Table 1
A least-squares fit for the additional p-mode frequencies (∗), which we found compared to the analysis by Kurtz et al. (2014), and for the other frequencies which are part of the same multiplets.
| Frequency [d-1] | Amplitude [mmag] | Phase [2π] | Δf [d-1] | Remarks | |
|
|
|||||
| ∗ | 22.94259 (0.00003) | 0.074 (0.006) | –0.30 (0.08) | – | – |
| ∗ | 22.96643 (0.00002) | 0.165 (0.008) | 0.46 (0.05) | 0.02383 (0.00004) | Δf/ 2 = 0.01192 (0.00002) |
| 23.50619 (0.00003) | 0.068 (0.006) | –0.29 (0.09) | – | – | |
| 23.52585 (0.00002) | 0.172 (0.008) | –0.43 (0.04) | 0.01965 (0.00004) | Δf/ 2 = 0.00983 (0.00002) | |
| ∗ | 23.53574 (0.00007) | 0.027 (0.005) | 0.47 (0.18) | 0.00990 (0.00007) | – |
| 23.54554 (0.00002) | 0.128 (0.007) | 0.37 (0.05) | 0.00980 (0.00007) | – | |
| 23.55533 (0.00003) | 0.067 (0.006) | 0.46 (0.09) | 0.00979 (0.00004) | – | |
| 23.56517 (0.00003) | 0.079 (0.006) | –0.07 (0.08) | 0.00984 (0.00004) | – | |
| 23.57502 (0.00004) | 0.059 (0.006) | 0.18 (0.10) | 0.00984 (0.00005) | – | |
| 23.58480 (0.00001) | 0.239 (0.009) | –0.16 (0.04) | 0.00978 (0.00004) | – | |
| ∗ | 23.56866 (0.00005) | 0.045 (0.005) | 0.08 (0.12) | – | – |
| ∗ | 23.58695 (0.00004) | 0.046 (0.006) | –0.39 (0.12) | 0.01829 (0.00006) | Δf/ 2 = 0.00915 (0.00003) |
| ∗ | 23.59023 (0.00002) | 0.109 (0.007) | –0.06 (0.06) | – | – |
Notes. Δf is the spacing between the given frequency and the preceding one. The provided errors are the formal error margins from the least-squares fit.
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