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首页> 外文期刊>Plasma Sources Science & Technology >Bistable solutions for the electron energy distribution function in electron swarms in xenon: a comparison between the results of first-principles particle simulations and conventional Boltzmann equation analysis
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Bistable solutions for the electron energy distribution function in electron swarms in xenon: a comparison between the results of first-principles particle simulations and conventional Boltzmann equation analysis

机译:氙电子群中电子能量分布函数的双稳态解:第一性原理粒子模拟结果与常规玻耳兹曼方程分析的比较

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摘要

At low reduced electric fields the electron energy distribution function in heavy noble gases can take two distinct shapes. This 'bistability effect'-in which electron-electron (Coulomb) collisions play an essential role-is analyzed here for Xe with a Boltzmann equation approach and with a first principles particle simulation method. The solution of the Boltzmann equation adopts the usual approximations of (i) searching for the distribution function in the form of two terms ('two-term approximation'), (ii) neglecting the Coulomb part of the collision integral for the anisotropic part of the distribution function, (iii) treating Coulomb collisions as binary events, and (iv) truncating the range of the electron-electron interaction beyond a characteristic distance. The particle-based simulation method avoids these approximations: the many-body interactions within the electron gas with a true (un-truncated) Coulomb potential are described by a molecular dynamics algorithm, while the collisions between electrons and the background gas atoms are treated with Monte Carlo simulation. We find a good general agreement between the results of the two techniques, which confirms, to a certain extent, the approximations used in the solution of the Boltzmann equation. The differences observed between the results are believed to originate from these approximations and from the presence of statistical noise in the particle simulations.
机译:在低还原电场下,重的稀有气体中的电子能量分布函数可以采取两种不同的形状。本文使用玻尔兹曼方程方法和第一原理粒子模拟方法针对Xe分析了这种“双稳态效应”,其中电子-电子(库仑)碰撞起着至关重要的作用。 Boltzmann方程的解采用以下常用近似方法:(i)以两个项的形式搜索分布函数(“两项近似”);(ii)忽略碰撞积分的库仑部分作为各向异性部分。分布函数;(iii)将库仑碰撞视为二元事件;(iv)将电子-电子相互作用的范围截断超过特征距离。基于粒子的模拟方法避免了这些近似方法:利用分子动力学算法描述了电子气中具有真实(未截断)库仑电势的多体相互作用,而电子与背景气体原子之间的碰撞则用蒙特卡洛模拟。我们在这两种技术的结果之间找到了良好的一般一致性,这在一定程度上确认了玻耳兹曼方程解中使用的近似值。据信,结果之间观察到的差异源自这些近似​​值以及粒子模拟中存在统计噪声。

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