<p>This paper is concerned with the existence and multiplicity of normalized solutions to the following Schrödinger–Poisson system: <Equation ID="Equ82"> <EquationSource Format="TEX">\( {\left\{ \begin{array}{ll} -\varepsilon ^2\Delta u + V(x) u - \phi |u|^{3} u = \lambda u + \mu |u|^{q-2} u + |u|^{4} u, &amp; ~\text {in } \mathbb {R}^{3},\\ -\varepsilon ^2\Delta \phi = |u|^{5},&amp; ~\text {in } \mathbb {R}^{3}, \end{array}\right. } \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <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>x</mi> <mo stretchy="false">)</mo> </mrow> <mi>u</mi> <mo>-</mo> <msup> <mrow> <mi>ϕ</mi> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>3</mn> </msup> <mi>u</mi> <mo>=</mo> <mi>λ</mi> <mi>u</mi> <mo>+</mo> <msup> <mrow> <mi>μ</mi> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>q</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>+</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>4</mn> </msup> <mi>u</mi> <mo>,</mo> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="3.33333pt" /> <mtext>in</mtext> <mspace width="0.333333em" /> <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> <msup> <mi>ε</mi> <mn>2</mn> </msup> <mi mathvariant="normal">Δ</mi> <mi>ϕ</mi> <mo>=</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>5</mn> </msup> <mo>,</mo> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="3.33333pt" /> <mtext>in</mtext> <mspace width="0.333333em" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </math></EquationSource> </Equation>with prescribed mass <Equation ID="Equ83"> <EquationSource Format="TEX">\(\begin{aligned} \int _{\mathbb {R}^{3}} |u|^{2} \, dx = a^2\varepsilon ^3, \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msub> <mo>∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <mspace width="0.166667em" /> <mi>d</mi> <mi>x</mi> <mo>=</mo> <msup> <mi>a</mi> <mn>2</mn> </msup> <msup> <mi>ε</mi> <mn>3</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(a &gt; 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <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>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(q \in \left( 2, \frac{10}{3} \right) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>∈</mo> <mfenced close=")" open="("> <mn>2</mn> <mo>,</mo> <mfrac> <mn>10</mn> <mn>3</mn> </mfrac> </mfenced> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq4"> <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. Here, <InlineEquation ID="IEq5"> <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> arises as a Lagrange multiplier, and the potential <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(V: \mathbb {R}^{3} \rightarrow [0, +\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>V</mi> <mo>:</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo stretchy="false">→</mo> <mrow> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mo>+</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is a continuous function satisfying suitable conditions. By combining truncation techniques with some adequate estimates, we establish that, for sufficiently small <InlineEquation ID="IEq7"> <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>, normalized solutions do exist. Moreover, by employing Ljusternik-Schnirelmann theory, we find a relationship between the number of positive solutions and the topology of the set where the potential <i>V</i> attains its minimum. Our work extends and complements recent contributions of X. Feng [<CitationRef CitationID="CR17">17</CitationRef>, <CitationRef CitationID="CR18">18</CitationRef>] (<i>Z. Angew. Math. Phys.</i> 2020), to the abstract setting of multiple normalized concentrating solutions. This study seems to be the first work dealing with the existence of multiple normalized semiclassical states for the Sobolev critical Schrödinger–Poisson system coupled with a nonlocal critical term in the whole space <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\mathbb R^3\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi mathvariant="double-struck">R</mi> <mn>3</mn> </msup> </math></EquationSource> </InlineEquation>.</p>

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Solutions with prescribed mass for critical Schrödinger–Poisson systems concentrating at a potential well

  • Qi Gao,
  • Xiaoming He,
  • Vicenţiu D. Rădulescu

摘要

This paper is concerned with the existence and multiplicity of normalized solutions to the following Schrödinger–Poisson system: \( {\left\{ \begin{array}{ll} -\varepsilon ^2\Delta u + V(x) u - \phi |u|^{3} u = \lambda u + \mu |u|^{q-2} u + |u|^{4} u, & ~\text {in } \mathbb {R}^{3},\\ -\varepsilon ^2\Delta \phi = |u|^{5},& ~\text {in } \mathbb {R}^{3}, \end{array}\right. } \) - ε 2 Δ u + V ( x ) u - ϕ | u | 3 u = λ u + μ | u | q - 2 u + | u | 4 u , in R 3 , - ε 2 Δ ϕ = | u | 5 , in R 3 , with prescribed mass \(\begin{aligned} \int _{\mathbb {R}^{3}} |u|^{2} \, dx = a^2\varepsilon ^3, \end{aligned}\) R 3 | u | 2 d x = a 2 ε 3 , where \(a > 0\) a > 0 , \(\mu > 0\) μ > 0 , \(q \in \left( 2, \frac{10}{3} \right) \) q 2 , 10 3 , and \(\varepsilon > 0\) ε > 0 is a small parameter. Here, \(\lambda \in \mathbb {R}\) λ R arises as a Lagrange multiplier, and the potential \(V: \mathbb {R}^{3} \rightarrow [0, +\infty )\) V : R 3 [ 0 , + ) is a continuous function satisfying suitable conditions. By combining truncation techniques with some adequate estimates, we establish that, for sufficiently small \(\varepsilon > 0\) ε > 0 , normalized solutions do exist. Moreover, by employing Ljusternik-Schnirelmann theory, we find a relationship between the number of positive solutions and the topology of the set where the potential V attains its minimum. Our work extends and complements recent contributions of X. Feng [17, 18] (Z. Angew. Math. Phys. 2020), to the abstract setting of multiple normalized concentrating solutions. This study seems to be the first work dealing with the existence of multiple normalized semiclassical states for the Sobolev critical Schrödinger–Poisson system coupled with a nonlocal critical term in the whole space \(\mathbb R^3\) R 3 .