2018
DOI: 10.1016/j.na.2018.06.016
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Global generalized solutions to a Keller–Segel system with nonlinear diffusion and singular sensitivity

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Cited by 20 publications
(8 citation statements)
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“…Moreover, he took into account asymptotic behavior of solutions to the system (1.5), and proved that v(•, t) * 0 in L ∞ (Ω) and v(•, t) → 0 in L p (Ω) as t → ∞ provided Ω u 0 ≤ m, − Ω ln( v0 v0 L ∞ (Ω) ) ≤ M , where m, M are positive constants. When ∆u is replaced by ∆u m (m ≥ 1), Yan et al [52] showed that if m > 1 + N −2 2N (N ≥ 2), the corresponding Neumann initial-boundary value problem admits a global generalized solution. When v does not stand for a nutrient to be consumed but a signalling substance produced by the bacteria themselves, i.e.…”
Section: Guoqiang Ren and Bin Liumentioning
confidence: 99%
“…Moreover, he took into account asymptotic behavior of solutions to the system (1.5), and proved that v(•, t) * 0 in L ∞ (Ω) and v(•, t) → 0 in L p (Ω) as t → ∞ provided Ω u 0 ≤ m, − Ω ln( v0 v0 L ∞ (Ω) ) ≤ M , where m, M are positive constants. When ∆u is replaced by ∆u m (m ≥ 1), Yan et al [52] showed that if m > 1 + N −2 2N (N ≥ 2), the corresponding Neumann initial-boundary value problem admits a global generalized solution. When v does not stand for a nutrient to be consumed but a signalling substance produced by the bacteria themselves, i.e.…”
Section: Guoqiang Ren and Bin Liumentioning
confidence: 99%
“…No matter biological relevance or mathematical meaning, we find it is worth addressing the basic solvability theory of the model (3). Inspired by the arguments in previous studies [8,13,14,26,27], we mainly investigate the global classical solution in a chemotactic movement with singular sensitivity by two stimuli. eorem 1 partially generalizes and improves previously known ones.…”
Section: Introductionmentioning
confidence: 99%
“…Yan and Li 27 studied the global generalized solutions to () by maximum principle and parabolic regularity theory. The global weak solution to the following chemotaxis system with additional cross‐diffusion {left left leftarrayutarray=·umuv,arrayinΩ,t>0,arrayτvtarray=Δv+δΔ(un)+uv,arrayinΩ,t>0,arrayu(x,0)array=u0(x),v(x,0)=v0(x),arrayinΩ, with no‐flux boundary condition umuv·ν=(v+δun)=0,onΩ,t>0 is proved by Carrillo et al 28 with the help of Alikakos iteration method.…”
Section: Introductionmentioning
confidence: 99%