Change in the rotational splittings of the ℓ = 1,m = 1 modes owing to the and ℓ = 4, m = 4, ν ≃ 300   μHz mode. Absolute values were considered. The energy of the mode was fixed in a way that v_obs = 1   km s^-1 for ℓ = 3, ν = 276   μHz at log τ_R =  −3 for Model 1. Black point are for Model 1 and red points for Model 2. The g-mode considered has ν = 305.14   μHz in Model 1 and ν = 301.02   μHz in Model 2.