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enables us to transfer the resultant objects to any substrate
such as a TEM grid (vide infra). These results indicate that the
formation of microspheres is substrate-independent, and the
objects can be prepared on different substrates for various
applications. In addition, neither light nor the water content
of the toluene solvent affected the resultant morphology;
similar microspheres composed of nanoplates were obtained
in the dark and also from water-saturated toluene solution. In
contrast, the drying speed, temperature, and solvent for the
Por/C60 blend strongly influence the resultant morphologies.
The microsphere morphology dominated only when the
drying process continued over 10 hours under a saturated
toluene atmosphere (see Figure S8 in the Supporting Infor-
mation). Without sufficient toluene vapor, disklike objects
were mainly formed, suggesting that these objects are
intermediates. Meanwhile, the microsphere objects were
obtained in the temperature range of 15–268C; at either
lower (108C) or higher (308C) temperatures, or with other
solvents such as benzene and p-xylene, we did not observe
microspheres on the Si surface.
Figure 1. SEM images of diverse objects of Por–C60 blend obtained
under different experimental conditions. Concentrations of C60 and Por
(in mgmLÀ1): a) 0.5, 0.05, b) 0.05, 0.05, c) 0.025, 0.25, d) 0.25, 0.25,
e) 0.5, 0. 25, f) 0.75, 0.25, respectively.
denotes the concentration of a repeating unit of Por in the
polymer shown in Scheme 1), highly monodisperse and
uniform microspheres (average size ca. 5 mm) comprising
nanoplates structures were predominantly obtained on the Si
wafer (Figure 2), accompanied by disklike objects (Figure S3
To obtain further insight into how C60 and Por organize in
the microspheres, we conducted Raman spectroscopy, X-ray
diffraction (XRD), and transmission electron microscopy
(TEM). Figure 3a shows Raman spectra recorded for micro-
spheres on a Si wafer. The corresponding spectra of C60 rods
Figure 2. SEM images of C60 microspheres of nanoplates. Concentra-
tions of C60 and Por (in mgmLÀ1): 0.5 and 0.25, respectively.
in the Supporting Information). Energy-dispersive X-ray
(EDX) spectroscopy analysis and element mapping revealed
that carbon is the main component of the microspheres, as
indicated by the prominent C peak; additional weak peaks
reveal the presence of O and Zn in the objects, indicating the
concomitance of Por in these microspheres (Figure S4 in the
Supporting Information and vide infra). As shown in Figure 2,
the microspheres range from 4–7 mm in diameter, and the
platelike building units were revealed to be 200–300 nm thick
from SEM images. Moreover, the size of the microspheres can
be fine-tuned by changing the concentration of C60. When the
C60 concentration was increased from 0.25 to 0.5, 1.0, and
2.0 mgmLÀ1, the average particle size increased from 3 to 5, 7,
and 10 mm, respectively, while the weight ratio between Por
and C60 was maintained at 1:2 (Figure S5 in the Supporting
Information). When we diluted the C60 solution to
0.1 mgmLÀ1, rodlike objects were mainly obtained.
Microspheres analogous to those obtained on the Si wafer
were also found on other substrates such as glass, indium tin
oxide coated glass, mica, and Al foil (Figure S6 in the
Supporting Information). Remarkably, both disk and micro-
sphere morphologies were also obtained from the slow
evaporation of a Por/C60 solution in toluene at the air–water
interface (Figure S7 in the Supporting Information), which
Figure 3. Raman spectra (a) and XRD patterns (b) of C60 powder, rods,
and microspheres.
obtained without Por under the same conditions and
untreated C60 powder are also shown for comparison. The
characteristic band for the Ag(2) pentagonal pinch mode in
the Raman spectra around 1460 cmÀ1 was observed for all of
microspheres, C60 rods, and untreated C60 (Figure 3a). This
indicates that only monomeric C60 molecules are involved in
these objects because the Ag(2) line shifts to lower frequency
in polymerized C60.[19] It should be noted, however, that the
Ag(2) band showed a substantial 3 cmÀ1 shift for microspheres
(1466 cmÀ1) relative to those observed for C60 rods and
untreated C60 (both at 1463 cmÀ1). This shift may be attributed
to supramolecular interactions between the porphyrin poly-
mer and C60. X-ray diffraction (XRD) patterns for micro-
spheres recorded on a Si substrate are shown in Figure 3b.
The well-defined XRD patterns of the microspheres match
very well with those of C60 rods and untreated C60. Thus these
patterns were readily assigned as a classic fcc structure: four
strong peaks are indexed as (111), (220), (311), and (222) from
the fcc lattices, indicating that the microspheres have pure fcc
crystal structure. In contrast, previously obtained C60 crystals
ꢀ 2009 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2009, 48, 9646 –9651