<p>We determine the principal term of the asymptotics of the integrated density of states (IDS) <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="209_2025_3840_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(N(\lambda )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo stretchy="false">(</mo> <mi>λ</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> for the Schrödinger operator with point interactions on <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="209_2025_3840_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\({\textbf{R}}^3\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="bold">R</mi> </mrow> <mn>3</mn> </msup> </math></EquationSource> </InlineEquation> as <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="209_2025_3840_Article_IEq5.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="74" /> </InlineMediaObject> <EquationSource Format="TEX">\(\lambda \rightarrow -\infty ,\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo stretchy="false">→</mo> <mo>-</mo> <mi>∞</mi> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> provided that the set of positions of the point obstacles is the Poisson configuration, and the interaction parameters are bounded i.i.d. random variables. In particular, we prove <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="209_2025_3840_Article_IEq6.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="133" /> </InlineMediaObject> <EquationSource Format="TEX">\(N(\lambda ) = O(|\lambda |^{-3/2})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mrow> <mo stretchy="false">(</mo> <mi>λ</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mi>O</mi> <mo stretchy="false">(</mo> <mo stretchy="false">|</mo> <mi>λ</mi> <msup> <mo stretchy="false">|</mo> <mrow> <mo>-</mo> <mn>3</mn> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> as <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="209_2025_3840_Article_IEq7.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="74" /> </InlineMediaObject> <EquationSource Format="TEX">\(\lambda \rightarrow -\infty .\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo stretchy="false">→</mo> <mo>-</mo> <mi>∞</mi> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation> In the case that all interaction parameters are equal to a constant, we give a more detailed asymptotics of <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="209_2025_3840_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="44" /> </InlineMediaObject> <EquationSource Format="TEX">\(N(\lambda ),\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo stretchy="false">(</mo> <mi>λ</mi> <mo stretchy="false">)</mo> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> and verify the result by a numerical method using the R programming language. As a byproduct, we give a rigorous definition of the Schrödinger operators with point interactions on a bounded open set with the Dirichlet or Neumann boundary conditions by the method of quadratic form, and study fundamental properties about the counting functions of eigenvalues; e.g., Dirichlet–Neumann bracketing, etc.</p>

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Integrated density of states for the Poisson point interactions on \({\textbf{R}}^3\)

  • Masahiro Kaminaga,
  • Takuya Mine,
  • Fumihiko Nakano

摘要

We determine the principal term of the asymptotics of the integrated density of states (IDS) \(N(\lambda )\) N ( λ ) for the Schrödinger operator with point interactions on \({\textbf{R}}^3\) R 3 as \(\lambda \rightarrow -\infty ,\) λ - , provided that the set of positions of the point obstacles is the Poisson configuration, and the interaction parameters are bounded i.i.d. random variables. In particular, we prove \(N(\lambda ) = O(|\lambda |^{-3/2})\) N ( λ ) = O ( | λ | - 3 / 2 ) as \(\lambda \rightarrow -\infty .\) λ - . In the case that all interaction parameters are equal to a constant, we give a more detailed asymptotics of \(N(\lambda ),\) N ( λ ) , and verify the result by a numerical method using the R programming language. As a byproduct, we give a rigorous definition of the Schrödinger operators with point interactions on a bounded open set with the Dirichlet or Neumann boundary conditions by the method of quadratic form, and study fundamental properties about the counting functions of eigenvalues; e.g., Dirichlet–Neumann bracketing, etc.