Influence of a liquid crystalline block on the microdomain structure of block copolymers

Abstract

AbstractWe report on the phase behavior and microdomain structure of two types of diblock copolymers containing a liquid crystal (LC) block joined to a flexible coil block. Consideration of the symmetry groups of the liquid crystalline phases and of the block copolymer microdomain structures provides a rationale for predicting the possible types of liquid crystalline block copolymer morphologies. Both previously reported and newly discovered structural types are identified. Possible organizational schemes are developed for the mesogens and periodic disclination defects with respect to the intermaterial dividing surfaces separating the liquid crystalline and flexible coil domains. The first type of copolymer investigated has a rod‐like LC block whereas the second type copolymer has a side chain LC block. Five different rod‐coil diblocks based on poly(hexyl isocyanate‐b‐styrene) P(HIC‐b‐S) were synthesized by anionic polymerization. Wavy lamellae, zig‐zag and arrowhead microdomain morphologies corresponding to smectic‐C and smectic‐O structures were observed depending on the composition. These layered phases have the director (PHIC chain axis) tilted at various orientations with respect to the layer normal. Side‐chain LC diblocks based on functionalized poly(isoprene‐b‐styrene) P(I‐b‐S) were also investigated. These polymers were synthesized using polymer analogous chemistry from P(I‐b‐S) precursors. Three different mesogenic groups were attached to the PI blocks: one based on biphenyl benzoate and two based on azobenzene. The microdomain structures found for the functionalized poly(isoprene side‐chain LC‐b‐styrene) P(ILC‐b‐S) diblocks are typical of traditional coil‐coil diblocks (lamellae and cylinders). However, these morphologies possess an additional smectic layering of the mesogens within the microdomains of the LC block. In the case of the rod‐coil diblocks, the transformation from an initially isotropic state to the final microphase separated solid state occurs via nematic and then smectic liquid crystalline states, whereas for the side‐chain LC‐coil cases, the microphase separation transition occurs prior to development of orientational order. The long‐range microdomain order of LC block‐coil block copolymers can extend over very large distances due to the influence of the orientational ordering of the LC block.