Renormalization of the Einstein-Hilbert action
arXiv:1911.04178 · doi:10.1007/JHEP05(2020)064
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 can have boundaries and corners for . We show that the conformal anomaly when is even is independent of . When is odd the renormalized action is a finite term that we show is independent of when is also odd. When 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 AdS and show that background subtraction agrees with counterterm renormalization only if we use the infinite series expansion for the counterterm.
arXiv comment64 pages
References in corpus (18)
- The Dynamics of General Relativity
- A Stress Tensor for Anti-de Sitter Gravity
- The Holographic Weyl anomaly
- Embedding AdS Black Holes in Ten and Eleven Dimensions
- Holographic Dual of BCFT
- Phases of R-charged Black Holes, Spinning Branes and Strongly Coupled Gauge Theories
- The Gravitational Action in Asymptotically AdS and Flat Spacetimes
- The large D limit of General Relativity
- Holographic Renormalization of Asymptotically Flat Spacetimes
- Regularization of odd-dimensional AdS gravity: Kounterterms
- Hamiltonian formulation of f(Riemann) theories of gravity
- Boundary Term in Metric f(R) Gravity: Field Equations in the Metric Formalism
- Variational Principle for Gravity with Null and Non-null boundaries: A Unified Boundary Counter-term
- Boundary and Corner Terms in the Action for General Relativity
- Free energy and boundary anomalies on spaces
- Renormalized AdS gravity and holographic entanglement entropy of even-dimensional CFTs
- On the classification of consistent boundary conditions for -Gravity
- Nonabelian M5-brane on