Stars with masses in the range of
and
luminosities of
populate the upper
left end of the Hertzsprung-Russell Diagram (HRD). During
their short lives of
107 yrs they evolve from hot O stars
on the main sequence towards cooler temperatures, first at almost
constant luminosities. They soon enter a phase of very strong
mass loss of up to
.
This
influences their further evolution dramatically: They do not
evolve further towards lower temperatures, i.e., towards the red
supergiant state, but rather turn in the HRD and become hotter
again, albeit later less luminous (e.g., Schaller et al. 1992;
Langer et al. 1994).
The region in the HRD where this turn occurs is known to be the domain of the Luminous Blue Variables (LBVs). There exists an empirical limit that separates a region in the HRD into which the most massive stars do not evolve, the so-called Humphreys-Davidson Limit (Humphreys & Davidson 1979, 1994). Here the stars not only exhibit large continuous mass loss, but at least some of them undergo giant eruptions. Both, the continuous wind and the eruptions lead to a peeling off of the outer parts of the stellar envelope and to the formation of circumstellar LBV nebulae (LBVN; e.g., Nota et al. 1995). Humphreys & Davidson (1994) classify 32 stars as LBVs and an additional 9 as candidates. 9 of the LBVs and candidate stars are located in the Milky Way and 10 in the Large Magellanic Cloud (LMC).
S 119 (
)
is one of
the LBVs in the LMC. It was classified as Ofpe/WN9 star by
Bohannan & Walborn (1989). Since the early eighties, there was
already the suspicion of a close relation between Ofpe/WN9 stars
and LBVs when R127, located again in the LMC and previously
classified as Ofpe/WN9 underwent an LBV outburst (Stahl et al.
1983). The evidence for a connection between the two stellar
classes has become even stronger since then, as longtime
spectroscopic monitoring of LBVs and Ofpe/WN9 stars became
available (see, e.g., Stahl & Wolf 1986; Wolf et al. 1988;
Bohannan & Walborn 1989; Nota et al. 1996; Pasquali et al.
1996).
After discovering a nebula around S 119, Nota et al. (1994)
classified the star as an LBV candidate. Their ESO New
Technology Telescope (NTT) image shows a nebula of
7
9
size (corresponding to
1.9 pc
2.1 pc for an assumed distance of the
LMC of 51.2 kpc), with a
brighter lobe. Their NTT/EMMI spectra indicate an expansion
velocity of the S 119 nebula of
25 km s-1, and a ratio of
H
/N
1, leading to [N II]
6583 Å/H
0.75. They derive a
radial velocity of the star and of the center of expansion in the
range of
100 - 140 km s-1. This casts doubt on S 119 being a
member of the LMC the radial velocity of which as derived from
H I observations (Rohlfs et al. 1984) is typically in the
range of
240 - 300 km s-1.
From the line ratio of [S II]6716/6731 Å Nota et al. (1994)
derived an electron density of
cm-3and - assuming an electron temperature of
K - estimated a nebula mass of
1.7
.
Similar results for the nebula were reported by Smith et al. (1998). They describe the nebula as elliptical of size
7
6, with
K as estimated from
the non-detection of the [N II]5755 Å line, and
cm-3. Little reddening and a radial
velocity of
km s-1 supports S 119 not being a
member of the main body of the LMC. The main stellar parameters
of S 119 have been determined by Crowther & Smith (1997) using
two different models to account for the contamination of the
nebula in the stellar spectrum:
,
,
and
.
In this contribution, we present results of an analysis of the kinematics of the nebula around S 119 and put it for the first time into perspective with the nebula's high-resolution morphology as obtained from Hubble Space Telescope (HST) images. Moreover, we use the non-detection of S 119 and its nebula with the High Resolution Imager (HRI) on board the Röntgensatellit (ROSAT) for determining and discussing upper limits of the X-ray emission.
Copyright ESO 2003