<p>In this paper, we study the <i>p</i>-Laplacian equation of the form <Equation ID="Equa"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="10114_2025_3304_Article_Equa.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="372" /> </MediaObject> <EquationSource Format="TEX">\(-\Delta_{p}u+h(x)\vert u \vert^{p-2}u=(R_{\alpha}* \vert u \vert^{q})\vert u \vert^{q-2}u+\vert u \vert ^{2q-2}u\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mo>−</mo> <msub> <mi mathvariant="normal">Δ</mi> <mrow> <mi>p</mi> </mrow> </msub> <mi>u</mi> <mo>+</mo> <mi>h</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> <mo fence="false" stretchy="false">|</mo> <mi>u</mi> <msup> <mo fence="false" stretchy="false">|</mo> <mrow> <mi>p</mi> <mo>−</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>=</mo> <mo stretchy="false">(</mo> <msub> <mi>R</mi> <mrow> <mi>α</mi> </mrow> </msub> <mo>∗</mo> <mo fence="false" stretchy="false">|</mo> <mi>u</mi> <msup> <mo fence="false" stretchy="false">|</mo> <mrow> <mi>q</mi> </mrow> </msup> <mo stretchy="false">)</mo> <mo fence="false" stretchy="false">|</mo> <mi>u</mi> <msup> <mo fence="false" stretchy="false">|</mo> <mrow> <mi>q</mi> <mo>−</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>+</mo> <mo fence="false" stretchy="false">|</mo> <mi>u</mi> <msup> <mo fence="false" stretchy="false">|</mo> <mrow> <mn>2</mn> <mi>q</mi> <mo>−</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> </math></EquationSource> </Equation> on lattice graphs ℤ<sup><i>N</i></sup>, where <i>N</i> ∈ ℕ*, <i>α</i> ∈ (0, <i>N</i>), <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10114_2025_3304_Article_IEq1.gif" Format="GIF" Height="25" Rendition="HTML" Resolution="72" Type="Linedraw" Width="147" /> </InlineMediaObject> <EquationSource Format="TEX">\(2 \leq p &lt; {2Nq \over N+\alpha}&lt;+\infty\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mn>2</mn> <mo>≤</mo> <mi>p</mi> <mo>&lt;</mo> <mrow> <mfrac> <mrow> <mn>2</mn> <mi>N</mi> <mi>q</mi> </mrow> <mrow> <mi>N</mi> <mo>+</mo> <mi>α</mi> </mrow> </mfrac> </mrow> <mo>&lt;</mo> <mo>+</mo> <mi mathvariant="normal">∞</mi> </math></EquationSource> </InlineEquation> and <i>R</i><sub><i>α</i></sub> represents the Green’s function of the discrete fractional Laplacian, which has no singularity at the origin but behaves as the Riesz potential at infinity. Under suitable assumptions on the potential <i>h</i>(<i>x</i>), we prove the existence of ground state solutions to the equation above by two different methods.</p>

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A Class of p-Laplacian Equations on Lattice Graphs

  • Lidan Wang

摘要

In this paper, we study the p-Laplacian equation of the form \(-\Delta_{p}u+h(x)\vert u \vert^{p-2}u=(R_{\alpha}* \vert u \vert^{q})\vert u \vert^{q-2}u+\vert u \vert ^{2q-2}u\) Δ p u + h ( x ) | u | p 2 u = ( R α | u | q ) | u | q 2 u + | u | 2 q 2 u on lattice graphs ℤN, where N ∈ ℕ*, α ∈ (0, N), \(2 \leq p < {2Nq \over N+\alpha}<+\infty\) 2 p < 2 N q N + α < + and Rα represents the Green’s function of the discrete fractional Laplacian, which has no singularity at the origin but behaves as the Riesz potential at infinity. Under suitable assumptions on the potential h(x), we prove the existence of ground state solutions to the equation above by two different methods.