<p>In this paper, we study the following linearly coupled elliptic system<Equation ID="Equ1"> <EquationNumber>(Pε)</EquationNumber> <EquationSource Format="TEX">\(\begin{cases}-\varepsilon^{2}\Delta u+P(x)u=u^{3}+\lambda(x)v &amp; \text{in} \ \Omega,\\ -\varepsilon^{2}\Delta v+Q(x)v=v^{3}+\lambda(x)u &amp; \text{in} \ \Omega,\\ u&gt;0,\ v&gt;0 &amp; \text{in} \ \Omega,\\ {\partial u\over \partial n}={\partial v\over \partial n}=0 &amp; \text{on}\ \partial \Omega,\end{cases}\)</EquationSource> </Equation>where <i>ε</i> &gt; 0, Ω is smooth and bounded in ℝ<sup>3</sup> with boundary <i>∂</i>Ω, and <i>n</i> is the outer normal vector defined on <i>∂</i>Ω.</p><p>Let <i>ω</i> be the unique positive radial solution of the well-known equation<Equation ID="Equa"> <EquationSource Format="TEX">\(-\Delta \omega+\omega=\omega^{3}, \quad\omega \in H^{1}(\mathbb{R}^{3}) ,\)</EquationSource> </Equation>and <i>μ</i><sub>1</sub> &lt; 0 be the first eigenvalue of the operator −Δ + id − 3<i>w</i><sup>2</sup> defined on <i>H</i><sup>1</sup>(ℝ<sup>3</sup>). Assume that <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(P(x), \ Q(x), \ \lambda(x) \in C^{1}(\overline{\Omega})\)</EquationSource> </InlineEquation> satisfy 0 &lt; λ(<i>x</i>) &lt; min{<i>P</i>(<i>x</i>), <i>Q</i>(<i>x</i>)},<Equation ID="Equb"> <EquationSource Format="TEX">\(P(x)=Q(x)=a_{i}&gt; 0, \quad \lambda(x)=\lambda_{i}\in (0,a_{i}),\quad \forall x \in N_{i}, \ i=1,2,\ldots, K,\)</EquationSource> </Equation>where (<i>a</i><sub><i>i</i></sub> − λ<sub><i>i</i></sub>)<i>μ</i><sub>1</sub> + 2λ<sub><i>i</i></sub> ≠ 0, {<i>N</i><sub><i>i</i></sub> ⊂ ∂Ω∣<i>i</i> = 1, 2,…, <i>K</i>} are pair-wise disjoint neighborhoods of the local minima (maxima) of the mean curvature <i>H</i>(<i>P</i>), <i>P</i> ∈ <i>∂</i>Ω. Via Lyapunov–Schmidt reduction method, we may construct a solution with <i>K</i> peaks to the system (<i>P</i><sub><i>ε</i></sub>) with each peak being on ∂Ω and locating near these local minima (maxima) points.</p>

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Multiple Boundary Peak Solutions for Linearly Coupled Schrödinger Systems

  • Ke Jin,
  • Lushun Wang

摘要

In this paper, we study the following linearly coupled elliptic system (Pε) \(\begin{cases}-\varepsilon^{2}\Delta u+P(x)u=u^{3}+\lambda(x)v & \text{in} \ \Omega,\\ -\varepsilon^{2}\Delta v+Q(x)v=v^{3}+\lambda(x)u & \text{in} \ \Omega,\\ u>0,\ v>0 & \text{in} \ \Omega,\\ {\partial u\over \partial n}={\partial v\over \partial n}=0 & \text{on}\ \partial \Omega,\end{cases}\) where ε > 0, Ω is smooth and bounded in ℝ3 with boundary Ω, and n is the outer normal vector defined on Ω.

Let ω be the unique positive radial solution of the well-known equation \(-\Delta \omega+\omega=\omega^{3}, \quad\omega \in H^{1}(\mathbb{R}^{3}) ,\) and μ1 < 0 be the first eigenvalue of the operator −Δ + id − 3w2 defined on H1(ℝ3). Assume that \(P(x), \ Q(x), \ \lambda(x) \in C^{1}(\overline{\Omega})\) satisfy 0 < λ(x) < min{P(x), Q(x)}, \(P(x)=Q(x)=a_{i}> 0, \quad \lambda(x)=\lambda_{i}\in (0,a_{i}),\quad \forall x \in N_{i}, \ i=1,2,\ldots, K,\) where (ai − λi)μ1 + 2λi ≠ 0, {Ni ⊂ ∂Ω∣i = 1, 2,…, K} are pair-wise disjoint neighborhoods of the local minima (maxima) of the mean curvature H(P), PΩ. Via Lyapunov–Schmidt reduction method, we may construct a solution with K peaks to the system (Pε) with each peak being on ∂Ω and locating near these local minima (maxima) points.