472 research outputs found

    Non-monotonic spontaneous magnetization in a Sznajd-like Consensus Model

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    Ising or Potts models of ferromagnetism have been widely used to describe locally interacting social or economic systems. We consider a related model, introduced by Sznajd to describe the evolution of consensus in a society. In this model, the opinion or state of any spins can only be changed through the influence of neighbouring pairs of similarly aligned spins. Such pairs can polarize their neighbours. We show that, assuming the global dynamics evolve in a synchronous manner, the two-state Sznajd model exhibits a non-monotonically decreasing overall orientation that has a maximum value when the system is subject to a finite value of noise. Reinterpreting the model in terms of opinions within a society we predict that consensus can be increased by the addition of an appropriate amount of random noise. These features are explained by the presence of islands of complete orientation that are stable in the absence of noise but removed via the presence of added noise.Comment: 6 pages, 6 figure

    Phase transitions, memory and frustration in a Sznajd-like model with synchronous updating

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    We introduce a consensus model inspired by the Sznajd Model. The updating is synchronous and memory plays here a decisive role in making possible the reaching of total consensus. We study the phase transition between the state with no-consensus to the state with total consensus.Comment: to be published in the IJMP

    Discontinuous Percolation Transitions in Epidemic Processes, Surface Depinning in Random Media and Hamiltonian Random Graphs

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    Discontinuous percolation transitions and the associated tricritical points are manifest in a wide range of both equilibrium and non-equilibrium cooperative phenomena. To demonstrate this, we present and relate the continuous and first order behaviors in two different classes of models: The first are generalized epidemic processes (GEP) that describe in their spatially embedded version - either on or off a regular lattice - compact or fractal cluster growth in random media at zero temperature. A random graph version of GEP is mapped onto a model previously proposed for complex social contagion. We compute detailed phase diagrams and compare our numerical results at the tricritical point in d = 3 with field theory predictions of Janssen et al. [Phys. Rev. E 70, 026114 (2004)]. The second class consists of exponential ("Hamiltonian", or formally equilibrium) random graph models and includes the Strauss and the 2-star model, where 'chemical potentials' control the densities of links, triangles or 2-stars. When the chemical potentials in either graph model are O(logN), the percolation transition can coincide with a first order phase transition in the density of links, making the former also discontinuous. Hysteresis loops can then be of mixed order, with second order behavior for decreasing link fugacity, and a jump (first order) when it increases

    U.S. Geological Survey (USGS) Circum-Arctic Resource Appraisal: Estimates of Undiscovered Oil and Gas North of the Arctic Circle

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    Using a geology-based probabilistic methodology, the USGS estimated the occurrence of undiscovered oil and gas in 33 geologic provinces thought to be prospective for petroleum. The sum of the mean estimates for each province indicates that 90 billion barrels of oil, 1,669 trillion cubic feet of natural gas, and 44 billion barrels of natural gas liquids may remain to be found in the Arctic, of which approximately 84 percent is expected to occur in offshore areas

    Violating conformal invariance: Two-dimensional clusters grafted to wedges, cones, and branch points of Riemann surfaces

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    We present simulations of 2-d site animals on square and triangular lattices in non-trivial geomeLattice animals are one of the few critical models in statistical mechanics violating conformal invariance. We present here simulations of 2-d site animals on square and triangular lattices in non-trivial geometries. The simulations are done with the newly developed PERM algorithm which gives very precise estimates of the partition sum, yielding precise values for the entropic exponent θ\theta (ZN∼μNN−θZ_N \sim \mu^N N^{-\theta}). In particular, we studied animals grafted to the tips of wedges with a wide range of angles α\alpha, to the tips of cones (wedges with the sides glued together), and to branching points of Riemann surfaces. The latter can either have kk sheets and no boundary, generalizing in this way cones to angles α>360\alpha > 360 degrees, or can have boundaries, generalizing wedges. We find conformal invariance behavior, θ∼1/α\theta \sim 1/\alpha, only for small angles (α≪2π\alpha \ll 2\pi), while θ≈const−α/2π\theta \approx const -\alpha/2\pi for α≫2π\alpha \gg 2\pi. These scalings hold both for wedges and cones. A heuristic (non-conformal) argument for the behavior at large α\alpha is given, and comparison is made with critical percolation.Comment: 4 pages, includes 3 figure

    Economic choices reveal probability distortion in macaque monkeys.

