Isofrequency pairing of geodesic orbits in Kerr geometry
Isofrequency pairing of geodesic orbits in Kerr geometry
Abstract
?
Bound geodesic orbits around a Kerr black hole can be parametrized by three constants of the motion: the (specific) orbital energy, angular momentum, and Carter constant. Generically, each orbit also has associated with it three frequencies, related to the radial, longitudinal, and (mean) azimuthal motions. Here, we note the curious fact that these two ways of characterizing bound geodesics are not in a one-to-one correspondence. While the former uniquely specifies an orbit up to initial conditions, the latter does not: there is a (strong-field) region of the parameter space in which pairs of physically distinct orbits can have the same three frequencies. In each such isofrequency pair, the two orbits exhibit the same rate of periastron precession and the same rate of Lense-Thirring precession of the orbital plane, and (in a certain sense) they remain “synchronized” in phase.
Warburton, Niels
88d3f12e-d930-438d-bb54-071292b0c1dc
Barack, Leor
f08e66d4-c2f7-4f2f-91b8-f2c4230d0298
Sago, Norichika
c4baa9a1-e4fb-448e-8818-f7d189ed2773
3 April 2013
Warburton, Niels
88d3f12e-d930-438d-bb54-071292b0c1dc
Barack, Leor
f08e66d4-c2f7-4f2f-91b8-f2c4230d0298
Sago, Norichika
c4baa9a1-e4fb-448e-8818-f7d189ed2773
Warburton, Niels, Barack, Leor and Sago, Norichika
(2013)
Isofrequency pairing of geodesic orbits in Kerr geometry.
Physical Review D, 87 (84012).
(doi:10.1103/PhysRevD.87.084012).
Abstract
Abstract
?
Bound geodesic orbits around a Kerr black hole can be parametrized by three constants of the motion: the (specific) orbital energy, angular momentum, and Carter constant. Generically, each orbit also has associated with it three frequencies, related to the radial, longitudinal, and (mean) azimuthal motions. Here, we note the curious fact that these two ways of characterizing bound geodesics are not in a one-to-one correspondence. While the former uniquely specifies an orbit up to initial conditions, the latter does not: there is a (strong-field) region of the parameter space in which pairs of physically distinct orbits can have the same three frequencies. In each such isofrequency pair, the two orbits exhibit the same rate of periastron precession and the same rate of Lense-Thirring precession of the orbital plane, and (in a certain sense) they remain “synchronized” in phase.
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PhysRevD.87.084012
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Published date: 3 April 2013
Organisations:
Applied Mathematics
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Local EPrints ID: 347768
URI: http://eprints.soton.ac.uk/id/eprint/347768
ISSN: 1550-7998
PURE UUID: 4217af49-7b17-4a0e-8441-1a91103bf213
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Date deposited: 30 Jan 2013 14:20
Last modified: 15 Mar 2024 03:21
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Author:
Niels Warburton
Author:
Norichika Sago
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