Convention: fundamental vector field uses the right action

The fundamental vector field X-sharp is defined by differentiating the right action p·exp(tX).
Convention: fundamental vector field uses the right action

Let π:PM\pi:P\to M be a with the right action (p,g)pg(p,g)\mapsto p\cdot g as in . Let g\mathfrak g be the of GG.

Convention

For XgX\in\mathfrak g, the fundamental vector field (also called the infinitesimal generator) is the X#Γ(TP)X^\#\in\Gamma(TP) defined by

Xp#  :=  ddtt=0(pexp(tX)),pP. X^\#_p \;:=\; \left.\frac{d}{dt}\right|_{t=0} \big(p\cdot \exp(tX)\big),\qquad p\in P.

With this convention:

  • X#X^\# is vertical and πX#=0\pi_*X^\#=0.
  • The connection 1-form ω\omega satisfies ω(X#)=X\omega(X^\#)=X.
  • Right translation behaves by (Rg)X#=(Ad(g1)X)#(R_g)_*X^\# = (\mathrm{Ad}(g^{-1})X)^\#.

This fixes sign conventions in identities involving of fundamental fields and in the structure equations for connections and curvature.

Examples

  1. Trivial bundle. If P=M×GP=M\times G with right action (x,h)g=(x,hg)(x,h)\cdot g=(x,hg), then at (x,h)(x,h) one has

    X(x,h)#=(0, (Rh)X), X^\#_{(x,h)}=(0,\ (R_h)_*X),

    i.e. the fundamental field points purely along the GG-factor.

  2. Right-invariant fields on GG. On P=GP=G viewed as a principal GG-bundle over a point with right action by right multiplication, X#X^\# is precisely the right-invariant vector field generated by XX.

  3. Sign comparison with a left action. If one instead defined fundamental fields using a left action Lexp(tX)L_{\exp(tX)}, the resulting infinitesimal generator differs by a sign in formulas relating brackets and the adjoint action; the present convention avoids that mismatch for principal bundles written with right actions.