2011A&A...525A..97M


Query : 2011A&A...525A..97M

2011A&A...525A..97M - Astronomy and Astrophysics, volume 525A97-97 (2011/1-1)

The search for magnetic fields in mercury-manganese stars.

MAKAGANIUK V., KOCHUKHOV O., PISKUNOV N., JEFFERS S.V., JOHNS-KRULL C.M., KELLER C.U., RODENHUIS M., SNIK F., STEMPELS H.C. and VALENTI J.A.

Abstract (from CDS):

A subclass of the upper main-sequence chemically peculiar stars, mercury-manganese (HgMn) stars were traditionally considered to be non-magnetic, showing no evidence of variability in their spectral line profiles. However, discoveries of chemical inhomogeneities on their surfaces imply that this assumption should be investigated. In particular, spectroscopic time-series of AR Aur, α And, and five other HgMn stars indicate the presence of chemical spots. At the same time, no signatures of global magnetic fields have been detected. We attempt to understand the physical mechanism that causes the formation of chemical spots in HgMn stars and gain insight into the potential magnetic field properties at their surfaces; we performed a highly sensitive search for magnetic fields for a large set of HgMn stars. With the aid of a new polarimeter attached to the HARPS spectrometer at the ESO 3.6m-telescope, we obtained high-quality circular polarization spectra of 41 single and double HgMn stars. Using a multi-line analysis technique on each star, we co-added information from hundreds of spectral lines to ensure significantly greater sensitivity to the presence of magnetic fields, including very weak fields. For the 47 individual objects studied, including six components of SB2 systems, we do not detect any magnetic fields at greater than the 3σ level. The lack of detection in the circular polarization profiles indicates that if strong fields are present on these stars, they must have complex surface topologies. For simple global fields, our detection limits imply upper limits to the fields present of 2-10Gauss in the best cases. We conclude that HgMn stars lack large-scale magnetic fields, which is typical of spotted magnetic Ap stars, of sufficient strength to form and sustain the chemical spots observed on HgMn stars. Our study confirms that in addition to magnetically altered atomic diffusion, there exists another differentiation mechanism operating in the atmospheres of late-B main sequence stars that can produce compositional inhomogeneities on their surfaces.

Abstract Copyright: ∼

Journal keyword(s): stars: chemically peculiar - stars: magnetic field - polarization

