<p>The aim of this paper is to establish multiple positive normalized solutions <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\((u,v,\lambda _1,\lambda _2)\in H^1(\mathbb {R}^N,\mathbb {R}^2)\times \mathbb {R}^2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo>,</mo> <mi>v</mi> <mo>,</mo> <msub> <mi>λ</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>λ</mi> <mn>2</mn> </msub> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <msup> <mi>H</mi> <mn>1</mn> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>,</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> <mo stretchy="false">)</mo> </mrow> <mo>×</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> to the following coupled Schrödinger system involving Sobolev critical exponent: <Equation ID="Equ65"> <EquationSource Format="TEX">\( {\left\{ \begin{array}{ll} -\Delta u+\lambda _1 u=\mu _1|u|^{p-2}u+\nu \alpha |u|^{\alpha -2}u|v|^\beta , x\in \mathbb {R}^N,\\ -\Delta v+\lambda _2 v=\mu _2|v|^{q-2}v+\nu \beta |v|^{\beta -2}v|u|^\alpha , x\in \mathbb {R}^N,\\ \int _{\mathbb {R}^N}|u|^2\textrm{d}x=a, \int _{\mathbb {R}^N}|v|^2\textrm{d}x=b, \end{array}\right. } N\ge 3, \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>+</mo> <msub> <mi>λ</mi> <mn>1</mn> </msub> <mi>u</mi> <mo>=</mo> <msub> <mi>μ</mi> <mn>1</mn> </msub> <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> <msup> <mrow> <mi>ν</mi> <mi>α</mi> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>α</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <msup> <mrow> <mo stretchy="false">|</mo> <mi>v</mi> <mo stretchy="false">|</mo> </mrow> <mi>β</mi> </msup> <mo>,</mo> <mi>x</mi> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>v</mi> <mo>+</mo> <msub> <mi>λ</mi> <mn>2</mn> </msub> <mi>v</mi> <mo>=</mo> <msub> <mi>μ</mi> <mn>2</mn> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi>v</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>q</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>v</mi> <mo>+</mo> <msup> <mrow> <mi>ν</mi> <mi>β</mi> <mo stretchy="false">|</mo> <mi>v</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>β</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>v</mi> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mi>α</mi> </msup> <mo>,</mo> <mi>x</mi> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <msub> <mo>∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <mtext>d</mtext> <mi>x</mi> <mo>=</mo> <mi>a</mi> <mo>,</mo> <msub> <mo>∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi>v</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <mtext>d</mtext> <mi>x</mi> <mo>=</mo> <mi>b</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> <mi>N</mi> <mo>≥</mo> <mn>3</mn> <mo>,</mo> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mu _1,\mu _2, \nu , a, b&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>μ</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>μ</mi> <mn>2</mn> </msub> <mo>,</mo> <mi>ν</mi> <mo>,</mo> <mi>a</mi> <mo>,</mo> <mi>b</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. We are particularly interested in the mass mixed case that <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(2&lt;p, q&lt;2+\frac{4}{N}, \alpha&gt;1, \beta &gt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>2</mn> <mo>&lt;</mo> <mi>p</mi> <mo>,</mo> <mi>q</mi> <mo>&lt;</mo> <mn>2</mn> <mo>+</mo> <mfrac> <mn>4</mn> <mi>N</mi> </mfrac> <mo>,</mo> <mi>α</mi> <mo>&gt;</mo> <mn>1</mn> <mo>,</mo> <mi>β</mi> <mo>&gt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\alpha +\beta =2^*:=\frac{2N}{N-2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>+</mo> <mi>β</mi> <mo>=</mo> <msup> <mn>2</mn> <mo>∗</mo> </msup> <mo>:</mo> <mo>=</mo> <mfrac> <mrow> <mn>2</mn> <mi>N</mi> </mrow> <mrow> <mi>N</mi> <mo>-</mo> <mn>2</mn> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation>. For sufficiently small <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\nu &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ν</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, we demonstrate that the above system admits two positive solutions, one of which serves as a local minimizer, and the other as a mountain pass solution. By developing some new technical lemmas on the interaction estimates, we are managed to resolves Soave’s open problem [<i>J. Funct. Anal.</i>, 2020, Remark 1.1] within the context of the system case. Notably, our existence result holds true for all dimensions <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(N\ge 3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>≥</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation>. Our results also significantly extend the result of Gou and Jeanjean [<i>Nonlinearity</i>, 2018, Theorem 1.1] to the Sobolev critical coupled case and removing the hypothesis “either <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(p,q\le \alpha +\beta -\frac{2}{N}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>,</mo> <mi>q</mi> <mo>≤</mo> <mi>α</mi> <mo>+</mo> <mi>β</mi> <mo>-</mo> <mfrac> <mn>2</mn> <mi>N</mi> </mfrac> </mrow> </math></EquationSource> </InlineEquation> or <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(|p-q|\le \frac{2}{N}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">|</mo> <mi>p</mi> <mo>-</mo> <mi>q</mi> <mo stretchy="false">|</mo> </mrow> <mo>≤</mo> <mfrac> <mn>2</mn> <mi>N</mi> </mfrac> </mrow> </math></EquationSource> </InlineEquation>" for <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(N\ge 5\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>≥</mo> <mn>5</mn> </mrow> </math></EquationSource> </InlineEquation>. Additionally, we also establish a sequence of properties for the local minimizer, including local uniqueness, continuity with respect to the small parameter <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\nu \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ν</mi> </math></EquationSource> </InlineEquation>, and the limiting profiles for <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\nu \rightarrow 0^+\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ν</mi> <mo stretchy="false">→</mo> <msup> <mn>0</mn> <mo>+</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Multiple positive solutions with prescribed masses for a coupled Schrödinger system: mass mixed and Sobolev critical coupled case

