Abstract

We obtain a closed form expression for the Action describing pure gravity, in light-cone gauge, in a four-dimensional Anti-de Sitter background. We perform a perturbative expansion of this closed form result to extract the cubic interaction vertex in this gauge.

Highlights

  • Quantum field theories of gravity are plagued by divergences that seem to rule out any straightforward attempt to unite quantum theory and the general theory of relativity

  • The KLT relations are valid on flat spacetime backgrounds so one question that motivates the present work is whether such perturbative ties between YangMills and gravity survive when we move to curved spacetime backgrounds

  • We describe how pure gravity is formulated in light-cone gauge on an AdS4 background

Read more

Summary

Introduction

Quantum field theories of gravity are plagued by divergences that seem to rule out any straightforward attempt to unite quantum theory and the general theory of relativity. The KLT relations are valid on flat spacetime backgrounds so one question that motivates the present work is whether such perturbative ties between YangMills and gravity survive when we move to curved spacetime backgrounds It is not clear how a Yang-Mills ↔ gravity relationship, on AdS4 , would trace back to a stringy origin. To achieve a light-cone formulation of higher spin fields (λ > 2) on curved backgrounds, it is essential to have as a guidepost the Action for pure gravity (λ = 2) on those backgrounds. This is one of the results we obtain here. We perform a perturbative expansion of this gauge-fixed Action to first order in the gravitational coupling constant and comment on the resulting interaction vertex

Preliminaries
Light-cone formulation
Light-cone Action
Perturbative expansion
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.