2007A&A...475.1053A


Query : 2007A&A...475.1053A

2007A&A...475.1053A - Astronomy and Astrophysics, volume 4751053-1065 (2007/12-1)

Weak magnetic fields in Ap/Bp stars. Evidence for a dipole field lower - limit and a tentative interpretation of the magnetic dichotomy.

AURIERE M., WADE G.A., SILVESTER J., LIGNIERES F., BAGNULO S., BALE K., DINTRANS B., DONATI J.F., FOLSOM C.P., GRUBERBAUER M., HUI BON HOA A., JEFFERS S., JOHNSON N., LANDSTREET J.D., LEBRE A., LUEFTINGER T., MARSDEN S., MOUILLET D., NASERI S., PALETOU F., PETIT P., POWER J., RINCON F., STRASSER S. and TOQUE N.

Abstract (from CDS):

We investigated a sample of 28 well-known spectroscopically-identified magnetic Ap/Bp stars, with weak, poorly-determined or previously undetected magnetic fields. The aim of this study is to explore the weak part of the magnetic field distribution of Ap/Bp stars. Using the MuSiCoS and NARVAL spectropolarimeters at Telescope Bernard Lyot (Observatoire du Pic du Midi, France) and the cross-correlation technique Least Squares Deconvolution (LSD), we obtained 282 LSD Stokes V signatures of our 28 sample stars, in order to detect the magnetic field and to infer its longitudinal component with high precision (median σ=40G). For the 28 studied stars, we obtained 27 detections of Stokes V Zeeman signatures from the MuSiCoS observations. Detection of the Stokes V signature of the 28th star (HD 32650) was obtained during science demonstration time of the new NARVAL spectropolarimeter at Pic du Midi. This result clearly shows that when observed with sufficient precision, all firmly classified Ap/Bp stars show detectable surface magnetic fields. Furthermore, all detected magnetic fields correspond to longitudinal fields which are significantly greater than some tens of G. To better characterise the surface magnetic field intensities and geometries of the sample, we phased the longitudinal field measurements of each star using new and previously-published rotational periods, and modeled them to infer the dipolar field intensity (Bd, measured at the magnetic pole) and the magnetic obliquity (β). The distribution of derived dipole strengths for these stars exhibits a plateau at about 1kG, falling off to larger and smaller field strengths. Remarkably, in this sample of stars selected for their presumably weak magnetic fields, we find only 2 stars for which the derived dipole strength is weaker than 300G. We interpret this ``magnetic threshold'' as a critical value necessary for the stability of large-scale magnetic fields, and develop a simple quantitative model that is able to approximately reproduce the observed threshold characteristics. This scenario leads to a natural explanation of the small fraction of intermediate-mass magnetic stars. It may also explain the near-absence of magnetic fields in more massive B and O-type stars.

