Fourier transform of exponential function

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Homework Help Overview

The discussion revolves around finding the Fourier transform of the function $$f_a(t) = e^{-a t^2}$$, given a sample function and its corresponding Fourier transform. The original poster expresses difficulty in computing the transform and mentions connections to concepts not covered in lectures.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to compute the Fourier transform directly but encounters convergence issues with the integrals. They explore the relationship between exponential and trigonometric functions and consider the implications of the Dirac delta function.
  • Some participants suggest rescaling time and frequency to relate the problem to the known Fourier transform of the sample function.
  • Another participant mentions the scaling property of Fourier transformations, encouraging a review of relevant properties covered in class.

Discussion Status

The discussion includes attempts to clarify the approach to the problem, with participants offering guidance on rescaling and properties of Fourier transforms. The original poster indicates they have resolved the problem, but the details of that resolution are not shared.

Contextual Notes

The original poster notes that certain concepts, such as the link between Fourier transforms and the Dirac delta function, have not been discussed in their coursework, which may affect their understanding of the problem.

Peter Alexander
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1. The problem statement, all variables, and given/known data
Task begins by giving sample function and a corresponding Fourier transform $$f(t) = e^{-t^2 / 2} \quad \Longleftrightarrow \quad F(\omega) = \sqrt{2 \pi} e^{-\omega^2 / 2}$$ and then asks to find the Fourier transform of $$f_a(t) = e^{-a t^2}$$

Homework Equations


The equation for Fourier transform, according to our textbook, is $$F(\omega) = \int_{-\infty}^{\infty} e^{i \omega t} f(t) d\omega$$ If I understand correctly, multiple notations exist, but this one was given to us.

The Attempt at a Solution


Normally the computation is pretty straightforward, simply plug ##f(t)## into the equation, perform some integration and done. However, this one gave me loads of troubles! A solution, according to output from Mathematica and our textbook solutions is $$F(\omega) = \sqrt{\frac{\pi}{a}} e^{-\frac{\omega ^2}{4 a}}$$ Some research later, I've found out that Fourier transform is linked to Dirac delta function, but this concept hasn't been discussed on lectures nor mentioned in the textbook. My suspicion is that link between exponential function and trigonometric functions (Euler's formula) can lead me a step closer to a solution.

Using Mathematica, I've seen that the integrand ##e^{i \omega t} f_a(t)## can be expressed as $$e^{t (-a t+i \omega )} = \cosh \left(a t^2-i t \omega \right)-\sinh \left(a t^2-i t \omega \right)$$ but since both integrals do not converge on ##(-\infty, \infty)## they cannot be computed. This claim was reafirmed when I tried integrading both functions in Mathematica.

At that point, I'm completely stuck. I thought about checking the given examples and trying to guess the value of Fourier transform this way, but even then I couldn't produce a solution. Would somebody be kind enough to help me?
 
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You need to rescale time such that ##f(t')## gives you ##f_a(t)##. Then rescale the frequency to ##\omega'## to recover the Fourier integral and then you can find ##F(\omega')## using the FT of the sample function.

Edit: To clarify what I meant, you want to find
$$
\int_{-\infty}^{\infty} e^{i \omega t} e^{-at^2} d\omega
$$
You know that
$$
\int_{-\infty}^{\infty} e^{i \omega t} e^{-t^2/2} d\omega = \sqrt{2\pi} e^{-\omega^2/2}
$$
so modify this equation by changing ##t## and ##\omega## until you get to the integral above.
 
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Are you familiar with the scaling property of Fourier transformations? If so, you should use it (and maybe review the proof). You should become familiar with the use of any property that has been covered to this point in your class.
 
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I actually solved it, can't believe it was that easy!
I would like to thank both of you for your time and effort helping me understand this problem.
 
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