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The fault-diameter and wide-diameter of twisted hypercubes

机译:扭曲超速度的故障直径和宽直径

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The l-fault-diameter of a graph G is the minimum d such that the diameter of G - X is at most d for any subset X of V(G) of size vertical bar X vertical bar = - 1. The -wide-diameter of G is the minimum integer d for which there exist at least l internally vertex disjoint paths of length at most d between any two distinct vertices in G. These two parameters measure the fault tolerance and transmission delay in communication networks modelled by graphs. Twisted hypercubes are variation of hypercubes defined recursively: K-1 is the only 0 -dimension twisted hypercube, and for n = 1, an n-dimensional twisted hypercube G(n) is obtained from the disjoint union of two (n - 1)-dimensional twisted hypercubes G'(n-1) and G"(n-1) by adding a perfect matching between V(G'(')(n-)) and V(G"(n-1)). Recently, two types of twisted hypercubes Z(n,k) and lin are introduced in Zhu (2017). This paper gives an upper bound for the n -fault diameters of special families of twisted hypercubes of dimension n. As a consequence of this result, the n-fault-diameter of H-n is (1 + 0(1)) n/log2(n.) For k = [log(2)(n) -2log(2)log(2)(n), the n-fault-diameter of Z(n,k) is also (1 + o(1))n/log2(n). This bound is asymptotically optimal, as any n-dimensional twisted hypercube has diameter greater than n/log2(n) Then we extend a result in Qi and Zhu (2017) about Z(n,)k toll, and prove that the K(n)-wide-diameter of H-n, is (1 + 0(1)) n/log2(n). (C) 2017 Published by Elsevier B.V.
机译:图G的L-故障直径是最小d,使得G-X的直径至大部分为V(g)的尺寸垂直条x垂直条的任何子集x& -1。-1。 - G的宽直径是最小的整数D,其中至少存在至少L的内部顶点不相交的路径最多d在G的任何两个不同顶点之间的D.这两个参数测量由图表建模的通信网络中的容错和传输延迟。扭曲的超胶质是递归定义的超速度的变化:K-1是唯一的0 -Dimension扭曲的超速度,并且对于N& = 1,从两个(n - 1)通过在V(g'(')(n-))和v(g“(n-1)之间添加完美匹配来实现 - 二维扭曲的超电平g'(n-1)和g”(n-1) 。最近,在朱(2017年)中引入了两种类型的扭曲超速Z(n,k)和林。本文给出了尺寸扭曲超机的特殊系列的n - 跳法的N -Fault直径的上限。由于该结果,Hn的n-Fault-Dategs是(1 + 0(1))n / log2(n。),用于k = [log(2)(n)-2log(2)log(2 )(n),z(n,k)的n-fauth-degator也是(1 + O(1))n / log2(n)。这种界限是渐近的最佳状态,因为任何n维扭曲的超立体具有大于n / log2(n)的直径,那么我们在qi和zhu(2017)中延伸了大约z(n,)k损失,并证明了k( N)-Wide-LOMID的直径为(1 + 0(1))n / log2(n)。 (c)2017年由Elsevier B.V发布。

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