<p>We study the fractional Schrödinger equations with a vanishing parameter: where <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2081_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="66" /> </InlineMediaObject> <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>, <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2081_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="57" /> </InlineMediaObject> <EquationSource Format="TEX">\(N&gt;2s\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>&gt;</mo> <mn>2</mn> <mi>s</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2081_Article_IEq3.gif" Format="GIF" Height="24" Rendition="HTML" Resolution="72" Type="Linedraw" Width="165" /> </InlineMediaObject> <EquationSource Format="TEX">\(2&lt;q&lt;p\le 2^*_s=\frac{2N}{N-2s}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>2</mn> <mo>&lt;</mo> <mi>q</mi> <mo>&lt;</mo> <mi>p</mi> <mo>≤</mo> <msubsup> <mn>2</mn> <mi>s</mi> <mo>∗</mo> </msubsup> <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> are fixed parameters and <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2081_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(\lambda &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> is a vanishing parameter. We investigate the asymptotic behaviour of positive ground state solutions for <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2081_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation> small, when <i>p</i> is subcritical, or critical Sobolev exponent <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2081_Article_IEq6.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(2^*_s\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mn>2</mn> <mi>s</mi> <mo>∗</mo> </msubsup> </math></EquationSource> </InlineEquation>. For <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2081_Article_IEq7.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="49" /> </InlineMediaObject> <EquationSource Format="TEX">\(p&lt;2_s^*\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>&lt;</mo> <msubsup> <mn>2</mn> <mi>s</mi> <mo>∗</mo> </msubsup> </mrow> </math></EquationSource> </InlineEquation>, the ground state solution asymptotically coincides with unique positive ground state solution of <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2081_Article_IEq8.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="160" /> </InlineMediaObject> <EquationSource Format="TEX">\((-\Delta )^s u+u=|u|^{p-2}u\)</EquationSource> <EquationSource Format="MATHML"><math> <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>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> </mrow> </math></EquationSource> </InlineEquation>, whereas for <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2081_Article_IEq9.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="48" /> </InlineMediaObject> <EquationSource Format="TEX">\(p=2_s^*\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>=</mo> <msubsup> <mn>2</mn> <mi>s</mi> <mo>∗</mo> </msubsup> </mrow> </math></EquationSource> </InlineEquation> the asymptotic behaviour of the solutions, after a rescaling, is given by the unique positive solution of the nonlocal critical Emden-Fowler type equation. Additionally, for <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2081_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(\lambda &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> small, we show the uniqueness and nondegeneracy of the positive ground state solution using these asymptotic profiles of solutions.</p>

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Fractional Schrödinger Equations with Mixed Nonlinearities: Asymptotic Profiles, Uniqueness and Nondegeneracy of Ground States

  • Mousomi Bhakta,
  • Paramananda Das,
  • Debdip Ganguly

摘要

We study the fractional Schrödinger equations with a vanishing parameter: where \(s\in (0,1)\) s ( 0 , 1 ) , \(N>2s\) N > 2 s , \(2<q<p\le 2^*_s=\frac{2N}{N-2s}\) 2 < q < p 2 s = 2 N N - 2 s are fixed parameters and \(\lambda >0\) λ > 0 is a vanishing parameter. We investigate the asymptotic behaviour of positive ground state solutions for \(\lambda \) λ small, when p is subcritical, or critical Sobolev exponent \(2^*_s\) 2 s . For \(p<2_s^*\) p < 2 s , the ground state solution asymptotically coincides with unique positive ground state solution of \((-\Delta )^s u+u=|u|^{p-2}u\) ( - Δ ) s u + u = | u | p - 2 u , whereas for \(p=2_s^*\) p = 2 s the asymptotic behaviour of the solutions, after a rescaling, is given by the unique positive solution of the nonlocal critical Emden-Fowler type equation. Additionally, for \(\lambda >0\) λ > 0 small, we show the uniqueness and nondegeneracy of the positive ground state solution using these asymptotic profiles of solutions.