Abstract

With the advent of gravitational wave astronomy and first pictures of the “shadow” of the central black hole of our milky way, theoretical analyses of black holes (and compact objects mimicking them sufficiently closely) have become more important than ever. The near future promises more and more detailed information about the observable black holes and black hole candidates. This information could lead to important advances on constraints on or evidence for modifications of general relativity. More precisely, we are studying the influence of weak teleparallel perturbations on general relativistic vacuum spacetime geometries in spherical symmetry. We find the most general family of spherically symmetric, static vacuum solutions of the theory, which are candidates for describing teleparallel black holes which emerge as perturbations to the Schwarzschild black hole. We compare our findings to results on black hole or static, spherically symmetric solutions in teleparallel gravity discussed in the literature, by comparing the predictions for classical observables such as the photon sphere, the perihelion shift, the light deflection, and the Shapiro delay. On the basis of these observables, we demonstrate that among the solutions we found, there exist spacetime geometries that lead to much weaker bounds on teleparallel gravity than those found earlier. Finally, we move on to a discussion of how the teleparallel perturbations influence the Hawking evaporation in these spacetimes.

Highlights

  • When studying isolated, astrophysical objects like stars, neutron stars, or black holes, the real physical system requires a high degree of sophistication and model building that can usually only be dealt with numerically

  • In this work we will construct a new family of static, asymptotically flat spherically symmetric vacuum solutions to weak f (T)-gravity, which can be interpreted as teleparallel perturbations of the Schwarzschild black hole of general relativity

  • In this article we have identified the general black hole family of spherically symmetric, static vacuum solutions of weak f (T)-gravity in Equations (25) and (26)

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Summary

Introduction

Astrophysical objects like stars, neutron stars, or black holes, the real physical system requires a high degree of sophistication and model building that can usually only be dealt with numerically. In this work we will construct a new family of static, asymptotically flat (which in the context of teleparallel gravity means that the metric obtained from the tetrad defines an asymptotically flat pseudo-Riemannian geometry) spherically symmetric vacuum solutions to weak f (T)-gravity, which can be interpreted as teleparallel perturbations of the Schwarzschild black hole of general relativity. They contain the solutions found in [45,46] for a very specific value of the determinant of the metric at the horizon (unlike in the GR case of the Schwarzschild geometry, this determinant at the horizon is not −r2 sin θ) These findings demonstrate that there is no unique spherically symmetric, asymptotically flat, static vacuum solution in this theory: the Birkhoff theorem does not hold. Afterwards we identify all black hole solutions of weak T-gravity

The General Static Spherically Symmetric Solution
The Black Hole Solution
The General Relativistic Perspective—Energy Conditions
Classical and Semi-Classical Properties
Particle Propagation Effects
The Event Horizon
Surface Gravity and Black Hole Temperature
Sparsity
Conclusions
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