Study of charged gravastar model in gravity
arXiv:2403.01094 · doi:10.1016/j.aop.2024.169636
Abstract
In recent days gravastar has been a very lucrative alternative to black holes, as it does not suffer from the singularity problem as well and it is based on sound physical grounds. Modified Symmetric teleparallel equivalent of gravity also has seen quite a few successes in recent years both in cosmology as well as in astrophysical objects like black holes and wormholes. In this paper, we have considered the charged gravastar in formulation and have solved it fully analytically and found various physical characteristics like energy density, entropy and EoS for the gravastar. We have used the Israel junction condition to make some phenomenological predictions regarding the potential of the thin shell around the gravastar. We have also studied the deflection of the angle caused by the gravastar. Finally, we conclude by noting how future radio telescopes could detect the gravastar shadow and how can one distinguish it from the black hole event horizon.
Annals of {physics published version
References in corpus (6)
- First M87 Event Horizon Telescope Results. I. The Shadow of the Supermassive Black Hole
- Testing the general relativistic ''no-hair'' theorems using the galactic center black hole SgrA*
- Tidal deformability and I-Love-Q relations for gravastars with polytropic thin shells
- Where are all the gravastars? Limits upon the gravastar model from accreting black holes
- Late-time acceleration in gravity: Analysis and constraints in an anisotropic background
- Stable and self consistent charged gravastar model within the framework of gravity
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- A note on the junction conditions in f(Q)-gravity