Abstract

We construct a nearest-neighbour interacting particle system of exclusion type, which illustrates a transition from slow to fast diffusion. More precisely, the hydrodynamic limit of this microscopic system in the diffusive space-time scaling is the parabolic equation ∂tρ=∇(D(ρ)∇ρ)\partial_tρ=\nabla (D(ρ)\nabla ρ), with diffusion coefficient D(ρ)=mρm−1 D(ρ)=mρ^{m-1} where m∈(0,2] m\in(0,2] , including therefore the fast diffusion regime in the range m∈(0,1) m\in(0,1) , and the porous {medium} equation for m∈(1,2) m\in(1,2) . The construction of the model is based on the generalized binomial theorem, and interpolates continuously in m m the already known microscopic porous medium model with parameter m=2 m=2 , the symmetric simple exclusion process with m=1 m=1 , going down to a fast diffusion model up to any m>0 m>0. The derivation of the hydrodynamic limit for the local density of particles on the one-dimensional torus is achieved via the entropy method -- with additional technical difficulties depending on the regime (slow or fast diffusion) and where new properties of the porous medium model need to be derived.

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