Nonlocal Boundary Value Problems Governed by Symmetric Nonlocal Operators
Leonhard Frerick, Julia Huschens, Michael Vu
TL;DR
The paper develops a comprehensive variational theory for nonlocal boundary value problems driven by symmetric transition kernels, extending beyond the standard diffusion kernel to a general operator $\mathcal{L}u = \mathrm{PV} \int_{\mathbb{R}^d} (u(x)-u(y)) \, K(x,\mathrm{d}y)$. It introduces a notion of $\lambda$-symmetry that enables a nonlocal integration-by-parts identity, and constructs nonlocal function spaces $V$ and $V_0$ with a bilinear form $\mathcal{B}$ to formulate weak solutions for Dirichlet and Neumann problems. Central to the analysis are nonlocal Friedrichs and Poincaré-type inequalities, which ensure well-posedness via the Lax–Milgram theorem and provide stability and uniqueness up to the natural kernel. The theory is illustrated by connecting to the discrete Poisson problem through stencil operators, yielding matrix formulations and a discrete maximum principle that align with the continuous nonlocal framework. This work broadens the scope of nonlocal models and offers a rigorous foundation for both analysis and discretization of nonlocal boundary value problems.
Abstract
Nonlocal boundary value problems with Dirichlet or Neumann boundary are well-studied for nonlocal operators of the type $\mathcal{L}_γu = \operatorname{PV} \int_{\mathbb{R}^d} \big(u(\cdot)-u(y)\big) γ(\cdot,y) \, \mathrm{d}y$ where the underlying kernel function $γ: \mathbb{R}^d \times \mathbb{R}^d \rightarrow [0,\infty)$ is assumed to be measurable and symmetric. In this paper, a theory is introduced for problems whose governing operator is of the more general type \[\mathcal{L}u:= \operatorname{PV} \int_{\mathbb{R}^d}\big(u(\cdot)-u(y)\big) \, K(\cdot, \mathrm{d}y)\] where ${K: \mathbb{R}^d \times \mathcal{B}(\mathbb{R}^d) \rightarrow [0,\infty]}$ is a symmetric transition kernel. Our main focus is on nonlocal Dirichlet and Neumann problems and a classical Hilbert space approach is developed for solving designated weak formulations. As an example, the discrete Poisson problem on $Ω=(0,1)^d$ is discussed.
