2008
DOI: 10.1214/ejp.v13-591
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Random walks and exclusion processes among random conductances on random infinite clusters: homogenization and hydrodynamic limit

Abstract: We consider a stationary and ergodic random field {ω(b) : b ∈ E d } parameterized by the family of bonds in Z d , d2. The random variable ω(b) is thought of as the conductance of bond b and it ranges in a finite interval [0, c0]. Assuming that the set of bonds with positive conductance has a unique infinite cluster C(ω), we prove homogenization results for the random walk among random conductances on C(ω). As a byproduct, applying the general criterion of [F] leading to the hydrodynamic limit of exclusion proc… Show more

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Cited by 36 publications
(70 citation statements)
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“…[DNS18]. Notice that in the nearest-neighbor percolation setting, similar homogenization results have also been obtained by Faggionato in [Fag08] under the additional assumption that the conductances are bounded from above.…”
Section: Resultssupporting
confidence: 74%
“…[DNS18]. Notice that in the nearest-neighbor percolation setting, similar homogenization results have also been obtained by Faggionato in [Fag08] under the additional assumption that the conductances are bounded from above.…”
Section: Resultssupporting
confidence: 74%
“…In this Section we recall some notation and results of [5,12,14]. Denote by T d = (R/Z) d = [0, 1) d the d-dimensional torus and fix a function W : R d → R such that (1) W (x 1 , . .…”
Section: W -Sobolev Spacementioning
confidence: 99%
“…Recently, the formal adjoint operator (d/dx)(d/dW ) and some non-linear versions were obtained as scaling limits of interacting particle systems in inhomogeneous media. They may model diffusions with permeable membranes at the points of the discontinuities of W , see [1,5,7,2,14] for further details. In [14], for instance, the author introduces an extension of the formal adjoint operator to higher dimensions and provides some results regarding this extension.…”
Section: Introductionmentioning
confidence: 99%
“…The second term on the left-hand side of the previous inequality is composed by a sum of positive parts. We can restrict this for any m ≤ n. By using (8) and the variational formula (24) for the Dirichlet form, we get that, for any function φ ∈ C 1 0 (Ω) and any functions ψ j ∈ F , j ∈ {−m, . .…”
Section: Cédric Bernardinmentioning
confidence: 99%