<p>Let <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(B_1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>B</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> denote the unit ball centered at the origin 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> with <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(N = 2 n \ge 4\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>=</mo> <mn>2</mn> <mi>n</mi> <mo>≥</mo> <mn>4</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(p&gt;2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>&gt;</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>. In this work we are interested in finding positive classical nonradial solutions <i>u</i> of <Equation ID="Equ59"> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{array}{ll} -\Delta u(x) + \frac{ \beta x \cdot \nabla u}{|x|^{2+\delta }} = u^{p-1} &amp; \text{ in } B_1 \backslash \{0\}, \\ u=0 &amp; \text{ on } \partial B_1. \\ \end{array}\right. \end{aligned}\)</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> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <mfrac> <mrow> <mi>β</mi> <mi>x</mi> <mo>·</mo> <mi mathvariant="normal">∇</mi> <mi>u</mi> </mrow> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mn>2</mn> <mo>+</mo> <mi>δ</mi> </mrow> </msup> </mfrac> <mo>=</mo> <msup> <mi>u</mi> <mrow> <mi>p</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <msub> <mi>B</mi> <mn>1</mn> </msub> <mrow> <mo stretchy="true">\</mo> <mrow> <mo stretchy="false">{</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> <mo>,</mo> </mrow> </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> <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="IEq5"> <EquationSource Format="TEX">\( \beta &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>β</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\( \delta &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>δ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. Note that for <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\( \delta &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>δ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> the gradient term is supercritical, in the sense that the term <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\( \beta (x \cdot \nabla u)/|x|^{2+\delta } \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>β</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>·</mo> <mi mathvariant="normal">∇</mi> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">/</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mn>2</mn> <mo>+</mo> <mi>δ</mi> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> exhibits a stronger singularity at the origin than in the critical case <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\delta = 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>δ</mi> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Nonradial solutions of a supercritical elliptic problem with supercritical drift

  • A. Aghajani,
  • C. Cowan

摘要

Let \(B_1\) B 1 denote the unit ball centered at the origin in \({\mathbb {R}}^N\) R N with \(N = 2 n \ge 4\) N = 2 n 4 and \(p>2\) p > 2 . In this work we are interested in finding positive classical nonradial solutions u of \(\begin{aligned} \left\{ \begin{array}{ll} -\Delta u(x) + \frac{ \beta x \cdot \nabla u}{|x|^{2+\delta }} = u^{p-1} & \text{ in } B_1 \backslash \{0\}, \\ u=0 & \text{ on } \partial B_1. \\ \end{array}\right. \end{aligned}\) - Δ u ( x ) + β x · u | x | 2 + δ = u p - 1 in B 1 \ { 0 } , u = 0 on B 1 . where \( \beta >0\) β > 0 and \( \delta >0\) δ > 0 . Note that for \( \delta >0\) δ > 0 the gradient term is supercritical, in the sense that the term \( \beta (x \cdot \nabla u)/|x|^{2+\delta } \) β ( x · u ) / | x | 2 + δ exhibits a stronger singularity at the origin than in the critical case \(\delta = 0\) δ = 0 .