Branches of the Black Hole Wave Function Need Not Contain Firewalls
Abstract
We discuss the branching structure of the quantum-gravitational wave function that describes the evaporation of a black hole. A global wave function which initially describes a classical Schwarzschild geometry is continually decohered into distinct semiclassical branches by the emission of Hawking radiation. The laws of quantum mechanics dictate that the wave function evolves unitarily, but this unitary evolution is only manifest when considering the global description of the wave function; it is not implemented by time evolution on a single semiclassical branch. Conversely, geometric notions like the position or smoothness of a horizon only make sense on the level of individual branches. We consider the implications of this picture for probes of black holes by classical observers in definite geometries, like those involved in the Almheiri-Marolf-Polchinski-Sully construction. We argue that individual branches can describe semiclassical geometries free of firewalls, even as the global wave function evolves unitarily. We show that the pointer states of infalling detectors that are robust under Hamiltonian evolution are distinct from, and incompatible with, those of exterior detectors stationary with respect to the black hole horizon, in the sense that the pointer bases are related to each other via nontrivial transformations that mix the system, apparatus, and environment. This result describes a Hilbert-space version of black hole complementarity.
Additional Information
© 2018 Published by the American Physical Society. Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI. Funded by SCOAP3. Received 20 December 2017; published 20 June 2018. We thank Ahmed Almheiri, Raphael Bousso, William Donnelly, Masahiro Hotta, Cindy Keeler, Yasunori Nomura, Don N. Page, Guillaume Verdon, and Koji Yamaguchi for helpful discussions. This work is supported by the U.S. Department of Energy, Office of Science, Office of High Energy Physics, under Award No. DE-SC0011632. N. B. is supported by the National Science Foundation, under Grant No. 82248-13067-44-PHPXH. A. C.-D. is supported by a Beatrice and Sai-Wai Fu Graduate Fellowship in Physics and the Gordon and Betty Moore Foundation through Grant No. 776 to the Caltech Moore Center for Theoretical Cosmology and Physics. J. P. is supported in part by the Simons Foundation and in part by the Natural Sciences and Engineering Research Council of Canada. G. N. R. is supported by the Miller Institute for Basic Research in Science at the University of California, Berkeley.Attached Files
Published - PhysRevD.97.126014.pdf
Submitted - 1712.04955.pdf
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Additional details
- Eprint ID
- 84217
- Resolver ID
- CaltechAUTHORS:20180109-165521863
- Department of Energy (DOE)
- DE-SC0011632
- NSF
- 82248-13067-44-PHPXH
- Beatrice and Sai-Wai Fu Graduate Fellowship, Caltech
- Gordon and Betty Moore Foundation
- 776
- Simons Foundation
- Natural Sciences and Engineering Research Council of Canada (NSERC)
- Miller Institute for Basic Research in Science
- SCOAP3
- Caltech Moore Center for Theoretical Cosmology and Physics
- Created
-
2018-01-10Created from EPrint's datestamp field
- Updated
-
2021-11-15Created from EPrint's last_modified field
- Caltech groups
- Walter Burke Institute for Theoretical Physics, Moore Center for Theoretical Cosmology and Physics
- Other Numbering System Name
- CALT-TH
- Other Numbering System Identifier
- 2017-068