Hamiltonians and canonical coordinates for spinning particles in curved space-time
Vojt\v{e}ch Witzany, Jan Steinhoff, and Georgios Lukes-Gerakopoulos

TL;DR
This paper develops Hamiltonian formalism and canonical coordinates for spinning particles in curved spacetime, aiding the modeling of gravitational waves from extreme-mass-ratio inspirals for LISA detection.
Contribution
It introduces Hamiltonians and canonical phase-space coordinates for various spin conditions, facilitating symplectic integration of spinning bodies in curved spacetime.
Findings
Motion is regular for typical EMRI spin ranges
Larger spins lead to weakly chaotic dynamics
Canonical coordinates improve numerical integration
Abstract
The spin-curvature coupling as captured by the so-called Mathisson-Papapetrou-Dixon (MPD) equations is the leading order effect of the finite size of a rapidly rotating compact astrophysical object moving in a curved background. It is also a next-to-leading order effect in the phase of gravitational waves emitted by extreme-mass-ratio inspirals (EMRIs), which are expected to become observable by the LISA space mission. Additionally, exploring the Hamiltonian formalism for spinning bodies is important for the construction of the so-called Effective-One-Body waveform models that should eventually cover all mass ratios. The MPD equations require supplementary conditions determining the frame in which the moments of the body are computed. We review various choices of these supplementary spin conditions and their properties. Then, we give Hamiltonians either in proper-time or…
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