Almgren-type monotonicity methods for the classification of behaviour at corners of solutions to semilinear elliptic equations (Q2871078)

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scientific article; zbMATH DE number 6248815
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Almgren-type monotonicity methods for the classification of behaviour at corners of solutions to semilinear elliptic equations
scientific article; zbMATH DE number 6248815

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    Almgren-type monotonicity methods for the classification of behaviour at corners of solutions to semilinear elliptic equations (English)
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    21 January 2014
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    semilinear elliptic equations
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    asymptotic behavior
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    domains with corners
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    monotonicity methods
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    In this paper, the authors study the behavior near corners of solutions to semilinear elliptic equations in domains with conical boundary points. More precisely, they consider a domain \(\Omega\subset\mathbb{R}^N\) (\(N\geq 2\)) with the following geometric property: there exist a positive number \(R\), a cone \(\mathcal{C}=\{(x',x_N)\in \mathbb{R}^{N-1}\times \mathbb{R}: x_N>|x'|g(x'/|x'|)\), if \(x'\neq 0\), and \(x_N>0\), if \(x'=0\}\), where \(g\in C^1(\mathbb{S}^{N-2})\) if \(N\geq 3\), and a function \(\varphi\in C^2(\mathbb{R}^{N-1}\setminus\{0\})\), with \(\varphi(0)=0\), and satisfying, for some \(\delta>0\),NEWLINENEWLINE(1) \(\sup_{\nu \in \mathbb{S}^{N-2}}|\varphi(t\nu)/t-g(\nu)|=O(t^\delta)\) \ as \ \(t\rightarrow 0^+\),NEWLINENEWLINE(2) \(\sup_{\nu \in \mathbb{S}^{N-2}}|\nabla \varphi(t\nu)-g(\nu)\nu-\nabla_{\mathbb{S}^{N-2}}g(\nu)|=O(t^\delta)\) \ as \ \(t\rightarrow 0^+\), where \(\mathbb{S}^{N-2}=\{-1,1\}\) and \(\nabla_{\mathbb{S}^{N-2}}g(\nu)=0\) if \(N=2\),NEWLINENEWLINE(3) \(|D^2\varphi(x')|=O(|x'|^{-1})\), \ as \ \(|x'|\rightarrow 0\),NEWLINENEWLINE\noindent such that \(\Omega \cap B(0,R)=\{(x',x_N)\in B_R: x_N>\varphi(x')\}\), where \(B(0,R)\) is the ball in \(\mathbb{R}^N\) centered at \(0\) with radius \(R\). The above conditions express the fact that, near the origin, the domain \(\Omega\) is a perturbation of the cone \(\mathcal{C}\), and the origin is a conical boundary point of \(\Omega\). Then, the authors study the behavior near the origin of solutions to the equationNEWLINENEWLINE\(-\)div\(\displaystyle{(A(x)\nabla u(x))+{\mathbf b}(x)\cdot\nabla u(x)-\frac{V(x/|x|)}{|x|^2}u(x)=h(x)u(x)+f(x,u(x))}\), \ \ \(x\in \Omega\),NEWLINENEWLINE\noindent with the boundary condition \(u=0\) on \(\partial \Omega \cap B(0,R)\), whereNEWLINENEWLINE- \(A:\Omega \rightarrow \mathcal{M}_{N\times N}\) is such that, for some \(C>0\), \(A(x)\xi\cdot\xi\geq C|\xi|^2\) , \((A(x))_{ij}=(A(x))_{ji}\), and \((A)_{ij}\in W^{1,\infty}(\Omega)\), for all \(\xi \in \mathbb{R}^N\), \(x\in \Omega\), and \(i,j=1,\dots,N\);NEWLINENEWLINE- the coefficients \({\mathbf b}\) and \(h\) are locally bounded and may be singular at \(0\) provided that suitable decay conditions are satisfied;NEWLINENEWLINE- the nonlinearity \(f\) is continuous in \(\Omega \times \mathbb{R}\) and has subcritical growth;NEWLINENEWLINE- \(V\equiv 0\) if \(N=2\), and \(V\) is Lipschitz continuous in \(\mathbb{S}^{N-1}\) and satisfiesNEWLINENEWLINE\(\displaystyle{\sup_{v\in \mathcal{D}(\mathcal{C})\setminus\{0\}}\frac{\int_\mathcal{C}|x|^{-2}V(x/|x|)v^2(x)dx}{\int_\mathcal{C}|\nabla v(x)|^2dx}<1}\),NEWLINENEWLINE\noindent where \(\mathcal{D}(\mathcal{C})\) is the completion of \(C_c^\infty(\mathcal{C})\) with respect to the norm \((\int_\mathcal{C}|\nabla(\cdot)|^2dx)^{\frac{1}{2}}\), if \(N\geq 3\);NEWLINENEWLINE\noindent The main result of this paper states that if \(u\in H^1(\Omega)\) is a non-trivial weak solution to the above problem, which is trivially extended outside \(\Omega\), then there exists an eigenvalue \(\mu(V)\) of the operator \(-\Delta_{\mathbb{S}^{N-1}}-V\) on the spherical cap \(\mathcal{C}\cap \mathbb{S}^{N-1}\), under null boundary conditions, such that, for any \(\alpha\in (0,1)\),NEWLINENEWLINE\(\displaystyle{\lim_{\lambda\rightarrow 0^+}\lambda^\gamma u(\lambda x)= |x|^{-\gamma}\psi\biggl(\frac{x}{|x|}\biggr)}\),NEWLINENEWLINE\noindent in \(H^1(B_1)\), in \(C_{\text{ loc}}^{1,\alpha}(\mathcal{C}\cap B_1)\) and in \(C_{\text{loc}}^{0,\alpha}(B_1\setminus \{0\})\), where \(\gamma={\frac{N-2}{2}}-\sqrt{(\frac{N-2}{2})^2+\mu(V)}\), and \(\psi\) is the eigenfunction associated to \(\mu(V)\), normalized with respect to the \(L^2\) norm.NEWLINENEWLINETwo direct consequences of the main result are:NEWLINENEWLINE- \ the following point-wise upper bound for the solution \(u\): \(u(x)=O(|x|^{-\gamma})\), as \(|x|\rightarrow 0^+\),NEWLINENEWLINE- \ the following unique continuation principle: if, for any \(k\in \mathbb{N}\), the solution \(u\) is such that \(u(x)=O(|x|^{k})\), as \(|x|\rightarrow 0^+\), then \(u\equiv0\) in \(\Omega\).NEWLINENEWLINEThe proof is based on the monotonicity method introduced in [\textit{F. J. Almgren, jun.}, Bull. Am. Math. Soc., New Ser. 8, 327--328 (1983; Zbl 0557.49021)] and extended to elliptic operators with variable coefficients in [\textit{N. Garofalo} and \textit{F.-H. Lin}, Indiana Univ. Math. J. 35, 245--268 (1986; Zbl 0678.35015)].
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