Calculation of a certain type of contour integral

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Discussion Overview

The discussion revolves around the computation of contour integrals, particularly when the pole is located on the boundary of the contour. Participants explore methods for handling such cases, referencing the Hilbert transform and related mathematical concepts.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant inquires about computing a contour integral with a pole on the boundary, noting a lack of resources in undergraduate complex analysis texts.
  • Another participant suggests that the contour can run around the pole in a small semi-circular arc, indicating that for a simple pole, the integral would yield half the residue if the contour runs through the pole.
  • A participant questions the validity of the approach, asserting that if the pole were outside the contour, the integral would be zero according to Cauchy's theorem.
  • References to examples of similar integrals are provided, including cases involving branch cuts and higher-order poles, suggesting that different methods may apply depending on the situation.
  • One participant elaborates on the calculation process for a simple pole, detailing the parametrization and limit process that leads to a contribution from the pole.
  • There is mention of a result regarding odd powers of poles and how they can be treated as principal value integrals, which also yields a half-residue result.

Areas of Agreement / Disagreement

Participants express differing views on the treatment of poles on the contour, with some supporting the proposed method of using semi-circular arcs while others raise concerns about the implications of Cauchy's theorem. No consensus is reached regarding the validity of the approaches discussed.

Contextual Notes

Participants reference various mathematical scenarios, including simple and higher-order poles, and the implications of contour shapes on the results. There is an acknowledgment of the complexity involved in these calculations and the need for careful consideration of the contour's path.

hunt_mat
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Hi,

During my research I came across a contour integral where the pole was on the boundary. I have never come across this before, do anyone of you know how I would go about computing this?

It involved the Hilbert transform and I can't find it in my undergraduate complex analysis books and I thought someone here might know.
On a similar note, if anyone has any good numerical routines for Hilbert transform, I would like to know.

Mat
 
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The way such a thing is dealt with is to have the contour run around the pole in a small semi-circular arc, in the limit that the radius of the arc tends to zero.

As long as it's a simple pole, the result is if a contour runs straight through a pole (which would correspond to a half-circle arc that excludes the pole from being inside the contour) the pole contributes half the residue to the integral. If the pole is at a corner of a contour (which corresponds to a quarter-circle arc around the contour) it would contribute 1/4 the residue.
 
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?
 
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.
 
Last edited:

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