Abstract

We investigate the influence of the small-world topology on the composition of information flow on networks. By appealing to the combinatorial Hodge theory, we decompose information flow generated by random threshold networks on the Watts-Strogatz model into three components: gradient, harmonic and curl flows. The harmonic and curl flows represent globally circular and locally circular components, respectively. The Watts-Strogatz model bridges the two extreme network topologies, a lattice network and a random network, by a single parameter that is the probability of random rewiring. The small-world topology is realized within a certain range between them. By numerical simulation we found that as networks become more random the ratio of harmonic flow to the total magnitude of information flow increases whereas the ratio of curl flow decreases. Furthermore, both quantities are significantly enhanced from the level when only network structure is considered for the network close to a random network and a lattice network, respectively. Finally, the sum of these two ratios takes its maximum value within the small-world region. These findings suggest that the dynamical information counterpart of global integration and that of local segregation are the harmonic flow and the curl flow, respectively, and that a part of the small-world region is dominated by internal circulation of information flow.

Highlights

  • Small-world topology of brain networks has been paid much attention in neuroscience

  • The aim of this paper is to reveal the influence of the smallworld topology on information flow generated by dynamical processes on it

  • We studied the composition of information flow generated by random threshold networks (RTNs) on the Watts-Strogatz small-world model

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Summary

Introduction

Small-world topology of brain networks has been paid much attention in neuroscience It is found ubiquitously in both structural and functional neuronal networks from those of local neuronal populations to large-scale brain areas (Bassett and Bullmore, 2006; Bullmore and Sporns, 2010; Poli et al, 2015). A network is called small-world when its mean path length is small and its clustering coefficient is large (Watts and Strogatz, 1998). Note that it is meaningful only for sparse networks since densely connected networks trivially satisfy the two features of the small-world topology (Markov et al, 2013)

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