A R T I C L E S
Simpson et al.
chlorination or partial cyclization defects could be avoided
(Figure 5). The yellow compound was soluble under gentle
warming in organic solvents such as chloroform, THF, and
toluene. Solution NMR studies, however, resulted, even under
heating, only in broad, unresolved spectra.
Due to the steric repulsion of the alkyl chain substituents,
the trimer molecule is very unlikely to assume a planar
conformation. The twisting of the three HBC-moieties out of
plane leads to the formation of a propeller-shaped object, as
illustrated by the calculated 3D-visualization in Figure 7. The
three blades can be expected to possess a certain degree of
rotational freedom around the bond connecting the core, thus
explaining the good observed solubility. Excluding the flexible
alkyl chains, such a rotor possesses a diameter of about 3 nm.
The out-of-plane twist of the HBC-sections is also confirmed
by the absorption spectrum of the propeller molecule, which is
depicted in Figure 6. The positions of the main bands are almost
unchanged as compared to the hexaalkyl HBC-“monomer” 4a.
This proves that the aromatic chromophores in 26 are HBC-
units, which are not in conjugation with each other. This is a
result of the torsion angle with respect to the benzene linker
and prevents an efficient electronic communication by overlap
of the pz orbitals. The peak width of the bands of 26 is, however,
increased. The comparison of the absorption spectra of the HBC-
“monomer” and its propeller-shaped trimer bears a striking
resemblance to the situation of the model compound C156 and
the C474 propeller as seen in Figure 2e. This serves as a
confirmation that an aromatic chromophore that is the same as
or very similar to that of C156 is present in the C474 propeller.
Figure 4. Raman spectra of propeller 9 (a) and the model compound 10b
(b).
the G- and D-bands, respectively, are typical features of PAHs,
carbonaceous materials, and disordered graphite.19 Slight dif-
ferences between the two spectra (i.e., relative intensities and
positions of the bands) appear in the spectral region at around
1300 cm-1 because of the higher sensitivity of the D-peak
frequency to molecular size and geometry than the G-peak.
Usually D-bands of PAHs show structured features composed
of a very strong band and a few low intensity lines. Minor
differences are observed in the positions of these low intensity
peaks of the two compounds. The direct comparison of the two
spectra also shows an increased intensity and broadening of the
D-peak of 9 in relation to the D-peak of the model compound
10b. For PAHs generally, the intensity of the D-peak with
respect to the G-band is dependent on the degree of π-electron
delocalization. The broadening of this band corresponds to the
convolution of Raman transitions from a distribution of aromatic
“domains” with different structures and dimensions. Therefore,
two conclusions can be drawn from the Raman measurements:
the subunits of the C474-propeller 9 and the C156 model
compound 10b are generally very similar; there are, however,
some defect structures present in the “propeller blades”.
A propeller-shaped model compound in which the partitioned
aromatic domains were unambiguous should further assist in
understanding the analytical data obtained for the propeller 9.
A suitable molecule can be prepared starting also from
1,3,5-tris-(4-iodophenyl)-benzene (14). By coupling 14 under
Hagihara-Sonogashira conditions with a phenylacetylene and
subsequent Diels-Alder reaction, an oligophenylene (25) is
accessible, bearing three separate hexaphenylbenzene moieties,
which cannot further interconnect. These can in turn be
planarized individually by cyclodehydrogenation, so that a trimer
of HBC-units (26) is formed, which is tethered in the center
via a trigonal benzene connector (Scheme 6). To enable
characterization by solution-based methods, alkyl substitution
in the form of 3,7-dimethyloctyl chains was possible by
employing suitably derivatized building blocks. Using 3 equiv
of iron(III) chloride as reagent, 26 was successfully formed as
a monodisperse compound by removing 36 hydrogens. Accord-
ing to the isotopically resolved MALDI-TOF mass spectrum,
Having clearly reached the limits of synthesis and spectro-
scopical characterization, it was desirable to further characterize
the C474 propeller objects also by visualization, for example,
by TEM. This attempt failed essentially because it was not
possible to prepare separated single molecules from the insoluble
compound on TEM grids. Only large particles with a very low
degree of order down to about 100 nm were observed,
corresponding to large clusters of the molecule.
Nevertheless, the available spectroscopical structure analysis
data were sufficient to be confident of the proposed three-
dimensional structure of 9 and to move on to apply the
cyclodehydrogenation conditions to a different geometric den-
drimer structure.
The dendrimer 11 possesses a tetraphenylmethane core
forcing the oligophenylene branches to adopt a tetrahedral
geometry (Scheme 3 and Figure 8a) which thus prevents a
complete planarization. Ideally, the removal of 136 hydrogens
should afford four planarized wings consisting of rigid PAHs,
which originate from the central core and point to the four
corners of a tetrahedron. The resulting molecule resembles a
tetra-bladed propeller (Figure 8c). The conditions for the
oxidative cyclodehydrogenation of dendrimer 11 with iron(III)
chloride were similar to those applied to the dendrimer 7. A
detailed analysis of the mass spectra became possible because
isotopic resolution of the individual peaks could be achieved
in this mass region. Using 0.75 equiv of iron(III) chloride per
intendendly removed hydrogen led to a partially cyclodehydro-
genated product with a peak maximum at 4800 Da. Employing
1.5 equiv afforded a product with the main peak at 4760 Da,
much closer to the desired mass of 4749 Da for the target
molecule 12c (Figure 9). Even better results were obtained with
(18) Shifrina, Z. B.; Averina, M. S.; Rusanov, A. L.; Wagner, M.; Mu¨llen, K.
Macromolecules 2000, 33, 3525-3529.
(19) Negri, F.; Castiglioni, C.; Tommasini, M.; Zerbi, G. J. Phys. Chem. A 2002,
106, 3306-3317.
(20) Using the molecular mechanics force field of Wavefunction Spartan Pro
1.0.5.
9
3144 J. AM. CHEM. SOC. VOL. 126, NO. 10, 2004