g1dg\omega=\mathrm{Ad}(g^{-1})A+g^{-1}dg, one computes

    Ω=Ad(g1)πU ⁣(dA+12[AA]), \Omega = \mathrm{Ad}(g^{-1})\,\pi_U^*\!\left(dA+\tfrac12[A\wedge A]\right),

    so the entire curvature is pulled back from the base.

  3. Abelian structure group. If GG is abelian, then [ωω]=0[\omega\wedge\omega]=0 and Ω=dω\Omega=d\omega. In particular for principal U(1)U(1)-bundles the curvature is just the exterior derivative of the connection form.