2008
DOI: 10.4310/cms.2008.v6.n2.a8
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The parabolic-parabolic Keller-Segel model in R2

Abstract: Abstract. This paper is devoted mainly to the global existence problem for the two-dimensional parabolic-parabolic Keller-Segel system in the full space. We derive a critical mass threshold below which global existence is ensured. Carefully using energy methods and ad hoc functional inequalities, we improve and extend previous results in this direction. The given threshold is thought to be the optimal criterion, but this question is still open. This global existence result is accompanied by a detailed discussi… Show more

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Cited by 167 publications
(186 citation statements)
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References 26 publications
(47 reference statements)
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“…For τ > 0, according to [7], solutions globally exist for any M < 8 π. However, it has not yet been proved that explosion occurs in finite time as soon as M > 8 π, for instance under some additional assumptions like a smallness condition on R R 2 |x| 2 n 0 (x) dx.…”
Section: Introductionmentioning
confidence: 99%
“…For τ > 0, according to [7], solutions globally exist for any M < 8 π. However, it has not yet been proved that explosion occurs in finite time as soon as M > 8 π, for instance under some additional assumptions like a smallness condition on R R 2 |x| 2 n 0 (x) dx.…”
Section: Introductionmentioning
confidence: 99%
“…This macroscopic model has been investigated by many authors (e.g. see [2,6,11,18]). If one looks at the kinetic level, a good model is the so-called Othmar-Dunbar-Alt system [20] which is based on velocity-jump processes and leads to the transport equation (1.2) for v ∈ V ⊂ R d where f (t, x, v) denotes the cellular density.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…There are many choices for the evolution of the chemoattractant, one of them is to use a parabolic diffusion equation, (e.g. see [6,8,10,11,17,21])…”
Section: T [S](t X V → V) = χ[V · ∇S(t X)] + mentioning
confidence: 99%
“…For mass greater than 8π , solutions blowup (under an additional assumption on the second moment [10 …”
Section: Resultsmentioning
confidence: 99%
“…Since much attention has been paid to the blowup problems for this system, recall that 8π is the critical value of initial mass ( u 0 (x) dx) for the existence problem. Namely, below this value, one can construct global solutions to the problem while for mass above 8π (with the second momentum |x| 2 u 0 (x)dx small enough, i.e., smaller than the value of g(M)-a monotone increasing function of mass M), the blowup occurs (see [10,Theorem 1.2…”
Section: )mentioning
confidence: 99%