2002A&A...382..921B


Query : 2002A&A...382..921B

2002A&A...382..921B - Astronomy and Astrophysics, volume 382, 921-934 (2002/2-2)

Radio and submillimetre observations of {epsilon Ori}.

BLOMME R., PRINJA R.K., RUNACRES M.C. and COLLEY S.

Abstract (from CDS):

In common with other early-type stars, ε Ori (B0 Ia) shows evidence for structure in its stellar wind. Variations in optical and ultraviolet line profiles reveal the presence of large-scale structure in the inner wind. The detection of X-rays and the existence of black troughs in saturated ultraviolet lines are indicative of small-scale structure. The geometric extent of both types of structure is poorly known. In principle, large-scale structure can be detected directly from very high spatial resolution observations that resolve the stellar wind. A simpler technique is to look for the presence of additional flux compared to that expected from a smooth wind. The run of this excess flux as a function of wavelength indicates how fast structure decays in the wind. If there is variability in the excess flux, it shows us that the structure must be large-scale. Such variability is suggested by two previous 6 cm radio observations of ε Ori: Abbott et al. (1980ApJ...238..196A) found 1.6±0.5mJy, while Scuderi et al. (1998A&A...332..251S) measured only 0.60±0.06mJy. This could indicate that the large-scale structure persists beyond ∼50R*. To further investigate this variability, we used the Very Large Array (VLA) to monitor ε Ori over a 5-day period in February 1999. We supplemented our data with observations from the VLA archive. In an attempt to resolve the stellar wind, we also obtained a series of high spatial resolution observations with the Multi-Element Radio Linked Interferometer Network (MERLIN) during January-March 1999. From this combined material we find no evidence for variability and we conclude that the Abbott et al. (1980ApJ...238..196A) flux determination is in error. The data do show substantial excess flux at millimetre wavelengths, compared to a smooth wind. This excess is confirmed by a submillimetre observation which we obtained with the James Clerk Maxwell Telescope (JCMT). The behaviour of ε Ori is therefore similar to what had been found previously for α Cam, δ Ori A, κ Ori and ζ Pup. While the present data do not allow very strong constraints, they show that considerable structure must persist up to at least ∼10R* in the wind of ε Ori. The combined radio fluxes are used to derive a mass-loss rate of log{dot}(M)(M/yr)=-5.73±0.04. This value is in good agreement with the Hα mass-loss rate. The good agreement between Hα and radio mass-loss rates for hot stars in general remains puzzling, as it implies that the same amount of structure is present in very different formation regions.

Abstract Copyright:

Journal keyword(s): stars: early-type - stars: individual: ε Ori - stars: mass-loss - stars: winds, outflows - continuum: stars radio

Simbad objects: 21

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Number of rows : 21
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2023
#notes
1 3C 48 QSO 01 37 41.2996631208 +33 09 35.080388820   16.62 16.20     ~ 2767 2
2 * psi Per Be* 03 36 29.3798227 +48 11 33.478941 3.60 4.17 4.23     B5Ve 412 0
3 V* HL Tau Or* 04 31 38.5107609312 +18 13 57.859747968   15.89 14.49 14.39   K5 1393 0
4 IRAS 04287+1807 mul 04 31 38.8 +18 13 57           ~ 796 0
5 * alf Cam s*b 04 54 03.0103983 +66 20 33.636467 3.47 4.34 4.29 4.18 4.18 O9Ia 659 1
6 ICRF J050321.1+020304 Sy2 05 03 21.19716454 +02 03 04.6765714   22.500 21.350 20.682   ~ 186 1
7 ICRF J052109.8+163822 Sy1 05 21 09.88596258 +16 38 22.0515459   19.37 18.84 18.480   ~ 835 1
8 ICRF J052217.4+011331 BLL 05 22 17.46744175 +01 13 31.1853463       20   ~ 61 1
9 * del Ori SB* 05 32 00.40009 -00 17 56.7424 0.96 2.02 2.41 2.32 2.54 O9.5IINwk 772 0
10 QSO B0529+075 QSO 05 32 38.9985483000 +07 32 43.344156480   19.0 19.00 17.50   ~ 209 1
11 * eps Ori s*b 05 36 12.81335 -01 12 06.9089 0.48 1.51 1.69 1.76 1.93 B0Ia 893 0
12 NAME Ori I As* 05 38 -02.8           ~ 606 0
13 QSO B0539-057 QSO 05 41 38.08336552 -05 41 49.4283917     20.4 20.70   ~ 245 2
14 ICRF J054236.1+495107 Sy1 05 42 36.13789710 +49 51 07.2337139   18.45 17.80 17.210   ~ 1449 1
15 * kap Ori s*b 05 47 45.3888404 -09 40 10.577707 0.87 1.88 2.06 2.09 2.27 B0.5Ia 567 0
16 QSO B0605-0834 BLL 06 07 59.69924014 -08 34 49.9783246     17.60 17.70   ~ 441 1
17 * zet Pup BY* 08 03 35.04754 -40 00 11.3321 0.89 1.98 2.25 2.36 2.58 O4I(n)fp 1146 1
18 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4252 2
19 QSO B1404+286 BLL 14 07 00.39441712 +28 27 14.6901341   16.13 15.35 10.29   ~ 753 2
20 * P Cyg s*b 20 17 47.2020844 +38 01 58.552724 4.66 5.24 4.82 4.28 4.02 B1-2Ia-0ep 1170 1
21 EM* AS 431 WR* 20 36 43.6322747712 +40 21 07.442607924     13.73 12.51   WN8(h)+B0.5V 216 0

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2023.10.04-05:44:34

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