Persistence and spreading speeds of parabolic-elliptic Keller-Segel models in shifting environments

Abstract

The current paper is concerned with the persistence and spreading speeds of the following Keller-Segel chemoattraction system in shifting environments, \begin{equation}\label{abstract-eq1} \begin{cases} u_t=u_{xx}-χ(uv_x)_x +u(r(x-ct)-bu),\quad x\in\R\cr 0=v_{xx}- νv+μu,\quad x\in\R, \end{cases} \end{equation} where $χ$, $b$, $ν$, and $μ$ are positive constants, { $c\in\R$ }, $r(x)$ is Hölder continuous, bounded, $r^*=\sup_{x\in\R}r(x)>0$, $r(\pm \infty):=\lim_{x\to \pm\infty}r(x)$ exist, and $r(x)$ satisfies either $r(-\infty)<0 χμ$ and $b\ge \big(1+\frac{1}{2}\frac{(\sqrt{r^*}-\sqrtν)_+}{(\sqrt{r^*}+\sqrtν)}\big)χμ$. In the case that $r(-\infty)<0 c^*:=2\sqrt{r^*}$, then the species becomes extinct in the habitat. If the moving speed $ -c^*\leq c c^*$, then the species will become extinct in the habitat. If $λ_{\infty}$, defined to be the generalized principle eigenvalue of the operator $u\to u_{xx}+cu_{x}+r(x)u$, is negative and the degradation rate $ν$ of the chemo-attractant is grater than or equal to some number $ν^*$, then the species will also become extinct in the habitat. If $λ_{\infty}>0$, then the species will persist surrounding the good habitat.