Physics Asked by ernst on December 26, 2020
Let the stochastic process ${X_t}$ be defined by the following SDE (Ito’s convention for discretization)
$dX_t=frac{1}{p}S_tg(X_t)dt+sqrt{2}dW_t$
where $W_t$ is a standard Wiener process, $g: mathrm{R}rightarrow mathrm{R}$ is a $C^{infty}$ function and $S_t$ is an other (white) stochastic process described by
begin{align}
&p(S_t=1)=p,quad p(S_t=0)=1-p\
& S_tperp S_tau, quad forall tneqtau
end{align}
where $pin(0,1]$
Informally you could think of $S_t$ as a telegraph process https://en.wikipedia.org/wiki/Telegraph_process
My questions are the following:
Does it make sense to define a process like $S_t$?
If 1) has positive answer, can I use the infinitesimal generator formalism (https://en.wikipedia.org/wiki/Infinitesimal_generator_(stochastic_processes)) to derive, for example the Fokker Planck equations for the process $X_t$?
If you have link to similar problems solved in any physics area it would be awesome.
Forgive me for being formally imprecise, I am not trained in pure math but I do use SDEs simulation schemes for engineering/physics problems.
I am not an authority in the subject, so the following remarks are based on my limited experience:
My own knowledge about telegraph process and the associated results traces back to the course on Functional methods for stochastic processes for physicists, based on the book by Klyatskin (in Russian). A google search showed me that there are several of his books published in English with somewhat different titles, and I am not sure which one corresponds to the one that I studied from: see here and here.
Correct answer by Vadim on December 26, 2020
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