2018
DOI: 10.1016/j.jcp.2018.09.007
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Numerical methods for the two-dimensional Vlasov–Poisson equation in the finite Larmor radius approximation regime

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Cited by 14 publications
(4 citation statements)
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“…The presence of a slow time scale and a fast one which is 2π-periodic is amenable to the two-scale framework [5][6][7][8][9]14,15]. Then, we consider the two time scales as independent by introducing Z p (t, s) (resp.…”
Section: Multiscale Numerical Schemesmentioning
confidence: 99%
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“…The presence of a slow time scale and a fast one which is 2π-periodic is amenable to the two-scale framework [5][6][7][8][9]14,15]. Then, we consider the two time scales as independent by introducing Z p (t, s) (resp.…”
Section: Multiscale Numerical Schemesmentioning
confidence: 99%
“…since Ûn 0 = Ûn 0 when ε = 0 (indeed, ⟨Q BGK ⟩ conserves gyromoments). This scheme is a consistent explicit first order time discretization of the gyrokinetic equation (8).…”
Section: Ap Properties Of Scheme B For the Gyrofluid Limitmentioning
confidence: 99%
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“…In the design of well-adapted numerical schemes to capture the slow part of the dynamics with a rather coarse discretization (compared to the fast scales), one could mention the two-scale convergence method [18,19], the micro-macro decomposition in [6], lifting with multiple time variables [8,9,10,4], exponential integrators [16,17], frequency filtering [21], and implicit-explicit time discretizations [12,13,36]. The reader is also referred to [5,7] for some numerical comparisons, including comparisons with more standard methods.…”
mentioning
confidence: 99%