Fig. 2 Fluorescence spectrum of copolymer 3, in the region of coumarin-2
emission, before and after grafting. Inset shows the spectrum of the same
copolymer in the region where the Ru(bpy)3 acceptor complex emits.
Fig. 3 UV spectrum of polymer 1, obtained by the copolymerization
route.
polymer. The absorption band at 290 nm is further increased due
to the two additional bipyridine ligands introduced by the
reaction. Fluorescence resonance energy transfer studies were
carried out to determine the efficiency of energy transfer from
the coumarin-2 chromophore to the ruthenium complex. The
efficiency was calculated by comparing the coumarin-2 emis-
sion in the starting polymer 3 (a donor model compound) to the
emission of this dye in the polymer obtained after grafting of
ruthenium (Fig. 2). Based on the quenching of this emission, an
energy transfer efficiency of 70% was determined for the
grafted copolymer. Additionally, a 5-fold increase of the
ruthenium emission was observed upon excitation of the
coumarin-2 units (lex = 350 nm) over excitation of the
ruthenium complex directly (lex = 465 nm), this type of
amplification is the direct result of energy transfer (Fig. 2,
inset).
Fig. 4 Fluorescence spectrum of polymer 1, obtained by the copoly-
merization route.
Although the grafting route enabled us to obtain a polymer
displaying good energy transfer characteristics, the functional-
ization of the polymer, estimated from the relative UV-Vis
absorbance of the coumarin-2 and Ru(bpy)3 units, was not
quantitative (ca. 30%) and some insoluble material was also
formed, decreasing the polymer yield. Therefore the copoly-
merization of monomers 4 and 5 was studied. The ruthenium-
containing monomer 4 was prepared using a modified literature
procedure.8 Polymerization of the monomers was then per-
formed at 90 °C with AIBN in DMF (mol fraction of 5 = 0.75).
The resulting polymer was purified by precipitation in Et2O and
extensive washing with MeOH. The UV-visible spectrum of the
polymer showed that incorporation of the ruthenium monomer
4 was as expected from the feed ratio, ca. 25%, with the
remainder of the polymer repeat units consisting of the
coumarin-containing monomer 5, therefore the copolymeriza-
tion route is much more effective for the introduction of the
Ru(bpy)3 complex than the grafting reaction.
The absorption spectrum of the copolymer (Fig. 3) is similar
to that of the material obtained by the grafting route except that
it displays stronger bipyridine and ruthenium metal to ligand
charge transfer bands at 290 and 465 nm. Excitation of this
polymer at 350 nm results in an emission spectrum (Fig. 4) that
is totally quenched at 440 nm (the coumarin emission),
indicating that quantitative energy transfer between the cou-
marin-2 and the Ru(bpy)3 units occurs in this copolymer.
Furthermore, the intensity of the ruthenium emission at 630 nm
is increased by a factor of 2.7 when the polymer is illuminated
at 350 nm vs. 465 nm. This increase is lower than that observed
for the grafted copolymer, again indicating that, as a result of
incomplete grafting, a higher concentration of donors relative to
acceptors was present in that case.
In conclusion, readily accessible linear copolymers contain-
ing coumarin-2 and Ru(bpy)3 units can provide quantitative
energy transfer from the coumarin-2 units to the ruthenium
centers. This finding opens interesting perspectives in the field
of solar energy conversion.9 The application of such a system to
photovoltaic devices is currently under investigation.
Financial support of this research by the AFOSR (F-
49620-01) and the U. S. Department of Energy (# DE-AC03-
76SF00098). Fellowship support from the Eastman Kodak
Company is also gratefully acknowledged (A. A).
Notes and references
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6 M. Wörner, G. Greiner and H. Rau, J. Phys. Chem., 1995, 99, 14161.
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Chem. Commun., 2001, 1160–1161
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