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Higher Spin Superalgebras in any Dimension and their Representations

M. A. Vasiliev

TL;DR

The work establishes a universal oscillator-based framework for higher spin algebras in arbitrary dimensions, showing that singleton representations of $o(d-1,2)$ underlie HS gauge theories in $AdS_d$ and that tensor products of these singletons reproduce the full spectrum of bulk massless fields, thereby generalizing the Flato–Fronsdal theorem beyond $d=4$. It constructs explicit HS algebras and their supersymmetric extensions using two-boson and spinor-extended oscillator realizations, together with projection methods to isolate the physical spectrum and ensure admissibility. The analysis introduces unfolded formulations for conformal fields, clarifies the AdS/CFT interpretation, and demonstrates isomorphisms with well-known lower-dimensional HS structures in $AdS_3$, $AdS_4$, and $AdS_5$. Overall, the paper provides a comprehensive group-theoretical basis for consistent HS gauge theories in any dimension, including a supersymmetric extension that acts on boundary conformal scalars and spinors as well as on bulk HS fields.

Abstract

Fock module realization for the unitary singleton representations of the $d-1$ dimensional conformal algebra $o(d-1,2)$, which correspond to the spaces of one-particle states of massless scalar and spinor in $d-1$ dimensions, is given. The pattern of the tensor product of a pair of singletons is analyzed in any dimension. It is shown that for $d>3$ the tensor product of two boson singletons decomposes into a sum of all integer spin totally symmetric massless representations in $AdS_d$, the tensor product of boson and fermion singletons gives a sum of all half-integer spin symmetric massless representations in $AdS_d$, and the tensor product of two fermion singletons in $d>4$ gives rise to massless fields of mixed symmetry types in $AdS_d$ depicted by Young tableaux with one row and one column together with certain totally antisymmetric massive fields. In the special case of $o(2,2)$, tensor products of 2d massless scalar and/or spinor modules contain infinite sets of 2d massless conformal fields of different spins. The obtained results extend the 4d result of Flato and Fronsdal \cite{FF} to any dimension and provide a nontrivial consistency check for the recently proposed higher spin model in $AdS_d$ \cite{d}. We define a class of higher spin superalgebras which act on the supersingleton and higher spin states in any dimension. For the cases of $AdS_3$, $AdS_4$, and $AdS_5$ the isomorphisms with the higher spin superalgebras defined earlier in terms of spinor generating elements are established.

Higher Spin Superalgebras in any Dimension and their Representations

TL;DR

The work establishes a universal oscillator-based framework for higher spin algebras in arbitrary dimensions, showing that singleton representations of underlie HS gauge theories in and that tensor products of these singletons reproduce the full spectrum of bulk massless fields, thereby generalizing the Flato–Fronsdal theorem beyond . It constructs explicit HS algebras and their supersymmetric extensions using two-boson and spinor-extended oscillator realizations, together with projection methods to isolate the physical spectrum and ensure admissibility. The analysis introduces unfolded formulations for conformal fields, clarifies the AdS/CFT interpretation, and demonstrates isomorphisms with well-known lower-dimensional HS structures in , , and . Overall, the paper provides a comprehensive group-theoretical basis for consistent HS gauge theories in any dimension, including a supersymmetric extension that acts on boundary conformal scalars and spinors as well as on bulk HS fields.

Abstract

Fock module realization for the unitary singleton representations of the dimensional conformal algebra , which correspond to the spaces of one-particle states of massless scalar and spinor in dimensions, is given. The pattern of the tensor product of a pair of singletons is analyzed in any dimension. It is shown that for the tensor product of two boson singletons decomposes into a sum of all integer spin totally symmetric massless representations in , the tensor product of boson and fermion singletons gives a sum of all half-integer spin symmetric massless representations in , and the tensor product of two fermion singletons in gives rise to massless fields of mixed symmetry types in depicted by Young tableaux with one row and one column together with certain totally antisymmetric massive fields. In the special case of , tensor products of 2d massless scalar and/or spinor modules contain infinite sets of 2d massless conformal fields of different spins. The obtained results extend the 4d result of Flato and Fronsdal \cite{FF} to any dimension and provide a nontrivial consistency check for the recently proposed higher spin model in \cite{d}. We define a class of higher spin superalgebras which act on the supersingleton and higher spin states in any dimension. For the cases of , , and the isomorphisms with the higher spin superalgebras defined earlier in terms of spinor generating elements are established.

Paper Structure

This paper contains 12 sections, 246 equations.