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Author: M.E.J. Newman Presenter: Guoliang Liu Date:5/4/2012
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Networks in the real world Properties of networks Random graphs Exponential random graphs and Markov graphs The small-world model Models of network growth Processes happening or happened
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Social networksInformation networksTechnological networksBiological networks
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Networks in the real world Properties of networks Random graphs Exponential random graphs and Markov graphs The small-world model Models of network growth Processes happening or happened
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The small-world effect Transitivity or clustering Degree distributions Network resilience Mixing patterns Degree correlations Community structure Network navigation Other network properties
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Started from 1960s by Stanley Milgram 6 steps between two nodes. Undirected networks, define l to be the mean geodesic distance between vertex pairs in a network: In case that networks have more than one component Small-world effect: the value l scales logarithmically or slower with network size or fixed mean degree.
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In many networks it is found that if vertex A is connected to vertex B and vertex B to vertex C, then there is a heightened probability that A is connected to C. Cluster coefficient: Global value Local value
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An example to calculate clustering coefficient C
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Resilience to the removal of vertices(or edges.). Popular in Epidemiology, in CS, the attack in complex networks. How to remove? Remove vertices at random Target some specific class of vertices, such as those with the highest degree. How to measure resilience? Distances l increasement on average. Thorough study by Holme et al. “attack vulnerability of complex networks”
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In most kinds of networks, and the probabilities of connection between vertices often depends on types. Food web Social network of couples(In social also called assortative mixing or homophily)
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How to measure mixing patterns? E ij : the number of edges in a network that connect vertices of types i and j. e ij measure the fraction of edges that fall between vertices of types i and j. Assortative mixing coefficient:
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A special case of assortative mixing according to a scalar vertex property is mixing according to vertex degree, referred as degree correlation.
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Ideas from Stanley Milgram’s experiment. Not only small-world effect. But also people are good at finding them. Target: build efficient database structures or better peer-to-peer computer networks. E.g. ”local search in unstructured networks”
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Giant component Betweenness centrality Self-similarity
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Networks in the real world Properties of networks Random graphs Exponential random graphs and Markov graphs The small-world model Models of network growth Processes happening or happened
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Poisson random graph Generalized random graphs
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Why we talk about Poisson random graphs? Basic intuition about the networks behaviors from the study of random graph. Poisson distribution is a classic one and later ideas all started from Poisson random graph
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Poisson random graphs Early work, simple model of a network G n,p, each pair connects with probability p Later, consider the mean degree z = p(n-1) When we focus on low-density, low-p state and high-density, high-p state. A single giant component The remainder of vertices occupying smaller components with exponential size distribution and finite mean size,
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Let u be the fraction of vertices on the graph that do not belong to the giant component. The fraction S of the graph occupied by the giant component is S = 1-u and
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Talk about again about Small-world effect in Poisson random graphs. The mean number of neighbors a distance l away from a vertex in a random graph is z d, and hence the value of d needed to encompass the entire network z l ~n. Thus l = logn/logz. Shortcomings of Poisson Low clustering coefficient C = p, when n is large, p~ n -1 ~0 Unlike the real-world distribution.
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Configuration model The vertex at the end of a randomly chosen edge is proportional to kp k. Excess degree(how many edges there are leaving such a vertex other than the one we arrived along) q k. Define two generating functions
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Consider the giant component: Consider the clustering coefficient
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Directed graphs Bipartite graphs Degree correlations
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Networks in the real world Properties of networks Random graphs Exponential random graphs and Markov graphs The small-world model Models of network growth Processes happening or happened
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Background: properties such as transitivity is not incorporated into random graph models.
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Exponential random graphs (P * models) is a set of measurable properties of a single graph. is a set of inverse-temperature of field parameters Each graph G appears with probability: Partition function Z is
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The calculation of the ensemble average of a graph observable is then found by taking a suitable derivative of free energy f=-logZ. There are ways to express f in closed form. But carrying through the entire field-theoretic program is not easy The question of how to carry out calculations in exponential random graph ensembles is open
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Networks in the real world Properties of networks Random graphs Exponential random graphs and Markov graphs The small-world model Models of network growth Processes happening or happened
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Less sophisticated but more tractable model of a network with high transitivity. Built on lattices of any dimension or topology( Take one dimension with L vertices, each vertex has k neighbors with fewer spacing away) Each edge Rewires randomly with possibility p (create shortcuts)
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Extreme 1, P=0, clustering coefficient C=(3k-3)/(4k-2), Mean geodesic distance tend to L/4k for large L Extreme 2, P=1, C~2k/L Mean geodesic distance logL/logK Numerical simulation by Watts and Strogatz showed there exists a sizable region in between there two extremes for which the model has both low path lengths and high transitivity.
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Modification of the rewiring methods Both ends of edges can be rewired Allow double edges and self edges(maintain original edges)
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A. Clustering coefficient By Barrat and Weigt By Newman B. Degree distribution(Since it is not the goal, behaves badly compared with real- world networks)
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C. Average path length P=0, l~ L/4k, large-world P=1, l~logL, small-world 0<P<1, no exact solution for the value l Attempts:
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The scaling form shows that we can go from large-world regime to the small-world one through Increasing p Increasing the system size L
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Networks in the real world Properties of networks Random graphs Exponential random graphs and Markov graphs The small-world model Models of network growth Processes happening or happened
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Goal of Previous models: Create networks that incorporate properties observed in real-world networks Goal of Models with growth: Explain network properties. Mainly aimed at explaining the origin of the highly skewed degree distributions.
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Price’s Model Basic work and later followed by many others Explanation for power-law: “the rich get richer”, also called cumulative advantage or preferential attachment Mean in-degree: The probability of attachment to a vertex should be proportional to k+k 0. k 0 = 1. The probability that a new edge attaches to any of the vertices with degree k is thus
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Price’s Model Another classic model: model of Barabasi and Albert(using undirected network) Krapivsky and Redner consider the age of vertices and their degrees with older vertices having higher mean degree.
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Networks in the real world Properties of networks Random graphs Exponential random graphs and Markov graphs The small-world model Models of network growth Processes happening
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A. percolation theory and network resilience B. Epidemiological processes The SIR model The SIS model C. Search on networks Exhaustive network search(eigenvector centrality) Guided network search Network navigation D. Other processes
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Study of graph models Other properties such as correlations, transitivity and community structure(degree distribution has been thoroughly done). Relations and differences of smaller components and largest component
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