Cusp singularities in f(R) gravity: pros and cons
arXiv:1506.06713 · doi:10.1088/1475-7516/2015/10/022
Abstract
We investigate cusp singularities in f(R) gravity, especially for Starobinsky and Hu-Sawicki dark energy models. We illustrate that, by using double-null numerical simulations, a cusp singularity can be triggered by gravitational collapses. This singularity can be cured by adding a quadratic term, but this causes a Ricci scalar bump that can be observed by an observer outside the event horizon. Comparing with cosmological parameters, it seems that it would be difficult to see super-Planckian effects by astrophysical experiments. On the other hand, at once there exists a cusp singularity, it can be a mechanism to realize a horizon scale curvature singularity that can be interpreted by a firewall.
19 pages, 11 figures
References in corpus (10)
- Models of f(R) Cosmic Acceleration that Evade Solar-System Tests
- Disappearing cosmological constant in f(R) gravity
- Constructing a counterexample to the black hole complementarity
- Generalized Uncertainty Principle: Implications for Black Hole Complementarity
- Thin-shell bubbles and information loss problem in anti de Sitter background
- Generation of a bubble universe using a negative energy bath
- Dynamics of magnetic shells and information loss problem
- Charged black holes in string-inspired gravity: I. Causal structures and responses of the Brans-Dicke field
- Charged black holes in string-inspired gravity: II. Mass inflation and dependence on parameters and potentials
- Curvature Singularity in f(R) Theories of Gravity
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