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Global renormalized solutions to reaction-cross-diffusion systems
Analysis of PDEs · Submitted 4 Nov 2017
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The global-in-time existence of renormalized solutions to reaction-cross-diffu-sion systems for an arbitrary number of variables in bounded domains with no-flux boundary conditions is proved.
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The abstract, sentence by sentence
The global-in-time existence of renormalized solutions to reaction-cross-diffu-sion systems for an arbitrary number of variables in bounded domains with no-flux boundary conditions is proved. The cross-diffusion part describes the segregation of population species and is a generalization of the Shigesada-Kawasaki-Teramoto model. The diffusion matrix is not diagonal and generally neither symmetric nor positive semi-definite, but the system possesses a formal gradient-flow or entropy structure. The reaction part includes reversible reactions of mass-action kinetics and does not obey any growth condition. The existence result generalizes both the condition on the reaction part required in the boundedness-by-entropy method and the proof of J. Fischer for reaction-diffusion systems with diagonal diffusion matrices.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The global-in-time existence of renormalized solutions to reaction-cross-diffu-sion systems for an arbitrary number of variables in bounded domains with no-flux boundary conditions is proved. | result 0.91 | 0.94 | 0.96 | asserted 1.00 |
| s1 | The cross-diffusion part describes the segregation of population species and is a generalization of the Shigesada-Kawasaki-Teramoto model. | background 0.93 | 0.15 | 0.03 | asserted 1.00 |
| s2 | The diffusion matrix is not diagonal and generally neither symmetric nor positive semi-definite, but the system possesses a formal gradient-flow or entropy structure. | background 0.72 | 0.39 | 0.03 | asserted 0.99 |
| s3 | The reaction part includes reversible reactions of mass-action kinetics and does not obey any growth condition. | contribution 0.55 | 0.46 | 0.03 | asserted 1.00 |
| s4 | The existence result generalizes both the condition on the reaction part required in the boundedness-by-entropy method and the proof of J. Fischer for reaction-diffusion systems with diagonal diffusion matrices. | contribution 0.55 | 0.81 | 0.10 | asserted 1.00 |
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The paper
Original abstract
The global-in-time existence of renormalized solutions to reaction-cross-diffu-sion systems for an arbitrary number of variables in bounded domains with no-flux boundary conditions is proved. The cross-diffusion part describes the segregation of population species and is a generalization of the Shigesada-Kawasaki-Teramoto model. The diffusion matrix is not diagonal and generally neither symmetric nor positive semi-definite, but the system possesses a formal gradient-flow or entropy structure. The reaction part includes reversible reactions of mass-action kinetics and does not obey any growth condition. The existence result generalizes both the condition on the reaction part required in the boundedness-by-entropy method and the proof of J. Fischer for reaction-diffusion systems with diagonal diffusion matrices.
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How the literature uses it
2 arXiv papers cite this in 9 sentences
Papers citing it · 5 sentences without a confident label
Builds on it 1 paper
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This paper is a continuation of our work [ref] , in which we proved the global existence of renormalized solutions to a class of reaction-cross-diffusion systems describing the evolution of population species.
Weak-strong uniqueness of renormalized solutions to reaction-cross-diffusion systems · Introduction · 0.92
Uses its method or tool 2 papers
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Then we can compute [equation] By choosing $ψ= 1$ , or more precisely a smooth version of $1$ with compact support in $[0,T-δ]$ then let $δ→0$ (see [ref] for more details) in the definition of the renormalized solutions, we get [equation] Our first goal now is to pass to the limit $η→0$ in [ref].
Trend to equilibrium of renormalized solutions to reaction-cross-diffusion systems · Proof of the main result · 0.89
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The proof of the lemma is the same as in step 1 of the proof of Lemma 11 in [ref] .
Weak-strong uniqueness of renormalized solutions to reaction-cross-diffusion systems · Some auxiliary results · 0.99
Compares with it 1 paper
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Also note that in [ref] the detailed balance diffusion condition was $π_i a_ij = π_j a_ji$ for some positive constants $π_i>0$.
Trend to equilibrium of renormalized solutions to reaction-cross-diffusion systems · Introduction · 0.86
What it cites · 7 sentences without a confident label
Uses the method or tool of 1 paper
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In this paper, we combine the entropy method used in [ref] and the concept of renormalized solutions of [ref] .
Global existence analysis of cross-diffusion population systems for multiple species · Introduction · 0.97
Cites as background 1 paper
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Let us briefly comment on conditions [ref] and [ref]; for details, we refer to [ref] .
Global existence analysis of cross-diffusion population systems for multiple species · Introduction · 0.95
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