A probabilistic representation for the gradient in a linear parabolic PDE with Neumann boundary condition
Abdelatif Benchérif Madani
TL;DR
This work develops a probabilistic representation for the gradient of the solution to a linear parabolic PDE with Neumann boundary in a smooth bounded domain by penalizing the reflecting diffusion and differentiating the resulting flow pathwise. By proving tightness of the penalized Jacobian processes in the Jakubowski $S$-topology and identifying limit points via a linear SDE with boundary interactions, the authors obtain a gradient formula: $\\partial_\\nu u(t,x) = \\mathbb{E}[\\nabla f(X^{x}(t)) \\cdot J^{x,\\nu}(t)]$, tying the gradient to the Jacobian along the diffusion flow. A differential-geometric viewpoint is employed, where the gradient is treated as a 1-form and the Weingarten map (shape operator) naturally appears in boundary contributions, leading to an absolute boundary condition framework. The paper also discusses extensions to nonconvex domains via localization, and to curved manifolds, highlighting the potential of this probabilistic approach for gradient computation in PDEs with complex boundaries.
Abstract
We give a probabilistic representation for the gradient of a 2nd order linear parabolic PDE $\partial_{t}u(t,x)=(1/2)a^{ij}\partial_{ij}u(t,x)+b^{i}\partial_{i}u(t,x)$ with Cauchy initial condition $u(0,x)=f(x)$ and Neumann boundary condition in a (closed) convex bounded smooth domain $D$ in $\mathbb{R}^{d}$, $d\geq 1$. The idea is to start from a penalized version of the associated reflecting diffusion $X^{x}$, proceed with a pathwise derivative, show that the resulting family of $ν$-directional Jacobians is tight in the Jakubowski S-topology with limit $J^{x,ν}$, solution of a certain linear SDE, and set $\mathbb{E}\left(\nabla f(X^{x}(t))\cdot J^{x,e_{i}}(t)\right)$ for the gradient $\partial_{i}u(t,x)$, where $x\in D$, $t\geq 0$, $e_{i}$ the canonical basis of $\mathbb{R}^{d}$ and $f$, the initial condition of the semigroup of $X^{x}$, is differentiable. Some more extensions and applications are discussed in the concluding remarks.
