1,657 research outputs found

    The partially asymmetric zero range process with quenched disorder

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    We consider the one-dimensional partially asymmetric zero range process where the hopping rates as well as the easy direction of hopping are random variables. For this type of disorder there is a condensation phenomena in the thermodynamic limit: the particles typically occupy one single site and the fraction of particles outside the condensate is vanishing. We use extreme value statistics and an asymptotically exact strong disorder renormalization group method to explore the properties of the steady state. In a finite system of LL sites the current vanishes as J∼L−zJ \sim L^{-z}, where the dynamical exponent, zz, is exactly calculated. For 0<z<10<z<1 the transport is realized by Na∼L1−zN_a \sim L^{1-z} active particles, which move with a constant velocity, whereas for z>1z>1 the transport is due to the anomalous diffusion of a single Brownian particle. Inactive particles are localized at a second special site and their number in rare realizations is macroscopic. The average density profile of inactive particles has a width of, ξ∼δ−2\xi \sim \delta^{-2}, in terms of the asymmetry parameter, δ\delta. In addition to this, we have investigated the approach to the steady state of the system through a coarsening process and found that the size of the condensate grows as nL∼t1/(1+z)n_L \sim t^{1/(1+z)} for large times. For the unbiased model zz is formally infinite and the coarsening is logarithmically slow.Comment: 12 pages, 9 figure

    Adsorption energies of NH 3

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    Inelastic neutron scattering study of NH4Y zeolites

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    Dynamics of an exclusion process with creation and annihilation

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    We examine the dynamical properties of an exclusion process with creation and annihilation of particles in the framework of a phenomenological domain-wall theory, by scaling arguments and by numerical simulation. We find that the length- and time scale are finite in the maximum current phase for finite creation- and annihilation rates as opposed to the algebraically decaying correlations of the totally asymmetric simple exclusion process (TASEP). Critical exponents of the transition to the TASEP are determined. The case where bulk creation- and annihilation rates vanish faster than the inverse of the system size N is also analyzed. We point out that shock localization is possible even for rates proportional to 1/N^a, 1<a<2.Comment: 16 pages, 8 figures, typos corrected, references added, section 4 revise
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