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Exact N=4 correlators of AdS(3)/CFT(2)

Ari Pakman, Amit Sever

TL;DR

The paper extends the AdS3/CFT2 correspondence to chiral $N=4$ operators, comparing exact bulk three-point functions in type IIB string theory on $AdS_3\times S^3\times M^4$ with boundary correlators of the symmetric orbifold CFT of $M^4$. It provides a closed-form bulk expression for these correlators, expressed in a factorized holomorphic/antiholomorphic form, and demonstrates exact agreement with boundary results of Lunin:2001pw for all $N=4$ chiral cases (including $M^4=T^4$) and extends to new bulk correlators for the $T^4$ case not previously computed on the boundary. The results rely on the $SL(2,R)_{k+2}$ and $SU(2)_{k-2}$ WZW structures and use $L(J_i,M_i)$ factors and $SU(2)$ 3j symbols to encode the fusion rules and selection rules. The discussion highlights the unexpected non-renormalization-like behavior across moduli space at large $N$ and outlines open questions regarding finite-$N$ corrections and the bulk interpretation of boundary fermion fusion choices.

Abstract

We extend to chiral N=4 operators the holographic agreement recently found between correlators of the symmetric orbifold of M^4 at large N and type IIB strings propagating in AdS(3) x S^3 x M^4, where M^4=T^4 or K3. We also present expressions for some bulk correlators not yet computed in the boundary.

Exact N=4 correlators of AdS(3)/CFT(2)

TL;DR

The paper extends the AdS3/CFT2 correspondence to chiral operators, comparing exact bulk three-point functions in type IIB string theory on with boundary correlators of the symmetric orbifold CFT of . It provides a closed-form bulk expression for these correlators, expressed in a factorized holomorphic/antiholomorphic form, and demonstrates exact agreement with boundary results of Lunin:2001pw for all chiral cases (including ) and extends to new bulk correlators for the case not previously computed on the boundary. The results rely on the and WZW structures and use factors and 3j symbols to encode the fusion rules and selection rules. The discussion highlights the unexpected non-renormalization-like behavior across moduli space at large and outlines open questions regarding finite- corrections and the bulk interpretation of boundary fermion fusion choices.

Abstract

We extend to chiral N=4 operators the holographic agreement recently found between correlators of the symmetric orbifold of M^4 at large N and type IIB strings propagating in AdS(3) x S^3 x M^4, where M^4=T^4 or K3. We also present expressions for some bulk correlators not yet computed in the boundary.

Paper Structure

This paper contains 3 sections, 16 equations.