<p>We study the following class of quasilinear degenerate elliptic equations with critical nonlinearity <Equation ID="Equ97"> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll}-\Delta _{\gamma ,p} u= \lambda |u|^{q-2}u+\left| u\right| ^{p_{\gamma }^{*}-2}u &amp; \text { in } \Omega \subset \mathbb {R}^N,\\ u=0 &amp; \text { on } \partial \Omega , \end{array}\right. } \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mrow> <mi>γ</mi> <mo>,</mo> <mi>p</mi> </mrow> </msub> <mi>u</mi> <mo>=</mo> <mi>λ</mi> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>q</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>+</mo> <msup> <mfenced close="|" open="|"> <mi>u</mi> </mfenced> <mrow> <msubsup> <mi>p</mi> <mrow> <mi>γ</mi> </mrow> <mrow> <mrow /> <mo>∗</mo> </mrow> </msubsup> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mi mathvariant="normal">Ω</mi> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mi>u</mi> <mo>=</mo> <mn>0</mn> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>on</mtext> <mspace width="0.333333em" /> <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">\(\Delta _{\gamma , p}u:=\sum _{i=1}^N X_i(|\nabla _\gamma u|^{p-2}X_i u)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="normal">Δ</mi> <mrow> <mi>γ</mi> <mo>,</mo> <mi>p</mi> </mrow> </msub> <mi>u</mi> <mo>:</mo> <mo>=</mo> <msubsup> <mo>∑</mo> <mrow> <mi>i</mi> <mo>=</mo> <mn>1</mn> </mrow> <mi>N</mi> </msubsup> <msub> <mi>X</mi> <mi>i</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mo stretchy="false">|</mo> </mrow> <msub> <mi mathvariant="normal">∇</mi> <mi>γ</mi> </msub> <mi>u</mi> <mrow> <msup> <mo stretchy="false">|</mo> <mrow> <mi>p</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <msub> <mi>X</mi> <mi>i</mi> </msub> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is the Grushin <i>p</i>-Laplace operator, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(z:=(x, y) \in \mathbb {R}^N\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>z</mi> <mo>:</mo> <mo>=</mo> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(N=m+n,\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>=</mo> <mi>m</mi> <mo>+</mo> <mi>n</mi> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(m,n \ge 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo>,</mo> <mi>n</mi> <mo>≥</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\nabla _\gamma =(X_1, \ldots , X_N)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="normal">∇</mi> <mi>γ</mi> </msub> <mo>=</mo> <mrow> <mo stretchy="false">(</mo> <msub> <mi>X</mi> <mn>1</mn> </msub> <mo>,</mo> <mo>…</mo> <mo>,</mo> <msub> <mi>X</mi> <mi>N</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is the Grushin gradient, defined as the system of vector fields <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(X_i=\frac{\partial }{\partial x_i}, i=1, \ldots , m\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>X</mi> <mi>i</mi> </msub> <mo>=</mo> <mfrac> <mi>∂</mi> <mrow> <mi>∂</mi> <msub> <mi>x</mi> <mi>i</mi> </msub> </mrow> </mfrac> <mo>,</mo> <mi>i</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> <mo>…</mo> <mo>,</mo> <mi>m</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(X_{m+j}=|x|^\gamma \frac{\partial }{\partial y_j}, j=1, \ldots , n\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>X</mi> <mrow> <mi>m</mi> <mo>+</mo> <mi>j</mi> </mrow> </msub> <mo>=</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mi>γ</mi> </msup> <mfrac> <mi>∂</mi> <mrow> <mi>∂</mi> <msub> <mi>y</mi> <mi>j</mi> </msub> </mrow> </mfrac> <mo>,</mo> <mi>j</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> <mo>…</mo> <mo>,</mo> <mi>n</mi> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\gamma &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>γ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. Here, <InlineEquation ID="IEq9"> <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 such that <InlineEquation ID="IEq10"> <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>, <InlineEquation ID="IEq11"> <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>, <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(q \in [p,p_\gamma ^*)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>∈</mo> <mo stretchy="false">[</mo> <mi>p</mi> <mo>,</mo> <msubsup> <mi>p</mi> <mi>γ</mi> <mo>∗</mo> </msubsup> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(p_{\gamma }^{*}=\frac{pN_\gamma }{N_\gamma -p}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>p</mi> <mrow> <mi>γ</mi> </mrow> <mrow> <mrow /> <mo>∗</mo> </mrow> </msubsup> <mo>=</mo> <mfrac> <mrow> <mi>p</mi> <msub> <mi>N</mi> <mi>γ</mi> </msub> </mrow> <mrow> <msub> <mi>N</mi> <mi>γ</mi> </msub> <mo>-</mo> <mi>p</mi> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq14"> <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> denotes the homogeneous dimension attached to the Grushin gradient. The results extend to the <i>p</i>-case the Brezis-Nirenberg type results in Alves-Gandal-Loiudice-Tyagi [J. Geom. Anal. 2024, 34(2),52]. The main crucial step is to preliminarily establish the existence of the extremals for the involved Sobolev-type inequality <Equation ID="Equ98"> <EquationSource Format="TEX">\( \int _{\mathbb {R}^N} |\nabla _{\gamma } u|^p dz \ge S_{\gamma ,p} \left( \int _{\mathbb {R}^N} |u|^{p_\gamma ^*} dz \right) ^{p/p_\gamma ^*} \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <msub> <mo>∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <msub> <mi mathvariant="normal">∇</mi> <mi>γ</mi> </msub> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mi>p</mi> </msup> <mi>d</mi> <mi>z</mi> <mo>≥</mo> <msub> <mi>S</mi> <mrow> <mi>γ</mi> <mo>,</mo> <mi>p</mi> </mrow> </msub> <msup> <mfenced close=")" open="("> <msub> <mo>∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <msubsup> <mi>p</mi> <mi>γ</mi> <mo>∗</mo> </msubsup> </msup> <mi>d</mi> <mi>z</mi> </mfenced> <mrow> <mi>p</mi> <mo stretchy="false">/</mo> <msubsup> <mi>p</mi> <mi>γ</mi> <mo>∗</mo> </msubsup> </mrow> </msup> </mrow> </math></EquationSource> </Equation>and their qualitative behavior as positive entire solutions to the limit problem <Equation ID="Equ99"> <EquationSource Format="TEX">\(\begin{aligned} -\Delta _{\gamma ,p} u= u^{p_{\gamma }^{*}-1}\quad \hbox {on}\, \mathbb {R}^N, \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mrow> <mi>γ</mi> <mo>,</mo> <mi>p</mi> </mrow> </msub> <mi>u</mi> <mo>=</mo> <msup> <mi>u</mi> <mrow> <msubsup> <mi>p</mi> <mrow> <mi>γ</mi> </mrow> <mrow> <mrow /> <mo>∗</mo> </mrow> </msubsup> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mspace width="1em" /> <mtext>on</mtext> <mspace width="0.166667em" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>whose study has independent interest.</p>

