In this paper, we are concerned with a class of parabolic-elliptic chemotaxis systems encompassing the prototype $$\left\{ \begin{ array}{ lll} &u_t = \nabla\cdot(\nabla u-\chi u\nabla v)+f(u), & x\in \Omega, t>0, \\[0.2cm] &0= \Delta v -v+u^\kappa, & x\in \Omega, t>0 \end{ array}\right. $$ with nonnegative initial condition for $u$ and homogeneous Neumann boundary conditions in a smooth bounded domain $\Omega\subset \mathbb{ R}^n(n\geq 2)$, where $\chi>0$, $\kappa>0$ and $f$ is a smooth growth source satisfying $f(0)\geq 0$ and $$ f(s)\leq a-bs^\theta, \quad s\geq 0, \text{ with some} a\geq 0, b>0, \theta>1. $$ Firstly, it is shown, either $$ \kappa<\frac{ 2}{ n}\quad \& \quad f\equiv 0, $$ or $$\theta>\kappa+1, $$ or $$ \theta-\kappa=1, \ \ b\geq \frac{ (\kappa n-2)}{ \kappa n}\chi, \eqno(*) $$ that the corresponding initial-value problem admits a unique classical solution that is uniformly bounded in space and time. Our proof is elementary and semigroup-free. Whilst, with the particular choices $\theta=2$ and $\kappa=1$, Tello and Winkler \cite{ TW07} use sophisticated estimates via the Neumann heat semigroup to obtain the global boundedness under the strict inequality in ($\ast$). Thereby, we improve their results to the "borderline" case $b=(\kappa n-2)/(\kappa n)\chi$ in this regard. Next, for an unbounded range of $\chi$, the system is shown to exhibit pattern formations, and, the emerging patterns are shown to converge weakly in $ L^\theta(\Omega)$ to some constants as $\chi\rightarrow \infty$. While, for small $\chi$ or large damping $b$, precisely $b>2\chi$ if $f(u)=u(a-bu^\kappa)$ for some $a, b>0$, we show that the system does not admit pattern formation and the large time behavior of solutions is comparable to its associated ODE+algebraic system.
Categories: math.AP