Open Access
Table 2.
Mass, large separations, core rotation, magnetic shifts, asymmetries, and field strength for every favourable detection.
| KIC | M(Ms) | ΔΠ1(s) | Δν(μHz) | νR, g(μHz) | (μHz) |
a | ![]() |
⟨Br2⟩1/2(kG) |
|---|---|---|---|---|---|---|---|---|
| 2584478 | 1.32 ± 0.06 | ![]() |
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0.26 | 106 ± 17 |
| 4066278 | 1.44 ± 0.07 | ![]() |
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S | 0.63 | > 73 ± 9 | |
| 4077249 | 1.32 ± 0.06 | ![]() |
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0.18 | 52 ± 7 |
| 4350501 | 1.55 ± 0.08 | ![]() |
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D | 0.33 | [39; 55]±23 |
| 4660930 | 1.60 ± 0.10 | ![]() |
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0.26 | 90 ± 34 |
| 4771876 | 1.10 ± 0.06 | ![]() |
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S | 0.29 | > 97 ± 11 | |
| 4995788 | 1.19 ± 0.06 | ![]() |
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S | 0.24 | > 69 ± 10 | |
| 5287034 | 1.25 ± 0.06 | ![]() |
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0.21 | 58 ± 9 |
| 6103082 | 1.31 ± 0.07 | ![]() |
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D | 0.54 | [190; 269]±39 |
| 6222530 | 1.37 ± 0.06 | ![]() |
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D | 0.43 | [196; 277]±22 |
| 6389421 | 1.13 ± 0.07 | ![]() |
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S | 0.38 | > 139 ± 13 | |
| 6758291 | 1.15 ± 0.07 | ![]() |
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D | 0.53 | [236; 334]±28 |
| 8350839 | 1.26 ± 0.08 | ![]() |
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S | 0.30 | > 56 ± 13 | |
| 8574234 | 1.06 ± 0.05 | ![]() |
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S | 0.36 | > 39 ± 4 | |
| 8687248 | 1.35 ± 0.07 | ![]() |
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S | 0.68 | > 155 ± 50 | |
| 8868464 | 1.43 ± 0.09 | ![]() |
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D | 0.26 | [80; 114]±21 |
| 9649838 | 1.69 ± 0.11 | ![]() |
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0.28 | 47 ± 17 |
| 10593078 | 1.52 ± 0.08 | ![]() |
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S | 0.32 | > 114 ± 6 | |
| 10784759 | 1.64 ± 0.10 | ![]() |
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0.20 | 151 ± 42 |
| 11087371 | 1.41 ± 0.08 | ![]() |
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S | 0.32 | > 52 ± 1 | |
| 11602793 | 1.38 ± 0.07 | ![]() |
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D | 0.19 | [18; 25]±4 |
| 12008916 | 1.47 ± 0.09 | ![]() |
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D | 0.21 | [35; 50]±4 |
| 12168062 | 1.49 ± 0.09 | ![]() |
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S | 1.72 | > 327 ± 52 |
Notes.
The ‘S’ and ‘D’ in column ‘a’ refer to ‘singlet’ and ‘doublet’ detection. Brackets indicate lower and upper bounds for the corresponding parameter. Masses are taken from Li et al. (2024).
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