Thermal one point functions, large and interior geometry of black holes
arXiv:2212.07758 · doi:10.1007/JHEP03(2023)256
Abstract
We study thermal one point functions of massive scalars in black holes. These are induced by coupling the scalar to either the Weyl tensor squared or the Gauss-Bonnet term. Grinberg and Maldacena argued that the one point functions sourced by the Weyl tensor exponentiate in the limit of large scalar masses and they contain information of the black hole geometry behind the horizon. We observe that the one point functions behave identically in this limit for either of the couplings mentioned earlier. We show that in an appropriate large limit, the one point function for the charged black hole in can be obtained exactly. These black holes in general contain an inner horizon. We show that the one point function exponentiates and contains the information of both the proper time between the outer horizon to the inner horizon as well as the proper length from the inner horizon to the singularity. We also show that Gauss-Bonnet coupling induced one point functions in black holes with hyperbolic horizons behave as anticipated by Grinberg-Maldacena. Finally, we study the one point functions in the background of rotating BTZ black holes induced by the cubic coupling of scalars.
arXiv comment40 pages, 4 figures, 1 table, reference added, typos corrected
References in corpus (22)
- Charged AdS Black Holes and Catastrophic Holography
- Towards a derivation of holographic entanglement entropy
- AdS3 Black Holes and a Stringy Exclusion Principle
- Topological Black Holes in Anti-de Sitter Space
- The Black Hole Singularity in AdS/CFT
- AdS/CFT Duals of Topological Black Holes and the Entropy of Zero-Energy States
- AdS/CFT 4-point functions: How to succeed at z-integrals without really trying
- Entropy Function for Heterotic Black Holes
- The Conformal Bootstrap at Finite Temperature
- A Cardy Formula for Three-Point Coefficients: How the Black Hole Got its Spots
- Proper time to the black hole singularity from thermal one-point functions
- The Large D Limit of Einstein's Equations
- AdS Membranes Wrapped on Surfaces of Arbitrary Genus
- Correlation functions in finite temperature CFT and black hole singularities
- Genus Two Partition Functions and Renyi Entropies of Large c CFTs
- Exact thermal correlators of holographic s
- A Holographic Model for Quantum Critical Responses
- Holographic Observables at Large
- Holographic correlation functions at finite density and/or finite temperature
- Sum rules and three point functions
- Shear sum rules at finite chemical potential
- The Special Role of Toroidal Black Holes in Holography
Cited by in corpus (8)
- Boundary signature of singularity in the presence of a shock wave
- Holographic Thermal Correlators for Hyperbolic s
- Diving into a holographic multi-band superconductor
- Chaotic and Thermal Aspects in the Highly Excited String S-Matrix
- Interior structure of the holographic s + p superconductor and chaotic-stable transition near the black hole singularity
- Finite Temperature at Finite Places
- Proper time to singularity and thermal correlators
- A holographic realization of correlation and mutual information