Table 4
Theoretical quantities derived from the evolution models for the Zeeman detected giants.
HD | Name | M ∗ | Evolution | R BCE | τ(Hp/ 2) | R (Hp/ 2) | τ(max) | R max | τ(RCE/ 2) | R (RCE/ 2) |
M ⊙ | phase | R ∗ | day | R ∗ | day | R ∗ | day | R ∗ | ||
|
||||||||||
Active Giants | ||||||||||
|
||||||||||
3229 | 14 Cet | 1.55 ± 0.1 | HGap | 0.936 | 0.68 | 0.94 | 1.52 | 0.94 | 0.27 | 0.97 |
4128 | β Cet | 3.5 ± 0.2 | He burning | 0.504 | 121 | 0.56 | 232 | 0.51 | 53 | 0.75 |
3.6 ± 0.2 | Base RGB | 0.47 | 135 | 0.53 | 246 | 0.48 | 59 | 0.73 | ||
9746 | OP And | 2.0 ± 0.5 | RGB (Li) | 0.044 | 25 | 0.06 | 160 | 0.79 | 118 | 0.52 |
2.0 ± 0.5 | He burning | 0.183 | 106 | 0.23 | 179 | 0.45 | 80 | 0.60 | ||
27536 | EK Eri | 1.9 ± 0.3 | Base RGB | 0.507 | 103 | 0.56 | 234 | 0.51 | 43 | 0.75 |
28307 | 77 Tau | 3. ± 0.2 | Base RGB | 0.553 | 95 | 0.62 | 179 | 0.57 | 41 | 0.79 |
31993 | V1192 Ori | 1.8 ± 0.5 | RGB (Li) | 0.054 | 32 | 0.07 | 129 | 0.36 | 107 | 0.53 |
1.7 ± 0.5 | He burning | 0.244 | 99 | 0.32 | 190 | 0.27 | 62 | 0.68 | ||
2. ± 0.5 | RGB | 0.059 | 37 | 0.08 | 145 | 0.34 | 116 | 0.53 | ||
33798 | V390 Aur | 2.25(*) ± 0.3 | Base RGB | 0.477 | 119 | 0.56 | 230 | 0.50 | 49 | 0.77 |
47442 | ν3 CMa | 4.5 ± 0.5 | Base RGB | 0.415 | 170 | 0.48 | 314 | 0.43 | 78 | 0.71 |
4.0 ± 0.5 | He burning | 0.401 | 160 | 0.46 | 300 | 0.41 | 74 | 0.71 | ||
68290 | 19 Pup | 2.5 ± 0.2 | Base RGB | 0.483 | 118 | 0.57 | 239 | 0.51 | 49 | 0.77 |
2.5 ± 0.2 | He burning | 0.406 | 162 | 0.47 | 335 | 0.41 | 67 | 0.71 | ||
72146 | FI Cnc | 2.4 ± 0.3 | Base RGB | 0.608 | 65 | 0.68 | 122 | 0.63 | 28 | 0.82 |
82210 | 24 UMa | 1.9 ± 0.1 | Base RGB | 0.625 | 55 | 0.67 | 95 | 0.63 | 24 | 0.81 |
85444 | 39 Hya | 3.75(*) ± 0.2 | BaseRGB | 0.639 | 59 | 0.69 | 101 | 0.65 | 26 | 0.83 |
111812 | 31 Com | 2.75(*) ± 0.1 | HGap | 0.745 | 34 | 0.75 | 58 | 0.74 | 15 | 0.85 |
112989 | 37 Com | 5.25 ± 0.4 | He burning | 0.977 | 91 | 61 | 154 | 0.57 | 38 | 0.78 |
5.25 ± 0.4 | Base RGB | 0.527 | 124 | 0.58 | 224 | 0.53 | 54 | 0.76 | ||
121107 | 7 Boo | 4.0 ± 0.7 | HGap | 0.729 | 34 | 0.75 | 63 | 0.72 | 14 | 0.86 |
141714 | δ CrB | 2.5 ± 0.1 | Base RGB | 0.457 | 133 | 0.52 | 271 | 0.47 | 56 | 0.74 |
145001 | κ HerA | 3.5 ± 0.3 | Base RGB | 0.654 | 50 | 0.71 | 85 | 0.66 | 22 | 0.83 |
150997 | η Her | 2.5 ± 0.3 | Base RBG | 0.512 | 110 | 0.58 | 217 | 0.53 | 47 | 0.77 |
2.7(*) ± 0.3 | He burning | 0.456 | 126 | 0.52 | 244 | 0.46 | 54 | 0.73 | ||
163993 | ξ Her | 3. ± 0.3 | Base RGB | 0.570 | 87 | 0.63 | 161 | 0.58 | 37 | 0.80 |
2.5 ± 0.3 | He burning | 0.451 | 119 | 0.52 | 209 | 0.47 | 51 | 0.73 | ||
203387 | ι Cap | 3. ± 0.2 | Base RGB | 0.663 | 48 | 0.71 | 79 | 0.67 | 21 | 0.84 |
205435 | ρ Cyg | 2.6 ± 0.2 | Base RGB | 0.449 | 141 | 0.51 | 289 | 0.45 | 59 | 0.73 |
218153 | KU Peg | 2.5 ± 0.2 | Base RGB | 0.562 | 85 | 0.65 | 165 | 0.60 | 36 | 0.82 |
223460 | OU And | 2.8 ± 0.2 | HGap | 0.755 | 15 | 0.83 | 36 | 0.76 | 9 | 0.88 |
|
||||||||||
CFHT and miscellaneous | ||||||||||
|
||||||||||
9270 | η Psc | 4.9 ± 0.5 | Base RGB | 0.640 | 67 | 0.68 | 121 | 0.644 | 28 | 0.820 |
28305 | ϵ Tau | 3.0 ± 0.2 | Base RGB | 0.387 | 168 | 0.45 | 335 | 0.39 | 73 | 0.69 |
2.5 ± 0.2 | He burning | 0.360 | 146 | 0.43 | 268 | 0.37 | 67 | 0.69 | ||
29139 | Aldebaran | 1.7 ± 0.5 | AGB | 0.048 | 31 | 0.06 | 284 | 0.98 | 104 | 0.53 |
2.0 ± 0.5 | RGB | 0.061 | 40 | 0.08 | 143 | 0.35 | 114 | 0.54 | ||
62509 | Pollux | 2.5 ± 0.3 | Base RGB | 0.382 | 162 | 0.45 | 330 | 0.39 | 68 | 0.68 |
2.5 ± 0.3 | He burning | 0.366 | 183 | 0.43 | 391 | 0.36 | 75 | 0.68 | ||
81797 | Alphard | 3.5 ± 0.5 | AGB | 0.064 | 59 | 0.07 | 768 | 0.93 | 142 | 0.49 |
124897 | Arcturus | 1.5(a)± 0.3 | AGB | 0.095 | 50 | 0.12 | 170 | 0.98 | 72 | 0.55 |
1.5(a)± 0.3 | RGB | 0.034 | 151 | 0.04 | 137 | 0.95 | 94 | 0.52 |
Notes. For each star we give: stellar mass, evolution phase, radius at the base of the convective envelope, and convective turnover times at different locations within the convective envelope. M∗ marked (*) indicates that the values are the result of the linear interpolation between two models. For some stars we indicate two possible evolution states (“RGB(Li)” means that we use the Li abundance as an additional indicator). The mass of Arcturus(a) is determined based on models computed at the metallicity of this star ([Fe/H] = −0.6; Lagarde et al. 2012).
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