Abstract

We construct an unfolded system for off-shell fields of arbitrary integer spin in 4d anti-de Sitter space. To this end we couple an on-shell system, encoding Fronsdal equations, to external Fronsdal currents for which we find an unfolded formulation. We present a reduction of the Fronsdal current system which brings it to the unfolded Fierz-Pauli system describing massive fields of arbitrary integer spin. Reformulating off-shell higher-spin system as the set of Schwinger–Dyson equations we compute propagators of higher-spin fields in the de Donder gauge directly from the unfolded equations. We discover operators that significantly simplify this computation, allowing a straightforward extraction of wave equations from an unfolded system.

Highlights

  • One of the central difficulties of HS gravity is that its full nonlinear action is unknown

  • We present a reduction of the Fronsdal current system which brings it to the unfolded FierzPauli system describing massive fields of arbitrary integer spin

  • As we show in subsection 5.1.1, the unfolded system for conserved J admits a reduction to an unfolded system that describes on-shell massive HS fields subjected to Fierz-Pauli conditions

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Summary

Essentials of the unfolded dynamics approach

Unfolded system (2.12) describes a massless scalar field φ(x) in AdS4.1 One sees from (2.15) that CN (Y |x) with N > 0 are descendant fields that form a tower of totally symmetrized traceless derivatives of the primary scalar φ(x). If J is an a priori unknown function, with (2.18) being the only relation involving it, one can treat (2.18) as the definition of J In this case the theory in question can be considered as lying off-shell: it describes two scalar fields, φ(x) and J(x), with primary φ totally unconstrained and descendant J defined by (2.18). Unfolding this system is equivalent to unfolding off-shell scalar φ. That determine the partition function Z and, the whole quantum theory

Unfolded on-shell HS fields and Fronsdal equations
Off-shell completion of the scalar field
On-shell reduction: a scalar field of arbitrary mass
Quantization: a scalar field propagator
Unfolded system for Fronsdal current
Conserved traceless HS current
On-shell reduction
Trace of the Fronsdal current
Double-traceless Fronsdal current
Off-shell HS fields unfolded
Coupling of HS currents to the Fronsdal system
Quantization: massless HS propagators in the de Donder gauge
Conclusion
A Notations and conventions
B Non-diagonal spin-s off-shell extension
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