Abstract

We examine how the Einstein-Hilbert action is renormalized by adding the usual counterterms and additional corner counterterms when the boundary surface has corners. A bulk geometry asymptotic to Hd+1 can have boundaries Sk× Hd−k and corners for 0 ≤ k < d. We show that the conformal anomaly when d is even is independent of k. When d is odd the renormalized action is a finite term that we show is independent of k when k is also odd. When k is even we were unable to extract the finite term using the counterterm method and we address this problem using instead the Kounterterm method. We also compute the mass of a two-charged black hole in AdS7 and show that background subtraction agrees with counterterm renormalization only if we use the infinite series expansion for the counterterm.

Highlights

  • The AdS-CFT correspondence relates Einstein gravity in the bulk with a conformal field theory on the boundary

  • When d is odd the renormalized action is a finite term that we show is independent of k when k is odd

  • We compute the mass of a two-charged black hole in AdS7 and show that background subtraction agrees with counterterm renormalization only if we use the infinite series expansion for the counterterm

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Summary

Introduction

The AdS-CFT correspondence relates Einstein gravity in the bulk with a conformal field theory on the boundary. If the boundary is viewed as a regulator surface near infinity, we may subtract the divergent terms in the on-shell action by adding a counterterm [16,17,18]. The on-shell value is a function of the boundary metric, I = I(hμν) To this action, one may add a boundary term that only depends on the boundary metric and its tangential derivatives without affecting the bulk equations of motion. One may add a boundary term that only depends on the boundary metric and its tangential derivatives without affecting the bulk equations of motion This can be used to construct a counterterm action [16,17,18]1. There are two figures that we placed at the end of the paper

Two different views of a noncompact boundary
Noncompact boundaries
One dimension
Two dimensions
Three dimensions
G 2 cosh ρ0 sinh ρ0
Arbitrary odd dimension
Arbitrary even dimension
Subleading order
The conformal anomaly
The counterterm
Pole cancelations
The Kounterterm method
The finite term on H3 revisited
The mass of a bulk geometry
The mass of AdS
The mass of a black hole in AdS7
Another formula for the counterterm
A Conventions for the Riemann tensor
C Mass of AdS by using truncated counterterm
Full Text
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