Scale-free networks Péter Kómár Statistical physics seminar 07/10/2008
2 Elements of graph theory I. A graph consists: vertices edges Edges can be: directed/undirected weighted/non-weighted self loops multiple edges Non-regular graph
3 Elements of graph theory II. Degree of a vertex: the number of edges going in and/or out Diameter of a graph: distance between the farthest vertices Density of a graph: sparse dense
4 Networks around us I. Internet: routers cables WWW: HTML pages hyperlinks Social networks: people social relationship
5 Networks around us II. Transportation systems: stations / routes routes / stations Nervous system: neurons axons and dendrites Biochemical pathways: chemical substances reactions
6 Real networks Properties: Self-organized structure Evolution in time (growing and varying) Large number of vertices Moderate density Relatively small diameter (Small World phenomenon) Highly centralized subnetworks
7 Random networks Measuring real networks: Relevant state-parameters Evolution in time Creating models: Analytical formulas Growing phenomenon Checking: ‘Raising’ random networks Measuring
8 Scale-free property A.-L. Barabási, R. Albert measured the vertex degree distribution → power-law tail: movie actors: www: US power grid: A.-L. Barabási, R. Albert (1999) ‘Emergence of Scaling in Random Networks’, Science Vol. 286 actors www
9 Small diameter A.-L. Barabási, R. Albert measured the diameter of a HTML graph documents, links found logarithmic dependence: ‘small world’ A.-L. Barabási, R. Albert, H. Jeong (2000) ‘Scale-free characteristics of random networks: the topology of the wold-wide web’, Physica A, Vol. 281 p
10 Erdős-Rényi graph (ER) Construction: N vertices probability of each edge: p ER Properties: p ER ≥ 1/N → → Asympt. connected degree distribution: Poisson (short tail) not centralized small diameter A.-L. Barabási, R. Albert, H. Jeong (1999) ‘Mean-field theory for scale-free random networks’, Physica A, Vol. 272 p (1960. P. Erdős, A. Rényi) N=10 4 p ER = 6∙ ∙ 10 -3
11 ER graph example
12 Small World graph (WS) Construction: N vertices in sequence 1 st and 2 nd neighbor edges rewiring probability: p WS Properties: p WS = 0 → clustered, 0 < p WS < 0.01 → clustered → small-world propery p WS = 1 → not clustered, A.-L. Barabási, R. Albert, H. Jeong (1999) ‘Mean-field theory for scale-free random networks’, Physica A, Vol. 272 p (1998. D.J. Watts, S.H. Strogatz)
13 WS graph example
14 ER graph - WS graph WSER
15 Barabási-Albert graph (BA) New aspects: Continuous growing Preferential attachment Construction: m 0 initial vertices in every step: +1 vertex with m edges P (edge to vertex i ) ~ degree of i A.-L. Barabási, R. Albert, H. Jeong (1999) ‘Mean-field theory for scale-free random networks’, Physica A, Vol. 272 p m 0 = 3 m = 2
16 Barabási-Albert graph II. Properties: Power-law distribution of degrees: Stationary scale-free state Very high clustering Small diameter A.-L. Barabási, R. Albert, H. Jeong (1999) ‘Mean-field theory for scale-free random networks’, Physica A, Vol. 272 p = m 0 = m N =
17 BA graph example
18 ER graph – BA graph
19 Mean-field approximation I. Time dependence of k i (continuous): solution: probability of an edge to i th vertex time of occurrence of the i th vertex A.-L. Barabási, R. Albert, H. Jeong (1999) ‘Mean-field theory for scale-free random networks’, Physica A, Vol. 272 p k i (t) t titititi ~ t 1/2
20 Mean-field approximation II. Distribution of degrees: Distribution of t i : Probability density: A.-L. Barabási, R. Albert, H. Jeong (1999) ‘Mean-field theory for scale-free random networks’, Physica A, Vol. 272 p
21 Without preferential attachment Uniform growth: Exponential degree distribution: A.-L. Barabási, R. Albert, H. Jeong (1999) ‘Mean-field theory for scale-free random networks’, Physica A, Vol. 272 p p(k)p(k)p(k)p(k) k scale-free exponential
22 Without growth Construction: Constant # of vertices + new edges with preferential attachment Properties: At early stages → power-law scaling After t ≈ N 2 steps → dense graph A.-L. Barabási, R. Albert, H. Jeong (1999) ‘Mean-field theory for scale-free random networks’, Physica A, Vol. 272 p t = N 5N 40N N=10 000
23 Conclusion Power-law = Growth + Pref. Attach. Varieties Non-linear attachment probability: → affects the power-law scaling Parallel adding of new edges → Continuously adding edges (eg. actors) → may result complete graph Continuous reconnecting (preferentially) → may result ripened state A.-L. Barabási, R. Albert, H. Jeong (1999) ‘Mean-field theory for scale-free random networks’, Physica A, Vol. 272 p
24 Network research today A.-L. Barabási, R. Albert, ‘Statistical Mechanics of Complex Networks’, arXiv:cond-mat/ v1 6 Jun 2001 Centrality Adjacency matrix Spectral density Attack tolerance
Thank you for the attention!
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27 ER – WS – BA