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Similar

S. Giusto, R. Russo, A. Tyukov, and C. Wen, “The CFT 6 origin of all tree-level 4-point correlators in AdS 3 × S 3 {}_{3}\times S^{3} ,” 2005.08560
Original
2005
Cited alongside, same era.
I. Bena, C.-W. Wang, and N. P. Warner, “Mergers and Typical Black Hole Microstates,” JHEP
2006
Cited alongside, same era.
I. Bena, A. Houppe, and N. P. Warner, “Delaying the Inevitable: Tidal Disruption in Microstate Geometries,” 2006.13939
Original
2006
Cited alongside, same era.
L. Cornalba, M. S. Costa, J. Penedones, and R. Schiappa, “Eikonal Approximation in AdS/CFT: From Shock Waves to Four-Point Functions,” JHEP
2007
Cited alongside, same era.
L. Cornalba, M. S. Costa, J. Penedones, and R. Schiappa, “Eikonal Approximation in AdS/CFT: Conformal Partial Waves and Finite N Four-Point Functions,” Nucl. Phys

Then

A. Galliani, S. Giusto, E. Moscato, and R. Russo, “Correlators at large c without information loss,” JHEP
Original
2016
Later among the works it cites.
M. S. Costa, T. Hansen, and J. Penedones, “Bounds for OPE coefficients on the Regge trajectory,” JHEP
Original
2017
Later among the works it cites.
D. Li, D. Meltzer, and D. Poland, “Conformal Bootstrap in the Regge Limit,” JHEP
Original
2017
Later among the works it cites.
A. Galliani, S. Giusto, and R. Russo, “Holographic 4-point correlators with heavy states,” JHEP
Original
2017
Later among the works it cites.
L. F. Alday, A. Bissi, and E. Perlmutter, “Holographic Reconstruction of AdS Exchanges from Crossing Symmetry,” JHEP

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2020

The Regge limit of AdS$_3$ holographic correlators

Giusto, Stefano, Hughes, Marcel R. R., Russo, Rodolfo

Understand

We study the Regge limit of 4-point AdS$_3 \times S^3$ correlators in the tree-level supergravity approximation and provide various explicit checks of the relation between the eikonal phase derived in the bulk picture and the anomalous dimensions of certain double-trace operators.

We consider both correlators involving all light operators and HHLL correlators with two light and two heavy multi-particle states.
These heavy operators have a conformal dimension proportional to the central charge and are pure states of the theory, dual to asymptotically AdS$_3 \times S^3$ regular geometries.
Deviation from AdS$_3 \times S^3$ is parametrised by a scale $\mu$ and is related to the conformal dimension of the dual heavy operator.