Henning S. Mortveit: Research

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Graph Dynamical Systems

The term Graph Dynamical Systems (GDS) covers many classes of dynamical systems. Several of these are constructed from the following common structural elements: If, for example, all the vertex maps are applied synchronously one obtains the class of generalized cellular automata (CA). In this case, the global map FKnKn is given by

F(x)v = fv(x[v])  .

This class is referred to as generalized CA since cellular automata are typically defined and studied over regular graphs or grids. If the vertex functions are applied asynchronously in the order specified by some word w = (w1, w2, … , wm) or permutation π = ( π1, π2, … πn) of v[Y] one obtains the class of Sequential Dynamical Systems (SDS). In this case it is convenient to introduce the Y-local maps Fi constructed from the vertex functions by

Fi (x) = (x1, x2, …, xi-1, fi(x[i]), xi+1, …, xn).

The SDS map F = [FY , w] : KnKn is the function composition

[FY ,w] = Fw(m) ° Fw(m-1) ° ··· ° Fw(2) ° Fw(1)  .

The phase space associated to a dynamical system with with map FKnKn is the finite (since K is finite) directed graph with vertex set Kn and edges (x,F(x)). The structure of the phase space is governed by the properties of the graph Y, the vertex functions (fi)i, and the permutation or word specifying the composition order. The research in this area uses techniques from, e.g. abstract algebra, combinatorics and probability theory to infer phase space properties based on the structure of the system constituents.

Graph dynamical systems constitute a natural framework for capturing distributed systems such as biological networks and epidemics over social networks, many of which are frequently referred to as complex systems.

Publications


Last updated: Mon Oct 1 12:45:44 EDT 2007