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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2019-08-01
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Series: | European Physical Journal C: Particles and Fields |
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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 |
work_keys_str_mv |
AT amawad rotatingchargedadssolutionsinquadraticftgravity AT gglnashed rotatingchargedadssolutionsinquadraticftgravity AT welhanafy rotatingchargedadssolutionsinquadraticftgravity |
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1724701390070087680 |