Fourier transform of a sum of shifted Gaussians

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Discussion Overview

The discussion revolves around the Fourier transform of a sum of shifted Gaussian functions, exploring the implications of linearity in Fourier transforms, and the complexities that arise when considering shifted Gaussians and delta functions. The scope includes theoretical aspects of Fourier analysis and mathematical reasoning related to transformations in one and two dimensions.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • One participant initially proposes that the Fourier transform of a sum of shifted Gaussians should yield another sum of Gaussians, but later acknowledges complications arising from the addition of more Gaussians.
  • Another participant states the linearity of the Fourier transform, asserting that the transform of a sum of functions equals the sum of their transforms.
  • A question is raised about whether the participant is adding the Gaussians or the underlying processes, suggesting a potential misunderstanding in the approach.
  • Clarification is sought on whether the participant meant to convolve the functions rather than multiply them, indicating a possible source of confusion in the transformation process.
  • The original poster expresses uncertainty about the results obtained when applying the Fourier transform to a shifted Gaussian multiplied by a delta function, noting unexpected complexities in the outcome.
  • The original poster mentions an interest in the real part of the transform and questions why the behavior becomes more complicated with additional Gaussians, despite the expectation that transforms could simply be summed.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the correct approach to the problem, and multiple competing views remain regarding the treatment of shifted Gaussians and the implications of convolution versus multiplication in the context of Fourier transforms.

Contextual Notes

The discussion highlights potential limitations in understanding the relationship between shifted Gaussians and delta functions, as well as the assumptions underlying the application of the convolution theorem. Specific mathematical steps and definitions are not fully resolved.

Kavorka
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My first thought was simply that the Fourier transform of a sum of Gaussians functions that are displaced from the origin by different amounts would just be another sum of Gaussians:

F{G1(x) + G2(x)} = F{G1(x)} + F{G1(x)}

where a generalized shifted Gaussian is: G(x) = G0exp[-(x - x0)2 / 2σ2]

with amplitude G0, standard deviation σ and offset on the x-axis of x0.

but I've been told this is wrong. I've found that the result becomes more complicated when you add more Gaussians, and that the Fourier transform of just two shifted Gaussians is a Gaussian multiplied by a periodic function (cosine). This comes from representing a shifted Gaussian as the non-shifted gaussian multipled by a shifted delta function. My first question is why you cannot do this in the way I first considered.

My second problem was with solving the problem in the new way. I found that the the Fourier transform of a Gaussian multipled by a shifted delta function is just a periodic function, not multiplied by any Gaussian function. It follows that the Fourier transform of a sum of delta functions multiplied by Gaussians is just a sum of perodic functions. But I know this result isn't true, and am tripping up on where I went wrong.

I'm trying to generalize an expression in 3-d space, but in 2-d space the function I'm transforming is:

δ(x-x0)*G0exp[-x2 / 2σ2]

The result I get ends up being a complicated constant multiplied by eix0u with u being the Fourier space variable. This can be expanded into a real cosine component and an imaginary sine component, and it is the real part I am interested in. Obviously this is not a Gaussian multiplied by a cosine, which is what I expected. The end behavior of the transform should go to 0. Also, I'm not finding how the transform becomes more complicated as you add more Gaussians, because you should just be able to sum the transforms.

Any idea where I am going wrong? I feel like I'm missing a fundamental understanding. I also tried to use the convolution theorem to solve this, but it seems to lead to more complicated work than just directly solving it. Can also show more work if needed, just not used to formatting
 
Last edited:
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The Fourier transform is linear. It holds that
$$F(f+g) = F(f) + F(g)$$
for any functions f and g (for which the Fourier transform is well defined).
 
Are you adding the Gaussians or the underlying processes?
 
Kavorka said:
This comes from representing a shifted Gaussian as the non-shifted gaussian multipled by a shifted delta function. My first question is why you cannot do this in the way I first considered.
Multiplied with or convolved with?
 
I mean convolved with. I ended up working it out, my first assumption was correct I just did the work wrong. I was wondering if anyone can take a look at my result

pOQg47d.png
 

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