Abstract

We aim at formulating a higher-spin gravity theory around AdS2 relevant for holography. As a first step, we investigate its kinematics by identifying the low-dimensional cousins of the standard higher-dimensional structures in higher-spin gravity such as the singleton, the higher-spin symmetry algebra, the higher-rank gauge and matter fields, etc. In particular, the higher-spin algebra is given here by [λ] and parameterized by a real parameter λ. The singleton is defined to be a Verma module of the AdS2 isometry subalgebra so (2, 1) ⊂ [λ] with conformal weight Delta =frac{1pm lambda }{2}. On the one hand, the spectrum of local modes is determined by the Flato-Fronsdal theorem for the tensor product of two such singletons. It is given by an infinite tower of massive scalar fields in AdS2 with ascending masses expressed in terms of λ. On the other hand, the higher-spin fields arising through the gauging of [λ] algebra do not propagate local degrees of freedom. Our analysis of the spectrum suggests that AdS2 higher-spin gravity is a theory of an infinite collection of massive scalars with fine-tuned masses, interacting with infinitely many topological gauge fields. Finally, we discuss the holographic CFT1 duals of the kinematical structures identified in the bulk.

Highlights

  • Introduction and summaryThe recent surge of interest in AdS2/CFT1 correspondence prompted by the Sachdev-YeKitaev (SYK) model [1–4] motivates a thorough investigation of lowest-dimensional higher-spin (HS) holographic duality

  • We investigate its kinematics by identifying the low-dimensional cousins of the standard higher-dimensional structures in higher-spin gravity such as the singleton, the higher-spin symmetry algebra, the higher-rank gauge and matter fields, etc

  • It is given by an infinite tower of massive scalar fields in AdS2 with ascending masses expressed in terms of λ

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Summary

Introduction and summary

The recent surge of interest in AdS2/CFT1 correspondence prompted by the Sachdev-YeKitaev (SYK) model [1–4] (see e.g. [5, 6] for reviews) motivates a thorough investigation of lowest-dimensional higher-spin (HS) holographic duality. Forms a higher-spin multiplet corresponding to the twisted-adjoint module (where RAdS stands for the curvature radius of the AdS2 spacetime) Applying the standard AdS2/CFT1 dictionary on (1.1), the boundary dual of this tower of scalar fields should be a collection of primary operators On with conformal weight ∆n = n−λ+1. The main result reviewed here is the Flato-Fronsdal type theorem which describes the tensor product of two singletons as an infinite collection of Verma modules with running conformal weights. These results allow to describe the higher-spin algebra as an infinite collection of Verma modules with running conformal dimensions and thereby identify the right-hand-side of the Flato-Fronsdal theorem as the twisted-adjoint representation. Appendix E builds the most general class of so(2, 1) actions on U so(2, 1) realized by inhomogeneous first-order differential operators in auxiliary variables

Singletons: fundamental representation
Spectra of bulk fields/boundary operators: bi-fundamental representation
Definition
Extra factorization
Oscillator realization
Universal enveloping algebra in Howe dual variables
Higher-spin quotient algebra
Module structure of the universal enveloping algebra
Adjoint action
Abstract definition of the twisted-adjoint action
Twist automorphism and compensator vector
Twisted-adjoint action on the universal enveloping algebra module
Towards the twisted-adjoint action on the higher-spin algebra
Verma modules as twisted-like representations
Twisted-like representations
Special values and factorization
AdS2 massive scalars and twisted-adjoint equations
Covariant derivatives
Gauge field equations
Massive scalar field equations
Comments on candidate interactions
B Basic star-product expressions
C Canonical basis
D Twisted basis
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