<p>In this article, we prove the decay estimate for the discrete Schrödinger equation (DS) on the hexagonal triangulation. The <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3026_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="59" /> </InlineMediaObject> <EquationSource Format="TEX">\(l^1\rightarrow l^\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>l</mi> <mn>1</mn> </msup> <mo stretchy="false">→</mo> <msup> <mi>l</mi> <mi>∞</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> dispersive decay rate is <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3026_Article_IEq2.gif" Format="GIF" Height="26" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="TEX">\(\left\langle t\right\rangle ^{-\frac{3}{4}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mfenced close="〉" open="〈"> <mi>t</mi> </mfenced> <mrow> <mo>-</mo> <mfrac> <mn>3</mn> <mn>4</mn> </mfrac> </mrow> </msup> </math></EquationSource> </InlineEquation>, which is faster than the decay rate of DS on the 2-dimensional lattice <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3026_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb {Z}^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">Z</mi> </mrow> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation>, which is <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3026_Article_IEq4.gif" Format="GIF" Height="26" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="TEX">\(\left\langle t\right\rangle ^{-\frac{2}{3}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mfenced close="〉" open="〈"> <mi>t</mi> </mfenced> <mrow> <mo>-</mo> <mfrac> <mn>2</mn> <mn>3</mn> </mfrac> </mrow> </msup> </math></EquationSource> </InlineEquation>, see [<CitationRef CitationID="CR33">33</CitationRef>]. The proof relies on the detailed analysis of singularities of the corresponding phase function and the theory of uniform estimates on oscillatory integrals developed by Karpushkin [<CitationRef CitationID="CR15">15</CitationRef>]. Moreover, we prove the Strichartz estimate and give an application to the discrete nonlinear Schrödinger equation (DNLS) on the hexagonal triangulation.</p>

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The asymptotic behavior of discrete Schrödinger equation on the hexagonal triangulation

  • Huabin Ge,
  • Bobo Hua,
  • Longsong Jia,
  • Puchun Zhou

摘要

In this article, we prove the decay estimate for the discrete Schrödinger equation (DS) on the hexagonal triangulation. The \(l^1\rightarrow l^\infty \) l 1 l dispersive decay rate is \(\left\langle t\right\rangle ^{-\frac{3}{4}}\) t - 3 4 , which is faster than the decay rate of DS on the 2-dimensional lattice \(\mathbb {Z}^2\) Z 2 , which is \(\left\langle t\right\rangle ^{-\frac{2}{3}}\) t - 2 3 , see [33]. The proof relies on the detailed analysis of singularities of the corresponding phase function and the theory of uniform estimates on oscillatory integrals developed by Karpushkin [15]. Moreover, we prove the Strichartz estimate and give an application to the discrete nonlinear Schrödinger equation (DNLS) on the hexagonal triangulation.