General Relativity solutions in modified gravity

Recent gravitational wave observations of binary black hole mergers and a binary neutron star merger by LIGO and Virgo Collaborations associated with its optical counterpart constrain deviation from General Relativity (GR) both on strong-field regime and cosmological scales with high accuracy, and f...

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Main Authors: Hayato Motohashi, Masato Minamitsuji
Format: Article
Language:English
Published: Elsevier 2018-06-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269318303320
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spelling doaj-56e74f0d4c6a4fe0b97552c5e2040b0e2020-11-24T23:13:11ZengElsevierPhysics Letters B0370-26932018-06-01781728734General Relativity solutions in modified gravityHayato Motohashi0Masato Minamitsuji1Center for Gravitational Physics, Yukawa Institute for Theoretical Physics, Kyoto University, Kyoto 606-8502, Japan; Corresponding author.Centro de Astrofísica e Gravitação – CENTRA, Departamento de Física, Instituto Superior Técnico – IST, Universidade de Lisboa – UL, Av. Rovisco Pais 1, 1049-001 Lisboa, PortugalRecent gravitational wave observations of binary black hole mergers and a binary neutron star merger by LIGO and Virgo Collaborations associated with its optical counterpart constrain deviation from General Relativity (GR) both on strong-field regime and cosmological scales with high accuracy, and further strong constraints are expected by near-future observations. Thus, it is important to identify theories of modified gravity that intrinsically possess the same solutions as in GR among a huge number of theories. We clarify the three conditions for theories of modified gravity to allow GR solutions, i.e., solutions with the metric satisfying the Einstein equations in GR and the constant profile of the scalar fields. Our analysis is quite general, as it applies a wide class of single-/multi-field scalar–tensor theories of modified gravity in the presence of matter component, and any spacetime geometry including cosmological background as well as spacetime around black hole and neutron star, for the latter of which these conditions provide a necessary condition for no-hair theorem. The three conditions will be useful for further constraints on modified gravity theories as they classify general theories of modified gravity into three classes, each of which possesses i) unique GR solutions (i.e., no-hair cases), ii) only hairy solutions (except the cases that GR solutions are realized by cancellation between singular coupling functions in the Euler–Lagrange equations), and iii) both GR and hairy solutions, for the last of which one of the two solutions may be selected dynamically. Keywords: Black hole, Modified gravityhttp://www.sciencedirect.com/science/article/pii/S0370269318303320
collection DOAJ
language English
format Article
sources DOAJ
author Hayato Motohashi
Masato Minamitsuji
spellingShingle Hayato Motohashi
Masato Minamitsuji
General Relativity solutions in modified gravity
Physics Letters B
author_facet Hayato Motohashi
Masato Minamitsuji
author_sort Hayato Motohashi
title General Relativity solutions in modified gravity
title_short General Relativity solutions in modified gravity
title_full General Relativity solutions in modified gravity
title_fullStr General Relativity solutions in modified gravity
title_full_unstemmed General Relativity solutions in modified gravity
title_sort general relativity solutions in modified gravity
publisher Elsevier
series Physics Letters B
issn 0370-2693
publishDate 2018-06-01
description Recent gravitational wave observations of binary black hole mergers and a binary neutron star merger by LIGO and Virgo Collaborations associated with its optical counterpart constrain deviation from General Relativity (GR) both on strong-field regime and cosmological scales with high accuracy, and further strong constraints are expected by near-future observations. Thus, it is important to identify theories of modified gravity that intrinsically possess the same solutions as in GR among a huge number of theories. We clarify the three conditions for theories of modified gravity to allow GR solutions, i.e., solutions with the metric satisfying the Einstein equations in GR and the constant profile of the scalar fields. Our analysis is quite general, as it applies a wide class of single-/multi-field scalar–tensor theories of modified gravity in the presence of matter component, and any spacetime geometry including cosmological background as well as spacetime around black hole and neutron star, for the latter of which these conditions provide a necessary condition for no-hair theorem. The three conditions will be useful for further constraints on modified gravity theories as they classify general theories of modified gravity into three classes, each of which possesses i) unique GR solutions (i.e., no-hair cases), ii) only hairy solutions (except the cases that GR solutions are realized by cancellation between singular coupling functions in the Euler–Lagrange equations), and iii) both GR and hairy solutions, for the last of which one of the two solutions may be selected dynamically. Keywords: Black hole, Modified gravity
url http://www.sciencedirect.com/science/article/pii/S0370269318303320
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