Suppose $\pi:P\rightarrow M$ is a principal bundle, $\omega\in \Omega^1(P;\mathfrak{g})$ is the connection one form and $\sigma(\cdot)$ is the fundamental vector field associated to some vector field in $\mathfrak{g}$. That is, for $X\in \mathfrak{g}$, the value of $\sigma(X)$ at $p\in P$ is given by
$ \begin{align*} \sigma(X)_p=\frac{d}{dt}\bigg|_{t=0}p\exp(tX). \end{align*}$
I am reading through some lecture notes at the moment and the author decomposes a vector field $u\in \mathfrak{X}(P)$ in to its horizontal and vertical components. So
$u=u_v + u_h$.
The author then takes the derivative $u_v f$ of some function $f$ defined on $P$. They make the argument that since this derivative at a point $p\in P$ depends only on the vector $u_v$ at $p$, they may assume $u_v = \sigma(\omega(u))$. I understand the idea of the derivative only depending on the vector at $p$. However, I am stuck on how they can assume that $u_v=\sigma(\omega(u))$. I don't understand how $u_v$ at $p$ is equal to $\sigma(\omega(u))$ at $p$. If anyone could help that would be greatly appreciated. Thanks!
EDIT:
Thanks very much for your detailed response. I have a few questions
1) Why have you written that map as $\rho_p$ instead of $L_p$? Isn't it just left multiplication? On that note, is it kosher to define left multiplication on $P$?
2)Is the reason $\sigma(X)_p=(\rho_p)_{*,e}X$
because $X=\frac{d}{dt}\big|_{t=0}\exp(tX)$,
so
$(\rho_p)_{*,e}X=(\rho_p)_{*,e}\frac{d}{dt}\big|_{t=0}\exp(tX)=\frac{d}{dt}\big|_{t=0}p\exp(tX)=\sigma(X)_p$??
3) Why does $R_g$ and $\delta_g$ being diffeomorphisms imply $\rho_p$ has constant rank? Why did you go to the effort of adding $g$ and $g^{-1}$?
4) Why does dim$V_p$=dim$\mathfrak{g}$ imply the map is surjective? I'm thinking that's just something from linear algebra I'm forgetting?
Thank you again!
It is true that $u_v(p) = \sigma(\omega(u_p))_p$. This is because since $u_v(p)$ is vertical, it is equal to $\sigma(X)_p$ for some $X\in \mathfrak g$. But $X = \omega(\sigma(X)_p) = \omega(u_v(p))$.