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

Click For Summary
The Fourier transform of e^{2\pi ikx} equals the delta function δ(k) because it behaves like a delta function, despite being a distribution rather than a conventional function. The integral does not converge for k ≠ 0, highlighting the idealized nature of the delta function, which is zero everywhere except at one point. The discussion emphasizes that while the delta function is not a function in the traditional sense, it serves a functional role similar to Fourier series coefficients in representing periodic functions. The Fourier transform operates within the framework of Hilbert space, where neither the delta function nor the exponential function fully meets the necessary criteria. For a rigorous understanding, exploring texts on distributions or generalized functions is recommended.
jasonc65
Messages
19
Reaction score
0
Why is it that the Fourier transform of e^{2\pi ikx} is equal to \delta(k) ? The delta function is supposed to be zero except at one point. But the integral doesn't converge for k \ne 0. Yet I see a lot of books on QFT use this identity.
 
Physics news on Phys.org
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 \int^\infty_{-\infty}e^{2\pi ikx} dx 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. :)
 
If there are an infinite number of natural numbers, and an infinite number of fractions in between any two natural numbers, and an infinite number of fractions in between any two of those fractions, and an infinite number of fractions in between any two of those fractions, and an infinite number of fractions in between any two of those fractions, and... then that must mean that there are not only infinite infinities, but an infinite number of those infinities. and an infinite number of those...

Similar threads

  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
Replies
1
Views
2K
  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 6 ·
Replies
6
Views
3K
  • · Replies 9 ·
Replies
9
Views
2K