Well, to be clear usually the white noise doesn't depend on the solution $X(t)$ because that would make the problem highly nonlinear if not just ill-posed. Even in 1d it is unclear how to study $$dX_{t}=adt+bdW(X_{t},t).$$
Instead, the generalization is that of including more coordinates but for the solution and possibly the noise too i.e. stochastic-pdes
$$du(t,x)=\mathcal{L}u(t,x)dt+b(u(t,x))\xi(t,x),$$
where $\xi(t,x)=\dot{W}(t,x)$ is called the space-time white noise (see below).
\begin{equation}
\mathbb{E}\left[\xi(z,t) \right] = 0;\quad \mathbb{E}\left[\xi(z,t)\xi(z',t') \right] = \delta(z-z')\delta(t-t').
\end{equation}
The Gaussian process $\{\dot{W}(A)\}_{A \in \mathscr B(\mathbb R^n)}$ with $E(\dot{W}(A))=0$ and $E(\dot{W}(A)\dot{W}(B))=\lambda^n(A\cap B)$ where $\lambda ^n$ is the n-dimensional Lesbegue measure is called White Noise.
We can consider for $A \in \mathscr B(\mathbb R^n)$ that $\dot{W}(A) = \int 1_A dW$ and for $h\in L^2(\mathbb R^n)$ we define $\dot{W}(h) = \int h(t)dW(t)$ which is the standard Wiener Integral.
For spacetime we consider the white noise $\dot{W}(A)$ over $A\in [0,T]\times \mathbb{R}$.
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