<p>We study the normalized solutions of the <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43034_2025_447_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>-critical Schrödinger–Poisson system with an external potential <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43034_2025_447_Article_IEq7.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="84" /> </InlineMediaObject> <EquationSource Format="TEX">\(V(x)=|x|^2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>V</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> in <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43034_2025_447_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb {R}}^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation>, which can be described by the constraint minimization problem. When the magnetic field is attractive, we prove that there is a threshold <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43034_2025_447_Article_IEq9.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="83" /> </InlineMediaObject> <EquationSource Format="TEX">\(a^*\in (0,\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>a</mi> <mo>∗</mo> </msup> <mo>∈</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> such that the constraint minimizer exists if and only if the interaction strength <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43034_2025_447_Article_IEq10.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="49" /> </InlineMediaObject> <EquationSource Format="TEX">\(a&lt;a^*\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>&lt;</mo> <msup> <mi>a</mi> <mo>∗</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>. Moreover, for the repulsive case, there exists a minimizer if <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43034_2025_447_Article_IEq10.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="49" /> </InlineMediaObject> <EquationSource Format="TEX">\(a&lt;a^*\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>&lt;</mo> <msup> <mi>a</mi> <mo>∗</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>, while there does not exist any minimizer if <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43034_2025_447_Article_IEq12.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="49" /> </InlineMediaObject> <EquationSource Format="TEX">\(a&gt;a^*\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>&gt;</mo> <msup> <mi>a</mi> <mo>∗</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>. Particularly, after analyzing its limiting behavior, we then obtain the uniqueness of positive minimizers as <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43034_2025_447_Article_IEq13.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(a\nearrow a^*\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>↗</mo> <msup> <mi>a</mi> <mo>∗</mo> </msup> </mrow> </math></EquationSource> </InlineEquation> by overcoming the sign-changing property of the logarithmic convolution and the non-invariance under translations of the harmonic potential.</p>

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Normalized solutions for the \(L^2\)-critical Schrödinger–Poisson system in \({\mathbb {R}}^2\)

  • Min Liu,
  • Shu Zhang

摘要

We study the normalized solutions of the \(L^2\) L 2 -critical Schrödinger–Poisson system with an external potential \(V(x)=|x|^2\) V ( x ) = | x | 2 in \({\mathbb {R}}^2\) R 2 , which can be described by the constraint minimization problem. When the magnetic field is attractive, we prove that there is a threshold \(a^*\in (0,\infty )\) a ( 0 , ) such that the constraint minimizer exists if and only if the interaction strength \(a<a^*\) a < a . Moreover, for the repulsive case, there exists a minimizer if \(a<a^*\) a < a , while there does not exist any minimizer if \(a>a^*\) a > a . Particularly, after analyzing its limiting behavior, we then obtain the uniqueness of positive minimizers as \(a\nearrow a^*\) a a by overcoming the sign-changing property of the logarithmic convolution and the non-invariance under translations of the harmonic potential.