EXCITED-STATE INTRAMOLECULAR PROTON-TRANSFER IN 2-(2'-HYDROXYPHENYL)BENZIMIDAZOLE AND 2-(2'-HYDROXYPHENYL)-BENZOXAZOLE - EFFECT OF ROTAMERISM AND HYDROGEN-BONDING
K. Das et al., EXCITED-STATE INTRAMOLECULAR PROTON-TRANSFER IN 2-(2'-HYDROXYPHENYL)BENZIMIDAZOLE AND 2-(2'-HYDROXYPHENYL)-BENZOXAZOLE - EFFECT OF ROTAMERISM AND HYDROGEN-BONDING, Journal of physical chemistry, 98(37), 1994, pp. 9126-9132
An excited-state intramolecular proton transfer (ESIPT) process in 2-(
2'-hydroxyphenyl)benzimidazole and -benzoxazole (HPBI and HBO, respect
ively) has been studied using steady-state and time-resolved emission
spectroscopy at various temperatures and by semiempirical quantum chem
ical methods. For both of them two distinct ground-state rotamers I an
d II respectively responsible for the ''normal'' and the ''tautomer''
emission have been detected. In hydrocarbon solvents at room temperatu
re and at 77 K the tautomer emission predominates over the normal emis
sion for both HPBI and HBO. This indicates that rotamer II, responsibl
e for the tautomer emission, is intrinsically stabler than rotamer I,
which causes the normal emission. In alcoholic glass at 77 K for HPBI
a dramatic enhancement of the normal emission is observed. It is sugge
sted that due to the increased solvation, the more polar rotamer I bec
omes stabler than II for HPBI in alcohol and the substantial temperatu
re variation is due to the change in the population of the two rotamer
s with temperature. From the detailed temperature variation in alcohol
ic medium the ground-state energy difference between rotamers I and II
is determined. In dioxane-water mixtures it is observed that with the
addition of water the quantum yield of the normal emission increases,
which is ascribed to the inhibition of the ESIPT process due to the f
ormation of an intermolecular hydrogen bond involving water. CNDO/S-CI
calculations were performed optimizing the ground: state geometry by
the AM1 method. Details of the energy, dipole moment, and charge distr
ibution of the rotamers in the ground state (S-0) and the first excite
d singlet state (S-1) and the barrier for the interconversion of I and
II in S-0, S-1, and first excited triplet state are discussed. The ca
lculation indicates that the barrier for the interconversion of the tw
o rotamers is too high in the excited state (S-1 and T-1) for free int
erconversion.