<p>We consider the elliptic equation with boundary singularities <Equation ID="Equ16"> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} -\Delta u=-\lambda |x|^{-s_{1}}|u|^{p-2}u+|x|^{-s_{2}}|u|^{q-2}u &amp; \text{ in } \varOmega , \\ u(x)=0 &amp; \text{ on } \partial \varOmega , \end{array}\right. } \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>=</mo> <mo>-</mo> <msup> <mrow> <mi>λ</mi> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mo>-</mo> <msub> <mi>s</mi> <mn>1</mn> </msub> </mrow> </msup> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>+</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mo>-</mo> <msub> <mi>s</mi> <mn>2</mn> </msub> </mrow> </msup> <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> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mi>Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mi>u</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> <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>Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(0\in \partial \Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>∈</mo> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\varOmega \subset \mathbb {R}^N \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>Ω</mi> <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">\(N\ge 3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>≥</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <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="IEq5"> <EquationSource Format="TEX">\(0\le s_1&lt; s_2 &lt; 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>≤</mo> <msub> <mi>s</mi> <mn>1</mn> </msub> <mo>&lt;</mo> <msub> <mi>s</mi> <mn>2</mn> </msub> <mo>&lt;</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(2&lt;q&lt;p&lt; 2^{*}(s_1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>2</mn> <mo>&lt;</mo> <mi>q</mi> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <mmultiscripts> <mn>2</mn> <mrow /> <mrow> <mrow /> <mo>∗</mo> </mrow> </mmultiscripts> <mrow> <mo stretchy="false">(</mo> <msub> <mi>s</mi> <mn>1</mn> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(q\le 2^{*}(s_2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>≤</mo> <mmultiscripts> <mn>2</mn> <mrow /> <mrow> <mrow /> <mo>∗</mo> </mrow> </mmultiscripts> <mrow> <mo stretchy="false">(</mo> <msub> <mi>s</mi> <mn>2</mn> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. This paper attempts to study the problem, aiming to provide new research approaches for completely addressing the Li–Lin open problem proposed by Y.Y. Li and C.-S. Lin (Arch. Ration. Mech. Anal. 203(3): 943–968, 2012). Specifically, we focus on its subcritical approximations for <i>q</i> in the range <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(2^{*}(s_2)&gt;q&gt;\frac{2-s_2}{2-s_1}p+\frac{2s_2-2s_1}{2-s_1}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mn>2</mn> <mrow /> <mrow> <mrow /> <mo>∗</mo> </mrow> </mmultiscripts> <mrow> <mo stretchy="false">(</mo> <msub> <mi>s</mi> <mn>2</mn> </msub> <mo stretchy="false">)</mo> </mrow> <mo>&gt;</mo> <mi>q</mi> <mo>&gt;</mo> <mfrac> <mrow> <mn>2</mn> <mo>-</mo> <msub> <mi>s</mi> <mn>2</mn> </msub> </mrow> <mrow> <mn>2</mn> <mo>-</mo> <msub> <mi>s</mi> <mn>1</mn> </msub> </mrow> </mfrac> <mi>p</mi> <mo>+</mo> <mfrac> <mrow> <mn>2</mn> <msub> <mi>s</mi> <mn>2</mn> </msub> <mo>-</mo> <mn>2</mn> <msub> <mi>s</mi> <mn>1</mn> </msub> </mrow> <mrow> <mn>2</mn> <mo>-</mo> <msub> <mi>s</mi> <mn>1</mn> </msub> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation>. To address the challenge that the energy functional associated with the equation is unbounded below on the Nehari manifold and fails to admit a global minimizer, we establish the existence of a positive solution that serves as a local minimizer of the energy functional on this manifold. Additionally, we investigate the asymptotic behavior of the positive solution and, through blow-up analysis, identify a new class of blow-up points located on the domain boundary. These boundary blow-up points exhibit distinct characteristics from those commonly reported in the literature.</p>

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A positive solution of the elliptic equation on a starshaped domain with boundary singularities

  • Zhi-Yun Tang,
  • Xianhua Tang

摘要

We consider the elliptic equation with boundary singularities \(\begin{aligned} {\left\{ \begin{array}{ll} -\Delta u=-\lambda |x|^{-s_{1}}|u|^{p-2}u+|x|^{-s_{2}}|u|^{q-2}u & \text{ in } \varOmega , \\ u(x)=0 & \text{ on } \partial \varOmega , \end{array}\right. } \end{aligned}\) - Δ u = - λ | x | - s 1 | u | p - 2 u + | x | - s 2 | u | q - 2 u in Ω , u ( x ) = 0 on Ω , where \(0\in \partial \Omega \) 0 Ω , \(\varOmega \subset \mathbb {R}^N \) Ω R N , \(N\ge 3\) N 3 , \(\lambda >0\) λ > 0 , \(0\le s_1< s_2 < 2\) 0 s 1 < s 2 < 2 , \(2<q<p< 2^{*}(s_1)\) 2 < q < p < 2 ( s 1 ) , \(q\le 2^{*}(s_2)\) q 2 ( s 2 ) . This paper attempts to study the problem, aiming to provide new research approaches for completely addressing the Li–Lin open problem proposed by Y.Y. Li and C.-S. Lin (Arch. Ration. Mech. Anal. 203(3): 943–968, 2012). Specifically, we focus on its subcritical approximations for q in the range \(2^{*}(s_2)>q>\frac{2-s_2}{2-s_1}p+\frac{2s_2-2s_1}{2-s_1}\) 2 ( s 2 ) > q > 2 - s 2 2 - s 1 p + 2 s 2 - 2 s 1 2 - s 1 . To address the challenge that the energy functional associated with the equation is unbounded below on the Nehari manifold and fails to admit a global minimizer, we establish the existence of a positive solution that serves as a local minimizer of the energy functional on this manifold. Additionally, we investigate the asymptotic behavior of the positive solution and, through blow-up analysis, identify a new class of blow-up points located on the domain boundary. These boundary blow-up points exhibit distinct characteristics from those commonly reported in the literature.