Open Access

Fig. 12


Resonant arguments (in radians versus time in Myr) σ = (g1 − g5) − (s1 − s2) (top) and θ = (s4 − s3) − 2(g4 − g3) (middle and bottom) for the different solutions La2004, La2010a,b,c,d. In the bottom plot, θ is displayed on a greater scale. One can see that the La2010 solutions are very close up to 50 Myr.

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