7 research outputs found

    Lower bounds on the dilation of plane spanners

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    (I) We exhibit a set of 23 points in the plane that has dilation at least 1.43081.4308, improving the previously best lower bound of 1.41611.4161 for the worst-case dilation of plane spanners. (II) For every integer n13n\geq13, there exists an nn-element point set SS such that the degree 3 dilation of SS denoted by δ0(S,3) equals 1+3=2.7321\delta_0(S,3) \text{ equals } 1+\sqrt{3}=2.7321\ldots in the domain of plane geometric spanners. In the same domain, we show that for every integer n6n\geq6, there exists a an nn-element point set SS such that the degree 4 dilation of SS denoted by δ0(S,4) equals 1+(55)/2=2.1755\delta_0(S,4) \text{ equals } 1 + \sqrt{(5-\sqrt{5})/2}=2.1755\ldots The previous best lower bound of 1.41611.4161 holds for any degree. (III) For every integer n6n\geq6 , there exists an nn-element point set SS such that the stretch factor of the greedy triangulation of SS is at least 2.02682.0268.Comment: Revised definitions in the introduction; 23 pages, 15 figures; 2 table

    The Stretch Factor of the Delaunay Triangulation Is Less Than 1.998

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    Let SS be a finite set of points in the Euclidean plane. Let DD be a Delaunay triangulation of SS. The {\em stretch factor} (also known as {\em dilation} or {\em spanning ratio}) of DD is the maximum ratio, among all points pp and qq in SS, of the shortest path distance from pp to qq in DD over the Euclidean distance pq||pq||. Proving a tight bound on the stretch factor of the Delaunay triangulation has been a long standing open problem in computational geometry. In this paper we prove that the stretch factor of the Delaunay triangulation of a set of points in the plane is less than ρ=1.998\rho = 1.998, improving the previous best upper bound of 2.42 by Keil and Gutwin (1989). Our bound 1.998 is better than the current upper bound of 2.33 for the special case when the point set is in convex position by Cui, Kanj and Xia (2009). This upper bound breaks the barrier 2, which is significant because previously no family of plane graphs was known to have a stretch factor guaranteed to be less than 2 on any set of points.Comment: 41 pages, 16 figures. A preliminary version of this paper appeared in the Proceedings of the 27th Annual Symposium on Computational Geometry (SoCG 2011). This is a revised version of the previous preprint [v1

    Drawing Graphs as Spanners

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    We study the problem of embedding graphs in the plane as good geometric spanners. That is, for a graph GG, the goal is to construct a straight-line drawing Γ\Gamma of GG in the plane such that, for any two vertices uu and vv of GG, the ratio between the minimum length of any path from uu to vv and the Euclidean distance between uu and vv is small. The maximum such ratio, over all pairs of vertices of GG, is the spanning ratio of Γ\Gamma. First, we show that deciding whether a graph admits a straight-line drawing with spanning ratio 11, a proper straight-line drawing with spanning ratio 11, and a planar straight-line drawing with spanning ratio 11 are NP-complete, R\exists \mathbb R-complete, and linear-time solvable problems, respectively, where a drawing is proper if no two vertices overlap and no edge overlaps a vertex. Second, we show that moving from spanning ratio 11 to spanning ratio 1+ϵ1+\epsilon allows us to draw every graph. Namely, we prove that, for every ϵ>0\epsilon>0, every (planar) graph admits a proper (resp. planar) straight-line drawing with spanning ratio smaller than 1+ϵ1+\epsilon. Third, our drawings with spanning ratio smaller than 1+ϵ1+\epsilon have large edge-length ratio, that is, the ratio between the length of the longest edge and the length of the shortest edge is exponential. We show that this is sometimes unavoidable. More generally, we identify having bounded toughness as the criterion that distinguishes graphs that admit straight-line drawings with constant spanning ratio and polynomial edge-length ratio from graphs that require exponential edge-length ratio in any straight-line drawing with constant spanning ratio

    Stretch Factor in a Planar Poisson-Delaunay Triangulation with a Large Intensity

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    International audienceLet X:=Xn{(0,0),(1,0)}X := X_n ∪ \{(0, 0), (1, 0)\}, where XnX_n is a planar Poisson point process of intensity nn. We provide a first non-trivial lower bound for the distance between the expected length of the shortest path between (0, 0) and (1, 0) in the Delaunay triangulation associated with XX when the intensity of XnX_n goes to infinity. Simulations indicate that the correct value is about 1.04. We also prove that the expected length of the so-called upper path converges to 35/3π235/3\pi^2, giving an upper bound for the expected length of the smallest path

    Constrained generalized Delaunay graphs are plane spanners

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    We look at generalized Delaunay graphs in the constrained setting by introducing line segments which the edges of the graph are not allowed to cross. Given an arbitrary convex shape C, a constrained Delaunay graph is constructed by adding an edge between two vertices p and q if and only if there exists a homothet of C with p and q on its boundary that does not contain any other vertices visible to p and q. We show that, regardless of the convex shape C used to construct the constrained Delaunay graph, there exists a constant t (that depends on C) such that it is a plane t-spanner of the visibility graph
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