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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2017-09-01
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Series: | Physics Letters B |
Online Access: | http://www.sciencedirect.com/science/article/pii/S0370269317305452 |
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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 |
work_keys_str_mv |
AT yvesbrihaye chargedblackholesinageneralizedscalartensorgravitymodel AT bettihartmann chargedblackholesinageneralizedscalartensorgravitymodel |
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1725919259468496896 |