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Conformal Higher Spin Symmetries of 4d Massless Supermultiplets and $osp(L,2M)$ Invariant Equations in Generalized (Super)Space

M. A. Vasiliev

TL;DR

The paper develops an unfolded, covariant description of free 4d massless supermultiplets with conformal higher spin symmetry, realized on Fock-modules dual to unitary doubletons of $su(2,2)$ and extended to $osp(L,2M)$-invariant generalized spaces. A Bogolyubov-type duality links nonunitary field-theory modules to unitary singleton representations, providing a unitarity-consistent quantization route for the $sp(2M)$-covariant dynamics and clarifying the spectrum across all spins. The framework yields explicit global higher spin transformations, worldline interpretations, and a proposed chain of AdS/CFT dualities across generalized symplectic spaces, suggesting a form of space-time dimension democracy. These results position $hu(m,n|8)$-type algebras and their self-conjugated reductions as the natural conformal higher spin symmetries for 4d massless multiplets and open avenues toward nonlinear higher spin dynamics and holography in generalized space-times.

Abstract

Realization of the conformal higher spin symmetry on the 4d massless field supermultiplets is given. The self-conjugated supermultiplets, including the linearized ${\cal N}=4$ SYM theory, are considered in some detail. Duality between non-unitary field-theoretical representations and the unitary doubleton--type representations of the 4d conformal algebra $su(2,2)$ is formulated in terms of a Bogolyubov transform. The set of 4d massless fields of all spins is shown to form a representation of $sp(8)$. The obtained results are extended to the generalized superspace invariant under $osp(L, 2M)$ supersymmetries. World line particle interpretation of the free higher spin theories in the $osp(2\N, 2M)$ invariant (super)space is given. Compatible with unitarity free equations of motion in the $osp(L,2M)$ invariant (super)space are formulated. A conjecture on the chain of $AdS_{d+1}/CFT_d \to AdS_{d}/CFT_{d-1} \to ...$ dualities in the higher spin gauge theories is proposed.

Conformal Higher Spin Symmetries of 4d Massless Supermultiplets and $osp(L,2M)$ Invariant Equations in Generalized (Super)Space

TL;DR

The paper develops an unfolded, covariant description of free 4d massless supermultiplets with conformal higher spin symmetry, realized on Fock-modules dual to unitary doubletons of and extended to -invariant generalized spaces. A Bogolyubov-type duality links nonunitary field-theory modules to unitary singleton representations, providing a unitarity-consistent quantization route for the -covariant dynamics and clarifying the spectrum across all spins. The framework yields explicit global higher spin transformations, worldline interpretations, and a proposed chain of AdS/CFT dualities across generalized symplectic spaces, suggesting a form of space-time dimension democracy. These results position -type algebras and their self-conjugated reductions as the natural conformal higher spin symmetries for 4d massless multiplets and open avenues toward nonlinear higher spin dynamics and holography in generalized space-times.

Abstract

Realization of the conformal higher spin symmetry on the 4d massless field supermultiplets is given. The self-conjugated supermultiplets, including the linearized SYM theory, are considered in some detail. Duality between non-unitary field-theoretical representations and the unitary doubleton--type representations of the 4d conformal algebra is formulated in terms of a Bogolyubov transform. The set of 4d massless fields of all spins is shown to form a representation of . The obtained results are extended to the generalized superspace invariant under supersymmetries. World line particle interpretation of the free higher spin theories in the invariant (super)space is given. Compatible with unitarity free equations of motion in the invariant (super)space are formulated. A conjecture on the chain of dualities in the higher spin gauge theories is proposed.

Paper Structure

This paper contains 18 sections, 299 equations.