1,668 research outputs found

    Ensuring Trust in One Time Exchanges: Solving the QoS Problem

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    We describe a pricing structure for the provision of IT services that ensures trust without requiring repeated interactions between service providers and users. It does so by offering a pricing structure that elicits truthful reporting of quality of service (QoS) by providers while making them profitable. This mechanism also induces truth-telling on the part of users reserving the service

    Novel Si(1-x)Ge(x)/Si heterojunction internal photoemission long wavelength infrared detectors

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    There is a major need for long-wavelength-infrared (LWIR) detector arrays in the range of 8 to 16 microns which operate with close-cycle cryocoolers above 65 K. In addition, it would be very attractive to have Si-based infrared (IR) detectors that can be easily integrated with Si readout circuitry and have good pixel-to-pixel uniformity, which is critical for focal plane array (FPA) applications. Here, researchers report a novel Si(1-x)Ge(x)/Si heterojunction internal photoemission (HIP) detector approach with a tailorable long wavelength infrared cutoff wavelength, based on internal photoemission over the Si(1-x)Ge(x)/Si heterojunction. The HIP detectors were grown by molecular beam epitaxy (MBE), which allows one to optimize the device structure with precise control of doping profiles, layer thickness and composition. The feasibility of a novel Si(1-x)Ge(x)/Si HIP detector has been demonstrated with tailorable cutoff wavelength in the LWIR region. Photoresponse at wavelengths 2 to 10 microns are obtained with quantum efficiency (QE) above approx. 1 percent in these non-optimized device structures. It should be possible to significantly improve the QE of the HIP detectors by optimizing the thickness, composition, and doping concentration of the Si(1-x)Ge(x) layers and by configuring the detector for maximum absorption such as the use of a cavity structure. With optimization of the QE and by matching the barrier energy to the desired wavelength cutoff to minimize the thermionic current, researchers predict near background limited performance in the LWIR region with operating temperatures above 65K. Finally, with mature Si processing, the relatively simple device structure offers potential for low-cost producible arrays with excellent uniformity

    Properties of weighted complex networks

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    We study two kinds of weighted networks, weighted small-world (WSW) and weighted scale-free (WSF). The weight wijw_{ij} of a link between nodes ii and jj in the network is defined as the product of endpoint node degrees; that is wij=(kikj)θw_{ij}=(k_{i}k_{j})^{\theta}. In contrast to adding weights to links during networks being constructed, we only consider weights depending on the `` popularity\rq\rq of the nodes represented by their connectivity. It was found that the both weighted networks have broad distributions on characterization the link weight, vertex strength, and average shortest path length. Furthermore, as a survey of the model, the epidemic spreading process in both weighted networks was studied based on the standard \emph{susceptible-infected} (SI) model. The spreading velocity reaches a peak very quickly after the infection outbreaks and an exponential decay was found in the long time propagation.Comment: 14 pages, 5 figure

    Log-Networks

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    We introduce a growing network model in which a new node attaches to a randomly-selected node, as well as to all ancestors of the target node. This mechanism produces a sparse, ultra-small network where the average node degree grows logarithmically with network size while the network diameter equals 2. We determine basic geometrical network properties, such as the size dependence of the number of links and the in- and out-degree distributions. We also compare our predictions with real networks where the node degree also grows slowly with time -- the Internet and the citation network of all Physical Review papers.Comment: 7 pages, 6 figures, 2-column revtex4 format. Version 2: minor changes in response to referee comments and to another proofreading; final version for PR

    Effect of the accelerating growth of communications networks on their structure

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    Motivated by data on the evolution of the Internet and World Wide Web we consider scenarios of self-organization of the nonlinearly growing networks into free-scale structures. We find that the accelerating growth of the networks establishes their structure. For the growing networks with preferential linking and increasing density of links, two scenarios are possible. In one of them, the value of the exponent γ\gamma of the connectivity distribution is between 3/2 and 2. In the other, γ>2\gamma>2 and the distribution is necessarily non-stationary.Comment: 4 pages revtex, 3 figure

    Scaling Behaviour of Developing and Decaying Networks

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    We find that a wide class of developing and decaying networks has scaling properties similar to those that were recently observed by Barab\'{a}si and Albert in the particular case of growing networks. The networks considered here evolve according to the following rules: (i) Each instant a new site is added, the probability of its connection to old sites is proportional to their connectivities. (ii) In addition, (a) new links between some old sites appear with probability proportional to the product of their connectivities or (b) some links between old sites are removed with equal probability.Comment: 7 pages (revtex

    Effects of aging and links removal on epidemic dynamics in scale-free networks

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    We study the combined effects of aging and links removal on epidemic dynamics in the Barab\'{a}si-Albert scale-free networks. The epidemic is described by a susceptible-infected-refractory (SIR) model. The aging effect of a node introduced at time tit_{i} is described by an aging factor of the form (t−ti)−β(t-t_{i})^{-\beta} in the probability of being connected to newly added nodes in a growing network under the preferential attachment scheme based on popularity of the existing nodes. SIR dynamics is studied in networks with a fraction 1−p1-p of the links removed. Extensive numerical simulations reveal that there exists a threshold pcp_{c} such that for p≥pcp \geq p_{c}, epidemic breaks out in the network. For p<pcp < p_{c}, only a local spread results. The dependence of pcp_{c} on β\beta is studied in detail. The function pc(β)p_{c}(\beta) separates the space formed by β\beta and pp into regions corresponding to local and global spreads, respectively.Comment: 8 pages, 3 figures, revtex, corrected Ref.[11

    Maximum flow and topological structure of complex networks

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    The problem of sending the maximum amount of flow qq between two arbitrary nodes ss and tt of complex networks along links with unit capacity is studied, which is equivalent to determining the number of link-disjoint paths between ss and tt. The average of qq over all node pairs with smaller degree kmink_{\rm min} is kmin≃ckmin_{k_{\rm min}} \simeq c k_{\rm min} for large kmink_{\rm min} with cc a constant implying that the statistics of qq is related to the degree distribution of the network. The disjoint paths between hub nodes are found to be distributed among the links belonging to the same edge-biconnected component, and qq can be estimated by the number of pairs of edge-biconnected links incident to the start and terminal node. The relative size of the giant edge-biconnected component of a network approximates to the coefficient cc. The applicability of our results to real world networks is tested for the Internet at the autonomous system level.Comment: 7 pages, 4 figure

    Structure of Growing Networks: Exact Solution of the Barabasi--Albert's Model

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    We generalize the Barab\'{a}si--Albert's model of growing networks accounting for initial properties of sites and find exactly the distribution of connectivities of the network P(q)P(q) and the averaged connectivity qˉ(s,t)\bar{q}(s,t) of a site ss in the instant tt (one site is added per unit of time). At long times P(q)∼q−γP(q) \sim q^{-\gamma} at q→∞q \to \infty and qˉ(s,t)∼(s/t)−β\bar{q}(s,t) \sim (s/t)^{-\beta} at s/t→0s/t \to 0, where the exponent γ\gamma varies from 2 to ∞\infty depending on the initial attractiveness of sites. We show that the relation β(γ−1)=1\beta(\gamma-1)=1 between the exponents is universal.Comment: 4 pages revtex (twocolumn, psfig), 1 figur
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