friend said:
Let me turn this around and ask, if it can be proved that the integral of the dirac delta does not change its value or its appearance (a change of coordinates only changes the variable used in the integral, but otherwise stays the same), would that prove that there does exist a coordinate independent intrinsic definition of the dirac delta?
You need to be more rigorous in what you want from "coordinate independent intrinsic definition". I say this because "Dirac is the identity element of the convolution"
is a coordinate independent intrinsic definition. Proving that there really is a distribution that satisfies that definition is long and tedious (it uses a technique called "approximating the identity") but is doable.
As to your specific question, I guess so?
Does the measure have to be integrated against a function of compact support? What about integrating against f(x)=1?
Ah. First consider this: suppose we have a smooth function whose domain is ℝ, ##f\in C^\infty(\mathbb{R})##. Now is this function an element of ##C(0,\infty)##? Well it isn't because the domains are different, but we can take f and restrict it to the positives and
that restriction is an element of ##C(0,\infty)##.
Same thing here. The Dirac
as a measure can be integrated against f(x)=1, but the Dirac
as a Schwartz distribution can't. Nonetheless, you can take the Dirac measure and restrict is to become a Schwartz measure.
I suppose you could do a formal sum over every point, p, in the set of your manifold, M, without referring to coordinate system. If you did this for every point in M, you'd get 1 for every p \in A \subset M for which δp(A)=1. Then Ʃpδp(A) would give you the size of A, right?
Yes, but in a trivial manner. p is always an element of A, so really you are just evaluating ##\sum_{p\in A}1##.
Edit: Oh wait you're summing over ##p \in M##? Then that means M is countable.