Thermal Hawking radiation of black hole with supertranslation field

Abstract Using the analytical solution for the Schwarzschild metric containing supertranslation field, we consider two main ingredients of calculation of the thermal Hawking black hole radiation: solution for eigenmodes of the d’Alambertian and solution of the geodesic equations for null geodesics....

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Main Author: Mikhail Z. Iofa
Format: Article
Language:English
Published: SpringerOpen 2018-01-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP01(2018)137
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spelling doaj-0b6888d67cf643ff82d65f6b5e6ef85a2020-11-25T01:38:53ZengSpringerOpenJournal of High Energy Physics1029-84792018-01-012018111510.1007/JHEP01(2018)137Thermal Hawking radiation of black hole with supertranslation fieldMikhail Z. Iofa0Skobeltsyn Institute of Nuclear Physics, Moscow State UniversityAbstract Using the analytical solution for the Schwarzschild metric containing supertranslation field, we consider two main ingredients of calculation of the thermal Hawking black hole radiation: solution for eigenmodes of the d’Alambertian and solution of the geodesic equations for null geodesics. For calculation of Hawking radiation it is essential to determine the behavior of both the eigenmodes and geodesics in the vicinity of horizon. The equation for the eigenmodes is solved, first, perturbatively in the ratio O(C)/M of the supertranslation field to the mass of black hole, and, next, non-perturbatively in the near- horizon region. It is shown that in any order of perturbation theory solution for the eigenmodes in the metric containing supertranslation field differs from solution in the pure Schwarzschild metric by terms of order L 1/2 = (1 − 2M/r)1/2. In the non-perturbative approach, solution for the eigenmodes differs from solution in the Schwarzschild metric by terms of order L 1/2 which vanish on horizon. Using the simplified form of geodesic equations in vicinity of horizon, it is shown that in vicinity of horizon the null geodesics have the same behavior as in the Schwarzschild metric. As a result, the density matrices of thermal radiation in both cases are the same.http://link.springer.com/article/10.1007/JHEP01(2018)137Black HolesModels of Quantum Gravity
collection DOAJ
language English
format Article
sources DOAJ
author Mikhail Z. Iofa
spellingShingle Mikhail Z. Iofa
Thermal Hawking radiation of black hole with supertranslation field
Journal of High Energy Physics
Black Holes
Models of Quantum Gravity
author_facet Mikhail Z. Iofa
author_sort Mikhail Z. Iofa
title Thermal Hawking radiation of black hole with supertranslation field
title_short Thermal Hawking radiation of black hole with supertranslation field
title_full Thermal Hawking radiation of black hole with supertranslation field
title_fullStr Thermal Hawking radiation of black hole with supertranslation field
title_full_unstemmed Thermal Hawking radiation of black hole with supertranslation field
title_sort thermal hawking radiation of black hole with supertranslation field
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2018-01-01
description Abstract Using the analytical solution for the Schwarzschild metric containing supertranslation field, we consider two main ingredients of calculation of the thermal Hawking black hole radiation: solution for eigenmodes of the d’Alambertian and solution of the geodesic equations for null geodesics. For calculation of Hawking radiation it is essential to determine the behavior of both the eigenmodes and geodesics in the vicinity of horizon. The equation for the eigenmodes is solved, first, perturbatively in the ratio O(C)/M of the supertranslation field to the mass of black hole, and, next, non-perturbatively in the near- horizon region. It is shown that in any order of perturbation theory solution for the eigenmodes in the metric containing supertranslation field differs from solution in the pure Schwarzschild metric by terms of order L 1/2 = (1 − 2M/r)1/2. In the non-perturbative approach, solution for the eigenmodes differs from solution in the Schwarzschild metric by terms of order L 1/2 which vanish on horizon. Using the simplified form of geodesic equations in vicinity of horizon, it is shown that in vicinity of horizon the null geodesics have the same behavior as in the Schwarzschild metric. As a result, the density matrices of thermal radiation in both cases are the same.
topic Black Holes
Models of Quantum Gravity
url http://link.springer.com/article/10.1007/JHEP01(2018)137
work_keys_str_mv AT mikhailziofa thermalhawkingradiationofblackholewithsupertranslationfield
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