Explicit integrators for the magnetized equations of motion in Particle in Cell codes
A new explicit time-reversible orbit integrator for the equations of motion in a static homogeneous magnetic field - called Cyclotronic integrator - is presented. Like Spreiter and Walter's Taylor expansion algorithm, for sufficiently weak electric field gradients this second order method does...
Main Authors: | , |
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Other Authors: | , |
Format: | Article |
Language: | English |
Published: |
Academic Press,
2010-09-28T12:46:50Z.
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Subjects: | |
Online Access: | Get fulltext |
Summary: | A new explicit time-reversible orbit integrator for the equations of motion in a static homogeneous magnetic field - called Cyclotronic integrator - is presented. Like Spreiter and Walter's Taylor expansion algorithm, for sufficiently weak electric field gradients this second order method does not require a fine resolution of the Larmor motion; it has however the essential advantage of being symplectic, hence time-reversible. The Cyclotronic integrator is only subject to a linear stability constraint ([OmegaDelta t] < pi, [Omega] being the Larmor angular frequency), and is therefore particularly suitable to electrostatic Particle In Cell codes with uniform magnetic field where [Omega]is larger than any other characteristic frequency, yet a resolution of the particles' gyromotion is required. Application examples and a detailed comparison with the well-known (time-reversible) Boris algorithm are presented; it is in particular shown that implementation of the Cyclotronic integrator in the kinetic codes SCEPTIC and Democritus can reduce the cost of orbit integration by up to a factor of ten. National Science Foundation (U.S.) and United States. Dept. of Energy (DE-FG02- 06ER54891) United States. Dept. of Energy (DE-FC02-99ER54512) |
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