Greybody factor for black holes in dRGT massive gravity

Abstract In general relativity, greybody factor is a quantity related to the quantum nature of a black hole. A high value of greybody factor indicates a high probability that Hawking radiation can reach infinity. Although general relativity is correct and has been successful in describing many pheno...

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Main Authors: Petarpa Boonserm, Tritos Ngampitipan, Pitayuth Wongjun
Format: Article
Language:English
Published: SpringerOpen 2018-06-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-018-5975-x
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spelling doaj-b3483516bbdc48ffa6de65005367f2042020-11-24T21:14:46ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522018-06-0178611210.1140/epjc/s10052-018-5975-xGreybody factor for black holes in dRGT massive gravityPetarpa Boonserm0Tritos Ngampitipan1Pitayuth Wongjun2Department of Mathematics and Computer Science, Faculty of Science, Chulalongkorn UniversityFaculty of Science, Chandrakasem Rajabhat UniversityThe Institute for Fundamental Study, Naresuan UniversityAbstract In general relativity, greybody factor is a quantity related to the quantum nature of a black hole. A high value of greybody factor indicates a high probability that Hawking radiation can reach infinity. Although general relativity is correct and has been successful in describing many phenomena, there are some questions that general relativity cannot answer. Therefore, general relativity is often modified to attain answers. One of the modifications is the ‘massive gravity’. The viable model of the massive gravity theory belongs to de Rham, Gabadadze and Tolley (dRGT). In this paper, we calculate the gravitational potential for the de Sitter black hole and for the dRGT black hole. We also derive the rigorous bound on the greybody factor for the de Sitter black hole and the dRGT black hole. It is found that the structure of potentials determines how much the rigorous bound on the greybody factor should be. That is, the higher the potential, the lesser the bound on the greybody factor will be. Moreover, we compare the greybody factor derived from the rigorous bound with the greybody factor derived from the matching technique. The result shows that the rigorous bound is a true lower bound because it is less than the greybody factor obtained from the matching technique.http://link.springer.com/article/10.1140/epjc/s10052-018-5975-x
collection DOAJ
language English
format Article
sources DOAJ
author Petarpa Boonserm
Tritos Ngampitipan
Pitayuth Wongjun
spellingShingle Petarpa Boonserm
Tritos Ngampitipan
Pitayuth Wongjun
Greybody factor for black holes in dRGT massive gravity
European Physical Journal C: Particles and Fields
author_facet Petarpa Boonserm
Tritos Ngampitipan
Pitayuth Wongjun
author_sort Petarpa Boonserm
title Greybody factor for black holes in dRGT massive gravity
title_short Greybody factor for black holes in dRGT massive gravity
title_full Greybody factor for black holes in dRGT massive gravity
title_fullStr Greybody factor for black holes in dRGT massive gravity
title_full_unstemmed Greybody factor for black holes in dRGT massive gravity
title_sort greybody factor for black holes in drgt massive gravity
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2018-06-01
description Abstract In general relativity, greybody factor is a quantity related to the quantum nature of a black hole. A high value of greybody factor indicates a high probability that Hawking radiation can reach infinity. Although general relativity is correct and has been successful in describing many phenomena, there are some questions that general relativity cannot answer. Therefore, general relativity is often modified to attain answers. One of the modifications is the ‘massive gravity’. The viable model of the massive gravity theory belongs to de Rham, Gabadadze and Tolley (dRGT). In this paper, we calculate the gravitational potential for the de Sitter black hole and for the dRGT black hole. We also derive the rigorous bound on the greybody factor for the de Sitter black hole and the dRGT black hole. It is found that the structure of potentials determines how much the rigorous bound on the greybody factor should be. That is, the higher the potential, the lesser the bound on the greybody factor will be. Moreover, we compare the greybody factor derived from the rigorous bound with the greybody factor derived from the matching technique. The result shows that the rigorous bound is a true lower bound because it is less than the greybody factor obtained from the matching technique.
url http://link.springer.com/article/10.1140/epjc/s10052-018-5975-x
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