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Emission Channels from Perturbed Quantum Black Holes

We calculate the emission of gravitational waves, gravitons, photons, and neutrinos from a perturbed Schwarzschild black hole (BH). The perturbation can be due to either classical or quantum sources and therefore the injected energy can be either positive or negative. The emission can be classical i...

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Detalles Bibliográficos
Autores principales: Brustein, Ram, Sherf, Yotam
Lenguaje:eng
Publicado: 2019
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.100.124005
http://cds.cern.ch/record/2663355
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author Brustein, Ram
Sherf, Yotam
author_facet Brustein, Ram
Sherf, Yotam
author_sort Brustein, Ram
collection CERN
description We calculate the emission of gravitational waves, gravitons, photons, and neutrinos from a perturbed Schwarzschild black hole (BH). The perturbation can be due to either classical or quantum sources and therefore the injected energy can be either positive or negative. The emission can be classical in nature, as in the case of gravitational waves, or of quantum nature, for gravitons and the additional fields. We first set up the theoretical framework for calculating the emission by treating the case of a minimally coupled scalar field and then present the results for the other fields. We perform the calculations in the horizon-locking gauge in which the BH horizon is deformed, following similar calculations of tidal deformations of BH horizons. The classical emission can be interpreted as due to a partial exposure of a nonempty BH interior, while the quantum emission can be interpreted as an increased Hawking radiation flux due to the partial exposure of the BH interior. The degree of exposure of the BH interior is proportional to the magnitude of the injected null energy.
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spelling cern-26633552023-10-04T07:27:56Zdoi:10.1103/PhysRevD.100.124005http://cds.cern.ch/record/2663355engBrustein, RamSherf, YotamEmission Channels from Perturbed Quantum Black Holesgr-qcGeneral Relativity and Cosmologyhep-thParticle Physics - TheoryWe calculate the emission of gravitational waves, gravitons, photons, and neutrinos from a perturbed Schwarzschild black hole (BH). The perturbation can be due to either classical or quantum sources and therefore the injected energy can be either positive or negative. The emission can be classical in nature, as in the case of gravitational waves, or of quantum nature, for gravitons and the additional fields. We first set up the theoretical framework for calculating the emission by treating the case of a minimally coupled scalar field and then present the results for the other fields. We perform the calculations in the horizon-locking gauge in which the BH horizon is deformed, following similar calculations of tidal deformations of BH horizons. The classical emission can be interpreted as due to a partial exposure of a nonempty BH interior, while the quantum emission can be interpreted as an increased Hawking radiation flux due to the partial exposure of the BH interior. The degree of exposure of the BH interior is proportional to the magnitude of the injected null energy.We calculate the emission of gravitational waves, gravitons, photons and neutrinos from a perturbed Schwarzschild blackhole (BH). The perturbation can be due to either classical or quantum sources and therefore the injected energy can be either positive or negative. The emission can be classical in nature, as in the case of gravitational waves, or of quantum nature, for gravitons and the additional fields. We first set up the theoretical framework for calculating the emission by treating the case of a minimally coupled scalar field and then present the results for the other fields. We perform the calculations in the horizon-locking gauge in which the BH horizon is deformed, following similar calculations of tidal deformations of BH horizons. The classical emission can be interpreted as due to a partial exposure of a nonempty BH interior, while the quantum emission can be interpreted as an increased Hawking radiation flux due to the partial exposure of the BH interior. The degree of exposure of the BH interior is proportional to the magnitude of the injected null energy.arXiv:1902.08449CERN-TH-2019-018oai:cds.cern.ch:26633552019-02-22
spellingShingle gr-qc
General Relativity and Cosmology
hep-th
Particle Physics - Theory
Brustein, Ram
Sherf, Yotam
Emission Channels from Perturbed Quantum Black Holes
title Emission Channels from Perturbed Quantum Black Holes
title_full Emission Channels from Perturbed Quantum Black Holes
title_fullStr Emission Channels from Perturbed Quantum Black Holes
title_full_unstemmed Emission Channels from Perturbed Quantum Black Holes
title_short Emission Channels from Perturbed Quantum Black Holes
title_sort emission channels from perturbed quantum black holes
topic gr-qc
General Relativity and Cosmology
hep-th
Particle Physics - Theory
url https://dx.doi.org/10.1103/PhysRevD.100.124005
http://cds.cern.ch/record/2663355
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