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arXiv 1603.03218math.PRmath-phmath.MP
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多粒子扩散限制聚集

Multi-Particle Diffusion Limited Aggregation

Vladas Sidoravicius, Alexandre Stauffer

摘要:

考虑了Z^d上的随机聚集模型.从位于晶格顶点的粒子开始,最初根据具有参数μ的乘积伯努利测度分布。此外,还有一个集合,它最初由原点组成。非聚集粒子的运动是连续时间的简单随机游动,遵守不相容规则,而聚集粒子不运动。当一个粒子试图跳到聚集体上时,聚集体通过将粒子附着到其表面而生长。这种演化被称为多粒子扩散限制聚集。我们的主要结果表明,如果d>1,粒子的初始密度足够大,则聚集体具有线性增长的臂的概率为正,即如果F(t)表示在时间t>0时聚集体最远离原点的点,则存在常数c>0,使得|F(t)|”t,最终。我们分析的关键概念要素是引入和研究一个新的增长过程。考虑从原点开始的第一次通过渗流过程,称为类型1。每当类型1即将占据新顶点时,以正概率,它不会这样做,而是会引发另一个第一通道渗透过程,称为类型2,它开始从该顶点传播。每个顶点只被第一个到达它的进程占用。这个过程可能有三个阶段:灭绝阶段,其中类型1最终被类型2集群包围,共存阶段,其中两种类型的无限集群出现,以及强大的生存阶段,其中类型1产生一个无限集群,成功地包围所有类型2集群。理解这个过程在其各个阶段的行为本身就具有数学意义。我们建立了一个强大的生存阶段的存在,并使用它来显示我们的主要结果。

英文摘要:

We consider a stochastic aggregation model on Z^d. Start with particles located at the vertices of the lattice, initially distributed according to the product Bernoulli measure with parameter μ. In addition, there is an aggregate, which initially consists of the origin. Non-aggregated particles move as continuous time simple random walks obeying the exclusion rule, whereas aggregated particles do not move. The aggregate grows by attaching particles to its surface whenever a particle attempts to jump onto it. This evolution is referred to as multi-particle diffusion limited aggregation. Our main result states that if on d>1 the initial density of particles is large enough, then with positive probability the aggregate has linearly growing arms, i.e. if F(t) denotes the point of the aggregate furthest away from the origin at time t>0, then there exists a constant c>0 so that |F(t)|>ct, for all t eventually. The key conceptual element of our analysis is the introduction and study of a new growth process. Consider a first passage percolation process, called type 1, starting from the origin. Whenever type 1 is about to occupy a new vertex, with positive probability, instead of doing it, it gives rise to another first passage percolation process, called type 2, which starts to spread from that vertex. Each vertex gets occupied only by the process that arrives to it first. This process may have three phases: an extinction phase, where type 1 gets eventually surrounded by type 2 clusters, a coexistence phase, where infinite clusters of both types emerge, and a strong survival phase, where type 1 produces an infinite cluster that successfully surrounds all type 2 clusters. Understanding the behavior of this process in its various phases is of mathematical interest on its own right. We establish the existence of a strong survival phase, and use this to show our main result.

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