Random Walk for Similarity Testing in Complex Networks

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Random Walk for Similarity Testing in Complex Networks Presented by: Shan Lu UMASS 2013/ 04/ 27

Heat content of networks: PL vs ER

Notations Graph : vertex set; : edge set Adjacency Matrix with Degree Matrix with Boundary set: collection of all boundary vertices ; the rest vertices are interior vertices .

Notations Laplacian matrix: Normalized Laplacian: Random walk Laplacian: Let be the eigenvalues of and the corresponding eigenvectors

Notations Choice of boundary nodes: Consider the subgraph with vertices in and let the boundary vertices be absorbing in the following heat equation in next page. Use instead of , but write into for convenience. Choice of boundary nodes: Should not affect the spectral decomposition much; Should not affect the structure of the graph much, such as make the graph disconnected Nodes with smaller degrees

Heat Equation and Heat Content Heat Equation associated with the normalized Laplacian : with a given initial condition. Heat Content:

Discrete time random walk approximation for the heat equation Random walk on graph: random walkers move from current vertex to a neighbor vertex with probability . Transition matrix . 2. Start with uniform initial condition . 3. Lazy random walk: At time ,

Simulation to approximate Heat Content Simulate Lazy Random Walk to approximate the Heat Content: Heat Equation Correction term with uniform initial condition

Graph generating models Barabási–Albert Model: starts out with nodes; each new node is connected to existing nodes with a probability proportional to the degree of the existing nodes. Erdős–Rényi model : , each edge is included in the graph with probability independent from every other edge.

Power Law graph v.s. Random graph Two groups of graphs: Power Law graphs and Random graphs. Average degree varies from 20 to 50 for both the two groups of graphs. Heat Contents in each group are plot in the same color. Power Law Graphs Random Graphs Boundary choice : the 4% (200 in 5000) smallest degree nodes

Power Law graph v.s. Random graph Power Law Graphs Random Graphs The initial time derivative of the heat contents for Power Law graphs with different mean degree The time derivative of the heat contents for the two groups of graphs

Power Law graph v.s. Random graph The eigenvalues of the normalized Laplacian satisfy the semicircle law under the condition that the minimum expected degree is relatively large. (Chung et. al. 2003) Laplacian Spectrum of two graphs with mean degree 20 Laplacian eigenvalues

Power Law graph v.s. Random graph E-R random graph

Other experiment results The randomness in boundary nodes selection does not impact the heat content behavior too much. For a given generating parameter, the heat content variance among different independently generated Power Law graphs decreases with the increasing of graph size.

Ongoing and Future Work Directed Networks Price’s Model in-degree: heavy tail; out degree: constant add node with constant number outgoing links c attach with probability proportional to in-degree plus constant a What if ? Krapivsky’s Model in-degree: heavy tail; out degree: heavy tail Multivariate heavy tail Effect of correlation

Thank you! Question?