Simbad objects: 46

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Number of rows : 46
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 * alf And a2* 00 08 23.25988 +29 05 25.5520 1.48 1.95 2.06 2.09 2.19 B8IV-VHgMn 479 1
2 V* AV Scl a2* 00 23 12.6093196608 -31 02 08.778859512 6.24 6.484 6.547     B9IV 105 0
3 * phi Phe SB* 01 54 22.0319152104 -42 29 48.942141036   5.055 5.109     A3V 120 0
4 HD 23950 * 03 49 55.0695142800 +22 14 38.936066064   6.046 6.070     B8III 121 0
5 * ups04 Eri SB* 04 17 53.6624004496 -33 47 54.052408258 3.07 3.44 3.56 3.57 3.68 B8V+B9.5V? 168 0
6 HD 28217 ** 04 27 28.7694788712 +11 12 44.209409004 5.58 5.902 5.870     B8IV 79 0
7 * 93 Tau Pu* 04 40 03.4199311320 +12 11 51.406702908   5.319 5.445     B8IV 83 0
8 * 66 Eri a2* 05 06 45.6527881872 -04 39 18.601025148 4.89 5.06 5.12     B9V 157 1
9 HD 33647 a2* 05 11 41.3498014 +00 30 52.459194   6.601 6.667     B8II/III 99 0
10 * mu. Lep a2* 05 12 55.9029641016 -16 12 19.668599100 2.78 3.18 3.29 3.30 3.42 B9IV:HgMn 294 1
11 * 17 Aur SB* 05 18 18.8960529504 +33 46 02.516925540   6.102 6.144     B9V+B9.5V 308 0
12 HD 34880 SB* 05 20 26.4073556606 -05 22 03.093419327 6 6.37 6.42     B8II 52 0
13 HD 35548 ** 05 25 31.0794483731 -00 32 38.128886484 6.34 6.52 6.56     B9III 159 0
14 HD 36881 SB* 05 35 13.2466726656 +10 14 24.278794332 5.66 5.734 5.638     B9IIIp 70 0
15 HD 42657 a2* 06 11 43.7171543332 -04 39 55.602985022 5.73 6.10 6.18     B8II/III 62 0
16 * gam CMa * 07 03 45.4934693195 -15 37 59.833212992 3.52 4.00 4.12 4.13 4.23 B8II 193 0
17 HD 53929 * 07 07 06.4712319600 +04 54 38.091397320 5.52 5.961 6.088     B9III 105 0
18 * zet CMi * 07 51 41.9887267800 +01 46 00.726461076 4.58 5.03 5.16 5.18 5.33 B8II 102 0
19 HD 65950 V* 07 57 45.2194757688 -60 55 35.265618408 6.56 6.86 6.87     B8III 104 0
20 HD 68099 * 08 11 16.5989180688 +09 49 16.446964692 5.54 5.956 6.072     B6III 62 0
21 HD 70235 * 08 19 29.5116324864 -34 35 24.484060464   6.348 6.437     B8Ib/II 39 0
22 * kap02 Vol * 08 20 00.5275254216 -71 30 19.361671236   5.496 5.608     B9/A0IV 77 0
23 HD 71833 * 08 28 53.4289442664 -20 57 01.427571180 6.2 6.611 6.684     B8II 50 0
24 HD 72208 SB* 08 31 54.4939363800 +09 48 50.757520896   6.76 6.83     B9.5VpHgMnEu 61 0
25 * 14 Hya a2* 08 49 21.7258429872 -03 26 34.891438308 4.87 5.22 5.31     B8IIIpHgMn 154 0
26 * kap Cnc a2* 09 07 44.8095541176 +10 40 05.519586828 4.70 5.13 5.24     B8IIImnp 376 0
27 * L Car * 10 22 58.1465809448 -66 54 05.385596996 4.35 4.86 4.99     B8V 120 0
28 HD 101189 PM* 11 38 07.2695736768 -61 49 35.512404852 4.96 5.13 5.14     ApHgMn 85 0
29 * gam Crv PM* 12 15 48.37081 -17 32 30.9496 2.12 2.47 2.58 2.62 2.71 B8III 249 1
30 * l Cen ** 12 39 52.5291353564 -39 59 14.286324017 4.16 4.56 4.64 4.66 4.75 B8II/III 122 0
31 * chi Lup SB* 15 50 57.5453432166 -33 37 37.728345509 3.77 3.909 3.946     B9III 318 0
32 * n Her * 16 32 35.6854246680 +05 31 16.391769564 5.39 5.57 5.63     B9.5III 126 0
33 HD 158704 SB* 17 31 44.3739544896 -26 16 10.957302300   5.983 6.052     B9pHgMn 79 0
34 HD 165493 * 18 08 30.1115839488 -45 46 01.234303212   6.061 6.163     B7/8II 41 0
35 * alf Lyr dS* 18 36 56.33635 +38 47 01.2802 0.03 0.03 0.03 0.07 0.10 A0V 2787 1
36 HD 175640 * 18 56 22.6598858520 -01 47 59.503936200 5.86 6.149 6.196     B9IIIpHgMnEu 160 0
37 HD 178065 SB* 19 07 09.0293341368 +00 38 27.491355672 6.31 6.584 6.538     B9III 103 0
38 * 21 Aql a2* 19 13 42.7011956712 +02 17 37.310297604 4.67 5.08 5.15     B8III 243 0
39 * 46 Aql * 19 42 12.8123363760 +12 11 35.740659732   6.234 6.321     B9III 120 0
40 V* AV Cap a2* 20 08 31.2713683776 -10 03 45.343113336   6.201 6.174     B9IV 79 0
41 * bet02 Cap SB* 20 20 46.5478935096 -14 47 05.603724348   6.08 6.10     B9/A0III/IV 143 0
42 HD 194783 * 20 28 46.7436015264 -35 35 45.106798308   5.980 6.077     B8II/III 44 0
43 * 30 Cap * 21 17 57.2864746704 -17 59 06.499058280   5.263 5.383     B5II/III 96 0
44 * rho Aqr SB* 22 20 11.9165745768 -07 49 15.966995808 4.94 5.286 5.339     B8III 88 0
45 HD 216831 Pu* 22 55 44.5079270976 +36 21 05.025021984   5.665 5.725     B7III 89 0
46 * bet Scl PM* 23 32 58.2607029954 -37 49 05.825575113 3.92 4.28 4.37 4.37 4.44 B9.5IIIpHgMnSi 194 0

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