Is the Fourier Transform of a Constant a Dirac Delta Function?

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Homework Help Overview

The discussion revolves around the Fourier transform of a constant function and its relationship to the Dirac delta function. Participants are exploring the mathematical properties and implications of this transformation.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to prove that the Fourier transform of a constant yields a Dirac delta function but encounters difficulties in demonstrating this for values of k other than zero. Other participants suggest starting from the properties of the delta function and its Fourier transform, as well as using contour integration to address ambiguities in the integral.

Discussion Status

Participants are actively engaging with the problem, offering various methods and insights. There is a mix of approaches being discussed, including direct computation and theoretical reasoning. No explicit consensus has been reached, but several productive lines of inquiry are being explored.

Contextual Notes

Some participants note the challenges posed by the integral's behavior at k=0 and the undefined nature for other values of k. The discussion also touches on the definitions of the Fourier transform and its inverse, which may influence the interpretation of results.

Kolahal Bhattacharya
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Homework Statement



Fourier transform of a constant

Homework Equations





The Attempt at a Solution



I am trying to prove that Fourier Transform of a constant is a Dirac delta function.I have fed f(x)=1 in the formula of Forward Fourier transform and got F(k)=int{exp[-ik*pi*x]}dx
I know that this is delta function with argument k.But cannot prove it.It's sure to give infinity at k=0.But,for other values of k I am not getting the integral=0.So,an attempt through the way of definition fails.Can anyone help me?
 
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Start with \delta(x) and Fourier transform it. You get a constant.
 
Here is a method how to do it.It took some time,however.

First, you find the F.T. of delta(x) and it turns out as a constant F(k)=1
Then,you did inverse transform of 1 which yields a delta function.
Like this: int{exp[ik'x']dk'}=2*pi*delta(x')
Putting k'=x and x'=-k,we have
int{exp[-ikx]dx}=2*pi*delta(-k)

Now consider the F.T. of a constant function g(x)=c
G(k)=int{c exp[-ikx]dx}=c[2*pi*delta(-k)]=2*pi*c delta(k)
 
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If you compute Int( exp(-ikx), x=-Infinity..Infinity) you get Infinity for k=0 and 2/k sin(k Infinity) that is undefined for k=/=0. To remove this ambiguity use the Residue theorem giving Int( exp(-ikz), z on C ) = 0 where C is the contour of a half-disk of radius R. Then using the parametrisation z = R exp (i alpha) and letting R->Infinity you will find Int( exp(-ikx), x=-Infinity..Infinity) = 0 for k =/=0. Using this reasoning you get that Int( exp(-ikx), x=-Infinity..Infinity) is "proportional" to delta(k).

To understand the factor 2*pi you have to work in the context of the definitions of the Fourier transform and of his inverse. These definitions results from the Fourier serie as T->Infinity, see http://en.wikipedia.org/wiki/Fourier_Transform.
 
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