4.6 Article

Coherence Scaling of Noisy Second-Order Scale-Free Consensus Networks

期刊

IEEE TRANSACTIONS ON CYBERNETICS
卷 52, 期 7, 页码 5923-5934

出版社

IEEE-INST ELECTRICAL ELECTRONICS ENGINEERS INC
DOI: 10.1109/TCYB.2021.3052519

关键词

Distributed average consensus; Gaussian white noise; multiagent systems; network coherence; scale-free network; small-world network

资金

  1. National Key Research and Development Program of China [2018YFB1305104, 2019YFB2101703]
  2. National Natural Science Foundation of China [61803248, 61872093, U19A2066, U20B2051]
  3. Shanghai Municipal Science and Technology Major Project [2018SHZDZX01]
  4. City University of Hong Kong [7005061]

向作者/读者索取更多资源

A striking discovery in network science is that real networked systems exhibit universal structural properties such as sparsity, scale-free, small-world, and loops. Researchers focus on second-order consensus in dynamic networks and find that it scales sublinearly with the number of vertices. This behavior is attributed to the joint influence of scale-free, small-world, and loopy topologies.
A striking discovery in the field of network science is that the majority of real networked systems have some universal structural properties. In general, they are simultaneously sparse, scale-free, small-world, and loopy. In this article, we investigate the second-order consensus of dynamic networks with such universal structures subject to white noise at vertices. We focus on the network coherence H-SO characterized in terms of the H-2-norm of the vertex systems, which measures the mean deviation of vertex states from their average value. We first study numerically the coherence of some representative real-world networks. We find that their coherence H-SO scales sublinearly with the vertex number N. We then study analytically H-SO for a class of iteratively growing networks-pseudofractal scale-free webs (PSFWs), and obtain an exact solution to H-SO, which also increases sublinearly in N, with an exponent much smaller than 1. To explain the reasons for this sublinear behavior, we finally study H-SO for Sierpinski gaskets, for which H-SO grows superlinearly in N, with a power exponent much larger than 1. Sierpinski gaskets have the same number of vertices and edges as the PSFWs but do not display the scale-free and small-world properties. We thus conclude that the scale-free, small-world, and loopy topologies are jointly responsible for the observed sublinear scaling of H-SO.

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