Bernstein-von Mises theorems for time evolution equations
Richard Nickl
TL;DR
The paper addresses statistical inference for initial conditions of infinite-dimensional time-evolution PDEs under discrete noisy observations. It develops a functional Bernstein–von Mises theory showing that, under a set of regularity and identifiability conditions, the non-Gaussian posterior over trajectories is well-approximated by a Gaussian measure in a negative Sobolev space, with convergence quantified in Wasserstein distance at rate $1/\sqrt{N}$. The Gaussian limit is constructed from a time-dependent Schrödinger equation with a rough Gaussian initial condition and is characterized via the inverse Fisher information operator, providing both posterior uncertainty quantification and practical computational implications. The analysis is instantiated for periodic non-linear reaction-diffusion equations, with detailed PDE results on existence, regularity, forward maps, linearisation, spectral properties, and the information operator, collectively enabling rigorous frequentist Bayesian guarantees for high-dimensional Bayesian data assimilation. These results offer a rigorous pathway to reliable uncertainty quantification and efficient computation in complex dynamical systems governed by parabolic PDEs.
Abstract
We consider a class of infinite-dimensional dynamical systems driven by non-linear parabolic partial differential equations with initial condition $θ$ modelled by a Gaussian process `prior' probability measure. Given discrete samples of the state of the system evolving in space-time, one obtains updated `posterior' measures on a function space containing all possible trajectories. We give a general set of conditions under which these non-Gaussian posterior distributions are approximated, in Wasserstein distance for the supremum-norm metric, by the law of a Gaussian random function. We demonstrate the applicability of our results to periodic non-linear reaction diffusion equations \begin{align*} \frac{\partial}{\partial t} u - Δu &= f(u) \\ u(0) &= θ\end{align*} where $f$ is any smooth and compactly supported reaction function. In this case the limiting Gaussian measure can be characterised as the solution of a time-dependent Schrödinger equation with `rough' Gaussian initial conditions whose covariance operator we describe.
