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Fig. 4


Integrand of the mode inertia for the m-components of the higher-frequency l = 2 multiplet at the time during the avoided crossing where it shows the strongest asymmetry (t = t0 + 3 Myr). The radial and horizontal displacements (ξr and ξh) were computed using a perturbative approach as explained in Sect. 3 (gray dashed lines) and with the code acor (solid black lines).

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