Infinite-time concentration in aggregation-diffuse equations with a given potential

Typically, aggregation-diffusion is modeled by parabolic equations that combine linear or nonlinear diffusion with a Fokker-Planck convection term. Under very general suitable assumptions, we prove that radial solutions of the evolution process converge asymptotically in time towards a stationary st...

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Main Authors: Carrillo, JA, Gomez Castro, D, Vázquez, JL
Format: Journal article
Language:English
Published: Elsevier 2021
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author Carrillo, JA
Gomez Castro, D
Vázquez, JL
author_facet Carrillo, JA
Gomez Castro, D
Vázquez, JL
author_sort Carrillo, JA
collection OXFORD
description Typically, aggregation-diffusion is modeled by parabolic equations that combine linear or nonlinear diffusion with a Fokker-Planck convection term. Under very general suitable assumptions, we prove that radial solutions of the evolution process converge asymptotically in time towards a stationary state representing the balance between the two effects. Our parabolic system is the gradient flow of an energy functional, and in fact we show that the stationary states are minimizers of a relaxed energy. Here, we study radial solutions of an aggregation-diffusion model that combines nonlinear fast diffusion with a convection term driven by the gradient of a potential, both in balls and the whole space. We show that, depending on the exponent of fast diffusion and the potential, the steady state is given by the sum of an explicit integrable function, plus a Dirac delta at the origin containing the rest of the mass of the initial datum. This splitting phenomenon is an uncommon example of blow-up in infinite time.
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spelling oxford-uuid:f9c19049-0126-4897-9a4a-40ea61d13de92022-05-16T08:31:16ZInfinite-time concentration in aggregation-diffuse equations with a given potentialJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:f9c19049-0126-4897-9a4a-40ea61d13de9EnglishSymplectic ElementsElsevier2021Carrillo, JAGomez Castro, DVázquez, JLTypically, aggregation-diffusion is modeled by parabolic equations that combine linear or nonlinear diffusion with a Fokker-Planck convection term. Under very general suitable assumptions, we prove that radial solutions of the evolution process converge asymptotically in time towards a stationary state representing the balance between the two effects. Our parabolic system is the gradient flow of an energy functional, and in fact we show that the stationary states are minimizers of a relaxed energy. Here, we study radial solutions of an aggregation-diffusion model that combines nonlinear fast diffusion with a convection term driven by the gradient of a potential, both in balls and the whole space. We show that, depending on the exponent of fast diffusion and the potential, the steady state is given by the sum of an explicit integrable function, plus a Dirac delta at the origin containing the rest of the mass of the initial datum. This splitting phenomenon is an uncommon example of blow-up in infinite time.
spellingShingle Carrillo, JA
Gomez Castro, D
Vázquez, JL
Infinite-time concentration in aggregation-diffuse equations with a given potential
title Infinite-time concentration in aggregation-diffuse equations with a given potential
title_full Infinite-time concentration in aggregation-diffuse equations with a given potential
title_fullStr Infinite-time concentration in aggregation-diffuse equations with a given potential
title_full_unstemmed Infinite-time concentration in aggregation-diffuse equations with a given potential
title_short Infinite-time concentration in aggregation-diffuse equations with a given potential
title_sort infinite time concentration in aggregation diffuse equations with a given potential
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