2015
DOI: 10.4208/cicp.070214.160115a
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Long Time Behaviour of an Exponential Integrator for a Vlasov-Poisson System with Strong Magnetic Field

Abstract: With the aim of solving in a four dimensional phase space a multi-scale VlasovPoisson system, we propose in a Particle-In-Cell framework a robust time-stepping method that works uniformly when the small parameter vanishes. As an exponential integrator, the scheme is able to use large time steps with respect to the typical size of the solution's fast oscillations. In addition, we show numerically that the method has accurate long time behaviour and that it is asymptotic preserving with respect to the limiting G… Show more

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Cited by 53 publications
(50 citation statements)
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“…In future work, we intend to implement the time stepping scheme introduced in [8]. This method allows to solve multiscale Vlasov-Poisson models by treating the stiff terms as an exponential integrator.…”
Section: Discussionmentioning
confidence: 99%
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“…In future work, we intend to implement the time stepping scheme introduced in [8]. This method allows to solve multiscale Vlasov-Poisson models by treating the stiff terms as an exponential integrator.…”
Section: Discussionmentioning
confidence: 99%
“…In this regard we deal with issues like optimized data structures, streamlined memory access and parallelization. In addition, we notice that, with the further aim to improve the recent time scheme in [8] and to extend it to more general problems than the aforementioned multiscale model, we need to have at our disposal a fast code yielding the reference solution. In the following, we understand by reference solution of a model its numerical solution calculated with classical numerical schemes and small enough numerical parameters.…”
Section: Introductionmentioning
confidence: 99%
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“…In this work, we consider the long-time Vlasov-Poisson equation with a strong external homogeneous magnetic field in four phase space dimensions as [19,18]. The distribution function f ε (t, x, v) depending on time t ≥ 0, on space x = (x 1 , x 2 )…”
Section: Introductionmentioning
confidence: 99%
“…Such system can already describe some physics; as an example, it can be seen as a limit of a Vlasov-Poisson system (see e.g. [6] and [9,13,20] for the numerics). As emphasized in [12], it is a building block for future drift kinetic simulations.…”
Section: Introductionmentioning
confidence: 99%