Sufficient condition for bounded Fourier transform

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SUMMARY

The discussion centers on establishing a sufficient condition for a function f: ℝ → ℝ such that its Fourier transform F = ℱ(f) is bounded, particularly under the assumption that F has compact support. The participants conclude that if f is in L1, then F is bounded, as the Fourier transform's magnitude is constrained by the absolute integral of f. The Fourier shift theorem plays a crucial role in the proof, demonstrating that if F is not bounded, it leads to a contradiction regarding the integrability of f.

PREREQUISITES
  • Understanding of Fourier transforms and their properties
  • Familiarity with the concept of compact support in functions
  • Knowledge of the Fourier shift theorem
  • Basic principles of L1 integrability
NEXT STEPS
  • Study the implications of the Fourier shift theorem in detail
  • Explore the relationship between compact support and boundedness of Fourier transforms
  • Investigate the properties of L1 spaces and their significance in Fourier analysis
  • Examine continuity arguments in the context of Fourier transforms
USEFUL FOR

Mathematicians, particularly those specializing in Fourier analysis, theoretical physicists, and anyone interested in the properties of Fourier transforms and their applications in signal processing.

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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