Letter: Charged Black Hole Solutions in Einstein-Born-Infeld Gravity with a Cosmological Constant
By S. Fernando, Donald Krug. 2003
180 citations recorded by the source corpus.
We construct black hole solutions to Einstein-Born-Infeld gravity with a cosmological constant. Since an elliptic function appears in the solutions for the metric, we construct horizons numerically. The causal structure of these solutions differs drastically from their counterparts in Einstein-Maxwell gravity with a cosmological constant. The charged de-Sitter black holes can have up to three horizons and the charged anti-de Sitter black hole can have one or two depending on the parameters chosen.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/0714c972292f7232331767a685db02d8f6fc9a4e
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In Astronomy and Astrophysics
- Shao-Wen Wei
- Yu-Xiao Liu
- Robert B. Mann
- D. Kubizňák
- Blaise Goutéraux
- S. Gunasekaran
- E. Kiritsis
- C. Charmousis
In Nuclear and High Energy Physics
- Blaise Goutéraux
- Shao-Wen Wei
- Yu-Xiao Liu
- Robert B. Mann
- D. Kubizňák
- E. Kiritsis
- S. Gunasekaran
- C. Charmousis
Citations in the corpus
- Topology of black hole thermodynamics (2021, background): “Now let us turn to the charged Born-Infeld (BI) AdS black hole [20], where besides the conventional critical point, a novel one shall emerge.”
- Extended phase space thermodynamics for charged and rotating black holes and Born-Infeld vacuum polarization (2012, background): “4 Critical behaviour The thermodynamic behaviour of Born-Infeld-AdS black holes and the corresponding phase transitions were studied in the grand canonical ensemble in [25] and in canonical ensemble in [22].”
- Effective holographic theories for low-temperature condensed matter systems (2010, background): “ctions between charge carriers. Only in the dilute charge limit the action linearizes to a Maxwell action. In this context, the relevant charged solution is the AdS-DBI-RN solutions first discussed in [38, 39]. In many cases the important dynamics of strongly coupled theory is driven by a scalar lead”