Why is Fourier transform of exp(ix) a delta?

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Discussion Overview

The discussion revolves around the Fourier transform of the exponential function \( e^{2\pi ikx} \) and its relationship to the delta function \( \delta(k) \). Participants explore the implications of this identity, its mathematical rigor, and the conceptual understanding of the delta function within the context of Fourier analysis and distributions.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions why the Fourier transform of \( e^{2\pi ikx} \) is equal to \( \delta(k) \), noting that the delta function is zero except at one point and that the integral does not converge for \( k \neq 0 \).
  • Another participant clarifies that the delta function is not a traditional function but behaves like one, raising questions about its definition at points where it is not zero.
  • A participant discusses the Fourier series for \( f(x) = \cos(x) \), suggesting that its coefficients lead to a similar understanding of the delta function as a generalized function or distribution.
  • Further elaboration on the behavior of the integral \( \int_{-\infty}^{\infty} e^{2\pi ikx} dx \) is presented, indicating that it behaves like a delta function, but also noting the lack of rigor in the informal treatment of these concepts.
  • Another participant suggests consulting literature on distributions or generalized functions for a more rigorous treatment of the topic.

Areas of Agreement / Disagreement

Participants express differing views on the nature of the delta function and its mathematical treatment, indicating a lack of consensus on the rigor of the explanations provided. Some participants seem to agree on the need for a more formal approach, while others challenge the informal interpretations presented.

Contextual Notes

The discussion highlights limitations in the understanding of the delta function and its properties, particularly regarding its classification as a function versus a distribution. There are also unresolved questions about the mathematical rigor of the Fourier transform and its implications for functions that do not satisfy traditional boundary conditions.

jasonc65
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Why is it that the Fourier transform of [tex]e^{2\pi ikx}[/tex] is equal to [tex]\delta(k)[/tex] ? The delta function is supposed to be zero except at one point. But the integral doesn't converge for [tex]k \ne 0[/tex]. Yet I see a lot of books on QFT use this identity.
 
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delta isn't a function (what is it at the point where it is not zero?)

It is the delta 'function' because it behaves as the delta function.
 
Suppose you were to ask for the Fourier Series for f(x)= cos(x)?

Since the Fourier Series is, by definition, a sum of sines and cosines that add to f(x).
Since f(x)= cos(x), its Fourier series coefficients are just a1= 1, all other coefficients are 0. The delta "function" (it's really a "distribution" or "generalized function") is the functional version of that.
 
HallsofIvy said:
Suppose you were to ask for the Fourier Series for f(x)= cos(x)?

Since the Fourier Series is, by definition, a sum of sines and cosines that add to f(x).
Since f(x)= cos(x), its Fourier series coefficients are just a1= 1, all other coefficients are 0. The delta "function" (it's really a "distribution" or "generalized function") is the functional version of that.
Very interesting. The integral [tex]\int^\infty_{-\infty}e^{2\pi ikx} dx[/tex] does in some ways behave like a delta function. And the delta function is an ideal function. However it's own Fourier transform is an exponential, which is a real funtion. The Fourier transform as an operator on Hilbert space is unitary, and squares to -1. Neither the delta function nor the exponential function are in Hilbert space, the latter because it doesn't satisfy boundary conditions, and the former because it isn't even a funtion. The idea is very informal and lacks rigour. I have never seen it given a rigorous basis.
 
Then get a book on "distributions" or "generalized functions" everything is done with complete rigor.
 
Thanks for the suggestion. :)
 

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