<p>In this paper, we study the existence and asymptotic behavior of normalized ground states of the following Schrödinger system with critical Sobolev exponent: <Equation ID="Equ43"> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{array}{ll} \displaystyle -\Delta u+\lambda _1u=|u|^4u+\mu vw&amp; \text{ in }\ \mathbb {R}^3,\\ \displaystyle -\Delta v+\lambda _2v=|v|^4v+\mu wu&amp; \text{ in }\ \mathbb {R}^3,\\ \displaystyle -\Delta w+\lambda _3w=|w|^4w+\mu uv&amp; \text{ in }\ \mathbb {R}^3,\\ \int \limits _{\mathbb {R}^3}u^2=a^2,\ \ \int \limits _{\mathbb {R}^3}v^2=b^2,\ \ \int \limits _{\mathbb {R}^3}w^2=c^2,\\ \end{array}\right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mstyle displaystyle="true" scriptlevel="0"> <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> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>4</mn> </msup> <mi>u</mi> <mo>+</mo> <mi>μ</mi> <mi>v</mi> <mi>w</mi> </mrow> </mstyle> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mspace width="4pt" /> <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 /> <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> <msup> <mrow> <mo stretchy="false">|</mo> <mi>v</mi> <mo stretchy="false">|</mo> </mrow> <mn>4</mn> </msup> <mi>v</mi> <mo>+</mo> <mi>μ</mi> <mi>w</mi> <mi>u</mi> </mrow> </mstyle> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mspace width="4pt" /> <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 /> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>w</mi> <mo>+</mo> <msub> <mi>λ</mi> <mn>3</mn> </msub> <mi>w</mi> <mo>=</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>w</mi> <mo stretchy="false">|</mo> </mrow> <mn>4</mn> </msup> <mi>w</mi> <mo>+</mo> <mi>μ</mi> <mi>u</mi> <mi>v</mi> </mrow> </mstyle> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mspace width="4pt" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <munder> <mo movablelimits="false">∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> </munder> <msup> <mi>u</mi> <mn>2</mn> </msup> <mo>=</mo> <msup> <mi>a</mi> <mn>2</mn> </msup> <mo>,</mo> <mspace width="4pt" /> <mspace width="4pt" /> <munder> <mo movablelimits="false">∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> </munder> <msup> <mi>v</mi> <mn>2</mn> </msup> <mo>=</mo> <msup> <mi>b</mi> <mn>2</mn> </msup> <mo>,</mo> <mspace width="4pt" /> <mspace width="4pt" /> <munder> <mo movablelimits="false">∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> </munder> <msup> <mi>w</mi> <mn>2</mn> </msup> <mo>=</mo> <msup> <mi>c</mi> <mn>2</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(a,b,c&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>,</mo> <mi>b</mi> <mo>,</mo> <mi>c</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and <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>. We show that there exists a normalized ground state for <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(0&lt;\mu &lt;\mu _0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>μ</mi> <mo>&lt;</mo> <msub> <mi>μ</mi> <mn>0</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>, the constant <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\mu _0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>μ</mi> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation> will be explicitly given. Furthermore, we obtain the asymptotic behavior of the minimizers as <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\mu \rightarrow 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>μ</mi> <mo stretchy="false">→</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Normalized ground states for Sobolev critical NLS system with quadratic interaction

  • Xiaoting Li,
  • Yuhua Li

摘要

In this paper, we study the existence and asymptotic behavior of normalized ground states of the following Schrödinger system with critical Sobolev exponent: \(\begin{aligned} \left\{ \begin{array}{ll} \displaystyle -\Delta u+\lambda _1u=|u|^4u+\mu vw& \text{ in }\ \mathbb {R}^3,\\ \displaystyle -\Delta v+\lambda _2v=|v|^4v+\mu wu& \text{ in }\ \mathbb {R}^3,\\ \displaystyle -\Delta w+\lambda _3w=|w|^4w+\mu uv& \text{ in }\ \mathbb {R}^3,\\ \int \limits _{\mathbb {R}^3}u^2=a^2,\ \ \int \limits _{\mathbb {R}^3}v^2=b^2,\ \ \int \limits _{\mathbb {R}^3}w^2=c^2,\\ \end{array}\right. \end{aligned}\) - Δ u + λ 1 u = | u | 4 u + μ v w in R 3 , - Δ v + λ 2 v = | v | 4 v + μ w u in R 3 , - Δ w + λ 3 w = | w | 4 w + μ u v in R 3 , R 3 u 2 = a 2 , R 3 v 2 = b 2 , R 3 w 2 = c 2 , where \(a,b,c>0\) a , b , c > 0 and \(\mu >0\) μ > 0 . We show that there exists a normalized ground state for \(0<\mu <\mu _0\) 0 < μ < μ 0 , the constant \(\mu _0\) μ 0 will be explicitly given. Furthermore, we obtain the asymptotic behavior of the minimizers as \(\mu \rightarrow 0\) μ 0 .