activity
20242026
collaborators

7 papers

math.NA2026

A HDG method with transmission variables for time-harmonic wave propagation problems with constant coefficients

Simone Pescuma, Gwénaël Gabard, Théophile Chaumont-Frelet +1

Iterative finite element solvers for time-harmonic wave problems are notoriously slow to converge, owing to fundamental properties of these problems. We present a variant of the hy…

math.NA2025

A posteriori error estimates and space-adaptive mesh refinements for time-dependent scattering problems

Théophile Chaumont-Frelet, Heiko Gimperlein, Ignacio Labarca-Figueroa +1

This work studies a posteriori error estimates and their use for time-dependent acoustic scattering problems, formulated as a time-dependent boundary integral equation based on a s…

math.NA2025

Adaptive boundary element methods for regularized combined field integral equations

Théophile Chaumont-Frelet, Gregor Gantner

While the exterior Helmholtz problem with Dirichlet boundary conditions is always well-posed, the associated standard boundary integral equations are not if the squared wavenumber…

math.NA2025

A quasi-interpolation operator yielding fully computable error bounds

T. Chaumont-Frelet, M. Vohralik

We design a quasi-interpolation operator from the Sobolev space to its finite-dimensional finite element subspace formed by piecewise polynomials on a simplicial mesh w…

math.NA2025

A posteriori error estimates for the finite element discretization of second-order PDEs set in unbounded domains

T. Chaumont-Frelet

We consider second-order PDE problems set in unbounded domains and discretized by Lagrange finite elements on a finite mesh, thus introducing an artificial boundary in the discreti…

math.NA2024

Damped energy-norm a posteriori error estimates for fully discrete approximations of the wave equation using C2-reconstructions with the leapfrog scheme

T. Chaumont-Frelet, A. Ern

We derive a posteriori error estimates for the the scalar wave equation discretized in space by continuous finite elements and in time by the explicit leapfrog scheme. Our analysis…