Well, this comes from probably an older definition of a Lie Algebra, where someone defines for a given Lie Group $G$ its associated Lie Algebra, to be given by
$$
\mathfrak{g}= \{ A \in M_{n \times n}(\mathbb{C}) \thinspace | \thinspace \forall t \in \mathbb{R}: \exp(tA) \in G\}.
$$
So, if you have an action of the Lie group $G$ on a set $V$ (or vector space, module etc.), then this action defines a new one on the same $V$ of the the Lie Algebra this time, given as follows
$$
\begin{split}
\mathfrak{g} \times V &\rightarrow V, \\
(X, u) &\mapsto X.u= \frac{d}{dt}(\exp(tX).u)_{t=0}.
\end{split}
$$
You can check on your own that this is indeed a new action. What you see in the book is essentially this thing, applied into the corresponding Lie Bracket.
Somewhere in here:
http://www.maths.gla.ac.uk/~ajb/dvi-ps/lie-bern.pdf
you can find all the possible questions you can come up with. However, if you need something else please do let me know.