Liquid crystals and harmonic maps in polyhedral domains

TL;DR

This paper studies nematic liquid crystal configurations in polyhedral domains, deriving energy bounds and exploring the existence and topology of minimizers, with implications for bistable display devices.

Contribution

It introduces new lower bounds for Dirichlet energy based on homotopy invariants and investigates the existence of smooth minimizers in polyhedral domains.

Findings

Lower bounds for energy depend on minimal connections between defects.

Upper bounds are obtained from conformal solutions, with ratios bounded independently.

Numerical results indicate some homotopy classes always have smooth minimizers.

Abstract

Unit-vector fields $\nvec$ on a convex polyhedron $P$ subject to tangent boundary conditions provide a simple model of nematic liquid crystals in prototype bistable displays. The equilibrium and metastable configurations correspond to minimisers and local minimisers of the Dirichlet energy, and may be regarded as $S^2$-valued harmonic maps on $P$. We consider unit-vector fields which are continuous away from the vertices of $P$. A lower bound for the infimum Dirichlet energy for a given homotopy class is obtained as a sum of minimal connections between fractional defects at the vertices of $P$. In certain cases, this lower bound can be improved by incorporating certain nonabelian homotopy invariants. For a rectangular prism, upper bounds for the infimum Dirichlet energy are obtained from locally conformal solutions of the Euler-Lagrange equations, with the ratio of the upper and lower bounds bounded independently of homotopy type. However, since the homotopy classes are not weakly closed, the infimum may not be realised; the existence and regularity properties of continuous local minimisers of given homotopy type are open questions. Numerical results suggest that some homotopy classes always contain smooth minimisers, while others may or may not depending on the geometry of $P$. Numerical results modelling a bistable device suggest that the observed nematic configurations may be distinguished topologically.