<p>In this paper we study the following critical anisotropic <i>p</i>-Laplace equation on infinite strip-like domains <Equation ID="Equ69"> <EquationSource Format="TEX">\(\begin{aligned} -\Delta _{p}^{H}u=\lambda |u|^{q-2}u+|u|^{p^{*}-2}u \ \ \ {\text{ in }} \ W^{1,p}_{0}(\Omega ), \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mo>-</mo> <msubsup> <mi mathvariant="normal">Δ</mi> <mrow> <mi>p</mi> </mrow> <mi>H</mi> </msubsup> <mi>u</mi> <mo>=</mo> <msup> <mrow> <mi>λ</mi> <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> <mmultiscripts> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow /> <mrow> <mmultiscripts> <mi>p</mi> <mrow /> <mrow> <mrow /> <mo>∗</mo> </mrow> </mmultiscripts> <mo>-</mo> <mn>2</mn> </mrow> </mmultiscripts> <mi>u</mi> <mspace width="4pt" /> <mspace width="4pt" /> <mspace width="4pt" /> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> </mrow> <mspace width="4pt" /> <msubsup> <mi>W</mi> <mn>0</mn> <mrow> <mn>1</mn> <mo>,</mo> <mi>p</mi> </mrow> </msubsup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\Omega =\omega \times \mathbb {R}^{N-m}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ω</mi> <mo>=</mo> <mi>ω</mi> <mo>×</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mrow> <mi>N</mi> <mo>-</mo> <mi>m</mi> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(1\le m&lt;N\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>≤</mo> <mi>m</mi> <mo>&lt;</mo> <mi>N</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\omega \subset \mathbb {R}^{m}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ω</mi> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>m</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> is an open bounded Lipschitz set, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(N\ge p^{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>≥</mo> <msup> <mi>p</mi> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation>, <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>, <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(1&lt;p\le q&lt;p^{*}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>&lt;</mo> <mi>p</mi> <mo>≤</mo> <mi>q</mi> <mo>&lt;</mo> <mmultiscripts> <mi>p</mi> <mrow /> <mrow> <mrow /> <mo>∗</mo> </mrow> </mmultiscripts> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(p^{*}=\frac{Np}{N-p}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mi>p</mi> <mrow /> <mrow> <mrow /> <mo>∗</mo> </mrow> </mmultiscripts> <mo>=</mo> <mfrac> <mrow> <mi mathvariant="italic">Np</mi> </mrow> <mrow> <mi>N</mi> <mo>-</mo> <mi>p</mi> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation> denotes the Sobolev critical exponent, <i>H</i> is a Finsler norm. The purpose of this paper are twofold: first using the anisotropic Sobolev inequality proved by Figalli et al. [Symmetry results for critical anisotropic <i>p</i>-Laplacian equations in convex cones, Geom. Funct. Anal., 2020], we establish the existence of nonnegative least energy solutions to the above equation through variational methods. Then by exploiting the Moser iteration technique and Brézis-Kato approach, we prove that for a suitable range of exponent <i>q</i>, these nonnegative weak solutions are in <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(L^{\infty }(\Omega )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mi>∞</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>.</p>

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On an Anisotropic Brézis-nirenberg Problem on Strip-like Domains

  • Yansheng Shen

摘要

In this paper we study the following critical anisotropic p-Laplace equation on infinite strip-like domains \(\begin{aligned} -\Delta _{p}^{H}u=\lambda |u|^{q-2}u+|u|^{p^{*}-2}u \ \ \ {\text{ in }} \ W^{1,p}_{0}(\Omega ), \end{aligned}\) - Δ p H u = λ | u | q - 2 u + | u | p - 2 u in W 0 1 , p ( Ω ) , where \(\Omega =\omega \times \mathbb {R}^{N-m}\) Ω = ω × R N - m with \(1\le m<N\) 1 m < N , \(\omega \subset \mathbb {R}^{m}\) ω R m is an open bounded Lipschitz set, \(N\ge p^{2}\) N p 2 , \(\lambda >0\) λ > 0 , \(1<p\le q<p^{*}\) 1 < p q < p , \(p^{*}=\frac{Np}{N-p}\) p = Np N - p denotes the Sobolev critical exponent, H is a Finsler norm. The purpose of this paper are twofold: first using the anisotropic Sobolev inequality proved by Figalli et al. [Symmetry results for critical anisotropic p-Laplacian equations in convex cones, Geom. Funct. Anal., 2020], we establish the existence of nonnegative least energy solutions to the above equation through variational methods. Then by exploiting the Moser iteration technique and Brézis-Kato approach, we prove that for a suitable range of exponent q, these nonnegative weak solutions are in \(L^{\infty }(\Omega )\) L ( Ω ) .