We have comprehensively studied the effect of nanoparticle selectivity on the self-assembly of symmetrical block copolymer (BCP) under cylindrical confinement using simulation and experiment. For the simulation, a coarse-grained molecular dynamics (CGMD) simulation has been utilized, and we investigated the confined assembly using nanoparticles with three different interactions with block copolymer: (i) neutral to both A (wall-attractive) and B (wall-repulsive) phases, (ii) B domain selective, and (iii) A domain selective. It is predicted that nonselective (neutral) nanoparticles (NPs) tend to be placed near the interface between radially alternating layers of A or B domains, while selective (A or B) NPs swell the corresponding phase, inducing discrete asymmetrical morphologies. We also find that pure asymmetrical BCP forms more radially perforated morphologies, while symmetrical BCP/NP forms more discrete morphologies. Experimentally, we have incorporated gold or magnetite NPs with the matching three types of selectivity toward symmetrical diblock PS-b-PI and electrospun them. The morphologies observed from our study have been quantified by morphological classification numbers to identify the degree of asymmetry formed. The qualitative and quantitative comparisons between experiment and simulation confirm the validity of the simulation tool and shed light on the NP's role on breaking the symmetry of BCP under cylindrical confinement.
■ INTRODUCTIONNanoparticles (NPs) have attracted much research interest for a wide variety of potential applications in biomedical, optical, and electronic fields. 1−4 In particular, nanoparticles are successfully incorporated into a polymer matrix to enhance material properties. 5−7 Due to their high surface energy, however, nanoparticles often self-aggregate in the polymer matrix, which prevents utilization of their large interfacial volume. Synergetic effects can arise from periodic spatial placement of the nanoparticles to fully maximize its utility. As one solution, the block copolymer has been used as a template for ordered placement of nanoparticles. Block copolymer (BCP) solutions and melts are known to self-assemble into a variety of nanoscale morphologies including spheres, rods, micelles, lamellae, vesicle tubules, and cylinders 8,9 depending on the volume fraction and interaction parameter between different blocks. Self-assembly of BCP has attracted increasing interest in recent years for applications in nanotechnology. 10,11 Precise control over the size, shape, and periodicity of these nanoscale microdomains is the key factor in providing opportunities for realization of nanoscale systems. It has been reported that BCP exhibits novel morphologies not seen in the bulk under a confined domain (D) which is commensurate with its equilibrium bulk periodic spacing (L 0 ). Shin et al. confined symmetrical polystyrene-b-polybutadiene (PS-b-PBD) in an alumina nanopore to obtain concentric ring morphology which was not observed in the bulk. 12 There are also other types of confi...