Charged black holes in a generalized scalar–tensor gravity model

We study 4-dimensional charged and static black holes in a generalized scalar–tensor gravity model, in which a shift symmetry for the scalar field exists. For vanishing scalar field the solution corresponds to the Reissner–Nordström (RN) solution, while solutions of the full scalar-gravity model hav...

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Main Authors: Yves Brihaye, Betti Hartmann
Format: Article
Language:English
Published: Elsevier 2017-09-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269317305452
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spelling doaj-21c9c295a84445a0b3bd1062dade40ba2020-11-24T21:42:02ZengElsevierPhysics Letters B0370-26931873-24452017-09-01772C47648210.1016/j.physletb.2017.06.069Charged black holes in a generalized scalar–tensor gravity modelYves Brihaye0Betti Hartmann1Physique Théorique e Mathématiques, Université de Mons, Place du Parc, 7000 Mons, BelgiumInstituto de Física de São Carlos (IFSC), Universidade de São Paulo (USP), CP 369, 13560-970, São Carlos, SP, BrazilWe study 4-dimensional charged and static black holes in a generalized scalar–tensor gravity model, in which a shift symmetry for the scalar field exists. For vanishing scalar field the solution corresponds to the Reissner–Nordström (RN) solution, while solutions of the full scalar-gravity model have to be constructed numerically. We demonstrate that these black holes support Galilean scalar hair up to a maximal value of the scalar–tensor coupling that depends on the value of the charge and can be up to roughly twice as large as that for uncharged solutions. The Hawking temperature TH of the hairy black holes at maximal scalar–tensor coupling decreases continuously with the increase of the charge and reaches TH=0 for the highest possible charge that these solutions can carry. However, in this limit, the scalar–tensor coupling needs to vanish. The limiting solution hence corresponds to the extremal RN solution, which does not support regular Galilean scalar hair due to its AdS2×S2 near-horizon geometry.http://www.sciencedirect.com/science/article/pii/S0370269317305452
collection DOAJ
language English
format Article
sources DOAJ
author Yves Brihaye
Betti Hartmann
spellingShingle Yves Brihaye
Betti Hartmann
Charged black holes in a generalized scalar–tensor gravity model
Physics Letters B
author_facet Yves Brihaye
Betti Hartmann
author_sort Yves Brihaye
title Charged black holes in a generalized scalar–tensor gravity model
title_short Charged black holes in a generalized scalar–tensor gravity model
title_full Charged black holes in a generalized scalar–tensor gravity model
title_fullStr Charged black holes in a generalized scalar–tensor gravity model
title_full_unstemmed Charged black holes in a generalized scalar–tensor gravity model
title_sort charged black holes in a generalized scalar–tensor gravity model
publisher Elsevier
series Physics Letters B
issn 0370-2693
1873-2445
publishDate 2017-09-01
description We study 4-dimensional charged and static black holes in a generalized scalar–tensor gravity model, in which a shift symmetry for the scalar field exists. For vanishing scalar field the solution corresponds to the Reissner–Nordström (RN) solution, while solutions of the full scalar-gravity model have to be constructed numerically. We demonstrate that these black holes support Galilean scalar hair up to a maximal value of the scalar–tensor coupling that depends on the value of the charge and can be up to roughly twice as large as that for uncharged solutions. The Hawking temperature TH of the hairy black holes at maximal scalar–tensor coupling decreases continuously with the increase of the charge and reaches TH=0 for the highest possible charge that these solutions can carry. However, in this limit, the scalar–tensor coupling needs to vanish. The limiting solution hence corresponds to the extremal RN solution, which does not support regular Galilean scalar hair due to its AdS2×S2 near-horizon geometry.
url http://www.sciencedirect.com/science/article/pii/S0370269317305452
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