Integration Problem: Solving \oint e-ax^2dx = 1/4\sqrt{}\pi/a^3

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The discussion revolves around solving the integral \oint e^{-ax^2}dx = \sqrt{\pi/a} and demonstrating that \oint x^2 e^{-ax^2}dx = 1/4\sqrt{\pi/a^3} for the limits from 0 to infinity. Participants suggest using integration by parts and differentiating the known integral with respect to 'a' to establish the relationship between the two integrals. The confusion arises from the different limits of integration and the notation used. Ultimately, the solution involves deriving the first integral and incorporating the derivative inside the integral to simplify the problem. The thread concludes with a method to generalize this approach for integrals of the form \int x^{2n} e^{-a x^2} dx.
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Homework Statement


Given that:

\oint e-ax^2dx = \sqrt{}\pi/a (between infinity and minus infinity)

show that

\ointx2e-ax^2dx = 1/4\sqrt{}\pi/a^3 (between 0 and infinity)



Homework Equations





The Attempt at a Solution


I assume integration by parts may be necessary, but not really sure how to go about it, ie. what is first expression really telling you as the limits are different to the second. I think it might also be the infinities confusing me so if someone could point me in the right direction that'd be appreciated.
 
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I assume that you meant
\int_{-\infty}^\infty
(click to see the LaTeX code) rather than \oint.

As for the problem, try differentiating with respect to a ;)
 
Hmmm ok so I have it starting to look right but I really can't quite see how they all relate to each other. If you differentiate \sqrt{\pi/a} with respect to a you get -1/2\sqrt{\pi/a^3} and if you differentiate e-ax^2 with respect to a you get -x2e-ax^2

which is looking good however maybe I'm just being stupid but I can't see what to do from there.
 
ok actually I think I have it now, thanks for the help!
 
Yep, so the trick is to take the first (standard) integral, derive it, and then pull the derivative inside the integral.

In fact, you can use that to derive a formula for
\int x^{2n} e^{-a x^2} \, dx
for any n = 0, 1, 2, ...
 
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