<p>We consider the following semilinear elliptic equation involving the fractional Laplacian <Equation ID="Equ49"> <EquationSource Format="TEX">\(\begin{aligned} (-\triangle )^su=-u^{-p} \hbox { in } B_1, \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi>▵</mi> <mo stretchy="false">)</mo> </mrow> <mi>s</mi> </msup> <mi>u</mi> <mo>=</mo> <mo>-</mo> <msup> <mi>u</mi> <mrow> <mo>-</mo> <mi>p</mi> </mrow> </msup> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <msub> <mi>B</mi> <mn>1</mn> </msub> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(p&gt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>&gt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(s\in (0,1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\((-\triangle )^s\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi>▵</mi> <mo stretchy="false">)</mo> </mrow> <mi>s</mi> </msup> </math></EquationSource> </InlineEquation> is the <i>s</i>-Laplacian and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(B_1=B_1(0)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>B</mi> <mn>1</mn> </msub> <mo>=</mo> <msub> <mi>B</mi> <mn>1</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is the unit ball in <InlineEquation ID="IEq5"> <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>. We first establish an optimal Hölder regularity estimate for solutions by using blow-up analysis and Liouville-type theorems. Subsequently, we give a convergence result for sequences of solutions with uniform Hölder continuity. These results are also used to show that the Hausdorff dimension of the rupture set <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\{u=0\}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">{</mo> <mi>u</mi> <mo>=</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> </math></EquationSource> </InlineEquation> satisfies: <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\dim _{\mathcal {H}} \{u=0\} \le N-2 \hbox { if } \frac{p+1}{2p}&lt;s&lt;1;\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mo>dim</mo> <mi mathvariant="script">H</mi> </msub> <mrow> <mo stretchy="false">{</mo> <mi>u</mi> <mo>=</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> <mo>≤</mo> <mi>N</mi> <mo>-</mo> <mn>2</mn> <mspace width="0.333333em" /> <mtext>if</mtext> <mspace width="0.333333em" /> <mfrac> <mrow> <mi>p</mi> <mo>+</mo> <mn>1</mn> </mrow> <mrow> <mn>2</mn> <mi>p</mi> </mrow> </mfrac> <mo>&lt;</mo> <mi>s</mi> <mo>&lt;</mo> <mn>1</mn> <mo>;</mo> </mrow> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\dim _{\mathcal {H}} \{u=0\} \le N-1 \hbox { if } 0&lt;s\le \frac{p+1}{2p}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mo>dim</mo> <mi mathvariant="script">H</mi> </msub> <mrow> <mo stretchy="false">{</mo> <mi>u</mi> <mo>=</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> <mo>≤</mo> <mi>N</mi> <mo>-</mo> <mn>1</mn> <mspace width="0.333333em" /> <mtext>if</mtext> <mspace width="0.333333em" /> <mn>0</mn> <mo>&lt;</mo> <mi>s</mi> <mo>≤</mo> <mfrac> <mrow> <mi>p</mi> <mo>+</mo> <mn>1</mn> </mrow> <mrow> <mn>2</mn> <mi>p</mi> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation>. In particular, the latter one is a new phenomenon arising from the fractional Laplacian.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Qualitative analysis of rupture set for a semilinear elliptic equation involving the fractional Laplacian

  • Enyu He,
  • Zuhan Liu,
  • Shan Zhang

摘要

We consider the following semilinear elliptic equation involving the fractional Laplacian \(\begin{aligned} (-\triangle )^su=-u^{-p} \hbox { in } B_1, \end{aligned}\) ( - ) s u = - u - p in B 1 , where \(p>1\) p > 1 , \(s\in (0,1)\) s ( 0 , 1 ) , \((-\triangle )^s\) ( - ) s is the s-Laplacian and \(B_1=B_1(0)\) B 1 = B 1 ( 0 ) is the unit ball in \(\mathbb {R}^N\) R N . We first establish an optimal Hölder regularity estimate for solutions by using blow-up analysis and Liouville-type theorems. Subsequently, we give a convergence result for sequences of solutions with uniform Hölder continuity. These results are also used to show that the Hausdorff dimension of the rupture set \(\{u=0\}\) { u = 0 } satisfies: \(\dim _{\mathcal {H}} \{u=0\} \le N-2 \hbox { if } \frac{p+1}{2p}<s<1;\) dim H { u = 0 } N - 2 if p + 1 2 p < s < 1 ; \(\dim _{\mathcal {H}} \{u=0\} \le N-1 \hbox { if } 0<s\le \frac{p+1}{2p}\) dim H { u = 0 } N - 1 if 0 < s p + 1 2 p . In particular, the latter one is a new phenomenon arising from the fractional Laplacian.