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    Economic choices are largely determined by two principal elements, reward value (utility) and probability. Although nonlinear utility functions have been acknowledged for centuries, nonlinear probability weighting (probability distortion) was only recently recognized as a ubiquitous aspect of real-world choice behavior. Even when outcome probabilities are known and acknowledged, human decision makers often overweight low probability outcomes and underweight high probability outcomes. Whereas recent studies measured utility functions and their corresponding neural correlates in monkeys, it is not known whether monkeys distort probability in a manner similar to humans. Therefore, we investigated economic choices in macaque monkeys for evidence of probability distortion. We trained two monkeys to predict reward from probabilistic gambles with constant outcome values (0.5 ml or nothing). The probability of winning was conveyed using explicit visual cues (sector stimuli). Choices between the gambles revealed that the monkeys used the explicit probability information to make meaningful decisions. Using these cues, we measured probability distortion from choices between the gambles and safe rewards. Parametric modeling of the choices revealed classic probability weighting functions with inverted-S shape. Therefore, the animals overweighted low probability rewards and underweighted high probability rewards. Empirical investigation of the behavior verified that the choices were best explained by a combination of nonlinear value and nonlinear probability distortion. Together, these results suggest that probability distortion may reflect evolutionarily preserved neuronal processing.This work was supported by the Wellcome Trust, European Research Council (ERC) and Caltech Conte Center.This is the final version of the article. It was first published by the Society for Neuroscience at http://www.jneurosci.org/content/35/7/3146.ful

    Large-scale Simulation of the Two-dimensional Kinetic Ising Model

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    We present Monte Carlo simulation results for the dynamical critical exponent zz of the two-dimensional kinetic Ising model using a lattice of size 106×10610^6 \times 10^6 spins. We used Glauber as well as Metropolis dynamics. The zz-value of 2.16±0.0052.16\pm 0.005 was calculated from the magnetization and energy relaxation from an ordered state towards the equilibrium state at TcT_c.Comment: 6 pages + 2 figures as separate uuencoded compressed tar file, Postscipt also available at http://wwwcp.tphys.uni-heidelberg.de/papers

    Pair Connectedness and Shortest Path Scaling in Critical Percolation

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    We present high statistics data on the distribution of shortest path lengths between two near-by points on the same cluster at the percolation threshold. Our data are based on a new and very efficient algorithm. For d=2d=2 they clearly disprove a recent conjecture by M. Porto et al., Phys. Rev. {\bf E 58}, R5205 (1998). Our data also provide upper bounds on the probability that two near-by points are on different infinite clusters.Comment: 7 pages, including 4 postscript figure

    Random Sequential Renormalization of Networks I: Application to Critical Trees

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    We introduce the concept of Random Sequential Renormalization (RSR) for arbitrary networks. RSR is a graph renormalization procedure that locally aggregates nodes to produce a coarse grained network. It is analogous to the (quasi-)parallel renormalization schemes introduced by C. Song {\it et al.} (Nature {\bf 433}, 392 (2005)) and studied more recently by F. Radicchi {\it et al.} (Phys. Rev. Lett. {\bf 101}, 148701 (2008)), but much simpler and easier to implement. In this first paper we apply RSR to critical trees and derive analytical results consistent with numerical simulations. Critical trees exhibit three regimes in their evolution under RSR: (i) An initial regime N0ν≲N<N0N_0^{\nu}\lesssim N<N_0, where NN is the number of nodes at some step in the renormalization and N0N_0 is the initial size. RSR in this regime is described by a mean field theory and fluctuations from one realization to another are small. The exponent ν=1/2\nu=1/2 is derived using random walk arguments. The degree distribution becomes broader under successive renormalization -- reaching a power law, pk∼1/kγp_k\sim 1/k^{\gamma} with γ=2\gamma=2 and a variance that diverges as N01/2N_0^{1/2} at the end of this regime. Both of these results are derived based on a scaling theory. (ii) An intermediate regime for N01/4≲N≲N01/2N_0^{1/4}\lesssim N \lesssim N_0^{1/2}, in which hubs develop, and fluctuations between different realizations of the RSR are large. Crossover functions exhibiting finite size scaling, in the critical region N∼N01/2→∞N\sim N_0^{1/2} \to \infty, connect the behaviors in the first two regimes. (iii) The last regime, for 1≪N≲N01/41 \ll N\lesssim N_0^{1/4}, is characterized by the appearance of star configurations with a central hub surrounded by many leaves. The distribution of sizes where stars first form is found numerically to be a power law up to a cutoff that scales as N0νstarN_0^{\nu_{star}} with νstar≈1/4\nu_{star}\approx 1/4
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