1,041 research outputs found

    Counting and Enumerating Crossing-free Geometric Graphs

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    We describe a framework for counting and enumerating various types of crossing-free geometric graphs on a planar point set. The framework generalizes ideas of Alvarez and Seidel, who used them to count triangulations in time O(2nn2)O(2^nn^2) where nn is the number of points. The main idea is to reduce the problem of counting geometric graphs to counting source-sink paths in a directed acyclic graph. The following new results will emerge. The number of all crossing-free geometric graphs can be computed in time O(cnn4)O(c^nn^4) for some c<2.83929c < 2.83929. The number of crossing-free convex partitions can be computed in time O(2nn4)O(2^nn^4). The number of crossing-free perfect matchings can be computed in time O(2nn4)O(2^nn^4). The number of convex subdivisions can be computed in time O(2nn4)O(2^nn^4). The number of crossing-free spanning trees can be computed in time O(cnn4)O(c^nn^4) for some c<7.04313c < 7.04313. The number of crossing-free spanning cycles can be computed in time O(cnn4)O(c^nn^4) for some c<5.61804c < 5.61804. With the same bounds on the running time we can construct data structures which allow fast enumeration of the respective classes. For example, after O(2nn4)O(2^nn^4) time of preprocessing we can enumerate the set of all crossing-free perfect matchings using polynomial time per enumerated object. For crossing-free perfect matchings and convex partitions we further obtain enumeration algorithms where the time delay for each (in particular, the first) output is bounded by a polynomial in nn. All described algorithms are comparatively simple, both in terms of their analysis and implementation

    Counting Triangulations and other Crossing-Free Structures Approximately

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    We consider the problem of counting straight-edge triangulations of a given set PP of nn points in the plane. Until very recently it was not known whether the exact number of triangulations of PP can be computed asymptotically faster than by enumerating all triangulations. We now know that the number of triangulations of PP can be computed in O∗(2n)O^{*}(2^{n}) time, which is less than the lower bound of Ω(2.43n)\Omega(2.43^{n}) on the number of triangulations of any point set. In this paper we address the question of whether one can approximately count triangulations in sub-exponential time. We present an algorithm with sub-exponential running time and sub-exponential approximation ratio, that is, denoting by Λ\Lambda the output of our algorithm, and by cnc^{n} the exact number of triangulations of PP, for some positive constant cc, we prove that cn≤Λ≤cn⋅2o(n)c^{n}\leq\Lambda\leq c^{n}\cdot 2^{o(n)}. This is the first algorithm that in sub-exponential time computes a (1+o(1))(1+o(1))-approximation of the base of the number of triangulations, more precisely, c≤Λ1n≤(1+o(1))cc\leq\Lambda^{\frac{1}{n}}\leq(1 + o(1))c. Our algorithm can be adapted to approximately count other crossing-free structures on PP, keeping the quality of approximation and running time intact. In this paper we show how to do this for matchings and spanning trees.Comment: 19 pages, 2 figures. A preliminary version appeared at CCCG 201

    Wall Crossing, Quivers and Crystals

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    We study the spectrum of BPS D-branes on a Calabi-Yau manifold using the 0+1 dimensional quiver gauge theory that describes the dynamics of the branes at low energies. The results of Kontsevich and Soibelman predict how the degeneracies change. We argue that Seiberg dualities of the quiver gauge theories, which change the basis of BPS states, correspond to crossing the "walls of the second kind." There is a large class of examples, including local del Pezzo surfaces, where the BPS degeneracies of quivers corresponding to one D6 brane bound to arbitrary numbers of D4, D2 and D0 branes are counted by melting crystal configurations. We show that the melting crystals that arise are a discretization of the Calabi-Yau geometry. The shape of the crystal is determined by the Calabi-Yau geometry and the background B-field, and its microscopic structure by the quiver Q. We prove that the BPS degeneracies computed from Q and Q' are related by the Kontsevich Soibelman formula, using a geometric realization of the Seiberg duality in the crystal. We also show that, in the limit of infinite B-field, the combinatorics of crystals arising from the quivers becomes that of the topological vertex. We thus re-derive the Gromov-Witten/Donaldson-Thomas correspondence
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