<p>In this article, we study the existence and the limit behavior of solutions with a prescribed <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(L^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation>-norm for a class of Chern–Simons–Schrödinger equations with combined nonlinearities with <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(0&lt;\alpha \le 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>α</mi> <mo>≤</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(0&lt;\beta \le \frac{p-2}{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>β</mi> <mo>≤</mo> <mfrac> <mrow> <mi>p</mi> <mo>-</mo> <mn>2</mn> </mrow> <mn>2</mn> </mfrac> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\omega &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ω</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. To obtain such solutions, we look for critical points of the energy functional on the mass constraint. When <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(q=4&lt;p&lt;\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>=</mo> <mn>4</mn> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>, by the general minimax theorem and constraint minimization approach, we prove the existence of a positive critical point <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(u^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>u</mi> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation> for the energy functional, and this positive solution is the ground state normalized solution. When <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(2&lt;q&lt;p,\,4&lt;p&lt;\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>2</mn> <mo>&lt;</mo> <mi>q</mi> <mo>&lt;</mo> <mi>p</mi> <mo>,</mo> <mspace width="0.166667em" /> <mn>4</mn> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>, by the blow-up analysis and constraint minimization approach, on the premise that there is a radial Mountain Pass type normalized solution <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\({\hat{u}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover accent="true"> <mi>u</mi> <mo stretchy="false">^</mo> </mover> </math></EquationSource> </InlineEquation> to the Chern–Simons–Schrödinger equations, we get the limit behavior: the radial Mountain Pass type normalized solutions converge to the ground state normalized solution <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(u^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>u</mi> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation> as <i>q</i> tending to 4.</p>

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Mass threshold of the limit behavior of normalized solutions for the Chern–Simons–Schrödinger equations with combined nonlinearities

  • Yingying Xiao,
  • Yipeng Qiu,
  • Yan Zhao,
  • Shengyue Xu

摘要

In this article, we study the existence and the limit behavior of solutions with a prescribed \(L^2\) L 2 -norm for a class of Chern–Simons–Schrödinger equations with combined nonlinearities with \(0<\alpha \le 1\) 0 < α 1 , \(0<\beta \le \frac{p-2}{2}\) 0 < β p - 2 2 and \(\omega >0\) ω > 0 . To obtain such solutions, we look for critical points of the energy functional on the mass constraint. When \(q=4<p<\infty \) q = 4 < p < , by the general minimax theorem and constraint minimization approach, we prove the existence of a positive critical point \(u^*\) u for the energy functional, and this positive solution is the ground state normalized solution. When \(2<q<p,\,4<p<\infty \) 2 < q < p , 4 < p < , by the blow-up analysis and constraint minimization approach, on the premise that there is a radial Mountain Pass type normalized solution \({\hat{u}}\) u ^ to the Chern–Simons–Schrödinger equations, we get the limit behavior: the radial Mountain Pass type normalized solutions converge to the ground state normalized solution \(u^*\) u as q tending to 4.