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Self-force in hyperbolic black hole encounters

Self-force in hyperbolic black hole encounters
Self-force in hyperbolic black hole encounters
Self-force methods can be applied in calculations of the scatter angle in two-body hyperbolic encounters, working order by order in the mass ratio (assumed small) but with no recourse to a weak-field approximation. This, in turn, can inform ongoing efforts to construct an accurate description of the general-relativistic binary dynamics via an effective-one-body description or other approaches. Existing self-force methods are to a large extent specialised to bound, inspiral orbits. Here we derive the first-order conservative self-force correction to the scattering angle, show its agreement with recent post-Minkowsian results, and develop a technique for (numerical) self-force calculations that can efficiently tackle scatter orbits. In the method, the metric perturbation is reconstructed from a Hertz potential that satisfies (mode-by-mode) a certain inhomogeneous version of the Teukolsky equation. The crucial ingredient in this formulation are certain jump conditions that the (multipole modes of the) Hertz potential must satisfy along the worldline of the small body's orbit. We present a closed-form expression for these jumps, for an arbitrary geodesic orbit in Schwarzschild spacetime. To begin developing the numerical infrastructure, a scalar-field evolution code on a Schwarzschild background (in 1+1D) is developed. Following this, results for the conservative scalar self-force corrections to the scatter angle are calculated. We continue by constructing a Teukolsky evolution code on a Schwarzschild background. This produces numerically unstable solutions due to unphysical homogeneous solutions of the Teukolsky equation at the horizon and null infinity being seeded by numerical error. This can be resolved by a change of variables to a Regge-Wheeler-like field. We then present a full numerical implementation of this method for circular and scatter orbits in Schwarzschild. We conclude with a discussion of the outlook for self-force calculations on scatter orbits.
University of Southampton
Long, Oliver
e20e8ea1-61c1-4998-9bf1-6938e7b8cdcb
Long, Oliver
e20e8ea1-61c1-4998-9bf1-6938e7b8cdcb
Barack, Leor
f08e66d4-c2f7-4f2f-91b8-f2c4230d0298

Long, Oliver (2022) Self-force in hyperbolic black hole encounters. University of Southampton, Doctoral Thesis, 139pp.

Record type: Thesis (Doctoral)

Abstract

Self-force methods can be applied in calculations of the scatter angle in two-body hyperbolic encounters, working order by order in the mass ratio (assumed small) but with no recourse to a weak-field approximation. This, in turn, can inform ongoing efforts to construct an accurate description of the general-relativistic binary dynamics via an effective-one-body description or other approaches. Existing self-force methods are to a large extent specialised to bound, inspiral orbits. Here we derive the first-order conservative self-force correction to the scattering angle, show its agreement with recent post-Minkowsian results, and develop a technique for (numerical) self-force calculations that can efficiently tackle scatter orbits. In the method, the metric perturbation is reconstructed from a Hertz potential that satisfies (mode-by-mode) a certain inhomogeneous version of the Teukolsky equation. The crucial ingredient in this formulation are certain jump conditions that the (multipole modes of the) Hertz potential must satisfy along the worldline of the small body's orbit. We present a closed-form expression for these jumps, for an arbitrary geodesic orbit in Schwarzschild spacetime. To begin developing the numerical infrastructure, a scalar-field evolution code on a Schwarzschild background (in 1+1D) is developed. Following this, results for the conservative scalar self-force corrections to the scatter angle are calculated. We continue by constructing a Teukolsky evolution code on a Schwarzschild background. This produces numerically unstable solutions due to unphysical homogeneous solutions of the Teukolsky equation at the horizon and null infinity being seeded by numerical error. This can be resolved by a change of variables to a Regge-Wheeler-like field. We then present a full numerical implementation of this method for circular and scatter orbits in Schwarzschild. We conclude with a discussion of the outlook for self-force calculations on scatter orbits.

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More information

Submitted date: March 2022
Published date: June 2022
Additional Information: Parts of this work have been published as: Oliver Long and Leor Barack. Time-domain metric reconstruction for hyperbolic scattering. Phys. Rev. D, 104(024014), Jul 2021.

Identifiers

Local EPrints ID: 457451
URI: http://eprints.soton.ac.uk/id/eprint/457451
PURE UUID: 97a66390-2a7e-4402-96f9-7c1441fca9fe
ORCID for Oliver Long: ORCID iD orcid.org/0000-0002-3897-9272
ORCID for Leor Barack: ORCID iD orcid.org/0000-0003-4742-9413

Catalogue record

Date deposited: 08 Jun 2022 16:50
Last modified: 17 Mar 2024 04:12

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Contributors

Author: Oliver Long ORCID iD
Thesis advisor: Leor Barack ORCID iD

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