lavidaenrosa said:
Thx, but I don't get it! Is there a way to show this? Or at least an explanation? I know the relation ∫δ(x-a) dx= θ(x-a) but I've never seen
∫δ(g(x)-a) dx =
There is a serious issue with (a), but first, let's simplify it. Around the positive zero ##x_n = (2n+1)\pi/2## of ##f(x) = x^2 \cos(x)## we have ##f(x) \approx f'(x_n) (x-x_n)##, so integration of ##\delta(f(x))## near there gives just ##1/f'(x_n)##, as you said. However, since f(x) is even, the corresponding term for ##x = -x_n## has ##f'(-x_n) = -f'(x_n)##, so the contributions from ##x = x_n## and ##x = -x_n## cancel.
So, all that matters is the value of ##\int_{-a}^a \delta(f(x)) \, dx## for small ##a > 0##, and this is where we run into trouble. For small ##|x|##, ##f(x)## looks like just plain ##x^2##, but the point is that its graph does not cross the x-axis; it grazes the x-axis from above, so one is essentially looking at ##2\int_0^a \delta(f(x)) \, dx##. This integrates only half of the ##\delta## function, so can either be regarded as non-existent, or can be looked at through a limiting procedure that gives ##\delta(\cdot)## in the limit. If you regard ##\delta(u)## as a limit of
even functions ##f_n(u)##, then your "half-##\delta##" integral would be one half of the usual. However, one can equally well regard ##\delta(u)## as a limit of unsymmetrical (not even) functions ##f_n(u)##, in which case the "half-##\delta##" integral can be a fraction other than 1/2---basically, you can make it equal anything from 0 to 1 if you want to.
However, let's not overlook the fact that f(0) = 0 in your case.