First we will define
$$
\frac{\partial}{\partial z} = \frac{1}{2}\left(\frac{\partial}{\partial x}+ \frac{1}{i}\frac{\partial}{\partial y}\right)
$$
and
$$
\frac{\partial}{\partial \bar{z}}=\frac{1}{2}\left(\frac{\partial}{\partial x}-\frac{1}{i}\frac{\partial}{\partial y}\right)
$$
I'm skipping some of the stuff in proposition 2.3 of Stein, however, the part I believe you will be interested in is the following,
If $f$ is holomorphic, then we have
$$
\frac{\partial f}{\partial \bar{z}}(z_0) = 0
$$
and
$$
f'(z_0) = \frac{\partial f}{\partial z}(z_0) = 2\frac{\partial u}{\partial z}(z_0).
$$
The Cauchy-Riemann equations give us
$$
f'(z_0) = \frac{\partial f}{\partial x}(z_0) = \frac{1}{i}\frac{\partial f}{\partial y}(z_0)\Rightarrow f'(z_0) = \frac{1}{2}\left(\frac{\partial f}{\partial x}(z_0) + \frac{1}{i}\frac{\partial f}{\partial y}(z_0)\right)=\frac{\partial f}{\partial z}(z_0).
$$
Now if we use the Cauchy-Riemann equations we see that $\frac{\partial f}{\partial z}(z_0) = 2\frac{\partial u}{\partial z}(z_0)$. It is useful (and quite simple) to derive this and I suggest you do so to get more comfortable with Cauchy-Riemann equations.