Relativistic and Electron Correlation Effects in Molecules of Heavy Elements

Author(s):  
G. L. Malli
1988 ◽  
Vol 102 ◽  
pp. 103-105
Author(s):  
M.H. Chen

AbstractThe experimental observations of the 3p63d92D – 3p53d102P transitions of the Co-like ions and 3p63d83F4– 3p53d93F3of the Fe-like ions have recently been extended to highly charged ions of heavy elements up to uranium (Z = 92). A comparison between the observed energies and calculated values from the Dirac-Fock model indicated persistent discrepancies of 3–4 eV for all ions. Systematic multiconfiguration Dirac–Fock calculations for these transitions have been carried out with emphasis on the effects of electron correlation. The previously found discrepancies between theory and experiment have mostly been removed after the inclusion of the electron–electron correlation effects in the theoretical calculations.


Author(s):  
Victor Giovanni de Pina ◽  
Bráulio Gabriel Alencar Brito ◽  
Guo -Q Hai ◽  
Ladir Cândido

We investigate many-electron correlation effects in neutral and charged coinage-metal clusters Cun, Agn, and Aun (n = 1 − 4) by ab initio calculations using fixed-node diffusion Monte Carlo (FN-DMC)...


2009 ◽  
Vol 109 (14) ◽  
pp. 3315-3324 ◽  
Author(s):  
Yasutaka Kitagawa ◽  
Yasuyuki Nakanishi ◽  
Toru Saito ◽  
Takashi Kawakami ◽  
Mitsutaka Okumura ◽  
...  

1993 ◽  
Vol 48 (1-2) ◽  
pp. 127-133 ◽  
Author(s):  
Kenneth E. Edgecombe ◽  
Vedene H. Smith, Jr. ◽  
Florian Müller-Plathe

Abstract Basis-set and electron-correlation effects on the appearance and disappearance of nonnuclear maxima in the electron density are examined in Li2 , Na2 , Na4 and Na5 . It is shown that nonnuclear attractors can be removed in all cases except Li2 . The appearance of a pseudoatom in a lithium molecule correlates remarkably well with the size of the region, in an atomic calculation, of V2r(r) for the valence shell of the atom. This and the fact that the pseudoatom is also present in the promolecule indicate that the pseudoatoms are remnants of, or in fact are portions of, atoms that are not perturbed enough in the molecule to remove an essentially atomic characteristic.


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