Abstract

The symmetric orbifold of T4\mathbb{T}^4 was recently shown to be exactly dual to string theory on AdS3×S3×T4{\rm AdS}_3\times {\rm S}^3 \times \mathbb{T}^4 with minimal (k=1k=1) NS-NS flux. The worldsheet theory is best formulated in terms of the hybrid formalism of Berkovits, Vafa & Witten (BVW), in terms of which the AdS3×S3{\rm AdS}_3\times {\rm S}^3 factor is described by a psu(1,1∣2)k\mathfrak{psu}(1,1|2)_k WZW model. At level k=1k=1, psu(1,1∣2)1\mathfrak{psu}(1,1|2)_1 has a free field realisation that is obtained from that of u(1,1∣2)1\mathfrak{u}(1,1|2)_1 upon setting a u(1)\mathfrak{u}(1) field, often called ZZ, to zero. We show that the free field version of the N=2{\cal N}=2 generators of BVW (whose cohomology defines the physical states) does not give rise to an N=2{\cal N}=2 algebra, but is rather contaminated by terms proportional to the ZZ-field. We also show how to overcome this problem by introducing additional ghost fields that implement the quotienting by ZZ.

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