877 research outputs found

    Hydrodynamic limit of asymmetric exclusion processes under diffusive scaling in d3d\ge 3

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    We consider the asymmetric exclusion process. We start from a profile which is constant along the drift direction and prove that the density profile, under a diffusive rescaling of time, converges to the solution of a parabolic equation

    Gaussian estimates for symmetric simple exclusion processes

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    We prove Gaussian tail estimates for the transition probability of nn particles evolving as symmetric exclusion processes on \bb Z^d, improving results obtained in \cite{l}. We derive from this result a non-equilibrium Boltzmann-Gibbs principle for the symmetric simple exclusion process in dimension 1 starting from a product measure with slowly varying parameter

    Coupled dark energy: a dynamical analysis with complex scalar field

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    The dynamical analysis for coupled dark energy with dark matter is presented, where a complex scalar field is taken into account and it is considered in the presence of a barothropic fluid. We consider three dark energy candidates: quintessence, phantom and tachyon. The critical points are found and their stabilities analyzed, leading to the three cosmological eras (radiation, matter and dark energy), for a generic potential. The results presented here enlarge the previous analyses found in the literature.Comment: 9 pages, version accepted for publication in EPJC. arXiv admin note: text overlap with arXiv:1505.0324

    Metastability of finite state Markov chains: a recursive procedure to identify slow variables for model reduction

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    Consider a sequence (ηN(t):t0)(\eta^N(t) :t\ge 0) of continuous-time, irreducible Markov chains evolving on a fixed finite set EE, indexed by a parameter NN. Denote by RN(η,ξ)R_N(\eta,\xi) the jump rates of the Markov chain ηtN\eta^N_t, and assume that for any pair of bonds (η,ξ)(\eta,\xi), (η,ξ)(\eta',\xi') arctan{RN(η,ξ)/RN(η,ξ)}\arctan \{R_N(\eta,\xi)/R_N(\eta',\xi')\} converges as NN\uparrow\infty. Under a hypothesis slightly more restrictive (cf. \eqref{mhyp} below), we present a recursive procedure which provides a sequence of increasing time-scales \theta^1_N, \dots, \theta^{\mf p}_N, θNjθNj+1\theta^j_N \ll \theta^{j+1}_N, and of coarsening partitions \{\ms E^j_1, \dots, \ms E^j_{\mf n_j}, \Delta^j\}, 1\le j\le \mf p, of the set EE. Let \phi_j: E \to \{0,1, \dots, \mf n_j\} be the projection defined by \phi_j(\eta) = \sum_{x=1}^{\mf n_j} x \, \mb 1\{\eta \in \ms E^j_x\}. For each 1\le j\le \mf p, we prove that the hidden Markov chain XNj(t)=ϕj(ηN(tθNj))X^j_N(t) = \phi_j(\eta^N(t\theta^j_N)) converges to a Markov chain on \{1, \dots, \mf n_j\}
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