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Isofrequency pairing of geodesic orbits in Kerr geometry

Niels WarburtonSchool of Mathematical Sciences and Complex and Adaptive Systems Laboratory, University College Dublin, Belfield, Dublin 4, IrelandLeor BarackSchool of Mathematics, University of Southampton, Southampton SO17 1BJ, United KingdomNorichika SagoFaculty of Arts and Science, Kyushu University, Fukuoka 819-0395, Japan
2013en
ABI

Аннотация

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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