Tricky integration (maybe delta function)

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The discussion revolves around integrating a complex function involving a delta function and a Fourier transform. The original poster has attempted various methods like substitution and integration by parts but found them ineffective. They recognize the connection to the delta function but are unsure how to apply it. A suggestion is made to use contour integration in the complex plane, although the poster expresses unfamiliarity with this method. Ultimately, the conversation highlights the need for proper techniques and possibly consulting a table of transforms for evaluation.
Kara386
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Homework Statement


I need to integrate

##\frac{A}{2a\sqrt{2\pi}} \int_{-\infty}^{\infty} \frac{e^{ik(x+x')}}{(b^2+k^2)}dk##

I have tried substitution and integration by parts and that hasn't worked. I can see that part of it is the delta function, but I don't really know how to use that fact! I think the delta function is

##\delta(x+x') = \frac{1}{2\pi}\int_{-\infty}^{\infty} e^{ik(x+x')}dk##

Which is almost exactly what I have. If it helps, this is from trying to reverse Fourier transform a function. How can I integrate this?

Homework Equations

The Attempt at a Solution

 
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Try a contour integration in the complex plane.
 
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vela said:
Try a contour integration in the complex plane.
That sounds well beyond anything we've been taught! I've never heard of contour integration, in the complex plane or otherwise... Is that the only method?
 
Maybe I have the integral wrong, let me double check.
 
Kara386 said:

Homework Statement


I need to integrate

##\frac{A}{2a\sqrt{2\pi}} \int_{-\infty}^{\infty} \frac{e^{ik(x+x')}}{(b^2+k^2)}dk##

I have tried substitution and integration by parts and that hasn't worked. I can see that part of it is the delta function, but I don't really know how to use that fact! I think the delta function is

##\delta(x+x') = \frac{1}{2\pi}\int_{-\infty}^{\infty} e^{ik(x+x')}dk##

Which is almost exactly what I have. If it helps, this is from trying to reverse Fourier transform a function. How can I integrate this?

Homework Equations

The Attempt at a Solution


Let ##x+x'= y##, so you want to evaluate
I(y) = \int_{-\infty}^{\infty} \frac{\exp(iky)}{k^2+b^2} \, dk.
Write ##\exp(iky) = \cos(ky) + i \sin(ky)##, and note that in the integral the denominator is even in ##k##, while ##\sin(ky)## is odd in ##k##. Therefore, without any need for computation we conclude that the imaginary part = 0 because the "##\sin##" term integrates to zero for any fixed ##y##. Thus, we have
I(y) = 2 \int_0^{\infty} \frac{\cos(ky)}{k^2+b^2} \, dk.

Assuming we can legitimately differentiate wrt ##y## under the integral sign, we have
\begin{array}{rcl}\frac{d^2}{dy^2} I(y) &amp;= &amp;2 \int_0^{\infty} \frac{-k^2 \cos(ky)}{k^2+b^2} \, dk \\<br /> &amp;=&amp; -2 \int_0^{\infty} \frac{(k^2 + b^2 - b^2)\cos(ky)}{k^2 + b^2} \\<br /> &amp;=&amp; - 2 \int_0^{\infty} \cos(ky) \, dy + 2 b^2 \int_0^{\infty} \frac{\cos(ky)}{k^2+b^2} \, dk \\<br /> &amp;=&amp; - 2 \int_0^{\infty} \cos(ky) \, dy + b^2 I(y) <br /> \end{array}<br />
Thus, you have a DE ##I''(y) - b^2 I(y) = f(y)##, where ##f(y) = -2 \int_0^{\infty} \cos(ky) \, dk##. Do you recognize ##f(y)## from somewhere?

Of course, to get the full ##I(y)## you need two boundary conditions on ##I(y)##, such as values of ##I(0)## and ##I'(0)##, and both of these can be obtained from results you have seen already (or can derive on your own).

There remains a serious issue, however: we just carelessly differentiated under the integral sign and further split the resulting integral into two separate integrations. Those manipulations need justification, but for now I will leave it.
 
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Kara386 said:
That sounds well beyond anything we've been taught! I've never heard of contour integration, in the complex plane or otherwise... Is that the only method?
Are you allowed to just look the transform in a table?
 
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Ray Vickson said:
Let ##x+x'= y##, so you want to evaluate
I(y) = \int_{-\infty}^{\infty} \frac{\exp(iky)}{k^2+b^2} \, dk.
Write ##\exp(iky) = \cos(ky) + i \sin(ky)##, and note that in the integral the denominator is even in ##k##, while ##\sin(ky)## is odd in ##k##. Therefore, without any need for computation we conclude that the imaginary part = 0 because the "##\sin##" term integrates to zero for any fixed ##y##. Thus, we have
I(y) = 2 \int_0^{\infty} \frac{\cos(ky)}{k^2+b^2} \, dk.

Assuming we can legitimately differentiate wrt ##y## under the integral sign, we have
\begin{array}{rcl}\frac{d^2}{dy^2} I(y) &amp;= &amp;2 \int_0^{\infty} \frac{-k^2 \cos(ky)}{k^2+b^2} \, dk \\<br /> &amp;=&amp; -2 \int_0^{\infty} \frac{(k^2 + b^2 - b^2)\cos(ky)}{k^2 + b^2} \\<br /> &amp;=&amp; - 2 \int_0^{\infty} \cos(ky) \, dy + 2 b^2 \int_0^{\infty} \frac{\cos(ky)}{k^2+b^2} \, dk \\<br /> &amp;=&amp; - 2 \int_0^{\infty} \cos(ky) \, dy + b^2 I(y)<br /> \end{array}<br />
Thus, you have a DE ##I''(y) - b^2 I(y) = f(y)##, where ##f(y) = -2 \int_0^{\infty} \cos(ky) \, dk##. Do you recognize ##f(y)## from somewhere?

Of course, to get the full ##I(y)## you need two boundary conditions on ##I(y)##, such as values of ##I(0)## and ##I'(0)##, and both of these can be obtained from results you have seen already (or can derive on your own).

There remains a serious issue, however: we just carelessly differentiated under the integral sign and further split the resulting integral into two separate integrations. Those manipulations need justification, but for now I will leave it.

Brilliant, thank you!
 
vela said:
Are you allowed to just look the transform in a table?
Maybe! I don't think we've been taught the right techniques to actually evaluate it. I'll ask my lecturer about the tables. Thanks for helping! :)
 

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