Abstract

Nematic liquid crystals are anisotropic fluids that self-assemble into vector fields, which are governed by geometrical and topological laws. Consequently, particulate or droplet inclusions self-assemble in nematic domains through a balance of topological defects. Here, we use double emulsions of water droplets inside radial nematic liquid crystal droplets to form various structures, ranging from linear chains to three-dimensional fractal structures. The system is modeled as a formation of satellite droplets, distributed around a larger, central core droplet and we extend the problem to explain the formation of fractal structures. We show that a distribution of droplet sizes plays a key role in determining the symmetry properties of the resulting geometric structures. The results are relevant to a variety of inclusions, ranging from colloids suspensions to multi-emulsion systems. Such systems have potential applications for novel switchable photonic structures as well as providing wider insights into the packing of self-assembled structures.

Highlights

  • Nematic liquid crystals are anisotropic fluids that self-assemble into vector fields, which are governed by geometrical and topological laws

  • We find that the size differences between the water droplets play a key role in the spontaneous formation of complex three-dimensional (3D) structures, ranging from linear chains to fractal structures

  • Adding a smaller inclusion with normal boundary conditions does not create any additional distortion to the radial director field

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Summary

Introduction

Nematic liquid crystals are anisotropic fluids that self-assemble into vector fields, which are governed by geometrical and topological laws. A spherical nematic droplet with radial boundary conditions must contain a radial-like singularity[9,12], known as a topological defect[13] (cf sink/source in fluid mechanics). This singularity can be replaced by any set of topologically equivalent structures, such as a defect loop or a combination of different defects[2,10,11,12]. A forced defect in a nematic director field will result in the creation of an accompanying defect of opposite topological charge[10,11,12]

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