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Quasilinear problems with critical Sobolev exponent for the Grushin p-Laplace operator

  • Somnath Gandal,
  • Annunziata Loiudice,
  • Jagmohan Tyagi

摘要

We study the following class of quasilinear degenerate elliptic equations with critical nonlinearity \(\begin{aligned} {\left\{ \begin{array}{ll}-\Delta _{\gamma ,p} u= \lambda |u|^{q-2}u+\left| u\right| ^{p_{\gamma }^{*}-2}u & \text { in } \Omega \subset \mathbb {R}^N,\\ u=0 & \text { on } \partial \Omega , \end{array}\right. } \end{aligned}\) - Δ γ , p u = λ | u | q - 2 u + u p γ - 2 u in Ω R N , u = 0 on Ω , where \(\Delta _{\gamma , p}u:=\sum _{i=1}^N X_i(|\nabla _\gamma u|^{p-2}X_i u)\) Δ γ , p u : = i = 1 N X i ( | γ u | p - 2 X i u ) is the Grushin p-Laplace operator, \(z:=(x, y) \in \mathbb {R}^N\) z : = ( x , y ) R N , \(N=m+n,\) N = m + n , \(m,n \ge 1\) m , n 1 , where \(\nabla _\gamma =(X_1, \ldots , X_N)\) γ = ( X 1 , , X N ) is the Grushin gradient, defined as the system of vector fields \(X_i=\frac{\partial }{\partial x_i}, i=1, \ldots , m\) X i = x i , i = 1 , , m , \(X_{m+j}=|x|^\gamma \frac{\partial }{\partial y_j}, j=1, \ldots , n\) X m + j = | x | γ y j , j = 1 , , n , where \(\gamma >0\) γ > 0 . Here, \(\Omega \subset \mathbb {R}^{N}\) Ω R N is a smooth bounded domain such that \(\Omega \cap \{x=0\}\ne \emptyset \) Ω { x = 0 } , \(\lambda >0\) λ > 0 , \(q \in [p,p_\gamma ^*)\) q [ p , p γ ) , where \(p_{\gamma }^{*}=\frac{pN_\gamma }{N_\gamma -p}\) p γ = p N γ N γ - p and \(N_\gamma =m+(1+\gamma )n\) N γ = m + ( 1 + γ ) n denotes the homogeneous dimension attached to the Grushin gradient. The results extend to the p-case the Brezis-Nirenberg type results in Alves-Gandal-Loiudice-Tyagi [J. Geom. Anal. 2024, 34(2),52]. The main crucial step is to preliminarily establish the existence of the extremals for the involved Sobolev-type inequality \( \int _{\mathbb {R}^N} |\nabla _{\gamma } u|^p dz \ge S_{\gamma ,p} \left( \int _{\mathbb {R}^N} |u|^{p_\gamma ^*} dz \right) ^{p/p_\gamma ^*} \) R N | γ u | p d z S γ , p R N | u | p γ d z p / p γ and their qualitative behavior as positive entire solutions to the limit problem \(\begin{aligned} -\Delta _{\gamma ,p} u= u^{p_{\gamma }^{*}-1}\quad \hbox {on}\, \mathbb {R}^N, \end{aligned}\) - Δ γ , p u = u p γ - 1 on R N , whose study has independent interest.