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Fig. 2.

image

Frequency differences of PM vs. UPM for radial modes with frequencies less than the acoustic cut-off frequency νac = c/(4πHp). Frequencies on the abscissa are normalized by the νmax of each models. Top panel: models J*: Teff ≃ 5900 K and log g = 4.0. Middle panel: models M*: Teff ≃ 5500 K and log g = 3.5. Bottom panel: models C*: Teff ≃ 6500 K and log g = 4.0.

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