The residue theorem is commonly used to calculate situations where the number of isolated singularities is limited. However, I am very curious whether the residue theorem can be extended to cases with infinite singularities.

I hope to find a concise function to explain this conjecture and find a few counterexamples. But it's not easy.

So, I will use an integration problem that I actually encountered as an example to illustrate. Of course, we are not limited to the example given below.

This integration problem was obtained when I attempted to solve a magnetic field problem. It is shown in the blow. $$ \int_{-\infty}^{\infty}{\frac{e^{gx}\cosh\mathrm{(}tx)\mathrm{e}^{jpx}}{x(x+\beta )\left[ a(e^{2gx}+1)+b(e^{2gx}-1) \right]}}\mathrm{d}x \\ where\,\,0<p,0<\beta ,0<a<b,0<t<g $$ In order to solve this inverse Fourier transform problem using residue theorem, let an auxiliary complex variable function： $$f(z)=\frac{e^{gz}\cosh\mathrm{(}tz)\mathrm{e}^{jpz}}{z(z+\beta )\left[ a(e^{2gz}+1)+b(e^{2gz}-1) \right]}$$

Obviously, the first-order pole of $f (z)$ is $0$, $-\beta$, and $$k_n=\frac{j2n\pi +\ln \left( \frac{b-a}{b+a} \right)}{2g}$$. Where, $n\in \mathbb{Z}$.

We can construct an infinitely large semicircular integral contour $C$ in the upper half complex plane. As shown in Fig.1.

Based on Jordan's lemma, it is convenient to calculate the integration of various arc paths on the integral contour C, including infinite diameter semi-circular arcs $C_R$ and small arcs $C_{\varepsilon 1}$、$C_{\varepsilon 2}$ and $C_{\varepsilon 3}$ near poles on the x-axis.

And, by calculation, we can confirm that the infinite series $\sum_{n=1}^{\infty}Res[f(z),k_n]$ is convergent.

So, our conjecture is whether $\oint_{C}f(z)dz = 2j\pi\sum_{n=1}^{\infty}Res[f(z),k_n]$ holds true. Will it is universally valid ?

Is this a proven problem? Or can we find a suitable counterexample. I have not found any relevant papers discussing this issue.

isolatedsingularities.) See for example math.stackexchange.com/a/1445021/87355 $\endgroup$