<p>This paper is devoted to study the slightly subcritical problem with double nonlocal terms <Equation ID="Equ47"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1123_Article_Equ47.gif" Format="GIF" Height="87" Rendition="HTML" Resolution="72" Type="Linedraw" Width="388" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{array}{ll} \displaystyle {(-\Delta )^{s}u=\bigg (\int _{\Omega }\frac{u^{2^{*}_{\alpha ,s}-\varepsilon }(y)}{|x-y|^{\alpha }}dy\bigg ) u^{2^{*}_{\alpha ,s}-1-\varepsilon }}, &amp; \text { in } \Omega ,\\ u&gt;0, &amp; \text { in } \Omega ,\\ u=0, &amp; \text { in } {\mathbb {R}}^{N}\setminus \Omega , \end{array}\right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mstyle displaystyle="true" scriptlevel="0"> <mrow> <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> <mrow> <mo maxsize="2.047em" minsize="2.047em" stretchy="true">(</mo> </mrow> <msub> <mo>∫</mo> <mi mathvariant="normal">Ω</mi> </msub> <mfrac> <mrow> <mmultiscripts> <mi>u</mi> <mrow /> <mrow> <mmultiscripts> <mn>2</mn> <mrow> <mi>α</mi> <mo>,</mo> <mi>s</mi> </mrow> <mrow> <mrow /> <mo>∗</mo> </mrow> </mmultiscripts> <mo>-</mo> <mi>ε</mi> </mrow> </mmultiscripts> <mrow> <mo stretchy="false">(</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> </mrow> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo>-</mo> <mi>y</mi> <mo stretchy="false">|</mo> </mrow> <mi>α</mi> </msup> </mfrac> <mi>d</mi> <mi>y</mi> <mrow> <mo maxsize="2.047em" minsize="2.047em" stretchy="true">)</mo> </mrow> <mmultiscripts> <mi>u</mi> <mrow /> <mrow> <mmultiscripts> <mn>2</mn> <mrow> <mi>α</mi> <mo>,</mo> <mi>s</mi> </mrow> <mrow> <mrow /> <mo>∗</mo> </mrow> </mmultiscripts> <mo>-</mo> <mn>1</mn> <mo>-</mo> <mi>ε</mi> </mrow> </mmultiscripts> </mrow> <mo>,</mo> </mrow> </mstyle> </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>&gt;</mo> <mn>0</mn> <mo>,</mo> </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> <mo>,</mo> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <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>where <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1123_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="58" /> </InlineMediaObject> <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> (with <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1123_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\(C^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>C</mi> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation> boundary regularity) is a smooth bounded domain with <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1123_Article_IEq3.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="57" /> </InlineMediaObject> <EquationSource Format="TEX">\(N&gt;2s\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>&gt;</mo> <mn>2</mn> <mi>s</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1123_Article_IEq4.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="151" /> </InlineMediaObject> <EquationSource Format="TEX">\(s\in (0,\min \{1,\frac{3N-2}{6}\})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mo movablelimits="true">min</mo> <mrow> <mo stretchy="false">{</mo> <mn>1</mn> <mo>,</mo> <mfrac> <mrow> <mn>3</mn> <mi>N</mi> <mo>-</mo> <mn>2</mn> </mrow> <mn>6</mn> </mfrac> <mo stretchy="false">}</mo> </mrow> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1123_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="144" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha \in (0,\min \{4s,N\})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mo movablelimits="true">min</mo> <mo stretchy="false">{</mo> <mn>4</mn> <mi>s</mi> <mo>,</mo> <mi>N</mi> <mo stretchy="false">}</mo> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1123_Article_IEq6.gif" Format="GIF" Height="24" Rendition="HTML" Resolution="72" Type="Linedraw" Width="84" /> </InlineMediaObject> <EquationSource Format="TEX">\(2^{*}_{\alpha ,s}=\frac{2N-\alpha }{N-2s}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mn>2</mn> <mrow> <mi>α</mi> <mo>,</mo> <mi>s</mi> </mrow> <mrow> <mrow /> <mo>∗</mo> </mrow> </mmultiscripts> <mo>=</mo> <mfrac> <mrow> <mn>2</mn> <mi>N</mi> <mo>-</mo> <mi>α</mi> </mrow> <mrow> <mi>N</mi> <mo>-</mo> <mn>2</mn> <mi>s</mi> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation> is the upper critical exponent in the sense of the Hardy-Littlewood-Sobolev inequality, and <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1123_Article_IEq7.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="40" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varepsilon &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ε</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> is a small parameter. Using the finite-dimensional reduction method, we construct a solution for the above problem which concentrates around the local minimum point of the Robin function as <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1123_Article_IEq8.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="11" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varepsilon \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ε</mi> </math></EquationSource> </InlineEquation> goes to zero.</p>

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Existence of solutions for a slightly subcritical fractional Choquard problem

  • Shengbing Deng,
  • Wenshan Luo

摘要

This paper is devoted to study the slightly subcritical problem with double nonlocal terms \(\begin{aligned} \left\{ \begin{array}{ll} \displaystyle {(-\Delta )^{s}u=\bigg (\int _{\Omega }\frac{u^{2^{*}_{\alpha ,s}-\varepsilon }(y)}{|x-y|^{\alpha }}dy\bigg ) u^{2^{*}_{\alpha ,s}-1-\varepsilon }}, & \text { in } \Omega ,\\ u>0, & \text { in } \Omega ,\\ u=0, & \text { in } {\mathbb {R}}^{N}\setminus \Omega , \end{array}\right. \end{aligned}\) ( - Δ ) s u = ( Ω u 2 α , s - ε ( y ) | x - y | α d y ) u 2 α , s - 1 - ε , in Ω , u > 0 , in Ω , u = 0 , in R N \ Ω , where \(\Omega \subset {\mathbb {R}}^{N}\) Ω R N (with \(C^2\) C 2 boundary regularity) is a smooth bounded domain with \(N>2s\) N > 2 s , \(s\in (0,\min \{1,\frac{3N-2}{6}\})\) s ( 0 , min { 1 , 3 N - 2 6 } ) , \(\alpha \in (0,\min \{4s,N\})\) α ( 0 , min { 4 s , N } ) , \(2^{*}_{\alpha ,s}=\frac{2N-\alpha }{N-2s}\) 2 α , s = 2 N - α N - 2 s is the upper critical exponent in the sense of the Hardy-Littlewood-Sobolev inequality, and \(\varepsilon >0\) ε > 0 is a small parameter. Using the finite-dimensional reduction method, we construct a solution for the above problem which concentrates around the local minimum point of the Robin function as \(\varepsilon \) ε goes to zero.