Table 4.
The best-fitting results of the l = 1 mixed mode frequencies considering the magnetism-induced perturbations in Eqs. (12), (13), and (16).
| KIC | ΔΠ1 (s) | q | εg | fshift (μHz) | Ωcore/2π (μHz) | Ωenv/2π (μHz) | a | δνg (μHz) |
|---|---|---|---|---|---|---|---|---|
| 4458118 |
 |
 |
 |
 |
 |
 |
 |
 |
| 5196300 |
 |
 |
 |
 |
 |
 |
 |
 |
| 5696081 |
 |
 |
 |
 |
 |
 |
 |
 |
| 6936091 |
 |
 |
 |
 |
 |
 |
 |
 |
| 7009365 |
 |
 |
 |
 |
 |
 |
 |
 |
| 7518143 |
 |
 |
 |
 |
 |
 |
 |
 |
| 8540034 |
 |
 |
 |
 |
 |
 |
 |
 |
| 8619145 |
 |
 |
 |
 |
 |
 |
 |
 |
| 8684542 |
 |
 |
 |
 |
 |
 |
 |
 |
| 9202471 |
 |
 |
 |
 |
 |
 |
 |
 |
| 9589420 |
 |
 |
 |
 |
 |
 |
 |
 |
| 10801792 |
 |
 |
 |
 |
 |
 |
 |
 |
| 11515377 |
 |
 |
 |
 |
 |
 |
 |
 |
Notes. The parameters are: period spacing ΔΠ1, the coupling factor q, g-mode phase εg, the frequency correction of l = 1 pure p mode fshift, core and envelope rotation rates Ωcore/2π and Ωenv/2π, the asymmetry parameter a, and the magnetic shift δνg.
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