2020
DOI: 10.1007/978-3-030-56750-7_11
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A Parallel Solver for a Preconditioned Space-Time Boundary Element Method for the Heat Equation

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Cited by 2 publications
(7 citation statements)
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“…We have described details of the applied Galerkin methods in Section 3. In addition we use the matrix V 11 h as the essential part of an operator preconditioner for D h [25,26,7], where V 11 h is the realisation of the single-layer operator for functions piecewise linear and globally continuous in space. We check the convergence of the approximations u h and w h corresponding to u and w to the known Cauchy data on a sequence of uniformly refined meshes Σ h .…”
Section: Convergencementioning
confidence: 99%
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“…We have described details of the applied Galerkin methods in Section 3. In addition we use the matrix V 11 h as the essential part of an operator preconditioner for D h [25,26,7], where V 11 h is the realisation of the single-layer operator for functions piecewise linear and globally continuous in space. We check the convergence of the approximations u h and w h corresponding to u and w to the known Cauchy data on a sequence of uniformly refined meshes Σ h .…”
Section: Convergencementioning
confidence: 99%
“…We aim to provide a complete and (hopefully) error-free presentation of details on the implementation of a Galerkin boundary element method for the three-dimensional heat equation considering all boundary integral operators. Galerkin methods have been considered in, e.g., [2,3,6,7] for 2d and [8,9,10] for 3d. Typically, implementational aspects are discussed only briefly and a lot of effort is necessary to transform the theoretical results into a performant computer code.…”
Section: Introductionmentioning
confidence: 99%
“…precluding point singularities admitted in the present work. The work [12] focuses again on space-time discretization of the heat equation, and addresses the solver complexity. A space-time DG discretization for the parabolic Navier-Stokes equation was proposed in [41].…”
Section: Previous Resultsmentioning
confidence: 99%
“…where P p (F x ) denotes the space of polynomials of degree at most p ∈ N 0 on F x , and the constants C 2|1 , C ∞|2 depend on p. The inequalities in (11) are obvious, while the inverse inequalities in (12) follow from the equivalence of norms in finite dimensional spaces and scaling; note that C ∞|2 ≥ 1. The constants in (12) depend linearly on the polynomial degree. Denote by P p the Legendre polynomials and by…”
Section: Inverse Inequalitiesmentioning
confidence: 99%
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