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通过局域态和扩展态求解非平衡带电粒子输运的广义玻尔兹曼方程。

Solution of a generalized Boltzmann's equation for nonequilibrium charged-particle transport via localized and delocalized states.

机构信息

College of Science, Technology and Engineering, James Cook University, Townsville, QLD 4811, Australia.

出版信息

Phys Rev E. 2016 Mar;93(3):032119. doi: 10.1103/PhysRevE.93.032119. Epub 2016 Mar 11.

Abstract

We present a general phase-space kinetic model for charged-particle transport through combined localized and delocalized states, capable of describing scattering collisions, trapping, detrapping, and losses. The model is described by a generalized Boltzmann equation, for which an analytical solution is found in Fourier-Laplace space. The velocity of the center of mass and the diffusivity about it are determined analytically, together with the flux transport coefficients. Transient negative values of the free particle center-of-mass transport coefficients can be observed due to the trapping to, and detrapping from, localized states. A Chapman-Enskog-type perturbative solution technique is applied, confirming the analytical results and highlighting the emergence of a density gradient representation in the weak-gradient hydrodynamic regime. A generalized diffusion equation with a unique global time operator is shown to arise, reducing to the standard diffusion equation and a Caputo fractional diffusion equation in the normal and dispersive limits. A subordination transformation is used to solve the generalized diffusion equation by mapping from the solution of a corresponding standard diffusion equation.

摘要

我们提出了一种用于描述散射碰撞、俘获、退俘获和损耗的通过组合局域态和离域态的带电粒子输运的广义相空间动力学模型。该模型由广义 Boltzmann 方程描述,在 Fourier-Laplace 空间中找到了其解析解。解析地确定了质心的速度及其扩散系数,以及通量输运系数。由于从局域态的俘获和退俘获,可以观察到自由粒子质心输运系数的瞬时负值。应用Chapman-Enskog 型微扰求解技术,证实了分析结果,并强调了在弱梯度流体力学区域中出现的密度梯度表示。显示出一个具有唯一全局时间算子的广义扩散方程的出现,它在正常和弥散极限下简化为标准扩散方程和 Caputo 分数阶扩散方程。通过从相应的标准扩散方程的解进行映射,使用从属变换来求解广义扩散方程。

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