The absorption and fluorescence spectra of
1,1‘-diethyl-2,2‘-cyanine (pseudoisocyanine, PIC) aggregates
have
been studied between 8 and 293 K in water/glycerol glass containing
2−4 M of alkali halogenides. In this
system the J-aggregates have a single sharp band and there is
practically no contamination with the monomeric
dye, dimers, or H-aggregates. This allowed us to better resolve
the high-energy portion of the spectrum and
to assign the middle 535 nm band to the upper exciton transition.
The excitonic splitting at 8 K is the same
for both the blue and the red forms of aggregates (1270 ± 10
cm-1). The average energy of exciton
components
(18195 ± 15 cm-1 for the blue form) was
found to be very close to the 0−0 energy of the first strong
site
of PIC monomer (18223 cm-1) embedded in a
9-aza-PIC iodide matrix, which is transparent above 500 nm
[Marchetti, A. P.; Scozzafava, M. Chem. Phys.
Lett. 1976, 41, 87]. The 0−0
frequency of the nonsolvated
PIC monomer cation (ν0
0 = 19716 ± 40
cm-1 or 507.2 ± 1 nm) was obtained from the
solvent shift
measurements at room temperature. The absorption bandwidths and
shifts of both the PIC cation in poly(methyl methacrylate) matrix and the aggregates were recorded in the
temperature range between 8 and 300
K. The thermal shift of band maxima was analysed in terms of the
change in dispersive shift and excitonic
splitting as a result of the expansion of the matrix and a pure thermal
or phonon-induced contribution. The
thermal shift and broadening behavior of molecular and excitonic
transitions reveals large differences in the
mechanism and strength of the coupling to low-frequency
vibrations.