Special Morse function on a Riemann surface Let $f: S \to \Bbb R$ be a Morse function on a Riemann surface. Let $x_0$ be a saddle point of $f$. Since $x_0$ is a critical point of $f$, it makes sense to talk about the bilinear forms $f_{z\overline{z}}(x_0)$, $f_{zz}(x_0)$ and $f_{\overline{z}\overline{z}}(x_0)$ as components of the real Hessian of $f$ at $x_0$ (if one only allows only complex coordinates).
Can $f$ be arranged so that the Hermitian form $f_{z\overline{z}}$, which can be defined on all $S$, is arbitrarily small (compared to some fixed Hermitian metric) and $|f_{zz}(x_0)|$(as a number) is arbitrarily big in a fixed coordinate system around $x_0$?
 A: First, let  me point out that only  the differential form $\newcommand{\pa}{\partial}$ $\newcommand{\bpa}{\bar{\partial}}$ $\pa\bpa f$ is well defined  globally on $S$. Locally
$$ \pa\bpa f= f_{z\bar{z}} dz\wedge d\bar{z}, $$
but  the coordinate $z$ is only locally defined. If  you choose different  a different local coordinate  $u$  you have an equality
$$ f_{z\bar{z}} dz\wedge d\bar{z}= \pa\bpa f=f_{u\bar{u}} du\wedge d\bar{u} \tag{A} $$
yet 
$$  f_{z\bar{z}} \neq f_{u\bar{u}}. $$
The equality (A)  implies that 
$$ f_{u\bar{u}}= f_{z\bar{z}} \cdot \left| \frac{dz}{du} \right|^2. $$
On the other hand,
$$\frac{d}{du} =\frac{dz}{du}\frac{d}{dz} $$
so that
$$\frac{d^2}{du^2}= \frac{d^2 z}{du^2} \frac{d}{dz}+ \left(\frac{dz}{du}\right)^2\frac{d^2}{dz^2}. $$
Hence, if  $z= au+bu^2+ O(u^3)$$,  $$ a\in \mathbb{C}\setminus 0$$,  we deduce
$$  f_{u\bar{u}}= |a|^2 f_{z\bar{z}}, $$
$$f_{uu}= a^2 f_{zz}. $$
In particular, at the critical point  $x_0$  we have
$$\left| \frac{f_{uu}}{f_{u\bar{u}}}\right|= \left| \frac{f_{zz}}{f_{z\bar{z}}}\right|.  $$
This proves that you cannot find a holomorphic coordinate  $u$ near $x_0$ that makes  $f_{u\bar{u}}$ very small and $f_{uu}$ very large.
Update.  $\newcommand{\ii}{\boldsymbol{i}}$ If $z=x+\ii y$,  then   using the equalities
$$\pa_z=\frac{1}{2}(\pa_x-\ii\pa_y),\;\;\pa_{\bar{z}}=\frac{1}{2}(\pa_x+\ii\pa_y), $$
we deduce 
$\DeclareMathOperator{\tr}{tr}$ $\DeclareMathOperator{\Hess}{Hess}$
$$
f_{z\bar{z}}=\frac{1}{4} (f_{xx}+f_{yy}) =\frac{1}{4}\tr \Hess(f), $$
$$ f_{zz}=\frac{1}{4}( f_{xx}+f_{yy}+2\ii f_{xy}). $$
As I mentioned in one of my comments,   you can choose $f$    so that the partials $f_{xx},f_{yy}, f_{xy}$ have any prescribed values at $x_0$, but observe that
$$\left|\frac{f_{zz}}{f_{z\bar{z}}}\right|^2=\frac{ (\tr \Hess(f))^2+(f_{xy})^2}{(\tr \Hess(f))^2}\geq 1. $$
