1999
DOI: 10.1002/(sici)1097-461x(1999)75:4/5<533::aid-qua18>3.0.co;2-o
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Critical nuclear charges forN-electron atoms

Abstract: One‐particle model with a spherically‐symmetric screened Coulomb potential is proposed to describe the motion of a loosely bound electron in a multielectron atom when the nuclear charge, which is treated as a continuous parameter, approaches its critical value. The critical nuclear charge, Zc, is the minimum charge necessary to bind N electrons. Parameters of the model are chosen to meet known binding energies of the neutral atom and the isoelectronic negative ion. This model correctly describes the asymptotic… Show more

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Cited by 40 publications
(35 citation statements)
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“…The method has a potential applicability in predicting stable and metastable atomic and molecular states. For future studies, we will investigate the bound and resonance state energies for two-electron systems (He-like atoms) and will be compared with the available experimental and theoretical data, for example, the finite-size scaling method [16,17]. It is also valuable to extend the present work to the cases of the two-dimensional problems [18].…”
Section: Resultsmentioning
confidence: 71%
“…The method has a potential applicability in predicting stable and metastable atomic and molecular states. For future studies, we will investigate the bound and resonance state energies for two-electron systems (He-like atoms) and will be compared with the available experimental and theoretical data, for example, the finite-size scaling method [16,17]. It is also valuable to extend the present work to the cases of the two-dimensional problems [18].…”
Section: Resultsmentioning
confidence: 71%
“…As a particular case, we may consider an infinitely heavy m 3 particle (r = 0), so that the critical charge ratio is −z 3 /z 2 > 0.94537. This value has to be compared to 0.91102 given in the literature [10].…”
Section: Illustration: Stability In the Cases M 1 = M 2 And M → ∞mentioning
confidence: 56%
“…In Section 3, we introduce two different methods to find the Sturmian functions whose eigenvalues form a discrete set given any boundary condition, and we plotted some of the results for a modified attractive Coulomb potential with a short range interaction. Finally, in Section 4, we show some applications of both the negative as well as positive energy Sturmians as basis set to solve the ${\cal N}$ ‐electron atom with a one‐active electron model 10. We show that this basis set is therefore suitable to construct the wave function of a given bound or scattering problem for both long range Coulomb potentials or short range ones.…”
Section: Introductionmentioning
confidence: 99%