Is Richard Robinett's Fourier Transform Convention Unconventional?

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Homework Statement


Richard Robinett defined the Fourier transform with an exp(-ikx) and the inverse Fourier transform with an exp(ikx). I have always seen the opposite convention and I thought it was not even a convention but a necessity to do it the other in order to apply it to some Gaussian equations. Has anyone ever seen this sign convention before?




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It really isn't relevant whether it's with a plus, or with a minus. I've seen in most cases

\phi (x)=\frac{1}{(2\pi)^{3/2}}\int dk \ \tilde{\phi}(k) e^{-ikx}.
 
Note that the integration is from -\infty to \infty. That's why the sign does not matter.
 
Furthermore, the constants in front also do not really matter, as long as they combine to give 1/(2 pi). There are a couple of theorems which depend on them (I think Parseval's theorem and the associated ones do), but it's all up to a constant. My supervisor (in physics) recommends just ignoring the constants, and adding them back in if you have to at the end :wink:
 
If you define the Fourier transform as dextercioby did:
\phi (x)=\frac{1}{(2\pi)^{3/2}}\int dk \phi(k) e^{-ikx}
then the inverse transform is:
\phi (k)=\frac{1}{(2\pi)^{3/2}}\int dx \phi(x) e^{ikx}
It is merely a matter of convention which is called which. There's no 'wrong' convention as long as you remain consistent.

On page 11 of 'Photons and Atoms' by Claude Cohen-Tannoudji et. al. the convention above is used. On page 97 of 'The Principles of QM' by P.A.M. Dirac, the convention is left deliciously ambiguous.
Dirac said:
These formulas have elementary significance. They show that either of the representations is given, apart from numerical coefficients, by the amplitudes of the Fourier components of the other.
 
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