<p>This article concerns the existence of multi-bump positive solutions for a class of fractional Schrödinger-Poisson system involving logarithmic nonlinearity <Equation ID="Equ45"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2014_Article_Equ45.gif" Format="GIF" Height="44" Rendition="HTML" Resolution="72" Type="Linedraw" Width="338" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{array}{ll} \left( -\Delta \right) ^{s} u+\lambda V(x)u-\phi u= u \log {u^{2}}&amp; \quad \text { in }\mathbb {R}^{3}, \\ \left( -\Delta \right) ^{t}\phi =u^{2}&amp; \quad \text { in }\mathbb {R}^{3}, \\ \end{array} \right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <msup> <mfenced close=")" open="("> <mo>-</mo> <mi mathvariant="normal">Δ</mi> </mfenced> <mi>s</mi> </msup> <mi>u</mi> <mo>+</mo> <mi>λ</mi> <mi>V</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mi>u</mi> <mo>-</mo> <mi>ϕ</mi> <mi>u</mi> <mo>=</mo> <mi>u</mi> <mo>log</mo> <msup> <mi>u</mi> <mn>2</mn> </msup> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="1em" /> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <msup> <mfenced close=")" open="("> <mo>-</mo> <mi mathvariant="normal">Δ</mi> </mfenced> <mi>t</mi> </msup> <mi>ϕ</mi> <mo>=</mo> <msup> <mi>u</mi> <mn>2</mn> </msup> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="1em" /> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2014_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="80" /> </InlineMediaObject> <EquationSource Format="TEX">\(s,t\in (0,1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>,</mo> <mi>t</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2014_Article_IEq2.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="82" /> </InlineMediaObject> <EquationSource Format="TEX">\(4s+2t\ge 3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>4</mn> <mi>s</mi> <mo>+</mo> <mn>2</mn> <mi>t</mi> <mo>≥</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation> and the nonnegative continuous function <i>V</i> has the deepening potential well <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2014_Article_IEq3.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="73" /> </InlineMediaObject> <EquationSource Format="TEX">\(int V^{-1}(0)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>i</mi> <mi>n</mi> <mi>t</mi> <msup> <mi>V</mi> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> consisting of <i>k</i> disjoint components <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2014_Article_IEq4.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="106" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Omega _{1},\Omega _{2}, \cdots ,\Omega _{k}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="normal">Ω</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi mathvariant="normal">Ω</mi> <mn>2</mn> </msub> <mo>,</mo> <mo>⋯</mo> <mo>,</mo> <msub> <mi mathvariant="normal">Ω</mi> <mi>k</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>. By applying suitable variational arguments, we analyze that the system has at least <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2014_Article_IEq5.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\(2^{k}-1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mn>2</mn> <mi>k</mi> </msup> <mo>-</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> multi-bump positive solutions as the parameter <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2014_Article_IEq6.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <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 large enough.</p>

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Multi-bump Solutions for a Logarithmic Fractional Schrödinger-Poisson System with Deepening Potential Well

  • Lin Li,
  • Huo Tao

摘要

This article concerns the existence of multi-bump positive solutions for a class of fractional Schrödinger-Poisson system involving logarithmic nonlinearity \(\begin{aligned} \left\{ \begin{array}{ll} \left( -\Delta \right) ^{s} u+\lambda V(x)u-\phi u= u \log {u^{2}}& \quad \text { in }\mathbb {R}^{3}, \\ \left( -\Delta \right) ^{t}\phi =u^{2}& \quad \text { in }\mathbb {R}^{3}, \\ \end{array} \right. \end{aligned}\) - Δ s u + λ V ( x ) u - ϕ u = u log u 2 in R 3 , - Δ t ϕ = u 2 in R 3 , where \(s,t\in (0,1)\) s , t ( 0 , 1 ) , \(4s+2t\ge 3\) 4 s + 2 t 3 and the nonnegative continuous function V has the deepening potential well \(int V^{-1}(0)\) i n t V - 1 ( 0 ) consisting of k disjoint components \(\Omega _{1},\Omega _{2}, \cdots ,\Omega _{k}\) Ω 1 , Ω 2 , , Ω k . By applying suitable variational arguments, we analyze that the system has at least \(2^{k}-1\) 2 k - 1 multi-bump positive solutions as the parameter \(\lambda >0\) λ > 0 is large enough.