Null Geodesics and Strong Field Gravitational Lensing of Black Hole with Global Monopole
Hindawi Publishing Corporation
Advances in High Energy Physics
Volume 2015, Article ID 854264, 11 pages
http://dx.doi.org/10.1155/2015/854264
Research Article
Null Geodesics and Strong Field Gravitational Lensing of Black
Hole with Global Monopole
M. Sharif1 and Sehrish Iftikhar1,2
1
Department of Mathematics, University of the Punjab, Quaid-e-Azam Campus, Lahore 54590, Pakistan
Department of Mathematics, Lahore College for Women University, Lahore 54000, Pakistan
2
Correspondence should be addressed to M. Sharif;
Received 16 July 2015; Revised 6 August 2015; Accepted 17 August 2015
Academic Editor: Rong-Gen Cai
Copyright © 2015 M. Sharif and S. Iftikhar. This is an open access article distributed under the Creative Commons Attribution
License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly
cited. The publication of this article was funded by SCOAP3 .
We study two interesting features of a black hole with an ordinary as well as phantom global monopole. Firstly, we investigate null
geodesics which imply unstable orbital motion of particles for both cases. Secondly, we evaluate deflection angle in strong field
regime. We then find Einstein rings, magnifications, and observables of the relativistic images for supermassive black hole at the
center of galaxy NGC4486B. We also examine time delays for different galaxies and present our results numerically. It is found that
the deflection angle for ordinary/phantom global monopole is greater/smaller than that of Schwarzschild black hole. In strong field
limit, the remaining properties of these black holes are quite different from the Schwarzschild black hole.
1. Introduction
Geodesics are associated with the motion of free particles
traveling along their trajectories whose nature depends upon
the spacetime. There are two types of geodesics followed by
physical particles, that is, timelike and null (light-like), related
to the propagation of massive and massless particles. The
study of motion of massless particles such as photons is
important from both astrophysical and theoretical points of
view. It has been observed that light path is affected by gravity
which means that path of a photon through spacetime may
be bent by the gravitational field of a massive object such as
a star or black hole (BH). The dynamics of test particle not
only helps to understand geometrical structure of spacetime
but also explains high energy phenomenon occurring near
BH such as accretion disks where particles move in circular
orbits and formation of jets in which particles escape.
Chandrasekhar [1] was the pioneer to investigate geodesic
motion of a test particle around Schwarzschild, ReissnerNordström (RN), and Kerr BHs. Fernando et al. [2] constructed geodesic structure of static charged BHs of dilaton
gravity and studied orbital motion of test particles. Konoplya
[3] analyzed motion of both massless and massive particles
around magnetized BHs and concluded that tidal force has
considerable effect on the motion of test particles. Leiva et
al. [4] studied geodesics of the Schwarzschild BH in rainbow
gravity and found that geodesics remain unchanged under
the influence of semiclassical effects. Guha and Bhattacharya
[5] determined that the null geodesics of five-dimensional RN
anti-de Sitter BH have a unique fixed point and are terminating orbits. Pradhan [6] found conditions for the existence
of ISCO (inner most stable circular orbit), marginally bound
circular orbit, and null circular geodesics in equatorial plane
for Kerr-Newman-Taub-NUT BH.
Deflection of light in gravitational field around a massive
object is referred to as gravitational lensing and an object
causing deflection is called gravitational lens. Gravitational
lensing is a powerful tool in cosmology as well as in astrophysics to understand distribution of mass in the large scale
structures of the universe as well as cluster of galaxies and
halos. It provides a useful way to estimate Hubble parameter
and detection of dark mater, dark energy, exoplanet, gravitational waves, and so forth. This phenomenon is divided into
two regimes: weak and strong lensing. Weak gravitational
lensing produces weakly distorted images of the source. In
this case, the gravitational lens is not strong enough to form
2
multiple images and high magnification. It helps in the measurement of distribution of luminous as well as dark matter
in the universe. If the lens is massive enough and the source
and lens are highly aligned, then multiple images are formed
from the background source. This phenomenon is known
as strong gravitational lensing. The distortion and position
of such multiple images carry important information about
distribution of mass in faraway galaxies and background
sources at large distance.
The theory of gravitational lensing was initially developed in weak field approximation but this approach cannot
describe the phenomena like high bending of light rays and
formation of infinite series of images. This motivates studying
the strong gravitational lensing, which not only helps to
understand these phenomena but also explains the winding
of light rays multiple times around a massive object before
reaching to the observer. After the pioneer work of Darwin
[7], much work has been done in the context of gravitational
lensing in strong field [8–11]. Virbhadra and Ellis [12] studied
strong field gravitational lensing of Schwarzschild BH and
found a sequence of relativistic images on both sides of optical
axis due to large deflection of light near the photon sphere.
Frittelli et al. [13] proposed an exact thin-lens equation whose
accuracy was shown in the strong field. Bozza [14] developed
a useful technique for spherically symmetric BHs in strong
field by expanding the deflection angle near the photon
sphere.
The image detection for low mass BHs is difficult but the
supermassive BHs such as Sgr 𝐴∗ are an interesting example
of deflection of light in strong field [15, 16]. Ding et al. [17]
considered noncommutative BH as gravitational lens and
found effect of noncommutative parameter similar to charge
by comparing with RN BH. Deng [18] studied gravitational
lensing of magnetically charged RN BH pierced by a cosmic
string in strong field and found increase in the deflection
angle. Sahu et al. [19] showed that strong gravitational lensing
can be used to distinguish BHs from naked singularities. Wei
et al. [20] explored strong lensing of Kerr-Taub-NUT BH and
found significant effect of NUT charge. Different authors [21–
29] studied gravitational lensing of many other astrophysical
spacetimes in strong field limit.
The fact that the universe is in the phase of accelerating
expansion is a major turning point in cosmology which indicates the existence of dark energy supported by several observational evidences. Dark energy is an elusive force having
large negative pressure. To understand its exact nature, several dynamical mode (...truncated)