Question on limits and little-o notation

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    Limits Notation
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Discussion Overview

The discussion revolves around the application of little-o notation in the context of Fourier theory, specifically regarding the relationship between the behavior of a function \( F(\omega) \) and its product with \( \omega \) as \( \omega \) approaches infinity. Participants are trying to clarify the steps leading to the conclusion that \( F(\omega) = o(|\omega|^{-2}) \) from the result \( \omega F(\omega) = o(|\omega|^{-1}) \).

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant notes that the author deduces \( F(\omega) = o(|\omega|^{-2}) \) from \( \omega F(\omega) = o(|\omega|^{-1}) \) but seeks clarification on this step.
  • Another participant suggests dividing both sides by \( \omega \) to analyze the limit, implying that this could lead to a misunderstanding of the notation.
  • Some participants express uncertainty about the interpretation of little-o notation, emphasizing that it should not be treated as an ordinary equation and that the limit definition must be carefully applied.
  • A participant points out that dividing \( \omega F(\omega) \) by \( \omega \) leads to \( F(\omega) \) approaching zero, questioning the validity of the conclusion drawn by the author.
  • There is a discussion about the correct interpretation of limits and how they relate to the little-o notation, with one participant attempting to clarify their reasoning through a series of limit transformations.

Areas of Agreement / Disagreement

Participants express differing views on the application of little-o notation and the steps leading to the conclusion about \( F(\omega) \). There is no consensus on how the author arrived at the conclusion, and the discussion remains unresolved regarding the correct interpretation and application of the notation.

Contextual Notes

Participants highlight potential confusion regarding the manipulation of limits and the implications of dividing by \( \omega \). There is an emphasis on the need for careful consideration of the definitions and relationships involved in the little-o notation.

mnb96
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Hello,

I was studying the theorem of smoothness/compactness in Fourier theory and at the very last step of the proof one gets the result that \omega F(\omega)\to 0 when x\to \infty. The author of the book writes this result in little-o notation as: \omega F(\omega) = o(|\omega|^{-1}) which I understand, but then he deduces directly that: F(\omega)=o(|\omega|^{-2}). Can anyone explain this last step? Thanks.
 
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Divide both sides by omega.
 
Hi Simon,

if I am not wrong the little-o notation is just a notation and I assume it cannot always be treated as a ordinary equation. The notation f(x) = o(g(x)) should be equivalent to the statement: \lim_{x\to \infty} \frac{f(x)}{g(x)}=0
If that is true then we have: \lim_{x\to \infty} \omega F(\omega)=0 and dividing numerator and denominator by \omega we get: \lim_{x \to \infty} \frac{F(\omega)}{\omega^{-1}}=0 which according to the definition above should be written as: F(\omega) = o(\omega^{-1}) which is not the expected result.
 
f(x)=o(g(x)) means that f grows slower than cg

if wF(w) grows slower than 1/|w| then F(w) must grow slower than ...
http://en.wikipedia.org/wiki/Little_O_notation
http://www.math.caltech.edu/~2010-11/1term/ma001a1/bigolittleo.pdf
 
Last edited by a moderator:
mnb96 said:
Hi Simon,

if I am not wrong the little-o notation is just a notation and I assume it cannot always be treated as a ordinary equation. The notation f(x) = o(g(x)) should be equivalent to the statement: \lim_{x\to \infty} \frac{f(x)}{g(x)}=0
If that is true then we have: \lim_{x\to \infty} \omega F(\omega)=0
This makes no sense. Do you mean \lim_{\omega\to\infty} \omega F(\omega)= 0?

and dividing numerator and denominator by \omega we get: \lim_{x \to \infty} \frac{F(\omega)}{\omega^{-1}}=0
? No, dividing both sides of \lim_{\omega\to\infty}\omega F(\omega)= 0 by \omega gives \lim_{\omega\to\infty}F(\omega)= 0.

If you are thinking of \omega F(\omega) as a fraction with denominator 1, "Dividing both numerator and denominator by \omega" gives \frac{F(\omega)}{\omega}. That is, the denominator is \omega, not \omega^{-1}.

which according to the definition above should be written as: F(\omega) = o(\omega^{-1}) which is not the expected result.
 
Hi HallsofIvy,
thanks for your reply. I haven't had time to come back to this earlier.
HallsofIvy said:
This makes no sense. Do you mean \lim_{\omega\to\infty} \omega F(\omega)= 0?

Yes. Sorry, I meant to write: \lim_{\omega \to \infty}\omega F(\omega)=0
HallsofIvy said:
If you are thinking of \omega F(\omega) as a fraction with denominator 1, "Dividing both numerator and denominator by \omega" gives \frac{F(\omega)}{\omega}. That is, the denominator is \omega, not \omega^{-1}.

Uhm...I am not sure about this claim. What I wanted to say was:
\lim_{\omega\to\infty} \omega F(\omega)=\lim_{\omega\to\infty} \frac{\omega F(\omega)}{1} = \lim_{\omega\to\infty} \frac{\frac{1}{\omega}\omega F(\omega)}{\frac{1}{\omega}1} = \lim_{\omega\to\infty} \frac{F(\omega)}{\frac{1}{\omega}} = \lim_{\omega\to\infty} \frac{F(\omega)}{\omega^{-1}}=0

As you see, the rightmost equality seems to imply that: F(\omega) = o(|\omega|^{-1}) but according to the textbook it should be: F(\omega) = o(|\omega|^{-2}). It is stilll totally unclear how the author arrived at this last conclusion.
 
Last edited:

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