Tangent unit-vector fields: nonabelian homotopy invariants and the Dirichlet energy
A. Majumdar, J.M. Robbins, M. Zyskin

TL;DR
This paper computes the minimal Dirichlet energy for tangent unit-vector fields on a spherical octant, revealing how nonabelian topological invariants influence energy bounds, with applications to nematic liquid crystals.
Contribution
It introduces a method to calculate the infimum Dirichlet energy for tangent boundary maps using nonabelian homotopy invariants, extending previous abelian-based results.
Findings
Explicit formulas for energy bounds involving nonabelian invariants
Construction of representatives with conformal or anticonformal properties
Demonstration of energy gap for nonconformal classes
Abstract
Let O be a closed geodesic polygon in S^2. Maps from O into S^2 are said to satisfy tangent boundary conditions if the edges of O are mapped into the geodesics which contain them. Taking O to be an octant of S^2, we compute the infimum Dirichlet energy, Ecal(H), for continuous maps satisfying tangent boundary conditions of arbitrary homotopy type H. The expression for Ecal(H) involves a topological invariant - the spelling length - associated with the (nonabelian) fundamental group of the n-times punctured two-sphere, pi_1(S^2 - {s_1,..., s_n},*). The lower bound for Ecal(H) is obtained from combinatorial group theory arguments, while the upper bound is obtained by constructing explicit representatives which, on all but an arbitrarily small subset of O, are alternatively locally conformal or anticonformal. For conformal and anticonformal classes (classes containing wholly conformal and…
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Taxonomy
TopicsMathematics and Applications · Advanced Differential Equations and Dynamical Systems · Homotopy and Cohomology in Algebraic Topology
