<p>In this paper, we consider the continuous Schrödinger operators <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40509_2025_365_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_c\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>H</mi> <mi>c</mi> </msub> </math></EquationSource> </InlineEquation> in <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40509_2025_365_Article_IEq4.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^2({{\mathbb {R}}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">R</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40509_2025_365_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(\delta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>δ</mi> </math></EquationSource> </InlineEquation>-point interactions supported on a slightly perturbed lattice <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40509_2025_365_Article_IEq6.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Γ</mi> </math></EquationSource> </InlineEquation> of <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40509_2025_365_Article_IEq7.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\ell {\mathbb {Z}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ℓ</mi> <mi mathvariant="double-struck">Z</mi> </mrow> </math></EquationSource> </InlineEquation> with a small parameter <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40509_2025_365_Article_IEq8.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(\ell &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ℓ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and its discrete approximation. Unlike equidistant lattices <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40509_2025_365_Article_IEq9.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\ell {{\mathbb {Z}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ℓ</mi> <mi mathvariant="double-struck">Z</mi> </mrow> </math></EquationSource> </InlineEquation>, it can be natural to construct the one-dimensional discrete Schrödinger operators <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40509_2025_365_Article_IEq10.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_d\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>H</mi> <mi>d</mi> </msub> </math></EquationSource> </InlineEquation> in <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40509_2025_365_Article_IEq11.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="37" /> </InlineMediaObject> <EquationSource Format="TEX">\(\ell ^2(\Gamma )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>ℓ</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Γ</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> by taking inspiration from the Shortley–Welley method utilized in the numerical analysis. In spirit to the method constructed by Exner et al. (Lett Math Phys 112(4):Paper No. 83, 15, 2022) for the equilateral lattice quantum graph Hamiltonian, we give an estimate for the resolvent difference between <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40509_2025_365_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_c\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>H</mi> <mi>c</mi> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40509_2025_365_Article_IEq10.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_d\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>H</mi> <mi>d</mi> </msub> </math></EquationSource> </InlineEquation> with an identification operator as <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40509_2025_365_Article_IEq14.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(\ell \rightarrow 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ℓ</mi> <mo stretchy="false">→</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Resolvent differences between 1-D Schrödinger operators with \(\delta \)-interactions and their discrete approximations

  • Hiroaki Niikuni

摘要

In this paper, we consider the continuous Schrödinger operators \(H_c\) H c in \(L^2({{\mathbb {R}}})\) L 2 ( R ) with \(\delta \) δ -point interactions supported on a slightly perturbed lattice \(\Gamma \) Γ of \(\ell {\mathbb {Z}}\) Z with a small parameter \(\ell >0\) > 0 and its discrete approximation. Unlike equidistant lattices \(\ell {{\mathbb {Z}}}\) Z , it can be natural to construct the one-dimensional discrete Schrödinger operators \(H_d\) H d in \(\ell ^2(\Gamma )\) 2 ( Γ ) by taking inspiration from the Shortley–Welley method utilized in the numerical analysis. In spirit to the method constructed by Exner et al. (Lett Math Phys 112(4):Paper No. 83, 15, 2022) for the equilateral lattice quantum graph Hamiltonian, we give an estimate for the resolvent difference between \(H_c\) H c and \(H_d\) H d with an identification operator as \(\ell \rightarrow 0\) 0 .