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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...

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Detalles Bibliográficos
Autores principales: Hossenfelder, S, Schwarz, Dominik J, Greiner, W
Lenguaje:eng
Publicado: 2002
Materias:
Acceso en línea:https://dx.doi.org/10.1088/0264-9381/20/11/325
http://cds.cern.ch/record/589463
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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.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2002
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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