The stellar energy distribution derived by
color calibration is not accurate due to uncertainties of the bolometric
magnitude () for hot stars with log
> 4.4
(Massey et al. 1995).
Therefore we need to place these stars in the H-R diagram with the help of spectral types
obtained by spectroscopy.
We deduced values of E(B-V), and log
which are listed
in Tables 1 and 2 where Cols. 1 and 2 give the stellar identification,
and Col. 3 the epoch 2000 coordinates.
We adopted a distance modulus
m - M = 18.5 (e.g. Panagia et al. 1991) for the LMC, and an ordinary ratio
R = 3.1 = AV/E(B-V).
The (B-V)0 intrinsic color indices, the
bolometric corrections (BC) and
for different spectral types were taken from Schmidt-Kaler (1982), except
for O stars for which the values from Chlebowski & Garmany (1991) were used.
For WR stars the
is from Hamann et al. (1991) and
Koesterke et al. (1991) and BC from Smith
Maeder (1989).
The differences between the observational and the theoretical values of the Q parameter
listed in Col. 7 of Tables 1 and 2, show that in a nebula and bad photometric conditions
this parameter is not reliable for hot stars,
contrary to the spectroscopy classification (e.g.
for the stars 5-31 and 5-52 instead of
) .
The resulting H-R diagrams log vs.
for both OB associations
are shown in Figs. 6a and b. We discriminated
between stars with spectral classifications and those with photometry only,
denoting them with different symbols.
We also overlaid a few stellar evolutionary tracks and isochrones calculated by
Schaerer et al. (1993) for a metallicity of Z = 0.008.
In Tables 1 and 2 the apparent magnitudes and the colors of the three WR + O
systems refer to the observed integrated magnitude, as is the case for the
spectroscopic binary star 5-65 of type O7If. The composite spectra are shown
in Fig. 5a and Fig. 5d.
The derived from these integrated magnitudes
does not have any clear meaning.
However these stars should be taken into account in the HR diagram and the IMF.
As a first approximation, since spectra of both components are visible, we
have assumed that these systems are composed of two stars of similar magnitudes,
and that the O components in the WR systems are of luminosity class V.
In the HR diagrams of Figs. 6a and b, we have plotted the positions of the
O+O and WR+O systems as they would appear with the values which
result from the apparent integrated magnitude and
of the O type
component. This illustrates how the stars would appear in the HR diagram if
we had no information about their binarity.
Arrows are drawn from these positions in the HR diagram to where the
components would be located assuming two equal magnitude stars of the observed
spectral types.
In LH 104 this procedure locates the WR+O systems in the
bin .
LH 101 seems to consist of two subpopulations (Table 4). A comparison with the
isochrones shows that the younger subgroup has an age of 2 Myr
and the older one of
3-6 Myr. As noted by Testor & Niemela (1996),
stars outside the nebulosity seem
to be somewhat more evolved than those inside the nebulosity. Thus sequential
star formation appears to be present even at scales less than 50 pc.
LH 104 consists mainly of a young population spreading out between 2 and 6 Myr (Table 4). The HR diagrams also show in both associations a group of older and less massive stars.
Notes to Table 4:
Column 1: Masses |
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