2012A&A...547A..90H


Query : 2012A&A...547A..90H

2012A&A...547A..90H - Astronomy and Astrophysics, volume 547A90-90 (2012/11-1)

Magnetic fields of HgMn stars.

HUBRIG S., GONZALEZ J.F., ILYIN I., KORHONEN H., SCHOELLER M., SAVANOV I., ARLT R., CASTELLI F., LO CURTO G., BRIQUET M. and DALL T.H.

Abstract (from CDS):

The frequent presence of weak magnetic fields on the surface of spotted late-B stars with HgMn peculiarity in binary systems has been controversial during the two last decades. Recent studies of magnetic fields in these stars using the least-squares deconvolution (LSD) technique have failed to detect magnetic fields, indicating an upper limit on the longitudinal field between 8 and 15G. In these LSD studies, assumptions were made that all spectral lines are identical in shape and can be described by a scaled mean profile. We re-analyse the available spectropolarimetric material by applying the moment technique on spectral lines of inhomogeneously distributed elements separately. Furthermore, we present new determinations of the mean longitudinal magnetic field for the HgMn star HD65949 and the hotter analog of HgMn stars, the PGa star HD19400, using FORS2 installed at the VLT. We also give new measurements of the eclipsing system ARAur with a primary star of HgMn peculiarity, which were obtained with the SOFIN spectropolarimeter installed at the Nordic Optical Telescope. We downloaded from the European Southern Observatory (ESO) archive the publically available HARPS spectra for eight HgMn stars and one normal and one superficially normal B-type star obtained in 2010. Out of this sample, three HgMn stars belong to spectroscopic double-lined systems. The application of the moment technique to the HARPS and SOFIN spectra allowed us to study the presence of the longitudinal magnetic field, the crossover effect, and quadratic magnetic fields.
Result. for the HgMn star HD65949 and the PGa star HD19400 are based on a linear regression analysis of low-resolution spectra obtained with FORS2 in spectropolarimetric mode. Our measurements of the magnetic field with the moment technique using spectral lines of several elements separately reveal the presence of a weak longitudinal magnetic field, a quadratic magnetic field, and the crossover effect on the surface of several HgMn stars as well as normal and superficially normal B-type stars. Furthermore, our analysis suggests the existence of intriguing correlations between the strength of the magnetic field, abundance anomalies, and binary properties. The results are discussed in the context of possible mechanisms responsible for the development of the element patches and complex magnetic fields on the surface of late B-type stars.

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Journal keyword(s): stars: chemically peculiar - stars: atmospheres - binaries: spectroscopic - stars: abundances - stars: early-type - stars: magnetic field

Simbad objects: 25

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Number of rows : 25
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 * phi Phe SB* 01 54 22.0319152104 -42 29 48.942141036   5.055 5.109     A3V 120 0
3 * tet Hyi ** 03 02 15.4488409848 -71 54 08.839047780   5.365 5.499     B8III/IV 102 0
4 * 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
5 * 66 Eri a2* 05 06 45.6527881872 -04 39 18.601025148 4.89 5.06 5.12     B9V 157 1
6 UCAC2 30135337 * 05 06 46.2895252656 -04 38 26.450432448 13.34 11.94 10.80 10.58 9.65 ~ 15 1
7 * 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
8 * 17 Aur SB* 05 18 18.8960529504 +33 46 02.516925540   6.102 6.144     B9V+B9.5V 308 0
9 Ass Aur OB 1 As* 05 22 +33.9           ~ 85 0
10 * gam CMa * 07 03 45.4934693195 -15 37 59.833212992 3.52 4.00 4.12 4.13 4.23 B8II 193 0
11 HD 64949 * 07 55 27.1411320048 -25 35 07.729365984   10.18 9.17     G8/K0III 5 0
12 HD 65949 * 07 57 47.6703410424 -60 36 34.921501344 7.99 8.31 8.37     B8/9 108 0
13 NGC 2516 OpC 07 58 00.5 -60 46 36           ~ 793 0
14 * kap Cnc a2* 09 07 44.8095541176 +10 40 05.519586828 4.70 5.13 5.24     B8IIImnp 376 0
15 * K Car * 10 30 20.1277680782 -71 59 34.057907711   4.751 4.710     A1V 90 0
16 NGC 3766 OpC 11 36 13.5 -61 36 42   5.66 5.3     ~ 222 0
17 HD 101189 PM* 11 38 07.2695736768 -61 49 35.512404852 4.96 5.13 5.14     ApHgMn 85 0
18 * chi Lup SB* 15 50 57.5453432166 -33 37 37.728345509 3.77 3.909 3.946     B9III 318 0
19 V* V373 Ser a2* 15 52 35.0679747816 -01 01 52.823239248   8.16 7.97     B9V 60 0
20 HD 177863 SB* 19 07 08.3266173557 -18 44 17.407077555   6.243 6.293     B8V 79 0
21 * 21 Aql a2* 19 13 42.7011956712 +02 17 37.310297604 4.67 5.08 5.15     B8III 243 0
22 HD 208459 * 21 56 20.6230016304 -04 45 22.956221628   9.14 7.54     M0III 11 0
23 * 21 Peg * 22 03 19.0326115488 +11 23 11.574375540   5.762 5.822     B9.5V 160 0
24 * 74 Aqr a2* 22 53 28.7049178152 -11 36 59.453153568 5.41 5.709 5.780     B8IV/V 160 0
25 * 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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