C O M M U N I C A T I O N S
The observed long-range ordered self-assembly of DPP materials
is driven by excluded volume interactions between rigid DPP
cylinders.10 In dry DPP films, where a ) D, SAXD scans show
the expected increase of cylinder diameters D with increasing size
of the dendron side chains (Figure 2c). Remarkably, the measured
D values agree very well with dimensional estimates that are based
on simple geometrical computer models of helical peptide back-
bones surrounded by dendritic side chains (12.9 and 29 Å for
glun-D0 and -D2, respectively). Comparison of SAXD scans of the
three glun-D1 molecules dissolved in m-cresol at the same concen-
tration (Figure 2d), shows that the periodicity of DPP stacks
increases with L. Knowing the amount of solvent in each sample,
we estimate that the thicknesses of DPP layers are 8.7, 11.4, and
14.1 nm, identical to the expected lengths L of the respective DPP
molecules.
In conclusion, we have developed a combined biosynthetic route
toward a new class of cylindrical dendrimers with predictable size,
shape, and solubility. Our DPP materials self-assemble into highly
ordered LC phases with ordering length-scales (a, d) controlled by
the dimensions of the DPP molecules. The modular nature of our
biosynthetic strategy can be used to expand the range of accessible
DPP interactions and shapes through the variation of peptide
sequences, dendron functionality, and dendron architectures. These
studies, as well as complete investigations of the unique liquid
crystalline phases formed in DPP solutions, are currently in
progress.
Figure 2. (a) SAXD pattern of glu76-D1 DPP dissolved in m-cresol (40 wt
% solvent) showing lamellar (along the z-axis) and hexagonal (along the
xy-plane) reflections. (b) Schematic illustration of the self-assembled
structure of DPP solutions. (c) SAXD data of dry films prepared from DPPs
with glu76 cores and varying dendron shells showing hexagonal packing
peaks. (d) SAXD data of glun-D1 samples at constant 40 wt % m-cresol
concentrations showing lamellar stacking peaks.
Acknowledgment. This work was supported by the NSF (Grants
DMR-0134874, -0094347, and -0076097) and the ACS-PRF (Grant
37669-G7). X-ray diffraction experiments were carried out at the
DND-CAT beam line of the Advance Photon Source (ANL),
supported by the DOE Contract No. W-31-102-Eng-38.
the integrated signal intensities of the backbone and side-chain
protons reveals essentially quantitative dendron-conjugation for all
synthesized DPPs, regardless of the size of the dendritic wedges
and despite the high density (1.5 Å/residue) of reactive glutamic
acid side chains. MALDI-TOF analyses also confirmed >95%
derivatization of the carboxylic acid groups. Importantly, the success
of our synthetic approach does not depend on 100% efficiency in
the grafting reaction: the L and D of the DPPs are fixed even if a
few of the glutamic acid side chains remain unreacted, as long as
the peptide is mostly covered by the dendrons.
The monodispersity and the R-helical conformation of the glun
peptide backbones establish the three discrete lengths L ) n × 1.5
Å ) 8.7, 11.4, and 14.1 nm for the synthesized DPPs, with four
diameters corresponding to the different types of dendron side
chains.9 The self-assembly of the DPPs was investigated in m-cresol.
Concentrated DPP/m-cresol solutions exhibit optical anisotropy
(birefringence) that increases with the DPP concentrations, indicat-
ing formation of ordered LC structures. Small-angle X-ray diffrac-
tion (SAXD) patterns of DPP/m-cresol solutions, sealed between
mica windows and oriented by gentle shearing, show two orthogonal
sets of sharp diffraction peaks (Figure 2a). Reflections with ratios
of 1:x3:x4 along the xy-plane indicate hexagonal packing of DPP
cylinders with well-defined spacing a between the cylinder axis.
Along the z-axis, reflections with ratios 1:2:3:4 reveal a layered
structure with periodicity d . a. The diffraction pattern is consistent
with the structure shown in Figure 2b: cylindrical DPPs form
periodically stacked layers with thickness equal to L, and hexagonal
packing of molecules within each layer; solvent occupies the space
between the molecules in each layer (a > D) and between the layers
(d > L).
Supporting Information Available: Experimental details (PDF).
This material is available free of charge via the Internet at http://
pubs.acs.org.
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