Solving Complex Integration Problems with \((*) Formula

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Discussion Overview

The discussion revolves around evaluating the integral \[ \int_{-\infty}^{\infty}\frac{e^{iax}}{x^2 - b^2}dx \] with \(a, b > 0\), focusing on the application of a specific formula for integrals with poles on the real axis. Participants explore the discrepancies in the results obtained using this formula and the implications of the conditions under which it can be applied.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant applies the formula \((*)\) for integrals with poles on the real axis and arrives at the result \(-\frac{\pi}{b}\sin(ab)\), questioning the validity of this approach.
  • Another participant calculates the principal value of the integral and arrives at the same result of \(-\frac{\pi}{b}\sin(ab)\), confirming the earlier participant's findings.
  • Some participants assert that the correct answer should be \(-\frac{2b}{\pi}\sin(ab)\), expressing confusion over the discrepancies in results.
  • There is a discussion about the applicability of the formula \((*)\), with one participant noting it is generally applicable only for simple poles on the real axis or when Laurent expansions do not include negative even powers.
  • Another participant mentions that the construction of the contour around the poles may influence the outcome, raising questions about the consistency of the integral's value.
  • One participant states that avoiding the poles results in the integral along any closed smooth path being zero, implying a relationship between contour integration and the results obtained.

Areas of Agreement / Disagreement

Participants express disagreement regarding the correct value of the integral, with multiple competing views on the application of the formula \((*)\) and the conditions under which it holds. The discussion remains unresolved with no consensus on the correct answer.

Contextual Notes

Participants highlight limitations related to the nature of the poles (simple vs. higher order) and the specific conditions under which the formula can be applied, indicating potential dependencies on the definitions used in the analysis.

Dustinsfl
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Consider
\[
\int_{-\infty}^{\infty}\frac{e^{iax}}{x^2 - b^2}dx
\]
where \(a,b>0\). The poles are \(x=\pm b\) which are on the x axis. Usually, if the poles are on the x axis, I use that the integral is
\[
2\pi i\sum_{\text{UHP}}\text{Res} + \pi i\sum_{\text{x axis}}\text{Res}\quad (*)
\]
which works in this problem http://mathhelpboards.com/analysis-50/integral-%3D-2pi-sum-res-uhp-pi-i-sum-res-real-axis-7576.html
However, if I use this formula on the integral above, I get the answer to be
\[
-\frac{\pi}{b}\sin(ab)
\]
when the answer is
\[
-\frac{2\pi}{b}\sin(ab)
\]
which would indicate \(2\pi i\) times the sum of the residual on the x axis. What is going wrong and when can and cannot I use the formula \((*)\)?
 
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$$PV \int^{\infty}_{-\infty} \frac{e^{iaz}}{z^2-b^2}\,dz$$

The function has only poles on the real axis at $$z=\pm b$$

so that becomes

$$PV \int^{\infty}_{-\infty}\frac{e^{iaz}}{z^2-b^2}\,dz= \pi i \lim_{z\to b}\, (z-b)\frac{e^{iaz}}{z^2-b^2}+\pi i \lim_{z\to -b}\, (z+b)\frac{e^{iaz}}{z^2-b^2}=\frac{\pi i e^{iab}}{2b}-\frac{\pi i e^{-iab} }{2b}=\frac{\pi i}{2b }(e^{iab}-e^{-iab})$$

which is equal to $$-\frac{\pi \sin(ab)}{b}$$ . As yours .

Note this the Principle value of the integral >
 
Last edited:
The answer is \(-\frac{2b}{\pi}\sin(ab)\) which isn't what we both have.
 
dwsmith said:
The answer is \(-\frac{2b}{\pi}\sin(ab)\) which isn't what we both have.

I cannot see how that would be the correct answer. why so sure ?
 
The answer in your textbook is not correct.

But just so you're aware, that formula is generally only applicable when the the poles on the real axis are simple poles.

But it is also applicable if none of the Laurent expansions about the poles on the real axis have terms of negative even power.

That's why $ \displaystyle \text{PV} \int_{-\infty}^{\infty} \frac{1}{x^{3}}\ dx = 0$.
 
Last edited:
@Random my professor says it depends on how we construct the contour around the poles. How true is that? Shouldn't the integral be the same?
 
If we avoid the poles then the integral along any closed smooth path is zero.
 

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