Evaluate ##\int_{-\infty}^{\infty} e^{-|x|}\delta(x^2 +2x -3) dx##

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SUMMARY

The integral ##\int_{-\infty}^{\infty} e^{-|x|}\delta(x^2 +2x -3) dx## evaluates to ##\frac{e^{-3}}{4}##. The Dirac delta function is non-zero only when its argument is zero, which occurs at the roots of the equation ##x^2 + 2x - 3 = 0##, specifically at ##x = 1## and ##x = -3##. Each root contributes to the integral, and the evaluation requires careful handling of the delta function's properties, particularly when dealing with non-linear arguments.

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Homework Statement
evaluate ##\int_{-\infty}^{\infty} e^{-|x|}\delta(x^2 +2x -3) dx##
Relevant Equations
##\int_{-\infty}^{\infty} \delta(x-a)f(x) dx = f(a)##
Hi,

Is it correct to say that the dirac delta function is equal to 0 except if the argument is 0?
Thus, ##x^2 +2x -3## must be equal to 0.

Then, we have x = 1 or -3. What does that means?

##\int_{-\infty}^{\infty} e^{-|x|}\delta(x^2 +2x -3) dx = e^{-1}## and/or ##e^{-3}## ?

Thank you
 
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The delta function argument will be zero at two points. Both will contribute to the integral. You also need to consider that ##\delta(ax) = \delta(x)/|a|## with the appropriate generalisation to non-linear arguments.
 
I'm not sure to fully understand.
What should be the result? In a case where the argument is 0 only if x = 1, the result would have been ##e^{-1}##
 
DragonBlight said:
I'm not sure to fully understand.
What should be the result? In a case where the argument is 0 only if x = 1, the result would have been ##e^{-1}##
No, this is incorrect. That is only true if you have something like ##\delta(x-1)##. Whether or not there are additional constants depend also on the derivative of the argument. See the Wikipedia entry https://en.wikipedia.org/wiki/Dirac_delta_function particularly under ”properties”.
 
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DragonBlight said:
Then, we have x = 1 or -3. What does that means?

##\int_{-\infty}^{\infty} e^{-|x|}\delta(x^2 +2x -3) dx = e^{-1}## and/or ##e^{-3}## ?
Naively, you might expect the result to be the sum of those two because the integral is essentially a sum, but it's a little more complicated.
DragonBlight said:
I'm not sure to fully understand.
What should be the result? In a case where the argument is 0 only if x = 1, the result would have been ##e^{-1}##
The one thing you know about the delta function is
$$\int f(x)\delta(x)\,dx = f(0).$$ Now consider an integral like
$$\int f(x)\delta(2x)\,dx.$$ Because of the ##2x## inside the delta function, it's not exactly in the same form as the first integral. Hence, it would be wrong to conclude the second integral is equal to ##f(0)## even though that's where the argument of the delta function is 0. If you use the substitution ##u=2x##, however, you can transform the integral into the form above so that you can evaluate it:
$$\int f(x)\delta(2x)\,dx = \int\underbrace{ \frac 12 f(u/2)}_{g(u)} \delta(u) \,du = \int g(u)\delta(u)\,du = g(0) = \frac 12 f(0).$$
 
So, can I replace the argument with u to find a "form" that I know for the delta function in every situation?

For example, ##u = x^2 +2x -3## and ##x = -1 \pm \sqrt{u + 4}##
Thus, I have ##e^{- 1 - \sqrt{u + 4}}## and ##\delta(u)##

So we have
##\int_{-\infty}^{\infty} e^{-1-\sqrt{u+4} \delta(u) \frac{du}{2\sqrt{u+4}}}##
For ##\delta(0)##
##=e^{-3}/4##
 
Something like that. You should read the Wikipedia page @Orodruin linked to, particularly the part about composition with a function.
 
DragonBlight said:
So, can I replace the argument with u to find a "form" that I know for the delta function in every situation?

For example, ##u = x^2 +2x -3## and ##x = -1 \pm \sqrt{u + 4}##
Thus, I have ##e^{- 1 - \sqrt{u + 4}}## and ##\delta(u)##

So we have
##\int_{-\infty}^{\infty} e^{-1-\sqrt{u+4} \delta(u) \frac{du}{2\sqrt{u+4}}}##
For ##\delta(0)##
##=e^{-3}/4##
You must be much more careful with your charge of variables in the integral. What are the bounds of the new integral?
 

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