Table 1.
Best-fit parameters of ξ Tau models. The ‘original’ one is taken from Nemravová et al. (2016), Table 15.
| Original | Reference | All-data | Tides | 5-component | |||
|---|---|---|---|---|---|---|---|
| Var. | Unit | val. | val. | val. | val. | val. | σ |
| msum | M⊙ | 8.881594 | 9.547810 | 9.549357 | 9.557040 | 10.410026 | 0.2 |
| q1 | 1 | 0.900146 | 0.948223 | 0.948717 | 0.948208 | 0.948885 | 0.001 |
| q2 | 1 | 0.880155 | 0.852451 | 0.854879 | 0.852786 | 0.876618 | 0.01 |
| q3 | 1 | 0.113367 | 0.175785 | 0.163744 | 0.177839 | 0.174983 | 0.01 |
| q4 | 1 | 0.080957 | 0.01 | ||||
| P1 | d | 7.148234 | 7.147145 | 7.147156 | 7.147136 | 7.147000 | 0.000010 |
| log e1 | 1 | −∞ | −2.8400 | −2.8525 | −2.8627 | −2.8212 | 0.01 |
| i1 | ° | 86.530 | 86.702 | 87.185 | 86.847 | 87.120 | 0.1 |
| Ω1 | ° | 331.364 | 328.461 | 328.368 | 328.451 | 328.428 | 1.0 |
| ϖ1 | ° | 245.479 | 113.967 | 116.317 | 119.557 | 120.890 | 1.0 |
| λ1 | ° | 61.501 | 58.399 | 58.359 | 58.369 | 58.208 | 0.1 |
| P2 | d | 145.744 | 145.792 | 145.785 | 145.784 | 145.772 | 0.01 |
| log e2 | 1 | −0.7044 | −0.6829 | −0.6829 | −0.6829 | −0.6826 | 0.01 |
| i2 | ° | 86.676 | 86.546 | 86.554 | 86.598 | 86.655 | 1.0 |
| Ω2 | ° | 328.902 | 328.347 | 328.349 | 328.347 | 328.444 | 1.0 |
| ϖ2 | ° | 338.521 | 341.105 | 341.108 | 341.106 | 341.447 | 1.0 |
| λ2 | ° | 64.198 | 63.587 | 63.587 | 63.587 | 63.811 | 1.0 |
| P3 | d | 18503.8 | 18876.8 | 18877.1 | 18878.9 | 18887.0 | 100 |
| log e3 | 1 | −0.2451 | −0.2421 | −0.2396 | −0.2420 | −0.2417 | 0.01 |
| i3 | ° | −26.275 | −23.748 | −23.031 | −23.820 | −23.956 | 1.0 |
| Ω3 | ° | 108.252 | 101.844 | 102.066 | 102.121 | 101.376 | 1.0 |
| ϖ3 | ° | 117.247 | 117.918 | 117.949 | 117.901 | 117.994 | 1.0 |
| λ3 | ° | 148.550 | 148.445 | 148.334 | 148.433 | 148.450 | 1.0 |
| T1 | K | 10540 | 11000 | 10540 | 10555 | 100 | |
| T2 | K | 10318 | 10602 | 10318 | 10318 | 100 | |
| T3 | K | 14046 | 14000 | 14046 | 13983 | 100 | |
| T4 | K | 6751† | 6487† | 6800† | 6737† | 300 | |
| T5 | K | 6737† | 300 | ||||
| log g1 | 1 | 4.364 | 4.337 | 4.364 | 4.355 | 0.01 | |
| log g2 | 1 | 4.343 | 4.355 | 4.343 | 4.343 | 0.01 | |
| log g3 | 1 | 4.300 | 4.238 | 4.300 | 4.257 | 0.01 | |
| log g4 | 1 | 4.240† | 4.258† | 4.237† | 4.241† | 0.01 | |
| log g5 | 1 | 4.241† | 0.01 | ||||
| vrot, 1 | km s−1 | 14.600 | 15.203 | 15.203 | 10 | ||
| vrot, 2 | km s−1 | 13.281 | 15.210 | 15.210 | 10 | ||
| vrot, 3 | km s−1 | 242.262 | 242.371 | 242.371 | 10 | ||
| vrot, 4 | km s−1 | 65.234 | 65.234 | 65.234 | 30 | ||
| vrot, 5 | km s−1 | 65.234 | 30 | ||||
| Δt1 | s | 800 | 100 | 100 | |||
| Δt2 | s | 800 | 100 | 100 | |||
| C20, 1 | 1 | 0.000 | 0.000 | 0.001 | |||
| C20, 2 | 1 | 0.000 | 0.000 | 0.001 | |||
| γ | km s−1 | 8.82 | 10.180 | 11.022 | 9.870 | 9.625 | 0.5 |
| d | pc | 67.88 | 65.994 | 66.138 | 66.015 | 67.947 | 1.0 |
| nsky | 96 | 106 | 106 | 106 | 106 | ||
| nrv | 834 | 260 | 822 | 1103 | 1103 | ||
| netv | 35 | 48 | 77 | 77 | 77 | ||
| necl | 4 | 47 | 47 | 47 | 47 | ||
| nvis | – | 16678 | 16678 | 16678 | 16678 | ||
| nclo | – | 4533 | 4533 | 4533 | 4533 | ||
| nt3 | – | 4117 | 4117 | 4117 | 4117 | ||
| nlc | – | – | 18489 | – | – | ||
| nsyn | – | – | 1753731 | – | – | ||
| nsed | – | 7 | 7 | 7 | 7 | ||
| nsed2 | – | 14 | 14 | 14 | 14 | ||
| n | 978 | 482 | 1798621 | 1354 | 1354 | ||
| χsky2 | 185 | 301 | 324 | 289 | 233 | ||
| χrv2 | 2237 | 1152 | 3686 | 3377 | 3286 | ||
| χetv2 | 151 | 20.2 | 76.6 | 392‡ | 453‡ | ||
| χecl2 | 3.3 | 20.3 | 144! | 21.1 | 43.4 | ||
| χvis2 | – | 174346 | 160495 | 174207 | 120467 | ||
| χclo2 | – | 62129 | 42703 | 61131 | 48651 | ||
| χt32 | – | 26618 | 23463 | 25681 | 18191 | ||
| χlc2 | – | – | 160870 | – | – | ||
| χsyn2 | – | – | 3246892 | – | – | ||
| χsed2 | – | 18.5 | 297! | 18.8 | 28.8 | ||
| χsed22 | – | 40.9 | 224! | 46.3 | 40.3 | ||
| χ2 | 2578 | 1553 | 3639180 | 4145 | 4085 |
Notes. The notation is as follows: mi for ∀i the masses; q1 = m2/m1, q2 = m3/(m1 + m2), and q3 = m4/(m1 + m2 + m3) are mass ratios; Pi period; log ei logarithm of eccentricity; ii inclination; Ωi longitude of the ascending node; ϖi longitude of the pericentre; λi mean longitude in orbit; Ti effective temperature; log gi logarithm of gravitational acceleration; vrot, i rotational velocity; C20, i oblateness; Δti tidal time lag; n number of observations; χ2 unreduced value; χ2/n would be reduced one; † constrained by mass using Harmanec (1988); ‡ with ETV uncertainties of the order of 10−4 d ≃ 0.1 min. The epoch of osculating elements is 2456224.724705 (TDB). The angular elements are expressed in the observer’s reference frame.
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