2014
DOI: 10.1063/1.4901033
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Instabilities of collisionless current sheets revisited: The role of anisotropic heating

Abstract: In this work, we investigate the influence of the anisotropic heating on the spontaneous instability and evolution of thin Harris-type collisionless current sheets, embedded in antiparallel magnetic fields. In particular, we explore the influence of the macroparticle shape-function using a 2D version of the PIC code ACRONYM. We also investigate the role of the numerical collisionality due to the finite number of macroparticles in PIC codes. It is shown that it is appropriate to choose higher order shape functi… Show more

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Cited by 11 publications
(11 citation statements)
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“…The heating is along y, which will be considered the parallel direction in the following (and x or z, the perpendicular, colder directions). The Weibel instability has already been observed in antiparallel magnetic reconnection in previous investigations using similar parameters and geometry [78][79][80] . It has also been more frequently detected in relativistic pair plasmas, because in them the space available for its growth inside the CS is larger (see Ref.…”
Section: Acknowledgmentssupporting
confidence: 69%
See 1 more Smart Citation
“…The heating is along y, which will be considered the parallel direction in the following (and x or z, the perpendicular, colder directions). The Weibel instability has already been observed in antiparallel magnetic reconnection in previous investigations using similar parameters and geometry [78][79][80] . It has also been more frequently detected in relativistic pair plasmas, because in them the space available for its growth inside the CS is larger (see Ref.…”
Section: Acknowledgmentssupporting
confidence: 69%
“…The latter is, perhaps, due to the anisotropic heating of the background plasma population, different from the current carriers. Note that low resolution PiC simulations, with low order shape functions, without current smoothing, too small number of particle per cells or not resolving well enough the smallest electron length scales might not display accurately the structure of the off-diagonal terms of the electron pressure or electron inertia, due to the enhanced effective collisionality or numerical heating effects 80,96 .…”
Section: Acknowledgmentsmentioning
confidence: 99%
“…[ and other ones, useful under some specific conditions. By default, we use the second order shape function TSC to reduce the intrinsic PiC shot noise and the associated numerical heating without affecting the computational performance too much [52,53,41]. Once the sources of the electromagnetic fields in Eqs.…”
Section: Particle Mover (Pic Part)mentioning
confidence: 99%
“…We employ on average 64 particles per cell per species. The charge distribution of each finite-size particle is represented by third-order cubic splines [79], which improve energy conservation and reduce the relative amount of particle noise compared to lower-order splines [80,81]. At each step, we also apply a second-order compensated binomial filter [79] on the electric current and on the electromagnetic fields felt by the particles.…”
mentioning
confidence: 99%