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Table 2

Mode identification and linear nonadiabatic growth rates, κ0, from the best seismic model of KIC 08626021.

Id. Frequency ℓ k Ckℓ κ0 † δ νt Pm(th) δ νo Pm(obs) D Comment
(μHz) (μHz) (day) (μHz) (day)
f2,0 5073.23411 1 3 0.426 2 × 10-13−7 × 10-12 0.0148 780 0.0064 ~700 1 × 104−5 × 105 Hysteresis regime⋆
f1,0 4309.91490 1 4 0.456 2 × 10-12−4 × 10-11 0.0187 620 0.00034 ~620 3 × 103−6 × 104 Intermediate regime
f3,0 3681.80287 1 5 0.469 1 × 10-11−2 × 10-10 0.0223 518 ... 263 7 × 102−1 × 104 Intermediate regime
f6 3294.36928 1 6 0.467 2 × 10-11−4 × 10-10 ... ... ... ... ...
f9 6981.26129 2 4 0.121 7 × 10-12−7 × 10-11 ... ... ... ... ...
f5 4398.37230 2 8 0.152 4 × 10-10−5 × 10-9 ... ... ... ... ...
f7 3677.99373 2 10 0.154 2 × 10-9−4 × 10-8 ... ... ... ... ...
f4 2658.77740 2 15 0.161 1 × 10-7−6 × 10-7 ... ... ... ... ...

Notes.

(†)

A range of values is given for the growth rate, reflecting calculations using various treatments and hypotheses on the efficiency of convection (see text);

(⋆)

the frequencies are locked but the amplitudes are still modulated.

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