<p>In this paper, we consider the following Schrödinger–Poisson system <Equation ID="Equ85"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2024_1895_Article_Equ85.gif" Format="GIF" Height="43" Rendition="HTML" Resolution="72" Type="Linedraw" Width="330" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} -\Delta u+u+\Phi (y)u=Q_n(y)|u|^{p-2}u, \hspace{3mm}y \in {\mathbb {R}}^3,\\ -\Delta \Phi (y) =u^2, \hspace{3mm}y \in {\mathbb {R}}^3, \end{array}\right. } \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>+</mo> <mi>u</mi> <mo>+</mo> <mi mathvariant="normal">Φ</mi> <mrow> <mo stretchy="false">(</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> <mi>u</mi> <mo>=</mo> <msub> <mi>Q</mi> <mi>n</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> <msup> <mrow> <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> <mspace width="8.53581pt" /> <mi>y</mi> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi mathvariant="normal">Φ</mi> <mrow> <mo stretchy="false">(</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msup> <mi>u</mi> <mn>2</mn> </msup> <mo>,</mo> <mspace width="8.53581pt" /> <mi>y</mi> <mo>∈</mo> <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_2024_1895_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="68" /> </InlineMediaObject> <EquationSource Format="TEX">\(p\in (4,6)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>4</mn> <mo>,</mo> <mn>6</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2024_1895_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="TEX">\(Q_n\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>Q</mi> <mi>n</mi> </msub> </math></EquationSource> </InlineEquation> are concrete bounded functions whose self-focusing core <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2024_1895_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="80" /> </InlineMediaObject> <EquationSource Format="TEX">\(supp\{Q_n^+\}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mi>u</mi> <mi>p</mi> <mi>p</mi> <mo stretchy="false">{</mo> <msubsup> <mi>Q</mi> <mi>n</mi> <mo>+</mo> </msubsup> <mo stretchy="false">}</mo> </mrow> </math></EquationSource> </InlineEquation> shrinks to a finite set of points as <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2024_1895_Article_IEq4.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="58" /> </InlineMediaObject> <EquationSource Format="TEX">\(n\rightarrow \infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo stretchy="false">→</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>. We prove the existence of positive ground state solution <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2024_1895_Article_IEq5.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(u_n\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>u</mi> <mi>n</mi> </msub> </math></EquationSource> </InlineEquation> corresponding to <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2024_1895_Article_IEq6.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="TEX">\(Q_n\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>Q</mi> <mi>n</mi> </msub> </math></EquationSource> </InlineEquation> and study the limiting profile of <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2024_1895_Article_IEq7.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(u_n\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>u</mi> <mi>n</mi> </msub> </math></EquationSource> </InlineEquation> as <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2024_1895_Article_IEq8.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="58" /> </InlineMediaObject> <EquationSource Format="TEX">\(n\rightarrow \infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo stretchy="false">→</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>. We also prove the existence of localized bound state solutions for above Schrödinger–Poisson system by using penalization method. Moreover, by using Green’s representation formula, we improve the result in [<CitationRef CitationID="CR14">14</CitationRef>, Theorem 1.3] for nonlinear Schrödinger equation.</p>

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Limiting Profile of Solutions for Schrödinger–Poisson System with Shrinking Self-Focusing Core

  • Wei Shuai,
  • Jianghua Ye

摘要

In this paper, we consider the following Schrödinger–Poisson system \(\begin{aligned} {\left\{ \begin{array}{ll} -\Delta u+u+\Phi (y)u=Q_n(y)|u|^{p-2}u, \hspace{3mm}y \in {\mathbb {R}}^3,\\ -\Delta \Phi (y) =u^2, \hspace{3mm}y \in {\mathbb {R}}^3, \end{array}\right. } \end{aligned}\) - Δ u + u + Φ ( y ) u = Q n ( y ) | u | p - 2 u , y R 3 , - Δ Φ ( y ) = u 2 , y R 3 , where \(p\in (4,6)\) p ( 4 , 6 ) and \(Q_n\) Q n are concrete bounded functions whose self-focusing core \(supp\{Q_n^+\}\) s u p p { Q n + } shrinks to a finite set of points as \(n\rightarrow \infty \) n . We prove the existence of positive ground state solution \(u_n\) u n corresponding to \(Q_n\) Q n and study the limiting profile of \(u_n\) u n as \(n\rightarrow \infty \) n . We also prove the existence of localized bound state solutions for above Schrödinger–Poisson system by using penalization method. Moreover, by using Green’s representation formula, we improve the result in [14, Theorem 1.3] for nonlinear Schrödinger equation.