The ground state properties of isodiazene have been determined by standard
ab initio approaches. The vertical excitation energies of isodiazene for th
e low-lying valence and Rydberg excited states have been calculated by the
CASSCF and related MR-CISD and MCQDPT methods. The assignment of the experi
mental value of 1.95 eV to the transition to the (A) over tilde(1)A(2) (2b(
2) n, 2b(1) pi*) state has been confirmed. The experimentally observed abso
rption occuring in the range 3.96-4.88 eV, possibly at 4.77 eV, is assigned
to the transition to the lowest-lying singlet Rydberg state (B) over tilde
(1)B(2) (2b(2) n, 6a(1) 3s). The equilibrium structures of isodiazene in th
e lowest-lying singlet and triplet excited states (1,3)(n,pi*) are found to
be twisted with the C-8 symmetry. It can be expected that isodiazene, as w
ell as 1,2-diazene, has no well-defined equilibrium structures on the (1,3)
A "(n,pi*) potential energy surfaces due to the low inversion barriers. The
relative stabilities of isodiazene and 1,2-diazene are Found to be quite d
ifferent in the (1,3)(n,pi*) states than in the ground state. For the verti
cal spectra of the two isoelectronic molecules, isodiazene and formaldehyde
, it was found that the orders of singlet electronic states are similar, bu
t the relative stabilities of triplet states are different and the vertical
excitation energies of isodiazene are generally lower. The (1)(n,pi*)-(3)(
n,pi*) gap is much greater for isodiazene (1.30 eV) than for formaldehyde (
0.38 eV) and hence intersystem crossing of these states of isodiazene is hi
ghly improbable. (C) 2000 Elsevier Science B.V. All rights reserved.