<p>In this paper, we study the following Schrödinger-Poisson equation with critical growth: <Equation ID="Equ113"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="526_2024_2923_Article_Equ113.gif" Format="GIF" Height="54" Rendition="HTML" Resolution="72" Type="Linedraw" Width="456" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{aligned}&amp;-\Delta u + \mu V(x) u+ K(x)\phi u = \lambda h(x) f(u) + (u^+)^5,\ \ \ \ \textrm{in } \ \ \ \ {\mathbb {R}}^3,\\&amp;-\Delta \phi =K(x)u^2, \ \ \ \ \textrm{in } \ \ \ \ {\mathbb {R}}^3, \end{aligned}\right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd /> <mtd columnalign="left"> <mrow> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>+</mo> <mi>μ</mi> <mi>V</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mi>u</mi> <mo>+</mo> <mi>K</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mi>ϕ</mi> <mi>u</mi> <mo>=</mo> <mi>λ</mi> <mi>h</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <msup> <mrow> <mo stretchy="false">(</mo> <msup> <mi>u</mi> <mo>+</mo> </msup> <mo stretchy="false">)</mo> </mrow> <mn>5</mn> </msup> <mo>,</mo> <mspace width="4pt" /> <mspace width="4pt" /> <mspace width="4pt" /> <mspace width="4pt" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mspace width="4pt" /> <mspace width="4pt" /> <mspace width="4pt" /> <mspace width="4pt" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow /> </mtd> <mtd columnalign="left"> <mrow> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>ϕ</mi> <mo>=</mo> <mi>K</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <msup> <mi>u</mi> <mn>2</mn> </msup> <mo>,</mo> <mspace width="4pt" /> <mspace width="4pt" /> <mspace width="4pt" /> <mspace width="4pt" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mspace width="4pt" /> <mspace width="4pt" /> <mspace width="4pt" /> <mspace width="4pt" /> <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="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2024_2923_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mu \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>μ</mi> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2024_2923_Article_IEq4.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> are large parameters, the potential <i>V</i> is non-negative, decays to zero at infinity, or there are no restrictions on <i>V</i> at infinity. When <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2024_2923_Article_IEq5.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="70" /> </InlineMediaObject> <EquationSource Format="TEX">\(\textrm{int}V^{-1}(0)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>int</mtext> <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> possesses multiple disjoint bounded components, by developing some techniques in variational methods, we prove the existence of multi-bump solutions for <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2024_2923_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mu &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>μ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> large and the concentration behavior of multi-bump solutions as <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2024_2923_Article_IEq7.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="71" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mu \rightarrow +\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>μ</mi> <mo stretchy="false">→</mo> <mo>+</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Multi-bump solutions to Schrödinger-Poisson equations with critical growth in \({\mathbb {R}}^3\)

  • Jian Zhang

摘要

In this paper, we study the following Schrödinger-Poisson equation with critical growth: \(\begin{aligned} \left\{ \begin{aligned}&-\Delta u + \mu V(x) u+ K(x)\phi u = \lambda h(x) f(u) + (u^+)^5,\ \ \ \ \textrm{in } \ \ \ \ {\mathbb {R}}^3,\\&-\Delta \phi =K(x)u^2, \ \ \ \ \textrm{in } \ \ \ \ {\mathbb {R}}^3, \end{aligned}\right. \end{aligned}\) - Δ u + μ V ( x ) u + K ( x ) ϕ u = λ h ( x ) f ( u ) + ( u + ) 5 , in R 3 , - Δ ϕ = K ( x ) u 2 , in R 3 , where \(\mu \) μ , \(\lambda >0\) λ > 0 are large parameters, the potential V is non-negative, decays to zero at infinity, or there are no restrictions on V at infinity. When \(\textrm{int}V^{-1}(0)\) int V - 1 ( 0 ) possesses multiple disjoint bounded components, by developing some techniques in variational methods, we prove the existence of multi-bump solutions for \(\mu >0\) μ > 0 large and the concentration behavior of multi-bump solutions as \(\mu \rightarrow +\infty \) μ + .