<p>This paper studies the following fractional Schrödinger equation <Equation ID="Equ107"> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} \displaystyle (- \Delta )^s u+\lambda u+ |u|^{q-2}u =|u|^{p-2}u \quad \quad \text {in} \ \mathbb { R}^N, \ N\ge 2, \\ \displaystyle \int _{\mathbb {R}^N}|u|^2dx=a&gt;0, \end{array}\right. } \end{aligned}\)</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> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">)</mo> </mrow> <mi>s</mi> </msup> <mi>u</mi> <mo>+</mo> <mi>λ</mi> <mi>u</mi> <mo>+</mo> <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> <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> <mspace width="1em" /> <mspace width="1em" /> <mtext>in</mtext> <mspace width="4pt" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>,</mo> <mspace width="4pt" /> <mi>N</mi> <mo>≥</mo> <mn>2</mn> <mo>,</mo> </mrow> </mstyle> </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> <mi>N</mi> </msup> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <mi>d</mi> <mi>x</mi> <mo>=</mo> <mi>a</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </mstyle> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\( s\in (0, 1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(2&lt; p, q \le 2_s^*:=\frac{2N}{N-2s}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>2</mn> <mo>&lt;</mo> <mi>p</mi> <mo>,</mo> <mi>q</mi> <mo>≤</mo> <msubsup> <mn>2</mn> <mi>s</mi> <mo>∗</mo> </msubsup> <mo>:</mo> <mo>=</mo> <mfrac> <mrow> <mn>2</mn> <mi>N</mi> </mrow> <mrow> <mi>N</mi> <mo>-</mo> <mn>2</mn> <mi>s</mi> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation> is the fractional critical Sobolev exponent. By giving different assumptions on <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(2&lt;p&lt;q\le 2_s^*\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>2</mn> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <mi>q</mi> <mo>≤</mo> <msubsup> <mn>2</mn> <mi>s</mi> <mo>∗</mo> </msubsup> </mrow> </math></EquationSource> </InlineEquation>, we get the existence, non-existence and concentration behavior of solutions for the above problem. It is worth emphasizing that some of the results are new, even for Laplacian operator.</p>

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Normalized solutions and limit profiles of the fractional Schrödinger equation with mixed-type nonlinearities

  • Jin-Cai Kang,
  • Chun-Lei Tang

摘要

This paper studies the following fractional Schrödinger equation \(\begin{aligned} {\left\{ \begin{array}{ll} \displaystyle (- \Delta )^s u+\lambda u+ |u|^{q-2}u =|u|^{p-2}u \quad \quad \text {in} \ \mathbb { R}^N, \ N\ge 2, \\ \displaystyle \int _{\mathbb {R}^N}|u|^2dx=a>0, \end{array}\right. } \end{aligned}\) ( - Δ ) s u + λ u + | u | q - 2 u = | u | p - 2 u in R N , N 2 , R N | u | 2 d x = a > 0 , where \( s\in (0, 1)\) s ( 0 , 1 ) and \(2< p, q \le 2_s^*:=\frac{2N}{N-2s}\) 2 < p , q 2 s : = 2 N N - 2 s is the fractional critical Sobolev exponent. By giving different assumptions on \(2<p<q\le 2_s^*\) 2 < p < q 2 s , we get the existence, non-existence and concentration behavior of solutions for the above problem. It is worth emphasizing that some of the results are new, even for Laplacian operator.