The discovery of electrically
conducting organic crystals and polymers has widened the range of
potential optoelectronic materials, provided they exhibit sufficiently
high charge carrier mobilities and are easy to make and process. Organic
single crystals have high charge carrier mobilities but are usually
impractical because they are difficult to process, whereas polymers
have good processability but low mobilities. Liquid crystals exhibit
mobilities approaching those of single crystals and are suitable for
applications, but demanding fabrication and processing methods limit
their use. We have shown that the self-assembly of fluorinated tapered
dendrons can drive the formation of supramolecular liquid crystals
with promising optoelectronic properties from a wide range of organic
donor and acceptor moieties (e.g., Figure 1).
Figure 1. a.) Molecular structure
of electron acceptor (A), whose electron mobility in the columnar
rectangular phase is (2.3 ±0.4) x10-3 cm2V-1s-1. The mobility
is approximately three times higher in the lower temperature (25°C)
glassy phase.
b.) Molecular structure of an electron donor (D), whose hole mobility
in the columnar hexagonal phase is (1.5 ±0.3) x10-3.
Attaching conducting organic donor
or acceptor groups to the apex of the dendrons leads to supramolecular
nanometer scale columns (Figure 2) that contain in their cores p-stacks
of donors, acceptors, or donor-acceptor complexes exhibiting tight
packing and high charge carrier mobilities, demonstrating the viability
of synthetic supramolecular chemistry for electronic materials. When
we use functionalized dendrons and amorphous polymers carrying compatible
side groups, they coassemble so that the polymer is incorporated in
the centre of the columns through donor-acceptor interactions and
exhibits enhanced charge carrier mobilities. We anticipate that this
simple and versatile strategy for producing conductive p-stacks of
aromatic groups, surrounded by helical dendrons, will lead to a new
class of supramolecular materials suitable for electronic and optoelectronic
applications. Interfacial interactions and solidification conditions
are critical for obtaining the desired alignment of columns, for effective
charge transport (Figure 3).
Figure 2. The glassy-phase molecular
arrangement in the supramolecular column self-assembled from
molecule A.
Figure 3. Films of molecule D on hydrophobic
indium-tin oxide, cooled a.) rapidly 20°C/min and b.)
slowly 0.1°C/min, and viewed between crossed polarizers.
The dark appearance in (b) indicates that the supramolecular
columns are nearly perpendicular to the film surface.
Figures from Percec et al., Nature
419,384 (2002).