237 research outputs found

    Organized versus self-organized criticality in the abelian sandpile model

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    We define stabilizability of an infinite volume height configuration and of a probability measure on height configurations. We show that for high enough densities, a probability measure cannot be stabilized. We also show that in some sense the thermodynamic limit of the uniform measures on the recurrent configurations of the abelian sandpile model (ASM) is a maximal element of the set of stabilizable measures. In that sense the self-organized critical behavior of the ASM can be understood in terms of an ordinary transition between stabilizable and non-stabilizableComment: 17 pages, appeared in Markov Processes and Related Fields 200

    Loss without recovery of Gibbsianness during diffusion of continuous spins

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    We consider a specific continuous-spin Gibbs distribution μt=0\mu_{t=0} for a double-well potential that allows for ferromagnetic ordering. We study the time-evolution of this initial measure under independent diffusions. For `high temperature' initial measures we prove that the time-evoved measure μt\mu_{t} is Gibbsian for all tt. For `low temperature' initial measures we prove that μt\mu_t stays Gibbsian for small enough times tt, but loses its Gibbsian character for large enough tt. In contrast to the analogous situation for discrete-spin Gibbs measures, there is no recovery of the Gibbs property for large tt in the presence of a non-vanishing external magnetic field. All of our results hold for any dimension d2d\geq 2. This example suggests more generally that time-evolved continuous-spin models tend to be non-Gibbsian more easily than their discrete-spin counterparts

    Large deviations for quantum spin systems

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    We consider high temperature KMS states for quantum spin systems on a lattice. We prove a large deviation principle for the distribution of empirical averages 1ΛiΛXi\frac{1}{|\Lambda|} \sum_{i\in\Lambda} X_i, where the XiX_i's are copies of a self-adjoint element XX (level one large deviations). From the analyticity of the generating function, we obtain the central limit theorem. We generalize to a level two large deviation principle for the distribution of 1ΛiΛδXi\frac{1}{|\Lambda|}\sum_{i\in\Lambda} \delta_{X_i}.Comment: 22 page

    Testing the irreversibility of a Gibbsian process via hitting and return times

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    We introduce estimators for the entropy production of a Gibbsian process based on the observation of a single or two typical trajectories. These estimators are built with adequate hitting and return times. We then study their convergence and fluctuation properties. This provides statisticals test for the irreversibility of Gibbsian processes.Comment: 16 pages; Corrected version; To appear in Nonlinearit

    Matching with shift for one-dimensional Gibbs measures

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    We consider matching with shifts for Gibbsian sequences. We prove that the maximal overlap behaves as clognc\log n, where cc is explicitly identified in terms of the thermodynamic quantities (pressure) of the underlying potential. Our approach is based on the analysis of the first and second moment of the number of overlaps of a given size. We treat both the case of equal sequences (and nonzero shifts) and independent sequences.Comment: Published in at http://dx.doi.org/10.1214/08-AAP588 the Annals of Applied Probability (http://www.imstat.org/aap/) by the Institute of Mathematical Statistics (http://www.imstat.org

    Freezing transitions in non-Fellerian particle systems

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    Non-Fellerian processes show phenomena that are unseen in standard interacting particle systems. We consider freezing transitions in one-dimensional non-Fellerian processes which are built from the abelian sandpile additions to which in one case, spin flips are added, and in another case, the so called anti-sandpile subtractions. In the first case and as a function of the sandpile addition rate, there is a sharp transition from a non-trivial invariant measure to the invariant measure of the sandpile process. For the combination sandpile plus anti-sandpile, there is a sharp transition from one frozen state to the other anti-stat
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