Abstract

In this paper, we study the weak gravitational deflection of relativistic massive particles for a receiver and source at finite distance from the lens in stationary, axisymmetric and asymptotically flat spacetimes. For this purpose, we extend the generalized optical metric method to the generalized Jacobi metric method by using the Jacobi–Maupertuis Randers–Finsler metric. More specifically, we apply the Gauss–Bonnet theorem to the generalized Jacobi metric space and then obtain an expression for calculating the deflection angle, which is related to Gaussian curvature of generalized optical metric and geodesic curvature of particles orbit. In particular, the finite-distance correction to the deflection angle of signal with general velocity in the the Kerr black hole and Teo wormhole spacetimes are considered. Our results cover the previous work of the deflection angle of light, as well as the deflection angle of massive particles in the limit for the receiver and source at infinite distance from the lens object. In Kerr black hole spacetime, we compared the effects due to the black hole spin, the finite-distance of source or receiver, and the relativistic velocity in microlensings and lensing by galaxies. It is found in these cases, the effect of black hole spin is usually a few orders larger than that of the finite-distance and relativistic velocity, while the relative size of the latter two could vary according to the particle velocity, source or observer distance and other lensing parameters.

Highlights

  • One of the main quantities in the study of gravitational lensing (GL) is the deflection angle

  • In the weak field approximation, we have studied the gravitational deflection of massive particles for a receiver and source at finite distance from stationary, axisymmetric and asymptotically flat lens

  • We have extended the generalized optical metric method to generalized Jacobi metric method according to the Jacobi–Maupertuis Randers–Finsler (JMRF) metric

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Summary

Introduction

One of the main quantities in the study of GL is the deflection angle. Various approaches relying on the geodesics were built to calculate it. We shall extend the study to the finitedistance gravitational deflection of the relativistic massive particles in the weak field limits and compare the effects of spacetime spin, finite distance and subluminal velocity in the microlensing and supermassive BH lensing cases. To this end, we mainly consider the generalized optical metric method [47,48]. One of the present authors recently used JMRF and GB theorem to study the effect of the Lorentz symmetry breaking constant on the finite-distance deflection angle of massive particles in an asymptotically non-flat Kerr-like spacetime in bumblebee gravity model [55].

JMRF metric
Motion of massive particle on the equatorial plane
The GB theorem
The generalized Jacobi metric method
Kerr-JMRF metric
Gaussian curvature
Geodesic curvature
Deflection angle
Teo wormholes
Conclusion and discussions
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