Is Richard Robinett's Fourier Transform Convention Unconventional?

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Homework Help Overview

The discussion revolves around the Fourier transform conventions as defined by Richard Robinett, specifically the use of exp(-ikx) for the forward transform and exp(ikx) for the inverse transform. Participants are exploring whether this convention is unconventional compared to more commonly seen definitions.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Some participants question the relevance of the sign in the Fourier transform, suggesting that the integration limits from -∞ to ∞ make the sign inconsequential. Others discuss the importance of constants in the transform equations and their implications for theorems like Parseval's theorem. The original poster expresses confusion over the necessity of a specific convention for Gaussian equations.

Discussion Status

The conversation is ongoing, with participants sharing differing views on the significance of the sign convention and constants in the Fourier transform. Some guidance has been offered regarding the flexibility of conventions as long as consistency is maintained, but no consensus has been reached on the necessity of one convention over another.

Contextual Notes

Participants are referencing specific texts that utilize different conventions, highlighting the ambiguity in definitions across literature. The discussion is framed within the context of homework help, suggesting constraints related to academic expectations and the need for clarity in definitions.

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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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The Attempt at a Solution

 
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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

[tex]\phi (x)=\frac{1}{(2\pi)^{3/2}}\int dk \ \tilde{\phi}(k) e^{-ikx}[/tex].
 
Note that the integration is from [itex]-\infty[/itex] to [itex]\infty[/itex]. 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:
[tex]\phi (x)=\frac{1}{(2\pi)^{3/2}}\int dk \phi(k) e^{-ikx}[/tex]
then the inverse transform is:
[tex]\phi (k)=\frac{1}{(2\pi)^{3/2}}\int dx \phi(x) e^{ikx}[/tex]
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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