45,163 research outputs found

    Mediatic graphs

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    Any medium can be represented as an isometric subgraph of the hypercube, with each token of the medium represented by a particular equivalence class of arcs of the subgraph. Such a representation, although useful, is not especially revealing of the structure of a particular medium. We propose an axiomatic definition of the concept of a `mediatic graph'. We prove that the graph of any medium is a mediatic graph. We also show that, for any non-necessarily finite set S, there exists a bijection from the collection M of all the media on a given set S (of states) onto the collection G of all the mediatic graphs on S.Comment: Four axioms replaced by two; two references added; Fig.6 correcte

    Partition Function Expansion on Region-Graphs and Message-Passing Equations

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    Disordered and frustrated graphical systems are ubiquitous in physics, biology, and information science. For models on complete graphs or random graphs, deep understanding has been achieved through the mean-field replica and cavity methods. But finite-dimensional `real' systems persist to be very challenging because of the abundance of short loops and strong local correlations. A statistical mechanics theory is constructed in this paper for finite-dimensional models based on the mathematical framework of partition function expansion and the concept of region-graphs. Rigorous expressions for the free energy and grand free energy are derived. Message-passing equations on the region-graph, such as belief-propagation and survey-propagation, are also derived rigorously.Comment: 10 pages including two figures. New theoretical and numerical results added. Will be published by JSTAT as a lette

    Representing convex geometries by almost-circles

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    Finite convex geometries are combinatorial structures. It follows from a recent result of M.\ Richter and L.G.\ Rogers that there is an infinite set TrrT_{rr} of planar convex polygons such that TrrT_{rr} with respect to geometric convex hulls is a locally convex geometry and every finite convex geometry can be represented by restricting the structure of TrrT_{rr} to a finite subset in a natural way. An \emph{almost-circle of accuracy} 1−ϵ1-\epsilon is a differentiable convex simple closed curve SS in the plane having an inscribed circle of radius r1>0r_1>0 and a circumscribed circle of radius r2r_2 such that the ratio r1/r2r_1/r_2 is at least 1−ϵ1-\epsilon. % Motivated by Richter and Rogers' result, we construct a set TnewT_{new} such that (1) TnewT_{new} contains all points of the plane as degenerate singleton circles and all of its non-singleton members are differentiable convex simple closed planar curves; (2) TnewT_{new} with respect to the geometric convex hull operator is a locally convex geometry; (3) as opposed to TrrT_{rr}, TnewT_{new} is closed with respect to non-degenerate affine transformations; and (4) for every (small) positive ϵ∈ℜ\epsilon\in\real and for every finite convex geometry, there are continuum many pairwise affine-disjoint finite subsets EE of TnewT_{new} such that each EE consists of almost-circles of accuracy 1−ϵ1-\epsilon and the convex geometry in question is represented by restricting the convex hull operator to EE. The affine-disjointness of E1E_1 and E2E_2 means that, in addition to E1∩E2=∅E_1\cap E_2=\emptyset, even ψ(E1)\psi(E_1) is disjoint from E2E_2 for every non-degenerate affine transformation ψ\psi.Comment: 18 pages, 6 figure
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