the Riesz representation theorem is perhaps the mathematical "keystone" that connects our pictures of the discrete and continuous worlds. without this theorem, mathematicians could not have rigorously defined integration over expressions involving Dirac delta functions (something that physicists had first intuited without proof).

It allows us to transfer ideas about inner product spaces over to their dual spaces of linear functionals:

https://en.wikipedia.org/wiki/Riesz_representation_theorem

#Dirac #DiracDelta #mathematics

Riesz representation theorem - Wikipedia

- the #Diracdelta function, although not a function, is a finite Borel measure. Its Fourier transform is a constant function (whose specific value depends upon the form of the Fourier transform used).
lemma does not hold for arbitrary distributions. #Diracdelta function distribution formally has a finite integral over the real line, but its #Fourier transform is a constant (the exact value depends on the form of the transform used) and does not vanish at infinity.
An approximate identity I in a #convolution algebra plays the same role as a sequence of function approximations to the #Diracdelta function (I).
#Fejér kernels of #Fourier series theory give rise to an approximate identity.
An approximate identity I in a #convolution algebra plays the same role as a sequence of function approximations to the #Diracdelta function (I).
#Fejér kernels of #Fourier series theory give rise to an approximate identity.

For #Diracdelta distribution δ
on ℝ, then mδ = m(0)δ, and if δ′ is the derivative of the delta distribution, then

mδ '=m(0)δ '-m'δ =m(0)δ'-m'(0)δ

For #Diracdelta distribution δ
on ℝ, then mδ = m(0)δ, and if δ′ is the derivative of the delta distribution, then

mδ '=m(0)δ '-m'δ =m(0)δ'-m'(0)δ