Dirac delta function homework help

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Discussion Overview

The discussion revolves around the properties and implications of the Dirac delta function, particularly in the context of integrals involving multiple delta functions. Participants explore whether expressions like \(\int_{-\infty}^{\infty} f(x)\delta(x-a)\delta(x-b)dx\) have any meaningful interpretation, especially when \(a\) and \(b\) are constants.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants assert that the integral \(\int_{-\infty}^{\infty} f(x)\delta(x-a)\delta(x-b)dx\) does not have a defined meaning, suggesting it equals zero if forced to assign a value.
  • Others propose that defining a generalized function \(g(x) = f(x)\delta(x-a)\) leads to a different interpretation of the second integral, although they express uncertainty about its correctness.
  • One participant argues that \(g(x)\) is not a constant but rather a function multiplied by the delta function, leading to confusion about its properties during integration.
  • Another participant references Schwartz's theorem, stating that multiplying two distributions is problematic, indicating a deeper theoretical concern regarding the manipulation of delta functions.
  • There is a discussion about whether \(g(x)\) can be considered a Lebesgue square measurable function, with some participants questioning the validity of such a conclusion.
  • A later reply suggests that if \(a\) or \(b\) were treated as variables rather than constants, the expression could be interpreted as a distribution, leading to a different outcome when convolved with another function.

Areas of Agreement / Disagreement

Participants express differing views on the meaning and validity of the integral involving multiple delta functions. There is no consensus on whether the expression has a defined meaning or how to interpret it correctly.

Contextual Notes

Participants highlight limitations in the manipulation of distributions, particularly regarding the multiplication of delta functions and the implications for integrals involving them. The discussion reflects unresolved mathematical steps and assumptions about the nature of generalized functions.

shoehorn
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Suppose that we take the delta function [tex]\delta(x)[/tex] and a function f(x). We know that

[tex]\int_{-\infty}^{\infty} f(x)\delta(x-a)\,dx = f(a).[/tex]

However, does the following have any meaning?

[tex]\int_{-\infty}^{\infty} f(x)\delta(x-a)\delta(x-b)dx,[/tex]

for some constants [tex]-\infty<a,b<\infty[/tex].
 
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shoehorn said:
Suppose that we take the delta function [tex]\delta(x)[/tex] and a function f(x). We know that

[tex]\int_{-\infty}^{\infty} f(x)\delta(x-a)\,dx = f(a).[/tex]

However, does the following have any meaning?

[tex]\int_{-\infty}^{\infty} f(x)\delta(x-a)\delta(x-b)dx,[/tex]

for some constants [tex]-\infty<a,b<\infty[/tex].

Remember that [itex]\delta[/itex] is not a true function. It is a "distribution" or "generalized function". The first integral is defined for distributions but the second isn't. (If we were to force a meaning on it, the only reasonable value it could have would be 0.)

You could do that in more than one dimension:
[tex]\int_{x=-\infty}^{\infty}\int_{y=-\infty}^{\infty}f(x,y)\delta(x-a)\delta(y-b)dydx= f(a,b)[/itex][/tex]
 
Here's what I was thinking about it. The integral

[tex]\int_{-\infty}^\infty \, f(x)\delta(x-a) dx[/tex]

integrates a function f(x) times a distribution [tex]\delta[/tex], so the whole thing is an integral of a generalized function, dependent on x. Suppose now that I define a generalized function [tex]g(x)[/tex] according to

[tex]g(x) \equiv f(x)\delta(x-a).[/tex]

Then the second integral becomes

[tex]\int_{-\infty}^\infty f(x)\delta(x-a)\delta(x-b)\,dx = \int_{-\infty}^\infty g(x) \delta(x-b).[/tex]

My instinct is to then conclude that

[tex]\int_{-\infty}^\infty g(x)\delta(x-b)\, dx = g(b) = f(b)\delta(b-a)[/tex]

Thus, the second integral is itself something which has meaning only if it appears within an integral. Yet you don't think that this is correct?
 
Last edited:
the function g(x) is basiclly a constant (f(a)) times the dirac delta function. so in your second integral you want the integral of the product of two different DD functions times a constant, that would equal 0
 
daniel_i_l said:
the function g(x) is basiclly a constant (f(a)) times the dirac delta function. so in your second integral you want the integral of the product of two different DD functions times a constant, that would equal 0

I'm afraid I don't see how you conclude that g(x) is a constant. Going with the definition I gave above,

[tex]g(x)\equiv f(x)\delta(x-a)[/tex]

for some function f(x). The only relationship between g(x) and f(a) is

[tex]\int_{-\infty}^\infty g(x)\,dx = \int_{-\infty}^\infty f(x)\delta(x-a)\,dx = f(a),[/tex]

i.e., the integral of g(x) is equal to f(a).
 
shoehorn said:
I'm afraid I don't see how you conclude that g(x) is a constant.
I didn't say that it was a constant, i said that is was equal to a constant times the DD function. what i meant to say that was in this case you could look at g(x) as being g(x) = f(a)*DD(x-a) when you're doing the integral. so you're right, it doesn't really equal f(a)*DD(x-a) but when you integrate you get the same resault when you interchange the two.
and anyway f(b)DD(b) = 0.
 
Last edited:
- Shoehorn according to "Schwartz theorem2 you can't multiply 2 distribution..this is really "nasty" since avoiding this (if we could) we would have solved divergences in the form [tex]\int_{0}^{\infty}dx x^{n}[/tex] using "Casual perturbation theory2 (see wikipedia) although i believe that for big n:

[tex]\delta (x-a) \delta (x-b) =n^{2}\pi e^{-n^{2}((x-a)^2 +(x-b)^2)} <br /> [/tex] for n tending to [tex]\infty[/tex]
 
shoehorn said:
As a result, if, for example, f(x) is [tex]L^2[/tex], then g(x) is [tex]L^2[/tex] also.


How do you conclude something that is not even a function is actually a lebesgue square measurable function?
 
matt grime said:
How do you conclude something that is not even a function is actually a lebesgue square measurable function?

Oops, sorry. I was editing a post earlier and pasted that in by accident. Please ignore it - it's obviously not true. :-)
 
  • #10
shoehorn said:
However, does the following have any meaning?

[tex]\int_{-\infty}^{\infty} f(x)\delta(x-a)\delta(x-b)dx,[/tex]

for some constants [tex]-\infty<a,b<\infty[/tex].
No.

However, if a (or b) was a variable, then this expression could be considered a distribution. Convolving it with h(a) gives:

[tex] \int_{-\infty}^{+\infty}\int_{-\infty}^{+\infty}<br /> f(x) h(a) \delta(x-a) \delta(x-b) \, da \, dx<br /> = f(b) h(b)[/tex]
 

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