<p>Let <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(n\ge 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>≥</mo> <mn>2</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>, and <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\Omega \subset \mathbb {R}^n\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ω</mi> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> be a bounded Lipschitz domain. This paper is devoted to the study of Green functions for the fractional Neumann problem <Equation ID="Equ121"> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{aligned} (-\Delta )^su&amp;=f &amp; \text {in}\ \ \Omega ,\\ \mathcal {N}_s u&amp;=0 &amp; \text {in}\ \ \mathbb {R}^n\setminus \Omega , \end{aligned}\right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">)</mo> </mrow> <mi>s</mi> </msup> <mi>u</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <mi>f</mi> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mtext>in</mtext> <mspace width="4pt" /> <mspace width="4pt" /> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow> <mrow /> <msub> <mi mathvariant="script">N</mi> <mi>s</mi> </msub> <mi>u</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <mn>0</mn> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mtext>in</mtext> <mspace width="4pt" /> <mspace width="4pt" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo lspace="0.15em" rspace="0.15em" stretchy="false">\</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>and the regional fractional Neumann problem <Equation ID="Equ122"> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{aligned} (-\Delta )^s_\Omega u&amp;=f &amp; \text {in}\ \ \Omega ,\\ \partial ^{2s-1}_{\varvec{\nu }} u&amp;=0 &amp; \text {on}\ \ \partial \Omega , \end{aligned}\right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msubsup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">)</mo> </mrow> <mi mathvariant="normal">Ω</mi> <mi>s</mi> </msubsup> <mi>u</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <mi>f</mi> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mtext>in</mtext> <mspace width="4pt" /> <mspace width="4pt" /> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow> <mrow /> <msubsup> <mi>∂</mi> <mrow> <mi mathvariant="bold-italic">ν</mi> </mrow> <mrow> <mn>2</mn> <mi>s</mi> <mo>-</mo> <mn>1</mn> </mrow> </msubsup> <mi>u</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <mn>0</mn> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mtext>on</mtext> <mspace width="4pt" /> <mspace width="4pt" /> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>often referred to as Neumann functions. Here, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\mathcal {N}_s\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">N</mi> <mi>s</mi> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\partial ^{2s-1}_{\varvec{\nu }}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>∂</mi> <mrow> <mi mathvariant="bold-italic">ν</mi> </mrow> <mrow> <mn>2</mn> <mi>s</mi> <mo>-</mo> <mn>1</mn> </mrow> </msubsup> </math></EquationSource> </InlineEquation> denote the nonlocal normal derivative in <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\mathbb {R}^n\setminus \Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo lspace="0.15em" rspace="0.15em" stretchy="false">\</mo> <mi mathvariant="normal">Ω</mi> </mrow> </math></EquationSource> </InlineEquation> and the fractional normal derivative on <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\partial \Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> </mrow> </math></EquationSource> </InlineEquation> respectively. Precisely, we establish the existence and uniqueness of Neumann functions for the fractional Neumann problem and the regional fractional Neumann problem respectively. Moreover, we also obtain global pointwise upper bound estimates, fractional Sobolev type estimates, and Hölder continuity estimates for such Neumann functions. Furthermore, a representation formula for the weak solution to the nonhomogeneous (regional) fractional Neumann problem is obtained by using the Neumann function.</p>

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Neumann functions for the fractional Laplace equations on Lipschitz domains

  • Wenxian Ma,
  • Sibei Yang

摘要

Let \(n\ge 2\) n 2 , \(s\in (0,1)\) s ( 0 , 1 ) , and \(\Omega \subset \mathbb {R}^n\) Ω R n be a bounded Lipschitz domain. This paper is devoted to the study of Green functions for the fractional Neumann problem \(\begin{aligned} \left\{ \begin{aligned} (-\Delta )^su&=f & \text {in}\ \ \Omega ,\\ \mathcal {N}_s u&=0 & \text {in}\ \ \mathbb {R}^n\setminus \Omega , \end{aligned}\right. \end{aligned}\) ( - Δ ) s u = f in Ω , N s u = 0 in R n \ Ω , and the regional fractional Neumann problem \(\begin{aligned} \left\{ \begin{aligned} (-\Delta )^s_\Omega u&=f & \text {in}\ \ \Omega ,\\ \partial ^{2s-1}_{\varvec{\nu }} u&=0 & \text {on}\ \ \partial \Omega , \end{aligned}\right. \end{aligned}\) ( - Δ ) Ω s u = f in Ω , ν 2 s - 1 u = 0 on Ω , often referred to as Neumann functions. Here, \(\mathcal {N}_s\) N s and \(\partial ^{2s-1}_{\varvec{\nu }}\) ν 2 s - 1 denote the nonlocal normal derivative in \(\mathbb {R}^n\setminus \Omega \) R n \ Ω and the fractional normal derivative on \(\partial \Omega \) Ω respectively. Precisely, we establish the existence and uniqueness of Neumann functions for the fractional Neumann problem and the regional fractional Neumann problem respectively. Moreover, we also obtain global pointwise upper bound estimates, fractional Sobolev type estimates, and Hölder continuity estimates for such Neumann functions. Furthermore, a representation formula for the weak solution to the nonhomogeneous (regional) fractional Neumann problem is obtained by using the Neumann function.