I. Shim et al., ELECTRONIC STATES AND NATURE OF BONDING IN THE MOLECULE RHN BY ALL-ELECTRON AB-INITIO CALCULATIONS, Journal of molecular structure. Theochem, 393, 1997, pp. 127-139
In the present work, all-electron ab initio multi-configuration self-c
onsistent-field (CASSCF) and multi-reference configuration interaction
(MRCI) calculations have been carried out to determine the low-lying
electronic states of the molecule RhN. In addition, the relativistic c
orrections for the one-electron Darwin contact term and the relativist
ic mass-velocity correction have been determined in perturbation calcu
lations. The spectroscopic constants for the seven low-lying electroni
c states have been derived by solving the Schrodinger equation for the
nuclear motion numerically. The predicted ground state of RhN is (1)
Sigma(+), and this state is separated from the states (II)-I-3, (II)-I
-1, (5) Delta, (3) Sigma(-), (3) Delta and (1) Delta by transition ene
rgies of 1833, 4278, 6579, 8042, 9632, and 13886 cm(-1), respectively.
For the (1) Sigma(+) ground state, the equilibrium distance has been
determined as 1.640 (A) over circle, and the vibrational frequency as
846 cm(-1). The chemical bond in the (1) Sigma(+) electronic ground st
ate has triple bond character due to the formation of delocalized bond
ing pi and sigma orbitals. The chemical bond in the RhN molecule is po
lar with charge transfer from Rh to N giving rise to a dipole moment o
f 2.08 Debye at 3.1 a.u. in the (1) Sigma(+) ground state. An approxim
ate treatment of the spin-orbit coupling effect shows that the lowest-
lying spin-orbit coupled state is 0(+). This state is essentially deri
ved from the (1) Sigma(+) ground state. The second and third state, 0(
+) and 0(-), mainly arise from the (II)-I-3 state. The dissociation en
ergy of the RhN molecule in its (1) Sigma(+) ground state has been der
ived as 1.74 eV. (C) 1997 Elsevier Science B.V.