A two-step Monte Carlo algorithm for interaction between resonant ions and radio frequency waves

T. Johnson , L.-G. Eriksson
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Abstract

This paper presents a new Monte Carlo algorithm intended for use in orbit following Monte Carlo codes (OFMC) to describe resonant interaction of ions with Radio Frequency (RF) waves in axi-symmetric toroidal plasmas. The algorithm is based on a quasi-linear description of the wave–particle interaction and its effect on the distribution function of a resonating ion species. The algorithm outlined in the present paper utilises a two-step approach for the evaluation of the Monte Carlo operator that has better efficiency and a stronger convergence than the standard Euler–Maruyama scheme. The algorithm preserves the reciprocity of the diffusion process. Furthermore, it simplifies how the displacement of the resonance position, as a result of wave–particle interaction, is accounted for. Such displacements can have a noticeable effect on the deterministic part of the Monte Carlo operator. The fundamental nature of guiding centre displacements of resonant ions as a result of wave–particle interaction is reviewed.

共振离子与射频波相互作用的两步蒙特卡洛算法
本文提出了一种新的蒙特卡罗算法,用于轨道跟踪蒙特卡罗代码(OFMC),以描述轴对称环形等离子体中离子与射频(RF)波的共振相互作用。该算法基于对波-粒子相互作用的准线性描述及其对共振离子种类分布函数的影响。本文概述的算法采用两步法评估蒙特卡罗算子,与标准的欧拉-马鲁山方案相比,效率更高,收敛性更强。该算法保留了扩散过程的互易性。此外,它还简化了共振位置位移的计算方法,这是波粒相互作用的结果。这种位移会对蒙特卡罗算子的确定性部分产生明显影响。本文回顾了共振离子的导引中心位移是波粒相互作用的结果这一基本性质。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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