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Asymptotic behavior as $p\rightarrow\infty$ of least energy solutions of a $(p,q(p))$-Laplacian problem

Published 31 Oct 2017 in math.AP | (1710.11287v2)

Abstract: [ \left{ \begin{array} [c]{lll} -\left( \Delta_{p}+\Delta_{q(p)}\right) u=\lambda_{p}\left\vert u(x_{u})\right\vert {p-2}u(x_{u})\delta_{x_{u}} & \mathrm{in} & \Omega\ u=0 & \mathrm{on} & \partial\Omega, \end{array} \right. ] where $x_{u}$ is the (unique) maximum point of $\left\vert u\right\vert ,$ $\delta_{x_{u}}$ is the Dirac delta distribution supported at $x_{u},$ [ \lim_{p\rightarrow\infty}\frac{q(p)}{p}=Q\in\left{ \begin{array} [c]{lll} (0,1) & \mathrm{if} & N<q(p)<p\\ (1,\infty) & \mathrm{if} & N<p<q(p) \end{array} \right. \] and $\lambda_{p}\>0$ is such that [ \min\left{ \frac{\left\Vert \nabla u\right\Vert {\infty}}{\left\Vert u\right\Vert _{\infty}}:0\not \equiv u\in W{1,\infty}(\Omega)\cap C{0}(\overline{\Omega})\right} \leq\lim_{p\rightarrow\infty}(\lambda _{p}){\frac{1}{p}}<\infty. ]

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