Abstract <p>In this paper, we investigate the tensor sum <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(H_{\mu,\lambda}\)</EquationSource> <!--LobJMat2561140Rasulov-m1--> </InlineEquation> with <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mu,\lambda&gt;0\)</EquationSource> <!--LobJMat2561140Rasulov-m2--> </InlineEquation>, constructed from two Friedrichs models perturbed by rank two operators. The Hamiltonian <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(H_{\mu,\lambda}\)</EquationSource> <!--LobJMat2561140Rasulov-m3--> </InlineEquation> describes a system of three quantum particles on a d-dimensional lattice. We define a set of parameters <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\mu\)</EquationSource> <!--LobJMat2561140Rasulov-m4--> </InlineEquation> and <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\lambda\)</EquationSource> <!--LobJMat2561140Rasulov-m5--> </InlineEquation> such that the essential spectrum of the Hamiltonian <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(H_{\mu,\lambda}\)</EquationSource> <!--LobJMat2561140Rasulov-m6--> </InlineEquation> is given by the union of one, two, or three closed intervals. The point spectrum of the Hamiltonian <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(H_{\mu,\lambda}\)</EquationSource> <!--LobJMat2561140Rasulov-m7--> </InlineEquation> is investigated through finite integrals appearing in the Fredholm determinant associated with the Friedrichs model.</p>

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Essential and Point Spectrum of a Model Hamiltonian Associated with the Three-particle Quantum Systems on a Lattice

  • Tulkin Rasulov,
  • Bekzod Bahronov

摘要

Abstract

In this paper, we investigate the tensor sum \(H_{\mu,\lambda}\) with \(\mu,\lambda>0\) , constructed from two Friedrichs models perturbed by rank two operators. The Hamiltonian \(H_{\mu,\lambda}\) describes a system of three quantum particles on a d-dimensional lattice. We define a set of parameters \(\mu\) and \(\lambda\) such that the essential spectrum of the Hamiltonian \(H_{\mu,\lambda}\) is given by the union of one, two, or three closed intervals. The point spectrum of the Hamiltonian \(H_{\mu,\lambda}\) is investigated through finite integrals appearing in the Fredholm determinant associated with the Friedrichs model.