2019
DOI: 10.1002/ctpp.201900117
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Collisional gyrokinetic full‐f particle‐in‐cell simulations on open field lines with PICLS

Abstract: Applying gyrokinetic simulations for theoretical turbulence and transport studies to the plasma edge and scrape-off layer (SOL) presents significant challenges. To in particular account for steep density and temperature gradients in the SOL, the "full-f" code PICLS was developed. PICLS is a gyrokinetic particle-in-cell (PIC) code and is based on an electrostatic model with a linearized field equation and uses kinetic electrons. In previously published results we were applying PICLS to the well-studied 1D paral… Show more

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Cited by 4 publications
(2 citation statements)
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“…To determine the exact source of these contributions, future work must use a large number of particles while keeping the 3D geometry. In addition, the inclusion of a controllable collision operator would allow for a detailed study of collisions in 3D reconnection (Pezzi 2017;Donnel et al 2019;Boesl et al 2020;Pezzi et al 2021).…”
Section: Discussionmentioning
confidence: 99%
“…To determine the exact source of these contributions, future work must use a large number of particles while keeping the 3D geometry. In addition, the inclusion of a controllable collision operator would allow for a detailed study of collisions in 3D reconnection (Pezzi 2017;Donnel et al 2019;Boesl et al 2020;Pezzi et al 2021).…”
Section: Discussionmentioning
confidence: 99%
“…This type of collision operator has been implemented in various gyrokinetic codes, earliest as a Fourier‐space version in GKV [ 7 ] and later in other codes such as GYSELA [ 8 ] , PICLS [ 9 ] , and COGENT [ 10 ] . Recently another implementation in the code GKEYLL [ 11,12 ] has been published, with a discretization based on a discontinuous Galerkin (DG) scheme.…”
Section: Introductionmentioning
confidence: 99%