Guo, Jong-Shenq; Wu, Chang-Hong Front propagation for a two-dimensional periodic monostable lattice dynamical system. (English) Zbl 1195.34118 Discrete Contin. Dyn. Syst. 26, No. 1, 197-223 (2010). The authors study wave propagation for the system \[ u_t=\nabla\cdot(A(x)\nabla u)+f(x,u),\quad x\in \mathbb{R}^n,t>0,\tag{1} \]where \(A\) and \(f\) are periodic in \(x\). The traveling waves for the one-dimensional spatial discrete version of (1) is considered in [J.-S. Guo and F. Hamel, Math. Ann. 335, No. 3, 489–525 (2006; Zbl 1116.35063)], the results of which are extended to the two dimensional spatial discrete version in the present article. The authors investigate the following system: \[ \begin{aligned} u^{\prime}_{i,j}(t)=p_{i+1,j}u_{i+1,j}(t)+p_{i,j}u_{i-1,j}(t)+q_{i,j+1}u_{i,j+1}(t)+q_{i,j}u_{i,j-1}(t)\\ -D_{i,j}u_{i,j}(t)+f(i,j,u_{i,j}(t)),\quad t\in \mathbb{R},(i,j)\in \mathbb{Z}^2,\\ u_{i+N,j}\left(t+\frac{Nr}{c}\right)=u_{i,j}(t)=u_{i,j+N}\left(t+\frac{Ns}{c}\right),\quad t\in \mathbb{R},(i,j)\in \mathbb{Z}^2,c\not=0,\\ \lim\limits_{ri+sj\to -\infty}u_{i,j}(t)=1,\quad \lim\limits_{ri+sj\to +\infty}u_{i,j}(t)=0,\quad t\in \mathbb{R},\\ 0\leq u_{i,j}(t)\leq 1, \quad t\in \mathbb{R},(i,j)\in \mathbb{Z}^2,\end{aligned}\tag{2} \]where \[ \begin{aligned} D_{i,j}=p_{i+1,j}+p_{i,j}+q_{i,j+1}+q_{i,j}, \quad {i,j}\in \mathbb{Z}^2,\\ p_{i+N,j}=p_{i,j}=p_{i,j+N},\quad q_{i+N,j}=q_{i,j}=q_{i,j+N}, \quad {i,j}\in \mathbb{Z}^2,\\ f(i+N,j,s)=f(i,j,s)=f(i,j+N,s), \quad {i,j}\in \mathbb{Z}^2,s\in [0,1]\end{aligned} \]for some positive integer \(N\). Here, \(c\) is the wave speed, \((r,s)=(\cos\theta,\sin\theta)\) with \(\theta \in [0,2\pi)\). Let \(u(\cdot)=\left\{u_{i,j}(\cdot)\right\}\) be the wave profile. Under some assumptions, the authors show the following conclusions: 8mm (a) there is a \(c_*\) such that (2) admits a traveling wave solution for \(c\geq c_*\); (b) if (2) admits a traveling wave solution for \(c\not=0\), then \(c\geq c_*\); (c) if \(u(\cdot)\) is a traveling wave solution of (2) with \(c\not=0\), then \(u(\cdot)\) is strictly increasing in \(t\); (d) by constructing a discrete approximate system for (1) in the two dimensional case, the minimal wave speed of the approximate system converges to the minimal wave speed of (1). Reviewer: Peixuan Weng (Guangzhou) Cited in 1 ReviewCited in 9 Documents MSC: 34K31 Lattice functional-differential equations 34K10 Boundary value problems for functional-differential equations 35K57 Reaction-diffusion equations Keywords:traveling wave solution; two dimensional periodic lattice dynamical system; monostable nonlinearity; minimal wave speed Citations:Zbl 1116.35063 PDFBibTeX XMLCite \textit{J.-S. Guo} and \textit{C.-H. Wu}, Discrete Contin. Dyn. Syst. 26, No. 1, 197--223 (2010; Zbl 1195.34118) Full Text: DOI