11 research outputs found

    Abelian networks II. Halting on all inputs

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    Abelian networks are systems of communicating automata satisfying a local commutativity condition. We show that a finite irreducible abelian network halts on all inputs if and only if all eigenvalues of its production matrix lie in the open unit disk.Comment: Supersedes sections 5 and 6 of arXiv:1309.3445v1. To appear in Selecta Mathematic

    Absorbing-state phase transition and activated random walks with unbounded capacities

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    In this article, we study the existence of an absorbing-state phase transition of an Abelian process that generalises the Activated Random Walk (ARW). Given a vertex transitive G=(V,E), we associate to each site x∈V a capacity wx≥0, which describes how many inactive particles x can hold, where {wx}x∈V is a collection of i.i.d random variables. When G is an amenable graph, we prove that if E[wx]0. Moreover, in the former case, we provide bounds for the critical density that match the ones available in the classical Activated Random Walk

    Abelian networks III. The critical group

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    The critical group of an abelian network is a finite abelian group that governs the behavior of the network on large inputs. It generalizes the sandpile group of a graph. We show that the critical group of an irreducible abelian network acts freely and transitively on recurrent states of the network. We exhibit the critical group as a quotient of a free abelian group by a subgroup containing the image of the Laplacian, with equality in the case that the network is rectangular. We generalize Dhar's burning algorithm to abelian networks, and estimate the running time of an abelian network on an arbitrary input up to a constant additive error.Comment: supersedes sections 7 and 8 of arXiv:1309.3445v1. To appear in the Journal of Algebraic Combinatoric

    Uniform threshold for fixation of the stochastic sandpile model on the line

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    We consider the abelian stochastic sandpile model. In this model, a site is deemed unstable when it contains more than one particle. Each unstable site, independently, is toppled at rate 11, sending two of its particles to neighbouring sites chosen independently. We show that when the initial average density is less than 1/21/2, the system locally fixates almost surely. We achieve this bound by analysing the parity of the total number of times each site is visited by a large number of particles under the sandpile dynamics.Comment: 21 pages including bibliography, 19 withou

    Abelian networks IV. Dynamics of nonhalting networks

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    An abelian network is a collection of communicating automata whose state transitions and message passing each satisfy a local commutativity condition. This paper is a continuation of the abelian networks series of Bond and Levine (2016), for which we extend the theory of abelian networks that halt on all inputs to networks that can run forever. A nonhalting abelian network can be realized as a discrete dynamical system in many different ways, depending on the update order. We show that certain features of the dynamics, such as minimal period length, have intrinsic definitions that do not require specifying an update order. We give an intrinsic definition of the \emph{torsion group} of a finite irreducible (halting or nonhalting) abelian network, and show that it coincides with the critical group of Bond and Levine (2016) if the network is halting. We show that the torsion group acts freely on the set of invertible recurrent components of the trajectory digraph, and identify when this action is transitive. This perspective leads to new results even in the classical case of sinkless rotor networks (deterministic analogues of random walks). In Holroyd et. al (2008) it was shown that the recurrent configurations of a sinkless rotor network with just one chip are precisely the unicycles (spanning subgraphs with a unique oriented cycle, with the chip on the cycle). We generalize this result to abelian mobile agent networks with any number of chips. We give formulas for generating series such as n1rnzn=det(11zDA) \sum_{n \geq 1} r_n z^n = \det (\frac{1}{1-z}D - A ) where rnr_n is the number of recurrent chip-and-rotor configurations with nn chips; DD is the diagonal matrix of outdegrees, and AA is the adjacency matrix. A consequence is that the sequence (rn)n1(r_n)_{n \geq 1} completely determines the spectrum of the simple random walk on the network.Comment: 95 pages, 21 figure
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