Here is my attempt. Consider the analytic function $g : \Bbb{C} \setminus \{0\} \to \Bbb{C}$ defined by $g(z) = f(\frac{1}{z})$. Note that $$\lim_{|z| \to 0} |g(z)| = \lim_{|z| \to 0} |f(\frac{1}{z})| = \infty,$$ which tells us that $z=0$ is a pole of $g$, say of order $m$. This means that the Laurent expansion of $g$ at $z=0$ in $\Bbb{C} \setminus \{0\}$ looks something like:
$$g(z) = a_m z^{-m} + a_{m+1} z^{-m+1} + ... a_1 z^{-1} + a_0 + a_{-1} z + a_{-2} z^2 + ...$$
which gives us Laurent series expansion of $f$ after replacing $\frac{1}{z}$ by $z$: $$f(z) = ... + a_{-2}z^{-2} + a_{-1} …