R. Disselkamp et al., CASSCF STUDY OF THE GROUND-STATE AND LOWEST LYING 3S RYDBERG STATES OF ABCO, Journal of physical chemistry, 99(19), 1995, pp. 7227-7230
An ab initio CASSCF study of the ground and first two excited 3s Rydbe
rg states (A(1), E) of azabicyclo[2.2.2]octane (ABCO) is presented. Th
e calculations support a previous assignment of the lowest energy tran
sition of ABCO as 2A(1) <-- 1A(1). The excited Rydberg state molecular
orbital 2A(1) is composed of 2p nitrogen, 3s nitrogen, and 3s carbon
orbitals. An examination of the HOMO and LUMO natural orbitals for thi
s state suggests that the atomic 3s carbon orbitals located on the car
bon atoms bonded to the tertiary nitrogen atom contribute roughly 80%
to each orbital. In fact, on the basis of these calculations, a more a
ccurate description of this Rydberg transition is as a two-electron ex
citation from S-0[2p(z)(N)](2) to a partially delocalized R(1)[3s(C)3s
(N)](2). The transition 2A(1) <-- 1A(1) is found experimentally at 39
080 cm(-1) and is calculated to appear at 36 067 cm(-1). An extended b
asis set calculation employing [3s plus 3p(x,y,z)(N)] orbitals does no
t alter these conclusions significantly. The second excited Rydberg st
ate (of E symmetry) is calculated to lie ca. 4000 cm(-1) above the fir
st. This state is calculated at the 3s active space level to be compos
ed of a 2p(z) nitrogen orbital (HOMO) and carbon atomic 3s orbitals lo
cated on the carbon atoms bonded to the nitrogen atom (LUMO). Employin
g a [3s plus 3p(N)] active space again has only a small effect on the
orbital composition of the excited E Rydberg state. On the basis of th
e energy separation between the 2A(1) and E Rydberg states, one can as
sign the second observed Rydberg transition to the E <-- 1A(1) excitat
ion. Geometry-optimized structures show that the C-N-C apex angle incr
eases upon electronic excitation R(2), R(1) <-- S-0, supporting a prev
ious assignment of cage compression vibrational modes in the vibronic
activity of these transitions. The effect of Rydberg state excitation
is analyzed in terms of charge redistribution in the ABCO molecule.