Abstract

The self-assembly of a high-χ silicon-containing side-chain liquid crystalline block copolymer (LC BCP) in bulk and in thin films is reported, and the structural transition process from the hexagonally packed cylinder (HEX) to the body-centered cubic structure (BCC) in thin films was examined by both reciprocal and real space experimental methods. The block copolymer, poly(dimethylsiloxane-b-11-(4'-cyanobiphenyl-4-yloxy)undecylmethacrylate) (PDMS-b-P(4CNB11C)MA) with a molecular weight of 19.5 kg mol-1 and a volume fraction of PDMS 27% self-assembled in bulk into a hierarchical nanostructure of sub-20 nm HEX cylinders of PDMS with the P(4CNB11C)MA block exhibiting a smectic LC phase with a 1.61 nm period. The structure remained HEX as the P(4CNB11C)MA block transformed to an isotropic phase at ∼120 °C. In the thin films, the PDMS cylindrical microdomains were oriented in layers parallel to the substrate surface. The LC block formed a smectic LC phase which transformed to an isotropic phase at ∼120 °C, and the microphase-separated nanostructure transformed from HEX to BCC spheres at ∼160 °C. The hierarchical structure as well as the dynamic structural transition of the thin films were characterized using in situ grazing-incidence small-angle X-ray scattering and grazing-incidence wide-angle X-ray scattering. The transient morphologies from the HEX to BCC structure in thin films were captured by scanning electron microscopy and atomic force microscopy, and the transition pathway was described.

Highlights

  • The self-assembly of block copolymers (BCPs) has been intensively investigated because of their ability to provide a variety of well-defined nanostructures with length scales of a few nm to over 100 nm, with applications in many nanotechnologies.[1,2,3,4,5,6,7,8] The introduction of a liquid crystallineFor applications such as nanolithography where small feature sizes are required, high interaction parameter (χ) block copolymers are preferred.[23]

  • The microphase separation of the PDMS-b-P(4CNB11C)MA block copolymer in bulk was investigated by small-angle X-ray scattering (SAXS) and transmission electron microscopy (TEM) experiments

  • TEM was used to confirm the morphology of the bulk sample

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Summary

Introduction

The self-assembly of block copolymers (BCPs) has been intensively investigated because of their ability to provide a variety of well-defined nanostructures with length scales of a few nm to over 100 nm, with applications in many nanotechnologies.[1,2,3,4,5,6,7,8] The introduction of a liquid crystallineFor applications such as nanolithography where small feature sizes are required, high interaction parameter (χ) block copolymers are preferred.[23]. Self-assembly of a silicon-containing side-chain liquid crystalline block copolymer in bulk and in thin films: kinetic pathway of a cylinder to sphere transition†

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