<p>In this paper, we study the elliptic system <Equation ID="Equa"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="10473_2025_218_Article_Equa.gif" Format="GIF" Height="65" Rendition="HTML" Resolution="72" Type="Linedraw" Width="292" /> </MediaObject> <EquationSource Format="TEX">\(\left\{\begin{array}{ll}-\Delta u +V(x) u=|v|^{p-2}v-\lambda_2|v|^{s_2-2}v, \\-\Delta v + V(x)v=|u|^{p-2}u-\lambda_1|u|^{s_1-2}u, \\ u,v \in H^1(\mathbb{R}^N)\end{array}\right.\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mo>{</mo> <mtable columnalign="left left" columnspacing="1em" rowspacing="4pt"> <mtr> <mtd> <mo>−</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>+</mo> <mi>V</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> <mi>u</mi> <mo>=</mo> <mrow> <mo stretchy="false">∣</mo> </mrow> <mi>v</mi> <msup> <mrow> <mo stretchy="false">∣</mo> </mrow> <mrow> <mi>p</mi> <mo>−</mo> <mn>2</mn> </mrow> </msup> <mi>v</mi> <mo>−</mo> <msub> <mi>λ</mi> <mn>2</mn> </msub> <mrow> <mo stretchy="false">∣</mo> </mrow> <mi>v</mi> <msup> <mrow> <mo stretchy="false">∣</mo> </mrow> <mrow> <msub> <mi>s</mi> <mn>2</mn> </msub> <mo>−</mo> <mn>2</mn> </mrow> </msup> <mi>v</mi> <mo>,</mo> </mtd> </mtr> <mtr> <mtd> <mo>−</mo> <mi mathvariant="normal">Δ</mi> <mi>v</mi> <mo>+</mo> <mi>V</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> <mi>v</mi> <mo>=</mo> <mrow> <mo stretchy="false">∣</mo> </mrow> <mi>u</mi> <msup> <mrow> <mo stretchy="false">∣</mo> </mrow> <mrow> <mi>p</mi> <mo>−</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>−</mo> <msub> <mi>λ</mi> <mn>1</mn> </msub> <mrow> <mo stretchy="false">∣</mo> </mrow> <mi>u</mi> <msup> <mrow> <mo stretchy="false">∣</mo> </mrow> <mrow> <msub> <mi>s</mi> <mn>1</mn> </msub> <mo>−</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>,</mo> </mtd> </mtr> <mtr> <mtd> <mi>u</mi> <mo>,</mo> <mi>v</mi> <mo>∈</mo> <msup> <mi>H</mi> <mn>1</mn> </msup> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo stretchy="false">)</mo> </mtd> </mtr> </mtable> <mo fence="true" stretchy="true" /> </mrow> </math></EquationSource> </Equation> with strongly indefinite structure and sign-changing nonlinearity. We overcome the absence of the upper semi-continuity assumption which is crucial in traditional variational methods for strongly indefinite problems. By some new tools and techniques we proved the existence of infinitely many geometrically distinct solutions if parameters <i>λ</i><sub>1</sub>, <i>λ</i><sub>2</sub> &gt; 0 small enough. To the best of our knowledge, our result seems to be the first result about infinitely many solutions for Hamiltonian system involving sign-changing nonlinearity.</p>

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Multiple solutions for a Hamiltonian elliptic system with sign-changing perturbation

  • Peng Chen,
  • Longjiang Gu,
  • Yan Wu

摘要

In this paper, we study the elliptic system \(\left\{\begin{array}{ll}-\Delta u +V(x) u=|v|^{p-2}v-\lambda_2|v|^{s_2-2}v, \\-\Delta v + V(x)v=|u|^{p-2}u-\lambda_1|u|^{s_1-2}u, \\ u,v \in H^1(\mathbb{R}^N)\end{array}\right.\) { Δ u + V ( x ) u = v p 2 v λ 2 v s 2 2 v , Δ v + V ( x ) v = u p 2 u λ 1 u s 1 2 u , u , v H 1 ( R N ) with strongly indefinite structure and sign-changing nonlinearity. We overcome the absence of the upper semi-continuity assumption which is crucial in traditional variational methods for strongly indefinite problems. By some new tools and techniques we proved the existence of infinitely many geometrically distinct solutions if parameters λ1, λ2 > 0 small enough. To the best of our knowledge, our result seems to be the first result about infinitely many solutions for Hamiltonian system involving sign-changing nonlinearity.