24,471 research outputs found

    Number of cycles in the graph of 312-avoiding permutations

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    The graph of overlapping permutations is defined in a way analogous to the De Bruijn graph on strings of symbols. That is, for every permutation π=π1π2...πn+1\pi = \pi_{1} \pi_{2} ... \pi_{n+1} there is a directed edge from the standardization of π1π2...πn\pi_{1} \pi_{2} ... \pi_{n} to the standardization of π2π3...πn+1\pi_{2} \pi_{3} ... \pi_{n+1}. We give a formula for the number of cycles of length dd in the subgraph of overlapping 312-avoiding permutations. Using this we also give a refinement of the enumeration of 312-avoiding affine permutations and point out some open problems on this graph, which so far has been little studied.Comment: To appear in the Journal of Combinatorial Theory - Series

    Cardinality of Rauzy classes

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    Rauzy classes define a partition of the set of irreducible (or indecomposable) permutations. They were defined by G. Rauzy as part of an induction algorithm for interval exchange transformations. In this article we prove an explicit formula for the cardinality of all Rauzy classes.Comment: 43 pages, 22 figure

    Universal behaviour of 3D loop soup models

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    These notes describe several loop soup models and their {\it universal behaviour} in dimensions greater or equal to 3. These loop models represent certain classical or quantum statistical mechanical systems. These systems undergo phase transitions that are characterised by changes in the structures of the loops. Namely, long-range order is equivalent to the occurrence of macroscopic loops. There are many such loops, and the joint distribution of their lengths is always given by a {\it Poisson-Dirichlet distribution}. This distribution concerns random partitions and it is not widely known in statistical physics. We introduce it explicitly, and we explain that it is the invariant measure of a mean-field split-merge process. It is relevant to spatial models because the macroscopic loops are so intertwined that they behave effectively in mean-field fashion. This heuristics can be made exact and it allows to calculate the parameter of the Poisson-Dirichlet distribution. We discuss consequences about symmetry breaking in certain quantum spin systems.Comment: 31 pages, 11 figures. Notes prepared for the 6th Warsaw School of Statistical Physics, held from 25 June to 2 July 2016 in Sandomierz, Polan
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