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Critical blow-up curve in a two-species chemotaxis system with two chemicals involving flux-limitation

Ziyue Zeng, Yuxiang Li

TL;DR

This work identifies a critical blow-up boundary for a flux-limited two-species chemotaxis system with two chemicals by recasting the problem in radial mass coordinates and proving a weak comparison principle. It then constructs singular subsolutions using a time-blowing function $y(t)$ to demonstrate finite-time blow-up when $n\ge 3$ and $p,q\in(0,1)$ with $p<\frac{n-2}{n-1}$ and $q<\frac{n-2}{n-1}$. Conversely, it proves global boundedness for general domains when either $p$ or $q$ exceeds the critical threshold, by leveraging semigroup estimates and bootstrapping arguments. The results delineate the precise blow-up vs boundedness border for flux-limited chemotaxis systems and extend the understanding of critical exponents in multi-species chemotaxis models.

Abstract

We investigate the following two-species chemotaxis system with two chemicals involving flux-limitation \begin{align}\tag{$\star$} \begin{cases} u_t = Δu - \nabla \cdot \left(u(1+|\nabla v|^2)^{-\frac{p}{2}}\nabla v\right), & x \in Ω, \ t > 0, \\ 0 = Δv - μ_w + w, \quad μ_{w}=f_Ω w, & x \in Ω, \ t > 0, \\ w_t = Δw - \nabla \cdot \left(w (1+|\nabla z|^2)^{-\frac{q}{2}} \nabla z\right), & x \in Ω, \ t > 0, \\ 0 = Δz - μ_u + u, \quad μ_{u}=f_Ω u, & x \in Ω, \ t > 0, \\ \frac{\partial u}{\partial ν} = \frac{\partial v}{\partial ν} = \frac{\partial w}{\partial ν} = \frac{\partial z}{\partial ν} = 0, & x \in \partial Ω, \ t > 0, \\ u(x, 0) = u_0(x), \quad w(x, 0) = w_0(x), & x \in Ω, \end{cases} \end{align} where $p,q \in \mathbb{R}$ and $Ω\subset \mathbb{R}^n$ is a smooth bounded domain. In this paper, we identify a critical blow-up curve ( i.e $p=\frac{n-2}{n-1}$ and $q=\frac{n-2}{n-1}$ in the square $(0,\frac{n-2}{n-1}] \times (0,\frac{n-2}{n-1}]$) for system ($\star$) with $n\geq 3$ and $p,q>0$. Specifically, \begin{itemize} \item when $Ω=B_R(0) \subset \mathbb{R}^n$ with $n\geq 3$, if $0<p<\frac{n-2}{n-1}$ and $0<q<\frac{n-2}{n-1}$, there exist radially symmetric initial data such that the corresponding solution blows up in finite time; \item for any general smooth bounded domain, if either $n=1$ ( with $p,q \in \mathbb{R}$ arbitrary) or $n\geq 2$ with $p>\frac{n-2}{n-1}$ or $q>\frac{n-2}{n-1}$, then solutions exist globally and remain bounded. \end{itemize}

Critical blow-up curve in a two-species chemotaxis system with two chemicals involving flux-limitation

TL;DR

This work identifies a critical blow-up boundary for a flux-limited two-species chemotaxis system with two chemicals by recasting the problem in radial mass coordinates and proving a weak comparison principle. It then constructs singular subsolutions using a time-blowing function to demonstrate finite-time blow-up when and with and . Conversely, it proves global boundedness for general domains when either or exceeds the critical threshold, by leveraging semigroup estimates and bootstrapping arguments. The results delineate the precise blow-up vs boundedness border for flux-limited chemotaxis systems and extend the understanding of critical exponents in multi-species chemotaxis models.

Abstract

We investigate the following two-species chemotaxis system with two chemicals involving flux-limitation \begin{align}\tag{} \begin{cases} u_t = Δu - \nabla \cdot \left(u(1+|\nabla v|^2)^{-\frac{p}{2}}\nabla v\right), & x \in Ω, \ t > 0, \\ 0 = Δv - μ_w + w, \quad μ_{w}=f_Ω w, & x \in Ω, \ t > 0, \\ w_t = Δw - \nabla \cdot \left(w (1+|\nabla z|^2)^{-\frac{q}{2}} \nabla z\right), & x \in Ω, \ t > 0, \\ 0 = Δz - μ_u + u, \quad μ_{u}=f_Ω u, & x \in Ω, \ t > 0, \\ \frac{\partial u}{\partial ν} = \frac{\partial v}{\partial ν} = \frac{\partial w}{\partial ν} = \frac{\partial z}{\partial ν} = 0, & x \in \partial Ω, \ t > 0, \\ u(x, 0) = u_0(x), \quad w(x, 0) = w_0(x), & x \in Ω, \end{cases} \end{align} where and is a smooth bounded domain. In this paper, we identify a critical blow-up curve ( i.e and in the square ) for system () with and . Specifically, \begin{itemize} \item when with , if and , there exist radially symmetric initial data such that the corresponding solution blows up in finite time; \item for any general smooth bounded domain, if either ( with arbitrary) or with or , then solutions exist globally and remain bounded. \end{itemize}
Paper Structure (4 sections, 10 theorems, 123 equations, 1 figure)

This paper contains 4 sections, 10 theorems, 123 equations, 1 figure.

Key Result

Proposition 1.1

Let $\Omega \subset \mathbb{R}^n$$(n \geq 1)$ be a smooth bounded domain. Assume that $\left(u_0, w_0\right)$ is as in $(eq1.1)$. Then there exist $T_{\max } \in(0, \infty]$ and uniquely determined positive functions satisfying $\int_{\Omega} v(\cdot,t) \mathrm{~d}x=0$ and $\int_{\Omega} z(\cdot,t) \mathrm{~d}x=0$ for all $t \in (0,T_{\max})$, such that eq1.1.0 is solved in the classical sense in

Figures (1)

  • Figure 1: “GB”: All solutions are globally bounded. “FTBU”: There exist solutions that blow up in finite time.

Theorems & Definitions (19)

  • Proposition 1.1
  • Theorem 1.2
  • Theorem 1.3
  • Remark 1.1
  • Lemma 2.1
  • proof
  • Lemma 2.2
  • proof
  • Lemma 3.1
  • proof
  • ...and 9 more