In filtering theory the Zakai equation is a linear stochastic partial differential equation for the un-normalized density of a hidden state. In contrast, the Kushner equation gives a non-linear stochastic partial differential equation for the normalized density of the hidden state. In principle either approach allows one to estimate a quantity function (the state of a dynamical system) from noisy measurements, even when the system is non-linear (thus generalizing the earlier results of Wiener and Kalman for linear systems and solving a central problem in estimation theory). The application of this approach to a specific engineering situation may be problematic however, as these equations are quite complex.[1] [2] The Zakai equation is a bilinear stochastic partial differential equation. It was named after Moshe Zakai.[3]
Assume the state of the system evolves according to
dx=f(x,t)dt+dw
and a noisy measurement of the system state is available:
dz=h(x,t)dt+dv
where
w,v
p(x,t)
dp=L[p]dt+phTdz
where
L[p]=-\sum
\partial(fip) | |
\partialxi |
+
12 | |
\sum |
\partial2p | |
\partialxi\partialxj |
As previously mentioned,
p
p
Note that if the last term on the right hand side is omitted (by choosing h identically zero), the result is a nonstochastic PDE: the familiar Fokker–Planck equation, which describes the evolution of the state when no measurement information is available.