Abstract

The relation between network structure and dynamics is determinant for the behavior of complex systems in numerous domains. An important long-standing problem concerns the properties of the networks that optimize the dynamics with respect to a given performance measure. Here we show that such optimization can lead to sensitive dependence of the dynamics on the structure of the network. Specifically, using diffusively coupled systems as examples, we demonstrate that the stability of a dynamical state can exhibit sensitivity to unweighted structural perturbations (i.e., link removals and node additions) for undirected optimal networks and to weighted perturbations (i.e., small changes in link weights) for directed optimal networks. As mechanisms underlying this sensitivity, we identify discontinuous transitions occurring in the complement of undirected optimal networks and the prevalence of eigenvector degeneracy in directed optimal networks. These findings establish a unified characterization of networks optimized for dynamical stability, which we illustrate using Turing instability in activator-inhibitor systems, synchronization in power-grid networks, network diffusion, and several other network processes. Our results suggest that the network structure of a complex system operating near an optimum can potentially be fine-tuned for a significantly enhanced stability compared to what one might expect from simple extrapolation. On the other hand, they also suggest constraints on how close to the optimum the system can be in practice. Finally, the results have potential implications for biophysical networks, which have evolved under the competing pressures of optimizing fitness while remaining robust against perturbations.

Highlights

  • Building on the classical fields of graph theory, statistical physics, and nonlinear dynamics, as well as on the increasing availability of large-scale network data, the field of network dynamics has flourished over the past 15 years [1,2]

  • A fundamental question at the core of the structuredynamics relation is that of optimization: which network structures optimize the dynamics of the system for a given function and what are the properties of such networks? The significance of addressing this question is twofold

  • The sensitive dependence of collective dynamics on the network structure, characterized here by a derivative that diverges at an optimal point, has several implications

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Summary

INTRODUCTION

Building on the classical fields of graph theory, statistical physics, and nonlinear dynamics, as well as on the increasing availability of large-scale network data, the field of network dynamics has flourished over the past 15 years [1,2]. The identification of the network structures that guarantee the best fitness of natural complex systems can provide insights into the mechanisms underlying their evolution Examples of such systems include neuronal networks, whose (synaptic) connectivity structure is believed to have been optimized through evolution or learning for categorization tasks [39], synchronization efficiency [40], dynamical complexity [41,42], information transfer efficiency [42,43], and/or wiring cost [40]. While specific examples can be found in the literature [44,45,46,47], no systematic study exists on general mechanisms and conditions for such sensitivity We provide such conditions in terms of the spectral degeneracy of the network by establishing the scaling relation between the stability and the perturbation size.

NETWORK DYNAMICS CONSIDERED
Optimization problem
Optimal networks
Sensitivity of optimal networks
Directed networks
Nonsensitivity of optimal networks
SENSITIVITY TO WEIGHTED PERTURBATIONS
Eigenvalue scaling for arbitrary networks
Bound on scaling exponent
Typical scaling behavior
Classification of networks by their sensitivity
Sensitivity in directed networks
Nonsensitivity in undirected networks
Generality of the scaling
SENSITIVITY IN EXAMPLE PHYSICAL SYSTEMS
Undirected networks under unweighted perturbations
Directed networks under weighted perturbations
Findings
DISCUSSION

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