Holographic Renormalization Group and Stress Tensor Operators

Abstract

The holographic duality conjectures a relation between strongly coupled quantum systems and quantum gravity in higher-dimensional spacetimes. Gravitational theories in two and three dimensions are meaningful examples for classical and quantum exploration due to their unique characteristics, notably the absence of propagating bulk degrees of freedom and the presence of only boundary degrees of freedom, distinguishing them from higher-dimensional counterparts. These gravitational theories exhibit complex interactions when the bulk spacetime has a finite size, regulated by Zamolodchikov's double-trace irrelevant \(T\overline{T}\) operator. This thesis aims to gain a holographic understanding of \(\mathrm{AdS}_3\) and JT gravity under the influence of the \(T\overline{T}\) deformation. Under a finite radial cutoff, these theories exhibit perturbative behavior that implies the emergence of the Nambu-Goto action for the corresponding boundary graviton action. We also conducted semi-classical calculations of observables related to finite-cutoff gravity and its dual \(T\overline{T}\)-deformed CFT description, including correlation functions involving stress tensors and gravitational Wilson lines, along with an analysis of their supersymmetric extensions. Additionally, we explored the implications of general stress tensor deformations within field-theoretic and holographic settings. This thesis integrates previously adapted publications while also pioneering new ground, notably exploring the definition of a quantum \(T\overline{T}\) operator beyond two dimensions with \(\frac{1}{N}\) corrections, investigating quantum-corrected higher point correlators for a planar boundary, and offering insights into a two-dimensional spherical boundary at a finite cutoff. Furthermore, throughout the thesis, we show more details in calculations at various points.