Sufficient condition for bounded Fourier transform

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Discussion Overview

The discussion revolves around identifying sufficient conditions for a function \( f \) such that its Fourier transform \( F \) is bounded, particularly under the assumption that \( F \) has compact support. Participants explore various mathematical arguments and theorems related to the boundedness of Fourier transforms.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant suggests that if \( f \) is in \( L^1 \), then \( F \) is bounded, regardless of whether \( F \) has compact support.
  • Another participant presents a proof sketch relying on the Fourier shift theorem and the compact support assumption, indicating that if \( F \) is not bounded, it leads to a contradiction if \( f \) is assumed to be in \( L^1 \).
  • A participant questions the validity of their argument, noting that the assumption about points in the support of \( F \) going to infinity may not hold in cases where \( F \) does not have compact support.
  • One participant acknowledges that the boundedness of \( F \) is indeed related to the absolute integrability of \( f \), thus refining their earlier argument.
  • Another participant proposes using a continuity argument combined with compactness to argue for the boundedness of the transform.
  • One participant introduces the reverse question, suggesting that if \( F \) is bounded with compact support, then \( f \) must be in \( L^1 \).

Areas of Agreement / Disagreement

Participants express differing views on the necessity of compact support for the boundedness of the Fourier transform and the implications of \( f \) being in \( L^1 \). The discussion remains unresolved regarding the generalization of the proof to cases where \( F \) does not have compact support.

Contextual Notes

Some arguments rely on specific assumptions about the behavior of the Fourier transform at points in its support, which may not universally apply. The discussion also highlights the dependence on definitions of boundedness and integrability.

mnb96
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Hello,

Let's suppose we are given a function f:\mathbb{R}\rightarrow \mathbb{R}, and we assume its Fourier transform F=\mathcal{F}(f) exists and has compact support.

What sufficient condition could we impose on f, in order to be sure that F is also bounded?
 
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f is L1 is certainly sufficient, even if F does not have compact support.
 
Thanks a lot!
I think I figured out a way to prove it, but it relies on the Fourier shift theorem and the compact support assumption.
The proof I sketched out is more or less like this:

- Let's suppose F is not bounded and has compact support
- Then there must be at least one point in the support of F where the Fourier transform goes to infinity.
- Let u be that point, and translate the Fourier transform so that u coincides with the origin.
- This means that the inverse FT of the translated F must have integral=infinity.
- But from the Fourier shift-theorem we know that such a function is simply f itself multplied by the complex sinusoid e-iux
-
Note that |\int_{-\infty}^{+\infty}f(x)e^{-iux}dx| \leq \int_{-\infty}^{+\infty}|f(x)|dx which means that f is not absolute integrable.
- Now if we assumed f was in L1 we would reach a contradiction

However I don't see how to generalize this argument to the case when F does not have compact support, e.g. F(u) might go to infinity only for u-->infinity which would render the "translation trick" useless.
 
I don't understand your argument. If f is in L1 then, as you noted, the Fourier transform is bounded at every point by the integral of |f(x)|.
 
Yes. I have just realized that I in my proof I don't need the statement "there must be at least one point in the support of F where the Fourier transform goes to infinity". The inequality that I wrote simply says that the magnitude of the F at each point is bounded by the absolute integral of f.
Thanks again for clarifying this.
 
mnb96 said:
Thanks a lot!
I think I figured out a way to prove it, but it relies on the Fourier shift theorem and the compact support assumption.
The proof I sketched out is more or less like this:

- Let's suppose F is not bounded and has compact support
- Then there must be at least one point in the support of F where the Fourier transform goes to infinity.
- Let u be that point, and translate the Fourier transform so that u coincides with the origin.
- This means that the inverse FT of the translated F must have integral=infinity.
- But from the Fourier shift-theorem we know that such a function is simply f itself multplied by the complex sinusoid e-iux
-
Note that |\int_{-\infty}^{+\infty}f(x)e^{-iux}dx| \leq \int_{-\infty}^{+\infty}|f(x)|dx which means that f is not absolute integrable.
- Now if we assumed f was in L1 we would reach a contradiction

However I don't see how to generalize this argument to the case when F does not have compact support, e.g. F(u) might go to infinity only for u-->infinity which would render the "translation trick" useless.

Cant we use a continuity argument together with compactness to argue boundedness of the transform?
 
mnb96 said:
Yes. I have just realized that I in my proof I don't need the statement "there must be at least one point in the support of F where the Fourier transform goes to infinity". The inequality that I wrote simply says that the magnitude of the F at each point is bounded by the absolute integral of f.
Thanks again for clarifying this.
If you look at the reverse question. F bounded with compact support implies f is L1.
 

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