On the Algebraic Structure of Higher-Spin Field Equations and New Exact Solutions

TL;DR

This thesis explores the algebraic structure of higher-spin field equations, reviews Vasiliev's approach, and introduces new exact solutions in four-dimensional space-times with various signatures, advancing understanding of higher-spin gauge theories.

Contribution

It presents original results including new exact solutions of Vasiliev's equations in 4D and a novel representation theory of the higher-spin algebra, extending previous formulations.

Findings

Found new exact solutions with various symmetries and parameters

Developed a harmonic expansion mapping operators to isometry algebra representations

Proposed a regularization scheme for higher-derivative interactions

Abstract

This Thesis reviews Vasiliev's approach to Higher-Spin Gauge Theory and contains some original results concerning new exact solutions of the Vasiliev equations and the representation theory of the higher-spin algebra. The review part covers the various formulations of the free theory as well as Vasiliev's full nonlinear equations, in particular focusing on their algebraic structure and on their properties in various space-time signatures. Then, the original results are presented. First, the 4D Vasiliev equations are formulated in space-times with signatures (4-p,p) and non-vanishing cosmological constant, and some new exact solutions are found, depending on continuous and discrete parameters: (a) an SO(4-p,p)-invariant family of solutions; (b) non-maximally symmetric solutions with vanishing Weyl tensors and higher-spin gauge fields, that differ from the maximally symmetric background solutions in the auxiliary field sector; and (c) solutions of the chiral models with an infinite tower of Weyl tensors proportional to totally symmetric products of two principal spinors. These are apparently the first exact 4D solutions with non-vanishing massless higher-spin fields. Finally, a generalized harmonic expansion of the Vasiliev's master zero-form is performed as a map from the associative algebra A of operators on the singleton phase space to representations of the background isometry algebra that include one-particle states along with linearized runaway solutions. Such Harish-Chandra modules are unitarizable in a Tr_A-norm rather than in the standard Killing norm. We also take the first steps towards a regularization scheme for handling strongly coupled higher-derivative interactions within this operator formalism.