Abstract

Systems which consist of many localized constituents interacting with each other can be represented by complex networks. Consistently, network science has become highly popular in vast fields focusing on natural, artificial and social systems. We numerically analyze the growth of dd-dimensional geographic networks (characterized by the index αG≥0α_G\geq0; d=1,2,3,4d = 1, 2, 3, 4) whose links are weighted through a predefined random probability distribution, namely P(w)∝e−∣w−wc∣/τP(w) \propto e^{-|w - w_c|/τ}, ww being the weight (wc≥0;  τ>0) (w_c \geq 0; \; τ> 0). In this model, each site has an evolving degree kik_i and a local energy εi≡∑j=1kiwij/2\varepsilon_i \equiv \sum_{j=1}^{k_i} w_{ij}/2 (i=1,2,...,Ni = 1, 2, ..., N) that depend on the weights of the links connected to it. Each newly arriving site links to one of the pre-existing ones through preferential attachment given by the probability Πij∝εi/dij αA    (αA≥0)Π_{ij}\propto \varepsilon_{i}/d^{\,α_A}_{ij} \;\;(α_A \ge 0), where dijd_{ij} is the Euclidean distance between the sites. Short- and long-range interactions respectively correspond to αA/d>1α_A/d>1 and 0≤αA/d≤10\leq α_A/d \leq 1; αA/d→∞α_A/d \to \infty corresponds to interactions between close neighbors, and αA/d→0α_A/d \to 0 corresponds to infinitely-ranged interactions. The site energy distribution p(ε)p(\varepsilon) corresponds to the usual degree distribution p(k)p(k) as the particular instance (wc,τ)=(2,0)(w_c,τ)=(2,0). We numerically verify that the corresponding connectivity distribution p(ε)p(\varepsilon) converges, when αA/d→∞α_A/d\to\infty, to the weight distribution P(w)P(w) for infinitely narrow distributions (i.e., τ→∞, ∀wcτ\to \infty, \,\forall w_c) as well as for wc→0, ∀τw_c\to0, \, \forallτ.

Explore this paper’s authors, topics and related work.

Building this map preview

BZPEER is loading the nearby papers, people, topics and institutions for this page.

Reviews 0

Write a reviewWrite

No reviews yet.

Discussion 0

Add a commentWrite

No comments yet.