<p>We consider the following nonlocal Brézis-Nirenberg type critical Choquard problem involving the Grushin operator <Equation ID="Equ22"> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{aligned} -\Delta _\gamma&amp;u =\lambda u + \left( \displaystyle \int _\Omega \frac{|u(w)|^{2^{*}_{\gamma ,\mu }}}{d(z-w)^\mu }dw\right) |u|^{2^{*}_{\gamma ,\mu }-2}u \quad &amp; \text {in} \ \Omega ,\\ u&amp;= 0 \quad &amp; \text {on} \, \partial \Omega , \end{aligned} \right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi>γ</mi> </msub> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>u</mi> <mo>=</mo> <mi>λ</mi> <mi>u</mi> <mo>+</mo> <mfenced close=")" open="("> <mstyle displaystyle="true" scriptlevel="0"> <msub> <mo>∫</mo> <mi mathvariant="normal">Ω</mi> </msub> <mfrac> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>w</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">|</mo> </mrow> <msubsup> <mn>2</mn> <mrow> <mi>γ</mi> <mo>,</mo> <mi>μ</mi> </mrow> <mrow> <mrow /> <mo>∗</mo> </mrow> </msubsup> </msup> <mrow> <mi>d</mi> <msup> <mrow> <mo stretchy="false">(</mo> <mi>z</mi> <mo>-</mo> <mi>w</mi> <mo stretchy="false">)</mo> </mrow> <mi>μ</mi> </msup> </mrow> </mfrac> <mi>d</mi> <mi>w</mi> </mstyle> </mfenced> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <msubsup> <mn>2</mn> <mrow> <mi>γ</mi> <mo>,</mo> <mi>μ</mi> </mrow> <mrow> <mrow /> <mo>∗</mo> </mrow> </msubsup> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mspace width="1em" /> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mtext>in</mtext> <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> <mn>0</mn> <mspace width="1em" /> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mtext>on</mtext> <mspace width="0.166667em" /> <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">\(\Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Ω</mi> </math></EquationSource> </InlineEquation> is an open bounded domain in <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathbb {R}^N\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(N \ge 3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>≥</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation>, with <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\Omega \cap \{ x=0\} \ne \emptyset \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ω</mi> <mo>∩</mo> <mo stretchy="false">{</mo> <mi>x</mi> <mo>=</mo> <mn>0</mn> <mo stretchy="false">}</mo> <mo>≠</mo> <mi mathvariant="normal">∅</mi> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\lambda &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> is a parameter. Here, <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\Delta _\gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Δ</mi> <mi>γ</mi> </msub> </math></EquationSource> </InlineEquation> represents the Grushin operator, defined as <Equation ID="Equ23"> <EquationSource Format="TEX">\( \Delta _\gamma u(z) = \Delta _x u(z) +(1+\gamma )^2 |x|^{2\gamma } \Delta _y u(z), \quad \gamma \ge 0, \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <msub> <mi mathvariant="normal">Δ</mi> <mi>γ</mi> </msub> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>z</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi>x</mi> </msub> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>z</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <msup> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo>+</mo> <mi>γ</mi> <mo stretchy="false">)</mo> </mrow> <mn>2</mn> </msup> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mn>2</mn> <mi>γ</mi> </mrow> </msup> <msub> <mi mathvariant="normal">Δ</mi> <mi>y</mi> </msub> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>z</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mspace width="1em" /> <mi>γ</mi> <mo>≥</mo> <mn>0</mn> <mo>,</mo> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(z=(x,y)\in \Omega \subset \mathbb {R}^m\times \mathbb {R}^n\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>z</mi> <mo>=</mo> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>m</mi> </msup> <mo>×</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(m+n=N \ge 3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo>+</mo> <mi>n</mi> <mo>=</mo> <mi>N</mi> <mo>≥</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(2^{*}_{\gamma ,\mu }= \frac{2N_\gamma -\mu }{N_\gamma -2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mn>2</mn> <mrow> <mi>γ</mi> <mo>,</mo> <mi>μ</mi> </mrow> <mrow> <mrow /> <mo>∗</mo> </mrow> </msubsup> <mo>=</mo> <mfrac> <mrow> <mn>2</mn> <msub> <mi>N</mi> <mi>γ</mi> </msub> <mo>-</mo> <mi>μ</mi> </mrow> <mrow> <msub> <mi>N</mi> <mi>γ</mi> </msub> <mo>-</mo> <mn>2</mn> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation> is the Sobolev critical exponent in the Hardy-Littlewood context with <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(N_\gamma = m+(1+\gamma )n\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>N</mi> <mi>γ</mi> </msub> <mo>=</mo> <mi>m</mi> <mo>+</mo> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo>+</mo> <mi>γ</mi> <mo stretchy="false">)</mo> </mrow> <mi>n</mi> </mrow> </math></EquationSource> </InlineEquation> is the homogeneous dimension associated to the Grushin operator and <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(0&lt;\mu &lt;N_\gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>μ</mi> <mo>&lt;</mo> <msub> <mi>N</mi> <mi>γ</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>. The homogeneous norm related to the Grushin operator is denoted by <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(d(\cdot )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>d</mi> <mo stretchy="false">(</mo> <mo>·</mo> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. In this article, we prove the existence of bifurcation from any eigenvalue <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\lambda ^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>λ</mi> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation> of <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(-\Delta _\gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi>γ</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> under Dirichlet boundary conditions. Furthermore, we show that in a suitable left neighborhood of <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\lambda ^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>λ</mi> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation>, the number of nontrivial solutions to the problem is at least twice the multiplicity of <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\lambda ^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>λ</mi> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation>.</p>

