integral involving hyperbolic tangent and cosine

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I am looking for the solution to the following integral

$$\int_{\mathbb{R}} \frac{\tanh(x)\cos(xt)}{x(x^2+1/4+\alpha)}dx \quad\text{with}\quad \alpha, t\in \mathbb{R}$$.

Any hints at approaching the solution or the solution itself would be much thanked for.

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The first step I would take (if you're doing it by hand) is converting the trig functions to something easier to work with (their exponential definitions):

$\tanh(x) = {e^x - e^{-x}\over e^{x} + e^{-x}}$

$\cos(xt) = {e^{-ixt} - e^{ixt}\over 2}$

Next I would try integration by parts (It's not the $u,v$ form you're used to):

$\int[f(x)g(x)dx] = f(x)\int[g(x) dx] - \int[{d \over dx}[f(x)]\int[g(x) dx] dx]$

However, integrating the trig part alone produces a rather messy result...

https://www.wolframalpha.com/input/?i=integral(tanh(x)*cos(tx))

But, combined with the polynomial in the denominator, and the fact you're integrating over all reals, might have a simpler result. (Wolfram Alpha isn't able to compute your actual integral)

Edit:

Actually, there might be a better method. Still using integration by parts, let:

$f(x) = \tanh(x)$

$g(x) = {\cos(xt) \over x(x^2 + 1/4 + a)}$

Integrating $g(x)$, as seen here:

https://www.wolframalpha.com/input/?i=integral(cos(tx)%2F(x(x%5E2+%2B+(1%2F4)+%2B+a)))

Is a little more workable, because the $Si(x)$ and $Ci(x)$ have nice identities for the limits $-\infty$ and $\infty$:

$Si(-\infty) = -\pi / 2$

$Si(\infty) = \pi / 2$

$Ci(-\infty) = \pi i$

$Ci(\infty) = 0$

Edit:

Okay now I'm invested. Letting:

$A = \sqrt{a + 1/4}$

Then making the $g(x)$ integral neater (don't be scared):

$\int[g(x)dx] = -{1 \over 2A^2}(\cosh(At)(Ci(t(x-Ai)) + Ci(t(x+Ai))) + i\sinh(At)(Si(t(-x+Ai)) + Si(t(x+Ai)))-2Ci(tx))$

However this is indefinite. The definite integral (using our identities) is magically simple:

$\int_{-\infty}^{\infty}[g(x)dx] = {\pi i \over A^2}(1 + \cosh(At))$

This is a constant (with respect to $x$). Now this is where I made a mistake saying you can pull out the $g(x)$ integral. The integral inside the right integral is actually indefinite:

$\int_a^b[f(x)g(x)dx] = f(x)|_a^b\int_a^b[g(x) dx] - \int_a^b[{d \over dx}[f(x)]\int[g(x) dx] dx]$

Where ${d \over dx}[\tanh(x)] = sech^2(x)$

Meaning it's still complicated. Sorry about that.