000001955 001__ 1955
000001955 005__ 20160701171656.0
000001955 0247_ $$2DOI$$a10.1051/0004-6361:20011612
000001955 037__ $$aASTROimport-112
000001955 100__ $$aBlomme, R.
000001955 245__ $$aRadio and submillimetre observations of epsilon Ori
000001955 260__ $$c2002
000001955 520__ $$aIn common with other early-type stars, epsilon 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 epsilon Ori: Abbott et al. (\cite{Abbott+al80}) found 1.6 +/- 0.5 mJy, while Scuderi et al. (\cite{Scuderi+al98}) measured only 0.60 +/- 0.06 mJy. This could indicate that the large-scale structure persists beyond ~ 50 R*. To further investigate this variability, we used the Very Large Array (VLA) to monitor epsilon 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. (\cite{Abbott+al80}) 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 epsilon Ori is therefore similar to what had been found previously for alpha Cam, delta Ori A, kappa Ori and zeta Pup. While the present data do not allow very strong constraints, they show that considerable structure must persist up to at least ~ 10 R* in the wind of epsilon Ori. The combined radio fluxes are used to derive a mass-loss rate of log dot {M} (Msun/yr)= -5.73 +/- 0.04. This value is in good agreement with the Ha mass-loss rate. The good agreement between Ha 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. 
000001955 700__ $$a Prinja, R. K.
000001955 700__ $$a Runacres, M. C.
000001955 700__ $$a Colley, S.
000001955 773__ $$c921-934$$pAstronomy and Astrophysics$$v382$$y2002
000001955 85642 $$ahttp://esoads.eso.org/abs/2002A%26A...382..921B
000001955 905__ $$apublished in
000001955 980__ $$aREFERD