<p>In this paper, we deal with the following weakly coupled nonlinear Schrödinger system <Equation ID="Equ27"> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} - \Delta _\alpha u + \omega u = |u|^2 u + \beta u |v|^2&amp; \quad \textrm{in}\ \mathbb {R}^2,\\ - \Delta v + \tilde{\omega } v = |v|^2 v + \beta |u|^2 v&amp; \quad \textrm{in}\ \mathbb {R}^2, \end{array}\right. } \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi>α</mi> </msub> <mi>u</mi> <mo>+</mo> <mi>ω</mi> <mi>u</mi> <mo>=</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <mi>u</mi> <mo>+</mo> <mi>β</mi> <mi>u</mi> <msup> <mrow> <mo stretchy="false">|</mo> <mi>v</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="1em" /> <mtext>in</mtext> <mspace width="4pt" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>v</mi> <mo>+</mo> <mover accent="true"> <mi>ω</mi> <mo stretchy="false">~</mo> </mover> <mi>v</mi> <mo>=</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>v</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <mi>v</mi> <mo>+</mo> <mi>β</mi> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <mi>v</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="1em" /> <mtext>in</mtext> <mspace width="4pt" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <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">\(-\Delta _\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi>α</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> denotes the Laplacian operator with a point interaction, and <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ω</mi> </math></EquationSource> </InlineEquation> is greater than a suitable positive constant, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\tilde{\omega }&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mover accent="true"> <mi>ω</mi> <mo stretchy="false">~</mo> </mover> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\beta \geqslant 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>β</mi> <mo>⩾</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. For any <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\beta \geqslant 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>β</mi> <mo>⩾</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, this system admits the existence of a ground state solution which can have only one nontrivial component or two nontrivial components and which could be regular or singular. We analyse this phenomenon showing how this depends strongly on the parameters. Moreover, we study the asymptotic behaviour of ground state solutions whenever <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\beta \rightarrow \infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>β</mi> <mo stretchy="false">→</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Coupled nonlinear Schrödinger equations with point interaction: existence and asymptotic behaviour

  • Yuki Osada,
  • Alessio Pomponio

摘要

In this paper, we deal with the following weakly coupled nonlinear Schrödinger system \(\begin{aligned} {\left\{ \begin{array}{ll} - \Delta _\alpha u + \omega u = |u|^2 u + \beta u |v|^2& \quad \textrm{in}\ \mathbb {R}^2,\\ - \Delta v + \tilde{\omega } v = |v|^2 v + \beta |u|^2 v& \quad \textrm{in}\ \mathbb {R}^2, \end{array}\right. } \end{aligned}\) - Δ α u + ω u = | u | 2 u + β u | v | 2 in R 2 , - Δ v + ω ~ v = | v | 2 v + β | u | 2 v in R 2 , where \(-\Delta _\alpha \) - Δ α denotes the Laplacian operator with a point interaction, and \(\omega \) ω is greater than a suitable positive constant, \(\tilde{\omega }>0\) ω ~ > 0 , and \(\beta \geqslant 0\) β 0 . For any \(\beta \geqslant 0\) β 0 , this system admits the existence of a ground state solution which can have only one nontrivial component or two nontrivial components and which could be regular or singular. We analyse this phenomenon showing how this depends strongly on the parameters. Moreover, we study the asymptotic behaviour of ground state solutions whenever \(\beta \rightarrow \infty \) β .