<p>We study the <i>Hamiltonian elliptic system</i><Equation ID="Equ1"> <EquationNumber>0.1</EquationNumber> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{aligned} -\Delta u&amp;= \lambda |v|^{r-1}v +|v|^{p-1}v \qquad&amp;\hbox {in} \ \ \Omega ,\\ -\Delta v&amp;= \mu |u|^{s-1}u +|u|^{q-1}u \qquad&amp;\hbox {in} \ \ \Omega ,\\ u&amp;&gt;0, \ v&gt;0 \qquad \,&amp;\hbox {in} \ \ \Omega ,\\ u&amp;=v = 0 \qquad \quad&amp;\hbox {on} \quad \partial \Omega , \end{aligned} \right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <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> <msup> <mrow> <mi>λ</mi> <mo stretchy="false">|</mo> <mi>v</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>r</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mi>v</mi> <mo>+</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>v</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mi>v</mi> <mspace width="2em" /> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mtext>in</mtext> <mspace width="4pt" /> <mspace width="4pt" /> <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> <msup> <mrow> <mi>μ</mi> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>s</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mi>u</mi> <mo>+</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>q</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mi>u</mi> <mspace width="2em" /> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mtext>in</mtext> <mspace width="4pt" /> <mspace width="4pt" /> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow> <mrow /> <mi>u</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> <mspace width="4pt" /> <mi>v</mi> <mo>&gt;</mo> <mn>0</mn> <mspace width="2em" /> <mspace width="0.166667em" /> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mtext>in</mtext> <mspace width="4pt" /> <mspace width="4pt" /> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow> <mrow /> <mi>u</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <mi>v</mi> <mo>=</mo> <mn>0</mn> <mspace width="2em" /> <mspace width="1em" /> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mtext>on</mtext> <mspace width="1em" /> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <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 smooth bounded domain, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\( \mu \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>μ</mi> </math></EquationSource> </InlineEquation> are nonnegative parameters and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(r,s,p,q&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>r</mi> <mo>,</mo> <mi>s</mi> <mo>,</mo> <mi>p</mi> <mo>,</mo> <mi>q</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. Our study includes the case in which the nonlinearities in (<InternalRef RefID="Equ1">0.1</InternalRef>) are concave near the origin and convex near infinity, and we focus on the region of non-negative <i>pairs of parameters</i> <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\((\lambda ,\mu )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi>λ</mi> <mo>,</mo> <mi>μ</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> that guarantee existence and multiplicity of solutions of (<InternalRef RefID="Equ1">0.1</InternalRef>). In particular, we show the existence of a strictly decreasing curve <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\lambda _*(\mu )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mi>λ</mi> <mrow> <mrow /> <mo>∗</mo> </mrow> <mrow /> </mmultiscripts> <mrow> <mo stretchy="false">(</mo> <mi>μ</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> on an interval <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\([0, \mu ]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mi>μ</mi> <mo stretchy="false">]</mo> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\lambda _*(0)&gt; 0, \lambda _*(\mu ) = 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mi>λ</mi> <mrow> <mrow /> <mo>∗</mo> </mrow> <mrow /> </mmultiscripts> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> <mmultiscripts> <mi>λ</mi> <mrow> <mrow /> <mo>∗</mo> </mrow> <mrow /> </mmultiscripts> <mrow> <mo stretchy="false">(</mo> <mi>μ</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and such that the system has two solutions for <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\((\lambda ,\mu )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi>λ</mi> <mo>,</mo> <mi>μ</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> below the curve, one solution for <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\((\lambda , \mu )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi>λ</mi> <mo>,</mo> <mi>μ</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> on the curve and no solution for <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\((\lambda , \mu )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi>λ</mi> <mo>,</mo> <mi>μ</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> above the curve. A similar statement holds reversing <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\mu \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>μ</mi> </math></EquationSource> </InlineEquation>.</p>

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Multiplicity results for a subcritical Hamiltonian system with concave-convex nonlinearities

  • Oscar Agudelo,
  • Bernhard Ruf,
  • Carlos Vélez

摘要

We study the Hamiltonian elliptic system 0.1 \(\begin{aligned} \left\{ \begin{aligned} -\Delta u&= \lambda |v|^{r-1}v +|v|^{p-1}v \qquad&\hbox {in} \ \ \Omega ,\\ -\Delta v&= \mu |u|^{s-1}u +|u|^{q-1}u \qquad&\hbox {in} \ \ \Omega ,\\ u&>0, \ v>0 \qquad \,&\hbox {in} \ \ \Omega ,\\ u&=v = 0 \qquad \quad&\hbox {on} \quad \partial \Omega , \end{aligned} \right. \end{aligned}\) - Δ u = λ | v | r - 1 v + | v | p - 1 v in Ω , - Δ v = μ | u | s - 1 u + | u | q - 1 u in Ω , u > 0 , v > 0 in Ω , u = v = 0 on Ω , where \(\Omega \subset \mathbb {R}^N\) Ω R N is a smooth bounded domain, \(\lambda \) λ and \( \mu \) μ are nonnegative parameters and \(r,s,p,q>0\) r , s , p , q > 0 . Our study includes the case in which the nonlinearities in (0.1) are concave near the origin and convex near infinity, and we focus on the region of non-negative pairs of parameters \((\lambda ,\mu )\) ( λ , μ ) that guarantee existence and multiplicity of solutions of (0.1). In particular, we show the existence of a strictly decreasing curve \(\lambda _*(\mu )\) λ ( μ ) on an interval \([0, \mu ]\) [ 0 , μ ] with \(\lambda _*(0)> 0, \lambda _*(\mu ) = 0\) λ ( 0 ) > 0 , λ ( μ ) = 0 and such that the system has two solutions for \((\lambda ,\mu )\) ( λ , μ ) below the curve, one solution for \((\lambda , \mu )\) ( λ , μ ) on the curve and no solution for \((\lambda , \mu )\) ( λ , μ ) above the curve. A similar statement holds reversing \(\lambda \) λ and \(\mu \) μ .