<p>We extend the celebrate global compactness result of Struwe (Math Z 187:511–517, 1984) to a class of critical nonlinear problems involving the spectral fractional Laplacian with mixed Dirichlet–Neumann boundary conditions. We study the behavior of the non-negative sequences failing the Palais–Smale condition for the energy functional associated with the problem: <Equation ID="Equ32"> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{array}{lll} (-\Delta )^s u =|u|^{\frac{4s}{n-2s}}u , \, \hspace{71.13188pt} \text{ in } \Omega ,\\ \\ \displaystyle \hspace{11.38092pt}\mathscr {B}(u) := 1_{\Gamma _0}u+1_{\Gamma _1}\dfrac{\partial u}{\partial \nu }=0 \hspace{11.38092pt} \text{ on } \partial \Omega ,\\ \end{array} \right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <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> <mo>=</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mfrac> <mrow> <mn>4</mn> <mi>s</mi> </mrow> <mrow> <mi>n</mi> <mo>-</mo> <mn>2</mn> <mi>s</mi> </mrow> </mfrac> </msup> <mi>u</mi> <mo>,</mo> <mspace width="0.166667em" /> <mspace width="71.13188pt" /> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow /> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mstyle displaystyle="true" scriptlevel="0"> <mrow> <mrow /> <mspace width="11.38092pt" /> <mi mathvariant="script">B</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>:</mo> <mo>=</mo> <msub> <mn>1</mn> <msub> <mi mathvariant="normal">Γ</mi> <mn>0</mn> </msub> </msub> <mi>u</mi> <mo>+</mo> <msub> <mn>1</mn> <msub> <mi mathvariant="normal">Γ</mi> <mn>1</mn> </msub> </msub> <mstyle displaystyle="true" scriptlevel="0"> <mfrac> <mrow> <mi>∂</mi> <mi>u</mi> </mrow> <mrow> <mi>∂</mi> <mi>ν</mi> </mrow> </mfrac> </mstyle> <mo>=</mo> <mn>0</mn> <mspace width="11.38092pt" /> <mspace width="0.333333em" /> <mtext>on</mtext> <mspace width="0.333333em" /> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mstyle> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(s\in (1/2,1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>1</mn> <mo stretchy="false">/</mo> <mn>2</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\Omega \subset \mathbb {R}^n, n\ge 2\)</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> <mo>,</mo> <mi>n</mi> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, is a bounded domain whose boundary <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\partial \Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> </mrow> </math></EquationSource> </InlineEquation> is decomposed into two closed parts <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\overline{\Gamma }_0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mover> <mi mathvariant="normal">Γ</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\overline{\Gamma }_1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mover> <mi mathvariant="normal">Γ</mi> <mo>¯</mo> </mover> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation>. The main theorem of this paper provides, under condition (<i>H</i>) below, an accurate description of any non-convergent Palais–Smale sequence, showing that it converges weakly to a critical point plus a finite sum of “bubbles” that capture the energy loss and concentrate at points in <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\Omega \cup \Gamma _1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ω</mi> <mo>∪</mo> <msub> <mi mathvariant="normal">Γ</mi> <mn>1</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>.</p>

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A global compactness theorem for fractional nonlinear problems with non-homogeneous boundary conditions

  • Mohammed Ali Mohammed Al-Ghamdi,
  • Aymen Bensouf,
  • Hichem Chtioui

摘要

We extend the celebrate global compactness result of Struwe (Math Z 187:511–517, 1984) to a class of critical nonlinear problems involving the spectral fractional Laplacian with mixed Dirichlet–Neumann boundary conditions. We study the behavior of the non-negative sequences failing the Palais–Smale condition for the energy functional associated with the problem: \(\begin{aligned} \left\{ \begin{array}{lll} (-\Delta )^s u =|u|^{\frac{4s}{n-2s}}u , \, \hspace{71.13188pt} \text{ in } \Omega ,\\ \\ \displaystyle \hspace{11.38092pt}\mathscr {B}(u) := 1_{\Gamma _0}u+1_{\Gamma _1}\dfrac{\partial u}{\partial \nu }=0 \hspace{11.38092pt} \text{ on } \partial \Omega ,\\ \end{array} \right. \end{aligned}\) ( - Δ ) s u = | u | 4 s n - 2 s u , in Ω , B ( u ) : = 1 Γ 0 u + 1 Γ 1 u ν = 0 on Ω , where \(s\in (1/2,1)\) s ( 1 / 2 , 1 ) and \(\Omega \subset \mathbb {R}^n, n\ge 2\) Ω R n , n 2 , is a bounded domain whose boundary \(\partial \Omega \) Ω is decomposed into two closed parts \(\overline{\Gamma }_0\) Γ ¯ 0 and \(\overline{\Gamma }_1\) Γ ¯ 1 . The main theorem of this paper provides, under condition (H) below, an accurate description of any non-convergent Palais–Smale sequence, showing that it converges weakly to a critical point plus a finite sum of “bubbles” that capture the energy loss and concentrate at points in \(\Omega \cup \Gamma _1\) Ω Γ 1 .