Function corresponds to $\sum_{n=1}^\infty \frac{(-1)^n}{n^2+\alpha^2}$ using the Fourier expansion

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Find the function corresponds to $\sum_{n=1}^\infty \frac{(-1)^n}{n^2+\alpha^2}$ using the Fourier expansion

$$ f(x)=\frac{a_0}{2}+\sum_{n=1}^\infty (a_n\cos(nx)+b_n\sin(nx)) $$ where $$\frac{a_0}{2}=\frac{1}{2\pi}\int_{-\pi}^{\pi} f(x)dx,\\{a_n}=\frac{1}{\pi}\int_{-\pi}^{\pi} f(x)\cos(n x)dx,\\{b_n}=\frac{1}{\pi}\int_{-\pi}^{\pi} f(x)\sin(nx)dx$$

$$ \sum_{n=1}^\infty \frac{(-1)^n}{n^2+\alpha^2}=\sum_{n=1}^\infty \frac{\cos(n\pi x)}{n^2+\alpha^2} $$ How do I proceed further ?

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As far as I can understand, the task is to find such a function that its Fourier series coincides with the given one at some point. $$ \frac{a_0}{2}+\sum_{n=1}^\infty \frac{(-1)^n\cos(n x)}{n^2+\alpha^2} +b_n\sin(nx) $$ Then at $x=0$, we will get the series subtracting $a_0$ if it is not zero.

Thus we need to find such an $f$ that $$ \frac{1}{\pi} \int_{-\pi}^\pi f(x)\cos(nx) dx = \frac{1}{n^2+\alpha^2}. $$ This is guessing work. Let's keep it simple and try the first thing which comes to a head. Consider $f(x)=\cos(\alpha x)$. This gives $$ \frac{1}{\pi} \int_{-\pi}^\pi f(x)\cos(nx) dx =\frac{2 \alpha (-1)^n \sin (\pi \alpha )}{\pi \alpha ^2-\pi n^2} $$ This is not exactly what we wanted, but let's change $\cos(\alpha x) \rightarrow \cos(i \alpha x)+\cos(-i \alpha x) $, the result is: $$ \frac{4 \alpha (-1)^n \sinh (\pi \alpha )}{\pi \left(\alpha ^2+n^2\right)}. $$ This is better. Thus the function we are interested in is $$ f=(\cos(i\alpha x)+\cos(-i\alpha x))\frac{\pi}{4\alpha \sinh(\pi\alpha)}=\frac{1}{2\alpha^2}+\sum_{n=1}^\infty \frac{(-1)^n\cos(n x)}{n^2+\alpha^2} +b_n\sin(nx). $$ It gives the answer for $x=0$ $$ \frac{\pi}{2\alpha \sinh(\pi\alpha)}-\frac{1}{2\alpha^2}=\sum_{n=1}^\infty \frac{(-1)^n}{n^2+\alpha^2} $$

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You may use the Poisson summation formula:

If $f\in L_1(\mathbb{R})$ and $\widehat{f}\in L_1(\mathbb{R})$, then $Pf(x)=\sum_{n\in\mathbb{Z}}f(x+n)$ converges uniformly, $f\in\mathcal{C}(\mathbb{S}^1)$, and $$Pf(x)=\sum_{n\in\mathbb{Z}} \widehat{f}(n) e^{2\pi kx}$$ where $\widehat{f}$ is the Fourier transform of $f$.

Using the fact that $\frac12 e^{-|2\pi t|}=\frac{1}{2\pi}\int^\infty_{-\infty} \frac{e^{-i2\pi tx}}{1+x^2}\,dx$, (this requires a little bit of Fourier analysis on $\mathbb{R}$, or some knowledge on characteristic functions of certain probability distributions), we have that

$$\sum_{n\in\mathbb{Z}} e^{-2\pi a |n|}e^{-2\pi kx}=Pf(x)=\frac{1}{\pi}\sum_{n\in\mathbb{Z}}\frac{a}{a^2+|x+n|^2}$$ At $x=0$ one gets \begin{align} \frac{\pi}{2a}\frac{1+e^{-2\pi a}}{1-e^{-2\pi a}}&=\sum^\infty_{n=1}\frac{1}{a^2+n^2} +\frac{1}{2a^2}=\sum^\infty_{n=1}\frac{1}{a^2+(2n-1)^2}+\frac{1}{2a^2} +\frac14\sum^{\infty}_{n=1}\frac{1}{\big(\tfrac{a}{2}\big)^2+ n^2}\\ &=\sum^\infty_{n=1}\frac{1}{a^2+(2n-1)^2} +\frac{1}{2a^2} + \frac{1}{4}\Big(\frac{\pi}{a}\frac{1+e^{-\pi a}}{1-e^{-\pi a}}-\frac{2}{a^2} \Big)\\ &=\sum^\infty_{n=1}\frac{1}{a^2+(2n-1)^2}+\frac{\pi}{4a}\frac{1+e^{-\pi a}}{1-e^{-\pi a}} \end{align} Hence $$ \sum^\infty_{n=1}\frac{1}{a^2+(2n-1)^2} =\frac{\pi}{2a}\frac{1+e^{-2\pi a}}{1-e^{-2\pi a}} -\frac{\pi}{4a}\frac{1+e^{-\pi a}}{1-e^{-\pi a}} $$

The series in the OP can be then expressed as $$\begin{align} \sum^\infty_{n=1}\frac{(-1)^n}{a^2+n^2}&=-\sum^\infty_{n=1}\frac{1}{a^2+(2n-1)^2}+\frac14\sum^{\infty}_{n=1}\frac{1}{\big(\tfrac{a}{2}\big)^2+ n^2}\\ &=-\frac{\pi}{2a}\frac{1+e^{-2\pi a}}{1-e^{-2\pi a}} +\frac{\pi}{2a}\frac{1+e^{-\pi a}}{1-e^{-\pi a}}-\frac{1}{2a^2} \\ &=\frac{\pi}{2a}\Big(\frac{1+e^{-\pi a}}{1-e^{-\pi a}}-\frac{1+e^{-2\pi a}}{1-e^{-2\pi a}}\Big)-\frac{1}{2a^2} \\ &=\frac{\pi}{2a}\operatorname{csch}(\pi a)-\frac{1}{2a^2} \end{align} $$