Abstract
We study certain infinite families of two-particle operators exchanged in 4pt correlators $⟨{\mathcal{O}}_{{p}_{1}}{\mathcal{O}}_{{p}_{2}}{\mathcal{O}}_{{p}_{3}}{\mathcal{O}}_{{p}_{4}}⟩$ of tensor multiplets living on the ${\mathrm{AdS}}_{3}\ifmmode\times\else\texttimes\fi{}{S}^{3}$ background. This is the weakly curved, weakly coupled SUGRA theory dual to the D1-D5 system with RR flux. At tree level in Mellin space, all these correlators are nicely determined by a single amplitude, which makes manifest the large $p$ limit, the connection with the flat space S-matrix, and a six dimensional conformal symmetry. We compute the $(1,1)\ifmmode\times\else\texttimes\fi{}\overline{(1,1)}$ superconformal blocks for the two-dimensional $\mathcal{N}=(4,4)$ conformal theory at the boundary, and then we obtain a formula for the anomalous dimensions of the two-particle operators exchanged in the symmetric and antisymmetric flavor channels. These anomalous dimensions solve a mixing problem which is analogous to the one in ${\mathrm{AdS}}_{5}\ifmmode\times\else\texttimes\fi{}{S}^{5}$ with interesting modifications. Along the way we show how the $(1,1)\ifmmode\times\else\texttimes\fi{}\overline{(1,1)}$ superconformal blocks relate to those in $\mathcal{N}=4$ SYM in four dimensions, and provide new intuition on the known data for ${\mathrm{AdS}}_{5}\ifmmode\times\else\texttimes\fi{}{S}^{5}$.
Highlights
Understanding what are the possible UV completions of classical gravity is one of the most exciting and challenging problems of modern theoretical physics
The dual conformal field theory that we are studying has N 1⁄4 ð4; 4Þ superconformal symmetry in 2d, and the relevant superconformal blocks belong to the product ð1; 1Þ × ð1; 1Þ, where the notation (1,1) refers to superconformal blocks of SUð1; 1j2Þ, studied in [39]
It is simple to see that the N 1⁄4 ð4; 4Þ Ward identity, 1⁄2ð∂x þ ∂yÞGx1⁄4y 1⁄4 0; 1⁄2ð∂xþ ∂y ÞGx1⁄4y 1⁄4 0 ð18Þ is satisfied for any C, S and H
Summary
Understanding what are the possible UV completions of classical gravity is one of the most exciting and challenging problems of modern theoretical physics. Valuable help might come from solving the same problem, but in spaces with an AdS factor, where the AdS/CFT correspondence plays an important role [1] In such circumstances, would a low energy field theorist be able to reconstruct the underlying curved string theory, let us say, out of scattering data of gravitons and single particles operators? The same twoparticle bootstrap program was extended to compute one-loop 4pt amplitudes of arbitrary external single particle operators, carrying Kaluza-Klein charge under the sphere. The spectrum of anomalous dimensions of two-particle operators in AdS5 × S5 is not completely lifted by tree level supergravity [11,14], but. Following the unmixing approach of [11,14], we will compute tree level anomalous dimensions of certain two-particle operators with flavor, denoted afterwards by OþðrsÞ, exchanged in hOp1 Op2 Op3 Op4 i. We will show that, as a byproduct of our studies here, superconformal blocks for both AdS5 × S5 and AdS3 × S3 can be treated at once by using the ð1; 1Þ × ð1; 1Þ formalism that we will introduce
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