hunt_mat said:
Do you have a reference? The same idea is used in deriving the solution of the Benjamin-Ono equation.
Surely if the pole was outside of the contour the integral would be zero by Cauchy's theorem. Am I missing something?
No, it's not zero because in the limit that the arc around the pole goes to zero the contour goes straight through the pole, so there is a contribution.
Consider:
\oint_c dz \frac{f(z)}{z-z_0}
where f(z) is analytic everywhere inside and on the contour. If the pole of the integrand at z_0 lies on our contour C, we go around it in a semi-circular arc of radius \epsilon, as \epsilon \rightarrow 0. This part of the curve we'll parametrize by z-z_0 = \epsilon \exp(i\theta). This gives
\int_\pi^0 d\theta i\epsilon e^{i\theta} \frac{f(z_0 + \epsilon e^{i\theta})}{\epsilon e^{i\theta}}
If we now take the limit \epsilon \rightarrow 0, we get
-i\int_0^\pi d\theta f(z_0) = -i\pi f(z_0)
which is half of the residue of f(z) at z_0 (with a minus sign because we traversed over the pole in a clockwise rotation).
Note that this calculation wouldn't work if the pole weren't simple, i.e., if the pole were (z-z_0)^m, with m > 1.
(However, jackmell's link suggests that if the pole is an odd power and our contour through it is a straight line segment, then treating the straight line segment as a principal value integral gives the half-residue again.)
jackmell said:
Hello Mute. Perhaps you would find this thread interesting which suggests we can do similar calculations with higher-ordered poles. See post #6 by JMerry.
http://www.artofproblemsolving.com/...67&t=182057&hilit=mainstream+complex+analysis
That is interesting. I had not heard of this result before. Also interesting is that the contour through the pole in this case must be a straight line segment.