This is follow up to my last question on summing over countably infinite sets. I understand the idea conceptually now but I am still stuck when dealing with a concrete example. Specifically, consider
$$\sum_{\omega \in \Lambda^*}\frac{1}{\omega^2}$$ where $\Lambda^*$ is a lattice in the complex plane without the origin. This sum has come up in several books when the author is defining the $\wp$ elliptic function. Apparently, it diverges but I haven't been able to find the details of why it does. Intuitively, I would think it would converge since for large $|\omega|$ one would expect $|1/\omega^2|$ to decay very rapidly.
How would I even begin to analyze such a sum? I think the issue is my intuition from the sum $\sum \frac{1}{n^2}$ which does converge is corrupting my understanding.
Thanks.
Roughly speaking the sum behaves (for large $m,n$) like $\sum_{m,n \ne 0}\frac{1}{m^2+n^2}$ and that is divergent since the sum say in m for fixed $n$ is about $\frac{1}{n}$, so the double sum behaves like the harmonic sum.
(if $a \ge 1$, $\int_1^{\infty}\frac{dx}{x^2+a^2}<\sum_{m \ge 1}\frac{1}{m^2+a^2}<\int_0^{\infty}\frac{dx}{x^2+a^2}$ so $\frac{\pi}{2a}-O(\frac{1}{a^2})< \sum_{m \ge 1}\frac{1}{m^2+a^2} < \frac{\pi}{2a}$