<p>We consider the critical Hénon equation <Equation ID="Equ30"> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} -\Delta u=|x|^\alpha |u|^{\frac{4}{N-2}}u\;\;&amp; \text {in}\;B_1,\\ u=0\;\;&amp; \text {on}\;\partial B_1, \end{array}\right. } \end{aligned}\)</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> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mi>α</mi> </msup> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mfrac> <mn>4</mn> <mrow> <mi>N</mi> <mo>-</mo> <mn>2</mn> </mrow> </mfrac> </msup> <mi>u</mi> <mspace width="0.277778em" /> <mspace width="0.277778em" /> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mtext>in</mtext> <mspace width="0.277778em" /> <msub> <mi>B</mi> <mn>1</mn> </msub> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mi>u</mi> <mo>=</mo> <mn>0</mn> <mspace width="0.277778em" /> <mspace width="0.277778em" /> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mtext>on</mtext> <mspace width="0.277778em" /> <mi>∂</mi> <msub> <mi>B</mi> <mn>1</mn> </msub> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\alpha &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(B_1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>B</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> is the unit ball centered at the origin in <InlineEquation ID="IEq3"> <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="IEq4"> <EquationSource Format="TEX">\(N\ge 3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>≥</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation>. It is well-known that the above problem admits a unique positive radial solution <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(u_\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>u</mi> <mi>α</mi> </msub> </math></EquationSource> </InlineEquation>. We first study the asymptotic behavior of <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(u_\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>u</mi> <mi>α</mi> </msub> </math></EquationSource> </InlineEquation> as <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\alpha \rightarrow 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo stretchy="false">→</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, which highlights a new interesting phenomenon of the Hénon equation and provides an affirmative answer to Hirano’s conjecture in 2009. Furthermore, we show that if <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation> is small enough, <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(u_\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>u</mi> <mi>α</mi> </msub> </math></EquationSource> </InlineEquation> is non-degenerate and the Morse index of <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(u_\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>u</mi> <mi>α</mi> </msub> </math></EquationSource> </InlineEquation> is <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(N+1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>+</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>. These show the qualitative properties of <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(u_\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>u</mi> <mi>α</mi> </msub> </math></EquationSource> </InlineEquation> are significantly different from those of solutions to power subcritical elliptic problem.</p><p>Based on above qualitative results, we can build infinitely many non-radial sign-changing bubbling solutions to the critical Hénon equation in <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\mathbb {R}^5\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>5</mn> </msup> </math></EquationSource> </InlineEquation>, whose energy can be arbitrarily large. It seems that this is the first existence result of non-radial sign-changing solutions to the critical Hénon equation.</p>

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Some new observations on the Hénon equation with critical Sobolev exponent

  • Zhongyuan Liu,
  • Peng Luo

摘要

We consider the critical Hénon equation \(\begin{aligned} {\left\{ \begin{array}{ll} -\Delta u=|x|^\alpha |u|^{\frac{4}{N-2}}u\;\;& \text {in}\;B_1,\\ u=0\;\;& \text {on}\;\partial B_1, \end{array}\right. } \end{aligned}\) - Δ u = | x | α | u | 4 N - 2 u in B 1 , u = 0 on B 1 , where \(\alpha >0\) α > 0 , \(B_1\) B 1 is the unit ball centered at the origin in \(\mathbb {R}^N\) R N , \(N\ge 3\) N 3 . It is well-known that the above problem admits a unique positive radial solution \(u_\alpha \) u α . We first study the asymptotic behavior of \(u_\alpha \) u α as \(\alpha \rightarrow 0\) α 0 , which highlights a new interesting phenomenon of the Hénon equation and provides an affirmative answer to Hirano’s conjecture in 2009. Furthermore, we show that if \(\alpha \) α is small enough, \(u_\alpha \) u α is non-degenerate and the Morse index of \(u_\alpha \) u α is \(N+1\) N + 1 . These show the qualitative properties of \(u_\alpha \) u α are significantly different from those of solutions to power subcritical elliptic problem.

Based on above qualitative results, we can build infinitely many non-radial sign-changing bubbling solutions to the critical Hénon equation in \(\mathbb {R}^5\) R 5 , whose energy can be arbitrarily large. It seems that this is the first existence result of non-radial sign-changing solutions to the critical Hénon equation.