2,973 research outputs found

    Fork-decompositions of matroids

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    For the abstract of this paper, please see the PDF file

    On matroids of branch-width three

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    For the abstract of this paper, please see the PDF file

    The structure of the 3-separations of 3-connected matroids II

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    The authors showed in an earlier paper that there is a tree that displays, up to a natural equivalence, all non-trivial 3-separations of a 3-connected matroid. The purpose of this paper is to show that if certain natural conditions are imposed on the tree, then it has a uniqueness property. In particular; suppose that, from every pair of edges that meet at a degree-2 vertex and have their other ends of degree at least three, one edge is contracted. Then the resulting tree is unique

    The structure of the 3-separations of 3-connected matroids

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    Special Issue Dedicated to Professor W.T. TutteTutte defined a k-separation of a matroid M to be a partition (A,B) of the ground set of M such that āˆ£Aāˆ£,āˆ£Bāˆ£ ā‰„ k and r(A) + r(B) āˆ’ r(M) < k. If, for all m < n, the matroid M has no m-separations, then M is n-connected. Earlier, Whitney showed that (A,B) is a 1-separation of M if and only if A is a union of 2-connected components of M. When M is 2-connected, Cunningham and Edmonds gave a tree decomposition of M that displays all of its 2-separations. When M is 3-connected, this paper describes a tree decomposition of M that displays, up to a certain natural equivalence, all non-trivial 3-separations of M

    Computer model calibration with large non-stationary spatial outputs: application to the calibration of a climate model

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    Bayesian calibration of computer models tunes unknown input parameters by comparing outputs with observations. For model outputs that are distributed over space, this becomes computationally expensive because of the output size. To overcome this challenge, we employ a basis representation of the model outputs and observations: we match these decompositions to carry out the calibration efficiently. In the second step, we incorporate the non-stationary behaviour, in terms of spatial variations of both variance and correlations, in the calibration. We insert two integrated nested Laplace approximation-stochastic partial differential equation parameters into the calibration. A synthetic example and a climate model illustration highlight the benefits of our approach

    Recoiling Black Holes in Quasars

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    Recent simulations of merging black holes with spin give recoil velocities from gravitational radiation up to several thousand km/s. A recoiling supermassive black hole can retain the inner part of its accretion disk, providing fuel for a continuing QSO phase lasting millions of years as the hole moves away from the galactic nucleus. One possible observational manifestation of a recoiling accretion disk is in QSO emission lines shifted in velocity from the host galaxy. We have examined QSOs from the Sloan Digital Sky Survey with broad emission lines substantially shifted relative to the narrow lines. We find no convincing evidence for recoiling black holes carrying accretion disks. We place an upper limit on the incidence of recoiling black holes in QSOs of 4% for kicks greater than 500 km/s and 0.35% for kicks greater than 1000 km/s line-of-sight velocity.Comment: 4 pages, 4 figures, uses emulateapj, Submitted to ApJ Letter

    Quasi-graphic matroids

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    Frame matroids and lifted-graphic matroids are two interesting generalizations of graphic matroids. Here we introduce a new generalization, quasi-graphic matroids, that unifies these two existing classes. Unlike frame matroids and lifted-graphic matroids, it is easy to certify that a matroid is quasi-graphic. The main result of the paper is that every 3-connected representable quasi-graphic matroid is either a lifted-graphic matroid or a rame matroid

    Tangles, tree-decompositions, and grids in matroids

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    A tangle in a matroid is an obstruction to small branch-width. In particular, the maximum order of a tangle is equal to the branch-width. We prove that: (i) there is a tree-decomposition of a matroid that ā€œdisplaysā€ all of the maximal tangles, and (ii) when M is representable over a ļ¬nite ļ¬eld, each tangle of suļ¬ƒciently large order ā€œdominatesā€ a large grid-minor. This extends results of Robertson and Seymour concerning Graph Minors

    Branch-width and well-quasi-ordering in matroids and graphs

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    AbstractWe prove that a class of matroids representable over a fixed finite field and with bounded branch-width is well-quasi-ordered under taking minors. With some extra work, the result implies Robertson and Seymour's result that graphs with bounded tree-width (or equivalently, bounded branch-width) are well-quasi-ordered under taking minors. We will not only derive their result from our result on matroids, but we will also use the main tools for a direct proof that graphs with bounded branch-width are well-quasi-ordered under taking minors. This proof also provides a model for the proof of the result on matroids, with all specific matroid technicalities stripped off

    On inequivalent representations of matroids over non-prime ļ¬elds

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    For each ļ¬nite ļ¬eld FF of prime order there is a constant cc such that every 4-connected matroid has at most cc inequivalent representations over FF. We had hoped that this would extend to all ļ¬nite ļ¬elds, however, it was not to be. The (m,n)(m,n)-mace is the matroid obtained by adding a point freely to M(Km,n)M(K_{m,n}). For all nā‰„3n \geq 3, the (3,n)(3,n)-mace is 4-connected and has at least 2n2n representations over any ļ¬eld FF of non-prime order qā‰„9q \geq 9. More generally, for nā‰„mn \geq m, the (m,n)(m,n)-mace is vertically (m+1)(m+1)-connected and has at least 2n2n inequivalent representations over any ļ¬nite ļ¬eld of non-prime order qā‰„mmq\geq m^m
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