Using the living nickel(II)-mediated polymerization of carbodiimides, the chiral (R)-or (S)-N-1-phenethyl-N′-methylcarbodiimide (PMC) monomers were polymerized with a new TIPS protected alkyne functional nickel initiator forming PPMC with an excess single-handed screw sense and the alkyne moiety covalently attached to the terminus of the polymer, as confirmed by 1 H NMR and MALDI-TOF MS. After deprotection, the alkyne end groups of rigid-rod PPMC-2 were coupled with azide-terminated, random-coil PS and PEG homopolymers forming a novel class of helical-b-coil block copolymers. In the thin-film, all synthesized diblock copolymers formed interesting nanofibular morphologies when subject to specific conditions. The triblock RCP-4, however, adopted unique macroporous morphology as identified by AFM and SEM with average pore diameters of ca. 832 ± 194 nm. The origin of this was found to be associated with the ordering of large, hollow vesicle aggregates upon solvent evaporation followed by the melting of these aggregates filling in the hollow interior forming the submicron pores observed. Furthermore, the size of these aggregates can be easily modulated in a linear fashion from 272 to 1648 nm simply by increasing the concentration of RCP-4 in THF. Finally, the three PPMC−PEG copolymers synthesized were found to adopt lyotropic cholesteric mesophases in concentrated toluene solutions (ca. 30 wt %).
■ INTRODUCTIONThe tunable self-assembly and microphase separation of conventional coil−coil block copolymer (CCP) have been studied and modeled extensively. 1,2 The ability to covalently bind polymers of varying composition and structure allows for the combination of polymer properties often with synergistic effects and expanded function. The self-assembly of these macromolecules is governed by a variety of noncovalent forces such as hydrophobic/hydrophilic interactions, electrostatic interactions, hydrogen bonding, and microphase separation. To date, directed block copolymer self-assembly remains as one of the most powerful, versatile methods of tailoring nanometer-size features.The synthesis of rigid rod-b-random coil block copolymers, however, has only recently attracted significant attention due to their unique capabilities to form stable supramolecular structures with a wide array of unique self-assembly behaviors observed in solution and the solid state. 3−6 The anisotropic nature of rigidrod blocks characteristically results in lyotropic/thermotropic liquid crystallinity with nematic or highly ordered smectic mesophases adopted in solution and/or in the melt. 7,8 Therefore, the assembly behaviors of rod−coil block copolymers (RCP) in solution and the solid state vastly differ from those of CCPs arising from a combination of microphase immiscibility of the two blocks and the self-organization behaviors of the rigid-rod block.