<p>The paper deals with the existence of normalized solutions for the following planar Schrödinger-Poisson system with <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2470_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation>-constraint: <Equation ID="Equ83"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2470_Article_Equ83.gif" Format="GIF" Height="76" Rendition="HTML" Resolution="72" Type="Linedraw" Width="501" /> </MediaObject> <EquationSource Format="TEX">\({\left\{ \begin{array}{ll}-\Delta u+\lambda u+V(x)u+\mu \phi u= \left( e^{u^2}-1-u^2\right) u+\gamma |u|^{p-2} u, &amp; x \in \mathbb {R}^2, \\ \Delta \phi =2 \pi u^2, &amp; x \in \mathbb {R}^2,\\ \int _{\mathbb {R}^2} u^2 \textrm{d} x=m^{2}, \end{array}\right. }\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>+</mo> <mi>λ</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>μ</mi> <mi>ϕ</mi> <mi>u</mi> <mo>=</mo> <mfenced close=")" open="("> <msup> <mi>e</mi> <msup> <mi>u</mi> <mn>2</mn> </msup> </msup> <mo>-</mo> <mn>1</mn> <mo>-</mo> <msup> <mi>u</mi> <mn>2</mn> </msup> </mfenced> <mi>u</mi> <mo>+</mo> <mi>γ</mi> <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> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>x</mi> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mi mathvariant="normal">Δ</mi> <mi>ϕ</mi> <mo>=</mo> <mn>2</mn> <mi>π</mi> <msup> <mi>u</mi> <mn>2</mn> </msup> <mo>,</mo> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>x</mi> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <msub> <mo>∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> </msub> <msup> <mi>u</mi> <mn>2</mn> </msup> <mtext>d</mtext> <mi>x</mi> <mo>=</mo> <msup> <mi>m</mi> <mn>2</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </math></EquationSource> </Equation>where <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2470_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="82" /> </InlineMediaObject> <EquationSource Format="TEX">\(m,\mu ,\gamma &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo>,</mo> <mi>μ</mi> <mo>,</mo> <mi>γ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2470_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="66" /> </InlineMediaObject> <EquationSource Format="TEX">\(p \in (2,4]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>2</mn> <mo>,</mo> <mn>4</mn> <mo stretchy="false">]</mo> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2470_Article_IEq4.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\( \lambda \in \mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation> is a Lagrange multiplier, <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2470_Article_IEq5.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="177" /> </InlineMediaObject> <EquationSource Format="TEX">\(V \in C^{2}\left( \mathbb {R}^2\backslash \{0\},(0, \infty )\right) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>V</mi> <mo>∈</mo> <msup> <mi>C</mi> <mn>2</mn> </msup> <mfenced close=")" open="("> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> <mrow> <mo stretchy="true">\</mo> <mrow> <mo stretchy="false">{</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> <mo>,</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </mfenced> </mrow> </math></EquationSource> </InlineEquation> is a potential function. It is worth noting that the term <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2470_Article_IEq6.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="112" /> </InlineMediaObject> <EquationSource Format="TEX">\((e^{u^2}-1-u^2) u\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <msup> <mi>e</mi> <msup> <mi>u</mi> <mn>2</mn> </msup> </msup> <mo>-</mo> <mn>1</mn> <mo>-</mo> <msup> <mi>u</mi> <mn>2</mn> </msup> <mo stretchy="false">)</mo> <mi>u</mi> </mrow> </math></EquationSource> </InlineEquation> exhibits critical exponential growth characteristic. Besides this, we also need to consider the perturbation term <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2470_Article_IEq7.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="65" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma |u|^{p-2} u\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mrow> <mi>γ</mi> <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> </mrow> </math></EquationSource> </InlineEquation> focusing on the case <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2470_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="66" /> </InlineMediaObject> <EquationSource Format="TEX">\(p\in (2,4]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>2</mn> <mo>,</mo> <mn>4</mn> <mo stretchy="false">]</mo> </mrow> </math></EquationSource> </InlineEquation> and linear term <i>V</i>(<i>x</i>)<i>u</i>. By employing a range of variational methods to obtain the ground state solution of the equation, we also leverage the Moser function to establish an upper bound for the mountain pass level <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2470_Article_IEq9.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="32" /> </InlineMediaObject> <EquationSource Format="TEX">\(C_{\gamma , \mu }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>C</mi> <mrow> <mi>γ</mi> <mo>,</mo> <mi>μ</mi> </mrow> </msub> </math></EquationSource> </InlineEquation>, which restores compactness. This allows us to further derive the mountain pass-type solution. Moreover, we further analyze the asymptotic behavior of these solutions.</p>

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Normalized Solutions of Planar Schrödinger-Poisson System Involving Moser-Trudinger Critical Growth and Potential

  • Xin Song,
  • Li Wang

摘要

The paper deals with the existence of normalized solutions for the following planar Schrödinger-Poisson system with \(L^2\) L 2 -constraint: \({\left\{ \begin{array}{ll}-\Delta u+\lambda u+V(x)u+\mu \phi u= \left( e^{u^2}-1-u^2\right) u+\gamma |u|^{p-2} u, & x \in \mathbb {R}^2, \\ \Delta \phi =2 \pi u^2, & x \in \mathbb {R}^2,\\ \int _{\mathbb {R}^2} u^2 \textrm{d} x=m^{2}, \end{array}\right. }\) - Δ u + λ u + V ( x ) u + μ ϕ u = e u 2 - 1 - u 2 u + γ | u | p - 2 u , x R 2 , Δ ϕ = 2 π u 2 , x R 2 , R 2 u 2 d x = m 2 , where \(m,\mu ,\gamma >0\) m , μ , γ > 0 , \(p \in (2,4]\) p ( 2 , 4 ] , \( \lambda \in \mathbb {R}\) λ R is a Lagrange multiplier, \(V \in C^{2}\left( \mathbb {R}^2\backslash \{0\},(0, \infty )\right) \) V C 2 R 2 \ { 0 } , ( 0 , ) is a potential function. It is worth noting that the term \((e^{u^2}-1-u^2) u\) ( e u 2 - 1 - u 2 ) u exhibits critical exponential growth characteristic. Besides this, we also need to consider the perturbation term \(\gamma |u|^{p-2} u\) γ | u | p - 2 u focusing on the case \(p\in (2,4]\) p ( 2 , 4 ] and linear term V(x)u. By employing a range of variational methods to obtain the ground state solution of the equation, we also leverage the Moser function to establish an upper bound for the mountain pass level \(C_{\gamma , \mu }\) C γ , μ , which restores compactness. This allows us to further derive the mountain pass-type solution. Moreover, we further analyze the asymptotic behavior of these solutions.