Table 4
Rotationally split triplets based on BTr and SMEI observations.
| ID | IDobs | m | f m | P0 | ⟨ δfrot ⟩ | n g |
|
|
||||||
| f 15 | −1 | 0.4173(11) | ||||
| ν 1 | 0 | 0.42031(89) | 2.3997(51) | 0.00302(88) | 39 | |
| f 16 | 1 | 0.4234(14) | ||||
|
|
||||||
| f 13 | −1 | 0.55775(38) | ||||
| ν 2 | 0 | 0.56125(32) | 1.7818(10) | 0.00351(33) | 29 | |
| f 14 | 1 | 0.56476(52) | ||||
|
|
||||||
| f 9 | −1 | 0.59867(30) | ||||
| ν 3 | 0 | 0.60201(50) | 1.6611(14) | 0.00333(50) | 27 | |
| f 10 | 1 | 0.60535(92) | ||||
|
|
||||||
| f 17 | −1 | 0.6440(13) | ||||
| ν 4 | 0 | 0.64727(75) | 1.5449(18) | 0.00325(71) | 25 | |
| f 18 | 1 | 0.65052(73) | ||||
|
|
||||||
| f 7 | −1 | 0.69813(32) | ||||
| ν 5 | 0 | 0.70132(56) | 1.4259(11) | 0.00319(54) | 23 | |
| f 8 | 1 | 0.7045(11) | ||||
|
|
||||||
| f 1 | −1 | 0.83881(9) | ||||
| ν 6 | 0 | 0.84139(10) | 1.1885(1) | 0.00258(10) | 19 | |
| f 3 | 1 | 0.84398(17) | ||||
| → | 0 | 0.84086(16) | 1.1893(2) | 0.00246(15) | ||
|
|
||||||
| f 3 | −1 | 0.88363(29) | ||||
| ν 7 | 0 | 0.88597(16) | 1.1287(2) | 0.00233(16) | 18 | |
| f 4 | 1 | 0.88831(14) | ||||
| → | 0 | 0.88578(13) | 1.1289(2) | 0.00243(12) | ||
|
|
||||||
| f 11 | −1 | 0.92511(63) | ||||
| ν 8 | 0 | 0.92706(36) | 1.0787(4) | 0.00193(36) | 17 | |
| f 12 | 1 | 0.92901(31) | ||||
|
|
||||||
| f 5 | −1 | 0.97975(10) | ||||
| ν 9 | 0 | 0.98203(15) | 1.0183(2) | 0.00229(15) | 16 | |
| f 6 | 1 | 0.98431(29) | ||||
| → | 0 | 0.98164(15) | 1.0187(2) | 0.00257(16) | ||
Notes. In the case of BTr, the unresolved central (m = 0) component f0 is determined from the midpoint of the observed f± 1 components and P0 is the corresponding period. The split frequency ⟨ δfrot ⟩ is then half the difference between the m = 1 and m = −1 component and ng gives the radial order of the best-fit model frequency (see Sect. 7). In the case of SMEI (labeled by an arrow in the first column), f0 and ⟨ δfrot ⟩ are determined from a Lorentzian fit to the data. Frequencies and periods are given in units of d-1 and d, respectively.
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