I am reading the proof of the equivalence between the Lie derivative and the Lie bracket. We define the Lie derivative $\mathcal{L}_X Y$ as $F'(0)$ where $F(t)=\Phi_{{-t}_{*\Phi_t(p)}}(Y_ {{\Phi_t(p)}})$ and $\Phi_t$ is the local flow of $X$ in a neighbourhood of $X$.
The proof is separated in cases. I don't understand the case where $X(p)=0$ but $X$ is not identically zero. The author says that there is a continuity argument over $[X,Y]$ and $\mathcal{L}_X Y$ that proves the result, but which is that argument?