I am having problems in evaluating the following Cauchy principal value
$$\int_{-\infty}^{+\infty} \frac{\cos(3x)}{x-1}d x$$
I know it is supposed to show my work, but I got barely nothing. I tried with using $\cos(x) = (z + z^{-1})/2$ (clearly adapting it to $\cos(3x)$, but I think something went wrong because I got $0$ (I have the solution, it shall be $-\pi \sin(3)$.
Also, I would like a "true proof", like with contour integration explained. Sometimes theory comes easier with an example.
Thank you!
I am unable to draw the contour lines in the books-fancy way, so I will avoid it.
Let's proceed by considering the following integral instead:
$$\int \frac{e^{3iz}}{z-1}\ \text{d}z$$
steppint into the complex plane, remembering that $e^{ix} = i\sin(x) + \cos(x)$, integrated along a closed contour (the "typical one", the upper semi-circle, to be clear).
We have to modify it, though, because the above function has a pole at $z = 1$ and this point must be avoided by means of a semicircular indentation of a small radius, say $\epsilon$, in the contour.
Notice that $\frac{e^{3iz}}{z-1}$ is analytic at all points lying on, and interior to, this contour.
Integrating this function around the chosen path and putting $z = x$ where appropriate we have
$$\int_{-R}^{1 - \epsilon} \frac{e^{3ix}}{x-1} \text{d}x + \int_{|z-1| = \epsilon} \frac{e^{3iz}}{z-1} \text{d}z + \int_{1 + \epsilon}^R \frac{e^{3ix}}{x-1}\text{d}x + \int_{|z| = R} \frac{e^{3iz}}{z-1}\text{d}z = 0$$
Allowint $R\to +\infty$ and invoking Jordan's lemma, we can easily argue that the integral around the semicircle of radius $R$ goes to zero.
Taking the limit $\epsilon \to 0$ we can evaluate the integral over the semicircular indentation at $z = 1$.
Now we invoke the following:
THEOREM
Let $f(z)$ have a simple pole at $z_0$. An arc $C_0$ of radius $r$ is constructed using $z_0$ as its center. The arc subtends an angle $\alpha$ at $z_0$. Then
$$\lim_{r\to 0} \int_{C_0} f(z) \text{d}z = 2\pi i\left[\frac{\alpha}{2\pi}\text{Res}[f(z), z_0]\right]$$
where the integration is done in the counterclockwise direction (for a clockwise direction, a factor $-1$ is placed on the right).
We use that Theorem with $\epsilon = r$, $f(z) = \frac{e^{3iz}}{z-1}$ and $z_0 = 1$. The angle $\alpha = \pi$ (for a semicircle) and we find the second integral on the left becomes in the limit: $-i\pi e^{3i}$.
The minus sign appears because of the clockwise direction of integration.
With $R\to +\infty$ and $\epsilon \to 0$ we rewrite:
$$\lim_{R\to +\infty} \lim_{\epsilon \to 0} \left[\int_{-R}^{1 - \epsilon} \frac{e^{3ix}}{x-1} \text{d}x + \int_{1 + \epsilon}^R \frac{e^{3ix}}{x-1}\text{d}x \right] + i\pi e^{3i} = 0$$
The sum of the two integral in the brackets becomes, with the limits indicates, the Cauchy principal value of
$$\int_{-\infty}^{+\infty} \frac{e^{3ix}}{x-1}\text{d}x = \int_{-\infty}^{+\infty} \frac{\cos(3x) + i\sin(3x)}{x-1}\ \text{d}x$$
Thus
$$\int_{-\infty}^{+\infty} \frac{\cos(3x)}{x-1}\text{d}x + i\int_{-\infty}^{+\infty}\frac{\sin(3x)}{x-1}\ \text{d}x = i\pi e^{3i}$$
Remembering indeed that
$$i\pi e^{3i} = i\pi (\cos(3) + i\sin(3)]$$
We obtain eventually the real and the imaginary part:
$$\int_{-\infty}^{+\infty} \frac{\cos(3x)}{x-1}\text{d}x = -\pi \sin(3)$$
and
$$\int_{-\infty}^{+\infty}\frac{\sin(3x)}{x-1}\ \text{d}x = \pi \cos(3)$$
as wanted.