Free Access

Table 3

Measurements of the mean longitudinal magnetic field using sets of lines belonging to different elements.

MJD Phase BzTi BzTi,n BzCr BzCr,n BzFe BzFe,n BzY BzY,n
[G] [G] [G] [G] [G] [G] [G] [G]

HD 11753
55 203.0356 0.098 0 ± 16 12 ± 16 18 ± 11 −1 ± 20
55 204.0228 0.203 −39 ± 12 0 ± 13 −14 ± 11 −24 ± 13 −48 ± 11 −17 ± 13
55 205.0518 0.308 −3 ± 10 −18 ± 13 −7 ± 11 9 ± 15
55 206.0271 0.413 8 ± 9 −11 ± 16 −2 ± 11 10 ± 15
55 207.0207 0.518 1 ± 10 8 ± 11 12 ± 10 −3 ± 10
55 199.0975 0.678 7 ± 12 20 ± 15 18 ± 16 4 ± 15
55 209.0147 0.729 12 ± 11 20 ± 8 8 ± 11 18 ± 19
55 200.0549 0.783 26 ± 9 63 ± 19 −12 ± 17 25 ± 7 10 ± 8 45 ± 19
55 210.0368 0.832 9 ± 10 −9 ± 16 15 ± 11 4 ± 11
55 201.0296 0.888 32 ± 21 14 ± 23 20 ± 10 43 ± 20
55 202.0438 0.993 20 ± 14 22 ± 16 1 ± 6 24 ± 15

41 Eri A – more massive, with stronger Hg and Fe lines
55 210.2561 0.276 −89 ± 22 31 ± 25 −38 ± 23
55 201.2687 0.483 −6 ± 21 −3 ± 14
55 212.2414 0.673 36 ± 25 29 ± 10
55 213.2305 0.870 98 ± 47 39 ± 33

41 Eri B – less massive with stronger Mn and Ti lines
55 210.2561 0.276 94 ± 35 81 ± 28
55 201.2687 0.483 −6 ± 21 −3 ± 14
55 212.2414 0.673 −103 ± 27 −34 ± 30 −31 ± 10 −1 ± 11
55 213.2305 0.870 −72 ± 29 −40 ± 22

66 Eri A
55 203.2457 0.063 −17 ± 74 −11 ± 43
55 209.2426 0.194 119 ± 86 32 ± 58
55 204.2384 0.250 27 ± 72 34 ± 26
55210.2476 0.384 5 ± 86 −61 ± 54
55 205.2570 0.442 13 ± 74 −1 ± 35
55 211.2523 0.573 −16 ± 47 −20 ± 40
55 206.2375 0.627 −30 ± 66 −40 ± 32
55 212.2290 0.757 −54 ± 49 −71 ± 32
55 207.2363 0.816 −138 ± 62 −25 ± 23
55 202.2262 0.870 −41 ± 73 −48 ± 50

66 Eri B
55 203.2445 0.063 14 ± 38 76 ± 44
55 209.2415 0.194 −95 ± 29 −37 ± 31 −34 ± 42
55 204.2372 0.250 −7 ± 32 −13 ± 40
55 210.2464 0.384 −63 ± 40 −6 ± 32
55 205.2558 0.442 −81 ± 63 −41 ± 49
55 211.2506 0.573 −16 ± 47 −20 ± 40
55 206.2364 0.627 41 ± 35 −30 ± 37
55212.2273 0.757 68 ± 30 61 ± 33
55 207.2351 0.816 35 ± 23 24 ± 28
55 202.2251 0.870 16 ± 49 66 ± 43
HD 33904
55 204.7676 −32 ± 11 −3 ± 14

AR Aur A
55 544.1347 0.030 −138 ± 97 −160 ± 89 −213 ± 108
55 553 2003 0.223 62 ± 96 −29 ± 76 −101 ± 93
55 554.0300 0.424 266 ± 110 82 ± 41 254 ± 88
55 555.1200 0.687 −199 ± 63 64 ± 65 −207 ± 67 33 ± 69 −216 ± 68 78 ± 72
55 556.0350 0.908 −335 ± 94 −70 ± 98 −220 ± 59 −30 ± 65 −353 ± 100 −50 ± 112

AR Aur B
55 544.1347 0.030 208 ± 116 263 ± 85 −61 ± 80
55 553 2003 0.223 201 ± 136 140 ± 58
55 554.0300 0.424 −162 ± 61 −116 ± 63
55 555.1200 0.687 196 ± 73 165 ± 74
55 556.0350 0.908 71 ± 102 93 ± 89

HD 53244
55 204.2799 62 ± 43 85 ± 49 98 ± 46

HD 78316
55 202.3038 −22 ± 15 −52 ± 23 −32 ± 10 −4 ± 11
55 211.2873 84 ± 38 −13 ± 18 3 ± 17

HD 101189
55 201.3629 −74 ± 24 22 ± 25 −24 ± 18 −42 ± 26 −37 ± 11 −6 ± 12

HD 179761
55 319.4267 −88 ± 49

HD 209459
55 417 1494 99 ± 22 24 ± 21 68 ± 20 −5 ± 19 53 ± 17 9 ± 18
55 421.2598 31 ± 16 12 ± 19 27 ± 10

HD 221507
55 210.0485 78 ± 44 95 ± 58 56 ± 24 78 ± 25 −14 ± 24

Notes. Our phase zero for 66 Eri refers to conjunction i. Asterisks indicate rotation phases where the spectral lines of both components overlap. All quoted errors are 1σ uncertainties.

Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.

Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.

Initial download of the metrics may take a while.