Positive profiles for the perturbed nonlocal dispersal equations (Q6622647)
From MaRDI portal
| This is the item page for this Wikibase entity, intended for internal use and editing purposes. Please use this page instead for the normal view: Positive profiles for the perturbed nonlocal dispersal equations |
scientific article; zbMATH DE number 7930184
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Positive profiles for the perturbed nonlocal dispersal equations |
scientific article; zbMATH DE number 7930184 |
Statements
Positive profiles for the perturbed nonlocal dispersal equations (English)
0 references
22 October 2024
0 references
In this paper, the authors study the sharp patterns of the perturbed nonlocal dispersal equation\N\[\N \int_{\Omega}J(x-y)u(y)dy -u(x)+\lambda u(x)+ \epsilon b(x)u(x) - a(x)u^{p}(x)=0,\qquad x\in \bar{\Omega},\tag{1}\N\]\Nwhere \(\Omega \subset \mathbb R^{N}(N \geqslant 1)\) is a smooth bounded domain, \(p>1, \lambda\in \mathbb R\) and \(\epsilon > 0\) are parameters. Moreover, \(J\in C(\mathbb R^{n})\) such that \(J >0\) in \(B_{1}\) (the unit ball), \(J=0\) in \(\mathbb R^{N} \setminus B_{1} , J(x) =J(-x)\) in \(B_{1}\) with \(\int_{\mathbb R^{N}} J(x)dx = 1\) and \(a,b\in C(\bar{\Omega}),a(x)> 0\) and \(b(x)\neq 0\) for \(x\in\bar{\Omega}\). The nonlocal eigenvalue problem\N\[\N \int _{\Omega}J (x-y)u(y)dy-u(x) + \epsilon b(x)u(x)=-\lambda u(x),\qquad x\in \bar{\Omega}\tag{2}\N\]\Nplays an important role in the study of positive solutions for \((1)\).\N\NA real number \(\lambda \in \mathbb R\) is called a principal eigenvalue of \((2)\) if there is \(u\in C(\bar{\Omega})\) with \(u(x)> 0\) for \(x\in \bar{\Omega}\) such that \((2)\) holds. The principal spectrum point of \((2)\), denoted by \(\lambda_{PS}(\epsilon,b,\Omega)\), is defined by \(\lambda_{PS}(\epsilon,b,\Omega) =\operatorname{Sup} \{ \mathrm{Re} \lambda: \lambda\in \sigma(\varPsi)\}\), where \(\sigma(\varPsi)\) stands for the spectrum set of \(\varPsi\) acting on \(C(\bar{\Omega}),\) where \(\varPsi u=\int_{\Omega} J(x-y)u(y)dy-u(x)+\epsilon b(x)u(x).\) The generalized principal eigenvalue of \(\varPsi\) or \((2)\), denoted by \(\lambda_{GP} (\epsilon,b,\Omega)\) is defined by \(\lambda_{GP}(\epsilon,b,\Omega) = \sup\{ \lambda\in \mathbb R:\exists u\in C (\bar{\Omega}),u > 0\text{ such that }\varPsi u\leq -\lambda u(x)\}\).\N\NIn the first part of this paper, the authors investigate the asymptotic behaviour of the principal spectrum point or generalized principal eigenvalue of \((2)\) with respect to parameter \(\epsilon\). The main conclusion will be used in the study of asymptotic profiles for the positive solutions of \((1)\). However, in this paper, no example is given to illustrate the results obtained.
0 references
positive solution
0 references
patterns
0 references
nonlocal dispersal
0 references
0 references
0 references
0 references
0 references
0 references
0 references
0 references