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conditions (CuCl/CuCl2 in pyridine).[9] The resulting mole-
small, discrete micelles. The diameters of the micelles and the
pores were measured to be approximately 3.5 nm and 3–5 nm,
respectively. The micellar diameter is about twice the length
of the molecule and thus indicates the presence of dimeric
micelles with a face-to-face stacking of the aromatic basal
planes. Further apparent evidence for the formation of in-
plane dimeric micelles was provided by topochemical poly-
merization of the sheets. Polymerization of the diacetylene
groups by irradiation of the solution with UV light for 6 h
yielded only dimers (see Figure S1 in the Supporting Infor-
mation). This result demonstrates that the primary structure
of the 2D sheets consists of dimeric micelles in which the two
aromatic planes within the micellar core face one another in
a slipped p–p stack for efficient dimerization of the diacety-
lene groups.[10]
1
cules were characterized by H and 13C NMR spectroscopy
and MALDI-TOF mass spectrometry and were shown to be
in full agreement with the structures presented.
Molecule 1 self-assembles into nanoporous sheets in
dilute aqueous solutions. Cryogenic transmission electron
microscopy (cryo-TEM) showed sheetlike objects with
curved edges against the vitrified solution background (Fig-
ure 2a); this observation is indicative of the formation of
flexible sheets in bulk solution. Notably, a high-resolution
To further confirm the primary structure of the 2D
aggregates, we conducted vapor pressure osmometry (VPO)
measurements in 1,4-dioxane in the concentration range of
6.1 to 17.7 gkgÀ1 (sample/solvent). The molecular weight of
the primary aggregate was measured to be 3617.3 Da, which is
twice that of the single molecule (1772.2 Da; see Figure S2)
and indicative of the formation of a dimeric aggregate. To
gain insight into the packing arrangement of the dimeric
micelles, we performed molecular-modeling experiments
through quantum-mechanical calculations with the
GAMESS software (Figure 2d). Energy minimization
showed that the aromatic plane adopts a boat conformation
in which the central benzene ring protrudes from the opposite
side of the basal plane to that occupied by the dendrimer. The
paired aromatic segments are “slipped” with respect to one
another to reduce steric hindrance between the protruding
benzene rings. The slipped stacking of the aromatic segments
is reflected in a red-shifted absorption maximum in aqueous
solution relative to that in chloroform (Figure 2c)[11] and
efficient topochemical polymerization of the dimeric micelles
as described above.
All of these observations indicate that 1 self-assembles
through a face-to-face stacking arrangement of the flat
aromatic segments into dimeric micelles with a flat aromatic
core. These dimeric micelles in turn grow laterally through
side-to-side hydrophobic interactions to form 2D sheets.
However, the lateral association of the dimeric micelles leads
to in-plane defects as a result of the weak lateral interactions
between the very thin aromatic cores owing to the slipped
packing arrangement. Thus, porous sheets are formed. This
weak lateral association of the micelles is also reflected in the
formation of flexible sheets.
Figure 2. a) Cryo-TEM image of a solution of 1 (200 mm; scale bar:
200 nm). b) Negatively stained TEM image of nanoporous sheets from
a 100 mm aqueous solution of 1 (scale bar: 100 nm). The insets in (a)
and (b) show magnified images (scale bars: 20 nm) and the line scan
profile along the yellow line. c) Absorption and emission spectra of
1 (100 mm) in CHCl3 (red line) and aqueous solution (black line);
lex =318 nm. d) Molecular modeling of the dimeric micelle without
coronene and the dimeric micelle containing coronene.
To investigate the role of the dimeric stacking of the
aromatic planes in the formation of the 2D porous sheets, we
modified the molecular structure. With the aim of interfering
with the dimeric stacking of the aromatic planes, we replaced
the monosubstituted aromatic segment with a basal plane
disubstituted at the two opposite faces to form 2 (Figure 1). In
great contrast to 1, 2 formed only irregular aggregates in
solution (see Figure S3). This behavior implies that the
dimeric stacking of the aromatic planes is essential for the
formation of a well-defined 2D porous structure.
image revealed that the sheets contained in-plane nanopores
with an average diameter of approximately 4 nm (Figure 2a,
inset). To obtain more information on these sheets, we also
performed TEM experiments with the samples cast onto
a TEM grid (and negatively stained with uranyl acetate). A
low-magnification image showed planar sheets with rugged
surfaces against a dark background. A higher-magnification
image showed that the rugged surfaces consisted of uniform
micelles and nanopores (Figure 2b, inset) and thus suggested
that the sheets had formed through a lateral association of
The formation of 2D sheets based on pairs of face-to-face-
stacked aromatic molecules stimulated us to investigate
2
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Angew. Chem. Int. Ed. 2013, 52, 1 – 5
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