What role does the delta function play in quantum mechanics and field theory?

[Ratzinger]

As I read in my quantum mechanics book the delta function is sometimes called the sampling function because it samples the value of the function at one point.
\int {\delta (x - x')} f(x')dx' = f(x)

But then I opened a quantum field book and I found equations like that:
\phi (x) = \frac{1}{{(2\pi )^{3/2} }}\int {d^4 p\delta (p^2 } - m^2 )A(p)e^{ - ip \cdot x}

(\partial _\nu \partial ^\nu + m^2 )\phi (x) = \frac{1}{{(2\pi )^{3/2} }}\int {d^4 p( - p^2 } + m^2 )\delta (p^2 - m^2 )A(p)e^{ - ip \cdot x}

Can someone explain me what the delta function does here? What it is sampling? How these equations work?

thank you

 

[Hurkyl]

The delta function does the same thing!

I don't know if "sampling" is a good adjective, but I'll run with it. In the integral

\int d^4 p \, \delta (p^2 - m^2 )A(p)e^{ - ip \cdot x}

you're "sampling" the function A(p)e^{ - ip \cdot x} over the region where p^2 - m^2 = 0.

We can reduce this down to the known case, if we like, as follows: we can split this up into an iterated integral, with p_0 being the innermost. Then we have:

<br /> \iiint \int \delta(p_0^2 - \vec{p}\,{}^2 - m^2) A(p) e^{-ip \cdot x} \, dp_0 \, d^3 \vec{p}<br />

so the innermost integral is of the form:

<br /> \int \delta(x^2 - a^2) f(x) \, dx<br />

Now, if I make the substitution u = x^2, we have du = 2 x dx so that dx = du / 2 \sqrt{u}, and the integral becomes

(yes, I know I'm being lazy with the bounds -- note that when tracing x over (-\infty, +\infty), u traces over [0, +\infty) twice! I really should break the integral up into two parts)

<br /> \int \delta(u - a^2) f(\sqrt{u}) \frac{1}{2 \sqrt{u}} \, du<br />

which becomes (one term for each of the times u traces over 0, +\infty):

<br /> f(a) \frac{1}{2a} - f(-a) \frac{1}{-2a}<br /> = \frac{f(a) + f(-a)}{2a}<br />

I'll leave it to you to work out the general case when the argument to \delta is an arbitrary function of the dummy variable.

Anyways, if my intuition about these things is anywhere close to accurate, your integral for \phi(x) should reduce to a surface integral over the hypersurface given by the equation p^2 - m^2 = 0.

 

[Norman]

As I read in my quantum mechanics book the delta function is sometimes called the sampling function because it samples the value of the function at one point.
\int {\delta (x - x&#039;)} f(x&#039;)dx&#039; = f(x)
But then I opened a quantum field book and I found equations like that:
\phi (x) = \frac{1}{{(2\pi )^{3/2} }}\int {d^4 p\delta (p^2 } - m^2 )A(p)e^{ - ip \cdot x}
(\partial _\nu \partial ^\nu + m^2 )\phi (x) = \frac{1}{{(2\pi )^{3/2} }}\int {d^4 p( - p^2 } + m^2 )\delta (p^2 - m^2 )A(p)e^{ - ip \cdot x}
Can someone explain me what the delta function does here? What it is sampling? How these equations work?
thank you

notice here that the delta function has as its argument quadratic functions. It can be a little confusing about what to do with these. Well just use this formula:
\delta[g(x)]=\sum_i\frac{\delta(x-x_i)}{|g&#039;(x_i)|}
by the way, the sum is over the roots of g.
In your equation above, after you use this step everything should be clear- it functions just how you would expect it to.
and check out this page for help with dirac delta functions
http://mathworld.wolfram.com/DeltaFunction.html

 

[Ratzinger]

thanks Hurykl, thanks Norman, thanks physicsforums, thanks the Internet

and a great weekend to everybody