Light Bending Under General Relativity: A Study of Pulsar–Black Hole Binaries [HBNI Th277]

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dc.contributor.author Jyotijwal Debnath
dc.date.accessioned 2026-04-02T08:28:09Z
dc.date.available 2026-04-02T08:28:09Z
dc.date.issued 2026
dc.date.submitted 2026-01-07
dc.identifier.uri https://dspace.imsc.res.in/xmlui/handle/123456789/917
dc.description.abstract Pulsars are precise cosmic clocks whose timing signals enable stringent tests of general relativity. In binary systems, several propagation delays arise due to orbital motion and gravitational effects, including the Romer delay, Shapiro delay, Einstein delay, and an additional geometric delay caused by gravitational light bending.Light bending also modifies the observed rotational phase of the pulsar, producing longitudinal and latitudinal bending delays and potentially distorting the pulse profile. While earlier studies treated these effects using weak-field approximations, this work adopts a more general approach and refers to them collectively as bending delays.These delays are most significant near superior conjunction, when the pulsar is behind its companion relative to the observer. This study investigates bending effects in pulsar–black hole binaries using realistic system parameters. The results are consistent with existing approximate models, except away from superior conjunction where such approximations fail.Both non-rotating (Schwarzschild) and rotating (Kerr) black hole companions are analyzed. The spin of the black hole has negligible impact on overall bending delays, although small frame-dragging contributions (longitudinal and latitudinal FD delays) of nanosecond order are identified, with discontinuities at specific orbital phases.The dependence of bending delays on parameters such as eccentricity, orbital period, and companion mass is also examined. Pulse profile analysis shows that for stellar-mass black holes, the signal strength increases without significant shape change, especially near superior conjunction.In the strong-field case of supermassive black hole companions, both the shape and strength of the pulse profile change significantly due to the Einstein ring exceeding the beam size, consistent with gravitational lensing theory.Overall, this work highlights the importance of light bending effects in pulsar–black hole binaries for precision timing and strong-field tests of gravity. en_US
dc.description.tableofcontents Summary List of Figures List of Tables 1Introduction 1.1Overview and structure of the thesis 1.2Emission Mechanism of Pulsars 1.2.1Rotation-Powered Emission 1.2.2Curvature Radiation and Synchrotron Radiation From Pulsars Pulsar emission geometry 1.3.1The Lighthouse Model of Pulsar Emission 1.3.2Pulsar beam model Use of the Models Described in This Section Binary Pulsars, Bending Delays, and Pulsar Timing Formation of Binary Pulsars 2.1.1Recycled Pulsars 2.2Co-ordinate geometry relevant for binary pulsars 2.3Modelling the evolution of the orbit and spins 2.4Pulsar Timing 2.4.1Effect of the Solar System’s Gravitational Field 2.4.2Effect of the Interstellar Medium (ISM) 2.4.3Effect of companion’s gravitational field for a binary pulsar Bending Delay 3 A Study of the Light Bending Phenomenon: Pulsar in a Binary With a Schwarzschild Black Hole 3.1General Relativistic Formalism for Bending Delay 3.2Distortion of the beam and the pulse shape 3.3Numerical study of bending delay 3.4 4 Previous Studies on Bending Delay in Binary Pulsars 3.3.1Features of the bending delay: demonstration for the Double Pulsar 3.3.2Bending delay in pulsar−black hole binaries 3.3.3Distortion of the beam and the change in the pulse profile due to the bending Conclusions Exploring the Light Bending Phenomenon for a Pulsar in a Binary With aRotating Black Hole The effect of the spin of the companion on the bending delay: A full general relativistic study Impact of Companion Spin on Bending Delay 4.2Numerical study 4.3Exploring the bending delay when the companion is a supermassive black hole 4.4 5Conclusion A Rotational Transformations A.1 Conversion from the I-frame to b-frame A.1.1 Conversion from the I′ -frame to the s-frame A.1.2 Conversion from the s-frame to b-frame A.1.3 Conversion from I-frame to b-frame A.2 Conversion from the L-frame to T-frame A.3 Conversion from the T-frame to b-frame A.4 Conversion from the m-frame to I-frame A.5 Conversion relation between the bh′ -frame and the s-frame A.6 Conversion between the bh′ -frame and the b-frame A.7 Conversion between bh′ -frame and T-frame 152B Details of Calculations for the Schwarzchild Spacetime B.1 Equations of motion of light rays in the Schwarzchild spacetime B.2 Geodesics in the Schwarzchild space time B.2.1Impact parameter D B.2.2Geodesics for D = 0 B.2.3Null Geodesics for D = 0 B.2.4Null geodesics for D ̸= 0 B.3 Initial Direction of the light rays B.3.1 The light ray initially travelling away from the companion (u ini- tially decreasing) B.3.2 The light ray initially travelling towards the companion (u ini- tially increasing): c (solid blue curve in Fig. B.4 Solving the geodesic equation for D > 3 3GM c2 B.1), regardless of the initial direction of the light ray C Details of Calculations for the Kerr Spacetime C.1 Equations of motion of light rays in the Kerr spacetime C.2 Null geodesics C.2.1θ integrals C.2.2r integrals C.3 Elliptical integrals in the form of algebraic integration C.4 Derivations of useful expressions needed for θ integrations C.4.1Derivation of Eq. (C.43) C.4.2Derivation of Eq. (C.53) C.4.3Derivation of Eq. (C.59a), i.e., the relation between Ψ j and ΓJ C.5 Calculation methods of pr /pt , pθ /pt and pφ /pt using the initial position and the initial direction of the light ray C.5.1 Conditions satisfied by |Dq | D Geometrical Explanation for The Pulse Profile Distortion Near The Superior Conjunction 225 D.1 Configurations Other Than Superior Conjunction D.2 Superior Conjunction Configuration with a Stellar-Mass Black Hole Bibliography 237 en_US
dc.publisher.publisher The Institute of Mathematical Sciences
dc.subject Pulsar–Black Hole Binaries en_US
dc.subject Light Bending Phenomenon en_US
dc.subject Schwarzchild Spacetime en_US
dc.title Light Bending Under General Relativity: A Study of Pulsar–Black Hole Binaries [HBNI Th277] en_US
dc.type.degree Ph.D en_US
dc.type.institution HBNI en_US
dc.description.advisor Manjari Bagchi
dc.description.pages 247p. en_US
dc.type.mainsub Physics en_US
dc.type.hbnibos Physical Sciences en_US


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