Abstract

In this paper, we show that via a novel construction every rank-3 root system induces a root system of rank 4. Via the Cartan-Dieudonné theorem, an even number of successive Coxeter reflections yields rotations that in a Clifford algebra framework are described by spinors. In three dimensions these spinors themselves have a natural four-dimensional Euclidean structure, and discrete spinor groups can therefore be interpreted as 4D polytopes. In fact, we show that these polytopes have to be root systems, thereby inducing Coxeter groups of rank 4, and that their automorphism groups include two factors of the respective discrete spinor groups trivially acting on the left and on the right by spinor multiplication. Special cases of this general theorem include the exceptional 4D groups D4, F4 and H4, which therefore opens up a new understanding of applications of these structures in terms of spinorial geometry. In particular, 4D groups are ubiquitous in high energy physics. For the corresponding case in two dimensions, the groups I2(n) are shown to be self-dual, whilst via a similar construction in terms of octonions each rank-3 root system induces a root system in dimension 8; this root system is in fact the direct sum of two copies of the corresponding induced 4D root system.

Highlights

  • Root systems are useful mathematical abstractions, which are polytopes that generate reflection (Coxeter) groups

  • Closure of the root system is ensured by closure of the spinor group. This has very interesting consequences for the automorphism group of these root systems, which contains two factors of the spinor group acting from the left and the right [4]

  • One finds that the 4D root systems induced in this way contain mostly the exceptional root systems that generate the exceptional Coxeter groups D4, F4 and H4

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Summary

Introduction

Root systems are useful mathematical abstractions, which are polytopes that generate reflection (Coxeter) groups. The rotations (i.e. the special orthogonal group) are doubly covered by geometric products of an even number of unit vectors, resulting in spinors, or ‘rotors’. In Geometric Algebra, a vector ‘a’ transforms under a rotation in the plane defined by n ∧ m via successive reflection in hyperplanes determined by the unit vectors ‘n’ and ‘m’ as a′′ = mnanm =: RaR, (4)

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