Abstract <p>We study the discrete spectrum of the generalized Friedrichs model <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12202_2025_8192_Article_IEq1.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="67" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_{\lambda_{1}\lambda_{2}}(p),\)</EquationSource> <!--LobJMat2560017Kurbanov-m1--> </InlineEquation> which is associated with a system of two particles moving on a one-dimensional lattice <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12202_2025_8192_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb{Z}\)</EquationSource> <!--LobJMat2560017Kurbanov-m2--> </InlineEquation>. The model depends on parameters <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12202_2025_8192_Article_IEq3.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="73" /> </InlineMediaObject> <EquationSource Format="TEX">\(\lambda_{1},\lambda_{2}\in\mathbb{R}\)</EquationSource> <!--LobJMat2560017Kurbanov-m3--> </InlineEquation> and <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12202_2025_8192_Article_IEq4.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(p\in\mathbb{T}\)</EquationSource> <!--LobJMat2560017Kurbanov-m4--> </InlineEquation>. We prove under certain conditions, the existence of eigenvalues of <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12202_2025_8192_Article_IEq1.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="67" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_{\lambda_{1}\lambda_{2}}(p),\)</EquationSource> <!--LobJMat2560017Kurbanov-m5--> </InlineEquation> that eigenvalues lie below its essential spectrum. We also partition the first quadrant of the <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12202_2025_8192_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\((\lambda_{1},\lambda_{2})\)</EquationSource> <!--LobJMat2560017Kurbanov-m6--> </InlineEquation>-plane into several connected components, such that for each connected component, and for each fixed value of <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12202_2025_8192_Article_IEq7.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(p\)</EquationSource> <!--LobJMat2560017Kurbanov-m7--> </InlineEquation> in <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12202_2025_8192_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="60" /> </InlineMediaObject> <EquationSource Format="TEX">\(U_{\delta}(p_{\textrm{min}})\)</EquationSource> <!--LobJMat2560017Kurbanov-m8--> </InlineEquation> (where <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12202_2025_8192_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="60" /> </InlineMediaObject> <EquationSource Format="TEX">\(U_{\delta}(p_{\textrm{min}})\)</EquationSource> <!--LobJMat2560017Kurbanov-m9--> </InlineEquation> is <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12202_2025_8192_Article_IEq10.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(\delta\)</EquationSource> <!--LobJMat2560017Kurbanov-m10--> </InlineEquation>-neighborhood of the point <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12202_2025_8192_Article_IEq11.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(p_{\textrm{min}}\)</EquationSource> <!--LobJMat2560017Kurbanov-m11--> </InlineEquation>), the operator <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12202_2025_8192_Article_IEq12.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_{\lambda_{1}\lambda_{2}}(p)\)</EquationSource> <!--LobJMat2560017Kurbanov-m12--> </InlineEquation> has an exact number of eigenvalues below its essential spectrum.</p>

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The Discrete Spectrum of the Generalized Friedrichs Model with a Rank-Two Perturbation

  • Sh. Kh. Kurbanov,
  • S. S. Abduvayitov

摘要

Abstract

We study the discrete spectrum of the generalized Friedrichs model \(H_{\lambda_{1}\lambda_{2}}(p),\) which is associated with a system of two particles moving on a one-dimensional lattice \(\mathbb{Z}\) . The model depends on parameters \(\lambda_{1},\lambda_{2}\in\mathbb{R}\) and \(p\in\mathbb{T}\) . We prove under certain conditions, the existence of eigenvalues of \(H_{\lambda_{1}\lambda_{2}}(p),\) that eigenvalues lie below its essential spectrum. We also partition the first quadrant of the \((\lambda_{1},\lambda_{2})\) -plane into several connected components, such that for each connected component, and for each fixed value of \(p\) in \(U_{\delta}(p_{\textrm{min}})\) (where \(U_{\delta}(p_{\textrm{min}})\) is \(\delta\) -neighborhood of the point \(p_{\textrm{min}}\) ), the operator \(H_{\lambda_{1}\lambda_{2}}(p)\) has an exact number of eigenvalues below its essential spectrum.