Abstract

Nonsingular Ayon-Beato-Garcia (ABG) spherically symmetric static black hole (BH) with charge to mass ratio q=g/2m is metric solution of Born Infeld nonlinear Maxwell-Einstein theory. Central region of the BH behaves as (anti-)de Sitter for (|q|>1) |q|<1. In the case where |q|=1, the BH central region behaves as Minkowski flat metric. Nonlinear Electromagnetic (NEM) fields counterpart causes deviation of light geodesics and so light rays will be forced to move on from effective metric. In this paper we study weak and strong gravitational lensing of light rays by seeking effects of NEM fields counterpart on image locations and corresponding magnification. We set our calculations to experimentally observed Sgr A⁎ BH. In short we obtained the following: for large distances, the NEM counterpart is negligible and it reduces to linear Maxwell fields. The NEM field enlarges radius of the BH photon sphere linearly by raising |q|>1 but decreases by raising |q|≤1. Sign of deflection angle of bending light rays is changed in presence of NEM effects with respect to ones obtained in absence of NEM fields. Absolute value of deflection angle rises by increasing |q|→1. Image locations in weak deflection limit (WDL) decrease (increases) by raising 0<|q|<1 in presence (absence) of NEM fields. By raising the closest distance of the bending light rays image locations in WDL change from left (right) to right (left) in absence (presence) of NEM fields. In WDL, radius of Einstein rings and corresponding magnification centroid become larger (smaller) in presence (absence) of NEM fields. Angular separation called s between the innermost and outermost relativistic images increases (decreases) by increasing 0<|q|<1 in absence (presence) of NEM fields. Corresponding magnification r decreases (increases) by raising 0<|q|<1 in absence (presence) of NEM fields.

Highlights

  • Since the advent of Einstein’s general relativity theory, black holes and the singularity problem of curved space-time become challenging subjects in modern physics

  • Nonsingular metric solutions are obtained from the Einstein field equation [5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26]. In the latter situations the Einstein field equation is coupled with suitable Nonlinear Electromagnetic (NEM) fields for which the Ricci and the Kretschmann scalars become regular in whole space-time

  • Kraniotis studied gravitational lensing of KNdS and KNAdS black hole in [31], where closed form analytic solutions of the null geodesics and the gravitational lens equations have been obtained versus the Appell-Lauricella generalized hypergeometric functions and the elliptic functions of Weierstrass

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Summary

Introduction

Since the advent of Einstein’s general relativity theory, black holes and the singularity problem of curved space-time become challenging subjects in modern (quantum) physics. Kraniotis studied gravitational lensing of KNdS and KNAdS black hole in [31], where closed form analytic solutions of the null geodesics and the gravitational lens equations have been obtained versus the Appell-Lauricella generalized hypergeometric functions and the elliptic functions of Weierstrass. Strong deflection limits of light rays can distinguish gravitational lensing between naked singularity and regular black holes background [47]. We should point that the nonsingular charged black holes obtained from NEM models in curved space-time cause the photons to not move along null geodesics. In this work we study gravitational lensing of light rays moving on the ABG nonsingular black hole in presence of NEM fields counterparts.

ABG Space-Time
Effective Metric for Photon Trajectories
Deflection Angle
Images Locations
Concluding Remark
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