Angewandte
Chemie
solvent, heat, and mechanical stress. Moreover, the surface of
the cross-linked flakelike objects combines a water-repellent
nature with durability.
(ca. 4.5 nm), we propose that the molecular arrangement in
the assembly is a bilayer structure with interdigitated and/or
disordered alkyl chains.
The fullerene derivative 1 was obtained in five steps[13,14]
starting from 1-hexadecyne (see Scheme S1 in the Supporting
Information) and unambiguously characterized by 1H and
13C NMR, FTIR, and UV/Vis spectroscopy, and MALDI-
TOF mass spectrometry. Self-organized objects were pre-
pared from 1 as follows: A solution of 1 (2.2 mg, 1 mmol) in a
mixture of THF/MeOH (3:2 v/v, 1 mL) at 508C was cooled to
208C and stored at À148C for 24 h to afford a dark-yellow
precipitate in quantitative yield. MeOH (3 mL) was added to
ensure complete formation of the precipitate, which was
stable in solution at room temperature. Flakelike micro-
particles of compound 2, which was used as a reference, were
prepared according to our previously published procedure[11c]
by heating a solution of 2 (1 mm) in 1,4-dioxane to 708C
followed by cooling to room temperature. The self-assembled
particles were removed from the dispersions and spread onto
a water surface to form a compact and uniform particle layer
at the air–water interface, which was then transferred onto
various substrates (Si, quartz, or glass) and dried under
vacuum for further studies.[15]
The field-emission scanning electron microscopy (SEM,
Figure 1a) image shows that 1 reproducibly self-assembles
into flakelike particles around 1 mm in size with crumpled
petal-shaped structures around 100 nm in thickness. High-
resolution cryogenic transmission electron microscopy (HR-
cryo-TEM) studies at the edge of the particle reveal a multi-
lamellar structure (Figure 1b). Fast Fourier transform (FFT)
analysis (Figure 1b, inset) indicates a lamellar periodicity of
(5.7 Æ 0.1) nm. In addition, the appearance of third-order
spots in the FFT indicated that the lamellar organization is
highly periodic. By taking into account the dimensions of 1
The multilamellar arrangement suggested from HR-cryo-
TEM studies is consistent with the XRD analysis of 1. As
shown in Figure 1c, the XRD pattern of the bulk precipitate
of 1 measured at 258C displays reflections of the (001) to
(009) planes, which indicate a long-range ordered lamellar
structure. The interlayer distance obtained from the XRD
analysis is 6.0 nm, which is slightly larger than that obtained
from TEM analysis and may result from different exper-
imental conditions such as temperature or pressure. More-
over, the two broad halos that appear at approximately 10.38
and 19.48 can be attributed to the in-plane average distance
between neighboring C60 molecules (ca. 8.7 nm) and the
average distance between molten alkyl chains (ca. 0.46 nm,
see below), respectively. The UV/Vis spectrum of the
particles of 1 at 258C shows three bands with absorption
maxima at 333, 270, and 256 nm. When compared to the
absorption maxima of a solution of 1 in n-hexane, these bands
are red-shifted by 17, 16, and 2 nm, respectively, which
indicates p–p interactions between the neighboring C60
molecules in the assembled objects (see Figure S2 in the
Supporting Information).[11] The FTIR spectrum of the
particles of 1 at 258C displays asymmetric and symmetric
methylene stretching bands at 2924 and 2852 cmÀ1, respec-
tively, which suggests that the alkyl chains are not in a
crystalline state.[16] This result is in agreement with differential
scanning calorimetry (DSC) data of the bulk precipitate of 1.
A broad shoulder around 158C and a peak centered at
29.18C, which correspond to the pretransition and the solid–
liquid crystalline transition of the alkyl chain, are observed
with DH and DS values of 55.4 kJmolÀ1 and 180 JmolÀ1 KÀ1,
respectively, for the later peak (see Figure S9a in the
Supporting Information). In addition, because of the ortho-
rhombic subcell structure of the oligomethylene units, the
methylene scissoring mode shows a broadly split band at
around 1463 cmÀ1 in the FTIR spectrum, which indicates that
parts of the alkyl chains could be interdigitated (Figure S3 in
the Supporting Information).[17] These results confirm that the
assembled particle of 1 is composed of bilayer structural
subunits with noncrystalline and partially interdigitated alkyl
chains (Scheme 1b).
Photoinduced cross-linking studies on the flakelike par-
ticles with cross-linkable DA and fullerene moieties were
carried out. Photoreactions of the DA moieties were studied
by FTIR spectroscopy (Figure 2). Upon irradiation at 258C
with a 150 W low-pressure Hg lamp, the IR absorption bands
at 2256 and 2191 cmÀ1, assigned to the asymmetric vibrational
mode of the DA monomer, gradually decreased. This is
accompanied by the appearance of a new band centered at
2212 cmÀ1, which is assigned to the asymmetric vibrational
[12a,c]
ꢀ
mode of the C C bond in the poly(diacetylenes) (PDs).
Figure 1. a) SEM image of the self-organized particles of 1 prepared
from THF/MeOH solution. The inset shows an enlarged particle
image (scale bar=500 nm). b) HR-cryo-TEM image of the edge of one
particle. The inset shows the corresponding FFT analysis showing the
1st, 2nd, and 3rd order spots. The periodicity of the lamellae is
5.7 nm. c) X-ray diffraction pattern of the self-organized particles of 1
at 258C. The corresponding d-spacing value is 6.0 nm.
To unambiguously assign the spectral changes, an IR inves-
tigation of the precursor molecule of 1 (Scheme S1 in the
Supporting Information) containing the DA moieties was
carried out. UV irradiation caused a similar trend in the FTIR
spectra (Figure S4 in the Supporting Information). The bands
at 2256 and 2179 cmÀ1 gradually disappeared, and a new band
Angew. Chem. Int. Ed. 2009, 48, 2166 –2170
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