Rotating charged AdS solutions in quadratic f(T) gravity

Abstract We present a class of asymptotically anti-de Sitter charged rotating black hole solutions in f(T) gravity in N-dimensions, where $$f(T)=T+\alpha T^{2}$$ f(T)=T+αT2 . These solutions are nontrivial extensions of the solutions presented in Lemos (Phys Lett B 353:46–51. arXiv:gr-qc/9404041, 19...

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Main Authors: A. M. Awad, G. G. L. Nashed, W. El Hanafy
Format: Article
Language:English
Published: SpringerOpen 2019-08-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-019-7182-9
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spelling doaj-87755522696048aca1b0dbc1ddd69a712020-11-25T02:59:36ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522019-08-017981810.1140/epjc/s10052-019-7182-9Rotating charged AdS solutions in quadratic f(T) gravityA. M. Awad0G. G. L. Nashed1W. El Hanafy2Department of Physics, School of Sciences and Engineering, American University in CairoCentre for Theoretical Physics, the British University in EgyptCentre for Theoretical Physics, the British University in EgyptAbstract We present a class of asymptotically anti-de Sitter charged rotating black hole solutions in f(T) gravity in N-dimensions, where $$f(T)=T+\alpha T^{2}$$ f(T)=T+αT2 . These solutions are nontrivial extensions of the solutions presented in Lemos (Phys Lett B 353:46–51. arXiv:gr-qc/9404041, 1995) and Awad (Class Quantum Gravity 20:2827–2834. arXiv:hep-th/0209238, 2003) in the context of general relativity. They are characterized by cylindrical, toroidal or flat horizons, depending on global identifications. The static charged black hole configurations obtained in Awad et al. (JHEP 07:136. arXiv:1706.01773, 2017) are recovered as special cases when the rotation parameters vanish. Similar to Awad et al. (JHEP 07:136. arXiv:1706.01773, 2017) the static black holes solutions have two different electric multipole terms in the potential with related moments. Furthermore, these solutions have milder singularities compared to their general relativity counterparts. Using the conserved charges expressions obtained in Ulhoa and Spaniol (Int J Mod Phys D 22:1350069. arXiv:1303.3144, 2013) and Maluf and Ulhoa (Gen Relativ Grav 41:1233–1247. arXiv:0810.1934, 2009) we calculate the total mass/energy and the angular momentum of these solutions.http://link.springer.com/article/10.1140/epjc/s10052-019-7182-9
collection DOAJ
language English
format Article
sources DOAJ
author A. M. Awad
G. G. L. Nashed
W. El Hanafy
spellingShingle A. M. Awad
G. G. L. Nashed
W. El Hanafy
Rotating charged AdS solutions in quadratic f(T) gravity
European Physical Journal C: Particles and Fields
author_facet A. M. Awad
G. G. L. Nashed
W. El Hanafy
author_sort A. M. Awad
title Rotating charged AdS solutions in quadratic f(T) gravity
title_short Rotating charged AdS solutions in quadratic f(T) gravity
title_full Rotating charged AdS solutions in quadratic f(T) gravity
title_fullStr Rotating charged AdS solutions in quadratic f(T) gravity
title_full_unstemmed Rotating charged AdS solutions in quadratic f(T) gravity
title_sort rotating charged ads solutions in quadratic f(t) gravity
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2019-08-01
description Abstract We present a class of asymptotically anti-de Sitter charged rotating black hole solutions in f(T) gravity in N-dimensions, where $$f(T)=T+\alpha T^{2}$$ f(T)=T+αT2 . These solutions are nontrivial extensions of the solutions presented in Lemos (Phys Lett B 353:46–51. arXiv:gr-qc/9404041, 1995) and Awad (Class Quantum Gravity 20:2827–2834. arXiv:hep-th/0209238, 2003) in the context of general relativity. They are characterized by cylindrical, toroidal or flat horizons, depending on global identifications. The static charged black hole configurations obtained in Awad et al. (JHEP 07:136. arXiv:1706.01773, 2017) are recovered as special cases when the rotation parameters vanish. Similar to Awad et al. (JHEP 07:136. arXiv:1706.01773, 2017) the static black holes solutions have two different electric multipole terms in the potential with related moments. Furthermore, these solutions have milder singularities compared to their general relativity counterparts. Using the conserved charges expressions obtained in Ulhoa and Spaniol (Int J Mod Phys D 22:1350069. arXiv:1303.3144, 2013) and Maluf and Ulhoa (Gen Relativ Grav 41:1233–1247. arXiv:0810.1934, 2009) we calculate the total mass/energy and the angular momentum of these solutions.
url http://link.springer.com/article/10.1140/epjc/s10052-019-7182-9
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