Abstract

The helical self-assembly of cholesteric liquid crystals is a powerful motif in nature, enabling exceptional performance in many biological composites. Attempts to mimic these remarkable materials by drying cholesteric colloidal nanorod suspensions often yield films with a non-uniform mosaic-like character, severely degrading optical and mechanical properties. Here we show—using the example of cellulose nanocrystals—that these problems are due to rod length dispersity: uncontrolled phase separation results from a divergence in viscosity for short rods, and variations in pitch can be traced back to a twisting power that scales with rod length. We present a generic, robust and scalable method for fractionating nanorod suspensions, allowing us to interrogate key aspects of cholesteric self-assembly that were previously hidden by colloid dispersity. By controlled drying of fractionated suspensions, we can obtain mosaic-free films that are uniform in colour. Our findings unify conflicting observations and open routes to biomimetic artificial materials with performance that can compete with that of nature’s originals.

Highlights

  • The helical self-assembly of cholesteric liquid crystals is a powerful motif in nature, enabling exceptional performance in many biological composites

  • In a colloidal cholesteric liquid crystal phase[1], the nanorods align in a direction n that is helically modulated along an axis m⊥n

  • With access to these fractions, we can identify a helical twisting power (HTP), inspired by the corresponding concept in thermotropic cholesterics but with somewhat different interpretation in this case of a colloidal cholesteric. We find that this key parameter, determining the equilibrium helix pitch p0 at a certain cellulose nanocrystals (CNCs) concentration, increases with rod length

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Summary

Introduction

The helical self-assembly of cholesteric liquid crystals is a powerful motif in nature, enabling exceptional performance in many biological composites. Biphasic suspensions (w0 < W < w1) of fractions with long CNCs show rapid phase separation along gravity, reaching their final equilibrium state in about a day

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