Abstract

We reformulate the scattering amplitudes of 4D flat space gauge theory and gravity in the language of a 2D CFT on the celestial sphere. The resulting CFT structure exhibits an OPE constructed from 4D collinear singularities, as well as infinite-dimensional Kac-Moody and Virasoro algebras encoding the asymptotic symmetries of 4D flat space. We derive these results by recasting 4D dynamics in terms of a convenient foliation of flat space into 3D Euclidean AdS and Lorentzian dS geometries. Tree-level scattering amplitudes take the form of Witten diagrams for a continuum of (A)dS modes, which are in turn equivalent to CFT correlators via the (A)dS/CFT dictionary. The Ward identities for the 2D conserved currents are dual to 4D soft theorems, while the bulk-boundary propagators of massless (A)dS modes are superpositions of the leading and subleading Weinberg soft factors of gauge theory and gravity. In general, the massless (A)dS modes are 3D Chern-Simons gauge fields describing the soft, single helicity sectors of 4D gauge theory and gravity. Consistent with the topological nature of Chern-Simons theory, Aharonov-Bohm effects record the “tracks” of hard particles in the soft radiation, leading to a simple characterization of gauge and gravitational memories. Soft particle exchanges between hard processes define the Kac-Moody level and Virasoro central charge, which are thereby related to the 4D gauge coupling and gravitational strength in units of an infrared cutoff. Finally, we discuss a toy model for black hole horizons via a restriction to the Rindler region.

Highlights

  • The AdS/CFT correspondence [1,2,3,4,5,6,7] has revealed profound insights into the dualities equating theories with and without gravity

  • The resulting CFT structure exhibits an OPE constructed from 4D collinear singularities, as well as infinite-dimensional Kac-Moody and Virasoro algebras encoding the asymptotic symmetries of 4D flat space

  • We derive the central objects of this conjectured 2D CFT — namely the conserved currents and stress tensor — and show how the corresponding Kac-Moody and Virasoro algebras beautifully encode the asymptotic symmetries of 4D gauge theory [20,21,22,23,24] and gravity [25,26,27]

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Summary

Introduction

The AdS/CFT correspondence [1,2,3,4,5,6,7] has revealed profound insights into the dualities equating theories with and without gravity. In our formulation, these memory effects are naturally encoded as abelian and non-abelian Aharonov-Bohm phases from the encircling of hard particle “tracks” by CS gauge fields. We define bulk and boundary coordinates natural to achieve this mapping

Bulk coordinates
Milne region
Boundary coordinates
Approach
Mode expansion from Milne4 to AdS3
Witten diagrams in AdS3
Interaction vertices
Bulk-bulk propagator
Bulk-boundary propagator
Continuation from Milne4 to Mink4
Mink4 scattering amplitudes as CFT2 correlators
Conserved currents of CFT2
Mink4 soft theorems as CFT2 Ward identities
Equivalence of Milne4 and Mink4 soft limits
Kac-Moody algebra of CFT2
Chern-Simons theory and multiple soft emission
Abelian Chern-Simons theory
Non-Abelian Chern-Simons theory
Locating Chern-Simons theory in Mink4
Wess-Zumino-Witten model and multiple soft emission
3.10 Relation to memory effects
3.10.1 Chern-Simons memory and the Aharonov-Bohm effect
3.10.2 Chern-Simons level from internal soft exchange
3.11 Toy model for a black hole horizon
Gravity
Stress tensor of CFT2
Bulk-boundary propagator for AdS3 graviton
Ward identity for CFT2 stress tensor
Relationship to subleading soft theorems in Mink4
Virasoro algebra of CFT2
Equivalence to AdS3 gravity
Future directions
Full Text
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