Open Access
Fig. 13

Same as Fig. 10 for a = 1300 au.
Left: section for au2yr−2
at ΩG = 0 decreasing. The upper islands are due to librations of ωG
with e2 ≈ 1 − K2.
Right: section for
au2yr−2
at ΩG = 0 decreasing. The islands are due to librations of ωG
and oscillations of e2
around
.
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