Rhodamine B isothiocyanate was adsorbed onto microcrystalline
cellulose by two different
methods: deposition from ethanolic and aqueous solutions followed by
solvent evaporation and also from
aqueous solutions in equilibrium with the powdered solid and following
a dyeing protocol. After the
above-mentioned samples were carefully washed, the fluorescence quantum
yields (φF) determined were
about 0.40 ± 0.03 and 0.28 ± 0.03 for ethanol and water,
respectively, solvents that efficiently swell
cellulose, when these two solvents were used for sample preparation
with the first method, while for
dyed samples φF is only 0.10 ± 0.05. These values
for φF can be compared with 0.70 ± 0.03 obtained
for
rhodamine B entrapped in the polymer chains of microcrystalline
cellulose. X-ray photoelectron
spectroscopic studies present evidence for a smaller positive charge
density on the nitrogen atom for
dyed samples when compared with the adsorbed ones. This is
compatible with nitrogen atoms, which do
not participate in the conjugated system. These findings indicate
that rhodamine B has different
conformers in dyed samples as compared to adsorbed samples. In the
former case, the chemical bond,
anchoring the dye to microcrystalline cellulose, leads to nonplanar
conformers with smaller φF and
fluorescence lifetime (τF) values. In the latter
case, planar conformers predominate, with the consequent
increase of both lifetime and fluorescent quantum yield.
1,1‘-Diethyl-2,2‘-cyanine iodide and
1,1‘-diethyl-2,2‘-carbocyanine iodide were adsorbed onto
microcrystalline cellulose by two different methods: by deposition from
ethanolic solutions, followed by solvent
evaporation, and also from ethanolic solutions in equilibrium with the
powdered solid. Within experimental
error, both methods provided the same fluorescence quantum yield of the
adsorbed dyes in the concentration
range 0.01−5.0 μmol of dye per gram of cellulose. Ethanol
swells cellulose and some dye molecules become
entrapped within the natural polymer chains and in close contact with
the substrate. The use of
dichloromethane, a solvent which does not swell microcrystalline
cellulose, provides samples which exhibit
a smaller fluorescence quantum yield. This is consistent with a
larger degree of mobility (and also the
formation of nonplanar and less emissive conformers) of the cyanines
adsorbed on the surface of the solid
substrate, while entrapment provides more rigid, planar, and emissive
fluorophers. At the same time,
the adsorption isotherms of 2,2‘-cyanine on cellulose from alcoholic
and dichloromethane solutions show
that the specific cellulose surface area accessible for dye adsorption
is larger when adsorption is from
ethanol rather than from dichloromethane. For 2,2‘-cyanine the
fluorescence quantum yields (ΦF)
determined were about 0.08 when dichloromethane (a solvent which does
not swell cellulose) was used
for sample preparation, while with ethanol ΦF was
approximately 0.30. These values are about 3 orders
of magnitude higher than those in solution, showing the importance of
the rigid dry matrix in reducing
the nonradiative pathways of deactivation of the (π, π*) first
excited singlet state of this cyanine. X-ray
photoelectron spectroscopic studies present evidence for hydrogen
bonding of 2,2‘-cyanine to cellulose at
low loadings and for the formation of aggregates at higher loadings
adsorbing from both ethanol and
dichloromethane. This hydrogen bonding is assigned as involving
dye molecules entrapped within the
cellulose chains. On the other hand, for 2,2‘-carbocyanine,
evidence exists for an increase of hydrogen
bonding with dye loading. This result together with evidence from
ground-state diffuse reflectance absorption
and luminescence is compatible with dye molecules being firmly bonded
to the substrate by one of the
nitrogen atoms, with the other unbound.
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