Positive solutions of the \(p\)-Laplace Emden-Fowler equation in hollow thin symmetric domains. (Q2925948)

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scientific article; zbMATH DE number 6362249
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Positive solutions of the \(p\)-Laplace Emden-Fowler equation in hollow thin symmetric domains.
scientific article; zbMATH DE number 6362249

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    29 October 2014
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    Emden-Fowler equation
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    \(p\)-Laplacian
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    group invariant solution
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    least energy solution
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    positive solution
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    variational method
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    Positive solutions of the \(p\)-Laplace Emden-Fowler equation in hollow thin symmetric domains. (English)
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    Let \(\Omega\) be a bounded domain in \(\mathbb{R}^N\) with \(N\geq 2\) and let \(p\), \(q\geq 2\) with \(p<q<p^*\), where \(p^*=\infty\) if \(N\leq p\) and \(p^*=\frac{Np}{N-p}\) if \(N>p\) is the critical exponent for the Sobolev embedding. In this paper, the authors study certain symmetry properties of positive solutions to the Dirichlet problem for the Emden-Fowler equation NEWLINE\[NEWLINE-\Delta_p u= u^{q-1}\text{ in }\Omega, \, u=0\text{ on }\partial \Omega.\leqno{(P)}NEWLINE\]NEWLINE More precisely, they establish the following result: Let \(H,G\) be two closed subgroups of the orthogonal group \(O(N)\), let \(U\subset \mathbb{R}^N\) be a \(G\)-invariant domain, and let NEWLINE\[NEWLINER(u):=\left(\int_\Omega |\nabla u|^pdx\right)\left(\int_\Omega |u|^qdx\right)^{-\frac{p}{q}},\, u\in W_0^{1,p}(\Omega)\setminus \{0\},NEWLINE\]NEWLINE be the Rayleigh quotient. Assume that \(\Omega\) is a \(G\)-invariant proper subdomain of \(U\) and that \(\{hx: h\in H\}\) is a proper subset of \(\{gx: g\in G\}\) for all \(x\in \overline{U}\). Then, there exists a positive constant \(C\) depending only on \(H,G,p,q,U\) such that NEWLINE\[NEWLINE\inf_{u\in W_0^{1,p}(\Omega,H)\setminus \{0\}}R(u)<\inf_{u\in W_0^{1,p}(\Omega,G)\setminus \{0\}}R(u),NEWLINE\]NEWLINE whenever \(\lambda_p(\Omega)>C\). Here, \(\lambda_p(\Omega)\) is the first eigenvalue of the \(p\)-Laplacian on \(\Omega\) and \(W_0^{1,p}(\Omega,G)\) and \(W_0^{1,p}(\Omega,H)\) are the subspaces of all \(G\) invariant and \(H\) invariant functions of \(W_0^{1,p}(\Omega)\), respectively. As a consequence of the above inequality, no \(H\) invariant solution to problem \((P)\) which minimizes \(R(u)\) on \(W_0^{1,p}(\Omega,H)\) is \(G\)-invariant.NEWLINENEWLINE The proof is based on variational methods.
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