<p>In this paper, we use Legendre–Fenchel transform and a space decomposition to carry out Fountain theorem and dual Fountain theorem for the following elliptic system of Hamiltonian type: <Equation ID="Equ28"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2565_Article_Equ28.gif" Format="GIF" Height="74" Rendition="HTML" Resolution="72" Type="Linedraw" Width="217" /> </MediaObject> <EquationSource Format="TEX">\( {\left\{ \begin{array}{ll} \begin{aligned} -\Delta u&amp; =H_v(u, v) \,\quad &amp; &amp; \text {in}~\Omega ,\\ -\Delta v&amp; =H_u(u, v) \,\quad &amp; &amp; \text {in}~\Omega ,\\ u,\,v&amp; =0~~&amp; &amp; \text {on} ~ \partial \Omega ,\\ \end{aligned} \end{array}\right. } \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <msub> <mi>H</mi> <mi>v</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo>,</mo> <mi>v</mi> <mo stretchy="false">)</mo> </mrow> <mspace width="0.166667em" /> <mspace width="1em" /> </mrow> </mtd> <mtd /> <mtd columnalign="left"> <mrow> <mtext>in</mtext> <mspace width="3.33333pt" /> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow> <mrow /> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>v</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <msub> <mi>H</mi> <mi>u</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo>,</mo> <mi>v</mi> <mo stretchy="false">)</mo> </mrow> <mspace width="0.166667em" /> <mspace width="1em" /> </mrow> </mtd> <mtd /> <mtd columnalign="left"> <mrow> <mtext>in</mtext> <mspace width="3.33333pt" /> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow> <mrow /> <mi>u</mi> <mo>,</mo> <mspace width="0.166667em" /> <mi>v</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <mn>0</mn> <mspace width="3.33333pt" /> <mspace width="3.33333pt" /> </mrow> </mtd> <mtd /> <mtd columnalign="left"> <mrow> <mtext>on</mtext> <mspace width="3.33333pt" /> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow /> </mtd> </mtr> </mtable> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2565_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="48" /> </InlineMediaObject> <EquationSource Format="TEX">\(N\ge 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>≥</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2565_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="58" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Omega \subset \mathbb {R}^N\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ω</mi> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> is a bounded domain and <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2565_Article_IEq3.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="87" /> </InlineMediaObject> <EquationSource Format="TEX">\(H\in C^1( \mathbb {R}^2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>H</mi> <mo>∈</mo> <msup> <mi>C</mi> <mn>1</mn> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is strictly convex, even and subcritical. We mainly present two results: (i) When <i>H</i> is superlinear, the system has infinitely many solutions, whose energies tend to infinity. (ii) When <i>H</i> is sublinear, the system has infinitely many solutions, whose energies are negative and tend to 0. As a byproduct, the Lane–Emden system under subcritical growth has infinitely many solutions.</p>

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Infinitely many solutions for elliptic system with Hamiltonian type

  • Jia Zhang,
  • Weimin Zhang

摘要

In this paper, we use Legendre–Fenchel transform and a space decomposition to carry out Fountain theorem and dual Fountain theorem for the following elliptic system of Hamiltonian type: \( {\left\{ \begin{array}{ll} \begin{aligned} -\Delta u& =H_v(u, v) \,\quad & & \text {in}~\Omega ,\\ -\Delta v& =H_u(u, v) \,\quad & & \text {in}~\Omega ,\\ u,\,v& =0~~& & \text {on} ~ \partial \Omega ,\\ \end{aligned} \end{array}\right. } \) - Δ u = H v ( u , v ) in Ω , - Δ v = H u ( u , v ) in Ω , u , v = 0 on Ω , where \(N\ge 1\) N 1 , \(\Omega \subset \mathbb {R}^N\) Ω R N is a bounded domain and \(H\in C^1( \mathbb {R}^2)\) H C 1 ( R 2 ) is strictly convex, even and subcritical. We mainly present two results: (i) When H is superlinear, the system has infinitely many solutions, whose energies tend to infinity. (ii) When H is sublinear, the system has infinitely many solutions, whose energies are negative and tend to 0. As a byproduct, the Lane–Emden system under subcritical growth has infinitely many solutions.