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首页> 外文期刊>The Astrophysical journal >DETAILED NUMERICAL INVESTIGATION OF THE BOHM LIMIT IN COSMIC RAY DIFFUSION THEORY
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DETAILED NUMERICAL INVESTIGATION OF THE BOHM LIMIT IN COSMIC RAY DIFFUSION THEORY

机译:宇宙射线扩散理论中波姆极限的详细数值研究

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A standard model in cosmic ray diffusion theory is the so-called Bohm limit in which the particle mean free path is assumed to be equal to the Larmor radius. This type of diffusion is often employed to model the propagation and acceleration of energetic particles. However, recent analytical and numerical work has shown that standard Bohm diffusion is not realistic. In the present paper, we perform test-particle simulations to explore particle diffusion in the strong turbulence limit in which the wave field is much stronger than the mean magnetic field. We show that there is indeed a lower limit of the particle mean free path along the mean field. In this limit, the mean free path is directly proportional to the unperturbed Larmor radius like in the traditional Bohm limit, but it is reduced by the factor δB/B 0 where B 0 is the mean field and δB the turbulent field. Although we focus on parallel diffusion, we also explore diffusion across the mean field in the strong turbulence limit.
机译:宇宙射线扩散理论中的标准模型是所谓的Bohm极限,其中假定粒子平均自由程等于拉莫尔半径。这种类型的扩散通常用于模拟高能粒子的传播和加速。但是,最近的分析和数值研究表明标准的波姆扩散是不现实的。在本文中,我们执行测试粒子模拟以探索在强湍流极限中的粒子扩散,在强湍流极限中,波场比平均磁场要强得多。我们表明,沿平均场确实存在粒子平均自由程的下限。在此极限中,与传统的Bohm极限一样,平均自由程与不受扰动的拉莫尔半径成正比,但减小了因子δB/ B 0,其中B 0是平均场,而δB是湍流场。尽管我们专注于平行扩散,但我们还在强湍流极限中探索了整个平均场的扩散。

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