2009
DOI: 10.1016/j.jcp.2008.12.021
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Explicit time-reversible orbit integration in Particle In Cell codes with static homogeneous magnetic field

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Cited by 18 publications
(23 citation statements)
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“…We note that all of these substeps are time symmetric, i.e., ϕ T −h = (ϕ T h ) −1 , and so on. We also note that the subflows (12) and (14) . Its determinant is given by det ∂y 1 ∂y 0 = det exp hΩ( q) .…”
Section: Splitting Methodsmentioning
confidence: 81%
“…We note that all of these substeps are time symmetric, i.e., ϕ T −h = (ϕ T h ) −1 , and so on. We also note that the subflows (12) and (14) . Its determinant is given by det ∂y 1 ∂y 0 = det exp hΩ( q) .…”
Section: Splitting Methodsmentioning
confidence: 81%
“…Code operation in this regime is deferred to future work. The n part particles representing ions are advanced in Cartesian coordinates using the Cyclotronic integration scheme [19], in the frame moving with velocity v ⊥ where E conv vanishes. This enables us to use longer time-steps as the strong convective acceleration need not be resolved.…”
Section: Code Operationmentioning
confidence: 99%
“…[15]. A uniform external magnetic field B and a uniform convective electric field E conv drive a background cross-field drift v ⊥ = E conv ×B/B 2 ; hence in Eqs (1,2) Φ is the dust-induced potential perturbation, and E = E conv −∇Φ is the total electric field acting on the ions and electrons.…”
Section: Methods For Force Calculations 21 Sceptic3dmentioning
confidence: 99%