Arbitrary-order time-accurate semi-Lagrangian spectral approximations of the Vlasov–Poisson system
The Vlasov–Poisson system, modeling the evolution of non-collisional plasmas in the electrostatic limit, is approximated by a semi-Lagrangian technique. Spectral methods of periodic type are implemented through a collocation approach. Groups of particles are represented by the Fourier Lagrangian bas...
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Veröffentlicht in: | Journal of computational physics 2019-05, Vol.384 (C), p.349-375 |
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Sprache: | eng |
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Zusammenfassung: | The Vlasov–Poisson system, modeling the evolution of non-collisional plasmas in the electrostatic limit, is approximated by a semi-Lagrangian technique. Spectral methods of periodic type are implemented through a collocation approach. Groups of particles are represented by the Fourier Lagrangian basis and evolve, for a single timestep, along a high-order accurate representation of the local characteristic lines. The time-advancing technique is based on truncated Taylor series that can be, in principle, of any order of accuracy. A variant is obtained by coupling the phase space discretization with high-order accurate Backward Differentiation Formulas (BDF). At each timestep, particle displacements are reinterpolated and expressed in the original basis to guarantee the order of accuracy in all the variables at relatively low costs. Thus, these techniques combine the excellent features of spectral approximations with high-order time integration. The resulting method has excellent conservation properties. Indeed, it can be proven that the total number of particles, proportional to the total mass and charge, is conserved up to the machine precision. Series of numerical experiments are performed in order to assess the real performance. In particular, comparisons with standard benchmarks are examined.
•The Vlasov-Poisson system is approximated by unsplit high-order semi-Lagrangian methods.•Spectral Fourier collocation is implemented in the phase-space domain.•The Backward Differentiation Formula provides second and third order time schemes.•Perfect mass conservation is fulfilled.•Tests on standard benchmarks assess the performance of the methods. |
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ISSN: | 0021-9991 1090-2716 |
DOI: | 10.1016/j.jcp.2019.01.020 |