Abstract

We study an infinite system of independent symmetric random walks on a hierarchical group, in particular, the <em>c</em>-random walks. Such walks are used, e.g., in mathematical physics and population biology. The number variance problem consists in investigating if the variance of the number of “particles” $N_n(L)$ lying in the ball of radius $L$<em></em> at a given step $n$<em></em> remains bounded, or even better, converges to a finite limit, as $L\to\infty$. We give a necessary and sufficient condition and discuss its relationship to transience/recurrence property of the walk. Next we consider normalized fluctuations of $N_n(L)$ around the mean as $n\to\infty$ and $L$<em></em> is increased in an appropriate way. We prove convergence of finite dimensional distributions to a Gaussian process whose properties are discussed. As the $c$<em></em>-random walks mimic symmetric stable processes on $\mathbb{R}$, we compare our results with those obtained by Hambly and Jones (2007, 2009), who studied the number variance problem for an infinite system of independent symmetric stable processes on $\mathbb{R}$. Since the hierarchical group is an ultrametric space, corresponding results for symmetric stable processes and hierarchical random walks may be analogous or quite different, as has been observed in other contexts. An example of a difference in the present context is that for the stable processes a fluctuation limit process is a Gaussian process which is not Markovian and has long range dependent stationary increments, but the counterpart for hierarchical random walks is Markovian, and in a special case it has independent increments.

Highlights

  • Stochastic models on the d-dimensional Euclidean lattice Zd play a fundamental role in mathematical physics and population biology

  • The class of hierarchical models first introduced by Dyson [16] in 1969 have played an important role for gaining insight into these problems. One reason for this is that the models can be parametrized in the hierarchical lattice in such a way as to provide a “caricature” for the Euclidean lattice of dimension d of interest (e.g. d = 4 and dimensions “infinitesimally close” to 4 in the study of ferromagnetic models, see e.g. [5])

  • The other reason is that the structure of these models is such that it has been possible to carry out the renormalization group analysis in a rigorous way in the hierarchical lattice

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Summary

Introduction

Stochastic models on the d-dimensional Euclidean lattice Zd play a fundamental role in mathematical physics and population biology. For the Poisson model we show that with general rj the fluctuation limit exists and it is, up to a constant, the same process as that obtained in the previous case for a = 1.

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