THERMODYNAMICS OF COSMOLOGICAL HORIZONS IN F (T) GRAVITY
By Kazuharu Bamba, Chao-Qiang Geng. 2011
153 citations recorded by the source corpus.
We explore thermodynamics of the apparent horizon in f(T) gravity with both equilibrium and non-equilibrium descriptions. We find the same dual equilibrium/non-equilibrium formulation for f(T) as for f(R) gravity. In particular, we show that the second law of thermodynamics can be satisfied for the universe with the same temperature outside and inside the apparent horizon.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/84e5c11392341f30285858014fd38c7a2db7a205
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Astronomy and Astrophysics
- M. De Laurentis
- Emmanuel N. Saridakis
- Salvatore Capozziello
- Yi-Fu Cai
- A. Abdolmaleki
- K. Karami
- Sergei D. Odintsov
- Shin'ichi Nojiri
In Nuclear and High Energy Physics
- M. De Laurentis
- Salvatore Capozziello
- Yi-Fu Cai
- Emmanuel N. Saridakis
- A. Abdolmaleki
- K. Karami
- Sergei D. Odintsov
- Shin'ichi Nojiri
Citations in the corpus
- Solar system constraints on f(T) gravity (2012, unknown): “(2011a), Ferraro & Fiorini (2011a), Wei et al. (2011b), Capozziello et al. (2011), Wu & Yu (2011b), Bamba & Geng (2011), Geng et al. (2011), Wei (2012), Geng et al (2012), Wu & Geng (2011), Bohmer et al. (2012), Karami & Abdolmaleki (2011), Atazadeh& Darabi (2012), Farajollahi et al. (2012), Yang…”
- Generalized second law of thermodynamics in f(T) gravity (2012, background): “Besides examining the validity of the thermodynamical interpretation of gravity by expressing the gravitational field equations into the first law of thermodynamics in different spacetimes, it is also of great interest to investigate the validity of the generalized second law (GSL) of thermodynamics”
- f(T) teleparallel gravity and cosmology (2015, background): “In summary, in order for the second law of thermodynamics to be valid, from (366) we extract the requirement [282] Y ≡ − ( 4HT + Ṫ ) = 12H ( 2H(2) + Ḣ ) ≥ 0.”