Abstract

Three-dimensional conformal field theories (CFTs) with slightly broken higher spin symmetry provide an interesting laboratory to study general properties of CFTs and their roles in the AdS/CFT correspondence. In this work we compute the planar four-point functions at arbitrary ’t Hooft coupling λ in the CFTs with slightly broken higher spin symmetry. We use a bootstrap approach based on the approximate higher spin Ward identity. We show that the bootstrap equation is separated into two parts with opposite parity charges, and it leads to a recursion relation for the λ expansions of the correlation functions. The λ expansions terminate at order λ2 and the solutions are exact in λ. Our work generalizes the approach proposed by Maldacena and Zhiboedov to four-point correlators, and it amounts to an on-shell study for the 3D Chern-Simons vector models and their holographic duals in AdS4. Besides, we show that the same results can also be obtained rather simply from bosonization duality of 3D Chern-Simons vector models. The odd term at order O(λ) in the spinning four-point function relates to the free boson correlator through a Legendre transformation. This provides new evidence on the 3D bosonization duality at the spinning four-point function level. We expect this work can be generalized to a complete classification of general four-point functions of single trace currents.

Highlights

  • A class of 3D conformal field theories (CFTs) with slightly broken higher spin symmetry is given by U(N )k Chern-Simons (CS) theories coupled to a fundamental boson or fermion [22,23,24,25]

  • We show that the bootstrap equation is separated into two parts with opposite parity charges, and it leads to a recursion relation for the λ expansions of the correlation functions

  • The difference comes from the fact that the three-point functions have already been fixed by the conformal symmetry up to certain operator product expansion (OPE) coefficients, the approximate higher spin Ward identities for three-point correlators are essentially a set of algebraic equations of these coefficients; while the four-point correlators contain functions of the conformal invariant cross ratios, which are generically unknown besides certain constraints from permutation symmetry and current conservation laws

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Summary

Higher spin algebra and Ward identity

For completeness we briefly review the higher spin algebra and the higher spin Ward identity in conformal theories. The odd term is non-vanishing only for the spins satisfying the triangle rule si si+1+si+2 These results indicate that the theories with exact higher spin symmetry have connections with free theories. The odd term remains mysterious, and to understand the role of this term, it needs to explore more dynamical restrictions from higher spin symmetry. This is what has been fulfilled in [17, 21]

Exact higher spin symmetry
Slightly broken higher spin symmetry
Four-point functions from approximate higher spin Ward identity
Approximate higher spin Ward identity for the scalar correlator
General form of spinning four-point correlator
Bosonization duality at the level of four-point functions
Scalar four-point function from Legendre transformation
Spinning four-point function from Legendre transformation
Conclusions and discussions
A Conformal integration and D -function
B Conformal integrals in approximate higher spin Ward identity
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