Global Structure of Evaporating Black Holes
arXiv:gr-qc/9807031 · doi:10.1016/S0370-2693(99)00071-4
Abstract
By extending the charged Vaidya metric to cover all of spacetime, we obtain a Penrose diagram for the formation and evaporation of a charged black hole. In this construction, the singularity is time-like. The entire spacetime can be predicted from initial conditions if boundary conditions at the singularity are known.
arXiv commentLaTeX, 10 pages, 1 figure; v2: references added, uncorrupted figure file
Cited by in corpus (25)
- Are Extremal 2D Black Holes Really Frozen ?
- Can accretion disk properties observationally distinguish black holes from naked singularities?
- Vaidya spacetimes, black-bounces, and traversable wormholes
- The causal structure of dynamical charged black holes
- Gravitational collapse of a Hagedorn fluid in Vaidya geometry
- Null fluid collapse in brane world models
- Thermality of the Hawking flux
- Role of evaporation in gravitational collapse
- Internal structure of charged black holes
- Black hole evaporation and semiclassical thin shell collapse
- Surrounded Vaidya Solution by Cosmological Fields
- Surrounded Vaidya black holes: apparent horizon properties
- Ramifications of Lineland
- Black hole complementarity with local horizons and Horowitz-Maldacena's proposal
- The information recovery problem
- Nonstationary regime for quasinormal modes of the charged Vaidya metric
- Understanding black hole evaporation using explicitly computed Penrose diagrams
- Membrane Horizons: The Black Hole's New Clothes
- On maximal analytical extension of the Vaidya metric
- Growth of a Black Hole
- Evaporation of a nonsingular Reissner-Nordström black hole and information loss problem
- Information recovery from evaporating black holes
- Double null formulation of the general Vaidya metric
- Generalized Vaidya Spacetime in Cotton and Conformal Killing Theories
- A Model of the Collapse and Evaporation of Charged Black Holes