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Particle production in time-dependent gravitational fields: the expanding mass shell
We compute the production of particles from the gravitational field of an expanding mass shell. Contrary to the situation of Hawking radiation and the production of cosmological perturbations during cosmological inflation, the example of an expanding mass shell has no horizon and no singularity. We...
Autores principales: | , , |
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Lenguaje: | eng |
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2002
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Acceso en línea: | https://dx.doi.org/10.1088/0264-9381/20/11/325 http://cds.cern.ch/record/589463 |
_version_ | 1780899631056551936 |
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author | Hossenfelder, S Schwarz, Dominik J Greiner, W |
author_facet | Hossenfelder, S Schwarz, Dominik J Greiner, W |
author_sort | Hossenfelder, S |
collection | CERN |
description | We compute the production of particles from the gravitational field of an expanding mass shell. Contrary to the situation of Hawking radiation and the production of cosmological perturbations during cosmological inflation, the example of an expanding mass shell has no horizon and no singularity. We apply the method of `ray-tracing', first introduced by Hawking, and calculate the energy spectrum of the produced particles. The result depends on three parameters: the expansion velocity of the mass shell, its radius, and its mass. Contrary to the situation of a collapsing mass shell, the energy spectrum is non-thermal. Invoking time reversal we reproduce Hawking's thermal spectrum in a certain limit. |
id | cern-589463 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2002 |
record_format | invenio |
spelling | cern-5894632019-09-30T06:29:59Zdoi:10.1088/0264-9381/20/11/325http://cds.cern.ch/record/589463engHossenfelder, SSchwarz, Dominik JGreiner, WParticle production in time-dependent gravitational fields: the expanding mass shellGeneral Relativity and CosmologyWe compute the production of particles from the gravitational field of an expanding mass shell. Contrary to the situation of Hawking radiation and the production of cosmological perturbations during cosmological inflation, the example of an expanding mass shell has no horizon and no singularity. We apply the method of `ray-tracing', first introduced by Hawking, and calculate the energy spectrum of the produced particles. The result depends on three parameters: the expansion velocity of the mass shell, its radius, and its mass. Contrary to the situation of a collapsing mass shell, the energy spectrum is non-thermal. Invoking time reversal we reproduce Hawking's thermal spectrum in a certain limit.gr-qc/0210110CERN-TH-2002-286oai:cds.cern.ch:5894632002-10-31 |
spellingShingle | General Relativity and Cosmology Hossenfelder, S Schwarz, Dominik J Greiner, W Particle production in time-dependent gravitational fields: the expanding mass shell |
title | Particle production in time-dependent gravitational fields: the expanding mass shell |
title_full | Particle production in time-dependent gravitational fields: the expanding mass shell |
title_fullStr | Particle production in time-dependent gravitational fields: the expanding mass shell |
title_full_unstemmed | Particle production in time-dependent gravitational fields: the expanding mass shell |
title_short | Particle production in time-dependent gravitational fields: the expanding mass shell |
title_sort | particle production in time-dependent gravitational fields: the expanding mass shell |
topic | General Relativity and Cosmology |
url | https://dx.doi.org/10.1088/0264-9381/20/11/325 http://cds.cern.ch/record/589463 |
work_keys_str_mv | AT hossenfelders particleproductionintimedependentgravitationalfieldstheexpandingmassshell AT schwarzdominikj particleproductionintimedependentgravitationalfieldstheexpandingmassshell AT greinerw particleproductionintimedependentgravitationalfieldstheexpandingmassshell |