Fig. 3

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(A)symmetry of the Lamb resonance. Similar to Fig. 2, the imaginary part of the normalized pressure anomaly (Eq. (22)), which is associated with the semidiurnal tide, is plotted as a function of the normalized forcing frequency ω = (Ω − n⋆)/n⋆ = σ/2n⋆, for the same planetary-stellar parameters. We focus here on the high frequency regime around the Lamb resonance. Different panels correspond to different values of σbl, or different thermal inertias in the ground and the atmosphere. Allowing for thermal inertia results in a delayed ground response, of which the signature is clear in inducing an asymmetry in the spectral behavior around the resonance.
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