Fig. 12
Change in the rotational splitting of the ℓ = 1, ν = 2807.5 μHz p-mode owing to the ℓ = 4, m = 4 g-modes considering the τwave term. Here we assume the same energy for all modes and fix it so that vobs = 1 km s-1 for ℓ = 3, ν = 276 μHz at log τR = −3. Black points are for stable modes and green points for the unstable ones. Model 1 was used.
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