A microphase-separated poly(styrene-b-(lauryl-co-stearyl acrylate)-bstyrene) (SAS) triblock copolymer exhibiting a disordered spherical microstructure with randomly oriented grains was aligned through the application of large-amplitude oscillatory shear (LAOS) at a temperature below the order−disorder transition temperature of the triblock copolymer, yet above the glass transition temperature of the polystyrene spherical domains. The thermoplastic elastomeric behavior of the SAS triblock copolymer provided a convenient means to observe the aligned morphology. Following application of LAOS, the specimen was quenched to room temperature (below the glass transition temperature of polystyrene), and small-angle X-ray scattering data were obtained in the three principal shear directions: shear gradient, velocity, and vorticity directions. The analysis revealed that the SAS triblock copolymer formed coexisting face-centered cubic and hexagonally close-packed spherical microstructures. The presence of a close-packed microstructure is in stark contrast to an extensive body of literature on sphere-forming bulk block copolymers that favor body-centered cubic systems under quiescent conditions and under shear. The aligned microstructure observed in this bulk block copolymer was reminiscent of that observed in various spherical soft material systems such as colloidal spheres, sphere-forming block copolymer solutions, and star polymer solutions. The highly unanticipated observation of close-packed spherical microstructures in a neat block copolymer under shear is hypothesized to originate from the dispersity of the block copolymer.
■ INTRODUCTIONBlock copolymers composed of two incompatible polymers spontaneously self-assemble into various equilibrium nanoscale phases, including lamellae, hexagonally close-packed cylinders, body-centered cubic spheres, and a bicontinuous gyroid morphology. 1,2 These materials have many potential applications, such as thermoplastic elastomers, membranes for batteries, fuel cells and water purification, and solution-based assemblies for encapsulation of hydrophobic guest molecules and drug delivery. 1,2 Block copolymer morphologies formed spontaneously in the melt are randomly oriented, lacking longrange order, and the materials are macroscopically isotropic. The application of external forces, such as shear, 3 electric fields, 4,5 magnetic fields, 6 or preferential surfaces, 7 can lead to alignment of the block copolymer into anisotropic structures and induce long-range ordering. Control of structural orientation is key to manipulating the properties of these materials for desired applications.The application of shear, whether steady shear or largeamplitude oscillatory shear (LAOS), is a common approach for the alignment of bulk block copolymers. Extensive studies have focused on alignment of lamellae-forming systems through steady shear or LAOS. 3,8−16 Three possible alignment orientations have been identified as parallel, perpendicular, and transverse with respect to the shear flow direction....