- #1
kleinwolf
- 295
- 0
Consider the density probability function following the diffusion equation with diffusion parameter D, with the initial condition [tex] f(x,t=0)=\delta(x) [/tex] :
[tex] f(x,t)=\frac{e^{-\frac{x^2}{4Dt}}}{\sqrt{4\pi Dt}} [/tex]
From this : if t=0, then the particle is at x=0.
Consider a very small t>0...then we get [tex] P(A<x<A+dx)>0 \forall A>0, dx>0 [/tex].
Which means that : the particle has a non-vanishing prob. of having traveled a distance as big as you want in a time as small as you want.
Does anybody know if relativistic brownian motion was studied ?
There the function f should be compact...or something like that ?
[tex] f(x,t)=\frac{e^{-\frac{x^2}{4Dt}}}{\sqrt{4\pi Dt}} [/tex]
From this : if t=0, then the particle is at x=0.
Consider a very small t>0...then we get [tex] P(A<x<A+dx)>0 \forall A>0, dx>0 [/tex].
Which means that : the particle has a non-vanishing prob. of having traveled a distance as big as you want in a time as small as you want.
Does anybody know if relativistic brownian motion was studied ?
There the function f should be compact...or something like that ?