2021
DOI: 10.1051/m2an/2020077
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Error estimation of the Besse Relaxation Scheme for a semilinear heat equation

Abstract: The solution to the initial and Dirichlet boundary value problem for a semilinear, one dimensional heat equation is approximated by a numerical method that combines the Besse Relaxation Scheme in time [C. R. Acad. Sci. Paris S{\'e}r. I, vol. 326 (1998)] with a central finite difference method in space. A new, composite stability argument is developed, leading to an optimal, second-order error estimate in the discrete $L_t^{\infty}(H_x^2)-$norm at the time-nodes and in the discrete $L_t^{\infty}(H_x^1)-$nor… Show more

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Cited by 7 publications
(3 citation statements)
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“…We are not aware of any analytical results concerning the convergence of the fully discrete method for the nonlinear Schrödinger equation, but for the semilinear heat equation an analysis was recently provided in [38].…”
Section: Relaxation Methods (Re-fem)mentioning
confidence: 99%
“…We are not aware of any analytical results concerning the convergence of the fully discrete method for the nonlinear Schrödinger equation, but for the semilinear heat equation an analysis was recently provided in [38].…”
Section: Relaxation Methods (Re-fem)mentioning
confidence: 99%
“…One particularly important aspect is that the analytical equation (1.2) conserves the total energy of the system and it was numerically observed [34] that an analogous discrete energy conservation can be a crucial property of numerical schemes to get reliable approximations in practical situations. Time integrators that conserve a modified energy are for example the popular Besse relaxation scheme [15,16,52] and the family of exponential Runge-Kutta schemes proposed in [26]. Time integrators that conserve the exact energy (up to spatial discretization errors) are more rare and include the Crank-Nicolson method based on the averaging of densities [3,10,32,35,45] and the continuous Galerkin time stepping proposed in [39].…”
Section: Introductionmentioning
confidence: 99%
“…Practically, the discrete conservation of mass and energy is subject to the choice of the time integrator. Among others, mass conservative time discretizations have been studied in [57,61], time integrators that are mass conservative and symplectic are investigated in [3,25,51,54,56], energy conservative time discretizations in [34] and time discretization that preserve mass and energy simultaneously are addressed in [3,7,9,11,12,16,31,33,50,62]. For further discretizations we refer to [5,8,10,36,53] and the references therein.…”
Section: Introductionmentioning
confidence: 99%