Ab initio calculation of the electronic structure of the [Co(CN)6]3− ion

1979 ◽  
Vol 60 (2) ◽  
pp. 257-260 ◽  
Author(s):  
Mitsuru Sano ◽  
Hideo Yamatera ◽  
Yasuyo Hatano
1993 ◽  
Vol 280 (3) ◽  
pp. 398-414 ◽  
Author(s):  
R. Eibler ◽  
H. Erschbaumer ◽  
C. Temnitschka ◽  
R. Podloucky ◽  
A.J. Freeman

1993 ◽  
Vol 43 (9-10) ◽  
pp. 1003-1007 ◽  
Author(s):  
Wolf Gero Schmidt ◽  
Bernd Wenzien ◽  
Friedhelm Bechstedt

1974 ◽  
Vol 28 (2) ◽  
pp. 182-185 ◽  
Author(s):  
Tokio Yamabe ◽  
Tatsuhiro Aoyagi ◽  
Shinichi Nagata ◽  
Hideki Sakai ◽  
Kenichi Fukui

1971 ◽  
Vol 10 (5) ◽  
pp. 522-525 ◽  
Author(s):  
J. Demuynck ◽  
A. Veillard ◽  
G. Vinot

2010 ◽  
Vol 156-157 ◽  
pp. 1590-1593
Author(s):  
Xun Wang ◽  
Hong Sun ◽  
Yue Hua Wang ◽  
Zhen Ning Ma ◽  
Qing Jie Wang ◽  
...  

The shell model (SM) can simulate dipole and other properties concerning electrons. In this paper, an new scheme of SM potential is developed. Unlike the traditional SM, there are no harmonic spring between core and shell, and the potential functions are Coulomb potential multiplied by trigonometric function. The parameters of SM for hydrogen system were fitted by electronic structure data, which is from quantum chemistry ab initio calculation of H, + 2 H and 2 H . And the potential was examined by calculating the most stable structure of H2 and + 2 H by geometry optimization globally, which is agree with the ab initio calculation results. Furthermore, even the energy level of H atom can be calculated by this scheme SM potential, but the reasonable results can not obtained.


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