<p>In this paper, we study a fractional Hardy–Sobolev problem with a concave nonlinearity&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0;&#xa0; <Equation ID="Equ71"> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{array}{ll} (-\Delta )^\alpha u= \vert u\vert ^{2_\alpha ^{*}-2} u +\frac{\vert u\vert ^{2_\alpha ^{*}(s)-2}u}{\vert x\vert ^{s}}+ \lambda \vert u\vert ^{q-2}u &amp; \text{ in } \Omega , \\ u=0 &amp; \text{ on } \partial \Omega , \end{array}\right. \end{aligned}\)</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>α</mi> </msup> <mi>u</mi> <mo>=</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <msubsup> <mn>2</mn> <mi>α</mi> <mrow> <mrow /> <mo>∗</mo> </mrow> </msubsup> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>+</mo> <mfrac> <mrow> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <msubsup> <mn>2</mn> <mi>α</mi> <mrow> <mrow /> <mo>∗</mo> </mrow> </msubsup> <mrow> <mo stretchy="false">(</mo> <mi>s</mi> <mo stretchy="false">)</mo> </mrow> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> </mrow> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mi>s</mi> </msup> </mfrac> <mo>+</mo> <mi>λ</mi> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>q</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <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> <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> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(N \ge 4\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>≥</mo> <mn>4</mn> <mi>α</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(0&lt;\alpha &lt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>α</mi> <mo>&lt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(0&lt;s&lt;2\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>s</mi> <mo>&lt;</mo> <mn>2</mn> <mi>α</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(1&lt;q\le 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>&lt;</mo> <mi>q</mi> <mo>≤</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\lambda &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq6"> <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> is a bounded domain satisfying suitable geometric conditions. We introduce subcritical perturbations of this problem and prove the strong convergence of any bounded sequence of solutions in the associated fractional Sobolev space, based on estimates in fractional safe regions combined with a localized Pohozaev-type identity. As a consequence, we obtain multiplicity results. In the case <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(1&lt;q&lt;2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>&lt;</mo> <mi>q</mi> <mo>&lt;</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, the problem admits infinitely many solutions with negative energy, while for <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(1&lt;q\le 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>&lt;</mo> <mi>q</mi> <mo>≤</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, there exist infinitely many solutions with positive energy tending to <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(+\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>+</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Fractional Elliptic Equations with Combined Sobolev and Hardy–Sobolev Critical Exponents and Concave Nonlinearity: Compactness and Infinitely Many Solutions

  • Rachid Echarghaoui,
  • Mohamed Masmodi

摘要

In this paper, we study a fractional Hardy–Sobolev problem with a concave nonlinearity                                                                         \(\begin{aligned} \left\{ \begin{array}{ll} (-\Delta )^\alpha u= \vert u\vert ^{2_\alpha ^{*}-2} u +\frac{\vert u\vert ^{2_\alpha ^{*}(s)-2}u}{\vert x\vert ^{s}}+ \lambda \vert u\vert ^{q-2}u & \text{ in } \Omega , \\ u=0 & \text{ on } \partial \Omega , \end{array}\right. \end{aligned}\) ( - Δ ) α u = | u | 2 α - 2 u + | u | 2 α ( s ) - 2 u | x | s + λ | u | q - 2 u in Ω , u = 0 on Ω , where \(N \ge 4\alpha \) N 4 α , \(0<\alpha <1\) 0 < α < 1 , \(0<s<2\alpha \) 0 < s < 2 α , \(1<q\le 2\) 1 < q 2 , \(\lambda >0\) λ > 0 , and \(\Omega \subset \mathbb {R}^N\) Ω R N is a bounded domain satisfying suitable geometric conditions. We introduce subcritical perturbations of this problem and prove the strong convergence of any bounded sequence of solutions in the associated fractional Sobolev space, based on estimates in fractional safe regions combined with a localized Pohozaev-type identity. As a consequence, we obtain multiplicity results. In the case \(1<q<2\) 1 < q < 2 , the problem admits infinitely many solutions with negative energy, while for \(1<q\le 2\) 1 < q 2 , there exist infinitely many solutions with positive energy tending to \(+\infty \) + .