Section of Ad(P)

A smooth choice of an element in each fiber of the adjoint bundle, equivalently a globally defined gauge function with conjugation gluing laws.
Section of Ad(P)

Let Ad(P)M\mathrm{Ad}(P)\to M be the of a principal GG-bundle PP.

A section of Ad(P)\mathrm{Ad}(P) is a smooth map

s:MAd(P) s:M\to \mathrm{Ad}(P)

such that πAds=idM\pi_{\mathrm{Ad}}\circ s=\mathrm{id}_M, where πAd:Ad(P)M\pi_{\mathrm{Ad}}:\mathrm{Ad}(P)\to M is the bundle projection.

Equivalently, choose an {Ui}\{U_i\} and local trivializations of PP with gij:UiUjGg_{ij}:U_i\cap U_j\to G. Then a section ss is represented by smooth maps ai:UiGa_i:U_i\to G such that on overlaps

aj(x)=gij(x)1ai(x)gij(x). a_j(x)=g_{ij}(x)^{-1}\,a_i(x)\,g_{ij}(x).

This is the “gauge function” gluing law: local representatives differ by conjugation with the bundle cocycle.

Under pointwise multiplication in the fibers, the set of sections Γ(Ad(P))\Gamma(\mathrm{Ad}(P)) is a group, canonically isomorphic to the of PP.

Examples

  1. Trivial or trivialized case. If Ad(P)M×G\mathrm{Ad}(P)\cong M\times G, then sections are exactly smooth maps a:MGa:M\to G.
  2. Abelian groups. If GG is abelian, conjugation is trivial, so every section is again just a smooth map MGM\to G, regardless of whether PP is trivial.
  3. Central elements. If zZ(G)z\in Z(G), then the constant choice “zz in every fiber” defines a global section of Ad(P)\mathrm{Ad}(P); it corresponds to the gauge transformation ppzp\mapsto p\cdot z.