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Microscopic origin of the jump diffusion model

机译:跳跃扩散模型的微观起源

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The present paper is aimed at studying the microscopic origin of the jump diffusion. Starting fromthe N-body Liouville equation and making only the assumption that molecular reorientation isoverdamped, we derive and solve the new (hereafter generalized diffusion) equation. This is themost general equation which governs orientational relaxation of an equilibrium molecular ensemblein the hindered rotation limit and in the long time limit. The generalized diffusion equation is anextension of the small-angle diffusion equation beyond the impact approximation. We establish theconditions under which the generalized diffusion equation can be identified with the jump diffusionequation, and also discuss the similarities and differences between the two approaches.
机译:本文旨在研究跳跃扩散的微观起源。从N体Liouville方程开始,仅假设分子重新取向被过度阻尼,我们推导并求解了新的(以下称为广义扩散)方程。这是最一般的方程式,用于控制受阻旋转极限和长时间限制的平衡分子整体的取向松弛。广义扩散方程是小角扩散方程超越冲击近似的扩展。我们建立了用跳跃扩散方程识别广义扩散方程的条件,并讨论了这两种方法之间的异同。

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