2001
DOI: 10.1088/0264-9381/18/15/314
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On the motion of spinning test particles in plane gravitational waves

Abstract: The Mathisson-Papapetrou-Dixon equations for a massive spinning test particle in plane gravitational waves are analysed and explicit solutions constructed in terms of solutions of certain linear ordinary differential equations. For harmonic waves this system reduces to a single equation of Mathieu-Hill type. In this case spinning particles may exhibit parametric excitation by gravitational fields. For a spinning test particle scattered by a gravitational wave pulse, the final energy-momentum of the particle ma… Show more

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Cited by 26 publications
(42 citation statements)
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“…Besides a formal analysis of the MPD equations [7][8][9], there are particular studies on spinning particle dynamics in a Kerr background [10][11][12][13], scattering interactions with gravitational waves [14,15], and other applications. In particular, the MPD equations lend themselves well to numerical analysis with applications involving gravitational wave generation in a Kerr background [16,17], evidence of deterministic chaos within particle orbital dynamics [18][19][20][21], and particle motion in a Vaidya background with radially infalling radiation [22].…”
mentioning
confidence: 99%
“…Besides a formal analysis of the MPD equations [7][8][9], there are particular studies on spinning particle dynamics in a Kerr background [10][11][12][13], scattering interactions with gravitational waves [14,15], and other applications. In particular, the MPD equations lend themselves well to numerical analysis with applications involving gravitational wave generation in a Kerr background [16,17], evidence of deterministic chaos within particle orbital dynamics [18][19][20][21], and particle motion in a Vaidya background with radially infalling radiation [22].…”
mentioning
confidence: 99%
“…For example, spinning particles in gravitational [47] and electromagnetic fields [48] acquire a contribution to their momenta which is not parallel to velocity, while the canonical momentum of a charged particle generally does not even have a uniquely defined direction. Indeed, in some of the more 'natural' derivations of LAD [9,49,50], the troublesome Schott term (the derivative of acceleration) arises from taking the momentum to be p = m(ẋ−τẍ), which to a good approximation agrees with (2).…”
Section: Momentum and Velocitymentioning
confidence: 99%
“…Then this arrangement can respond so as to divert the ring from a geodesic path via the second and third terms (the tidal term cannot do this). There is a connection here with Dixon's equations [7] (see also [8] for the dynamics of spinning particles in gravitational waves) as well as an analogy with electromagnetic effects [9]. The first term is analogous to an electric field; the second term a magnetic field due to the coupling between mass current and the field.…”
Section: A Relativistic String In Fermi Normal Coordinatesmentioning
confidence: 99%