Dm. Chen et al., Resonance Raman spectra and excited-state structure of aggregated tetrakis(4-sulfonatophenyl)porphyrin diacid, J PHYS CH A, 105(16), 2001, pp. 3981-3988
Resonance Raman (RR) spectra of aggregates of tetrakis(4-sulfonatophenyl)po
rphyrin diacid (H4TSPP2-) excited near exciton absorption bands of 489 nm (
J(B) band) and 421 nm (H-B band) were recorded and analyzed, and RR intensi
ties of the aggregates and segregated monomers were calculated with time-de
pendent resonant Raman formulas for the Franck-Condon mechanism of enhancem
ent. Their UV-visible absorption spectra were also calculated spontaneously
. On the basis of the RR spectra and computed results, the ground and excit
ed-state structures as well as molecular packing of aggregated H4TSPP2- hav
e been studied. It was deduced from the analyses that there are large dimen
sionless displacements on the excited state along the nu (8), gamma (16), a
nd nu (2) coordinates for both aggregated and segregated H4TSPP2-. These no
rmal modes involve mainly the CalphaCm, CbetaCbeta bond stretching and Calp
haCmCalpha bond angle bending motions. The low-frequency RR bands (< 500 cm
(-1)) were greatly enhanced when the excitation wavelength approaches the J
(B) absorption band of H4TSPP2- aggregates, which was attributed to narrowi
ng of the J(B) band due to the exciton interaction. It was revealed that th
e 489 and 421 nm absorption bands of H4TSPP2- aggregates can be attributed
to two different exciton manifolds originating from the degenerated B state
(S-2 state) of H4TSPP2-. Davydov splitting of the aggregates evaluated fro
m molecular exciton theory is well-coincident with the measured values, whi
ch supports a one-dimensional ribbon model for H4TSPP2- aggregates.