AB-INITIO MCSCF STUDY ON ELECTRONICALLY EXCITED SINGLET-STATES OF FULVALENE SYSTEMS - ENERGY COMPONENT ANALYSIS OF THE PSEUDO-JAHN-TELLER EFFECT
Citation
A. Toyota et S. Koseki, AB-INITIO MCSCF STUDY ON ELECTRONICALLY EXCITED SINGLET-STATES OF FULVALENE SYSTEMS - ENERGY COMPONENT ANALYSIS OF THE PSEUDO-JAHN-TELLER EFFECT, The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory, 102(33), 1998, pp. 6668-6675
Categorie Soggetti
Chemistry Physical
SICI code
1089-5639(1998)102:33<6668:AMSOEE>2.0.ZU;2-2
Abstract
Geometry optimizations of the lowest (second) excited singlet states o
f the fulvalene systems were carried out by using the ab initio MCSCF
method with the 6-31G(d) basis set. The electronically excited molecul
es are found to undergo a pseudo-Jahn-Teller (JT) distortion from D-2h
to C-2 nu On the basis of the results obtained, an energy component a
nalysis of the total energy has been carried out to elucidate the phys
ical picture of the pseudo-JT effect. Inspection of the energy compone
nts comprised in the total energy reveals that the stability of a less
symmetric structure (C-2 nu) is attributable commonly to the energy l
owerings of the intenuclear repulsion term and the interelectronic rep
ulsive and kinetic terms due to sigma electrons. These observations ar
e consistent with an expansion of the carbon skeleton brought about by
the pseudo-JT bond distortion. It is further found that in triafulval
ene and heptafulvalene the nuclear-electron attractive and interelectr
onic repulsive terms due to pi electrons contribute to the pseudo-JT s
tabilization, respectively. In pentafulvalene and 7,7'-bis(bicyclo[4.
1.0]hepta-1,3,5-trienylidene), on the other hand, both the nuclear-ele
ctron attractive and interelectronic repulsive terms due to pi electro
ns contribute to the energetic stability of the C-2 nu structure. Subs
equently, heptafulvalene undergoes a pseudo-JT effect from the planar
C-2 nu to a nonplanar C-s structure. Interestingly, the stability of n
onplanar C-s structure results from the energy lowering of the nuclear
-electron attractive term. Moreover, the structural and electronic pro
perties inherent in the less symmetric C-2 nu and C-s nuclear arrangem
ents of the electronically excited molecules are discussed.