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Exact Solutions for Distributions of First-Passage Direct-Transit and Looping Times in Symmetric Cusp Potential Barriers and Wells

机译:对称尖峰势垒和井中首次通过直接通过和循环时间分布的精确解决方案

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摘要

For a particle diffusing in one dimension, the distribution of its first-passage time from point a to point b is determined by the durations of the particle trajectories that start from point a and are terminated as soon as they touch point b for the first time. Any such trajectory consists of looping and direct-transit segments. The latter is the final part of the trajectory that leaves point a and goes to point b without returning to point a. The rest of the trajectory is the looping segment that makes numerous loops which begin and end at the same point a without touching point b. In this article we discuss general relations between the first-passage time distribution and those for the durations of the two segments. These general relations allow us to find exact solutions for the Laplace transforms of the distributions of the first-passage, direct-transit, and looping times for transitions between two points separated by a symmetric cusp potential barrier or well of arbitrary height and depth, respectively. The obtained Laplace transforms are inverted numerically, leading to nontrivial dependences of the resulting distributions on the barrier height and the well depth.
机译:对于在一个维度上扩散的粒子,其第一次通过时间从点a到点b的分布取决于从点a开始并在它们第一次接触点b时终止的粒子轨迹的持续时间。 。任何这样的轨迹都由循环段和直行段组成。后者是轨迹的最后一部分,该轨迹离开点a并到达点b,而没有返回点a。轨迹的其余部分是循环段,该循环段形成许多循环,这些循环在相同点a处开始和结束,而没有接触点b。在本文中,我们讨论了第一次通过时间分布与两个时间段持续时间之间的一般关系。这些一般关系使我们能够找到分别通过对称尖峰势垒或任意高度和深度的井分开的两个点之间的过渡的首次通过,直接通过和循环时间分布的拉普拉斯变换的精确解。对获得的拉普拉斯变换进行数值反演,从而导致所得分布对势垒高度和阱深度的非平凡依赖。

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