Complete active space self‐consistent field potential energy surfaces, dipole moment functions, and spectroscopic properties of O3, CF2, NO−2, and NF+2

1991 ◽  
Vol 94 (1) ◽  
pp. 414-430 ◽  
Author(s):  
Kirk A. Peterson ◽  
Rudolph C. Mayrhofer ◽  
Edwin L. Sibert ◽  
R. Claude Woods
2008 ◽  
Vol 07 (04) ◽  
pp. 751-765 ◽  
Author(s):  
ZHIJI CAO ◽  
KRISHNAN BALASUBRAMANIAN

Spectroscopic properties of the low-lying electronic states of In 3 N , InN 3, and their ions are computed by the complete active-space self-consistent field (CASSCF) followed by multireference singles + doubles configuration interaction (MRSDCI) calculations. Our results predict that the spectra of In 3 N / InN 3 are substantially different from those of Ga 3 As / GaAs 3 and Al 3 P / AlP 3 tetramers. The ground state of In 3 N is a closed-shell 1 A ′1 state with a planar D 3h symmetry, whereas the ground state of InN 3 is a 1Σ+ state of linear In – N – N – N structure. The equilibrium geometries, vibrational frequencies, atomization energies, adiabatic ionization potentials, electron affinities, and other properties are discussed.


1996 ◽  
Vol 74 (5-6) ◽  
pp. 194-201 ◽  
Author(s):  
A. R. Allouche ◽  
M. Aubert-Frecon ◽  
F. Spiegelmann

Results of a complete active space self-consistent field treatment of the two lowest states of each symmetry 2A1, 2B1, and 2B2 of Li2H are reported. An isosceles triangle is predicted for the equilibrium geometry of the ground state (1)2A1 (RLiLi = 2.48 Å, RLiH = 1.70 Å) (1 Å = 10−10 m) and of the excited state (1)2B1 (RLiLi = 2.91 Å, RLiH = 1.58 Å) while a linear geometry is predicted for the (1)2B2, (2)2A1, (2)2B2, and (2)2B1 states with the following values for RLiH = RLiLi/2: 1-66, 1.57, 1.66, and 1.57 Å, respectively. Fitted analytical forms of the potential energy surfaces for the six states investigated are also displayed.


Sign in / Sign up

Export Citation Format

Share Document