A general recipe:
1) Derive your integral with respect to $\alpha$. This will produce an $x$ inside your integral that will kill the $x$ in the denominator, leaving you with just $\int _1 ^\infty \Bbb e ^{-x} \sin (\alpha x) \ \Bbb d x$.
2) Integrate by parts twice. If you do it just once it will not be enough. The first integration will turn $\sin$ into $\cos$ and produce some extra factors. The second will turn $\cos$ into $-\sin$ and some further extra factors. You will obtain a 1st degree equation where the unknown is precisely $\int _1 ^\infty \Bbb e ^{-x} \sin (\alpha x) \ \Bbb d x$, that will be trivial to find.
3) Remember that you began by deriving with respect to $\alpha$. Therefore, it is necessary now to integrate the result obtained at (2) with respect to it. This will be an indefinite integral, so will produce an integration constant.
4) Find the value of that integration constant by evaluating the integral given by the problem and your own result at some convenient value of $\alpha$. In this example, choose $\alpha = 0$ (i.e. take the limit toward $0$), because the given integral will be $0$ there.
PS: I meant that we don't have an analytic representation of the function, e.g. $F'(\alpha) = sin(x) cos(x) ln(x) / x^2$.
– Egor Okhterov Aug 13 '16 at 11:28