What is the inverse Fourier transform of e^{-|x|}?

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Homework Help Overview

The discussion revolves around the inverse Fourier transform of the function \( e^{-|x|} \) and the related integral calculation involving \( \frac{1}{1+t^2} e^{i \omega t} \). The original poster expresses difficulty in evaluating this integral directly.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to calculate the integral using various methods, including partial integration and substitutions, but finds them unhelpful. Some participants suggest using complex contour integration and the residue theorem as a potential approach.

Discussion Status

Participants are exploring different methods to evaluate the integral, with some suggesting established techniques from complex analysis. There is acknowledgment of the difficulty in the original poster's approach, and alternative methods are being discussed without reaching a consensus.

Contextual Notes

The original poster is preparing for an exam and is seeking assistance with a specific integral related to the inverse Fourier transform. There is mention of resources such as tables of integrals, indicating potential gaps in the original poster's approach.

MrSeaman
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Hi,

I got an exam in calculus in a few weeks, and lots of questions coming up. Here's one of them:

We learned that the Fourier Transform of

[tex]f(x) = e^{-|x|}[/tex]
is
[tex]\hat f(\omega) = \sqrt{\frac{2}{\pi}}\frac{1}{1+\omega^2}[/tex]

I've got no problem with this one. Now, since [tex]\hat f(\omega)[/tex] is Lebesgue - integrable, the inverse Fourier transform exists and should be

[tex]\hat \hat f(-x) = e^{-|x|}[/tex]

To show this the 'hard way', I want to calculate the integral

[tex]\sqrt{\frac{1}{2 \pi}} \int \limits_{-\infty}^\infty \frac{1}{1+t^2} e^{i \omega t} \mathrm{d} t[/tex]

Well, I just don't know how to do this one. Partial Integration doesn't seem to work, and I can't find neither a good substition nor a clever use of Fubini's Theorem.

Would be thankful for any help.
 
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I have never seen it derived directly. However, it is easily found in a table of definite integrals.
 
MrSeaman said:
To show this the 'hard way', I want to calculate the integral

[tex]\sqrt{\frac{1}{2 \pi}} \int \limits_{-\infty}^\infty \frac{1}{1+t^2} e^{i \omega t} \mathrm{d} t[/tex]

One way to do this is by using complex contour integration and the residue theorem.

Integrate

[tex]\int \frac{1}{1+z^2} e^{i \omega z} \mathrm{d} t[/tex]

along the closed contour that consists of the portion of the real axis from [itex]-R[/itex] to [itex]R[/itex] together with a closing counterclockwise semicircle of radius [itex]R[/itex] in the upper halfplane. Let [itex]R\rightarrow \infty[/itex]. Then:the closed contour encloses a pole at [itex]z=i[/itex]; the contibution from the semicircle goes to zero.

Repeat for a clockwise semicircle in the lower halfplane.

Regards,
George
 
Last edited:
As I was just told, it seems to be done by using the residue theorem of complex analysis.

edit: George was faster, thanks! Working it out...
 

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