Fig. 2

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Spectrum of semi-diurnal atmospheric thermal tides. Plotted is the imaginary part of the normalized pressure anomaly (; Eq. (22)) as a function of the normalized forcing frequency ω = (Ω − n⋆)/n⋆ = σ/2n⋆, where n⋆ is the mean motion of the stellar perturber. The planetary-stellar parameters are those of the fiducial planetary system defined in Sect. 3.1.
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