F. Würthner et al.
the absorption spectrum with a Stokes shift of only 11 nm.
The fwhm values of absorption and emission spectra are sig-
nificantly reduced to 850 and 786 cmꢀ1, respectively. Tem-
perature-dependent UV/Vis experiments in MCH testify the
reversibility of the self-assembly process. When the temper-
ature is raised from 10 to 908C, the sharp band at 598 nm
gradually disappears and the monomeric species is recov-
ered as evidenced by re-appearance of the broad spectrum
(Figure 2b). These spectral features clearly indicate the re-
versible formation of J-aggregates of PBI1 in apolar solvent
which is in contrast to the H-aggregating PBI2 and other
PBI-based organogelators.[10,11] The very intense J-band of
PBI1 with relatively small bathochromic shift suggests the
presence of tightly aggregated chromophores at a slip angle
close to the magic angle of 54.78 that is unprecedented for
this class of chromophores.[16,17] These unusual spectral and
packing features are encoded in the unique molecular struc-
ture of PBI1: a twisted p-conjugated core and additional
amide groups that can assist intermolecular H-bonds.
TEM (Figure 3a,b) as expected for lyotropic mesophases.[14]
These aggregates appear much more fluid-like as compared
to the entangled fibers observed for gels of PBI2[11b] (Fig-
ure 3e,f). They are able to cause an increase in viscosity of
the medium (Figure 1a) but are unable to gel the solvent.[19]
Interestingly, TEM images from a suspension of PBI1 gel in
acetone revealed distinctly different aggregate morphologies
as shown in Figure 3c and d. The willow-leaf-like aggregated
units appear to be more flexible and they can gradually en-
tangle to each other at the ends to give star-shaped struc-
tures. Those “stars” further intercross to form the 3D net-
workstructures, which are essential for gelation. Similar
spectroscopic and microscopic features of PBI1 could also
be observed in dioxane (Figures S4 and S6).
Similar optical properties of PBI1 can also be found in
acetone and dioxane, in which organogels were formed.
Temperature-dependent UV/Vis spectra of PBI1 in these
hydrogen-bond breaking solvents (Figure S4) clearly show J-
type aggregating behavior, that is, upon aggregation the ab-
sorption maximum shifts bathochromically. However, in
these solvents aggregation tookplace only at considerably
higher concentrations and lower temperatures (in acetone:
c>1.0 mm, T<308C and in dioxane: c>2.5 mm, T<208C;
see Supporting Information) when compared with that in
apolar solvent such as MCH. The relatively lower propensity
to aggregate formation of PBI1 in acetone and dioxane is
conceivable since the solvent molecules in these cases are
capable of interacting with the amide functionality of the
dye molecules through hydrogen bonding,[18] and thus can
weaken the inter-chromophoric interactions. However, at
significantly higher concentration and lower temperature,
dye aggregation was evidenced from distinct spectral
changes (bathochromic shift of ca. 39 nm in acetone) that
are indicative of a packing motif with more displaced dye
molecules according to exciton coupling theory[17] (see calcu-
lations in the Supporting Information). Further evidence of
solvent participation in hydrogen bonding with the amide
functionality of PBI1 was gathered from 1H NMR studies
(Figure S5). The amide protons of PBI1 were found to be
significantly downfield shifted in acetone compared to that
in chloroform or benzene as expected for hydrogen-bonding
interactions with the solvent molecules.
Figure 3. TEM images of PBI1 in MCH (1.010ꢀ4 m, a and b) and a sus-
pension of a gel in acetone (ca. 1.010ꢀ3 m, c and d); e) and f) show the
long aggregated fibers of PBI2 from a suspension of a gel in dioxane (ca.
1.010ꢀ3 m). The scale bar in a)–d) corresponds to 500 nm and in e) and
f) corresponds to 1000 nm.
Whilst the solution spectroscopic studies revealed the ag-
gregate formation in various solvents, transmission electron
microscopy (TEM) studies provided direct evidences for the
formation of extended networks. Figure 3 shows typical
TEM images of aggregated structures of PBI1 and PBI2 in
different solvents. As reported previously, PBI2 can form
long well-defined fibers and further entangle to network
structures in many apolar solvents.[11b] In contrast, for PBI1
less regular structures are observed. In MCH loosely con-
nected bundles of aggregate structures are visualized by
In contrast to the morphology of core-twisted PBI1, the
core-planar PBI2 gives very long (several microns) 1D fiber
in dioxane. This observation strongly indicates that the dif-
ferences in gelation behavior of these dyes are originated
from the structural change of the perylene cores. Possibly,
strong p–p interaction among planar PBI2 chromophores
8076
ꢀ 2008 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Eur. J. 2008, 14, 8074 – 8078