Random Boundary Geometry and Gravity Dual of $T\bar{T}$ Deformation
Shinji Hirano, Masaki Shigemori
TL;DR
This work develops Cardy’s random geometry approach to the $T\overline{T}$ deformation and provides a gravity-dual interpretation as an ensemble of AdS$_3$/BTZ spacetimes with randomly fluctuating boundary diffeomorphisms. It streamlines computations and extends the framework to correlation functions, showing that all-order energy spectra satisfy a Burgers-type flow and that thermal free energy evolves coherently under the same dynamics, with the gravity dual reproducing these results via the BTZ spectrum and on-shell action. The authors formulate precise field-theory PDEs for both energy and free energy and derive all-order correlator corrections, supporting a consistent holographic dictionary in which deformed observables are obtained by averaging undeformed gravity correlators over the diffeomorphism ensemble. This gravity-dual construction is contrasted with cutoff-AdS proposals and offers a broader, geometry-centric perspective on UV completion, non-locality, and entanglement features in $T\overline{T}$-deformed theories, with several directions for future work including rotation, other topologies, and chaos.
Abstract
We study the random geometry approach to the $T\bar{T}$ deformation of 2d conformal field theory developed by Cardy and discuss its realization in a gravity dual. In this representation, the gravity dual of the $T\bar{T}$ deformation becomes a straightforward translation of the field theory language. Namely, the dual geometry is an ensemble of AdS$_3$ spaces or BTZ black holes, without a finite cutoff, but instead with randomly fluctuating boundary diffeomorphisms. This reflects an increase in degrees of freedom in the renormalization group flow to the UV by the irrelevant $T\bar{T}$ operator. We streamline the method of computation and calculate the energy spectrum and the thermal free energy in a manner that can be directly translated into the gravity dual language. We further generalize this approach to correlation functions and reproduce the all-order result with universal logarithmic corrections computed by Cardy in a different method. In contrast to earlier proposals, this version of the gravity dual of the $T\bar{T}$ deformation works not only for the energy spectrum and the thermal free energy but also for correlation functions.
