Black-hole threshold solutions in stiff fluid collapse
Black-hole threshold solutions in stiff fluid collapse
Numerical studies of the gravitational collapse of a stiff (P = ?) fluid have found the now-familiar critical phenomena, namely scaling of the black-hole mass with a critical exponent and continuous self-similarity at the threshold of black-hole formation. Using the equivalence of an irrotational stiff fluid to a massless scalar field, we construct the critical solution as a scalar field solution by making a self-similarity ansatz. We find evidence that this solution has exactly one growing perturbation mode; both the mode and the critical exponent, ? 0.94, derived from its eigenvalue agree with those measured in perfect fluid collapse simulations. We explain why this solution is seen as a critical solution in stiff fluid collapse but not in scalar field collapse, and conversely why the scalar field critical solution is not seen in stiff fluid collapse, even though the two systems are locally equivalent.
6359-6375
Brady, Patrick R.
83392176-06db-47fe-9267-2eb168b3deb3
Choptuik, Matthew W.
1167c64b-0496-4fde-9ffd-e81230a65521
Gundlach, Carsten
586f1eb5-3185-4b2b-8656-c29c436040fc
Neilsen, David W.
33e7833c-78b1-4cf0-97ff-be7efa1f54c1
2002
Brady, Patrick R.
83392176-06db-47fe-9267-2eb168b3deb3
Choptuik, Matthew W.
1167c64b-0496-4fde-9ffd-e81230a65521
Gundlach, Carsten
586f1eb5-3185-4b2b-8656-c29c436040fc
Neilsen, David W.
33e7833c-78b1-4cf0-97ff-be7efa1f54c1
Brady, Patrick R., Choptuik, Matthew W., Gundlach, Carsten and Neilsen, David W.
(2002)
Black-hole threshold solutions in stiff fluid collapse.
Classical and Quantum Gravity, 19 (24), .
(doi:10.1088/0264-9381/19/24/306).
Abstract
Numerical studies of the gravitational collapse of a stiff (P = ?) fluid have found the now-familiar critical phenomena, namely scaling of the black-hole mass with a critical exponent and continuous self-similarity at the threshold of black-hole formation. Using the equivalence of an irrotational stiff fluid to a massless scalar field, we construct the critical solution as a scalar field solution by making a self-similarity ansatz. We find evidence that this solution has exactly one growing perturbation mode; both the mode and the critical exponent, ? 0.94, derived from its eigenvalue agree with those measured in perfect fluid collapse simulations. We explain why this solution is seen as a critical solution in stiff fluid collapse but not in scalar field collapse, and conversely why the scalar field critical solution is not seen in stiff fluid collapse, even though the two systems are locally equivalent.
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Published date: 2002
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Local EPrints ID: 29189
URI: http://eprints.soton.ac.uk/id/eprint/29189
ISSN: 0264-9381
PURE UUID: d43946bd-d9c0-4eff-a188-0d1d5a4733c9
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Date deposited: 11 May 2006
Last modified: 16 Mar 2024 03:15
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Author:
Patrick R. Brady
Author:
Matthew W. Choptuik
Author:
David W. Neilsen
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