113,488 research outputs found

    On cost-effective communication network designing

    Full text link
    How to efficiently design a communication network is a paramount task for network designing and engineering. It is, however, not a single objective optimization process as perceived by most previous researches, i.e., to maximize its transmission capacity, but a multi-objective optimization process, with lowering its cost to be another important objective. These two objectives are often contradictive in that optimizing one objective may deteriorate the other. After a deep investigation of the impact that network topology, node capability scheme and routing algorithm as well as their interplays have on the two objectives, this letter presents a systematic approach to achieve a cost-effective design by carefully choosing the three designing aspects. Only when routing algorithm and node capability scheme are elegantly chosen can BA-like scale-free networks have the potential of achieving good tradeoff between the two objectives. Random networks, on the other hand, have the built-in character for a cost-effective design, especially when other aspects cannot be determined beforehand.Comment: 6 pages, 4 figure

    Branching Ratio and CP Asymmetry of B_s \to K^*_0(1430)\pi Decays in the PQCD Approach

    Full text link
    In the two-quark model supposition for K0βˆ—(1430)K_0^{*}(1430), the branching ratios and the direct CP-violating asymmetries for decays BΛ‰s0β†’K0βˆ—0(1430)Ο€0,K0βˆ—+(1430)Ο€βˆ’\bar B_s^0\to K^{*0}_0(1430)\pi^0, K^{*+}_0(1430)\pi^- are studied by employing the perturbative QCD factorization approach. We find that although these two decays are both tree-dominated, the ratio of their penguin to tree contributions are very different: there is only a few percent for the decay BΛ‰s0β†’K0βˆ—+(1430)Ο€βˆ’\bar B_s^0\to K^{*+}_0(1430)\pi^-, while about 37% in scenario I, even 51% in scenario II for the decay BΛ‰s0β†’K0βˆ—0(1430)Ο€0\bar B_s^0\to K^{*0}_0(1430)\pi^0. It results that these two decays have very different values in the branching ratios and the direct CP asymmetries. The branching ratio of the decay BΛ‰s0β†’K0βˆ—+(1430)Ο€βˆ’\bar B_s^0\to K^{*+}_0(1430)\pi^- is at the order of 10βˆ’510^{-5}, and its direct CP asymmetry is about (20-30)%. While for the decay BΛ‰s0β†’K0βˆ—0(1430)Ο€0\bar B_s^0\to K^{*0}_0(1430)\pi^0, its direct CP-violating asymmetry is very large and about 90%, but it is difficult to measure it, because the branching ratio for this channel is small and only 10βˆ’710^{-7} order.Comment: 8pages, 2figure

    Evaluation of the EMC environment generated by a static var compensator

    Get PDF
    Describes an evaluation of the EMC environment generated by a static var compensator
    • …
    corecore