bisurea segments of the host and only form excimers with
neighboring pyrene guest molecules in the fibers (Fig. 1b).
In conclusion, we have shown that probe 5 is randomly
dispersed in the hard blocks of TPEs with matching bisurea
groups, but phase separates when the bisurea hard blocks have
a different alkyl spacer length between the urea groups. We are
currently investigating application of the observed selectivity
for colocalization and separation of multiple functional guests
in TPEs with more than one type of bisurea hard block.
This research was supported by NanoNed, a national
nanotechnology program coordinated by the Dutch Ministry
of Economic Affairs (project EPC.6338) and by the EU
Integrated Project NAIMO (No NMP4-CT-2004-500355).
Fig. 4 Fluorescence spectra (lexc = 358 nm) of thin films containing
1 and 10 mol% of 5 in 1 and 1 mol% of 5 in 4 at 10–30 ns delay time
after the excitation pulse (a) and decay of the emission between 400
and 700 nm of these films after the first 10 ns (b).
excimers in the films containing 3 and 10 mol% show almost no
broadening compared to the spectrum with 1 mol% of 5,
indicating that most guest molecules are dispersed up to at least
10 mol% (Fig. 3d). At much higher concentrations (20 and 30
mol%), the excitation spectra recorded at the emission wave-
length of 487 nm are broadened, however to a much lesser extent
than any of the non-matching excitation spectra containing only 1
mol% of 5. Also with UV/vis spectroscopy, the broadening of
spectra was only observed in the non-matching systems and at
very high concentrations in the matching system (Fig. S3, ESIw).
These observations establish that the needles observed by AFM in
these films are not an exclusive surface phenomenon, and that
they are in fact the phase separated pyrene molecules. Phase
separation of bisurea guests was already studied with DSC
measurements by Wisse et al.12
Notes and references
z The cleaning procedure comprises sonication in acetone for 15 min,
rubbing briefly with SDS soap solution, sonication in SDS soap
solution for 10 min, rinsing in a stream of demi water for 15 min
and finally sonication in isopropanol for 10 min.
y For polymer 4, a concentration of 1 mol% relative to the amount of
bisurea segments is not possible, therefore the weight concentration of
5 in 4 is kept the same as for 5 in 1.
1 (a) C. Fouquey, J. M. Lehn and A. M. Levelut, Adv. Mater., 1990,
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2 R. P. Sijbesma, F. H. Beijer, L. Brunsveld, B. J. B. Folmer, J. H. K.
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R. M. Kellogg and B. L. Feringa, Chem.–Eur. J., 1999, 5, 937–950.
5 M. de Loos, A. Friggeri, J. van Esch, R. M. Kellogg and B. L.
Feringa, Org. Biomol. Chem., 2005, 3, 1631–1639.
6 D. C. Popescu, M. M. J. Smulders, B. P. Pichon, N. Chebotareva, S.
Y. Kwak, O. L. J. van Asselen, R. P. Sijbesma, E. Di Masi and N. A.
J. M. Sommerdijk, J. Am. Chem. Soc., 2007, 129, 14058–14067.
7 M. R. J. Vos, P. H. H. Bomans, F. de Haas, P. M. Frederik, J. A.
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In order to study the effect of probe solubility on incorpora-
tion, a more soluble probe with a single pyrene moiety was
synthesized (6). When this molecule was mixed with the
matching polymer 1, the excimer band remained low even at
30 mol% incorporation, and no broadening was observed in
the excitation spectrum recorded at 487 nm (Fig. S4, ESIw).
Furthermore AFM showed that hard needle-like structures
were absent, which indicates that 6 is not phase separated from
the polymer matrix (Fig. S5, ESIw). These measurements
indicate that solubility is an important parameter in the
incorporation of probes in bisurea fibers, and that p-stacking
is a driving force for phase segregation of probe 5.
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investigated with time-gated fluorescence measurements.
Fig. 4a shows the emission spectra acquired in the time
interval between 10 and 30 ns after the pulsed excitation of
two films of polymer 1 containing 1 and 10 mol% of 5 and one
of polymer 4 containing 1 mol% of 5. The decay of the
emission between 400 and 700 nm cannot be described with
a single exponential decay (Fig. 4b). Therefore, decay times (t)
were fitted on the part of the curve after 40 ns for the films of
polymer 1 and on the part of the curve between 10 and 50 ns
for the film of polymer 4. In the film of 1 with 10 mol% of 5,
the emission decays considerably faster (t = 67 ns) than that
of the sample with only 1 mol% of 5 (t = 111 ns). The long
decay time is typical for pyrene.16 The shorter fluorescence
decay time of the 10 mol% sample could be caused by
concentrations quenching with enhanced non-radiative decay.
For the sample in polymer 4, the decay time is an order of
magnitude shorter (t = 8 ns). This reflects the fact that the
guest molecules in polymer 4 are phase-separated (Fig. 1c),
leading to short decay times, whereas at higher concentration
in the matching polymer 1 they are fully dispersed in the
ne
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¨
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ꢁc
This journal is The Royal Society of Chemistry 2008
Chem. Commun., 2008, 3915–3917 | 3917