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Bifurcation and multiplicity results for critical Grushin-Choquard problems

  • Suman Kanungo,
  • Pawan Kumar Mishra,
  • Giovanni Molica Bisci

摘要

We consider the following nonlocal Brézis-Nirenberg type critical Choquard problem involving the Grushin operator \(\begin{aligned} \left\{ \begin{aligned} -\Delta _\gamma&u =\lambda u + \left( \displaystyle \int _\Omega \frac{|u(w)|^{2^{*}_{\gamma ,\mu }}}{d(z-w)^\mu }dw\right) |u|^{2^{*}_{\gamma ,\mu }-2}u \quad & \text {in} \ \Omega ,\\ u&= 0 \quad & \text {on} \, \partial \Omega , \end{aligned} \right. \end{aligned}\) - Δ γ u = λ u + Ω | u ( w ) | 2 γ , μ d ( z - w ) μ d w | u | 2 γ , μ - 2 u in Ω , u = 0 on Ω , where \(\Omega \) Ω is an open bounded domain in \(\mathbb {R}^N\) R N , \(N \ge 3\) N 3 , with \(\Omega \cap \{ x=0\} \ne \emptyset \) Ω { x = 0 } , and \(\lambda >0\) λ > 0 is a parameter. Here, \(\Delta _\gamma \) Δ γ represents the Grushin operator, defined as \( \Delta _\gamma u(z) = \Delta _x u(z) +(1+\gamma )^2 |x|^{2\gamma } \Delta _y u(z), \quad \gamma \ge 0, \) Δ γ u ( z ) = Δ x u ( z ) + ( 1 + γ ) 2 | x | 2 γ Δ y u ( z ) , γ 0 , where \(z=(x,y)\in \Omega \subset \mathbb {R}^m\times \mathbb {R}^n\) z = ( x , y ) Ω R m × R n , \(m+n=N \ge 3\) m + n = N 3 and \(2^{*}_{\gamma ,\mu }= \frac{2N_\gamma -\mu }{N_\gamma -2}\) 2 γ , μ = 2 N γ - μ N γ - 2 is the Sobolev critical exponent in the Hardy-Littlewood context with \(N_\gamma = m+(1+\gamma )n\) N γ = m + ( 1 + γ ) n is the homogeneous dimension associated to the Grushin operator and \(0<\mu <N_\gamma \) 0 < μ < N γ . The homogeneous norm related to the Grushin operator is denoted by \(d(\cdot )\) d ( · ) . In this article, we prove the existence of bifurcation from any eigenvalue \(\lambda ^*\) λ of \(-\Delta _\gamma \) - Δ γ under Dirichlet boundary conditions. Furthermore, we show that in a suitable left neighborhood of \(\lambda ^*\) λ , the number of nontrivial solutions to the problem is at least twice the multiplicity of \(\lambda ^*\) λ .