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Emergence of the scale-invariant proportion in a flock from the metric-topological interaction.通过度量拓扑相互作用,鸟群中出现尺度不变比例。
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拓扑最近邻相互作用的动力学模型。

Kinetic Models for Topological Nearest-Neighbor Interactions.

作者信息

Blanchet Adrien, Degond Pierre

机构信息

1IAST/TSE, Université Toulouse Capitole, 21 Allée de Brienne, 31000 Toulouse, France.

2Department of Mathematics, Imperial College London, London, SW7 2AZ UK.

出版信息

J Stat Phys. 2017;169(5):929-950. doi: 10.1007/s10955-017-1882-z. Epub 2017 Oct 20.

DOI:10.1007/s10955-017-1882-z
PMID:32009675
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6959382/
Abstract

We consider systems of agents interacting through topological interactions. These have been shown to play an important part in animal and human behavior. Precisely, the system consists of a finite number of particles characterized by their positions and velocities. At random times a randomly chosen particle, the follower, adopts the velocity of its closest neighbor, the leader. We study the limit of a system size going to infinity and, under the assumption of propagation of chaos, show that the limit kinetic equation is a non-standard spatial diffusion equation for the particle distribution function. We also study the case wherein the particles interact with their closest neighbors and show that the corresponding kinetic equation is the same. Finally, we prove that these models can be seen as a singular limit of the smooth rank-based model previously studied in Blanchet and Degond (J Stat Phys 163:41-60, 2016). The proofs are based on a combinatorial interpretation of the rank as well as some concentration of measure arguments.

摘要

我们考虑通过拓扑相互作用进行交互的主体系统。这些相互作用已被证明在动物和人类行为中起着重要作用。确切地说,该系统由有限数量的粒子组成,这些粒子由其位置和速度来表征。在随机时刻,一个随机选择的粒子,即跟随者,采用其最近邻粒子,即领导者的速度。我们研究系统规模趋于无穷大时的极限情况,并在混沌传播的假设下,表明极限动力学方程是粒子分布函数的一个非标准空间扩散方程。我们还研究了粒子与其最近邻粒子相互作用的情况,并表明相应的动力学方程是相同的。最后,我们证明这些模型可以被视为先前在Blanchet和Degond(《统计物理杂志》163:41 - 60,2016)中研究的基于秩的光滑模型的奇异极限。证明基于秩的组合解释以及一些测度集中论证。