<p>The aim of this paper is to investigate the qualitative properties of the multi-peak solution <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2022_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\( u_\varepsilon \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>u</mi> <mi>ε</mi> </msub> </math></EquationSource> </InlineEquation> to the following Schrödinger-Poisson problem: <Equation ID="Equ118"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2022_Article_Equ118.gif" Format="GIF" Height="43" Rendition="HTML" Resolution="72" Type="Linedraw" Width="335" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} -\varepsilon ^{2}\Delta u + V(y)u + \Phi (y)u = |u|^{p-1}u, &amp; y \in \mathbb {R}^3, \\ -\Delta \Phi (y) = u^2, &amp; y \in \mathbb {R}^3, \end{array}\right. } \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <mo>-</mo> <msup> <mi>ε</mi> <mn>2</mn> </msup> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>+</mo> <mi>V</mi> <mrow> <mo stretchy="false">(</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> <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> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mi>u</mi> <mo>,</mo> </mrow> </mtd> <mtd columnalign="left"> <mrow> <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> </mrow> </mtd> <mtd columnalign="left"> <mrow> <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="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2022_Article_IEq2.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, <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2022_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="36" /> </InlineMediaObject> <EquationSource Format="TEX">\( V(y) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>V</mi> <mo stretchy="false">(</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> is a potential function, and <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2022_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="71" /> </InlineMediaObject> <EquationSource Format="TEX">\( 1&lt; p &lt; 5 \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <mn>5</mn> </mrow> </math></EquationSource> </InlineEquation>. Under the assumption that <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2022_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\( \{P_i\}_{i=1}^{m} \)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mrow> <mo stretchy="false">{</mo> <msub> <mi>P</mi> <mi>i</mi> </msub> <mo stretchy="false">}</mo> </mrow> <mrow> <mi>i</mi> <mo>=</mo> <mn>1</mn> </mrow> <mi>m</mi> </msubsup> </math></EquationSource> </InlineEquation> are the non-degenerate critical points of <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2022_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="36" /> </InlineMediaObject> <EquationSource Format="TEX">\( V(y) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>V</mi> <mo stretchy="false">(</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, we derive an explicit formula for the Morse index of <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2022_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\( u_\varepsilon \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>u</mi> <mi>ε</mi> </msub> </math></EquationSource> </InlineEquation>, closely related to the negative eigenvalues of the Hessian matrix <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2022_Article_IEq8.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="64" /> </InlineMediaObject> <EquationSource Format="TEX">\( D^2 V(P_i) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>D</mi> <mn>2</mn> </msup> <mi>V</mi> <mrow> <mo stretchy="false">(</mo> <msub> <mi>P</mi> <mi>i</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. As a consequence, we also establish the non-degeneracy of <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2022_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\( u_\varepsilon \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>u</mi> <mi>ε</mi> </msub> </math></EquationSource> </InlineEquation>. Unlike the classical Schrödinger equation, the presence of the non-local term <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2022_Article_IEq10.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="TEX">\( \Phi (y) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Φ</mi> <mo stretchy="false">(</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> introduces significant challenges in analyzing the asymptotic behavior of the eigenpairs associated with the linearized operator at <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2022_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\( u_\varepsilon \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>u</mi> <mi>ε</mi> </msub> </math></EquationSource> </InlineEquation>, which require precise and advanced analytical techniques.</p>

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Characterization and Behavior of Multi-Peak Solutions for the Schrödinger-Poisson System

  • Qing Guo,
  • Shixin Wen,
  • Jianghua Ye

摘要

The aim of this paper is to investigate the qualitative properties of the multi-peak solution \( u_\varepsilon \) u ε to the following Schrödinger-Poisson problem: \(\begin{aligned} {\left\{ \begin{array}{ll} -\varepsilon ^{2}\Delta u + V(y)u + \Phi (y)u = |u|^{p-1}u, & y \in \mathbb {R}^3, \\ -\Delta \Phi (y) = u^2, & y \in \mathbb {R}^3, \end{array}\right. } \end{aligned}\) - ε 2 Δ u + V ( y ) u + Φ ( y ) u = | u | p - 1 u , y R 3 , - Δ Φ ( y ) = u 2 , y R 3 , where \( \varepsilon > 0 \) ε > 0 is a small parameter, \( V(y) \) V ( y ) is a potential function, and \( 1< p < 5 \) 1 < p < 5 . Under the assumption that \( \{P_i\}_{i=1}^{m} \) { P i } i = 1 m are the non-degenerate critical points of \( V(y) \) V ( y ) , we derive an explicit formula for the Morse index of \( u_\varepsilon \) u ε , closely related to the negative eigenvalues of the Hessian matrix \( D^2 V(P_i) \) D 2 V ( P i ) . As a consequence, we also establish the non-degeneracy of \( u_\varepsilon \) u ε . Unlike the classical Schrödinger equation, the presence of the non-local term \( \Phi (y) \) Φ ( y ) introduces significant challenges in analyzing the asymptotic behavior of the eigenpairs associated with the linearized operator at \( u_\varepsilon \) u ε , which require precise and advanced analytical techniques.