<p>This work focus on the existence of normalized positive solutions to the following fractional Laplace equation (<InternalRef RefID="Equ1">1.1</InternalRef>) with a perturbation. For the mass-subcritical case, i.e., <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1930_Article_IEq1.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="104" /> </InlineMediaObject> <EquationSource Format="TEX">\(p \in (2,2+\frac{4\,s}{N})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>2</mn> <mo>,</mo> <mn>2</mn> <mo>+</mo> <mfrac> <mrow> <mn>4</mn> <mspace width="0.166667em" /> <mi>s</mi> </mrow> <mi>N</mi> </mfrac> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, we obtain a global minimizer with negative energy as <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1930_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="66" /> </InlineMediaObject> <EquationSource Format="TEX">\(h \in (\mathcal {H}_{1} ) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>h</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <msub> <mi mathvariant="script">H</mi> <mn>1</mn> </msub> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. On the other hand, for the mass-supercritical case, i.e., <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1930_Article_IEq3.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="110" /> </InlineMediaObject> <EquationSource Format="TEX">\( p \in (2+\frac{4\,s}{N},2_{s}^{*})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>2</mn> <mo>+</mo> <mfrac> <mrow> <mn>4</mn> <mspace width="0.166667em" /> <mi>s</mi> </mrow> <mi>N</mi> </mfrac> <mo>,</mo> <mmultiscripts> <mn>2</mn> <mrow> <mi>s</mi> </mrow> <mrow> <mrow /> <mo>∗</mo> </mrow> </mmultiscripts> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> where <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1930_Article_IEq4.gif" Format="GIF" Height="24" Rendition="HTML" Resolution="72" Type="Linedraw" Width="74" /> </InlineMediaObject> <EquationSource Format="TEX">\(2_{s}^{*}=\frac{2N}{N-2\,s}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mn>2</mn> <mrow> <mi>s</mi> </mrow> <mrow> <mrow /> <mo>∗</mo> </mrow> </mmultiscripts> <mo>=</mo> <mfrac> <mrow> <mn>2</mn> <mi>N</mi> </mrow> <mrow> <mi>N</mi> <mo>-</mo> <mn>2</mn> <mspace width="0.166667em" /> <mi>s</mi> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation>, there exists a mountain pass solution with positive energy as <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1930_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="66" /> </InlineMediaObject> <EquationSource Format="TEX">\(h \in (\mathcal {H}_{2} )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>h</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <msub> <mi mathvariant="script">H</mi> <mn>2</mn> </msub> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Existence of Normalized Positive Solution for Fractional Nonhomogeneous Elliptic Equations

  • Yulong Ye,
  • Yansheng Zhong

摘要

This work focus on the existence of normalized positive solutions to the following fractional Laplace equation (1.1) with a perturbation. For the mass-subcritical case, i.e., \(p \in (2,2+\frac{4\,s}{N})\) p ( 2 , 2 + 4 s N ) , we obtain a global minimizer with negative energy as \(h \in (\mathcal {H}_{1} ) \) h ( H 1 ) . On the other hand, for the mass-supercritical case, i.e., \( p \in (2+\frac{4\,s}{N},2_{s}^{*})\) p ( 2 + 4 s N , 2 s ) where \(2_{s}^{*}=\frac{2N}{N-2\,s}\) 2 s = 2 N N - 2 s , there exists a mountain pass solution with positive energy as \(h \in (\mathcal {H}_{2} )\) h ( H 2 ) .