Thanks for the interesting post. Looking forward to seeing where this series is going. Mostly for my own understanding, I’m going to mess around with fourier transforms and convolutions in this comment.
Proof that the fourier transform of the convolution of 2 functions is the product of their fourier transforms:
F[f⋆g]=∫dte−iωt∫dτf(τ)g(t−τ)
=∫dτf(τ)e−iωτ∫dte−iω(t−τ)g(t−τ)
Let u=t−τ. Then, holding τ constant, du=dt. So:
F[f⋆g]=∫dτf(τ)e−iωτ∫due−iωug(u)=F[f]F[g]
Fourier transform of a general Gaussian distribution, G(t)=e−(t−μσ)2:
Thanks for the interesting post. Looking forward to seeing where this series is going. Mostly for my own understanding, I’m going to mess around with fourier transforms and convolutions in this comment.
Proof that the fourier transform of the convolution of 2 functions is the product of their fourier transforms:
F[f⋆g]=∫dte−iωt∫dτf(τ)g(t−τ)
=∫dτf(τ)e−iωτ∫dte−iω(t−τ)g(t−τ)
Let u=t−τ. Then, holding τ constant, du=dt. So:
F[f⋆g]=∫dτf(τ)e−iωτ∫due−iωug(u)=F[f]F[g]
Fourier transform of a general Gaussian distribution, G(t)=e−(t−μσ)2:
F[G](ω)=∫dte−(t−μσ)2e−iωt
Let u=t−μ.
=∫due−(uσ)2e−iω(u+μ)=∫due−(uσ)2−iω(u+μ)
Now we complete the square:
=e−iωμ∫due−(uσ)2−iωu+(σω)2−(σω)2
=e−iωμe−(σω)2∫due−(uσ+iσω)2
Let v=(uσ+iσω), so that σdv=du.
=e−iωμe−(σω)2σ∫dve−v2=e−iωμe−(σω)2σ√π
We get a result of √π for the integral in v using a clever trick [https://en.wikipedia.org/wiki/Gaussian_integral#By_polar_coordinates]. So the result is:
F[G](ω)=σ√πe−iωμe−(σω)2
σ2 isn’t actually the variance here. The variance is σ2/2. Sorry for the confusing choice of variable name.