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

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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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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...