<p>In recent years, considerable attention has been paid to the discrete fractional Laplace operator. In this paper, we define the fractional Laplace operator <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13163_2025_555_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="47" /> </InlineMediaObject> <EquationSource Format="TEX">\((-\Delta )^{s}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">)</mo> </mrow> <mi>s</mi> </msup> </math></EquationSource> </InlineEquation> on arbitrary finite graphs for any <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13163_2025_555_Article_IEq2.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="40" /> </InlineMediaObject> <EquationSource Format="TEX">\(s&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. Moreover, we investigate its properties, in particular its spectral characteristics for <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13163_2025_555_Article_IEq3.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="71" /> </InlineMediaObject> <EquationSource Format="TEX">\(0&lt;s&lt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>s</mi> <mo>&lt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> and its limiting behavior as <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13163_2025_555_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="53" /> </InlineMediaObject> <EquationSource Format="TEX">\(s\rightarrow 0^+\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo stretchy="false">→</mo> <msup> <mn>0</mn> <mo>+</mo> </msup> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13163_2025_555_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="55" /> </InlineMediaObject> <EquationSource Format="TEX">\(s\rightarrow 1^-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo stretchy="false">→</mo> <msup> <mn>1</mn> <mo>-</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>. These properties differ significantly from the continuous setting. Finally, we address the solvability of a fractional Kazdan–Warner equation involving <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13163_2025_555_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="47" /> </InlineMediaObject> <EquationSource Format="TEX">\((-\Delta )^{s}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">)</mo> </mrow> <mi>s</mi> </msup> </math></EquationSource> </InlineEquation> by means of variational methods and the method of upper and lower solutions.</p>

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Fractional Laplace operator on finite graphs

  • Mengjie Zhang,
  • Yong Lin,
  • Yunyan Yang

摘要

In recent years, considerable attention has been paid to the discrete fractional Laplace operator. In this paper, we define the fractional Laplace operator \((-\Delta )^{s}\) ( - Δ ) s on arbitrary finite graphs for any \(s>0\) s > 0 . Moreover, we investigate its properties, in particular its spectral characteristics for \(0<s<1\) 0 < s < 1 and its limiting behavior as \(s\rightarrow 0^+\) s 0 + and \(s\rightarrow 1^-\) s 1 - . These properties differ significantly from the continuous setting. Finally, we address the solvability of a fractional Kazdan–Warner equation involving \((-\Delta )^{s}\) ( - Δ ) s by means of variational methods and the method of upper and lower solutions.