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An Exact Operator That Knows Its Location

Nikhil Anand, Hongbin Chen, A. Liam Fitzpatrick, Jared Kaplan, Daliang Li

TL;DR

This work constructs an exact bulk proto-field $\phi$ in $AdS_3$/CFT$_2$ by expressing it as an infinite Virasoro descendant expansion of a CFT$_2$ primary $\mathcal{O}$, with two complementary routes: a gravitational Wilson line (bulk-boundary OPE block) approach and a symmetry-based algebraic definition. The authors show that $\phi$ transforms as a bulk scalar under Virasoro diffeomorphisms and that its vacuum correlators reproduce bulk perturbation theory at large $c$, while remaining valid in general vacuum AdS$_3$ geometries, including BTZ black holes, enabling potentially non-perturbative probes of bulk locality and horizons. They provide an exact algebraic construction for $\phi$, derive explicit low-order solutions and a general framework in terms of orthogonal quasi-primaries, and establish a recursion relation for stress-tensor correlators that reproduces $\langle \phi\mathcal{O}T\rangle$, $\langle \phi\mathcal{O}TT\rangle$, and $\langle \phi\mathcal{O}T\bar T\rangle$. These results offer a non-perturbative handle on bulk reconstruction in $AdS_3$/CFT$_2$, with potential applications to bulk locality and horizon physics, and lay groundwork for extensions to more general holographic settings.

Abstract

We use conformal symmetry to define an AdS$_3$ proto-field $φ$ as an exact linear combination of Virasoro descendants of a CFT$_2$ primary operator $\mathcal{O}$. We find that both symmetry considerations and a gravitational Wilson line formalism lead to the same results. The operator $φ$ has many desirable properties; in particular it has correlators that agree with gravitational perturbation theory when expanded at large $c$, and that automatically take the correct form in all vacuum AdS$_3$ geometries, including BTZ black hole backgrounds. In the future it should be possible to use $φ$ to probe bulk locality and black hole horizons at a non-perturbative level.

An Exact Operator That Knows Its Location

TL;DR

This work constructs an exact bulk proto-field in /CFT by expressing it as an infinite Virasoro descendant expansion of a CFT primary , with two complementary routes: a gravitational Wilson line (bulk-boundary OPE block) approach and a symmetry-based algebraic definition. The authors show that transforms as a bulk scalar under Virasoro diffeomorphisms and that its vacuum correlators reproduce bulk perturbation theory at large , while remaining valid in general vacuum AdS geometries, including BTZ black holes, enabling potentially non-perturbative probes of bulk locality and horizons. They provide an exact algebraic construction for , derive explicit low-order solutions and a general framework in terms of orthogonal quasi-primaries, and establish a recursion relation for stress-tensor correlators that reproduces , , and . These results offer a non-perturbative handle on bulk reconstruction in /CFT, with potential applications to bulk locality and horizon physics, and lay groundwork for extensions to more general holographic settings.

Abstract

We use conformal symmetry to define an AdS proto-field as an exact linear combination of Virasoro descendants of a CFT primary operator . We find that both symmetry considerations and a gravitational Wilson line formalism lead to the same results. The operator has many desirable properties; in particular it has correlators that agree with gravitational perturbation theory when expanded at large , and that automatically take the correct form in all vacuum AdS geometries, including BTZ black hole backgrounds. In the future it should be possible to use to probe bulk locality and black hole horizons at a non-perturbative level.

Paper Structure

This paper contains 33 sections, 194 equations, 2 figures.

Figures (2)

  • Figure 1: This figure portrays a bulk-boundary OPE block used to compute the correlator (\ref{['eq:phiOTTb']}). The red line denotes the gravitational or Chern-Simons Wilson line, while the blue circle suggests radial quantization around the block, so that it creates a definite linear combination of Virasoro descendants of the identity. The explicit computation involves line integrals over stress tensor correlators.
  • Figure 2: Dashed (solid) lines are graviton (scalar) propagators.