Emission rates, the correspondence principle and the information paradox
From MaRDI portal
Publication:1570594
DOI10.1016/S0550-3213(98)00336-8zbMath0964.83029arXivhep-th/9706151OpenAlexW2022543152MaRDI QIDQ1570594
Publication date: 11 July 2000
Published in: Nuclear Physics. B (Search for Journal in Brave)
Full work available at URL: https://arxiv.org/abs/hep-th/9706151
Related Items (15)
Comments on black holes I: the possibility of complementarity ⋮ Schwarzschild fuzzball and explicitly unitary Hawking radiation ⋮ Statistical Interpretation of the Bekenstein Entropy for Systems with a Stretched Horizon ⋮ Dual geometries for a set of 3-charge microstates ⋮ 3-charge geometries and their CFT duals ⋮ Absorption of scalars by extended objects ⋮ A microscopic model for the black hole: black string phase transition ⋮ Dynamics of supertubes ⋮ Can we observe fuzzballs or firewalls? ⋮ Constructing `hair' for the three charge hole ⋮ A PROPOSAL TO RESOLVE THE BLACK HOLE INFORMATION PARADOX ⋮ Black holes and beyond ⋮ AdS/CFT duality and the black hole information paradox ⋮ What Exactly is the Information Paradox? ⋮ The flaw in the firewall argument
Cites Work
- Asymptotic level density in heterotic string theory and rotating black holes.
- Microscopic origin of the Bekenstein-Hawking entropy
- Interactions involving D-branes
- Emission of charged particles from four- and five-dimensional black holes
- Excitations of D-strings, entropy and duality
- Bound states of strings and \(p\)-branes
- D-branes and fat black holes
- \(D\)-brane approach to black hole quantum mechanics
- Comparing decay rates for black holes and D-branes
This page was built for publication: Emission rates, the correspondence principle and the information paradox