Property of the Dirac Delta Function

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SUMMARY

The Dirac delta function, denoted as δ(t), is defined such that δ(t) = ∞ when t = 0 and δ(t) = 0 otherwise. To demonstrate that the integral of δ(t) from negative infinity to infinity equals 1, one can utilize the limit of a sequence of functions, specifically f_m(t) = m * exp(-(mt)^2)/sqrt(π), as m approaches infinity. This approach aligns with the concept of distributions, where the integral of δ(t) can be computed through the limit of integrals of ordinary functions.

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  • Understanding of the Dirac delta function and its properties
  • Familiarity with limits and sequences of functions
  • Basic knowledge of integration techniques in calculus
  • Concept of distributions in mathematical analysis
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jaejoon89
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Homework Statement



How do you show that int[delta(t)]dt from negative infinity to infinity is 1?


Homework Equations



Dirac delta function defined as infinity if t = 0, 0 otherwise

The Attempt at a Solution



My teacher said that it has to do with m->infinity for the following function
f_m(t) = m*exp(-(mt)^2)/sqrt(pi)

I don't understand - what is this function exactly and how does the delta function property follow?
 
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The bad news: delta(t) isn't a function, and \int_{-\infty}^{+\infty} \quad \, dx isn't the integration operation you learned about in your elementary calculus class.

The good news: they're close enough for many purposes.


One of the methods to work with these "distributions" is to name them by means of a limit. (But this limit isn't calculated in the set of functions, so don't try to apply what you know of limits of functions) delta(t) can be named as the "limit" of the sequence of functions you mentioned.

Once you've named a distribution (names aren't unique), f(x) = \lim_{n \rightarrow +\infty} f_n(x) it's "integral" \int_{-\infty}^{+\infty} f(x) \, dx is defined to be:

\lim_{n \rightarrow +\infty} \int_{-\infty}^{+\infty}f_n(x) \, dx

This last expression has finally been written in terms of ordinary limits and ordinary integration of ordinary functions, and so it can be computed by ordinary means.



(For the record I haven't given all details about what's going on)
 
jaejoon89 said:
Dirac delta function defined as infinity if t = 0, 0 otherwise
That is not the definition of the delta function. Did your teacher actually say that? For most purposes, the defining property of the delta function can be taken as

\int_{-\infty}^{\infty} \delta(x-x') f(x') dx' = f(x).​

Your problem can be solved by choosing a suitable f in the integral.

(You posted this in "Advanced Physics", so I'm assuming you encountered this in a physics course. If you encountered it in a math course, the definition I gave is probably not precise enough. As Hurkyl said, the rigorous way to think about delta functions is in terms of what are called "distributions")
 
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