2013
DOI: 10.1137/110851511
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Enhanced Convergence Estimates for Semi-Lagrangian Schemes Application to the Vlasov--Poisson Equation

Abstract: We prove enhanced error estimates for high order semi-lagrangian discretizations of the Vlasov-Poisson equation. It provides new insights into optimal numerical strategies for the numerical solution of this problem. The new error estimate O min ∆x ∆t , 1 ∆x p + ∆t 2 is based on advanced error estimates for semi-lagrangian schemes, also equal to shifted Strang's schemes, for the discretization of the advection equation.

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Cited by 28 publications
(28 citation statements)
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“…-For the coarse mesh, we observe oscillations that increase when the time step get smaller; this is due to the fact that we use cubic spline interpolation which behave bad when the time step becomes small (see [10,24]). …”
Section: Kelvin-helmholtz Instability In a Periodic Box With Colella mentioning
confidence: 97%
“…-For the coarse mesh, we observe oscillations that increase when the time step get smaller; this is due to the fact that we use cubic spline interpolation which behave bad when the time step becomes small (see [10,24]). …”
Section: Kelvin-helmholtz Instability In a Periodic Box With Colella mentioning
confidence: 97%
“…To deal with the one-dimensional advection equations, a semi-Lagrangian method is used (see [9,6,7]). Since the characteristics can be solved exactly in this case (a does not depend on z), the error produced by the scheme comes from the splitting (error in time) and from the interpolation step (error in x and v).…”
Section: Numerical Examplesmentioning
confidence: 99%
“…all the L p norms of f ). Note that in this work, we do not address the delicate question of phase space approximation and focus only on time discretization effects (see [2,6,20]). …”
Section: Introductionmentioning
confidence: 99%
“…when the diagonal part of the tensor ε 0 ω (r) vanishes and the non-diagonal part remains non-zero. As shown in [9,10], for a 1D-counterpart of (3), in this case the time-harmonic electric field componentÊ x is not necessarily square integrable (for a demonstration of this behaviour with the help of a simpler example, namely the Budden problem, see e.g. [10]).…”
Section: Introductionmentioning
confidence: 98%