arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 2203.04868cond-mat.stat-mech
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阈值表面反应和本地时间重置

Threshold surface reactions and local time resetting

Paul C. Bressloff

摘要:

在本文中,我们考虑了一个阈值表面吸收机制的粒子扩散域包含一个单一的目标$\calU $。目标边界$\partial \calU$被认为是反应性表面,当在时间$t$与表面接触时,该反应性表面用$Z_0=h$改变颗粒的内部状态$Z_t$。状态$Z_t$被认为是所谓的边界局部时间的单调递减函数,并且一旦$Z_t$达到零就发生吸收。(The边界局部时间是布朗泛函,其确定粒子在$\partial \calU$的邻域中花费的时间量。)我们首先展示了如何分析阈值表面吸收的联合概率密度或广义传播子$P_0(\x,\ell,t|\x_0)$的情况下,一个完美的反射表面,其中$\X_t$和$\ell_t$分别表示粒子的位置和当地时间在时间$t$,和$\x_0$是初始位置的对$(\X_t,\ell_t)$。然后,我们介绍了一个广义的随机重置协议,其中的位置$\X_t$和内部状态$Z_t$重置到它们的初始值,$\X_t\rightarrow \x_0$和$Z_t\rightarrow h$,在泊松率$r$。后者在数学上等同于重置边界本地时间$\ell_t\rightarrow 0$。由于重置受更新过程控制,因此重置的存活概率可以用未重置的存活概率表示,这意味着吸收的统计可以通过计算$P_0(\x,\ell,t|\x_0)$相对于$t$的拉普拉斯变换来确定。我们将此与仅粒子位置被重置的情况进行对比,这不受更新过程的影响。我们说明了理论使用简单的例子,半线上的扩散和一个球形目标在一个球形域。

英文摘要:

In this paper we consider a threshold surface absorption mechanism for a particle diffusing in a domain containing a single target $\calU $. The target boundary $\partial \calU$ is taken to be a reactive surface that modifies an internal state $Z_t$ of the particle when in contact with the surface at time $t$, with $Z_0=h$. The state $Z_t$ is taken to be a monotonically decreasing function of the so-called boundary local time, and absorption occurs as soon as $Z_t$ reaches zero. (The boundary local time is a Brownian functional that determines the amount of time that the particle spends in a neighborhood of $\partial \calU$.) We first show how to analyze threshold surface absorption in terms of the joint probability density or generalized propagator $P_0(\x,\ell,t|\x_0)$ for the pair $(\X_t,\ell_t)$ in the case of a perfectly reflecting surface, where $\X_t$ and $\ell_t$ denote the particle position and local time at time $t$, respectively, and $\x_0$ is the initial position. We then introduce a generalized stochastic resetting protocol in which both the position $\X_t$ and the internal state $Z_t$ are reset to their initial values, $\X_t\rightarrow \x_0$ and $Z_t\rightarrow h$, at a Poisson rate $r$. The latter is mathematically equivalent to resetting the boundary local time, $\ell_t\rightarrow 0$. Since resetting is governed by a renewal process, the survival probability with resetting can be expressed in terms of the survival probability without resetting, which means that the statistics of absorption can be determined by calculating the Laplace transform of $P_0(\x,\ell,t|\x_0)$ with respect to $t$. We contrast this with the case where only particle position is reset, which is not governed by a renewal process. We illustrate the theory using the simple examples of diffusion on the half-line and a spherical target in a spherical domain.

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