Abstract

We study the shadow of the Cardoso–Pani–Rico black hole for different values of the black hole spin $$a_*$$ , the deformation parameters $$\epsilon _3^t$$ and $$\epsilon _3^r$$ , and the viewing angle i. We find that the main impact of the deformation parameter $$\epsilon _3^t$$ is the change of the size of the shadow, while the deformation parameter $$\epsilon _3^r$$ affects the shape of its boundary. In general, it is impossible to test the Kerr metric, because the shadow of a Kerr black hole can be reproduced quite well by a black hole with non-vanishing $$\epsilon _3^t$$ or $$\epsilon _3^r$$ . Deviations from the Kerr geometry could be constrained in the presence of high quality data and in the favorable case of a black hole with high values of $$a_*$$ and i. However, the shadows of some black holes with non-vanishing $$\epsilon _3^r$$ present peculiar features and the possible detection of these shadows could unambiguously distinguish these objects from the standard Kerr black holes of general relativity.

Highlights

  • Astrophysical black hole (BH) candidates are compact objects in X-ray binaries with a mass M ≈ 5–20 M and supermassive bodies at the center of galaxies with a mass M ∼ 105 to 1010 M [1]

  • In the framework of standard physics, the spacetime geometry around these objects should be described by the Kerr solution of general relativity

  • The two main techniques to probe the spacetime geometry around BH candidates are the study of the thermal spectrum of thin disks [11,12,13] and the analysis of the iron Kα line [14,15]

Read more

Summary

Introduction

Astrophysical black hole (BH) candidates are compact objects in X-ray binaries with a mass M ≈ 5–20 M and supermassive bodies at the center of galaxies with a mass M ∼ 105 to 1010 M [1]. The two main techniques to probe the spacetime geometry around BH candidates are the study of the thermal spectrum of thin disks (continuum-fitting method) [11,12,13] and the analysis of the iron Kα line [14,15] These techniques are normally used to measure the spin parameter of BH candidates under the assumption of the Kerr background, but they can be generalized to non-Kerr metrics to constrain possible deviations from the Kerr solution [16,17,18,19,20,21,22,23,24].

Black hole shadow
CPR metric
Description of the shadow
Results
Concluding remarks
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call