I roughly know that I will have to turn to the Uniformization Theorem for this and probably also to the Gauss-Bonnet Theorem. But I'm having trouble making it precise.
Here's what I can tell you:
$\scriptsize\text{(From Wikipedia)}$
- (Uniformization Theorem) Every simply-connected Riemann surface is conformally equivalent to $\mathbb {\hat C}$, $\mathbb C$ or $\mathbb D(\cong\mathbb H$).
- (Gauss-Bonnet) Take $\Sigma_g$ a closed orientable Riemann surface and $k$ its curvature, then $\iint_{\Sigma_g}k\; dA<0\iff g>1$.
I want to be able to deduce that, for $g>1$, every $\Sigma_g\cong \mathbb D/\Gamma$, where $\Gamma$ is some discrete group, and that it thus makes sense to study fundamental polyons of $\mathbb D$.
I feel like I need something more than just Uniformization and Gauss-Bonnet for this. Especially since the Uniformization Theorem only speaks of simply-connected Riemann surfaces.
I need to know what extra steps to take when I want to relate $\Sigma_g$'s (not simply-connected) to $\mathbb D/\Gamma$'s ($\neq\mathbb D$).
Edit
The comments gave me an idea:
Every $\Sigma_g$ has a universal cover $p:U\to\Sigma_g$. I can say $\Sigma_g=U/p$ and give it the induced metric $d_{\Sigma_g}(x,y)=\inf d_U(p^{-1}x,p^{-1}y).$ Then I use Gauss-Bonnet to say $$\iint_{\Sigma_g}k \;dA=\iint_S k \; dA<0,$$ where $S$ is a single sheet above $\Sigma_g$. $U$ is the sum of these sheets, so $\iint_U k\; dA<0$. By the Uniformisation Theorem $U$ must be conformally equivalent to $\mathbb D$.
Is this correct?