On the numerical dispersion of electromagnetic particle-in-cell code: Finite grid instability

JOURNAL OF COMPUTATIONAL PHYSICS

卷:297

Article

Meyers, M. D.^1,2  Huang, C. -K.¹  Zeng, Y.¹  Yi, S. A.¹  Albright, B. J.¹ 

[1] Los Alamos Natl Lab, Los Alamos, NM 87545 USA

[2] Univ Calif Los Angeles, Dept Phys & Astron, Los Angeles, CA 90095 USA

关键词: Particle-in-cell;    Plasma simulation;    Relativistic plasma drift;    Numerical dispersion relation;    Numerical instability;    Finite grid instability;   

DOI  :  10.1016/j.jcp.2015.05.037

来源: Elsevier

【 摘 要 】

The Particle-In-Cell (PIC) method is widely used in relativistic particle beam and laser plasma modeling. However, the PIC method exhibits numerical instabilities that can render unphysical simulation results or even destroy the simulation. For electromagnetic relativistic beam and plasma modeling, the most relevant numerical instabilities are the finite grid instability and the numerical Cherenkov instability. We review the numerical dispersion relation of the Electromagnetic PIC model. We rigorously derive the faithful 3-D numerical dispersion relation of the PIC model, for a simple, direct current deposition scheme, which does not conserve electric charge exactly. We then specialize to the Yee FDTD scheme. In particular, we clarify the presence of alias modes in an eigenmode analysis of the PIC model, which combines both discrete and continuous variables. The manner in which the PIC model updates and samples the fields and distribution function, together with the temporal and spatial phase factors from solving Maxwell's equations on the Yee grid with the leapfrog scheme, is explicitly accounted for. Numerical solutions to the electrostatic-like modes in the 1-D dispersion relation for a cold drifting plasma are obtained for parameters of interest. In the succeeding analysis, we investigate how the finite grid instability arises from the interaction of the numerical modes admitted in the system and their aliases. The most significant interaction is due critically to the correct representation of the operators in the dispersion relation. We obtain a simple analytic expression for the peak growth rate due to this interaction, which is then verified by simulation. We demonstrate that our analysis is readily extendable to charge conserving models. Published by Elsevier Inc.

【 授权许可】

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