Quasi-normal modes of static spherically symmetric black holes in f(R) theory

Abstract We study the quasi-normal modes (QNMs) of static, spherically symmetric black holes in f(R) theories. We show how these modes in theories with non-trivial f(R) are fundamentally different from those in general relativity. In the special case of $$f(R) = \alpha R^2$$ f(R)=αR2 theories, it ha...

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Main Authors: Sayak Datta, Sukanta Bose
Format: Article
Language:English
Published: SpringerOpen 2020-01-01
Series:European Physical Journal C: Particles and Fields
Online Access:https://doi.org/10.1140/epjc/s10052-019-7546-1
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spelling doaj-3e3a0a845b504372a832d83bec6edced2021-01-10T12:53:26ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522020-01-0180111310.1140/epjc/s10052-019-7546-1Quasi-normal modes of static spherically symmetric black holes in f(R) theorySayak Datta0Sukanta Bose1Inter-University Centre for Astronomy and AstrophysicsInter-University Centre for Astronomy and AstrophysicsAbstract We study the quasi-normal modes (QNMs) of static, spherically symmetric black holes in f(R) theories. We show how these modes in theories with non-trivial f(R) are fundamentally different from those in general relativity. In the special case of $$f(R) = \alpha R^2$$ f(R)=αR2 theories, it has been recently argued that iso-spectrality between scalar and vector modes breaks down. Here, we show that such a break down is quite general across all f(R) theories, as long as they satisfy $$f''(0)/(1+f''(0)) \ne 0$$ f′′(0)/(1+f′′(0))≠0 , where a prime denotes derivative of the function with respect to its argument. We specifically discuss the origin of the breaking of isospectrality. We also show that along with this breaking the QNMs receive a correction that arises when $$f''(0)/(1+f'(0)) \ne 0$$ f′′(0)/(1+f′(0))≠0 owing to the inhomogeneous term that it introduces in the mode equation. We discuss how these differences affect the “ringdown” phase of binary black hole mergers and the possibility of constraining f(R) models with gravitational-wave observations. We also find that even though the iso-spectrality is broken in f(R) theories, in general, nevertheless in the corresponding scalar-tensor theories in the Einstein frame it is unbroken.https://doi.org/10.1140/epjc/s10052-019-7546-1
collection DOAJ
language English
format Article
sources DOAJ
author Sayak Datta
Sukanta Bose
spellingShingle Sayak Datta
Sukanta Bose
Quasi-normal modes of static spherically symmetric black holes in f(R) theory
European Physical Journal C: Particles and Fields
author_facet Sayak Datta
Sukanta Bose
author_sort Sayak Datta
title Quasi-normal modes of static spherically symmetric black holes in f(R) theory
title_short Quasi-normal modes of static spherically symmetric black holes in f(R) theory
title_full Quasi-normal modes of static spherically symmetric black holes in f(R) theory
title_fullStr Quasi-normal modes of static spherically symmetric black holes in f(R) theory
title_full_unstemmed Quasi-normal modes of static spherically symmetric black holes in f(R) theory
title_sort quasi-normal modes of static spherically symmetric black holes in f(r) theory
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2020-01-01
description Abstract We study the quasi-normal modes (QNMs) of static, spherically symmetric black holes in f(R) theories. We show how these modes in theories with non-trivial f(R) are fundamentally different from those in general relativity. In the special case of $$f(R) = \alpha R^2$$ f(R)=αR2 theories, it has been recently argued that iso-spectrality between scalar and vector modes breaks down. Here, we show that such a break down is quite general across all f(R) theories, as long as they satisfy $$f''(0)/(1+f''(0)) \ne 0$$ f′′(0)/(1+f′′(0))≠0 , where a prime denotes derivative of the function with respect to its argument. We specifically discuss the origin of the breaking of isospectrality. We also show that along with this breaking the QNMs receive a correction that arises when $$f''(0)/(1+f'(0)) \ne 0$$ f′′(0)/(1+f′(0))≠0 owing to the inhomogeneous term that it introduces in the mode equation. We discuss how these differences affect the “ringdown” phase of binary black hole mergers and the possibility of constraining f(R) models with gravitational-wave observations. We also find that even though the iso-spectrality is broken in f(R) theories, in general, nevertheless in the corresponding scalar-tensor theories in the Einstein frame it is unbroken.
url https://doi.org/10.1140/epjc/s10052-019-7546-1
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