Nanocrystalline films of TiO2,
Al2O3, and ZrO2 were used as hosts
for the merocyanine 3-acetyl-5-(2-(3-ethyl-2-benzothiazolidinylidene)ethylidene)rhodanine (Mc2) to
scrutinize templating effects in the accommodation
of the dye within their porous network. Composed of interconnected
mesoscopic oxide particles and pores, these
films are transparent, allowing for a straightforward application of
transmission spectroscopy to unravel the optical
features of the incorporated dye species. Apart from
H-aggregation, the formation of two different types of two-dimensional assemblies was witnessed yielding red-shifted absorption
bands which were identified as J-aggregates,
one showing Davidov splitting, the other having a single exciton band.
The herringbone packing of the dye molecules
in the layered structure of Mc2 sodium salt octahydrate single crystals
was taken to model the double-banded
J-aggregate structure. On mesoscopic hydroxylated TiO2
anatase films, the structure of the Mc2 assemblies is
controlled by the texture of the highly porous substrates as well as
their surface charge. Furthermore, it responds in
a striking fashion to the presence of solvent in the ambient to which
the films are exposed. Double-banded (herringbone
structure) and single-banded (parallel alignment of the dye) absorption
spectra can thus be obtained. The role of
solvent is to stabilize one particular aggregate geometry through
intercalation into the Mc2 aggregate. Electron
injection into TiO2 from both types of J-aggregates is
observed. Laser flash photolysis experiments show that
energy
transfer from the monomer to the J-aggregate is operative prior to
charge injection. On hydroxylated Al2O3
and
ZrO2 surfaces Mc2 undergoes physisorption and formation of
H-aggregates exhibiting a blue-shifted absorption with
regard to the monomer spectrum. Contrary to the results obtained
for TiO2 substrates, aggregation is hardly
influenced
by solvent in the ambient. In particular no J-aggregates can be
formed on bare Al2O3 and ZrO2
substrates. However,
when the porous films are impregnated with concentrated hydroxide
solutions, H- as well as J-aggregates are formed
in humid air. At high humidity, due to the hygroscopic salt
coating, the pores are completely filled with water,
leading to the precipitation of the dye molecules forming H-aggregates.
At lower humidity an air−water interface
builds up within the pores and a double-banded J-aggregate spectrum
appears. The spectrum is almost identical to
the one measured on Mc2 sodium salt octahydrate single crystals with a
layered organic−inorganic structure.
Resonance fluorescence originating from the energetically lower
exciton band and internal conversion from the higher
to the lower exciton band take place.