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3. Reddening and absolute magnitudes

The parameters derived from the photometry are presented in Tables 2a and 2b. The HD numbers, MK types and the reddening-corrected quantities (b-y)0, m0, c0 and V0 together with the color excess E(b-y) are given in the first six columns. The absolute magnitude Mv, the true distance moduli V0-Mv (for a normal extinction law (R=3.2) and a coefficient 0.74=E(b-y)/E(B-V)) and the distance r in parsecs are listed in the last three columns. It is well known that the color excess and absolute magnitude determination via uvbytex2html_wrap_inline869 photometric quantities have to be done using different calibrations for the different spectral and luminosity classes. For this reason, special attention was paid to the spectral classification of the program stars. The MK spectral types used here were adopted after a rigorous discussion with W. Buscombe (1994, private communication) on the basis of his collection of MK classification data.

The color excesses for III, IV, V luminosity classes are obtained from the calibration given by Crawford (1978). The intrinsic colors of Kilkenny & Whittet (1985) are used for the early-type supergiants with values of c0 > -0.17 and the calibration of Crawford (1978) for values smaller than -0.17. For this calculation, a simple iteration procedure was adopted using [c1] as a first value of c0.

The absolute magnitude values for all stars are derived via tex2html_wrap_inline869. The Balona & Shobbrook (1984) calibration is used for luminosity classes III, IV, V. In this calibration, attempts are made to correct the main uncertainties in the curve fitting method due to the width of the main sequence and the evolution away from the main sequence of stars at the high-mass end. The errors in the Mv values derived in this way are expected to be about 0.2 mag. For the supergiants, the tex2html_wrap_inline1017 relation of Zhang (1983) is applied. As is shown in Table IX of Zhang (1983), the standard deviation one should expect applying this calibration is of the same order: 0.2 mag.

 

HD MK Mv(Sp) tex2html_wrap_inline1025 tex2html_wrap_inline1027
s.e.
90273 O7Vf -4.9 0.5 -5.63   0.73
91572 O7Vf -4.9 0.5 -5.11   0.21
91598 O9Ve -4.4 0.6 -5.28   0.88
92504 O8Vn -4.6 0.6 -4.53 -0.07
92850 O9Ib -6.1 0.8 -5.53 -0.57
93403 O5IIIf -6.1 ... -6.16   0.06
94024 O8Vn -4.6 0.6 -5.91   1.31
94370 O6IIIf -5.7 0.3 -5.54 -0.16
94963 O6Vf -5.1 0.6 -5.52  0.42
95589 O7I -6.5 0.5 -6.08 -0.48
96042 O9.5Ve -4.0 0.6 -3.88 -0.12
96264 O6V -5.1 0.6 -4.95 -0.15
96715 O4Vf -5.8 0.8 -5.62 -0.18
96946 O7IIIf -5.6 0.6 -6.02  0.42
97166 O7.5IIf -5.0 0.4 -5.52  0.52
97319 O7.5V -5.0 ... -4.83 -0.12
97399 O9V -4.4 0.6 -4.38 -0.02
97434 O7IIIn -5.6 0.6 -5.86  0.26
97597 O8V -4.6 0.6 -3.99 -0.61
97848 O7.5II -5.6 0.4 -4.80 -0.8
97913 O9.5V -4.0 0.6 -5.42  1.42
99160 O9III -5.3 0.7 -5.71  0.41
99546 O7V -4.9 0.5 -4.88 -0.02
305438 O8V -4.6 0.6 -4.71  0.11
Table 3: Mv-values derived via Spectral types and Htex2html_wrap_inline869 indices for 24 O-type stars. The differences are given in the last column

 

It is often questioned whether the distance determination via the values of Htex2html_wrap_inline869 is reliable for O-type stars. There are 24 O-type stars in the sample. To compare the results given by the Mv/(uvbytex2html_wrap_inline869) and Mv/Sp calibrations, we have calculated the Mv values via Mv/Sp calibrations of Conti et al. (1983) and have compared them to the values derived via the Balona & Shobbrook (1984) relation. The results can be seen in Table 3 (click here), where the HD numbers and MK types are listed in the first two columns. The spectroscopic Mv values with the corresponding errors, as given in Table 1 of Conti et al. (1983) are shown in the third column. Note that this is the standard deviation of the mean instead of the standard deviation used to estimate the uncertainties concerning the other calibrations discussed here. In the last two columns, the Mv(uvbytex2html_wrap_inline869) values obtained here and the corresponding differences (Mv/Sp - Mv/(uvbytex2html_wrap_inline869)) are shown for each star. Taking into account the standard errors of the calibrations, these determinations agree within their 1tex2html_wrap_inline1175 errors. Only three stars show larger differences which could be due to a wrong LC determination. Deriving the absolute magnitude via Htex2html_wrap_inline869, one should expect that emission in the stellar spectra would make the stars brighter. To avoid this, for all stars with emissions indicated in their spectral classifications, the absolute magnitudes are also estimated via the spectral type - absolute magnitude calibration of Humphreys & McElroy (1984) (for tex2html_wrap_inline1179 types) and Balona & Crampton (1974) (for tex2html_wrap_inline1181 types). The results of these different types of estimation agree well within the errors.

For 14 stars in the fields of Car OB1 and Car OB2 which are earlier than B4-type according to the PPM catalog but were not observed during this run, uvbytex2html_wrap_inline869 photometry is available in the literature. For these stars, we have also calculated the reddening-corrected quantities, color excesses, absolute magnitudes and the true distance moduli. These data are shown in Table 4. The third and forth columns of this table contain the MK classification and the sources of the photometric data. Also not included in our sample are thirteen stars referred by Humphreys (1978) to Car OB1 and one star referred to Car OB2. For most of them, tex2html_wrap_inline1185 photometry is available and the distances can be derived using a tex2html_wrap_inline1187 calibration. These stars are listed in Table 5. The photometric data and MK classifications are taken from the OB-star data base of Reed (1993) and the Mv values are calculated via the new tex2html_wrap_inline1187 calibration of Reed & Beatty (1995).


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