Fig. 10

Poincaré sections of the dynamics driven by both the planetary and galactic perturbations (Hamiltonian from Eq. (13)). The semi-major axis taken as parameter is
a = 500 au. The colour scale shows the maximum orbital change rate between two successive points (see titles), and the grey zones are forbidden. Top: section for au2yr−2
at ΩG = 0 decreasing. The islands located at e ≈ 0.8 are due to the resonance 2ω + Ω, and the islands located at e ≈ 0.2 are due to librations of ω
while I ≈ 63o
(Lidov–Kozai mechanism). Bottom: section for
au2yr−2
at ωG = 0 decreasing. The chaotic bands are due to the overlap of the resonances ω − Ω
and 2ω − Ω
(for I < 90o), or ω + Ω
and 2ω + Ω
(for I > 90o), and the islands located at I ≈ 90o
are due to librations of Ω
(orthogonal Laplace plane).
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