<p>In this work, we establish the multiplicity of positive solutions for the following critical fractional Choquard equation with a perturbation on the star-shaped bounded domain <Equation ID="Equ30"> <EquationSource Format="TEX">\(\begin{aligned} \begin{array}{c} (-\Delta )^s u = \lambda u +\alpha |u|^{p-2}u+ \left( \int \limits _{\Omega } \frac{|u(y)|^{2^{*}_{\mu ,s}}}{|x-y|^ \mu }\, dy\right) |u|^{2^{*}_{\mu ,s}-2}u\; \text {in} \; \Omega ,\\ u&gt;0\; \text {in}\; \Omega ,\;\\ u = 0\; \text {in} \; {\mathbb {R}}^{N}\backslash \Omega , \\ \int _{\Omega }|u|^2dx=d, \end{array} \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mtable> <mtr> <mtd> <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> <mi>λ</mi> <mi>u</mi> <mo>+</mo> <msup> <mrow> <mi>α</mi> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>+</mo> <mfenced close=")" open="("> <munder> <mo movablelimits="false">∫</mo> <mi mathvariant="normal">Ω</mi> </munder> <mfrac> <mmultiscripts> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">|</mo> </mrow> <mrow /> <mmultiscripts> <mn>2</mn> <mrow> <mi>μ</mi> <mo>,</mo> <mi>s</mi> </mrow> <mrow> <mrow /> <mo>∗</mo> </mrow> </mmultiscripts> </mmultiscripts> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo>-</mo> <mi>y</mi> <mo stretchy="false">|</mo> </mrow> <mi>μ</mi> </msup> </mfrac> <mspace width="0.166667em" /> <mi>d</mi> <mi>y</mi> </mfenced> <mmultiscripts> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow /> <mrow> <mmultiscripts> <mn>2</mn> <mrow> <mi>μ</mi> <mo>,</mo> <mi>s</mi> </mrow> <mrow> <mrow /> <mo>∗</mo> </mrow> </mmultiscripts> <mo>-</mo> <mn>2</mn> </mrow> </mmultiscripts> <mi>u</mi> <mspace width="0.277778em" /> <mtext>in</mtext> <mspace width="0.277778em" /> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd> <mrow> <mrow /> <mi>u</mi> <mo>&gt;</mo> <mn>0</mn> <mspace width="0.277778em" /> <mtext>in</mtext> <mspace width="0.277778em" /> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mspace width="0.277778em" /> </mrow> </mtd> </mtr> <mtr> <mtd> <mrow> <mrow /> <mi>u</mi> <mo>=</mo> <mn>0</mn> <mspace width="0.277778em" /> <mtext>in</mtext> <mspace width="0.277778em" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mrow> <mo stretchy="true">\</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mrow> </mtd> </mtr> <mtr> <mtd> <mrow> <mrow /> <msub> <mo>∫</mo> <mi mathvariant="normal">Ω</mi> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <mi>d</mi> <mi>x</mi> <mo>=</mo> <mi>d</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(s\in (0,1), N&gt;2s\)</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> <mo>,</mo> <mi>N</mi> <mo>&gt;</mo> <mn>2</mn> <mi>s</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\alpha \in {\mathbb {R}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(d&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>d</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(2&lt;p&lt;2^*_s:=\frac{2N}{N-2s}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>2</mn> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <msubsup> <mn>2</mn> <mi>s</mi> <mo>∗</mo> </msubsup> <mo>:</mo> <mo>=</mo> <mfrac> <mrow> <mn>2</mn> <mi>N</mi> </mrow> <mrow> <mi>N</mi> <mo>-</mo> <mn>2</mn> <mi>s</mi> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(2^{*}_{\mu ,s}:=\frac{2N-\mu }{N-2s}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mn>2</mn> <mrow> <mi>μ</mi> <mo>,</mo> <mi>s</mi> </mrow> <mrow> <mrow /> <mo>∗</mo> </mrow> </mmultiscripts> <mo>:</mo> <mo>=</mo> <mfrac> <mrow> <mn>2</mn> <mi>N</mi> <mo>-</mo> <mi>μ</mi> </mrow> <mrow> <mi>N</mi> <mo>-</mo> <mn>2</mn> <mi>s</mi> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation> represents the fractional Hardy-Littlewood-Sobolev critical exponent. Using the minimization technique over an appropriate set and the uniform mountain pass theorem, we prove the existence of first and second solutions, respectively.</p>

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Normalized solutions for fractional Choquard equation with critical growth on bounded domain

  • Divya Goel,
  • Asmita Rai

摘要

In this work, we establish the multiplicity of positive solutions for the following critical fractional Choquard equation with a perturbation on the star-shaped bounded domain \(\begin{aligned} \begin{array}{c} (-\Delta )^s u = \lambda u +\alpha |u|^{p-2}u+ \left( \int \limits _{\Omega } \frac{|u(y)|^{2^{*}_{\mu ,s}}}{|x-y|^ \mu }\, dy\right) |u|^{2^{*}_{\mu ,s}-2}u\; \text {in} \; \Omega ,\\ u>0\; \text {in}\; \Omega ,\;\\ u = 0\; \text {in} \; {\mathbb {R}}^{N}\backslash \Omega , \\ \int _{\Omega }|u|^2dx=d, \end{array} \end{aligned}\) ( - Δ ) s u = λ u + α | u | p - 2 u + Ω | u ( y ) | 2 μ , s | x - y | μ d y | u | 2 μ , s - 2 u in Ω , u > 0 in Ω , u = 0 in R N \ Ω , Ω | u | 2 d x = d , where \(s\in (0,1), N>2s\) s ( 0 , 1 ) , N > 2 s , \(\alpha \in {\mathbb {R}}\) α R , \(d>0\) d > 0 , \(2<p<2^*_s:=\frac{2N}{N-2s}\) 2 < p < 2 s : = 2 N N - 2 s , and \(2^{*}_{\mu ,s}:=\frac{2N-\mu }{N-2s}\) 2 μ , s : = 2 N - μ N - 2 s represents the fractional Hardy-Littlewood-Sobolev critical exponent. Using the minimization technique over an appropriate set and the uniform mountain pass theorem, we prove the existence of first and second solutions, respectively.