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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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 |
work_keys_str_mv |
AT hayatomotohashi generalrelativitysolutionsinmodifiedgravity AT masatominamitsuji generalrelativitysolutionsinmodifiedgravity |
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