Jump-preserving polynomial interpolation in non-manifold polyhedra
Martin Averseng
TL;DR
The paper tackles the challenge of discretizing PDEs on domains with a non-manifold crack or screen $\Gamma$ by constructing a jump-preserving, piecewise-polynomial interpolant $\Pi_h$ mapping $H^1(\Omega\setminus\Gamma)$ into a finite element space $V^p(\Omega_h;\Gamma)$. It introduces a robust, jump-aware interpolation framework that is idempotent ($$Π_h^2=Π_h$$), preserves homogeneous boundary data and the jumps across $\Gamma$, and provides both local and global Sobolev stability/approximation estimates in $H^t$ and $H^s$ spaces. A key methodological advance is the extension of Scott--Zhang style interpolation to non-manifold hypersurfaces via a multi-sides/bridges construction, including primal/dual bases and bridge functions, to manage multiple approach directions at a node. The framework yields a bounded discrete right-inverse to the jump operator and enables Galerkin error analysis for elliptic PDEs with prescribed jumps on $\Gamma$, with convergence $\|u-u_h\|_{H^1(\Omega\setminus\Gamma)} \lesssim h^{l-1}|u|_{H^l(\Omega\setminus\Gamma)}$ for $1\le l\le p+1$. Overall, the results significantly advance stable discretization techniques for non-manifold fracture-like geometries and thin obstacles in boundary-element and finite-element contexts.
Abstract
We construct a piecewise-polynomial interpolant $u \mapsto Πu$ for functions $u:Ω\setminus Γ\to \mathbb{R}$, where $Ω\subset \mathbb{R}^d$ is a Lipschitz polyhedron and $Γ\subset Ω$ is a possibly non-manifold $(d-1)$-dimensional hypersurface. This interpolant enjoys approximation properties in relevant Sobolev norms, as well as a set of additional algebraic properties, namely, $Π^2 = Π$, and $Π$ preserves homogeneous boundary values and jumps of its argument on $Γ$. As an application, we obtain a bounded discrete right-inverse of the "jump" operator across $Γ$, and an error estimate for a Galerkin scheme to solve a second-order elliptic PDE in $Ω$ with a prescribed jump across $Γ$.
