Scalar Resonant Relaxation of Stars Around a Massive Black Hole
Ben Bar-Or, Jean-Baptiste Fouvry

TL;DR
This paper develops a first-principles, parameter-free model for scalar resonant relaxation in nuclear star clusters around massive black holes, describing how stellar angular momentum evolves due to potential fluctuations.
Contribution
It provides the first complete calculation of diffusion coefficients for scalar resonant relaxation in spherical systems from fundamental principles, with an open source implementation.
Findings
Diffusion coefficients depend explicitly on the mean field stellar distribution.
The model describes potential fluctuations as correlated noise based on stellar orbits.
The approach enables parameter-free, first-principles predictions of angular momentum evolution.
Abstract
In nuclear star clusters, the potential is governed by the central massive black hole, so that stars move on nearly Keplerian orbits and the total potential is almost stationary in time. Yet, the deviations of the potential from the Keplerian one, due to the enclosed stellar mass and general relativity, will cause the stellar orbits to precess. Moreover, as a result of the finite number of stars, small deviations of the potential from spherical symmetry induce residual torques that can change the stars' angular momentum faster than the standard two-body relaxation. The combination of these two effects drives a stochastic evolution of orbital angular momentum, a process named "resonant relaxation". Owing to recent developments in the description of the relaxation of self-gravitating systems, we can now fully describe scalar resonant relaxation (relaxation of the magnitude of the angular…
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