Quasinormal modes as a distinguisher between general relativity and f(R) gravity: charged black-holes

Abstract The ring-down phase of black-hole perturbations is governed by the quasi-normal modes (QNM) and offer valuable insight into the nature of the objects emitting them, raising an interesting question: whether QNMs can be used to distinguish between theories of gravity? We construct a consisten...

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Main Authors: Soham Bhattacharyya, S. Shankaranarayanan
Format: Article
Language:English
Published: SpringerOpen 2018-09-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-018-6222-1
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spelling doaj-e2fcb13d705f4ff6a372e7392859ddd02020-11-24T21:26:23ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522018-09-0178911410.1140/epjc/s10052-018-6222-1Quasinormal modes as a distinguisher between general relativity and f(R) gravity: charged black-holesSoham Bhattacharyya0S. Shankaranarayanan1School of Physics, Indian Institute of Science Education and Research Thiruvananthapuram (IISER-TVM)Department of Physics, Indian Institute of Technology BombayAbstract The ring-down phase of black-hole perturbations is governed by the quasi-normal modes (QNM) and offer valuable insight into the nature of the objects emitting them, raising an interesting question: whether QNMs can be used to distinguish between theories of gravity? We construct a consistency test of general relativity (GR) which enables one to distinguish between general relativity and a specific class of modified theories of gravity: f(R). We show that an energetic inequality between scalar (polar) and vector (axial) type gravitational perturbations will exist for Reissner–Nördstrom solutions of GR - using which we find a novel method of determining the charge of a non-spinning black hole in GR. We then show that there will be a further energetic difference for charged black holes in f(R). Finally, we utilize this extra difference to construct a parameter to quantify deviation from GR.http://link.springer.com/article/10.1140/epjc/s10052-018-6222-1
collection DOAJ
language English
format Article
sources DOAJ
author Soham Bhattacharyya
S. Shankaranarayanan
spellingShingle Soham Bhattacharyya
S. Shankaranarayanan
Quasinormal modes as a distinguisher between general relativity and f(R) gravity: charged black-holes
European Physical Journal C: Particles and Fields
author_facet Soham Bhattacharyya
S. Shankaranarayanan
author_sort Soham Bhattacharyya
title Quasinormal modes as a distinguisher between general relativity and f(R) gravity: charged black-holes
title_short Quasinormal modes as a distinguisher between general relativity and f(R) gravity: charged black-holes
title_full Quasinormal modes as a distinguisher between general relativity and f(R) gravity: charged black-holes
title_fullStr Quasinormal modes as a distinguisher between general relativity and f(R) gravity: charged black-holes
title_full_unstemmed Quasinormal modes as a distinguisher between general relativity and f(R) gravity: charged black-holes
title_sort quasinormal modes as a distinguisher between general relativity and f(r) gravity: charged black-holes
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2018-09-01
description Abstract The ring-down phase of black-hole perturbations is governed by the quasi-normal modes (QNM) and offer valuable insight into the nature of the objects emitting them, raising an interesting question: whether QNMs can be used to distinguish between theories of gravity? We construct a consistency test of general relativity (GR) which enables one to distinguish between general relativity and a specific class of modified theories of gravity: f(R). We show that an energetic inequality between scalar (polar) and vector (axial) type gravitational perturbations will exist for Reissner–Nördstrom solutions of GR - using which we find a novel method of determining the charge of a non-spinning black hole in GR. We then show that there will be a further energetic difference for charged black holes in f(R). Finally, we utilize this extra difference to construct a parameter to quantify deviation from GR.
url http://link.springer.com/article/10.1140/epjc/s10052-018-6222-1
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