  • Qing Guo,
  • Qihan He,
  • Wei Shuai,
  • Xuexiu Zhong

摘要

The aim of this paper is to establish multiple positive normalized solutions \((u,v,\lambda _1,\lambda _2)\in H^1(\mathbb {R}^N,\mathbb {R}^2)\times \mathbb {R}^2\) ( u , v , λ 1 , λ 2 ) H 1 ( R N , R 2 ) × R 2 to the following coupled Schrödinger system involving Sobolev critical exponent: \( {\left\{ \begin{array}{ll} -\Delta u+\lambda _1 u=\mu _1|u|^{p-2}u+\nu \alpha |u|^{\alpha -2}u|v|^\beta , x\in \mathbb {R}^N,\\ -\Delta v+\lambda _2 v=\mu _2|v|^{q-2}v+\nu \beta |v|^{\beta -2}v|u|^\alpha , x\in \mathbb {R}^N,\\ \int _{\mathbb {R}^N}|u|^2\textrm{d}x=a, \int _{\mathbb {R}^N}|v|^2\textrm{d}x=b, \end{array}\right. } N\ge 3, \) - Δ u + λ 1 u = μ 1 | u | p - 2 u + ν α | u | α - 2 u | v | β , x R N , - Δ v + λ 2 v = μ 2 | v | q - 2 v + ν β | v | β - 2 v | u | α , x R N , R N | u | 2 d x = a , R N | v | 2 d x = b , N 3 , where \(\mu _1,\mu _2, \nu , a, b>0\) μ 1 , μ 2 , ν , a , b > 0 . We are particularly interested in the mass mixed case that \(2<p, q<2+\frac{4}{N}, \alpha>1, \beta >1\) 2 < p , q < 2 + 4 N , α > 1 , β > 1 , and \(\alpha +\beta =2^*:=\frac{2N}{N-2}\) α + β = 2 : = 2 N N - 2 . For sufficiently small \(\nu >0\) ν > 0 , we demonstrate that the above system admits two positive solutions, one of which serves as a local minimizer, and the other as a mountain pass solution. By developing some new technical lemmas on the interaction estimates, we are managed to resolves Soave’s open problem [J. Funct. Anal., 2020, Remark 1.1] within the context of the system case. Notably, our existence result holds true for all dimensions \(N\ge 3\) N 3 . Our results also significantly extend the result of Gou and Jeanjean [Nonlinearity, 2018, Theorem 1.1] to the Sobolev critical coupled case and removing the hypothesis “either \(p,q\le \alpha +\beta -\frac{2}{N}\) p , q α + β - 2 N or \(|p-q|\le \frac{2}{N}\) | p - q | 2 N " for \(N\ge 5\) N 5 . Additionally, we also establish a sequence of properties for the local minimizer, including local uniqueness, continuity with respect to the small parameter \(\nu \) ν , and the limiting profiles for \(\nu \rightarrow 0^+\) ν 0 + .