Abstract

It has recently been argued that the symmetric orbifold theory of $$ {\mathbb{T}}^4 $$ is dual to string theory on AdS3 × S3 × $$ {\mathbb{T}}^4 $$ at the tensionless point. At this point in moduli space, the theory possesses a very large symmetry algebra that includes, in particular, a $$ \mathcal{W} $$ ∞ algebra capturing the gauge fields of a dual higher spin theory. Using conformal perturbation theory, we study the behaviour of the symmetry generators of the symmetric orbifold theory under the deformation that corresponds to switching on the string tension. We show that the generators fall nicely into Regge trajectories, with the higher spin fields corresponding to the leading Regge trajectory. We also estimate the form of the Regge trajectories for large spin, and find evidence for the familiar logarithmic behaviour, thereby suggesting that the symmetric orbifold theory is dual to an AdS background with pure RR flux.

Highlights

  • Some progress relating the higher spin/CFT duality to the stringy AdS/CFT correspondence was made for the case of AdS3

  • In the limit where the large N = 4 superconformal algebra contracts to the more familiar small N = 4 algebra, the ‘perturbative part’ of the Wolf space cosets becomes a closed subsector of the symmetric orbifold (T4)⊗(N+1)/SN+1, which in turn is thought to be dual to string theory on AdS3 ×S3 ×T4 at the tensionless point

  • In the previous section we have studied the anomalous dimensions of the higher spin currents of the symmetric orbifold theory as one turns on the perturbation that corresponds to the string tension

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Summary

Introduction

Some progress relating the higher spin/CFT duality to the stringy AdS/CFT correspondence was made for the case of AdS3. In this paper we want to confirm, at least qualitatively, this picture by studying the perturbation of the symmetric orbifold theory that corresponds to switching on the string tension Under this perturbation, we expect that the symmetry algebra is broken down to the N = 4 superconformal algebra. We find evidence that the anomalous dimensions γ(s) behave as log s at large spin s, at least before any mixing effects are taken into account This is in agreement with expectations from the analysis of classical string solutions in AdS5, see [7] and, e.g., [8] for a review, or the explicit results for AdS3, see in particular [9, 10]. We have included an ancillary file in the arXiv submission of this paper which contains the numerical values of the diagonal elements of the mixing matrix for the quadratic and cubic generators, as well as analytic expressions for these diagonal elements

The symmetric orbifold
The quadratic fields
The cubic and higher order fields
The exactly marginal operators
Exactly marginal operators in the twisted sector
The perturbing fields
First order deformation analysis
Deformation by the untwisted sector perturbation fields
Deformation by the twisted sector perturbation fields
Second order deformation analysis
A more structural approach
Relation to bulk masses
The structure of the analysis
Spin 1
Spin 2
Spin 3
Partial diagonalisation for higher spin
Discussion
A Free field realisation of the chiral fields
Using Stokes’ theorem
Using separation of variables

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