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Fig. E.2

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Comparisons of the numerical integration results of three systems H¯Schubart${\bar H_{Schubart}}$, H¯Fourier${\bar H_{{\rm{Fourier}}}}$ and H¯Normal${\bar H_{{\rm{Normal}}}}$ In each frame, the initial condition corresponds to an equilibrium point (J2e, ψ2e = π) of the partial normal form H¯n*$\bar H_n^*$ for a same parameter J1 = −0.0179509. The normalization order is n = 1,…, 4 for frames (a)-(d). In each frame, the top panel shows the evolution of I1,J1, the second panel the evolution of P¯2${\bar P_2}$,I2,J2, the third panel θ1,ψ1, the fourth panel Q¯2${\bar Q_2}$,θ2,ψ2, as marked by different curves.

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