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Elliptic $p$-Laplacian systems with nonlinear boundary condition

Franziska Borer, Siegfried Carl, Patrick Winkert

Abstract

In this paper we study quasilinear elliptic systems given by \begin{equation*} \begin{aligned} -Δ_{p_1}u_1 & =-|u_1|^{p_1-2}u_1 \quad && \text{in } Ω,\newline -Δ_{p_2}u_2 & =-|u_2|^{p_2-2}u_2 \quad && \text{in } Ω,\newline |\nabla u_1|^{p_1-2}\nabla u_1 \cdot ν &=g_1(x,u_1,u_2) && \text{on } \partialΩ,\newline |\nabla u_2|^{p_2-2}\nabla u_2 \cdot ν &=g_2(x,u_1,u_2) && \text{on } \partialΩ, \end{aligned} \end{equation*} where $ν(x)$ is the outer unit normal of $Ω$ at $x \in \partialΩ$, $Δ_{p_i}$ denotes the $p_i$-Laplacian and $g_i\colon \partialΩ\times\mathbb{R}\times\mathbb{R}\to\mathbb{R}$ are Carathéodory functions that satisfy general growth and structure conditions for $i=1,2$. In the first part we prove the existence of a positive minimal and a negative maximal solution based on an appropriate construction of sub- and supersolution along with a certain behavior of $g_i$ near zero related to the first eigenvalue of the $p_i$-Laplacian with Steklov boundary condition. The second part is related to the existence of a third nontrivial solution by imposing a variational structure, that is, $(g_1,g_2)=\nabla g$ with a smooth function $(s_1,s_2)\mapsto g(x,s_1,s_2)$. By using the variational characterization of the second eigenvalue of the Steklov eigenvalue problem for the $p_i$-Laplacian together with the properties of the related truncated energy functionals, which are in general nonsmooth, we show the existence of a nontrivial solution whose components lie between the components of the positive minimal and the negative maximal solution.

Elliptic $p$-Laplacian systems with nonlinear boundary condition

Abstract

In this paper we study quasilinear elliptic systems given by \begin{equation*} \begin{aligned} -Δ_{p_1}u_1 & =-|u_1|^{p_1-2}u_1 \quad && \text{in } Ω,\newline -Δ_{p_2}u_2 & =-|u_2|^{p_2-2}u_2 \quad && \text{in } Ω,\newline |\nabla u_1|^{p_1-2}\nabla u_1 \cdot ν &=g_1(x,u_1,u_2) && \text{on } \partialΩ,\newline |\nabla u_2|^{p_2-2}\nabla u_2 \cdot ν &=g_2(x,u_1,u_2) && \text{on } \partialΩ, \end{aligned} \end{equation*} where is the outer unit normal of at , denotes the -Laplacian and are Carathéodory functions that satisfy general growth and structure conditions for . In the first part we prove the existence of a positive minimal and a negative maximal solution based on an appropriate construction of sub- and supersolution along with a certain behavior of near zero related to the first eigenvalue of the -Laplacian with Steklov boundary condition. The second part is related to the existence of a third nontrivial solution by imposing a variational structure, that is, with a smooth function . By using the variational characterization of the second eigenvalue of the Steklov eigenvalue problem for the -Laplacian together with the properties of the related truncated energy functionals, which are in general nonsmooth, we show the existence of a nontrivial solution whose components lie between the components of the positive minimal and the negative maximal solution.
Paper Structure (4 sections, 9 theorems, 140 equations)

This paper contains 4 sections, 9 theorems, 140 equations.

Key Result

Proposition 2.3

Let $p_i\in (1,\infty)$ and let $A_{p_i}\colon \mathcal{V}_i\to \mathcal{V}_i^*$ be given by operator-Api. Then $A_{p_i}$ is well-defined, bounded, continuous, monotone and of type (S$_+$), that is, $u_i^k\rightharpoonup u_i$ in $\mathcal{V}_i$ and $\limsup_{k\rightarrow\infty}\,\langle A_{p_i} (u_i

Theorems & Definitions (21)

  • Definition 2.1
  • Definition 2.2
  • Proposition 2.3
  • Definition 2.4
  • Theorem 2.5
  • Remark 3.1
  • Theorem 3.2
  • proof
  • Theorem 3.3
  • proof
  • ...and 11 more