Distinguishing causal time from Minkowski time and a model for the black hole quantum eigenstates
| dc.creator | Hooft, G. 't | |
| dc.date | 1997-11-18 | |
| dc.date.accessioned | 2026-07-07T06:32:26Z | |
| dc.date.available | 2026-07-07T06:32:26Z | |
| dc.description | A discussion is presented of the principle of black hole com- plementarity. It is argued that this principle could be viewed as a breakdown of general relativity, or alternatively, as the introduction of a time variable with multiple `sheets' or `branches' A consequence of the theory is that the stress-energy tensor as viewed by an outside observer is not simply the Lorentz-transform of the tensor viewed by an ingoing observer. This can serve as a justification of a new model for the black hole atmosphere, recently re-introduced. It is discussed how such a model may lead to a dynamical description of the black hole quantum states. | |
| dc.description | Plenary Lecture Notes ICMP97, Brisbane, Australia, July 1997. 12 pages LaTeX, 5 Figures Postscript | |
| dc.identifier | https://arxiv.org/abs/gr-qc/9711053 | |
| dc.identifier | http://arxiv.org/abs/gr-qc/9711053 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/98901 | |
| dc.subject | General Relativity and Quantum Cosmology | |
| dc.title | Distinguishing causal time from Minkowski time and a model for the black hole quantum eigenstates | |
| dc.type | text |