<p>In this paper, we consider a critical Choquard-type Brezis-Nirenberg problem in a smooth bounded domain <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\Omega \subset \mathbb {R}^3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ω</mi> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> </mrow> </math></EquationSource> </InlineEquation>, which extends the classical local Brezis-Nirenberg problem to a nonlocal setting via a Hardy-Littlewood-Sobolev (HLS) convolution term. The problem is given by <Equation ID="Equ41"> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{array}{ll} -\Delta u=\displaystyle \Big (\int _{\Omega }\frac{u^{2_\alpha ^*}(y)}{|x-y|^\alpha }dy\Big )|u|^{2_\alpha ^*-2}u+\lambda u, \ \ &amp; \text{ in }\ \Omega ,\\ u&gt;0, \ \ &amp; \text{ in }\ \Omega ,\\ u=0, \ \ &amp; \text{ on }\ \partial \Omega , \end{array} \right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mstyle displaystyle="true" scriptlevel="0"> <mrow> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>=</mo> <mrow> <mo maxsize="1.623em" minsize="1.623em" stretchy="true">(</mo> </mrow> <msub> <mo>∫</mo> <mi mathvariant="normal">Ω</mi> </msub> <mfrac> <mrow> <msup> <mi>u</mi> <msubsup> <mn>2</mn> <mi>α</mi> <mo>∗</mo> </msubsup> </msup> <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="1.623em" minsize="1.623em" stretchy="true">)</mo> </mrow> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <msubsup> <mn>2</mn> <mi>α</mi> <mo>∗</mo> </msubsup> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>+</mo> <mi>λ</mi> <mi>u</mi> <mo>,</mo> <mspace width="4pt" /> <mspace width="4pt" /> </mrow> </mstyle> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mspace width="4pt" /> <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> <mspace width="4pt" /> <mspace width="4pt" /> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mspace width="4pt" /> <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> <mspace width="4pt" /> <mspace width="4pt" /> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>on</mtext> <mspace width="0.333333em" /> <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>where <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(2_\alpha ^*=\frac{2N-\alpha }{N-2}=6-\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mn>2</mn> <mi>α</mi> <mo>∗</mo> </msubsup> <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> </mrow> </mfrac> <mo>=</mo> <mn>6</mn> <mo>-</mo> <mi>α</mi> </mrow> </math></EquationSource> </InlineEquation> (the upper critical exponent in the sense of the HLS inequality for <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(N=3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>=</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation>), <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\alpha \in (0,3)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>3</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, and <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> is a parameter. By using the Lyapunov-Schmidt reduction, we establish the existence of multiple blowing-up solutions that concentrate simultaneously around <i>k</i> distict points of <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Ω</mi> </math></EquationSource> </InlineEquation> as <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation> approaches a special value <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\lambda _0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>λ</mi> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation>, which is characterized by the Green function of <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(-\Delta -\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mo>-</mo> <mi>λ</mi> </mrow> </math></EquationSource> </InlineEquation>. We further extend this result to the corresponding Neumann boundary value problem. Our work fills the gap in the study of multiple blowing-up solutions for critical nonlocal Choquard equations, complementing existing results on single-bubble solutions and extending the determinant-based multi-bubble construction from local Brezis-Nirenberg problems to nonlocal settings.</p>

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Multiple blowing-up solutions for the Choquard type Brezis-Nirenberg problem in dimension three

  • Wenjing Chen,
  • Zexi Wang

摘要

In this paper, we consider a critical Choquard-type Brezis-Nirenberg problem in a smooth bounded domain \(\Omega \subset \mathbb {R}^3\) Ω R 3 , which extends the classical local Brezis-Nirenberg problem to a nonlocal setting via a Hardy-Littlewood-Sobolev (HLS) convolution term. The problem is given by \(\begin{aligned} \left\{ \begin{array}{ll} -\Delta u=\displaystyle \Big (\int _{\Omega }\frac{u^{2_\alpha ^*}(y)}{|x-y|^\alpha }dy\Big )|u|^{2_\alpha ^*-2}u+\lambda u, \ \ & \text{ in }\ \Omega ,\\ u>0, \ \ & \text{ in }\ \Omega ,\\ u=0, \ \ & \text{ on }\ \partial \Omega , \end{array} \right. \end{aligned}\) - Δ u = ( Ω u 2 α ( y ) | x - y | α d y ) | u | 2 α - 2 u + λ u , in Ω , u > 0 , in Ω , u = 0 , on Ω , where \(2_\alpha ^*=\frac{2N-\alpha }{N-2}=6-\alpha \) 2 α = 2 N - α N - 2 = 6 - α (the upper critical exponent in the sense of the HLS inequality for \(N=3\) N = 3 ), \(\alpha \in (0,3)\) α ( 0 , 3 ) , and \(\lambda >0\) λ > 0 is a parameter. By using the Lyapunov-Schmidt reduction, we establish the existence of multiple blowing-up solutions that concentrate simultaneously around k distict points of \(\Omega \) Ω as \(\lambda \) λ approaches a special value \(\lambda _0\) λ 0 , which is characterized by the Green function of \(-\Delta -\lambda \) - Δ - λ . We further extend this result to the corresponding Neumann boundary value problem. Our work fills the gap in the study of multiple blowing-up solutions for critical nonlocal Choquard equations, complementing existing results on single-bubble solutions and extending the determinant-based multi-bubble construction from local Brezis-Nirenberg problems to nonlocal settings.