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Approaching optimality in blow-up results for Keller–Segel systems with logistic-type dampening
Nonlinear Differential Equations and Applications (NoDEA) ( IF 1.2 ) Pub Date : 2021-02-27 , DOI: 10.1007/s00030-021-00677-9
Mario Fuest

Nonnegative solutions of the Neumann initial-boundary value problem for the chemotaxis system

in smooth bounded domains \(\Omega \subset {\mathbb {R}}^n\), \(n \ge 1\), are known to be global in time if \(\lambda \ge 0\), \(\mu > 0\) and \(\kappa > 2\). In the present work, we show that the exponent \(\kappa = 2\) is actually critical in the four- and higher dimensional setting. More precisely, if

$$\begin{aligned} \qquad n&\ge 4,&\quad \kappa \in (1, 2) \quad&\text {and} \quad \mu > 0 \\ \text {or}\qquad n&\ge 5,&\quad \kappa = 2 \quad&\text {and} \quad \mu \in \left( 0, \frac{n-4}{n}\right) , \end{aligned}$$

for balls \(\Omega \subset {\mathbb {R}}^n\) and parameters \(\lambda \ge 0\), \(m_0 > 0\), we construct a nonnegative initial datum \(u_0 \in C^0({{\overline{\Omega }}})\) with \(\int \nolimits _\Omega u_0 = m_0\) for which the corresponding solution (uv) of (\(\star \)) blows up in finite time. Moreover, in 3D, we obtain finite-time blow-up for \(\kappa \in (1, \frac{3}{2})\) (and \(\lambda \ge 0\), \(\mu > 0\)). As the corner stone of our analysis, for certain initial data, we prove that the mass accumulation function \(w(s, t) = \int \nolimits _0^{\root n \of {s}} \rho ^{n-1} u(\rho , t) \,\mathrm {d}\rho \) fulfills the estimate \(w_s \le \frac{w}{s}\). Using this information, we then obtain finite-time blow-up of u by showing that for suitably chosen initial data, \(s_0\) and \(\gamma \), the function \(\phi (t) = \int \nolimits _0^{s_0} s^{-\gamma } (s_0 - s) w(s, t)\) cannot exist globally.



中文翻译:

具有逻辑型阻尼的Keller-Segel系统的爆破结果接近最优

趋化系统的Neumann初边值问题的非负解

在平滑有界区域\(\欧米茄\子集{\ mathbb {R}} ^ N \) \(N \ GE 1 \) ,已知是全球时间如果\(\拉姆达\ GE 0 \) \ (\ mu> 0 \)\(\ kappa> 2 \)。在当前的工作中,我们表明指数\(\ kappa = 2 \)实际上在四维和更高维设置中至关重要。更确切地说,如果

$$ \ begin {aligned} \ qquad n&\ ge 4,&\ quad \ kappa \ in(1、2)\ quad&\ text {and} \ quad \ mu> 0 \\ \ text {or} \ qquad n&\ ge 5,&\ quad \ kappa = 2 \ quad&\ text {and} \ quad \ mu \ in \ left(0,\ frac {n-4} {n} \ right),\ end {aligned} $$

对于球\(\ Omega \ subset {\ mathbb {R}} ^ n \)和参数\(\ lambda \ ge 0 \)\(m_0> 0 \),我们构造了一个非负初始基准\(u_0 \ in C 1-4 0({{\划线{\欧米茄}}})\)\(\ INT \ nolimits _ \欧米茄U_0 = M_0 \)的量,相应溶液(Û,  v)的(\(\星\))在限定时间内爆炸。而且,在3D中,我们获得\(\ kappa \ in(1,\ frac {3} {2})\)()和\(\ lambda \ ge 0 \)\(\ mu > 0 \))。作为我们分析的基石,对于某些初始数据,我们证明了质量累积函数\(w(s,t)= \ int \ nolimits _0 ^ {\ root n \ of {s}} \ rho ^ {n-1} u(\ rho,t)\,\ mathrm {d} \ rho \ )满足估算值\(w_s \ le \ frac {w} {s} \)。使用该信息,我们然后得到有限时间吹胀的ù通过表明对于适当选择的初始数据,\(S_0 \)\(\伽马\) ,函数\(\披(T)= \ INT \ nolimits _0 ^ {s_0} s ^ {-\ gamma}(s_0-s w(s,t)\)不能全局存在。

更新日期:2021-02-28
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