1,271 research outputs found

    Matching Preclusion and Conditional Matching Preclusion Problems for Twisted Cubes

    Get PDF
    The matching preclusion number of a graph is the minimum number of edges whose deletion results in a graph that has neither perfect matchings nor almost-perfect matchings. For many interconnection networks, the optimal sets are precisely those induced by a single vertex. Recently, the conditional matching preclusion number of a graph was introduced to look for obstruction sets beyond those induced by a single vertex. It is defined to be the minimum number of edges whose deletion results in a graph with no isolated vertices that has neither perfect matchings nor almost-perfect matchings. In this paper, we find the matching preclusion number and the conditional matching preclusion number for twisted cubes, an improved version of the well-known hypercube. Moreover, we also classify all the optimal matching preclusion sets

    A multipath analysis of biswapped networks.

    Get PDF
    Biswapped networks of the form Bsw(G)Bsw(G) have recently been proposed as interconnection networks to be implemented as optical transpose interconnection systems. We provide a systematic construction of κ+1\kappa+1 vertex-disjoint paths joining any two distinct vertices in Bsw(G)Bsw(G), where κ1\kappa\geq 1 is the connectivity of GG. In doing so, we obtain an upper bound of max{2Δ(G)+5,Δκ(G)+Δ(G)+2}\max\{2\Delta(G)+5,\Delta_\kappa(G)+\Delta(G)+2\} on the (κ+1)(\kappa+1)-diameter of Bsw(G)Bsw(G), where Δ(G)\Delta(G) is the diameter of GG and Δκ(G)\Delta_\kappa(G) the κ\kappa-diameter. Suppose that we have a deterministic multipath source routing algorithm in an interconnection network GG that finds κ\kappa mutually vertex-disjoint paths in GG joining any 22 distinct vertices and does this in time polynomial in Δκ(G)\Delta_\kappa(G), Δ(G)\Delta(G) and κ\kappa (and independently of the number of vertices of GG). Our constructions yield an analogous deterministic multipath source routing algorithm in the interconnection network Bsw(G)Bsw(G) that finds κ+1\kappa+1 mutually vertex-disjoint paths joining any 22 distinct vertices in Bsw(G)Bsw(G) so that these paths all have length bounded as above. Moreover, our algorithm has time complexity polynomial in Δκ(G)\Delta_\kappa(G), Δ(G)\Delta(G) and κ\kappa. We also show that if GG is Hamiltonian then Bsw(G)Bsw(G) is Hamiltonian, and that if GG is a Cayley graph then Bsw(G)Bsw(G) is a Cayley graph

    From simple to complex networks: inherent structures, barriers and valleys in the context of spin glasses

    Full text link
    Given discrete degrees of freedom (spins) on a graph interacting via an energy function, what can be said about the energy local minima and associated inherent structures? Using the lid algorithm in the context of a spin glass energy function, we investigate the properties of the energy landscape for a variety of graph topologies. First, we find that the multiplicity Ns of the inherent structures generically has a lognormal distribution. In addition, the large volume limit of ln/ differs from unity, except for the Sherrington-Kirkpatrick model. Second, we find simple scaling laws for the growth of the height of the energy barrier between the two degenerate ground states and the size of the associated valleys. For finite connectivity models, changing the topology of the underlying graph does not modify qualitatively the energy landscape, but at the quantitative level the models can differ substantially.Comment: 10 pages, 9 figs, slightly improved presentation, more references, accepted for publication in Phys Rev
    corecore