1,720,971 research outputs found

    Quantum Methods for Interacting Particle Systems II, Glauber Dynamics for Ising Spin Systems

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    Using the formalism and the results described in [QMPS I] and in [QMPS III], we discuss the approach to termodynamic equilibrium for discrete spin systems in a framework that generalizes the one originally proposed by R. Glauber. Ergodicity for the process is proved by providing a lower bound extimate for their exponetial rate of convergence to equilibrium, in the high temperature regime. We give application to some (not necessarily ferromagnetic ) Ising-spin models. These results also gives an upper bound for the critical temperature of the d-dimensional Ising model, which in dimension two coincides with the real critical value calculated by the static approach

    Speed of Parallel Processing for Random Task Graphs

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    The random graph model of parallel computation introduced by Gelenbe et al. depends on three parameters: n, the number of tasks (vertices); F, the common distribution of Ti,. . . , T,, the task processing times, and p = p,, the probability for a given i < j that task i must be completed before task j is started. The total processing time is R,,, the maximum sum of T,’s along directed paths of the graph. We study the large n behavior of Rn when np,, grows sublinearly but superlogarithmically, the regime where the longest directed path contains about enp,, tasks. For an exponential (mean one) F, we prove that R,, is about 4np,. The “discrepancy” between 4 and e is a large deviation effect. Related results are obtained when np,, grows exactly logarithmically and when F is not exponential, but has a tail which decays (at least) exponentially fast

    On some features of quadratic unconstrained binary optimization with random coefficients

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    Quadratic Unconstrained Binary Optimization (QUBO or UBQP) is concerned with maximizing/minimizing the quadratic form H(J,eta)=W & sum;(i,j)J(i,j)eta(i)eta(j )with J a matrix of coefficients, eta is an element of {0,1}(N) and W a normalizing constant. In the statistical mechanics literature, QUBO is a lattice gas counterpart to the (generalized) Sherrington-Kirkpatrick spin glass model. Finding the optima of H is an NP-hard problem. Several problems in combinatorial optimization and data analysis can be mapped to QUBO in a straightforward manner. In the combinatorial optimization literature, random instances of QUBO are often used to test the effectiveness of heuristic algorithms. Here we consider QUBO with random independent coefficients and show that if the J(i,j)'s have zero mean and finite variance then, after proper normalization, the minimum and maximum per particle of H do not depend on the details of the distribution of the couplings and are concentrated around their expected values. Further, with the help of numerical simulations, we study the minimum and maximum of the objective function and provide some insight into the structure of the minimizer and the maximizer of H. We argue that also this structure is rather robust. Our findings hold also in the diluted case where each of the J(i,j)'s is allowed to be zero with probability going to 1 as N ->infinity in a suitable way

    On the Implications of the OFF Period Distribution in two-State Traffic Models

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    The goal of the letter is to highlight the impact of the inactive period distribution of an ON–OFF source on the autocor relation structure of the model. In particular, two discrete-time ON–OFF models, both with geometric distribution of the active period, are considered: the GeoGeo Model (GGM) and the ParetoGeo Model (PGM), characterized by a geometric and Pareto-like distribution of the OFF periods length, respectively. The two models are compared in terms of their main statistical features as well as queueing impact. The asymptotic behavior of the autocorrelation function for the proposed PGM has been analytically evaluated. It is shown it has a hyperbolic decay related to the tail behavior of the OFF periods distribution
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