<p>In this paper, we consider the existence and asymptotic behavior of solutions for the following nonlinear Schrödinger–Poisson system <Equation ID="Equ61"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1210_Article_Equ61.gif" Format="GIF" Height="43" Rendition="HTML" Resolution="72" Type="Linedraw" Width="469" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{array}{ll} -\Delta u+V(x)u+\lambda \phi (x)u =\big (a^+(x)+\mu a^-(x)\big )|u|^{p-2}u, \ \ \ &amp; x\in {\mathbb {R}}^3 , \\ -\Delta \phi =u^2, \ &amp; x\in {\mathbb {R}}^3, \end{array} \right. \end{aligned}\)</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>V</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mi>u</mi> <mo>+</mo> <mi>λ</mi> <mi>ϕ</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mi>u</mi> <mo>=</mo> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">(</mo> </mrow> <msup> <mi>a</mi> <mo>+</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <mi>μ</mi> <msup> <mi>a</mi> <mo>-</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">)</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="4pt" /> <mspace width="4pt" /> <mspace width="4pt" /> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>x</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>ϕ</mi> <mo>=</mo> <msup> <mi>u</mi> <mn>2</mn> </msup> <mo>,</mo> <mspace width="4pt" /> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>x</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="11784_2025_1210_Article_IEq1.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="185" /> </InlineMediaObject> <EquationSource Format="TEX">\(a\in C^{\alpha }({\mathbb {R}}^3,{\mathbb {R}})\ (\alpha \in (0,1))\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>∈</mo> <msup> <mi>C</mi> <mi>α</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo>,</mo> <mi mathvariant="double-struck">R</mi> <mo stretchy="false">)</mo> </mrow> <mspace width="4pt" /> <mrow> <mo stretchy="false">(</mo> <mi>α</mi> <mo>∈</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is a sign-changing function, <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1210_Article_IEq2.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="96" /> </InlineMediaObject> <EquationSource Format="TEX">\(V\in C({\mathbb {R}}^3,{\mathbb {R}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>V</mi> <mo>∈</mo> <mi>C</mi> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo>,</mo> <mi mathvariant="double-struck">R</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1210_Article_IEq3.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1210_Article_IEq4.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> are positive parameters and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1210_Article_IEq5.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>. Using quantitative deformation lemma and degree theory, we prove the existence of a positive ground state solution and a least energy sign-changing solution. Moreover, the asymptotic behavior of the two solutions as <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1210_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="55" /> </InlineMediaObject> <EquationSource Format="TEX">\(\lambda \rightarrow 0^+\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo stretchy="false">→</mo> <msup> <mn>0</mn> <mo>+</mo> </msup> </mrow> </math></EquationSource> </InlineEquation> or <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1210_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> are analyzed. In addition, when the set <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1210_Article_IEq8.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="151" /> </InlineMediaObject> <EquationSource Format="TEX">\(\{x\in {\mathbb {R}}^3:\ a(x)&gt;0\}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">{</mo> <mi>x</mi> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo>:</mo> <mspace width="4pt" /> <mi>a</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>&gt;</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> </math></EquationSource> </InlineEquation> possesses several disjoint components, we give the existence and asymptotic behavior of multi-bump sign-changing solutions.</p>

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Existence and asymptotic behavior of solutions for Schrödinger–Poisson system with indefinite nonlinearity

  • Yinbin Deng,
  • Wei Shuai,
  • Jianghua Ye

摘要

In this paper, we consider the existence and asymptotic behavior of solutions for the following nonlinear Schrödinger–Poisson system \(\begin{aligned} \left\{ \begin{array}{ll} -\Delta u+V(x)u+\lambda \phi (x)u =\big (a^+(x)+\mu a^-(x)\big )|u|^{p-2}u, \ \ \ & x\in {\mathbb {R}}^3 , \\ -\Delta \phi =u^2, \ & x\in {\mathbb {R}}^3, \end{array} \right. \end{aligned}\) - Δ u + V ( x ) u + λ ϕ ( x ) u = ( a + ( x ) + μ a - ( x ) ) | u | p - 2 u , x R 3 , - Δ ϕ = u 2 , x R 3 , where \(a\in C^{\alpha }({\mathbb {R}}^3,{\mathbb {R}})\ (\alpha \in (0,1))\) a C α ( R 3 , R ) ( α ( 0 , 1 ) ) is a sign-changing function, \(V\in C({\mathbb {R}}^3,{\mathbb {R}})\) V C ( R 3 , R ) , \(\lambda \) λ , \(\mu \) μ are positive parameters and \(p\in (4,6)\) p ( 4 , 6 ) . Using quantitative deformation lemma and degree theory, we prove the existence of a positive ground state solution and a least energy sign-changing solution. Moreover, the asymptotic behavior of the two solutions as \(\lambda \rightarrow 0^+\) λ 0 + or \(\mu \rightarrow +\infty \) μ + are analyzed. In addition, when the set \(\{x\in {\mathbb {R}}^3:\ a(x)>0\}\) { x R 3 : a ( x ) > 0 } possesses several disjoint components, we give the existence and asymptotic behavior of multi-bump sign-changing solutions.