Table 8
Extracted dipole modes and their parameters for KIC 9163796.
| ℓ | m | Frequency | Amplitude | FWHM or height |  |
δf | |
|---|---|---|---|---|---|---|---|
| [μHz] | [ppm] | [μHz] or [ppm2/μHz−1] | [] | [μHz] | |||
| 1 | … |  |
 |
 |
1.000 | − | |
| 1 | … |  |
 |
 |
1.000 | − | |
| 1 | … |  |
 |
 |
0.674 | − | |
| 1 | … |  |
 |
 |
… | − | |
| 1 | … |  |
 |
 |
1.000 | − | |
| 1 | … |  |
[sinc] |  |
… | − | |
| 1 | … |  |
 |
 |
… | − | |
| 1 | … |  |
 |
 |
… | − | |
| 1 | … |  |
[sinc] |  |
… | − | |
| 1 | … |  |
[sinc] |  |
… | − | |
| 1 | … |  |
 |
 |
… | − | |
| 1 | … |  |
 |
 |
… | − | |
| 1 | … |  |
 |
 |
… | − | |
| 1 | … |  |
 |
 |
… | − | |
| 1 | … |  |
 |
 |
… | − | |
| 1 | … |  |
 |
 |
… | − | |
| −1 |  |
 |
 |
… | |||
| 1 | 0 |  |
 |
 |
… | 0.278 ± 0.01 | |
| +1 |  |
 |
 |
0.990 | |||
| −1 |  |
[sinc] |  |
0.553 | |||
| 1 | 0 |  |
 |
 |
… | 0.157 ± 0.005 | |
| +1 |  |
 |
 |
… | |||
| 1 | −1 |  |
[sinc] |  |
… | ||
| 0 |  |
 |
 |
1.000 | 0.245 ± 0.003 | ||
| −1 |  |
 |
 |
0.998 | |||
| 1 | 0 |  |
 |
 |
0.986 | 0.23 ± 0.02 | |
| +1 |  |
 |
 |
1.000 | |||
| 1 | −1 |  |
[sinc] |  |
… | ||
| 0 |  |
 |
 |
… | 0.237 ± 0.002 | ||
| 1 | −1 |  |
 |
 |
… | ||
| +1 |  |
 |
 |
… | 0.15 ± 0.02 | ||
| 1 | −1 |  |
 |
 |
1.000 | ||
| +1 |  |
 |
 |
1.000 | 0.24 ± 0.009 | ||
| 1 | 0 |  |
[sinc] |  |
… | ||
| +1 |  |
[sinc] |  |
… | 0.254 ± 0.001 | ||
| 1 | 0 |  |
 |
 |
0.985 | ||
| +1 |  |
 |
 |
0.997 | 0.24 ± 0.01 | ||
| −1 |  |
 |
 |
… | |||
| 1 | 0 |  |
 |
 |
1.000 | 0.29 ± 0.01 | |
| +1 |  |
 |
 |
… | |||
Notes.The first and second column list the spherical degree and azimuthal
order m
of an identified dipole oscillation mode, respectively. For
resolved dipole modes, described through a Lorentzian profile,
the median centre frequency, the mode amplitude and its
full width at half maximum (FWHM) are given. For
unresolved peaks, described through a sinc function, the
median frequency and the mode height is given. For the
case of peaks with a low S/N, the detection probability
is reported, which ranges between 0 and 1, whereby 1
corresponds to a detection probability of 100%. In case of
rotationally split dipole modes the average separation of the
m = ± 1
modes is given for the individual component frequencies.
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