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Fig. 13

image

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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