<p>In this paper we study the following <i>p</i>-Laplacian Schrödinger-Poisson system with Sobolev critical exponent and mixed nonlinearities <Equation ID="Equ115"> <EquationSource Format="TEX">\( {\left\{ \begin{array}{ll} -\Delta _{p} u + \lambda u^{p-1} + \kappa \bigl (|x|^{-1}*|u|^{p}\bigr )u^{p-1} = |u|^{p^{*}-2}u + \mu |u|^{q-2}u, &amp; x\in \mathbb {R}^{3},\\ \displaystyle \int _{\mathbb {R}^{3}}|u|^{p}\,dx = a^{p}, \end{array}\right. } \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi>p</mi> </msub> <mi>u</mi> <mo>+</mo> <mi>λ</mi> <msup> <mi>u</mi> <mrow> <mi>p</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mo>+</mo> <msup> <mrow> <mi>κ</mi> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">(</mo> </mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msup> <msup> <mrow> <mrow /> <mo>∗</mo> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mi>p</mi> </msup> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">)</mo> </mrow> <msup> <mi>u</mi> <mrow> <mi>p</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mo>=</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <msup> <mi>p</mi> <mrow> <mrow /> <mo>∗</mo> </mrow> </msup> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>+</mo> <mi>μ</mi> <msup> <mrow> <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> </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"> <mstyle displaystyle="true" scriptlevel="0"> <mrow> <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> <mi>p</mi> </msup> <mspace width="0.166667em" /> <mi>d</mi> <mi>x</mi> <mo>=</mo> <msup> <mi>a</mi> <mi>p</mi> </msup> <mo>,</mo> </mrow> </mstyle> </mtd> </mtr> </mtable> </mrow> </mfenced> </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> is prescribed, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\kappa &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>κ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mu \in \mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>μ</mi> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(p&lt;q&lt;p^{*}=\frac{3p}{3-p}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>&lt;</mo> <mi>q</mi> <mo>&lt;</mo> <msup> <mi>p</mi> <mrow> <mrow /> <mo>∗</mo> </mrow> </msup> <mo>=</mo> <mfrac> <mrow> <mn>3</mn> <mi>p</mi> </mrow> <mrow> <mn>3</mn> <mo>-</mo> <mi>p</mi> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation> is the Sobolev critical exponent, and <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> appears as a Lagrange multiplier. We prove the existence of two normalized solutions, including a ground state, under the conditions <InlineEquation ID="IEq6"> <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> and <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(q \in \bigl (p, \frac{4p}{3}\bigr )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>∈</mo> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">(</mo> </mrow> <mi>p</mi> <mo>,</mo> <mfrac> <mrow> <mn>4</mn> <mi>p</mi> </mrow> <mn>3</mn> </mfrac> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. It is worth emphasizing that unlike the case <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\kappa =0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>κ</mi> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, the Schwarz spherical rearrangement method fails when <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\kappa &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>κ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, and the derivation of a strict subadditivity inequality for the minimal energy becomes delicate in order to exclude dichotomy of minimizing sequences. As far as we know, the existence of a second solution for the above problem has not been studied before. We also prove that no positive normalized solution exists when <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\mu \le 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>μ</mi> <mo>≤</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(q \in (p, p^{*})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mi>p</mi> <mo>,</mo> <msup> <mi>p</mi> <mrow> <mrow /> <mo>∗</mo> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, which extends earlier related results in the literature [<CitationRef AdditionalCitationIDS="CR36" CitationID="CR35">35</CitationRef>–<CitationRef CitationID="CR37">37</CitationRef>].</p>

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Multiple Normalized Solutions for the Quasilinear Sobolev Critical Schrödinger-Poisson System

  • Mengru Li,
  • Xiaoming He

摘要

In this paper we study the following p-Laplacian Schrödinger-Poisson system with Sobolev critical exponent and mixed nonlinearities \( {\left\{ \begin{array}{ll} -\Delta _{p} u + \lambda u^{p-1} + \kappa \bigl (|x|^{-1}*|u|^{p}\bigr )u^{p-1} = |u|^{p^{*}-2}u + \mu |u|^{q-2}u, & x\in \mathbb {R}^{3},\\ \displaystyle \int _{\mathbb {R}^{3}}|u|^{p}\,dx = a^{p}, \end{array}\right. } \) - Δ p u + λ u p - 1 + κ ( | x | - 1 | u | p ) u p - 1 = | u | p - 2 u + μ | u | q - 2 u , x R 3 , R 3 | u | p d x = a p , where \(a>0\) a > 0 is prescribed, \(\kappa >0\) κ > 0 , \(\mu \in \mathbb {R}\) μ R , \(p<q<p^{*}=\frac{3p}{3-p}\) p < q < p = 3 p 3 - p is the Sobolev critical exponent, and \(\lambda \in \mathbb {R}\) λ R appears as a Lagrange multiplier. We prove the existence of two normalized solutions, including a ground state, under the conditions \(\mu > 0\) μ > 0 and \(q \in \bigl (p, \frac{4p}{3}\bigr )\) q ( p , 4 p 3 ) . It is worth emphasizing that unlike the case \(\kappa =0\) κ = 0 , the Schwarz spherical rearrangement method fails when \(\kappa >0\) κ > 0 , and the derivation of a strict subadditivity inequality for the minimal energy becomes delicate in order to exclude dichotomy of minimizing sequences. As far as we know, the existence of a second solution for the above problem has not been studied before. We also prove that no positive normalized solution exists when \(\mu \le 0\) μ 0 and \(q \in (p, p^{*})\) q ( p , p ) , which extends earlier related results in the literature [3537].