Topologically massive higher spin gauge theories

TL;DR

This paper develops conformal higher-spin gauge theories in three-dimensional curved space, introducing gauge fields, invariants, and actions that describe massive higher-spin fields and their supersymmetric extensions.

Contribution

It introduces a new class of conformal higher-spin gauge fields and constructs gauge-invariant actions for massive higher-spin fields in 3D, including supersymmetric extensions.

Findings

Defined conformal spin-$rac{n}{2}$ gauge fields and their primary descendants.

Constructed Weyl and gauge invariant Chern-Simons-type actions.

Connected higher-derivative equations to unitary massive representations.

Abstract

We elaborate on conformal higher-spin gauge theory in three-dimensional (3D) curved space. For any integer $n>2$ we introduce a conformal spin-$\frac{n}{2}$ gauge field $h_{(n)} =h_{\alpha_1\dots \alpha_n}$ (with $n$ spinor indices) of dimension $(2-n/2)$ and argue that it possesses a Weyl primary descendant $C_{(n)}$ of dimension $(1+n/2)$. The latter proves to be divergenceless and gauge invariant in any conformally flat space. Primary fields $C_{(3)}$ and $C_{(4)}$ coincide with the linearised Cottino and Cotton tensors, respectively. Associated with $C_{(n)}$ is a Chern-Simons-type action that is both Weyl and gauge invariant in any conformally flat space. These actions, which for $n=3$ and $n=4$ coincide with the linearised actions for conformal gravitino and conformal gravity, respectively, are used to construct gauge-invariant models for massive higher-spin fields in Minkowski and anti-de Sitter space. In the former case, the higher-derivative equations of motion are shown to be equivalent to those first-order equations which describe the irreducible unitary massive spin-$\frac{n}{2}$ representations of the 3D Poincar\'e group. Finally, we develop ${\cal N}=1$ supersymmetric extensions of the above results.