1970
DOI: 10.1051/jphyscol:1970422
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The Pseudo-Atom : A Soluble Many Body Problem

Abstract: HAL is a multi-disciplinary open access archive for the deposit and dissemination of scientific research documents, whether they are published or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers. L'archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d'enseignement et de recherche français ou étrangers, des labor… Show more

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Cited by 11 publications
(10 citation statements)
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“…The agreement with our exact results puts the adiabatic-SCE and the adiabatic-ZPE approximations on firmer ground and gives confidence in employing the formalism of strictly correlated electrons in the adiabatic approximation for calculating response properties of strongly correlated systems. To illustrate some properties of the response function in the large interaction limit for an inhomogeneous system, let us analyze a model system of two harmonically confined electrons in three dimensions with a harmonic repulsion [59]. The Hamiltonian of the system is given bŷ…”
Section: Discussionmentioning
confidence: 99%
“…The agreement with our exact results puts the adiabatic-SCE and the adiabatic-ZPE approximations on firmer ground and gives confidence in employing the formalism of strictly correlated electrons in the adiabatic approximation for calculating response properties of strongly correlated systems. To illustrate some properties of the response function in the large interaction limit for an inhomogeneous system, let us analyze a model system of two harmonically confined electrons in three dimensions with a harmonic repulsion [59]. The Hamiltonian of the system is given bŷ…”
Section: Discussionmentioning
confidence: 99%
“…state energy at β 0 is equal to the energy of the first-excited state at β 1 ,is equal to the energy of 2th-excited state at β 2 etc, is equal to the energy of nth excited state at β n . 3 For the Coulomb the second-type representation is nothing but the well-known Sturm representation. 4 It belongs to the case VIII in the classification [5].…”
mentioning
confidence: 99%
“…In[3] so called pseudo atoms were introduced : quantum system made from atomic ones in which all Coulomb interactions are replaced by oscillator ones, attractive or repulsive as the case may be. The system described by (1) can be treated as modified twoelectron pseudo atom: where Coulomb attractive interactions are replaced by oscillator ones, while Coulomb repulsion remains unchanged or modified by the linear interaction.2 Precisely speaking, this means that for the parameters β 0 , β 1 , .…”
mentioning
confidence: 99%
“…A third example is the so-called pseudoatom model by Moshinsky and co-workers [14]. In this model both the electron-nucleus and electron-electron interactions are replaced by harmonic oscillator interactions (attractive in the first case and repulsive in the second).…”
Section: Discussionmentioning
confidence: 99%