{"title":"Asymptotic behavior of a three-dimensional haptotactic cross-diffusion system modeling oncolytic virotherapy","authors":"Yifu Wang, Chi Xu","doi":"10.1142/s0218202523400043","DOIUrl":null,"url":null,"abstract":"This paper deals with an initial-boundary value problem for a doubly haptotactic cross-diffusion system arising from the oncolytic virotherapy \\begin{equation*} \\left\\{ \\begin{array}{lll} u_t=\\Delta u-\\nabla \\cdot(u\\nabla v)+\\mu u(1-u)-uz,\\\\ v_t=-(u+w)v,\\\\ w_t=\\Delta w-\\nabla \\cdot(w\\nabla v)-w+uz,\\\\ z_t=D_z\\Delta z-z-uz+\\beta w, \\end{array} \\right. \\end{equation*} in a smoothly bounded domain $\\Omega\\subset \\mathbb{R}^3$ with $\\beta>0$,~$\\mu>0$ and $D_z>0$. Based on a self-map argument, it is shown that under the assumption $\\beta \\max \\{1,\\|u_0\\|_{L^{\\infty}(\\Omega)}\\}<1+ (1+\\frac1{\\min_{x\\in \\Omega}u_0(x)})^{-1}$, this problem possesses a uniquely determined global classical solution $(u,v,w,z)$ for certain type of small data $(u_0,v_0,w_0,z_0)$. Moreover, $(u,v,w,z)$ is globally bounded and exponentially stabilizes towards its spatially homogeneous equilibrium %constant equilibrium $(1,0,0,0)$ as $t\\rightarrow \\infty$.","PeriodicalId":3,"journal":{"name":"ACS Applied Electronic Materials","volume":null,"pages":null},"PeriodicalIF":4.3000,"publicationDate":"2022-10-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"ACS Applied Electronic Materials","FirstCategoryId":"100","ListUrlMain":"https://doi.org/10.1142/s0218202523400043","RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
引用次数: 0
Abstract
This paper deals with an initial-boundary value problem for a doubly haptotactic cross-diffusion system arising from the oncolytic virotherapy \begin{equation*} \left\{ \begin{array}{lll} u_t=\Delta u-\nabla \cdot(u\nabla v)+\mu u(1-u)-uz,\\ v_t=-(u+w)v,\\ w_t=\Delta w-\nabla \cdot(w\nabla v)-w+uz,\\ z_t=D_z\Delta z-z-uz+\beta w, \end{array} \right. \end{equation*} in a smoothly bounded domain $\Omega\subset \mathbb{R}^3$ with $\beta>0$,~$\mu>0$ and $D_z>0$. Based on a self-map argument, it is shown that under the assumption $\beta \max \{1,\|u_0\|_{L^{\infty}(\Omega)}\}<1+ (1+\frac1{\min_{x\in \Omega}u_0(x)})^{-1}$, this problem possesses a uniquely determined global classical solution $(u,v,w,z)$ for certain type of small data $(u_0,v_0,w_0,z_0)$. Moreover, $(u,v,w,z)$ is globally bounded and exponentially stabilizes towards its spatially homogeneous equilibrium %constant equilibrium $(1,0,0,0)$ as $t\rightarrow \infty$.