Relativistic stars in f ( R ) gravity, and absence thereof
By Tsutomu Kobayashi, K. Maeda. 2008
144 citations recorded by the source corpus.
Several f(R) modified gravity models have been proposed which realize the correct cosmological evolution and satisfy solar system and laboratory tests. Although nonrelativistic stellar configurations can be constructed, we argue that relativistic stars cannot be present in such f(R) theories. This problem appears due to the dynamics of the effective scalar degree of freedom in the strong gravity regime. Our claim thus raises doubts on the viability of f(R) models.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics, Oceanography
View Paper: https://www.semanticscholar.org/paper/015875dedf8b5956a3b274eb7ea5b63ac501aaea
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
- Pedro G. Ferreira
- T. Clifton
- Stephen A. Appleby
- R. Battye
- C. Skordis
- Antonio Padilla
- A. Starobinsky
- S. Tsujikawa
In Nuclear and High Energy Physics
- T. Clifton
- Pedro G. Ferreira
- Stephen A. Appleby
- R. Battye
- C. Skordis
- Antonio Padilla
- A. Starobinsky
- S. Tsujikawa
In Oceanography
- Stephen A. Appleby
- Pedro G. Ferreira
- R. Battye
- C. Skordis
- T. Clifton
- Antonio Padilla
- A. Starobinsky
- S. Tsujikawa
Citations in the corpus
- Modified Gravity and Cosmology (2011, background): “The existence of this type of instability was rediscovered in [706], for relativistic stars.”
- Approaches to understanding cosmic acceleration (2009, unknown): “Finally, it was recently shown [169, 170] that even models of f (R) that satisfy all of the above conditions might still face problems in the strong gravity regime.”
- Curing singularities in cosmological evolution of F(R) gravity (2009, background): “1) might become important should the trace T of the matter energy-momentum tensor change sign and become positive inside neutron stars, as happens in idealized ρ = const solutions considered in [57, 59].”