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Fig. 11

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Change in the rotational splitting of the  = 1, ν = 2807.5   μHz p-mode owing to  = 4 multiplets, assuming the same amplitude for all modes with different m but the same ℓ,n numbers, and considering the τNAf term. As before we assume the same energy for all modes and fix it so that the  = 3 = 276   μHz mode would have an observed velocity vobs = 1   km s-1 if it were to be observed at an optical depth log τR =  −3. Model 1 has been used.

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