M. Olivucci et al., A CONICAL INTERSECTION MECHANISM FOR THE PHOTOCHEMISTRY OF BUTADIENE - A MC-SCF STUDY, Journal of the American Chemical Society, 115(9), 1993, pp. 3710-3721
The excited state (2(1)Ag) reaction paths involved in the photochemica
l transformations of butadiene have been studied via ab initio MC-SCF
methods. It is demonstrated that the reaction funnel assumes the form
of a conical intersection region where the ground (1(1)Ag) and first e
xcited (2(1)Ag) potential energy surfaces are degenerate. This mechani
sm is consistent with experimental results for the photochemical isome
rization and is also consistent with the observed absence of fluoresce
nce from the 2(1)Ag state. Thus the currently accepted mechanisms for
butadiene photochemistry which involve radiationless decay at avoided
crossing minima need to be replaced with a model that involves fully e
fficient return to the ground state via a conical intersection. In add
ition to the minima on the excited state surface, the lowest energy po
ints on the conical intersection region have been fully optimized. The
conical intersection points have been characterized by computing the
gradient difference and non-adiabatic coupling vectors. Reaction paths
from the excited state minima to these conical intersections have bee
n computed. The lowest energy path from the s-trans minimum on the 2(1
)Ag potential energy surface involves the rotation of the central C-C
bond coupled with asynchronous disrotatory motion of the terminal meth
ylenes and leads to an s-transoid conical intersection region without
passing over a barrier. The reaction path from the s-cis minimum leads
to an s-cisoid conical intersection that lies some 4 kcal mol-1 above
this minima. The nature of the possible reaction paths on the excited
state is consistent with the fact that the major products of the phot
ochemical reactions of butadiene are s-cis/s-trans isomerization and d
ouble bond cis/trans isomerization. These findings are also consistent
with the directions of the gradient difference and non-adiabatic coup
ling vectors computed at a point where the system enters the conical i
ntersection. In particular, the directions of these two vectors near t
he s-cisoid conical intersection are consistent with the production of
cyclobutane as minor product.