ConceptComplete

Principal Bundles and Ehresmann Connections

Principal bundles provide the natural framework for connections in their full generality. The theory unifies Riemannian geometry, gauge theory, and the geometry of fiber bundles.


Principal Bundles

Definition7.8Principal $G$-bundle

Let GG be a Lie group. A principal GG-bundle over MM is a smooth fiber bundle π:P→M\pi: P \to M with a free right GG-action P×G→PP \times G \to P such that:

  1. The action preserves fibers: Ο€(pβ‹…g)=Ο€(p)\pi(p \cdot g) = \pi(p).
  2. The orbit space P/GP/G is diffeomorphic to MM via Ο€\pi.
  3. PP is locally trivial: each point of MM has a neighborhood UU with Ο€βˆ’1(U)β‰…UΓ—G\pi^{-1}(U) \cong U \times G equivariantly.
ExampleFrame bundle

The frame bundle Fr(M)β†’M\mathrm{Fr}(M) \to M of an nn-manifold has fiber over pp consisting of all ordered bases (frames) of TpMT_pM. It is a principal GL(n,R)\mathrm{GL}(n, \mathbb{R})-bundle. For a Riemannian manifold, the orthonormal frame bundle is a principal O(n)O(n)-bundle.


Ehresmann Connections

Definition7.9Ehresmann connection

An Ehresmann connection on a principal GG-bundle Pβ†’MP \to M is a GG-equivariant distribution HβŠ‚TPH \subset TP (the horizontal distribution) complementary to the vertical subbundle V=ker⁑(dΟ€)V = \ker(d\pi):

TpP=VpβŠ•HpforΒ allΒ p∈P,T_pP = V_p \oplus H_p \quad \text{for all } p \in P,

with Hpβ‹…g=(Rg)βˆ—HpH_{p \cdot g} = (R_g)_* H_p (GG-equivariance).

Definition7.10Connection 1-form

Equivalently, an Ehresmann connection is a g\mathfrak{g}-valued 1-form Ο‰βˆˆΞ©1(P;g)\omega \in \Omega^1(P; \mathfrak{g}) satisfying:

  1. Ο‰(A#)=A\omega(A^\#) = A for all A∈gA \in \mathfrak{g}, where A#A^\# is the fundamental vector field.
  2. Rgβˆ—Ο‰=Ad(gβˆ’1)Ο‰R_g^*\omega = \mathrm{Ad}(g^{-1})\omega (GG-equivariance).

The horizontal space is Hp=ker⁑(Ο‰p)H_p = \ker(\omega_p).


Associated Bundles and Induced Connections

Definition7.11Associated vector bundle

Given a principal GG-bundle Pβ†’MP \to M and a representation ρ:Gβ†’GL(V)\rho: G \to \mathrm{GL}(V), the associated vector bundle is E=PΓ—GV=(PΓ—V)/GE = P \times_G V = (P \times V)/G, where GG acts by (p,v)β‹…g=(pβ‹…g,ρ(gβˆ’1)v)(p, v) \cdot g = (p \cdot g, \rho(g^{-1})v).

Theorem7.3Correspondence of connections

There is a bijection between connections on a principal GG-bundle PP and connections on any associated vector bundle E=PΓ—GVE = P \times_G V. The Levi-Civita connection on a Riemannian manifold corresponds to a connection on the orthonormal frame bundle.

ExampleLine bundles and $U(1)$ connections

A Hermitian line bundle Lβ†’ML \to M is associated to a principal U(1)U(1)-bundle. A connection on LL is locally a 1-form A∈Ω1(U)A \in \Omega^1(U) (the vector potential), and the curvature is F=dAF = dA, a closed 2-form. The first Chern class c1(L)=[F2Ο€]∈H2(M;Z)c_1(L) = [\frac{F}{2\pi}] \in H^2(M; \mathbb{Z}) is a topological invariant.

RemarkChern-Weil theory

Given a connection Ο‰\omega on a principal GG-bundle with curvature Ξ©\Omega, and an Ad\mathrm{Ad}-invariant polynomial PP on g\mathfrak{g}, the form P(Ξ©)∈Ω2k(M)P(\Omega) \in \Omega^{2k}(M) is closed, and its cohomology class is independent of the connection. This produces characteristic classes: Chern classes (for U(n)U(n)-bundles), Pontryagin classes (for O(n)O(n)-bundles), and the Euler class (for oriented bundles). These are topological invariants of the bundle computed from any connection.