Abstract Copyright: ∼

Journal keyword(s): stars: chemically peculiar - stars: magnetic fields

VizieR on-line data: <Available at CDS (J/A+A/475/1053): stars.dat table3.dat>

Simbad objects: 37

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Number of rows : 37
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 V* HN And a2* 01 24 18.6765786624 +43 08 31.629475248   6.704 6.676     A4VpSrSi 153 0
2 * 43 Cas a2* 01 42 20.5269432072 +68 02 34.890489276 5.29 5.52 5.59     A0VpSiSrEuHgMn 123 0
3 HD 10589 PM* 01 43 31.7141425128 +10 28 15.365246916   9.68 9.18     F8 4 0
4 HD 15144 a2* 02 26 00.3479612520 -15 20 28.495226652 6.06 5.97 5.83 5.71 5.67 A3VpSrCrEu 185 0
5 * iot Cas a2* 02 29 03.94780 +67 24 08.9170           A3IIIpSr+F5V 268 0
6 * 21 Per a2* 02 57 17.2817216760 +31 56 03.193498176   5.081 5.093     A2VspSiEu 206 0
7 * 9 Tau a2* 03 36 58.0258965288 +23 12 39.846279780 6.960 6.840 6.730     A2p 110 0
8 * 56 Tau a2* 04 19 36.7048893816 +21 46 24.566827836   5.231 5.346     A0VpSi 193 0
9 * 11 Ori a2* 05 04 34.1491891634 +15 24 14.767720310   4.609 4.661     A1VpSiCr 156 0
10 V* BN Cam a2* 05 12 22.4545154808 +73 56 48.040416348 4.970 5.320 5.450     B9.5VpSi 106 0
11 * tet01 Ori C SB* 05 35 16.4662967280 -05 23 22.921811880 4.20 5.15 5.13 4.91 4.73 O7Vp 1479 1
12 NAME Ori I As* 05 38 -02.8           ~ 653 0
13 HD 37687 * 05 40 19.7244660720 -03 25 37.491283092 6.64 7.052 7.045     B7/8II/III 65 0
14 * 137 Tau a2* 05 52 22.2914333688 +14 10 18.428386584   5.532 5.586     A0VpSiSrCr 111 0
15 HD 40711 SB* 06 01 01.2946494792 +10 24 05.415878916   8.76 8.57     ApSrCrEu 41 0
16 V* V1155 Ori a2* 06 19 01.8426917616 +17 19 30.943758540 5.95 6.25 6.32     B9IIIpSi(Cr) 152 0
17 * 15 Cnc a2* 08 13 08.8680600240 +29 39 23.536760076   5.541 5.605     B8VpSi 138 0
18 * 3 Hya a2* 08 35 28.1987898408 -07 58 56.257821768 5.68 5.69 5.72     A1VpSrCr 178 0
19 * 45 Leo a2* 10 27 38.9889218664 +09 45 44.610005160 5.89 5.98 6.04     B9.5IV-VpSiCrSr(Mn) 144 0
20 HD 94427 * 10 53 56.7156975264 -12 26 04.372674396   7.73 7.36     ApSrEuCr 39 0
21 V* EP UMa a2* 11 09 39.7864853928 +67 12 36.756332280   6.278 6.061     A7IVpSr 88 0
22 * 65 UMa SB* 11 55 05.7460955088 +46 28 36.597092700   6.76 6.67     hA5VkA2mA3 150 0
23 * 65 UMa D * 11 55 11.3304120408 +46 28 11.166446208   7.007 6.965     F0IVspCrSrEu 89 0
24 Cl Melotte 111 OpC 12 11 54.9 +25 16 36           ~ 520 0
25 * 21 Com a2* 12 31 00.5605002264 +24 34 01.797245328   5.496 5.436     A2pv 295 0
26 * ome Her a2* 16 25 24.9546742056 +14 01 59.762072676 4.53 4.57 4.58 4.51 4.55 A2VpCrSr 242 0
27 * tau Sco * 16 35 52.9528530 -28 12 57.661515 1.55 2.56 2.81 2.93 3.18 B0V 959 0
28 * l Her a2* 16 47 46.4200216512 +05 14 48.291336960 5.20 5.22 5.24     A1VpSi 138 0
29 HD 171586 a2* 18 35 36.4929240936 +04 56 09.562670484 6.52 6.53 6.46     A0VpSrSi 84 0
30 V* QV Ser a2* 18 36 29.6322862008 +05 17 19.214997756 7.60 7.86 7.84     A0p 60 0
31 IC 4756 OpC 18 38 39.0 +05 26 14           ~ 274 0
32 * 19 Lyr a2* 19 11 46.0084477416 +31 17 00.443746788   5.866 5.932     B8IIIpSiSr 105 0
33 * 4 Cyg a2* 19 26 09.1269274848 +36 19 04.432147356 4.60 5.03 5.15     B8pSi(FeII) 148 0
34 HD 191612 SB* 20 09 28.6105997664 +35 44 01.286453904 7.40 8.07 7.80     O8fpe 250 0
35 HD 204411 a2* 21 26 51.6219389280 +48 50 06.599806584 5.54 5.38 5.31     A4VpSiCrHg 190 0
36 * bet Cep bC* 21 28 39.5968513 +70 33 38.574681 2.05 3.01 3.23 3.33 3.55 B0.5IIIs 756 0
37 * kap Psc a2* 23 26 55.9558721856 +01 15 20.177913204 4.94 4.98 4.94 4.87 4.90 A2VpSrCrSi 290 0

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