Table 2
Inferred rotation coefficients and uncertainties for ℓ = 1, | m | = 1 mode splittings with a rotation axis inclination of 90° for independent fits to each star (Cols. 4 and 5); for an ensemble fit for stars with similar synthetic rotation profiles (Cols. 6 and 7); for an ensemble fit for stars with rotation profiles where the rotation rate below the BCZ varied randomly up to 50% from 1035 nHz (Cols. 8 and 9).
Independent inversions | Ensemble inversions | |||||||
Ωc(1 ± 0.5) | ||||||||
T eff | r BCZ | ⟨ n ⟩ | Ω∗ ± σ(Ω∗) | ΔΩ ± σ(ΔΩ) |
![]() |
ΔΩ ± σ(ΔΩ) |
![]() |
ΔΩ ± σ(ΔΩ) |
[K] | [R] | [nHz] | [nHz] | [nHz] | [nHz] | [nHz] | [nHz] | |
|
||||||||
4538 | 0.65 | 27 | 693 ± 552 | 828 ± 1073 | 883 ± 173 | –111 ± 266 | 449 ± 173 | –111 ± 266 |
4676 | 0.64 | 24 | 1810 ± 607 | –838 ± 720 | 874 ± 178 | –111 ± 266 | 441 ± 178 | –111 ± 266 |
4860 | 0.61 | 22 | 1632 ± 676 | –641 ± 797 | 866 ± 184 | –111 ± 266 | 324 ± 184 | –111 ± 266 |
5599 | 0.73 | 22 | 1828 ± 587 | –1360 ± 1146 | 876 ± 164 | –111 ± 266 | 1146 ± 164 | –111 ± 266 |
5627 | 0.67 | 20 | 952 ± 699 | 254 ± 1336 | 890 ± 166 | –111 ± 266 | 726 ± 166 | –111 ± 266 |
5632 | 0.71 | 23 | 1422 ± 708 | –625 ± 1378 | 865 ± 174 | –111 ± 266 | 904 ± 174 | –111 ± 266 |
5701 | 0.70 | 22 | –467 ± 723 | 3056 ± 1394 | 925 ± 126 | –111 ± 266 | 795 ± 126 | –111 ± 266 |
5744 | 0.72 | 20 | –230 ± 627 | 2640 ± 1215 | 923 ± 137 | –111 ± 266 | 1421 ± 137 | –111 ± 266 |
5892 | 0.71 | 18 | 1823 ± 620 | –1358 ± 1195 | 880 ± 156 | –111 ± 266 | 718 ± 156 | –111 ± 266 |
5983 | 0.75 | 19 | 1649 ± 723 | –1078 ± 1405 | 891 ± 158 | –111 ± 266 | 961 ± 158 | –111 ± 266 |
6252 | 0.81 | 19 | 1382 ± 592 | –464 ± 1181 | 890 ± 162 | –111 ± 266 | 791 ± 162 | –111 ± 266 |
6408 | 0.84 | 21 | 1019 ± 583 | 271 ± 1170 | 890 ± 167 | –111 ± 266 | 1733 ± 167 | –111 ± 266 |
6661 | 0.91 | 17 | 942 ± 422 | 743 ± 1392 | 949 ± 109 | –111 ± 266 | 493 ± 109 | –111 ± 266 |
6663 | 0.88 | 19 | 380 ± 472 | 2591 ± 1518 | 931 ± 102 | –111 ± 266 | 1120 ± 102 | –111 ± 266 |
6680 | 0.89 | 18 | 1121 ± 431 | 112 ± 1407 | 942 ± 97 | –111 ± 266 | 1123 ± 97 | –111 ± 266 |
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