准平稳分布和弹性:从样本中得到什么?

J. Chazottes, P. Collet, S. Martínez, S. Méléard
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引用次数: 2

摘要

我们研究了一类几乎必然走向灭绝的多物种生灭过程,并承认其唯一的准平稳分布(简称qsd)。当以$K$和极限$K\to+\infty$进行缩放时,在任何固定的有限时间窗口中,这些过程的实现都接近于一个动力系统的轨迹,该系统的矢量场由出生率和死亡率定义。假设这个动力有一个独特的吸引不动点,我们在之前的工作中分析了大而有限$K$会发生什么,特别是不同的时间尺度出现。在目前的工作中,我们主要关注以下问题:观察一个实现过程,我们能否确定所谓的工程弹性?为了回答这个问题,我们建立了两种关系,将弹性(为动力系统定义的宏观量)和过程波动(为微观量)混合在一起。类似的关系在非平衡态统计力学中是众所周知的。为了利用这些关系,我们需要引入几个估计器,我们控制$\log K$(收敛到qsd的时间尺度)和$\exp(K)$(平均时间到消亡的时间尺度)之间的时间。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Quasi-stationary distributions and resilience: what to get from a sample?
We study a class of multi-species birth-and-death processes going almost surely to extinction and admitting a unique quasi-stationary distribution (qsd for short). When rescaled by $K$ and in the limit $K\to+\infty$, the realizations of such processes get close, in any fixed finite-time window, to the trajectories of a dynamical system whose vector field is defined by the birth and death rates. Assuming that this dynamical has a unique attracting fixed point, we analyzed in a previous work what happens for large but finite $K$, especially the different time scales showing up. In the present work, we are mainly interested in the following question: Observing a realization of the process, can we determine the so-called engineering resilience? To answer this question, we establish two relations which intermingle the resilience, which is a macroscopic quantity defined for the dynamical system, and the fluctuations of the process, which are microscopic quantities. Analogous relations are well known in nonequilibrium statistical mechanics. To exploit these relations, we need to introduce several estimators which we control for times between $\log K$ (time scale to converge to the qsd) and $\exp(K)$ (time scale of mean time to extinction).
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